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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mol. Neurosci.</journal-id>
<journal-title>Frontiers in Molecular Neuroscience</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mol. Neurosci.</abbrev-journal-title>
<issn pub-type="epub">1662-5099</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fnmol.2017.00394</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Neuroscience</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>The Contribution of L-Type Ca<sub>v</sub>1.3 Channels to Retinal Light Responses</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Shi</surname> <given-names>Liheng</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/458311/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Chang</surname> <given-names>Janet Ya-An</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/498698/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Yu</surname> <given-names>Fei</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Ko</surname> <given-names>Michael L.</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Ko</surname> <given-names>Gladys Y.-P.</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/78185/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Department of Veterinary Integrative Biosciences, Texas A&#x00026;M University</institution>, <addr-line>College Station, TX</addr-line>, <country>United States</country></aff>
<aff id="aff2"><sup>2</sup><institution>Texas A&#x00026;M Institute of Neuroscience, Texas A&#x00026;M University</institution>, <addr-line>College Station, TX</addr-line>, <country>United States</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Andrei Surguchov, University of Kansas Medical Center Research Institute, United States</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Henrique Prado von Gersdorff, Oregon Health and Science University, United States; Karin Dedek, University of Oldenburg, Germany</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Gladys Y.-P. Ko <email>gko&#x00040;cvm.tamu.edu</email></p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>05</day>
<month>12</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="collection">
<year>2017</year>
</pub-date>
<volume>10</volume>
<elocation-id>394</elocation-id>
<history>
<date date-type="received">
<day>07</day>
<month>07</month>
<year>2017</year>
</date>
<date date-type="accepted">
<day>10</day>
<month>11</month>
<year>2017</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2017 Shi, Chang, Yu, Ko and Ko.</copyright-statement>
<copyright-year>2017</copyright-year>
<copyright-holder>Shi, Chang, Yu, Ko and Ko</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>L-type voltage-gated calcium channels (LTCCs) regulate tonic neurotransmitter release from sensory neurons including retinal photoreceptors. There are three types of LTCCs (Ca<sub>v</sub>1.2, Ca<sub>v</sub>1.3, and Ca<sub>v</sub>1.4) expressed in the retina. While Ca<sub>v</sub>1.2 is expressed in all retinal cells including the M&#x000FC;ller glia and neurons, Ca<sub>v</sub>1.3 and Ca<sub>v</sub>1.4 are expressed in the retinal neurons with Ca<sub>v</sub>1.4 exclusively expressed in the photoreceptor synaptic terminals. Mutations in the gene encoding Ca<sub>v</sub>1.4 cause incomplete X-linked congenital stationary night blindness in humans. Even though Ca<sub>v</sub>1.3 is present in the photoreceptor inner segments and the synaptic terminals in various vertebrate species, its role in vision is unclear, since genetic alterations in Ca<sub>v</sub>1.3 are not associated with severe vision impairment in humans or in Ca<sub>v</sub>1.3-null (Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup>) mice. However, a failure to regulate Ca<sub>v</sub>1.3 was found in a mouse model of Usher syndrome, the most common cause of combined deafness and blindness in humans, indicating that Ca<sub>v</sub>1.3 may contribute to retinal function. In this report, we combined physiological and morphological data to demonstrate the role of Ca<sub>v</sub>1.3 in retinal physiology and function that has been undervalued thus far. Through <italic>ex vivo</italic> and <italic>in vivo</italic> electroretinogram (ERG) recordings and immunohistochemical staining, we found that Ca<sub>v</sub>1.3 plays a role in retinal light responses and synaptic plasticity. Pharmacological inhibition of Ca<sub>v</sub>1.3 decreased <italic>ex vivo</italic> ERG a- and b-wave amplitudes. In Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice, their dark-adapted ERG a-, b-wave, and oscillatory potential amplitudes were significantly dampened, and implicit times were delayed compared to the wild type (WT). Furthermore, the density of ribbon synapses was reduced in the outer plexiform layer of Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice retinas. Hence, Ca<sub>v</sub>1.3 plays a more prominent role in retinal physiology and function than previously reported.</p></abstract>
<kwd-group>
<kwd>L-type voltage-gated calcium channel</kwd>
<kwd>photoreceptor</kwd>
<kwd>ribbon synapses</kwd>
<kwd>electroretinogram</kwd>
</kwd-group>
<contract-num rid="cn001">NIHR21EY023339</contract-num>
<contract-sponsor id="cn001">National Institutes of Health<named-content content-type="fundref-id">10.13039/100000002</named-content></contract-sponsor>
<counts>
<fig-count count="6"/>
<table-count count="3"/>
<equation-count count="0"/>
<ref-count count="85"/>
<page-count count="17"/>
<word-count count="12223"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>Introduction</title>
<p>L-type voltage-gated calcium channels (LTCCs) are multi-subunit channel complexes composed of a pore-forming &#x003B1;1 subunit and auxiliary &#x003B2; and &#x003B1;2&#x003B4; subunits. In the retina and inner ear, LTCCs mediate tonic neurotransmitter release from the ribbon synapses (Barnes and Kelly, <xref ref-type="bibr" rid="B2">2002</xref>; Catterall et al., <xref ref-type="bibr" rid="B12">2005</xref>; Dolphin, <xref ref-type="bibr" rid="B16">2006</xref>). In cochlea hair cells, calcium influx through LTCCs triggers glutamate release from the inner hair cells onto the spiral ganglion neurons and participates in the fine-tuning of frequency detection of sound (Sheets et al., <xref ref-type="bibr" rid="B67">2012</xref>; Joiner and Lee, <xref ref-type="bibr" rid="B25">2015</xref>). In the retina, photoreceptors and bipolar cells release glutamate continuously in the dark as a result of depolarization-evoked activation of LTCCs (Barnes and Kelly, <xref ref-type="bibr" rid="B2">2002</xref>). In addition to neurotransmitter release, LTCCs are involved in the regulation of membrane excitability, resonance properties, endocytosis, and synaptic plasticity at reciprocal synapses in the photoreceptors, bipolar cells, and amacrine cells (Palmer et al., <xref ref-type="bibr" rid="B52">2003a</xref>,<xref ref-type="bibr" rid="B53">b</xref>; Hull and von Gersdorff, <xref ref-type="bibr" rid="B24">2004</xref>; Vigh et al., <xref ref-type="bibr" rid="B75">2005</xref>; Hull et al., <xref ref-type="bibr" rid="B22">2006a</xref>). Thus, LTCCs may participate in multiple functions in the retina. There are three types of LTCC&#x003B1;1 subunits, Ca<sub>v</sub>1.2, Ca<sub>v</sub>1.3, and Ca<sub>v</sub>1.4, present in the retina (Morgans, <xref ref-type="bibr" rid="B49">2001</xref>; Barnes and Kelly, <xref ref-type="bibr" rid="B2">2002</xref>; Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>; Lee et al., <xref ref-type="bibr" rid="B38">2015</xref>). Among them, Ca<sub>v</sub>1.4 is strongly expressed at the ribbon synapses (Morgans, <xref ref-type="bibr" rid="B49">2001</xref>; Lee et al., <xref ref-type="bibr" rid="B38">2015</xref>), and its function is the most well-characterized in the retina, since mutations in Ca<sub>v</sub>1.4 cause X-linked incomplete congenital stationary night blindness type 2 (CSNB2) in humans (Bech-Hansen et al., <xref ref-type="bibr" rid="B4">1998</xref>; Liu et al., <xref ref-type="bibr" rid="B41">2013</xref>). This is due to the essential role of Ca<sub>v</sub>1.4 in the formation of ribbon synapses between photoreceptor terminals and the second-order neurons during development (Liu et al., <xref ref-type="bibr" rid="B41">2013</xref>). However, there are small residual inner retinal light responses recorded from CSNB2 patients (Miyake et al., <xref ref-type="bibr" rid="B47">1986</xref>; Bradshaw et al., <xref ref-type="bibr" rid="B7">2004</xref>) suggesting that there might be other LTCC&#x003B1;1 subunits present at the photoreceptor synaptic terminals to transmit light information to the inner retina.</p>
<p>Compared to Ca<sub>v</sub>1.4, the functional roles of Ca<sub>v</sub>1.2 and Ca<sub>v</sub>1.3 are less known in the retina. While Cav1.2 is expressed in all retinal cells including the M&#x000FC;ller glia, Cav1.3 is expressed only in the retinal neurons (Xu et al., <xref ref-type="bibr" rid="B84">2002</xref>; Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>). Mutations of Ca<sub>v</sub>1.2 or Ca<sub>v</sub>1.3 cause severe cardiovascular dysfunctions in humans and animals (Seisenberger et al., <xref ref-type="bibr" rid="B66">2000</xref>; Splawski et al., <xref ref-type="bibr" rid="B70">2004</xref>; Striessnig et al., <xref ref-type="bibr" rid="B72">2014</xref>; Pinggera et al., <xref ref-type="bibr" rid="B56">2015</xref>; Pinggera and Striessnig, <xref ref-type="bibr" rid="B57">2016</xref>), and dysregulation of Ca<sub>v</sub>1.3 severely impairs hearing (Platzer et al., <xref ref-type="bibr" rid="B59">2000</xref>; Seisenberger et al., <xref ref-type="bibr" rid="B66">2000</xref>). In Ca<sub>v</sub>1.3-null mutant (Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup>) mice, the retina displays mild morphological changes in the outer plexiform layer (OPL) where photoreceptors and secondary neurons form synaptic contacts (Busquet et al., <xref ref-type="bibr" rid="B8">2010</xref>). Even though there is no specific report on vision loss in humans or animals with Ca<sub>v</sub>1.3 mutations, a failure to regulate Ca<sub>v</sub>1.3 is found in a mouse model of Usher syndrome, the most common cause of combined deafness and blindness in humans (Petit, <xref ref-type="bibr" rid="B55">2001</xref>; Kersten et al., <xref ref-type="bibr" rid="B26">2010</xref>; Joiner and Lee, <xref ref-type="bibr" rid="B25">2015</xref>), indicating that Ca<sub>v</sub>1.3 may contribute to retinal function and physiology that requires further investigation.</p>
<p>One potential function of Ca<sub>v</sub>1.3 in the retina may be in adaptive processes to external stimulation. In cultured retinal amacrine and ganglion cells, activation of glutamate receptors causes a rapid internalization of Ca<sub>v</sub>1.3 but not Ca<sub>v</sub>1.2 (Mizuno et al., <xref ref-type="bibr" rid="B48">2010</xref>) suggesting that Ca<sub>v</sub>1.3 is more &#x0201C;plastic&#x0201D; and responsive to potential light/dark stimulations. The plasticity of Ca<sub>v</sub>1.3 may serve as an acute adaptation to protect the inner retinal circuitry against glutamate excitotoxicity (Mizuno et al., <xref ref-type="bibr" rid="B48">2010</xref>). The mRNA and protein expressions of Ca<sub>v</sub>1.3 are rhythmic in circadian oscillations, in which there are more Ca<sub>v</sub>1.3 subunits inserted in the plasma membrane with larger Ca<sub>v</sub>1.3-currents recorded at night than during the day in the avian retina (Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>; Ko M. L. et al., <xref ref-type="bibr" rid="B31">2009</xref>). This indicates that Ca<sub>v</sub>1.3 may participate in fine-tuning the retinal light responses to anticipate the ambient light changes throughout the course of a day (Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>; Ko G. Y. et al., <xref ref-type="bibr" rid="B30">2009</xref>; Ko M. L. et al., <xref ref-type="bibr" rid="B31">2009</xref>). To further understand the role of Ca<sub>v</sub>1.3 in mammalian retinal physiology and function, we employed <italic>ex vivo</italic> and <italic>in vivo</italic> ERG studies to decipher the contribution of Ca<sub>v</sub>1.3 to retinal light responses. Using <italic>ex vivo</italic> ERG recordings, we were able to isolate the a-wave from the b-wave and carefully analyze the contribution of Ca<sub>v</sub>1.3 in the outer (a-wave) and inner (b-wave) retina. We further compared the retinal light responses from both outer and inner retina among the wild type (WT), Ca<sub>v</sub>1.3 heterozygous mutant (Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup>), and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice. Combined with our morphological observations, we provide new evidence on the contribution of Ca<sub>v</sub>1.3 to retinal light responses and synaptic transmission.</p>
</sec>
<sec sec-type="materials and methods" id="s2">
<title>Materials and methods</title>
<sec>
<title>Animals</title>
<p>Male C57BL/6J mice (WT) were purchased from Harlan (Houston, TX, USA) and used at 2&#x02013;3 months old in this study. The Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice (C57BL/6J background) were originally developed by Dr. J&#x000F6;rg Striessnig (University of Innsbruck, Innrain, Innsbruck, Austria; Platzer et al., <xref ref-type="bibr" rid="B59">2000</xref>). The Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> (heterozygous) breeding pair for generating Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> (homozygous knockout) was from Dr. Amy Lee (University of Iowa, Iowa City, IA, USA). The Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup>, Ca<sub>v</sub>1.3 <sup>&#x0002B;/&#x02212;</sup>, and Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x0002B;</sup> (WT) littermates used in this study were produced at Texas A&#x00026;M University (College Station, TX, USA). All animal experiments were approved by the Institutional Animal Care and Use Committee of Texas A&#x00026;M University. Mice were housed under temperature and humidity-controlled conditions with 12:12 h light-dark cycles.</p>
</sec>
<sec>
<title>HEK cell culture and transfection</title>
<p>The human HEK 293 cell line was purchased from American Type Culture Collection (ATCC, Manassas, VA, USA). The cells were maintained in DMEM (BioWhittaker, Walkersville, MD, USA) containing 10% FBS (HyClone, Pittsburgh, PA, USA), 50 u/ml penicillin/50 &#x003BC;g/ml streptomycin (Sigma-Aldrich, St. Louis, MO, USA), 1 mM sodium pyruvate (Life Technologies, Carlsbad, CA, USA), and 1x non-essential amino acids (Life Technologies) at 37&#x000B0;C under 5% CO<sub>2</sub>. Cells were cultured on coverslips and placed in a 24-well culture plate. Cells were seeded in each well to 70&#x02013;80% confluence 24 h prior to the transfection. Transfections were performed using Lipofectamine 2000 Transfection Reagent (Life Technologies) according to the manufacturer&#x00027;s protocol. The calcium channel &#x003B1;2&#x003B4;1 subunit (rat) expression vector was a gift from Dr. Terrance P. Snutch (University of British Columbia, Vancouver, Canada). The pCDNA-Ca<sub>v</sub>1.2 &#x003B1;1 subunit was originally generated by Dr. Diane Lipscombe (Brown University, Providence, Rhode Island, USA) and distributed through Addgene (Cambridge, MA, USA). The pCDNA-Ca<sub>v</sub>1.3 &#x003B1;1 subunit (mouse) was from Dr. Amy Lee. The pCMV-Sport-&#x003B2;2 subunit (mouse) was purchased from MGC cDNA clones collection (Dharmacon, GE, Lafayette, CO). Up to 500 ng DNA (150 ng for each plasmid) was transfected into the cultured HEK cells, and culture media was exchanged 12 h after transfection. Electrophysiological recordings were carried out 60 h after the transfection.</p>
</sec>
<sec>
<title>Patch-clamp electrophysiological recordings</title>
<p>The whole cell patch-clamp recordings for LTCCs were carried out as previously described (Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>; Shi et al., <xref ref-type="bibr" rid="B68">2009</xref>). The external solution was (in mM): 145 TEACl, 9 BaCl<sub>2</sub>, 0.5 MgCl<sub>2</sub>, 5.5 glucose, 0.1 NiCl<sub>2</sub>, and 5 HEPES, pH 7.4 adjusted with TEAOH. The pipette solution was (in mM): 125 Cs acetate, 20 CsCl, 3 MgCl<sub>2</sub>, 10 EGTA, and 5 HEPES, pH adjusted with CsOH. The holding potential for transfected HEK cells was set at &#x02212;65 mV. Currents were recorded at room temperature using an A-M Systems model 2400 patch-clamp amplifier (Sequim, WA, USA). Signals were low-pass filtered at 2 kHz and digitized at 5 kHz with Digidata 1550A interface and pCLAMP 10.5 software (Molecular Devices, Sunnyvale, CA, USA). The Ba<sup>2&#x0002B;</sup> current was recorded immediately after the whole-cell configuration was formed by gentle suction, and the ramp-voltage command (&#x02212;80 to &#x0002B;60 mV in 500 ms) was applied to elicit Ba<sup>2&#x0002B;</sup> currents. D-cis-diltiazem (diltiazem; Sigma-Aldrich) was first dissolved in water and further diluted in external recording solutions to the appropriate final concentrations as denoted in the results. The cells were first recorded in normal external solution for baseline currents, followed by perfusion with diltiazem (DIL), and the ramp-voltage command was elicited once per minute after perfusion with DIL. The controls were recorded following the same protocol but perfused with an external solution without DIL. The peak current amplitudes were normalized as the percentage (%) to the original baseline amplitude (set at 100%) for each cell recorded.</p>
</sec>
<sec>
<title><italic>Ex vivo</italic> electroretinogram (ERG) recordings</title>
<p>Mice were dark adapted for at least 3 h prior to the recordings. All experiments were performed under dim red light as previously described (Kolesnikov and Kefalov, <xref ref-type="bibr" rid="B35">2012</xref>). This <italic>ex vivo</italic> ERG recording technique and the configuration of the recording chamber were originally designed by Dr. Vladimir Kefalov (Washington University, St. Louis, MO, USA). Mouse retinas were dissected out in oxygen saturated dissection medium containing 1 mg/ml BSA and 13.6 mg/ml L-15 (Sigma-Aldrich) at 37&#x000B0;C. Retinas were transferred to an <italic>ex vivo</italic> ERG recording chamber (OcuScience, Henderson, NV, USA) and perfused with a buffer containing (in mM): 112 NaCl, 3.6 KCl, 2.4 MgCl<sub>2</sub>, 20 NaHCO<sub>3</sub>, 3 Na succinate, 0.02 EDTA, 10 Glucose, 10 HEPES (pH 7.4), 0.72 mg/ml L-15, 0.1% MEM vitamins, and MEM non-essential amino acids (Sigma-Aldrich) at 37&#x000B0;C. The electrode solution in the recording chamber contained (in mM): 140 NaCl, 2.4 MgCl<sub>2</sub>, 1.2 CaCl<sub>2</sub>, 3 HEPES (pH 7.4). In order to isolate the ERG a-wave and observe photoreceptor responses, the perfusion solution was supplemented with 2 mM L-glutamate and 10 &#x003BC;M DL-AP-4, and the electrode solution was supplemented with 2 mM L-glutamate and 10 mM BaCl<sub>2</sub> to block the higher order photo-responses (Kolesnikov and Kefalov, <xref ref-type="bibr" rid="B35">2012</xref>)<sub>.</sub> Nitrendipine (EMD Millipore, Billerica, MA) was first dissolved in dimethylsulfoxide (DMSO), and further diluted in the external recording solution to 10 &#x003BC;M as the final concentration. A portable ERG device (OcuScience) was used for <italic>ex vivo</italic> ERG recordings. The ERG measurements were carried out sequentially at light intensities of 0.1, 0.3, 1.0, and 3.0 cd&#x000B7;s/m<sup>2</sup>. Each ERG response was an average of 4 light flashes at a specific light intensity. A 1-min recovery period was allowed between different intensities. The amplitudes and implicit times of a- and b-waves were recorded and analyzed by using the ERGView 4.4 software (OcuScience). <italic>Ex vivo</italic> results were normalized to the original baseline amplitude prior to the perfusion with the calcium channel inhibitors (diltiazem or nitrendipine) and reported as a change in percentage from the original baseline amplitude.</p>
</sec>
<sec>
<title><italic>In vivo</italic> ERG recordings</title>
<p>Male mice at 3 months old were used for <italic>in vivo</italic> ERG recordings (performed as previously described; Chang et al., <xref ref-type="bibr" rid="B13">2015</xref>). Mice were dark-adapted for at least 8 h then anesthetized with an intraperitoneal injection of Avertin (0.5 mL/25 g-body weight of 2% 2,2,2-tribromoethanol, 1.25% <italic>tert</italic>-amyl alcohol; Fisher Scientific, Pittsburgh, PA, USA). Pupils were dilated using a single drop of a 1% tropicamide and 2.5% phenylephrine mixture for 5 min. Mice were placed on a heating pad to maintain body temperatures at 37&#x000B0;C. The ground electrode was placed on the tail and the reference electrode placed under the skin in the cheek below the eye. A drop of Goniovisc (Hub Pharmaceuticals, Rancho Cucamonga, CA, USA) was applied on the surface of the cornea to keep it moist, and the threaded recording electrode conjugated to a mini contact lens (Ocuscience) was placed on top of the cornea. A dim red light was used for all preparatory procedures but was turned off during the ERG recording. A portable ERG device was used for measurements of light responses from a series of light stimulations at 0.1, 0.3, 1, 3, 10, and 25 cd&#x000B7;s/m<sup>2</sup>. Low light intensities (0.1, 0.3, 1.0, and 3.0 cd&#x000B7;s/m<sup>2</sup>) were flashed four times at 10 s intervals and the traces were averaged for a final ERG measurement. High light intensities (10 and 25 cd&#x000B7;s/m<sup>2</sup>) only had one flash. A 1 min recovery period was programmed between each light intensity. Amplitudes and implicit times of a- and b-waves were recorded and analyzed, and the oscillatory potentials were band-pass filtered between 100 and 300 Hz using the ERGView 4.4 software. The a-wave implicit time was measured from the onset of the light stimulus to the most hyperpolarized point (trough) of the a-wave, while the b-wave implicit time was measured from the onset of the light stimulus to the highest peak of the b-wave.</p>
</sec>
<sec>
<title>Immunohistochemistry</title>
<p>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x0002B;</sup> (WT) littermate mice were first anesthetized with isoflurane followed by cervical dislocation. The eyes were excised and fixed in Zamboni fixative (American Matertech Scientific Inc, Lodi, CA, USA) then cryo-protected in a 30% sucrose-PBS solution. Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x0002B;</sup> eyes were embedded side by side in Tissue-Tek O.C.T. Compound (Sakura Finetek Inc, Torrance, CA, USA) and stored at &#x02212;80&#x000B0;C. The frozen eye sections (10 &#x003BC;m) were cut using a cryostat (Leica Biosystem, Buffalo Grove, IL, USA) and mounted on glass slides. The sections were washed with PBS and incubated with a blocking solution containing 10% goat serum for 2 h at room temperature, followed by incubation with the primary antibodies (anti-Ribeye&#x0002B;anti-Ca<sub>v</sub>1.4 or anti-Ca<sub>v</sub>1.3 alone) at 4&#x000B0;C overnight. Sections were then washed three times with PBS containing 0.1% Triton 100 (PBST), incubated with a secondary antibody at room temperature for 2 h in a dark chamber, washed with PBST, and covered with the ProLong Gold antifade reagents containing 4&#x02032;,6-diamidino-2-phenylindole (DAPI; Life Technologies) and a glass coverslip. The primary antibodies used were rabbit anti-Ca<sub>v</sub>1.3 (1:100; Chemicon/Millipore Sigma, St. Louis, MO, USA), mouse anti-ribeye (1:100; Millipore) and rabbit anti-Ca<sub>v</sub>1.4 (1:1000; a generous gift from Dr. Amy Lee, University of Iowa, Iowa City, IA). The secondary antibodies used were Alexa fluor 488 goat anti-rabbit IgG (1:200; Life Technologies) and Cy5 goat anti-mouse IgG (1:200; Abcam, Cambridge, MA, USA). The images were captured with a Zeiss LSM 780 NLO Multiphoton Microscope (Carl Zeiss AG, Oberkochen, Germany). The images from WT or Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> were taken under the identical setting (light intensity, magnification, and capture time) for Ribeye or Ca<sub>v</sub>1.4.</p>
<p>Quantification of Ribeye positive and Ca<sub>v</sub>1.4 positive synaptic terminals: After images were captured, we used &#x0201C;Fiji,&#x0201D; an image processing package that is an open-source platform for biological image analysis (Schindelin et al., <xref ref-type="bibr" rid="B64">2012</xref>) to analyze our images. The &#x0201C;analyze particle&#x0201D; function in the Image J (software in &#x0201C;Fiji&#x0201D;) to quantify all fluorescent positive structures (as in pixels). Briefly, the threshold of individual fluorescent channel (red for Ribeye positive and green for Ca<sub>v</sub>1.4 positive) was automatically adjusted. The setting in the Image J software: particle size was from 0 to infinity, and circularity was from 0 to 1.0. We also used the &#x0201C;Coloc 2&#x0201D; (available at <ext-link ext-link-type="uri" xlink:href="https://imagej.net/Coloc_2">https://imagej.net/Coloc_2</ext-link>), a plugin utility to determine the colocalization of Ribeye and Ca<sub>v</sub>1.4. One stained retinal section was used per mouse. Three areas per retinal section were randomly selected. Channel 1 was assigned as red fluorescence (Ribeye positive), and channel 2 was assigned as green fluorescence (Ca<sub>v</sub>1.4 positive). The Li&#x00027;s Intensity Correlation Quotient (ICQ) value (Li et al., <xref ref-type="bibr" rid="B39">2004</xref>) was generated to determine the degree of Ribeye and Ca<sub>v</sub>1.4 colocalization: for colocalized staining 0 &#x0003C; ICQ &#x02264; 0.5; ICQ &#x0003D; &#x0007E;0 for random staining; for segregated staining 0 &#x0003E; ICQ &#x02265; &#x02212;0.5.</p>
</sec>
<sec>
<title>Western blotting</title>
<p>Samples were collected and prepared as described previously (Ko M. L. et al., <xref ref-type="bibr" rid="B31">2009</xref>; Huang et al., <xref ref-type="bibr" rid="B21">2013</xref>; Lin et al., <xref ref-type="bibr" rid="B40">2015</xref>). Retinas were homogenized in a Tris lysis solution (50 mM Tris, 1 mM EDTA, 150 mM NaCl, 1% NP-40) including phosphatase (50 mM NaF, 1 mM Na<sub>3</sub>VO<sub>4</sub>) and protease inhibitors (Sigma-Aldrich). After centrifugation to remove cellular debris, an equal volume of 2x Laemmli buffer was added to each sample lysate, then the samples were heated at 95&#x000B0;C for 5 min. Proteins were separated by SDS-PAGE (10% gels) for 1&#x02013;2 h. Proteins were then transferred to nitrocellulose membranes and probed by primary antibodies. The primary antibodies used were rabbit anti-Ca<sub>v</sub>1.3 antibody (1:1,000; Chemicon/ Millipore Sigma) and rabbit anti-actin antibody (1:1,000; Cell Signaling Technology, Danvers, MA, USA). Actin was used for loading controls. The secondary antibody (goat anti-rabbit) conjugated to horseradish peroxidase (1:1,000; Cell Signaling Technology) and the Femto and Pico electrochemiluminescense (ECL) kits (Pierce ThermoFisher Scientific, Waltham, MA, USA) were used to visualize the blots.</p>
</sec>
<sec>
<title>Statistical analyses</title>
<p>All data are presented as mean &#x000B1; SEM (standard error of mean). Based on this study, as well as previously published data by us and our unpublished results, the data for our patch-clamp electrophysiological recordings, <italic>in vivo</italic> ERG, <italic>ex vivo</italic> ERG, and morphological analyses were all in normal distribution. One-way analysis of variance (ANOVA) with Tukey <italic>post hoc</italic> tests were used for statistical analyses between the various treatment groups or between the WT, Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> (heterozygous mutant), and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> homozygous mutant groups. The Student&#x00027;s <italic>t</italic>-test was used to compare between WT and Ca<sub>v</sub>1.3 <sup>&#x02212;/&#x02212;</sup>. Throughout, <italic>p</italic> &#x0003C; 0.05 was regarded as significant.</p>
</sec>
</sec>
<sec sec-type="results" id="s3">
<title>Results</title>
<sec>
<title>Distinguishing Ca<sub>v</sub>1.2 currents from Ca<sub>v</sub>1.3 through pharmacological inhibition</title>
<p>We first determined which pharmacological inhibitor could effectively differentiate Ca<sub>v</sub>1.2 from Ca<sub>v</sub>1.3, since there is no commercially available inhibitor that will selectively block Ca<sub>v</sub>1.2 but not Ca<sub>v</sub>1.3 (Cooper et al., <xref ref-type="bibr" rid="B14">1987</xref>; Xu and Lipscombe, <xref ref-type="bibr" rid="B85">2001</xref>). Among the LTCC inhibitors, dihydropyridines, phenylalkylamines, and benzothiazepines have lower affinities for Ca<sub>v</sub>1.3 compared to Ca<sub>v</sub>1.2 (Cai et al., <xref ref-type="bibr" rid="B9">1997</xref>; Hockerman et al., <xref ref-type="bibr" rid="B20">2000</xref>; Schnee and Ricci, <xref ref-type="bibr" rid="B65">2003</xref>; Baumann et al., <xref ref-type="bibr" rid="B3">2004</xref>; Tarabova et al., <xref ref-type="bibr" rid="B74">2007</xref>; Bissig et al., <xref ref-type="bibr" rid="B6">2013</xref>; Berkowitz et al., <xref ref-type="bibr" rid="B5">2014</xref>). Particularly, the half maximal inhibitory concentration (IC50) of diltiazem (DIL) for Ca<sub>v</sub>1.3 is more than 10 times higher than Ca<sub>v</sub>1.2 (Cai et al., <xref ref-type="bibr" rid="B9">1997</xref>; Hockerman et al., <xref ref-type="bibr" rid="B20">2000</xref>; Schnee and Ricci, <xref ref-type="bibr" rid="B65">2003</xref>; Baumann et al., <xref ref-type="bibr" rid="B3">2004</xref>; Tarabova et al., <xref ref-type="bibr" rid="B74">2007</xref>; Bissig et al., <xref ref-type="bibr" rid="B6">2013</xref>; Berkowitz et al., <xref ref-type="bibr" rid="B5">2014</xref>), so we took advantage of using DIL at a lower concentration to inhibit Ca<sub>v</sub>1.2 with minimal effects on Ca<sub>v</sub>1.3. However, a caveat we faced was that the effectiveness of DIL on Ca<sub>v</sub>1.2 vs. Ca<sub>v</sub>1.3 was not compared in the same cell type or preparation in previous reports (Cai et al., <xref ref-type="bibr" rid="B9">1997</xref>; Hockerman et al., <xref ref-type="bibr" rid="B20">2000</xref>; Schnee and Ricci, <xref ref-type="bibr" rid="B65">2003</xref>; Baumann et al., <xref ref-type="bibr" rid="B3">2004</xref>; Tarabova et al., <xref ref-type="bibr" rid="B74">2007</xref>; Bissig et al., <xref ref-type="bibr" rid="B6">2013</xref>; Berkowitz et al., <xref ref-type="bibr" rid="B5">2014</xref>). Hence, we first set forth using HEK 293 cells transfected with Ca<sub>v</sub>1.2 or Ca<sub>v</sub>1.3 and recorded the LTCC currents to identify a concentration of DIL that would inhibit Ca<sub>v</sub>1.2 without affecting Ca<sub>v</sub>1.3.</p>
<p>The HEK 293 cells were co-transfected with Ca<sub>v</sub>1.2 or Ca<sub>v</sub>1.3 and &#x003B2;2&#x0002B;&#x003B1;2&#x003B4;1 auxiliary subunits. Ba<sup>2&#x0002B;</sup> currents were recorded in the absence or presence of DIL. After 5 min of perfusion, the control cells (extracellular solution added H<sub>2</sub>O, the vehicle) had a decrease of 20% from the baseline, which was due to the run-down of the current. After 5 min of perfusion with extracellular solution containing DIL (10, 100, or 400 &#x003BC;M), the current amplitudes all decreased to &#x0003C;50% of baseline (data not shown). Since perfusion for 2 min did not elicit any current run-down in the control cells, we chose to compare the inhibitory effects of DIL after 2 min of perfusion to avoid current run-down issues. Extracellular perfusion with 10 or 100 &#x003BC;M DIL for 2 min significantly decreased the Ca<sub>v</sub>1.2-LTCC currents by 27 and 30%, respectively, while perfusion of 400 &#x003BC;M DIL for 2 min further decreased Ca<sub>v</sub>1.2 currents by 71% (Figures <xref ref-type="fig" rid="F1">1A&#x02013;C</xref>; Control: 96 &#x000B1; 4%; DIL 10 &#x003BC;M: 73 &#x000B1; 6%; DIL 100 &#x003BC;M: 70 &#x000B1; 4%; DIL 400 &#x003BC;M: 29 &#x000B1; 4%). However, extracellular perfusion with 10 &#x003BC;M DIL did not inhibit Ca<sub>v</sub>1.3-LTCC currents, while perfusion with 400 &#x003BC;M DIL did (Figures <xref ref-type="fig" rid="F1">1D&#x02013;F</xref>; Control: 95 &#x000B1; 4%; DIL 10 &#x003BC;M: 98 &#x000B1; 5%; DIL 400 &#x003BC;M: 42 &#x000B1; 9%). This result indicates that Ca<sub>v</sub>1.2 is more sensitive to DIL inhibition compared to Ca<sub>v</sub>1.3 in transfected HEK cells, so treatments with 10 &#x003BC;M DIL could selectively dampen Ca<sub>v</sub>1.2 with minimal impact on Ca<sub>v</sub>1.3.</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Different concentrations of diltiazem (DIL) are able to differentiate Ca<sub>v</sub>1.2-LTCC from Ca<sub>v</sub>1.3-LTCC currents in cultured HEK cells. The LTCC currents were recorded from Ca<sub>v</sub>1.2-transfected HEK cells <bold>(A&#x02013;C)</bold> and Ca<sub>v</sub>1.3-transfected HEK cells <bold>(D&#x02013;F)</bold> under the whole-cell patch-clamp configuration. <bold>(A)</bold> Perfusion with DIL at 10, 100, or 400 &#x003BC;M significantly decreases Ca<sub>v</sub>1.2-LTCC currents recorded from HEK cells transfected with Ca<sub>v</sub>1.2. <bold>(B)</bold> Perfusion with 10, 100, or 400 &#x003BC;M DIL for 2 min causes a reduction of Ca<sub>v</sub>1.2-LTCC currents. <bold>(A,B)</bold> The asterisk (<sup>&#x0002A;</sup>) indicates a statistically significant difference between the control and the 10, 100, and 400 &#x003BC;M DIL groups; &#x0201C;&#x00026;&#x0201D; indicates that the 400 &#x003BC;M DIL group is statistically different from the other 3 groups; &#x0201C;n.s.&#x0201D; indicates that there is no statistical difference between the 10 and 100 &#x003BC;M DIL groups. <bold>(C)</bold> Representative traces recorded from the Ca<sub>v</sub>1.2-transfected HEK cells perfused with 0 (control), 10, 100, or 400 &#x003BC;M DIL are shown. <bold>(D)</bold> Diltiazem (DIL) at 400 &#x003BC;M, but not at 10 &#x003BC;M, causes a decrease in Ca<sub>v</sub>1.3-LTCC currents recorded from HEK cells transfected with Ca<sub>v</sub>1.3. <bold>(E)</bold> Perfusion with 400 &#x003BC;M DIL for 2 min causes a reduction of Ca<sub>v</sub>1.3-LTCC currents by more than 50%. <bold>(D,E)</bold> &#x0201C;&#x00026;&#x0201D; indicates that the 400 &#x003BC;M DIL group is statistically significant from the control and the 10 &#x003BC;M DIL group. <bold>(F)</bold> Representative traces recorded from the Ca<sub>v</sub>1.3-transfected HEK cells perfused with 0 (control), 10, or 400 &#x003BC;M DIL are shown. <sup>&#x0002A;, &#x00026;</sup><italic>p</italic> &#x0003C; 0.05.</p></caption>
<graphic xlink:href="fnmol-10-00394-g0001.tif"/>
</fig>
</sec>
<sec>
<title>Inhibition of LTCCs decreases retinal light sensitivities</title>
<p>The ERG has long been used to determine overall retinal light sensitivities (Newman and Odette, <xref ref-type="bibr" rid="B51">1984</xref>). The ERG a-wave reflects the photoreceptor responses to light stimulation, while the ERG b-wave represents the secondary light-evoked inner retinal responses, which reflects the summation from photoreceptor-bipolar cell synaptic transmission as well as responses from bipolar, amacrine, and M&#x000FC;ller cells (Newman and Odette, <xref ref-type="bibr" rid="B51">1984</xref>; Pinto et al., <xref ref-type="bibr" rid="B58">2007</xref>). We employed the <italic>ex vivo</italic> transretinal ERG technique originally developed by Dr. Vladimir J. Kefalov (Vinberg et al., <xref ref-type="bibr" rid="B78">2014</xref>), which allowed us to further dissect the contributions of LTCCs in retinal light responses from isolated mouse retinas. These <italic>ex vivo</italic> ERG recordings measure the light-induced voltage changes across the isolated retina from the photoreceptors to the ganglion cell layer (Vinberg et al., <xref ref-type="bibr" rid="B78">2014</xref>), and it significantly improves the signal-to-noise ratio compared to <italic>in vivo</italic> ERGs and allows for easy assessments of pharmacological treatments in the isolated retina through extracellular perfusion (Kolesnikov and Kefalov, <xref ref-type="bibr" rid="B35">2012</xref>; Vinberg et al., <xref ref-type="bibr" rid="B78">2014</xref>).</p>
<p>Both retinas were isolated from a dark-adapted mouse and placed in a dual-recording chamber. The <italic>ex vivo</italic> ERG responses elicited at various light intensity flashes were recorded before and after perfusion with LTCC blockers under dim red lighting. We first tested the inhibitory effect of DIL and found that perfusion with 10 &#x003BC;M DIL for 10 min reached its maximal inhibition of the ERG responses, since continuous perfusion at this concentration for 30 min, or perfusion with higher concentrations of DIL (20, 50, or 100 &#x003BC;M), did not further decrease the ERG amplitudes. After ERG responses were first recorded under normal perfusion buffer, 10 &#x003BC;M DIL was perfused for 10 min to inhibit Ca<sub>v</sub>1.2 followed by another round of ERG recordings. Subsequently, after perfusion with 10 &#x003BC;M nitrendipine (NIT) for another 10 min to further inhibit both Ca<sub>v</sub>1.2 and Ca<sub>v</sub>1.3, a third round of ERG responses were recorded. The representative <italic>ex vivo</italic> ERG waveforms are presented in Figures <xref ref-type="fig" rid="F2">2A&#x02013;D</xref>. We found that both DIL and NIT did not significantly affect the ERG a-wave responses (Figures <xref ref-type="fig" rid="F2">2E</xref>). Inhibition of LTCCs with DIL or NIT largely decreased the ERG b-wave responses (Figures <xref ref-type="fig" rid="F2">2F</xref>), indicating that Ca<sub>v</sub>1.2 and Ca<sub>v</sub>1.3 were involved in post-photoreceptor and inner retinal light responses.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Differential contributions of LTCCs to retinal light responses as measured by <italic>ex vivo</italic> ERGs. Mice were dark adapted for at least 3 h, and the retinas were excised and placed in an <italic>ex vivo</italic> ERG recording chamber. The ERG responses were recorded under 4 different light intensities: 0.1, 0.3, 1, and 3 cd&#x000B7;s/m<sup>2</sup>. The ERG recordings were performed with normal perfusion buffer (Control), followed by perfusion with 10 &#x003BC;M DIL to inhibit Ca<sub>v</sub>1.2, and subsequently perfused with 10 &#x003BC;M nitrendipine (NIT) to block both Ca<sub>v</sub>1.2 and Ca<sub>v</sub>1.3. <bold>(A&#x02013;D)</bold> Representative ERG waveforms recorded in different solutions (control, 10 &#x003BC;M DIL, and 10 &#x003BC;M NIT) are shown, which were recorded under light intensities of 0.1, 0.3, 1, and 3 cd&#x000B7;s/m<sup>2</sup>, respectively. <bold>(E)</bold> Perfusion with 10 &#x003BC;M DIL or 10 &#x003BC;M NIT for 10 min did not have significant effect on the ERG a-wave amplitudes. <bold>(F)</bold> Perfusion with 10 &#x003BC;M DIL or 10 &#x003BC;M NIT for 10 min decreased ERG b-wave amplitudes. The asterisk (<sup>&#x0002A;</sup>) indicates a statistically significant difference between the control and the 10 &#x003BC;M NIT group; &#x0201C;&#x00023;&#x0201D; indicates that the 10 &#x003BC;M DIL group is statistically different from the control. <sup>&#x0002A;, &#x00023;</sup><italic>p</italic> &#x0003C; 0.05.</p></caption>
<graphic xlink:href="fnmol-10-00394-g0002.tif"/>
</fig>
<p>While the ERG a-wave represents the photoreceptor light responses, under higher light intensity stimulations, the a-wave is often contaminated by the rising phase of the b-wave responses. Without pharmacological isolation of the a-wave, there was no specific effect elicited by NIT or DIL determined. In order to assess the role of LTCCs in photoreceptor light responses, we isolated the photoreceptor responses (ERG a-wave) with a perfusion solution containing 2 mM L-glutamate and 10 &#x003BC;M DL-AP-4 and an electrode solution containing 2 mM L-glutamate and 10 mM BaCl<sub>2</sub> to block the higher order retinal light responses (Kolesnikov and Kefalov, <xref ref-type="bibr" rid="B35">2012</xref>). After a-wave isolation, we found that both DIL (10 &#x003BC;M) and NIT (10 &#x003BC;M) were able to reduce the ERG a-wave amplitudes but NIT caused a larger decrease (Figures <xref ref-type="fig" rid="F3">3A&#x02013;D</xref>), indicating that both Ca<sub>v</sub>1.2 and Ca<sub>v</sub>1.3 were involved in photoreceptor light-evoked responses. In addition, at a lower light intensity stimulation (0.3 cd.s/m<sup>2</sup>), DIL did not significantly affect the ERG a-wave as it did at higher light intensity stimulations (1 and 3 cd.s/m<sup>2</sup>), but NIT significantly decreased the ERG a-wave at all three light intensity stimulations. This suggests that Ca<sub>v</sub>1.3 in photoreceptors might be more sensitive to changes in ambient light intensities, which echoes the notion that Ca<sub>v</sub>1.3 is &#x0201C;plastic&#x0201D; in responding to external stimulations. Since NIT and DIL were able to dampen isolated a-wave, this could partially explain the reduction of <italic>ex vivo</italic> ERG b-wave by NIT and DIL shown in Figure <xref ref-type="fig" rid="F2">2</xref>.</p>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Differential contributions of LTCCs in <italic>ex vivo</italic> ERG a-wave responses. Mice were dark adapted for at least 3 h, and the retinas were excised and placed in an <italic>ex vivo</italic> ERG recording chamber. The ERG a-wave (photoreceptor) responses were isolated with a perfusion solution containing 2 mM L-glutamate and 10 &#x003BC;M DL-AP-4 and an electrode solution containing 2 mM L-glutamate and 10 mM BaCl<sub>2</sub> to block the higher order of retinal photo-responses. The photoreceptor light responses were recorded under 3 different light intensities: 0.3, 1, and 3 cd&#x000B7;s/m<sup>2</sup>. The ERG recordings were first done with normal perfusion buffer (Control), followed by perfusion with 10 &#x003BC;M DIL, then perfusion with 10 &#x003BC;M NIT. <bold>(A&#x02013;C)</bold> Representative ERG a-waves recorded in different solutions (control, 10 &#x003BC;M DIL, and 10 &#x003BC;M NIT) are shown, under light intensities of 0.3, 1, and 3 cd&#x000B7;s/m<sup>2</sup>, respectively. <bold>(D)</bold> Perfusion with 10 &#x003BC;M DIL and 10 &#x003BC;M NIT for 10 min each decreased ERG a-wave amplitudes. The asterisk (<sup>&#x0002A;</sup>) indicates that the 10 &#x003BC;M DIL or 10 &#x003BC;M NIT group is significantly different from the control. <sup>&#x0002A;</sup><italic>p</italic> &#x0003C; 0.05.</p></caption>
<graphic xlink:href="fnmol-10-00394-g0003.tif"/>
</fig>
</sec>
<sec>
<title>Retinal light responses are decreased in both Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice</title>
<p>Since all Ca<sub>v</sub> (Ca<sub>v</sub>1.2, 1.3, and 1.4) channels are expressed in the retina, our pharmacological studies (Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F3">3</xref>) could not exclude the possibility that DIL and NIT might inhibit Ca<sub>v</sub>1.4. Thus, to further verify the role of Ca<sub>v</sub>1.3 in retinal light sensitivities, we recorded retinal light responses using <italic>in vivo</italic> ERG recordings from Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> homozygous null, Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> heterozygous, and wild type (WT) mice at 2.5 months old. Mice were dark adapted overnight for at least 8 h prior to ERG recordings with various light intensities at 0.1, 0.3, 1, 3, 10, and 25 cd&#x000B7;s/m<sup>2</sup> (Figure <xref ref-type="fig" rid="F4">4A</xref>). There were 3 Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x0002B;</sup> (WT) mice from the littermates and 5 WT mice purchased from the vendor. There was no statistical difference in the ERG amplitudes and implicit times recorded between these two WT groups, so we merged the data as a single WT group. But both Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice had significantly decreased ERG a-wave amplitudes (Figure <xref ref-type="fig" rid="F4">4B</xref>) and delayed implicit times (Figure <xref ref-type="fig" rid="F4">4C</xref>) compared to that of WT mice. Similarly, the ERG b-wave amplitudes were decreased (Figure <xref ref-type="fig" rid="F4">4D</xref>) and implicit times delayed (Figure <xref ref-type="fig" rid="F4">4E</xref>) in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to WT mice (Table <xref ref-type="table" rid="T1">1</xref>).</p>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Retinal light responses are decreased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mutant mice. The scotopic ERG amplitudes are decreased and implicit times delayed in both Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> (heterozygous mutant) and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> (homozygous mutant) mice compared to the wild type (WT) mice. All mice were dark adapted for at least 8 h. Retinal light responses were measured when mice were exposed to a series of light intensities from 0.1 to 25 cd&#x000B7;s/m<sup>2</sup>. <bold>(A)</bold> Representative ERG wave forms recorded from WT (left), Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> (middle), and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> (right) mouse eyes in response to each stimulating light intensity. The superimposed ERG traces from the WT (black), Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> (blue), and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> (red) mice elicited at 1 cd.s/m<sup>2</sup> light intensity are shown in the box. <bold>(B)</bold> The average ERG a-wave amplitudes are decreased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. <bold>(C)</bold> The average ERG a-wave implicit times are increased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. <bold>(D)</bold> The average ERG b-wave amplitudes are decreased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. <bold>(E)</bold> The average ERG b-wave implicit times are increased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. The asterisk (<sup>&#x0002A;</sup>) indicates a statistically significant difference between the WT and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice; &#x0201C;&#x00023;&#x0201D; indicates a statistically significant difference between the WT and Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> mice; &#x0201C;&#x00026;&#x0201D; indicates a statistically significant difference between the Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice. <sup>&#x0002A;, &#x00023;, &#x00026;</sup><italic>p</italic> &#x0003C; 0.05.</p></caption>
<graphic xlink:href="fnmol-10-00394-g0004.tif"/>
</fig>
<table-wrap position="float" id="T1">
<label>Table 1</label>
<caption><p>Dark-adapted retinal light responses (Data for Figures <xref ref-type="fig" rid="F4">4B&#x02013;E</xref>).</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Light intensity (cd&#x000B7;s/m<sup>2</sup>)</bold></th>
<th valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>a-wave amplitude (&#x003BC;V)</bold></th>
<th valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>a-wave implicit time (ms)</bold></th>
</tr>
<tr>
<th/>
<th valign="top" align="center"><bold>WT</bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></th>
<th valign="top" align="center"><bold>WT</bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">0.1</td>
<td valign="top" align="center">123.4 &#x000B1; 8.0</td>
<td valign="top" align="center">96.9 &#x000B1; 7.5</td>
<td valign="top" align="center">74.0 &#x000B1; 10.4<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
<td valign="top" align="center">22.3 &#x000B1; 0.4</td>
<td valign="top" align="center">26.0 &#x000B1; 1.1<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.037</td>
<td valign="top" align="center">26.8 &#x000B1; 1.5<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.020</td>
</tr>
<tr>
<td valign="top" align="left">0.3</td>
<td valign="top" align="center">184.4 &#x000B1; 15.0</td>
<td valign="top" align="center">137.5 &#x000B1; 8.8<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.01</td>
<td valign="top" align="center">96.8 &#x000B1; 8.1<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00002<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>P</italic> &#x0003D; 0.042</td>
<td valign="top" align="center">20.0 &#x000B1; 0.6</td>
<td valign="top" align="center">24.8 &#x000B1; 0.7<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.00008</td>
<td valign="top" align="center">24.3 &#x000B1; 1.1<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
</tr>
<tr>
<td valign="top" align="left">1</td>
<td valign="top" align="center">193.4 &#x000B1; 9.2</td>
<td valign="top" align="center">153.0 &#x000B1; 8.8<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.008</td>
<td valign="top" align="center">113.9 &#x000B1; 10.4<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000004,<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>P</italic> &#x0003D; 0.017</td>
<td valign="top" align="center">15.8 &#x000B1; 0.8</td>
<td valign="top" align="center">19.2 &#x000B1; 0.9<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>P</italic> &#x0003D; 0.040</td>
<td valign="top" align="center">19.4 &#x000B1; 1.4</td>
</tr>
<tr>
<td valign="top" align="left">3</td>
<td valign="top" align="center">243.4 &#x000B1; 14.8</td>
<td valign="top" align="center">187.7 &#x000B1; 9.9<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.006</td>
<td valign="top" align="center">134.9 &#x000B1; 13.1<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000002,<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>P</italic> &#x0003D; 0.015</td>
<td valign="top" align="center">10.6 &#x000B1; 0.3</td>
<td valign="top" align="center">13.6 &#x000B1; 0.8<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.011</td>
<td valign="top" align="center">13.4 &#x000B1; 0.9<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.036</td>
</tr>
<tr>
<td valign="top" align="left">10</td>
<td valign="top" align="center">278.7 &#x000B1; 16.2</td>
<td valign="top" align="center">224.3 &#x000B1; 11.7<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.016</td>
<td valign="top" align="center">157.2 &#x000B1; 13.7<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000002,<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.005</td>
<td valign="top" align="center">9.8 &#x000B1; 0.3</td>
<td valign="top" align="center">12.6 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">12.3 &#x000B1; 0.9<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.015</td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td valign="top" align="left">25</td>
<td valign="top" align="center">303.5 &#x000B1; 18.6</td>
<td valign="top" align="center">241.2 &#x000B1; 12.3<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.011</td>
<td valign="top" align="center">174.4 &#x000B1; 14.0<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000003,<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.01</td>
<td valign="top" align="center">8.4 &#x000B1; 0.3</td>
<td valign="top" align="center">10.4 &#x000B1; 0.4<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
<td valign="top" align="center">9.9 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.036</td>
</tr> <tr>
<td valign="top" align="left"><bold>Light intensity (cd&#x000B7;s/m<sup>2</sup>)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>b-wave amplitude (&#x003BC;V)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>b-wave implicit time (ms)</bold></td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td/>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
</tr> <tr>
<td valign="top" align="left">0.1</td>
<td valign="top" align="center">534.5 &#x000B1; 35.6</td>
<td valign="top" align="center">392.2 &#x000B1; 28.7<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.004</td>
<td valign="top" align="center">278.6 &#x000B1; 23.2<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000005,<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.035</td>
<td valign="top" align="center">34.4 &#x000B1; 0.6</td>
<td valign="top" align="center">43.8 &#x000B1; 2.2<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">43.7 &#x000B1; 2.6<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.007</td>
</tr>
<tr>
<td valign="top" align="left">0.3</td>
<td valign="top" align="center">665.6 &#x000B1; 38.6</td>
<td valign="top" align="center">453.6 &#x000B1; 31.2<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.00008</td>
<td valign="top" align="center">336.5 &#x000B1; 25.8<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0000001<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.049</td>
<td valign="top" align="center">32.5 &#x000B1; 0.6</td>
<td valign="top" align="center">40.2 &#x000B1; 1.8<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.004</td>
<td valign="top" align="center">39.7 &#x000B1; 2.1<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.015</td>
</tr>
<tr>
<td valign="top" align="left">1</td>
<td valign="top" align="center">671.3 &#x000B1; 36.9</td>
<td valign="top" align="center">488.0 &#x000B1; 30.9<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0005</td>
<td valign="top" align="center">353.7 &#x000B1; 28.4<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0000002,<break/> <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.019</td>
<td valign="top" align="center">31.1 &#x000B1; 0.6</td>
<td valign="top" align="center">37.1 &#x000B1; 1.1<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
<td valign="top" align="center">36.9 &#x000B1; 1.8<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.005</td>
</tr>
<tr>
<td valign="top" align="left">3</td>
<td valign="top" align="center">680.4 &#x000B1; 36.5</td>
<td valign="top" align="center">508.8 &#x000B1; 31.4<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">347.1 &#x000B1; 40.7<sup>&#x0002A;, &#x00026;</sup><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0000005, <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.008</td>
<td valign="top" align="center">30.1 &#x000B1; 0.5</td>
<td valign="top" align="center">35.5 &#x000B1; 1.0<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
<td valign="top" align="center">36.1 &#x000B1; 1.7<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
</tr>
<tr>
<td valign="top" align="left">10</td>
<td valign="top" align="center">833.0 &#x000B1; 45.4</td>
<td valign="top" align="center">616.1 &#x000B1; 35.9<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0007</td>
<td valign="top" align="center">440.5 &#x000B1; 35.5<sup>&#x0002A;, &#x00026;</sup><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0000001, <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.010</td>
<td valign="top" align="center">31.3 &#x000B1; 0.7</td>
<td valign="top" align="center">37.3 &#x000B1; 0.9<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
<td valign="top" align="center">36.8 &#x000B1; 1.3<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
</tr>
<tr>
<td valign="top" align="left">25</td>
<td valign="top" align="center">874.7 &#x000B1; 47.9</td>
<td valign="top" align="center">655.3 &#x000B1; 36.4<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
<td valign="top" align="center">470.8 &#x000B1; 39.9<sup>&#x0002A;, &#x00026;</sup><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0000002, <xref ref-type="table-fn" rid="TN3"><sup>&#x00026;</sup></xref><italic>p</italic> &#x0003D; 0.010</td>
<td valign="top" align="center">30.2 &#x000B1; 0.6</td>
<td valign="top" align="center">36.1 &#x000B1; 0.8<xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><break/> <xref ref-type="table-fn" rid="TN2"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.00004</td>
<td valign="top" align="center">35.9 &#x000B1; 1.2<xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><break/> <xref ref-type="table-fn" rid="TN1"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0004</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn id="TN1"><label>&#x0002A;</label><p><italic>Denotes Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> significantly different from WT</italic>.</p></fn>
<fn id="TN2"><label>&#x00023;</label><p><italic>Denotes Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> significantly different from WT</italic>.</p></fn>
<fn id="TN3"><label>&#x00026;</label><p><italic>Denotes Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> significantly different from Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></italic>.</p></fn>
<p><italic>Significance was determined when one-way ANOVA Tukey post hoc tests achieved <sup>&#x0002A;</sup>p &#x0003C; 0.05</italic>.</p>
</table-wrap-foot>
</table-wrap>
<p>We further analyzed the ERG oscillatory potentials (OP1-OP4), which largely represent the inner retinal responses especially from amacrine cells (Wachtmeister and Dowling, <xref ref-type="bibr" rid="B81">1978</xref>; Wachtmeister, <xref ref-type="bibr" rid="B80">1998</xref>; Pinto et al., <xref ref-type="bibr" rid="B58">2007</xref>). Both Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice had decreased OP1-4 amplitudes (Figures <xref ref-type="fig" rid="F5">5A,C,E,G</xref>) and delayed OP1-4 implicit times (Figures <xref ref-type="fig" rid="F5">5B,D,F,H</xref>) compared to WT mice (Table <xref ref-type="table" rid="T2">2</xref>). Hence, these <italic>in vivo</italic> ERG data clearly demonstrate that Ca<sub>v</sub>1.3 contributes to both outer and inner retinal light responses.</p>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>The inner retinal light responses are decreased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mutant mice. The oscillatory potential (OP) amplitudes are decreased and implicit times delayed in both Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the wild type (WT). The OPs were analyzed after the scotopic ERG responses were filtered between 100 and 300 Hz band-pass using the ERGView4.4 software (Ocuscience). <bold>(A,B)</bold> The average OP1 amplitudes <bold>(A)</bold> are decreased, but the implicit time <bold>(B)</bold> is increased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. <bold>(C,D)</bold> The average OP2 amplitudes <bold>(C)</bold> are decreased, but the implicit time <bold>(D)</bold> is increased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. <bold>(E,F)</bold> The average OP3 amplitudes <bold>(E)</bold> are decreased, but the implicit time <bold>(F)</bold> is increased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. <bold>(G,H)</bold> The average OP4 amplitudes <bold>(G)</bold> are decreased, but the implicit time <bold>(H)</bold> is increased in Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice compared to the WT. The asterisk (<sup>&#x0002A;</sup>) indicates a statistically significant difference between the WT and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice; &#x0201C;&#x00023;&#x0201D; indicates a statistically significant difference between the WT and Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> mice. <sup>&#x0002A;, &#x00023;</sup><italic>p</italic> &#x0003C; 0.05.</p></caption>
<graphic xlink:href="fnmol-10-00394-g0005.tif"/>
</fig>
<table-wrap position="float" id="T2">
<label>Table 2</label>
<caption><p>Oscillatory Potential Responses (Data for Figures <xref ref-type="fig" rid="F5">5A&#x02013;H</xref>).</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Light intensity (cd&#x000B7;s/m<sup>2</sup>)</bold></th>
<th valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP1 amplitude (&#x003BC;V)</bold></th>
<th valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP1 implicit time (ms)</bold></th>
</tr>
<tr>
<th/>
<th valign="top" align="center"><bold>WT</bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></th>
<th valign="top" align="center"><bold>WT</bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">0.1</td>
<td valign="top" align="center">29.7 &#x000B1; 1.7</td>
<td valign="top" align="center">24.8 &#x000B1; 2.4</td>
<td valign="top" align="center">16.0 &#x000B1; 1.7<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0002</td>
<td valign="top" align="center">19.9 &#x000B1; 0.3</td>
<td valign="top" align="center">23.9 &#x000B1; 0.6<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.004</td>
<td valign="top" align="center">25.0 &#x000B1; 1.4<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0005</td>
</tr>
<tr>
<td valign="top" align="left">0.3</td>
<td valign="top" align="center">31.3 &#x000B1; 1.9</td>
<td valign="top" align="center">27.1 &#x000B1; 2.4</td>
<td valign="top" align="center">25.5 &#x000B1; 4.3</td>
<td valign="top" align="center">18.0 &#x000B1; 0.4</td>
<td valign="top" align="center">21.7 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">23.3 &#x000B1; 1.3<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
</tr>
<tr>
<td valign="top" align="left">1</td>
<td valign="top" align="center">32.4 &#x000B1; 1.6</td>
<td valign="top" align="center">30.0 &#x000B1; 2.3</td>
<td valign="top" align="center">26.6 &#x000B1; 4.4</td>
<td valign="top" align="center">15.9 &#x000B1; 0.4</td>
<td valign="top" align="center">19.2 &#x000B1; 0.4<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">20.5 &#x000B1; 1.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
</tr>
<tr>
<td valign="top" align="left">3</td>
<td valign="top" align="center">47.7 &#x000B1; 2.5</td>
<td valign="top" align="center">31.7 &#x000B1; 3.0<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
<td valign="top" align="center">27.3 &#x000B1; 3.7<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0002</td>
<td valign="top" align="center">14.2 &#x000B1; 0.3</td>
<td valign="top" align="center">16.8 &#x000B1; 0.4<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.041</td>
<td valign="top" align="center">18.4 &#x000B1; 1.3<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.001,</td>
</tr>
<tr>
<td valign="top" align="left">10</td>
<td valign="top" align="center">71.1 &#x000B1; 5.8</td>
<td valign="top" align="center">42.6 &#x000B1; 4.2<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0003</td>
<td valign="top" align="center">35.7 &#x000B1; 4.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00003</td>
<td valign="top" align="center">16.6 &#x000B1; 0.4</td>
<td valign="top" align="center">19.8 &#x000B1; 0.4<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0003</td>
<td valign="top" align="center">20.0 &#x000B1; 0.8<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0003</td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td valign="top" align="left">25</td>
<td valign="top" align="center">84.7 &#x000B1; 7.0</td>
<td valign="top" align="center">43.2 &#x000B1; 4.1<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.000003</td>
<td valign="top" align="center">35.9 &#x000B1; 3.9<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0000005</td>
<td valign="top" align="center">15.5 &#x000B1; 0.4</td>
<td valign="top" align="center">18.8 &#x000B1; 0.4<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
<td valign="top" align="center">19.3 &#x000B1; 0.8<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00005</td>
</tr> <tr>
<td valign="top" align="left"><bold>Light intensity (cd&#x000B7;s/m<sup>2</sup>)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP2 amplitude (&#x003BC;V)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP2 implicit Time (ms)</bold></td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td/>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
</tr> <tr>
<td valign="top" align="left">0.1</td>
<td valign="top" align="center">174.1 &#x000B1; 18.3</td>
<td valign="top" align="center">102.7 &#x000B1; 9.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
<td valign="top" align="center">69.9 &#x000B1; 10.5<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00001</td>
<td valign="top" align="center">26.7 &#x000B1; 0.4</td>
<td valign="top" align="center">31.2 &#x000B1; 0.6<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.005</td>
<td valign="top" align="center">32.8 &#x000B1; 1.7<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0004</td>
</tr>
<tr>
<td valign="top" align="left">0.3</td>
<td valign="top" align="center">201.9 &#x000B1; 17.2</td>
<td valign="top" align="center">114.4 &#x000B1; 10.3<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.00006</td>
<td valign="top" align="center">84.4 &#x000B1; 11.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000001</td>
<td valign="top" align="center">24.9 &#x000B1; 0.4</td>
<td valign="top" align="center">28.9 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.005</td>
<td valign="top" align="center">30.9 &#x000B1; 1.5<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
</tr>
<tr>
<td valign="top" align="left">1</td>
<td valign="top" align="center">191.2 &#x000B1; 20.3</td>
<td valign="top" align="center">111.9 &#x000B1; 11.2<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.001</td>
<td valign="top" align="center">84.7 &#x000B1; 11.5<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000006</td>
<td valign="top" align="center">22.9 &#x000B1; 0.3</td>
<td valign="top" align="center">26.5 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">28.1 &#x000B1; 1.3<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00009</td>
</tr>
<tr>
<td valign="top" align="left">3</td>
<td valign="top" align="center">154.8 &#x000B1; 14.8</td>
<td valign="top" align="center">88.7 &#x000B1; 10.3<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0006</td>
<td valign="top" align="center">62.3 &#x000B1; 9.0<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00001</td>
<td valign="top" align="center">21.1 &#x000B1; 0.3</td>
<td valign="top" align="center">24.8 &#x000B1; 0.4<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.006</td>
<td valign="top" align="center">26.5 &#x000B1; 1.5<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0002</td>
</tr>
<tr>
<td valign="top" align="left">10</td>
<td valign="top" align="center">239.8 &#x000B1; 20.2</td>
<td valign="top" align="center">137.8 &#x000B1; 13.1<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.00006</td>
<td valign="top" align="center">96.5 &#x000B1; 10.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00005</td>
<td valign="top" align="center">23.7 &#x000B1; 0.5</td>
<td valign="top" align="center">27.4 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0006</td>
<td valign="top" align="center">28.1 &#x000B1; 1.0<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0002</td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td valign="top" align="left">25</td>
<td valign="top" align="center">249.5 &#x000B1; 20.1</td>
<td valign="top" align="center">148.5 &#x000B1; 14.1<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
<td valign="top" align="center">107.1 &#x000B1; 11.4<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000001</td>
<td valign="top" align="center">22.9 &#x000B1; 0.5</td>
<td valign="top" align="center">26.5 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0008</td>
<td valign="top" align="center">27.4 &#x000B1; 1.0<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
</tr> <tr>
<td valign="top" align="left"><bold>Light intensity (cd&#x000B7;s/m<sup>2</sup>)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP3 amplitude (&#x003BC;V)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP3 implicit Time (ms)</bold></td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td/>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
</tr> <tr>
<td valign="top" align="left">0.1</td>
<td valign="top" align="center">238.6 &#x000B1; 28.5</td>
<td valign="top" align="center">124.8 &#x000B1; 13.9<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0006</td>
<td valign="top" align="center">78.4 &#x000B1; 12.7<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000008</td>
<td valign="top" align="center">34.3 &#x000B1; 0.5</td>
<td valign="top" align="center">39.2 &#x000B1; 0.7<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.025</td>
<td valign="top" align="center">41.4 &#x000B1; 2.4<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
</tr>
<tr>
<td valign="top" align="left">0.3</td>
<td valign="top" align="center">272.4 &#x000B1; 29.5</td>
<td valign="top" align="center">137.9 &#x000B1; 13.8<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.00008</td>
<td valign="top" align="center">92.6 &#x000B1; 15.2<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000002</td>
<td valign="top" align="center">32.4 &#x000B1; 0.5</td>
<td valign="top" align="center">36.8 &#x000B1; 0.6<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.024</td>
<td valign="top" align="center">39.4 &#x000B1; 2.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0006</td>
</tr>
<tr>
<td valign="top" align="left">1</td>
<td valign="top" align="center">229.0 &#x000B1; 29.7</td>
<td valign="top" align="center">125.4 &#x000B1; 14.1<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
<td valign="top" align="center">88.8 &#x000B1; 14.8<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
<td valign="top" align="center">30.6 &#x000B1; 0.5</td>
<td valign="top" align="center">34.7 &#x000B1; 0.6<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.014</td>
<td valign="top" align="center">36.6 &#x000B1; 1.8<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0007</td>
</tr>
<tr>
<td valign="top" align="left">3</td>
<td valign="top" align="center">186.2 &#x000B1; 25.3</td>
<td valign="top" align="center">101.2 &#x000B1; 12.50<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">68.7 &#x000B1; 11.2<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
<td valign="top" align="center">29.6 &#x000B1; 0.5</td>
<td valign="top" align="center">33.3 &#x000B1; 0.8</td>
<td valign="top" align="center">35.1 &#x000B1; 1.9<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.005</td>
</tr>
<tr>
<td valign="top" align="left">10</td>
<td valign="top" align="center">334.6 &#x000B1; 36.2</td>
<td valign="top" align="center">160.4 &#x000B1; 17.9<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.00003</td>
<td valign="top" align="center">111.0 &#x000B1; 14.2<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000001</td>
<td valign="top" align="center">31.0 &#x000B1; 0.6</td>
<td valign="top" align="center">35.2 &#x000B1; 0.6<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.006</td>
<td valign="top" align="center">36.7 &#x000B1; 1.5<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0004</td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td valign="top" align="left">25</td>
<td valign="top" align="center">347.8 &#x000B1; 37.8</td>
<td valign="top" align="center">170.8 &#x000B1; 18.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0004</td>
<td valign="top" align="center">117.7 &#x000B1; 13.2<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.000001</td>
<td valign="top" align="center">30.1 &#x000B1; 0.6</td>
<td valign="top" align="center">34.2 &#x000B1; 0.5<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
<td valign="top" align="center">35.6 &#x000B1; 1.4<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0002</td>
</tr> <tr>
<td valign="top" align="left"><bold>Light intensity (cd&#x000B7;s/m<sup>2</sup>)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP4 amplitude (&#x003BC;V)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>OP4 implicit Time (ms)</bold></td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td/>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>WT</bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup></bold></td>
<td valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup></bold></td>
</tr> <tr>
<td valign="top" align="left">0.1</td>
<td valign="top" align="center">74.3 &#x000B1; 9.1</td>
<td valign="top" align="center">40.3 &#x000B1; 3.0<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0007</td>
<td valign="top" align="center">25.3 &#x000B1; 5.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00001</td>
<td valign="top" align="center">44.2 &#x000B1; 0.6</td>
<td valign="top" align="center">49.3 &#x000B1; 0.8</td>
<td valign="top" align="center">51.6 &#x000B1; 3.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.013</td>
</tr>
<tr>
<td valign="top" align="left">0.3</td>
<td valign="top" align="center">70.9 &#x000B1; 7.5</td>
<td valign="top" align="center">42.1 &#x000B1; 4.6<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.003</td>
<td valign="top" align="center">29.0 &#x000B1; 5.4<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00007</td>
<td valign="top" align="center">42.3 &#x000B1; 0.6</td>
<td valign="top" align="center">46.9 &#x000B1; 0.8</td>
<td valign="top" align="center">49.6 &#x000B1; 2.7<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.006</td>
</tr>
<tr>
<td valign="top" align="left">1</td>
<td valign="top" align="center">65.5 &#x000B1; 9.0</td>
<td valign="top" align="center">36.9 &#x000B1; 4.1<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.006</td>
<td valign="top" align="center">26.8 &#x000B1; 4.8<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0005</td>
<td valign="top" align="center">41.2 &#x000B1; 0.6</td>
<td valign="top" align="center">44.8 &#x000B1; 0.6</td>
<td valign="top" align="center">46.7 &#x000B1; 2.2<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.01</td>
</tr> <tr>
<td valign="top" align="left">3</td>
<td valign="top" align="center">67.5 &#x000B1; 8.3</td>
<td valign="top" align="center">34.1 &#x000B1; 4.4<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0005</td>
<td valign="top" align="center">24.3 &#x000B1; 4.3<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00004</td>
<td valign="top" align="center">40.1 &#x000B1; 0.6</td>
<td valign="top" align="center">44.0 &#x000B1; 0.7</td>
<td valign="top" align="center">46.7 &#x000B1; 2.1<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
</tr>
<tr>
<td valign="top" align="left">10</td>
<td valign="top" align="center">75.9 &#x000B1; 8.2</td>
<td valign="top" align="center">41.8 &#x000B1; 4.7<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0005</td>
<td valign="top" align="center">30.3 &#x000B1; 3.6<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.00002</td>
<td valign="top" align="center">41.7 &#x000B1; 0.7</td>
<td valign="top" align="center">45.9 &#x000B1; 0.7<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.025</td>
<td valign="top" align="center">47.0 &#x000B1; 1.9<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.008</td>
</tr>
<tr>
<td valign="top" align="left">25</td>
<td valign="top" align="center">84.8 &#x000B1; 9.4</td>
<td valign="top" align="center">44.9 &#x000B1; 4.9<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.0004</td>
<td valign="top" align="center">37.8 &#x000B1; 5.4<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.0001</td>
<td valign="top" align="center">40.5 &#x000B1; 0.7</td>
<td valign="top" align="center">44.7 &#x000B1; 0.7<xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><break/><xref ref-type="table-fn" rid="TN5"><sup>&#x00023;</sup></xref><italic>p</italic> &#x0003D; 0.015</td>
<td valign="top" align="center">46.0 &#x000B1; 1.8<xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><break/><xref ref-type="table-fn" rid="TN4"><sup>&#x0002A;</sup></xref><italic>p</italic> &#x0003D; 0.002</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn id="TN4"><label>&#x0002A;</label><p><italic>Denotes Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> significantly different from WT</italic>.</p></fn>
<fn id="TN5"><label>&#x00023;</label><p><italic>Denotes Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> significantly different from WT</italic>.</p></fn>
<p><italic>Significance was determined when one-way ANOVA Tukey post hoc tests achieved <sup>&#x0002A;</sup>p &#x0003C; 0.05</italic>.</p>
</table-wrap-foot>
</table-wrap>
</sec>
<sec>
<title>Deletion of Ca<sub>v</sub>1.3 &#x003B1;1 subunit affects the density of ribbon synapses in the retinal outer plexiform layer (OPL)</title>
<p>Our ERG results revealed that deletion of Ca<sub>v</sub>1.3 had an impact on the retinal light responses, mainly on the b-wave amplitude, suggesting that the light signal from the photoreceptors to the inner retina, as well as the light responses in the inner retinal neurons were dampened. The Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retina (&#x02212;/&#x02212;) had the least protein expression of Ca<sub>v</sub>1.3 compared to the WT or Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> (&#x0002B;/&#x02212;) retina as shown by Western blots (Figure <xref ref-type="fig" rid="F6">6A</xref>, right panel, arrow head). Hence, we carried out immunostaining to examine any potential morphological changes in the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retina.</p>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>Immunofluorescent changes of Ca<sub>v</sub>1.3, Ca<sub>v</sub>1.4, and Ribeye in Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mouse retinas. Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x0002B;</sup> (WT) and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retinal sections (10 &#x003BC;m) were stained for Ca<sub>v</sub>1.3, Ca<sub>v</sub>1.4, and Ribeye. <bold>(A)</bold> Representative images at a lower magnification (20 X) of WT (upper panel) and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> (lower panel) retinal sections. DAPI stains the cell nucleus. BF: bright field; ONL: outer nuclear layer; OPL: outer plexiform layer; INL: inner nuclear layer; IPL: inner plexiform layer. The scale bar &#x0003D; 50 &#x003BC;m. Right panel: The Western blots from Ca<sub>v</sub>1.3 transfected HEK cells (HEK&#x0002B;), Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x0002B;</sup> (WT) retina, Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> retina, and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retina show the protein band of Ca<sub>v</sub>1.3 at &#x0007E;250 kD. Actin serves as the loading controls. <bold>(B)</bold> Representative images at a higher magnification (40 X) of WT and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retinal sections stained for Ca<sub>v</sub>1.4 and Ribeye. The scale bar &#x0003D; 50 &#x003BC;m. <bold>(C)</bold> Fluorescent images focused on the OPL at a higher magnification (80 X) from WT and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retinal sections are shown. The scale bar &#x0003D; 5 &#x003BC;m. The images taken at this magnification were used for statistical analyses (Table <xref ref-type="table" rid="T3">3</xref>).</p></caption>
<graphic xlink:href="fnmol-10-00394-g0006.tif"/>
</fig>
<p>There was no noticeable morphological change of the overall retinal organization in the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retina compared to the WT (Figure <xref ref-type="fig" rid="F6">6A</xref>). In the WT retina, Ca<sub>v</sub>1.3 was present in the photoreceptor inner segment (IS), outer nuclear layer (ONL), OPL, inner nuclear layer (INL), inner plexiform layer (IPL), and the retinal ganglion cells (Figure <xref ref-type="fig" rid="F6">6A</xref>). Even though Ca<sub>v</sub>1.3 existed in the OPL, it was not exclusively co-localized with Ribeye at the ribbon synapses (Figure <xref ref-type="fig" rid="F6">6B</xref>), indicating that Ca<sub>v</sub>1.3 is present at the synaptic terminals but maybe not specifically at the ribbon structure. The Ca<sub>v</sub>1.3 fluorescence in the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retinal section could be the background staining.</p>
<p>Since one of the essential roles of LTCCs is governing the tonic release of neurotransmitters from photoreceptors, we focused on the OPL and detected two major proteins (Ribeye and Ca<sub>v</sub>1.4) that are present in the photoreceptor ribbon synapses. Ca<sub>v</sub>1.4 is largely expressed in the OPL, which contains the synaptic terminals of rod and cone photoreceptors (Figure <xref ref-type="fig" rid="F6">6A</xref>). Staining with Ribeye, ribbon synapses have a horseshoe-like shape in the OPL, and Ca<sub>v</sub>1.4 is mostly co-localized within the synaptic ribbons (Figure <xref ref-type="fig" rid="F6">6C</xref>), which is consistent with a previous report (Lee et al., <xref ref-type="bibr" rid="B38">2015</xref>). We quantified both Ribeye positive and Ca<sub>v</sub>1.4 positive staining at the OPL using &#x0201C;Fiji&#x0201D; with &#x0201C;Coloc 2&#x0201D; to analyze their colocalization. &#x0201C;Fiji&#x0201D; is an image processing package that is an open-source platform for biological image analysis (Schindelin et al., <xref ref-type="bibr" rid="B64">2012</xref>). The Li&#x00027;s Intensity Correlation Quotient (ICQ) value (Li et al., <xref ref-type="bibr" rid="B39">2004</xref>) was generated in this software package to determine the degree of Ribeye and Ca<sub>v</sub>1.4 colocalization: for colocalized/dependent staining 0 &#x0003C; ICQ &#x02264; &#x0002B;0.5; ICQ &#x0003D; &#x0007E;0 for random staining; for segregated staining 0 &#x0003E; ICQ &#x02265; &#x02212;0.5. In WT and Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mouse retinas, Ribeye and Ca<sub>v</sub>1.4 were highly colocalized, with Li&#x00027;s ICQ at &#x0007E;0.35 for both. With further quantification using Image J to analyze the Ribeye or Ca<sub>v</sub>1.4 positive structure, we found that WT retinas had significantly higher Ribeye positive and Ca<sub>v</sub>1.4 positive structures at the OPL compared to that in the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mouse retinas (Table <xref ref-type="table" rid="T3">3</xref>, Supplementary Figure <xref ref-type="supplementary-material" rid="SM1">1</xref>). Thus, deletion of Ca<sub>v</sub>1.3 had a negative impact on the photoreceptor ribbon synapses.</p>
<table-wrap position="float" id="T3">
<label>Table 3</label>
<caption><p>Analyses of synaptic structures at the OPL.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Fiji Coloc2 analysis</bold></th>
<th valign="top" align="center"><bold>WT (<italic>n</italic> &#x0003D; 5)</bold></th>
<th valign="top" align="center"><bold>Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> (<italic>n</italic> &#x0003D; 5)</bold></th>
<th valign="top" align="center"><bold><italic>t</italic>-test</bold></th>
</tr>
</thead>
<tbody>
<tr style="border-bottom: thin solid #000000;">
<td valign="top" align="left">Li&#x00027;s ICQ for colocalization of Ribeye and Ca<sub>v</sub>1.4</td>
<td valign="top" align="center">0.352 &#x000B1; 0.012</td>
<td valign="top" align="center">0.357 &#x000B1; 0.007</td>
<td valign="top" align="center"><italic>P</italic> &#x0003D; 0.70</td>
</tr> <tr style="border-bottom: thin solid #000000;">
<td valign="top" align="left" colspan="4"><bold>Image J analysis of fluorescent positive structures at the OPL</bold></td>
</tr> <tr>
<td valign="top" align="left">Ribeye positive (pixels)</td>
<td valign="top" align="center">5,579.8 &#x000B1; 522.60</td>
<td valign="top" align="center">4,011.6 &#x000B1; 278.98</td>
<td valign="top" align="center"><xref ref-type="table-fn" rid="TN6"><sup>&#x0002A;</sup></xref><italic>p &#x0003D; 0.029</italic></td>
</tr>
<tr>
<td valign="top" align="left">Ca<sub>v</sub>1.4 positive (pixels)</td>
<td valign="top" align="center">5,272.6 &#x000B1; 660.42</td>
<td valign="top" align="center">3,164.2 &#x000B1; 214.84</td>
<td valign="top" align="center"><xref ref-type="table-fn" rid="TN6"><sup>&#x0002A;</sup></xref><italic>p &#x0003D; 0.016</italic></td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<p><italic>Significance was determined when the Student&#x00027;s t-test achieved</italic></p>
<fn id="TN6"><label>&#x0002A;</label><p><italic>p &#x0003C; 0.05</italic>.</p></fn>
</table-wrap-foot>
</table-wrap>
</sec>
</sec>
<sec sec-type="discussion" id="s4">
<title>Discussion</title>
<p>In rod and cone photoreceptors, Ca<sub>v</sub>1.3 exists in the inner segments, cell bodies, and synaptic terminals (Firth et al., <xref ref-type="bibr" rid="B17">2001</xref>; Xu et al., <xref ref-type="bibr" rid="B84">2002</xref>; Morgans et al., <xref ref-type="bibr" rid="B50">2005</xref>; Hull et al., <xref ref-type="bibr" rid="B23">2006b</xref>; Cristofanilli et al., <xref ref-type="bibr" rid="B15">2007</xref>; Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>). Even though there is no report on obvious visual deficiencies in animals or humans with Ca<sub>v</sub>1.3 mutations, in a previous study (Busquet et al., <xref ref-type="bibr" rid="B8">2010</xref>), a failure to regulate Ca<sub>v</sub>1.3 is found in a mouse model of Usher syndrome, the most common cause of combined deafness and blindness in humans (Petit, <xref ref-type="bibr" rid="B55">2001</xref>; Joiner and Lee, <xref ref-type="bibr" rid="B25">2015</xref>). One Usher protein, USH2D (whirlin), is known to interact with Ca<sub>v</sub>1.3 in the retinal photoreceptors (Kersten et al., <xref ref-type="bibr" rid="B26">2010</xref>). Hence, Ca<sub>v</sub>1.3 may play a role in retinal light responses.</p>
<p>We first used pharmacological blockers to identify the role of Ca<sub>v</sub>1.3 in retinal physiology and function. In previously published reports, the effectiveness of DIL on Ca<sub>v</sub>1.2 vs. Ca<sub>v</sub>1.3 was not compared in the same cell type or preparation (Cai et al., <xref ref-type="bibr" rid="B9">1997</xref>; Hockerman et al., <xref ref-type="bibr" rid="B20">2000</xref>; Schnee and Ricci, <xref ref-type="bibr" rid="B65">2003</xref>; Baumann et al., <xref ref-type="bibr" rid="B3">2004</xref>; Tarabova et al., <xref ref-type="bibr" rid="B74">2007</xref>; Bissig et al., <xref ref-type="bibr" rid="B6">2013</xref>; Berkowitz et al., <xref ref-type="bibr" rid="B5">2014</xref>), so we set forth using HEK cells transfected with Ca<sub>v</sub>1.2 or Ca<sub>v</sub>1.3 and identified that DIL at 10 &#x003BC;M effectively inhibited Ca<sub>v</sub>1.2 but not Ca<sub>v</sub>1.3 (Figure <xref ref-type="fig" rid="F1">1</xref>). By applying 10 &#x003BC;M DIL or NIT in our <italic>ex vivo</italic> ERG studies, we found that both Ca<sub>v</sub>1.2 and Ca<sub>v</sub>1.3 contributed to retinal light responses (Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F3">3</xref>). Unfortunately, we could not completely distinguish the contribution of Ca<sub>v</sub>1.2 from Ca<sub>v</sub>1.3 in <italic>ex vivo</italic> retinal light responses, even though <italic>ex vivo</italic> ERG recordings have enhanced signal-to-noise ratios compared to <italic>in vivo</italic> ERGs and allow easy assessments of pharmacological treatments in the isolated retina (Kolesnikov and Kefalov, <xref ref-type="bibr" rid="B35">2012</xref>; Vinberg et al., <xref ref-type="bibr" rid="B78">2014</xref>). One possible explanation is that DIL and NIT might also affect Ca<sub>v</sub>1.4 in the retina. Thus, we next used a genetic strategy to verify the role of Ca<sub>v</sub>1.3 in retinal function.</p>
<p>We used Ca<sub>v</sub>1.3-null mice (Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup>) to further verify the role of Ca<sub>v</sub>1.3 in retinal light responses recorded by ERG. While the ERG a-wave reflects the photoreceptor light responses, the ERG b-wave represents the inner retinal light responses (Pinto et al., <xref ref-type="bibr" rid="B58">2007</xref>), including the light-evoked depolarization of ON bipolar cells (Stockton and Slaughter, <xref ref-type="bibr" rid="B71">1989</xref>) and amacrine cells, especially with the OP components of the b-wave reflecting the amacrine cell responses (Korol et al., <xref ref-type="bibr" rid="B36">1975</xref>; Palmowski-Wolfe et al., <xref ref-type="bibr" rid="B54">2006</xref>). Compared to the WT, the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice had significantly dampened retinal light responses in both ERG a- and b-waves, as well as the OPs (Figures <xref ref-type="fig" rid="F4">4</xref>, <xref ref-type="fig" rid="F5">5</xref> and Tables <xref ref-type="table" rid="T1">1</xref>, <xref ref-type="table" rid="T2">2</xref>). Interestingly, Ca<sub>v</sub>1.3 is expressed in the lobular appendages of AII amacrine cells (Habermann et al., <xref ref-type="bibr" rid="B19">2003</xref>), and Ca<sub>v</sub>1.3 is responsible for glycine release from the AII amacrine cells (Balakrishnan et al., <xref ref-type="bibr" rid="B1">2015</xref>). Thus, our ERG recordings from Ca<sub>v</sub>1.3 <sup>&#x02212;/&#x02212;</sup> mice with decreased OPs might reflect impaired crossover inhibition from amacrine cells (Menger et al., <xref ref-type="bibr" rid="B46">1998</xref>; Habermann et al., <xref ref-type="bibr" rid="B19">2003</xref>; Balakrishnan et al., <xref ref-type="bibr" rid="B1">2015</xref>).</p>
<p>An alternative explanation is that the decreased OPs and b-wave in Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice were caused by impaired neurotransmission from photoreceptors to bipolar cells. Since our immunostaining showed that in Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mouse retina, there was a significant decrease of Ca<sub>v</sub>1.4 positive ribbon synapses at the OPL. We previously showed that deletion of Ca<sub>v</sub>1.3 decreases the distribution of retinoschisin (RS1) in the retinal OPL (Shi et al., <xref ref-type="bibr" rid="B69">2017</xref>). Retinoschisin is an extracellular adhesion protein mainly secreted from photoreceptors and bipolar cells (Reid et al., <xref ref-type="bibr" rid="B60">1999</xref>, <xref ref-type="bibr" rid="B62">2003</xref>; Reid and Farber, <xref ref-type="bibr" rid="B61">2005</xref>). Mutations in the gene encoding RS1 cause X-linked juvenile retinoschisis that features disorganization of retinal cell layers, disruption of synaptic structures and neurotransmission between photoreceptors and bipolar cells, and progressive photoreceptor degeneration (Weber et al., <xref ref-type="bibr" rid="B82">2002</xref>), since RS1 is critical in stabilizing the synaptic connections during development (Takada et al., <xref ref-type="bibr" rid="B73">2004</xref>; Vijayasarathy et al., <xref ref-type="bibr" rid="B76">2006</xref>, <xref ref-type="bibr" rid="B77">2008</xref>). Retinoschisin interacts with both Ca<sub>v</sub>1.3 and Ca<sub>v</sub>1.4 (Shi et al., <xref ref-type="bibr" rid="B68">2009</xref>, <xref ref-type="bibr" rid="B69">2017</xref>). While LTCCs are critical for RS1 secretion, RS1 augments LTCCs (Ko et al., <xref ref-type="bibr" rid="B33">2008</xref>; Shi et al., <xref ref-type="bibr" rid="B68">2009</xref>, <xref ref-type="bibr" rid="B69">2017</xref>). Thus, the decreased density of synaptic ribbons in the OPL (Figure <xref ref-type="fig" rid="F6">6</xref>) as well as decreased ERG b-wave in Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice might be in part due to the decreased RS1.</p>
<p>In a previous report, with 7-min light pulses, the light peak (LP) of ERGs recorded from Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> is reduced compared to the WT littermates (Wu et al., <xref ref-type="bibr" rid="B83">2007</xref>). The LP of the ERG is caused by a depolarization of the basolateral plasma membrane of the retinal pigment epithelium (RPE). Since Ca<sub>v</sub>1.3 is also expressed in the RPE (Rosenthal et al., <xref ref-type="bibr" rid="B63">2006</xref>), the decreased LP observed in Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice further provides evidence that Ca<sub>v</sub>1.3 contributes to retinal light responses. However, contradicting previous reports that Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice only have mild decreases in ERG a- and b-waves compared to the WT littermates (Wu et al., <xref ref-type="bibr" rid="B83">2007</xref>; Busquet et al., <xref ref-type="bibr" rid="B8">2010</xref>), we found that the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice had significantly lower ERG a-, b-waves, and OPs compared to the WT littermates and the WT purchased from the vendor. One possible explanation is the recording procedure or instrumentation differences. But in their morphological study, the OPL of the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retina has more clusters of puncta or patches when labeled with the synaptic marker Ribeye, differing from the horseshoe-like appearance in the WT retina (Busquet et al., <xref ref-type="bibr" rid="B8">2010</xref>). This observation is similar to our immunostaining with the synaptic ribbon marker Ribeye and Ca<sub>v</sub>1.4 that the ribbon synapse density at the OPL of the Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mouse retina was decreased compared to the WT (Figure <xref ref-type="fig" rid="F6">6</xref>, Table <xref ref-type="table" rid="T3">3</xref>). Our morphological study showing decreased ribbon synapses in the OPL of Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retinas echoes the decreased ERG responses recorded from Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> mice. Hence, these results confirm the functional importance of Ca<sub>v</sub>1.3 in retinal physiology.</p>
<p>One major functional role of LTCCs is to govern the tonic neurotransmitter release from the ribbon synapses of photoreceptors and bipolar cells (von Gersdorff et al., <xref ref-type="bibr" rid="B79">1996</xref>; Barnes and Kelly, <xref ref-type="bibr" rid="B2">2002</xref>; Hull et al., <xref ref-type="bibr" rid="B23">2006b</xref>). Both Ca<sub>v</sub>1.3 and Ca<sub>v</sub>1.4 are expressed in the synaptic terminals of photoreceptors. While Ca<sub>v</sub>1.3 is present from the inner segments to synaptic terminals of photoreceptors (Firth et al., <xref ref-type="bibr" rid="B17">2001</xref>; Xu et al., <xref ref-type="bibr" rid="B84">2002</xref>; Morgans et al., <xref ref-type="bibr" rid="B50">2005</xref>; Hull et al., <xref ref-type="bibr" rid="B23">2006b</xref>; Cristofanilli et al., <xref ref-type="bibr" rid="B15">2007</xref>; Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>), Ca<sub>v</sub>1.4 is strongly expressed at the ribbon synapses (Morgans, <xref ref-type="bibr" rid="B49">2001</xref>; Morgans et al., <xref ref-type="bibr" rid="B50">2005</xref>; Liu et al., <xref ref-type="bibr" rid="B41">2013</xref>). Ca<sub>v</sub>1.4 clearly plays a pivotal role in the maintenance of structure and function of the ribbon synapses in the OPL during development, since its deletion causes ribbon synapses to stay in an immature state (Liu et al., <xref ref-type="bibr" rid="B41">2013</xref>). Two major biophysical characteristics of Ca<sub>v</sub>1.4 that differ from other LTCCs are the absence of calcium-dependent inactivation and the slow voltage-dependent inactivation, which make Ca<sub>v</sub>1.4 ideally suited for the tonic calcium influx at the photoreceptor synaptic terminal for neurotransmitter release in the dark (Koschak et al., <xref ref-type="bibr" rid="B37">2003</xref>; McRory et al., <xref ref-type="bibr" rid="B45">2004</xref>). Mutations of <italic>cacna1f</italic>, the gene encoding Ca<sub>v</sub>1.4, cause CSNB2 (Bech-Hansen et al., <xref ref-type="bibr" rid="B4">1998</xref>; Liu et al., <xref ref-type="bibr" rid="B41">2013</xref>). One would expect a total loss of ERG post-photoreceptor components from CSNB2 patients. However, these patients still have a small residual b-wave with slower kinetics (Bradshaw et al., <xref ref-type="bibr" rid="B7">2004</xref>), indicating that there could be other LTCCs present at the photoreceptor-bipolar cell synapses enabling the inner retina to still respond to light signals. Our results showed the density of photoreceptor ribbon synapses decreased in the OPL of Ca<sub>v</sub>1.3<sup>&#x02212;/&#x02212;</sup> retina, which supports the notion that Ca<sub>v</sub>1.3 also contributes to synaptic transmission in photoreceptors and other inner retinal neurons. In cochlea hair cells, Ca<sub>v</sub>1.3 is required for the maintenance of ribbon synapses, and calcium influx through Ca<sub>v</sub>1.3 fine tunes the size of synaptic ribbons during development (Sheets et al., <xref ref-type="bibr" rid="B67">2012</xref>; Joiner and Lee, <xref ref-type="bibr" rid="B25">2015</xref>). This phenomena has also been observed in pinealocyte synaptic ribbons (Sheets et al., <xref ref-type="bibr" rid="B67">2012</xref>) and might be present in other cell types. Our study sheds light that Ca<sub>v</sub>1.3 may also contribute to the maintenance of photoreceptor ribbon synapses.</p>
<p>Although there is evidence showing the presence of Ca<sub>v</sub>1.4 in bipolar cell synapses (Morgans, <xref ref-type="bibr" rid="B49">2001</xref>), we only detected Ca<sub>v</sub>1.4 in the OPL, not IPL, which is consistent with another study (Lee et al., <xref ref-type="bibr" rid="B38">2015</xref>). Our results suggest that Ca<sub>v</sub>1.3 along with Ca<sub>v</sub>1.2, but not Ca<sub>v</sub>1.4, are the major LTCCs in bipolar cells. Compared to Ca<sub>v</sub>1.2, Ca<sub>v</sub>1.3 activates at a more negative voltage and inactivates more slowly during depolarization. Ca<sub>v</sub>1.3 is less sensitive to dihydropyridine inhibition and calcium-induced inactivation than Ca<sub>v</sub>1.2 (Platzer et al., <xref ref-type="bibr" rid="B59">2000</xref>; Xu and Lipscombe, <xref ref-type="bibr" rid="B85">2001</xref>). These biophysical properties make Ca<sub>v</sub>1.3 more suitable to trigger neurotransmitter release in bipolar cells and sustain their depolarization. Therefore, deletion of Ca<sub>v</sub>1.3 dampens the neuro-signal relay in bipolar cells leading to decreased ERG b-waves.</p>
<p>Another aspect of Ca<sub>v</sub>1.3 function is its role in short-term retina adaptation to external stimulation. Activation of glutamate receptors causes a rapid internalization of Ca<sub>v</sub>1.3 in cultured amacrine and ganglion neurons (Mizuno et al., <xref ref-type="bibr" rid="B48">2010</xref>), suggesting that Ca<sub>v</sub>1.3 is highly responsive to changes in light stimulation, and such plasticity of Ca<sub>v</sub>1.3 may serve as an acute adaptation to protect the inner retinal circuitry against glutamate excitotoxicity (Mizuno et al., <xref ref-type="bibr" rid="B48">2010</xref>). Besides the short-term adaptation that the retina possesses in response to light or dark stimulation, the retina is able to undergo longer term adaptation that can last for hours to days, which includes regulation by the intrinsic retinal circadian oscillators (Green and Besharse, <xref ref-type="bibr" rid="B18">2004</xref>). Interestingly, the retinal light responses measured by ERG are under circadian control (Lu et al., <xref ref-type="bibr" rid="B42">1995</xref>; Manglapus et al., <xref ref-type="bibr" rid="B43">1998</xref>; McGoogan and Cassone, <xref ref-type="bibr" rid="B44">1999</xref>; Cameron et al., <xref ref-type="bibr" rid="B10">2008</xref>; Cameron and Lucas, <xref ref-type="bibr" rid="B11">2009</xref>). While the circadian rhythm of ERG a-waves can be explained by the circadian regulation of cGMP-gated cation channels (Ko et al., <xref ref-type="bibr" rid="B27">2001</xref>, <xref ref-type="bibr" rid="B28">2003</xref>, <xref ref-type="bibr" rid="B29">2004</xref>), the rhythmic changes in ERG b-waves have not yet been clearly defined, in which the circadian rhythm of Ca<sub>v</sub>1.3 (Ko et al., <xref ref-type="bibr" rid="B32">2007</xref>, <xref ref-type="bibr" rid="B34">2013</xref>; Ko M. L. et al., <xref ref-type="bibr" rid="B31">2009</xref>; Huang et al., <xref ref-type="bibr" rid="B21">2013</xref>; Lin et al., <xref ref-type="bibr" rid="B40">2015</xref>) might partially explain the circadian rhythmicity of ERG b-waves. In summary, combining the morphological and physiological data, Ca<sub>v</sub>1.3 contributes to synaptic transmission and inner retinal light responses. The role of Ca<sub>v</sub>1.3 in retinal physiology and function is more prominent than previously reported.</p>
</sec>
<sec id="s5">
<title>Author contributions</title>
<p>LS and GK designed the experiment. LS and JC, performed the experiment. LS, JC, FY, and GK analyzed the data. LS, MK, and GK wrote the manuscript. LS, JC, FY, MK, and GK edited the manuscript.</p>
<sec>
<title>Conflict of interest statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</sec>
</body>
<back>
<ack><p>We thank Dr. Amy Lee (University of Iowa, Iowa City, IA) for generous gifts of pCDNA-Ca<sub>v</sub>1.3 &#x003B1;1 subunit (mouse) and anti-Ca<sub>v</sub>1.4 antibody, and Ms. Jussara Fernandes Hagen in Dr. Amy Lee&#x00027;s laboratory for generating the Ca<sub>v</sub>1.3<sup>&#x0002B;/&#x02212;</sup> heterozygous breeding pair. We thank Dr. Terrance P. Snutch (University of British Columbia, Vancouver, Canada) for the calcium channel &#x003B1;2&#x003B4;1 subunit expression vector. We thank Mr. Andy Kim for technical assistance. We are very grateful for the fruitful comments and insights from Drs. Amy Lee, J&#x000F6;rg Striessnig, and Alexandra Koschak (University of Innsbruck, Innrain, Innsbruck, Austria). This work was supported in part by NIHR21EY023339 to GK.</p>
</ack>
<sec sec-type="supplementary-material" id="s6">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fnmol.2017.00394/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fnmol.2017.00394/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Image1.TIF" id="SM1" mimetype="image/tif" xmlns:xlink="http://www.w3.org/1999/xlink">
<label>Supplementary Figure 1</label>
<caption><p>Statistical analyses of synaptic structures at OPL (the Table <xref ref-type="table" rid="T3">3</xref> data plotted). Each datum point represents the average from a single mouse retina. <italic>N</italic> &#x0003D; 5 (mice) for each group. <sup>&#x0002A;</sup><italic>p</italic> &#x0003C; 0.05.</p></caption></supplementary-material>
</sec>
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