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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mar. Sci.</journal-id>
<journal-title>Frontiers in Marine Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mar. Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-7745</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fmars.2017.00365</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Marine Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Use of Open Source Hardware and Software Platforms to Quantify Spectrally Dependent Differences in Photochemical Efficiency and Functional Absorption Cross Section within the Dinoflagellate <italic>Symbiodinium</italic> spp.</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Hoadley</surname> <given-names>Kenneth D.</given-names></name>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<xref ref-type="author-notes" rid="fn003"><sup>&#x02020;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/318998/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Warner</surname> <given-names>Mark E.</given-names></name>
<uri xlink:href="http://loop.frontiersin.org/people/303609/overview"/>
</contrib>
</contrib-group>
<aff><institution>School of Marine Science and Policy, University of Delaware</institution>, <addr-line>Lewes, DE</addr-line>, <country>United States</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Thomas K. Frazer, University of Florida, United States</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Bojan Tamburic, University of Technology Sydney, Australia; Oscar Schofield, Rutgers University, The State University of New Jersey, United States</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Kenneth D. Hoadley <email>khoadley&#x00040;mbari.org</email></p></fn>
<fn fn-type="other" id="fn002"><p>This article was submitted to Coral Reef Research, a section of the journal Frontiers in Marine Science</p></fn>
<fn fn-type="present-address" id="fn003"><p>&#x02020;Present Address: Kenneth D. Hoadley, Monterey Bay Aquarium Research Institute. Moss Landing, CA, United States</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>17</day>
<month>11</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="collection">
<year>2017</year>
</pub-date>
<volume>4</volume>
<elocation-id>365</elocation-id>
<history>
<date date-type="received">
<day>18</day>
<month>05</month>
<year>2017</year>
</date>
<date date-type="accepted">
<day>30</day>
<month>10</month>
<year>2017</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2017 Hoadley and Warner.</copyright-statement>
<copyright-year>2017</copyright-year>
<copyright-holder>Hoadley and Warner</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>Active chlorophyll <italic>a</italic> fluorescence is an essential tool for understanding photosynthetic activity within cnidarian/dinoflagellate symbioses. Fluorescence measurement is typically achieved by utilizing a blue or red monochromatic excitation light source. However, algal photosynthetic pigments can differ in their absorption spectra, potentially leading to excitation wavelength dependent measurements of maximal and light acclimated PSII photosynthetic quantum yield (Fv/Fm or Fq&#x02032;/Fm&#x02032;) and functional absorption cross section (&#x003C3;<sub>PSII</sub> or &#x003C3;<sub>PSII&#x02032;</sub>). Here we utilized an open source hardware development platform to construct a multispectral excitation fluorometer to assess spectrally dependent differences in photochemistry within four different <italic>Symbiodinium</italic> species (two of each ITS2-type A4 and B1). Multivariate analysis of light acclimated photochemical signatures showed separation between most alga types. These spectrally dependent differences in light acclimated PSII efficiency and PSII functional absorption cross section likely reflect changes in light harvesting compounds, their connectivity to the PSII reaction centers and the balance between photochemical and non-photochemical fluorescence quenching. Additionally, acclimation to low (20 &#x003BC;mol photons m<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup>) and high (200 &#x003BC;mol photons m<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup>) light conditions was examined in two of these symbionts types (ITS-2 type A4 and B1) As expected, chlorophyll a cell<sup>&#x02212;1</sup> decreased under high light acclimation in both symbionts. However, only A4 saw a subsequent reduction in absorbance whereas cellular volume decreased in the B1 (<italic>S. minutum</italic>) symbiont. In response to high light acclimation, Fv/Fm was significantly lower at all excitation wavelengths for the B1 symbiont where as efficiencies remained the same for A4. However, high-light acclimated Fq&#x02032;/Fm&#x02032; levels decreased in both symbionts, but only when measured using the 615 or 625 nm excitation wavelengths. Non-photochemical quenching within the antennae bed was downregulated under high light acclimation in the A4 symbiont, but only when measured using the 505 and 530 nm excitation wavelengths. Such changes in Fq&#x02032;/Fm&#x02032; and antennae bed quenching highlight the benefits of spectrally resolved photochemical measurements. Additionally, the utilization of Arduino and Bitscope hardware exemplifies the potential of open source development platforms for construction of highly customizable instrumentation for photosynthetic research.</p>
</abstract>
<kwd-group>
<kwd>multispectral fluorometer</kwd>
<kwd>absorbance</kwd>
<kwd>light acclimation</kwd>
<kwd>open source</kwd>
<kwd>coral photobiology</kwd>
</kwd-group>
<contract-num rid="cn001">1316055</contract-num>
<contract-num rid="cn001">1258065</contract-num>
<contract-sponsor id="cn001">National Science Foundation<named-content content-type="fundref-id">10.13039/100000001</named-content></contract-sponsor>
<counts>
<fig-count count="6"/>
<table-count count="2"/>
<equation-count count="1"/>
<ref-count count="44"/>
<page-count count="12"/>
<word-count count="7694"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>Introduction</title>
<p>Dinoflagellates within the genus <italic>Symbiodinium</italic> can form unique symbioses with various marine invertebrate species, including jellyfish, sea anemones, giant clams, soft corals, and hard corals or scleractinians. These symbioses are pivotal for the ecological success of many of these organisms as they provide a major carbon source to their hosts via translocation of energy rich photosynthate (Muscatine et al., <xref ref-type="bibr" rid="B27">1984</xref>; Muscatine, <xref ref-type="bibr" rid="B26">1990</xref>). This genus contains a high degree of genetic diversity which is currently organized into nine broad clades (designated by the letters A&#x02013;I), some of which contain hundreds of distinct species (LaJeunesse, <xref ref-type="bibr" rid="B20">2001</xref>). Importantly, different <italic>Symbiodinium</italic>s can have significant influence on the host&#x00027;s response to changes in the environment (Baker, <xref ref-type="bibr" rid="B1">2003</xref>). For example, in corals, thermal tolerance is often associated with the specific symbiont type (Kemp et al., <xref ref-type="bibr" rid="B17">2006</xref>; LaJeunesse et al., <xref ref-type="bibr" rid="B21">2009</xref>; Silverstein et al., <xref ref-type="bibr" rid="B34">2011</xref>; Ortiz et al., <xref ref-type="bibr" rid="B30">2012</xref>). However, matching physiological characteristics with specific symbiont types can be difficult and time consuming. There is a real need within the coral reef community to match physiological variability with genetic variance across symbiont types to better understand what/how these symbioses will respond under future climate conditions.</p>
<p>Such phenotypic assessment (Phenomics) is gaining momentum within other photobiological fields where comprehension of genetic variability has far outpaced phenotypic descriptions (Furbank and Tester, <xref ref-type="bibr" rid="B5">2011</xref>). Phenotypic structure across different symbiont types grown in culture has been documented using photophysiological metrics as measured using active chlorophyll fluorometric measurements (Suggett et al., <xref ref-type="bibr" rid="B35">2015</xref>). However, environmental variables such as light intensity and the spectral characteristics inherent to the coral host in which the symbiont resides can also influence photobiological behavior (Iglesias-Prieto and Trench, <xref ref-type="bibr" rid="B16">1997b</xref>; Iglesias-Prieto et al., <xref ref-type="bibr" rid="B11">2004</xref>; Wangpraseurt et al., <xref ref-type="bibr" rid="B40">2012</xref>, <xref ref-type="bibr" rid="B41">2014</xref>). The potential for phenotypic variance within a single species also increases the difficulty of matching physiology with genotype in symbiodinium (Iglesias-Prieto and Trench, <xref ref-type="bibr" rid="B16">1997b</xref>; Iglesias-Prieto et al., <xref ref-type="bibr" rid="B11">2004</xref>).</p>
<p>The genus <italic>Symbiodinium</italic> contains a number of different photopigments, some involved with light harvesting, while others act as accessory pigments where they can either channel additional energy toward the photosynthetic reaction centers, or dissipate excess light energy (Iglesias-Prieto and Trench, <xref ref-type="bibr" rid="B14">1994</xref>, <xref ref-type="bibr" rid="B16">1997b</xref>). The light harvesting compounds; peridinin-chlorophyll-a-protein (PCP) and chl a-chl c(2)-peridinin-protein (acpPC) have been particularly well-studied and comprise the primary light harvesting units within <italic>Symbiodinium</italic> (Iglesias-Prieto et al., <xref ref-type="bibr" rid="B12">1991</xref>, <xref ref-type="bibr" rid="B13">1993</xref>; Niedzwiedzki et al., <xref ref-type="bibr" rid="B29">2013</xref>, <xref ref-type="bibr" rid="B28">2014</xref>). The relative abundance of these different photopigments can differ across symbiont types (Hennige et al., <xref ref-type="bibr" rid="B8">2009</xref>) and potentially offer another biological parameter that can be utilized to study species specific phenotypes within the genus <italic>Symbiodinium</italic>. As was demonstrated with symbionts housed within <italic>Porites</italic> and <italic>Montipora</italic>, host coral specimens found in Kaneohe Bay, absorbance based measurements can under certain circumstances provide some information on the abundance of photopigment concentrations (Hochberg et al., <xref ref-type="bibr" rid="B10">2006</xref>). However, additional instrumentation is needed to understand the active role of these pigments within the photosynthetic apparatus.</p>
<p>Single turnover (ST) active chlorophyll-<italic>a</italic> fluorometers utilize a short (&#x0003C;300 &#x003BC;s) saturation light pulse to induce charge separation and reduction of the primary electron acceptor Q<sub>a</sub> within the PSII reaction center (Kolber and Falkowski, <xref ref-type="bibr" rid="B18">1998</xref>). A major advantage of ST fluorometery is the additional measurement of the functional absorption cross section of PSII (&#x003C3;<sub>PSII</sub>) (Suggett et al., <xref ref-type="bibr" rid="B37">2003</xref>), which measures the proportion of light captured by light harvesting proteins attached to a reaction center and utilized by PSII. In these instruments, saturation/excitation lamps are typically centered at a 450&#x02013;500 nm wavelength to target peak absorbance of chlorophyll-<italic>a</italic>. However, by adjusting the excitation wavelength, it is possible to preferentially target other light harvesting photopigments. For example, by utilizing LEDs with peak emission centered at 447, 505 or 530 nm, we are able to preferentially excite at the peak absorption &#x0201C;soret&#x0201D; bands for the pigments Chl <italic>a/c</italic><sub>2</sub>, diadinoxanthin, and peridinin, respectively (Niedzwiedzki et al., <xref ref-type="bibr" rid="B29">2013</xref>, <xref ref-type="bibr" rid="B28">2014</xref>). Longer wavelengths such as 625 nm may transfer energy directly to the Chl <italic>a</italic> molecule (Niedzwiedzki et al., <xref ref-type="bibr" rid="B28">2014</xref>). Preferential excitation may provide further insight into how pigment orientation and connectivity to the PSII reaction center may differ across environmental conditions or across symbiont types. However, such systems come at a high cost and alternative systems could be highly beneficial toward improving our understanding of <italic>Symbiodinium</italic> photobiology.</p>
<p>Hardware and software platforms designed to help teach coding and programming languages to the next generation of engineers are becoming increasingly popular within the scientific community. These platforms offer sophisticated microcontrollers as a base with which to design customized instrumentation at a low cost. The high cost of commercially available research instrumentation can be heavily restrictive to many laboratories. Research questions/initiatives often must cater to the available instrumentation, thereby limiting the scope of possible questions or experimental options. Open-sourced hardware and software platforms have the potential to revolutionize how scientists conduct research by allowing for cheap purpose built instrumentation. Sophisticated instrumentation can be cheaply designed and built around a specific research question/topic. For example, the MultispeQ is an instrument developed to compare photophysiological parameters in plants across the world in an effort to tie in physiological differences with known genetic variance (Kuhlgert et al., <xref ref-type="bibr" rid="B19">2016</xref>). The OpenROV project (<ext-link ext-link-type="uri" xlink:href="http://www.openrov.com">www.openrov.com</ext-link>) represents another open-source platform which utilizes both the Arduino and Beaglebone hardware to construct a low cost remotely operated underwater vehicle which can be adapted with different instrumentation for both recreational and/or research purposes. These low-cost, yet highly sophisticated instruments represent an emerging trend in research that have great potential moving forward.</p>
<p>In this study, we utilize open source platforms to construct a low-cost multispectral ST fluorometer to characterize potential photo-physiological differences across four symbiont types from two clades (A and B) living within the anemone <italic>Exaptasia pallida</italic>. We further characterized the light acclimation process within two of these symbionts and describe a spectrally dependent response which differed across the <italic>Symbiodinium</italic> types. This study serves as an example of the potential for furthering scientific inquiry through customized, purpose built instruments via the open source concept and designed for specific research questions.</p>
</sec>
<sec sec-type="materials and methods" id="s2">
<title>Materials and methods</title>
<sec>
<title>Development of host and symbiont combinations</title>
<p>Symbiont strain identification was determined through partial amplification of the ITS2 nuclear ribosomal DNA region and a region of the chloroplast 23S rDNA as described in LaJeunesse and Trench (<xref ref-type="bibr" rid="B22">2000</xref>) and Zhang et al. (<xref ref-type="bibr" rid="B43">2000</xref>). The two strains of ITS-2 type A4 utilized within this study were collected from <italic>E. pallida</italic> anemones in a mangrove habitat in Key Largo, FL (Hawkins et al., <xref ref-type="bibr" rid="B7">2016</xref>). The A4-a strain represents a natural host and symbiont combination whereas the A4-b strain represents the genotype KLAp2 isolated from the anemone population and then utilized to re-infect aposymbiotic anemones originating from the same Key Largo mangrove habitat (as described in Hawkins et al., <xref ref-type="bibr" rid="B7">2016</xref>). Both the B1-a and B1-b strains represent separate <italic>S. minutum</italic> genotypes and are housed within <italic>E. pallida</italic> (clone CC7, donated by J. Pringle, Stanford University) (Sunagawa et al., <xref ref-type="bibr" rid="B38">2009</xref>). The B1-a strain represents a <italic>S. minutum</italic> variant that is naturally found within <italic>E. pallida</italic> and the B1-b strain was originally isolated from a Caribbean gorgonian (<italic>Plexaura kuna</italic>) (the BURR culture collection, donated by M.A. Coffroth, University of Buffalo). All host symbiont combinations were maintained in stable symbioses for at least 6 months prior to experimentation.</p>
<p>Each host/symbiont combination was maintained in small glass bowls (9 cm diameter, 130-mL volume) filled with artificial seawater (Instant Ocean) at a temperature of 26&#x000B0;C and salinity of 34 ppt. Lighting was maintained at 40 &#x003BC;mol photons m<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup> with a 14:10 h light dark cycle using cool white fluorescent bulbs. Anemones were fed <italic>Artemia nauplii</italic> twice per week and seawater in each bowl was changed every 3 days.</p>
</sec>
<sec>
<title>Experimental conditions</title>
<p>For comparisons of spectrally dependent quantum yield and functional absorption cross section measurements across symbiont types, four different host/symbiont combinations (A4-a, A4-b, B1-a, and B1-b) were maintained in separate glass bowls with 3&#x02013;4 anemones per bowl. Anemones were maintained at 20 &#x003BC;mol photons m<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup> on a 14:10 h light:dark cycle. For spectrally dependent characterization across low and high light acclimated cells, additional bowls for A4-a and B1-a were kept at 200 &#x003BC;mol photons m<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup> on a 14:10 h light:dark cycle. All bowls were cleaned and filled with fresh artificial seawater every 3 days and anemones were fed twice per week. Temperature was maintained at 26&#x000B0;C. Anemones were acclimated to their respective light conditions over a 2-week period prior to taking chlorophyll a fluorescence measurements and sampling anemones for chlorophyll a concentration, cell count, and cell volume measurements.</p>
</sec>
<sec>
<title>Chlorophyll a fluorescence measurements</title>
<sec>
<title>Construction of open-sourced fluorometer</title>
<p>The fluorometer prototype consists of combining several commercially available pieces of electronics. The Bitscope comes with a fully functional software program whereas the Arduino comes with its own code compiler. A schematic of the constructed fluorometer is provided in Figure <xref ref-type="fig" rid="F1">1</xref> and the components are listed in Table <xref ref-type="table" rid="T1">1</xref>. In brief, excitation was achieved using CREE XLamp XP-E2 LED. Three LEDs wired in series on a metal core printed circuit board (MCPCB) were utilized per excitation color (Channel). Specific LED colors (447, 505, 530, 597, 615, and 625 nm) were chosen due to their commercial availability and for their overlap with peak photopigment absorption values (Niedzwiedzki et al., <xref ref-type="bibr" rid="B29">2013</xref>, <xref ref-type="bibr" rid="B28">2014</xref>). Excitation of each Channel was controlled using logic MOSFET transistors connected to separate IO pins on an Arduino UNO microcontroller board. Power to the LEDs was supplied by a 12-volt AC-DC power converter (Mean-Well). A voltage regulator controlled power to each LED. However, due to performance differences across the LED colors, irradiance differed across wavelengths (447 nm &#x0003D; 34,172; 505 nm &#x0003D; 16,209; 530 nm &#x0003D; 18,401; 597 nm &#x0003D; 24,089; 615 nm &#x0003D; 35,983; 625 nm &#x0003D; 43,662 &#x003BC;mol photons m<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup>). Although similar irradiance across all excitation wavelengths is ideal, such differences should not affect the calculation of absorption cross section so long as light levels are not so low as to allow for reoxidation of the <inline-formula><mml:math id="M2"><mml:msubsup><mml:mrow><mml:mtext>Q</mml:mtext></mml:mrow><mml:mrow><mml:mtext>A</mml:mtext></mml:mrow><mml:mrow><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:math></inline-formula> site within the PSII reaction center (Kolber and Falkowski, <xref ref-type="bibr" rid="B18">1998</xref>). Excitation irradiance values were monitored throughout using an incident quantum sensor (LI-192, LiCor) to ensure stability throughout measurements. Fluorescence rise kinetics were detected with a PIN photodiode (Hammamatsu) connected to a LT122 operational amplifier (Linear Technology) along with a longband pass filter (Schott-RG695). The operational amplifier circuit came prefabricated as part of a Demonstration Circuit Board (1416; Linear Technology) and powered using a &#x000B1; 15 volt DC-DC (CUI) power supply. The resulting analog output from the PIN photodiode was recorded using a 10AU pocket analyzer (Bitscope). Control of each excitation channel, and the trigger to record data with the 10 AU pocket analyzer was achieved using the Arduino IDE. The Arduino control script is available on github (<ext-link ext-link-type="uri" xlink:href="https://github.com/khoadley/Fluorometer">https://github.com/khoadley/Fluorometer</ext-link>). Light emission and fluorescence detection were directed by glass fiber optic light guides (19.05-mm diameter) oriented at a 90-degree angle to each other.</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Schematic for the open source multispectral fluorometer. Names of Individual parts are listed in Table <xref ref-type="table" rid="T1">1</xref>. Black and red lines illustrate wire connections between hardware.</p></caption>
<graphic xlink:href="fmars-04-00365-g0001.tif"/>
</fig>
<table-wrap position="float" id="T1">
<label>Table 1</label>
<caption><p>Equipment list for fluorometer build.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Letter</bold></th>
<th valign="top" align="left"><bold>Hardware</bold></th>
<th valign="top" align="left"><bold>Company</bold></th>
<th valign="top" align="left"><bold>Description</bold></th>
<th valign="top" align="left"><bold>Approximate Price (USD)</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">A</td>
<td valign="top" align="left">Arduino UNO</td>
<td valign="top" align="left">Arduino</td>
<td valign="top" align="left">Microcontroller</td>
<td valign="top" align="left">$24.95</td>
</tr>
<tr>
<td valign="top" align="left">B</td>
<td valign="top" align="left">BitScope BS10</td>
<td valign="top" align="left">BitScope</td>
<td valign="top" align="left">Oscilloscope</td>
<td valign="top" align="left">$245.00</td>
</tr>
<tr>
<td valign="top" align="left">C</td>
<td valign="top" align="left">1416A</td>
<td valign="top" align="left">Linear Tech</td>
<td valign="top" align="left">Photodiode amplifier</td>
<td valign="top" align="left">$70</td>
</tr>
<tr>
<td valign="top" align="left">D</td>
<td valign="top" align="left">&#x000B1; 15 vdc power source</td>
<td valign="top" align="left">CUI</td>
<td valign="top" align="left">DC-DC power converter</td>
<td valign="top" align="left">$30</td>
</tr>
<tr>
<td valign="top" align="left">E</td>
<td valign="top" align="left">24 vdc power source</td>
<td valign="top" align="left">Mean-Well</td>
<td valign="top" align="left">AC-DC Converter</td>
<td valign="top" align="left">$35</td>
</tr>
<tr>
<td valign="top" align="left">F</td>
<td valign="top" align="left">Voltage Regulator</td>
<td valign="top" align="left">Drok</td>
<td valign="top" align="left">Voltage Regulator</td>
<td valign="top" align="left">$16.89</td>
</tr>
<tr>
<td valign="top" align="left">G</td>
<td valign="top" align="left">PDB-C109-ND</td>
<td valign="top" align="left">Digi-Key</td>
<td valign="top" align="left">PIN photodiode</td>
<td valign="top" align="left">$71.60</td>
</tr>
<tr>
<td valign="top" align="left">H</td>
<td valign="top" align="left">RG695</td>
<td valign="top" align="left">Schott</td>
<td valign="top" align="left">Long Bandpass filter</td>
<td valign="top" align="left">$40</td>
</tr>
<tr>
<td valign="top" align="left">I</td>
<td valign="top" align="left">IRL-520</td>
<td valign="top" align="left">Vishay</td>
<td valign="top" align="left">MOSFET</td>
<td valign="top" align="left">&#x0003C;$2.00 each</td>
</tr>
<tr>
<td valign="top" align="left">J</td>
<td valign="top" align="left">XP-E (Royal Blue)</td>
<td valign="top" align="left">Cree LED</td>
<td valign="top" align="left">447 nm Excitation</td>
<td valign="top" align="left">$15</td>
</tr>
<tr>
<td valign="top" align="left">K</td>
<td valign="top" align="left">Luxeon Rebel (Blue)</td>
<td valign="top" align="left">Luxeon LED</td>
<td valign="top" align="left">505 nm Excitation</td>
<td valign="top" align="left">$15</td>
</tr>
<tr>
<td valign="top" align="left">L</td>
<td valign="top" align="left">XP-E (Green)</td>
<td valign="top" align="left">Cree LED</td>
<td valign="top" align="left">530 nm Excitation</td>
<td valign="top" align="left">$15</td>
</tr>
<tr>
<td valign="top" align="left">M</td>
<td valign="top" align="left">XP-E (Amber)</td>
<td valign="top" align="left">Cree LED</td>
<td valign="top" align="left">597 nm Excitation</td>
<td valign="top" align="left">$15</td>
</tr>
<tr>
<td valign="top" align="left">N</td>
<td valign="top" align="left">XP-E (Red Orange)</td>
<td valign="top" align="left">Cree LED</td>
<td valign="top" align="left">615 nm Excitation</td>
<td valign="top" align="left">$15</td>
</tr>
<tr>
<td valign="top" align="left">O</td>
<td valign="top" align="left">XP-E (Red)</td>
<td valign="top" align="left">Cree LED</td>
<td valign="top" align="left">625 nm Excitation</td>
<td valign="top" align="left">$15</td>
</tr>
<tr>
<td valign="top" align="left">P</td>
<td/>
<td valign="top" align="left">Digikey</td>
<td valign="top" align="left">Resistor</td>
<td valign="top" align="left">&#x0003C;$1 each</td>
</tr>
<tr>
<td valign="top" align="left">Q</td>
<td valign="top" align="left">Aspheric Lens</td>
<td valign="top" align="left">Newport</td>
<td valign="top" align="left">Aspheric condenser</td>
<td valign="top" align="left">71</td>
</tr>
<tr style="border-top: thin solid #000000;">
<td/>
<td/>
<td/>
<td/>
<td valign="top" align="left">Total: $712.44</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<p><italic>Figure letters correspond to Figure <xref ref-type="fig" rid="F1">1</xref></italic>.</p>
</table-wrap-foot>
</table-wrap>
<p>Measurements were made 1 h after lights were turned off and consisted of six iterations of a 150 &#x003BC;s flash for each of the six excitation wavelengths. Light acclimated fluorescence measurements were then recorded following a 5-min exposure to a cool white actinic LED light source (CREE R5) at an intensity of 200 &#x003BC;mol photons m<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup>. Reference curves for each channel and light stage were recorded using a solid fluorescence standard (Walz). Fluorescence induction curves were processed in R with the non-linear curve (nlc) fitting package using equations adapted from Kolber and Falkowski (<xref ref-type="bibr" rid="B18">1998</xref>) by Dr. Matt Oliver (University of Delaware). Briefly, the data is fit to the equation:
<disp-formula id="E1"><mml:math id="M3"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:mrow><mml:mtext>F</mml:mtext><mml:mo>=</mml:mo><mml:msub><mml:mtext>F</mml:mtext><mml:mrow><mml:mn>0</mml:mn><mml:mtext>EST</mml:mtext></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msup><mml:mstyle><mml:mrow><mml:msub><mml:mtext>F</mml:mtext><mml:mrow><mml:mtext>vEST</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:mstyle><mml:mo>&#x02217;</mml:mo></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mo>&#x02212;</mml:mo><mml:mtext>exp</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mo>&#x02212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:msup><mml:mtext>C</mml:mtext><mml:mo>*</mml:mo></mml:msup><mml:mtext>x</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>/</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
Where F<sub>0EST</sub>, F<sub>vEST</sub>, and C are derived through iterative curve fitting. F<sub>0</sub> and F<sub>m</sub> are equal to F at the initial and final time point within the curve, respectively. The functional absorption cross section is determined by dividing C by the light irradiance measured from the corresponding excitation LED (R script is also available via Github: <ext-link ext-link-type="uri" xlink:href="https://github.com/khoadley/Fluorometer">https://github.com/khoadley/Fluorometer</ext-link>). The proportion of non-photochemical quenching which is occurring within the light harvesting pigments (non-photochemical quenching in the antennae bed) was calculated as 1-(&#x003C3;<sub>PSII</sub>&#x00027;/&#x003C3;<sub>PSII</sub>) where <inline-formula><mml:math id="M4"><mml:msubsup><mml:mrow><mml:mi>&#x003C3;</mml:mi></mml:mrow><mml:mrow><mml:mtext>PSII</mml:mtext></mml:mrow><mml:mrow><mml:mi>&#x02032;</mml:mi></mml:mrow></mml:msubsup></mml:math></inline-formula> and &#x003C3;<sub>PSII</sub> reflect the light and dark acclimated functional absorption cross section of PSII (Gorbunov et al., <xref ref-type="bibr" rid="B6">2001</xref>; Hennige et al., <xref ref-type="bibr" rid="B8">2009</xref>).</p>
</sec>
<sec>
<title>Commercially available instrument</title>
<p>On the final sampling interval, the maximum quantum yield of photosystem II (PSII, Fv/Fm) and the functional absorption cross section of PSII (&#x003C3;<sub>PSII</sub>) were also measured using a fluorescence induction and relaxation (FIRe) fluorometer (Satlantic Inc., Halifax) (<bold>Figure 6</bold>). Measurements were taken 1 h after the start of the dark period and consisted of five iterations of a 120 &#x003BC;s single turnover flash and analyzed by fitting each fluorescence transient curve using the <italic>FIREPRO</italic> software (Kolber and Falkowski, <xref ref-type="bibr" rid="B18">1998</xref>; Hennige et al., <xref ref-type="bibr" rid="B8">2009</xref>).</p>
</sec>
</sec>
<sec>
<title>Algal cell number, volume, and chlorophyll a concentration</title>
<p>Each anemone was ground in 1 mL of seawater using a 1.5 mL glass tenbroeck tissue grinder. A 200-&#x003BC;L sample of the resulting homogenate was removed and fixed with 10 &#x003BC;L 1% glutaraldehyde and used for algal cell counts and volume as described below. The remaining homogenate was centrifuged (5,000 &#x000D7; g) for 5 min to separate the host and symbiont portions. The supernatant was removed for calculating host protein concentration. The remaining algal cell pellet was utilized for calculating chlorophyll a concentration. Algal cell density and volume was assessed by replicate hemocytometer counts (<italic>n</italic> &#x0003D; 6) under 100x magnification. Samples were photographed using a Nikon microphot-FXA epifluorescent microscope and then analyzed by computer using Image J software (NIH) using methods similar to Suggett et al. (<xref ref-type="bibr" rid="B35">2015</xref>). For photopigment quantification, pelleted cells were lysed in 90% methanol with a bead beater (BioSpec) for 60 s, incubated at &#x02212;20&#x000B0;C for 2 h and then centrifuged for 5 min at 5,000 rpm to remove remaining debris. Chlorophyll <italic>a</italic> concentration was then calculated using established protocols (Porra et al., <xref ref-type="bibr" rid="B31">1989</xref>). Host protein concentrations were measured by the BCA method (Thermo Scientific), with bovine serum albumin used for standards. All absorbance measurements (chlorophyll and protein) were performed with a plate reader (FLUOstar Omega BMG labtech).</p>
</sec>
<sec>
<title>Spectral absorbance</title>
<p>For high and low light acclimated symbiont types, spectral absorbance measurements were performed as described in Enr&#x000ED;quez et al. (<xref ref-type="bibr" rid="B3">2005</xref>) with reflectance (<italic>R</italic>) measured using a spectrometer (USB2000 Ocean Optics) and absorbance (<italic>A</italic>) calculated as <italic>A</italic> &#x0003D; log[1/<italic>R</italic>]. Three traces were recorded per sample and a spectralon reflectance standard was utilized as a blank. Irradiance was provided by a full spectrum halogen light source (KL2500 LCD Schott). A running average was applied to each replicate trace prior to averaging. Significant differences among high and low light treatments were tested at absorbance wavelengths corresponding to those utilized by the chlorophyll <italic>a</italic> fluorometer (447, 505, 530, 597, 615, 625 nm).</p>
</sec>
<sec>
<title>Statistical analysis</title>
<p>Data-sets were tested for homogeneity of variance and normality of distribution using the Levene and Shapiro-Wilks tests, respectively. Data violating assumptions of normality and homoscedasticity (<italic>p</italic> &#x0003C; 0.05) were log transformed and retested. Significant differences in Fq&#x02032;/Fm&#x02032; and &#x003C3;<sub>PSII</sub>&#x02032; values across all four symbiont types were tested by a one-way ANOVA (Figures <xref ref-type="fig" rid="F2">2A,B</xref>), followed by pairwise comparison across all four symbiont types with Tukey <italic>post-hoc</italic> analyses. Significant separation across symbiont types was assessed using an ANalyses Of SIMilarities test (ANOSIM) with 9,999 permutations. A <italic>post-hoc</italic> analysis of separation was not performed due to low replicate numbers (<italic>n</italic> &#x0003D; 3). Photo-physiological differences across all four symbiont types were visualized using non-metric multidimensional scaling (nMDS) on Euclidean distances after log (x&#x0002B;1) transformation (Ziegler et al., <xref ref-type="bibr" rid="B44">2014</xref>). For high and low light acclimation comparisons, data were compared with a <italic>T</italic>-test with Bonferonni correction (Figures <xref ref-type="fig" rid="F3">3</xref>&#x02013;<bold>5</bold>). Data comparison between the FIRe and Open-Sourced fluorometer was performed by a two-way analysis of variance (ANOVA) between light and symbiont type (<bold>Figure 6</bold>). As the primarily focus was to assess the similarity of responses detected between fluorimeters, significant effects were not followed up with <italic>post-hoc</italic> analyses. All statistical analyses were performed using R software with the &#x0201C;vegan,&#x0201D; &#x0201C;car,&#x0201D; &#x0201C;edgeR,&#x0201D; &#x0201C;gplots,&#x0201D; and &#x0201C;pgirmess&#x0201D; packages installed.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Differences in fluorescence signature across symbiont types. <bold>(A)</bold> Effective quantum efficiency of PSII and <bold>(B)</bold> Light adapted absorption cross section (&#x003C3;<sub>PSII</sub>) for (dark blue) B1-a, (light blue) A4-a, (dark green) B1-b, and (light green) A4-b. Bars represent the mean and &#x000B1;SE for low light adapted samples. <bold>(C)</bold> Principle components analysis using light adapted &#x003C3;<sub>PSII</sub> and Fv&#x00027;/Fm&#x00027; for all four species. Ellipses represent a 95% confidence around the mean for each symbiont type.</p></caption>
<graphic xlink:href="fmars-04-00365-g0002.tif"/>
</fig>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Spectrally dependent maximum and effective quantum yields of PSII photochemistry in anemones photoacclimated to two light levels. Maximum quantum yields for high and low light acclimated <bold>(A)</bold> A4-a and <bold>(B)</bold> B1-a symbiont strains. High and low light acclimated effective quantum yields for <bold>(C)</bold> A4-a and <bold>(D)</bold> B1-a symbiont types. Dark bars represent low-light and gray bars represent high-light acclimated anemones. Error bars represent &#x000B1;SE. Asterisks represent significant differences between low and high light conditions.</p></caption>
<graphic xlink:href="fmars-04-00365-g0003.tif"/>
</fig>
</sec>
</sec>
<sec sec-type="results" id="s3">
<title>Results</title>
<sec>
<title>Effective quantum yield and functional absorption cross section in different symbionts</title>
<p>Effective quantum yield of PSII (Fq&#x02032;/Fm&#x02032;) varied across symbiont types and excitation wavelengths (Figure <xref ref-type="fig" rid="F2">2A</xref>). Symbiont type B1-b had between 15 and 23% higher yields than all others (<italic>P</italic> &#x0003D; 0.0005) at 505 nm. In addition, Fq&#x02032;/Fm&#x02032; in anemones harboring B1-b was 30% greater than strain B1-a at 447 nm (<italic>P</italic> &#x0003D; 0.02456) and 24% higher than strains B1-a and A4-a at 530 nm (<italic>P</italic> &#x0003D; 0.01324) (Figure <xref ref-type="fig" rid="F2">2A</xref>). Symbiont strain A4-b had significantly greater (at least 42% higher) light acclimated absorption cross section values than the A4-a strain under all excitation wavelengths (<italic>P</italic> &#x0003C; 0.034) (Figure <xref ref-type="fig" rid="F2">2B</xref>). The A4-b symbiont strain had at least 28% greater light acclimated absorption cross section values than the two B1 strains when measured using 505, 597, and 615 nm excitation wavelengths (<italic>P</italic> &#x0003C; 0.009) (Figure <xref ref-type="fig" rid="F2">2B</xref>). Analysis of similarity (ANOSIM) confirmed a strong separation across symbiont types (<italic>R</italic> &#x0003D; 0.7068, <italic>P</italic> &#x0003D; 0.0014). Additionally, the MDS analysis shows that the direction of separation between the two Clade A symbionts differs from that of the two Clade B symbionts (Figure <xref ref-type="fig" rid="F2">2C</xref>). This is likely due to differences in Fq&#x02032;/Fm&#x02032; driving the majority of separation between the two clade B symbionts (Figure <xref ref-type="fig" rid="F2">2A</xref>) whereas differences in the absorption cross section account for separation between clade A symbionts (Figure <xref ref-type="fig" rid="F2">2B</xref>).</p>
</sec>
<sec>
<title>Spectrally dependent maximum quantum yield of PSII and antennae bed quenching</title>
<p>The maximum quantum yield of PSII was statistically indistinguishable between low and high light acclimated animals harboring the A4-a symbiont strain at all excitation wavelengths (Figure <xref ref-type="fig" rid="F3">3A</xref>). However, Fv/Fm declined by 12&#x02013;23% under high light acclimation across all six excitation wavelengths in anemones harboring the B1-a strain (<italic>P</italic> &#x0003D; 0.02875, 0.0054, 0.0071, 0.0093, 0.0053, 0.0015 for 447, 505, 530, 597, 615, and 625 nm, respectively) (Figure <xref ref-type="fig" rid="F3">3B</xref>). There was a significant drop in the effective quantum yield in both sets of anemones, but only under the longer excitation wavelengths, with reductions for 615 nm (<italic>P</italic> &#x0003D; 0.0121, 31% reduction) and 625 nm (<italic>P</italic> &#x0003D; 0.0055, 27% reduction) for A4-a anemones and 597 nm (<italic>P</italic> &#x0003D; 0.0088, 19% reduction), 615 nm (<italic>P</italic> &#x0003D; 0.0140, 26% reduction) and 625 nm (<italic>P</italic> &#x0003D; 0.0381, 25% reduction) for B1-a anemones (Figures <xref ref-type="fig" rid="F3">3C,D</xref>). High light acclimation in the A4-a anemones resulted in a significant decrease in non-photochemical quenching within the antennae bed at excitation wavelengths of 505 nm (<italic>P</italic> &#x0003D; 0.0372, 40% reduction) and 530 nm (<italic>P</italic> &#x0003D; 0.0385, 29% reduction) (Figure <xref ref-type="fig" rid="F4">4A</xref>). Non-significant reduction in antennae bed quenching was also observed using a 447 nm excitation wavelength, with a <italic>P</italic>-value of 0.05032 (Figure <xref ref-type="fig" rid="F4">4A</xref>), There were no significant changes in non-photochemical quenching in the antennae bed for the B1-a symbiont (Figure <xref ref-type="fig" rid="F4">4B</xref>). Excitation wavelength 597 nm was excluded from Figure <xref ref-type="fig" rid="F4">4</xref> as antennae bed quenching was very low as the wavelength has limited overlap with any major photopigments (Iglesias-Prieto et al., <xref ref-type="bibr" rid="B12">1991</xref>; Iglesias-Prieto and Trench, <xref ref-type="bibr" rid="B15">1997a</xref>).</p>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Spectrally dependent antennae bed non-photochemical quenching for A4-a <bold>(A)</bold> and B1-a <italic>Symbiodinium</italic> <bold>(B)</bold>. Bars represent the mean and &#x000B1;SE for (black) low and (gray) high light acclimated samples. Asterisks represent significant differences between low and high light conditions.</p></caption>
<graphic xlink:href="fmars-04-00365-g0004.tif"/>
</fig>
</sec>
<sec>
<title>Absorption spectra and instrument comparison</title>
<p>There were no differences between absorption spectra of high and low light acclimated anemones harboring the B1-a strain (Figure <xref ref-type="fig" rid="F5">5B</xref>). However, differences were observed for the A4-a strain, where absorption was significantly lower (57%) at 447, 498, and 513 nm in high light acclimated animals (Figure <xref ref-type="fig" rid="F5">5C</xref>). When comparing the open-source instrument to the commercially produced FIRe fluorometer, similar absolute values, along with a significant reduction in Fv/Fm in response to high light was noted with both devices (<italic>P</italic> &#x0003D; 0.0033 and <italic>P</italic> &#x0003D; 0.0057, respectively; Figure <xref ref-type="fig" rid="F6">6A</xref>). However, using the open-sourced fluorometer, an interactive effect between symbiont type and light was also found (<italic>P</italic> &#x0003D; 0.041) as high-light reductions in Fv/Fm were only significant for the B1-a strain (Figure <xref ref-type="fig" rid="F6">6A</xref>). Although PSII functional absorption cross section is calculated in different units, both instruments detected similar total responses to high light acclimation where &#x003C3;<sub>PSII</sub> was significantly higher under high light acclimation (<italic>P</italic> &#x0003D; 0.0007 for FIRe and <italic>P</italic> &#x0003D; 0.0289 for open-sourced (Figure <xref ref-type="fig" rid="F6">6B</xref>).</p>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>LED output and whole anemone absorption Spectra. <bold>(A)</bold> Spectral characteristics for all six LED as well as the actinic light source. <bold>(B)</bold> Absorption spectra for the B1 symbiont under low (black) and high (gray) light conditions. <bold>(C)</bold> Absorption spectra for the B1 symbiont under low (black) and high (gray) light conditions. The solid line represents the average value and the gray area bounded by the dotted lines represent the standard deviation. Asterisks represent significant differences between low and high light conditions at the specific wavelengths.</p></caption>
<graphic xlink:href="fmars-04-00365-g0005.tif"/>
</fig>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>Comparison of open source and FIRe fluorometers. <bold>(A)</bold> Average maximum quantum yield of PSII (Fv/Fm) and <bold>(B)</bold> functional absorption cross section of PSII (&#x003C3;<sub>PSII</sub>). Left and right axes reflect &#x003C3;<sub>PSII</sub> units for the open-sourced and FIRe fluorometers respectively. Error bars represent &#x000B1;SE.</p></caption>
<graphic xlink:href="fmars-04-00365-g0006.tif"/>
</fig>
</sec>
<sec>
<title>Symbiont cell density, volume, and chlorophyll content</title>
<p>Under low light conditions, cell density was 49&#x02013;57% higher in B1-b as compared to the other symbiont strains (<italic>P</italic> &#x0003D; 0.0099). No significant differences in chlorophyll cell<sup>&#x02212;1</sup> were observed across symbiont strains. However, symbiont strain B1-a had 49&#x02013;76% higher cell volume (<italic>P</italic> &#x0003D; 0.0066) (Table <xref ref-type="table" rid="T2">2</xref>) than the other three symbiont types. With respect to high-light acclimation, a two-way ANOVA revealed an interactive effect between light and symbiont type as B1-a cell volume significantly decreased by 28% under high light conditions, were as the A4-a symbiont did not change (<italic>P</italic> &#x0003D; 0.0216). Only chlorophyll content significantly declined by 73 and 59% under high light (<italic>P</italic> &#x0003D; 0.0132) within B1-a and A4-a symbiont strains, respectively (Table <xref ref-type="table" rid="T2">2</xref>).</p>
<table-wrap position="float" id="T2">
<label>Table 2</label>
<caption><p>Symbiont physiology.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Symbiont type</bold></th>
<th valign="top" align="left"><bold>Light level</bold></th>
<th valign="top" align="left"><bold>Cell density (&#x003BC;g host protein<sup>&#x02212;1</sup>)</bold></th>
<th valign="top" align="left"><bold>Cell volume (&#x003BC;m<sup>&#x02212;3</sup>)</bold></th>
<th valign="top" align="left"><bold>Chlorophyll (pg cell<sup>&#x02212;1</sup>)</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">B1-b</td>
<td valign="top" align="left">Low</td>
<td valign="top" align="center">3453 &#x000B1; 397</td>
<td valign="top" align="center">394 &#x000B1; 34</td>
<td valign="top" align="center">5.18 &#x000B1; 0.7</td>
</tr>
<tr>
<td valign="top" align="left">A4-b</td>
<td valign="top" align="left">Low</td>
<td valign="top" align="center">2226 &#x000B1; 104</td>
<td valign="top" align="center">466 &#x000B1; 39</td>
<td valign="top" align="center">4.44 &#x000B1; 0.6</td>
</tr>
<tr>
<td valign="top" align="left">B1-a</td>
<td valign="top" align="left">Low</td>
<td valign="top" align="center">2196 &#x000B1; 129</td>
<td valign="top" align="center">694 &#x000B1; 63</td>
<td valign="top" align="center">4.17 &#x000B1; 0.8</td>
</tr>
<tr>
<td valign="top" align="left">A4-a</td>
<td valign="top" align="left">Low</td>
<td valign="top" align="center">2317 &#x000B1; 237</td>
<td valign="top" align="center">452 &#x000B1; 51</td>
<td valign="top" align="center">4.10 &#x000B1; 1.4</td>
</tr>
<tr>
<td valign="top" align="left">B1-a</td>
<td valign="top" align="left">High</td>
<td valign="top" align="center">2019 &#x000B1; 125</td>
<td valign="top" align="center">502 &#x000B1; 58</td>
<td valign="top" align="center">1.14 &#x000B1; 0.5</td>
</tr>
<tr>
<td valign="top" align="left">A4-a</td>
<td valign="top" align="left">High</td>
<td valign="top" align="center">2070 &#x000B1; 353</td>
<td valign="top" align="center">470 &#x000B1; 21</td>
<td valign="top" align="center">1.69 &#x000B1; 0.2</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec sec-type="discussion" id="s4">
<title>Discussion</title>
<p>Our results demonstrate wavelength dependent responses in both effective quantum yield and the functional absorption cross section of PSII across different symbionts. <italic>Symbiodinium</italic> have two major light harvesting complexes, the membrane bound Chla a-Chla C<sub>2</sub>-peridinin-protein-complex (acpPC) and the soluble Peridinin-Chlorophyll Protein (PCP) complex, both of which absorb light predominantly between 400 and 550 nm (Iglesias-Prieto et al., <xref ref-type="bibr" rid="B12">1991</xref>, <xref ref-type="bibr" rid="B13">1993</xref>; Niedzwiedzki et al., <xref ref-type="bibr" rid="B29">2013</xref>, <xref ref-type="bibr" rid="B28">2014</xref>). Importantly, Iglesias-Prieto and Trench (<xref ref-type="bibr" rid="B16">1997b</xref>) demonstrated how the relative abundance of these different light harvesting compounds could vary across symbiont types growing in culture and/or with respect to high vs. low light acclimation. This was further refined by Hennige et al. (<xref ref-type="bibr" rid="B8">2009</xref>) whom used high performance liquid chromatography (HPLC) to compare the relative photopigment concentrations across eight different symbiont types. Such differences may give rise to the spectrally dependent differences across algal species observed here (Figure <xref ref-type="fig" rid="F2">2</xref>). Data from this study largely agree with previous work that used a commercially available multi-spectral pulse amplitude modulation (PAM) fluorometer with a symbiotic coral, that also documented clear wavelength dependencies in <italic>Symbiodinium</italic> photochemical activity (Szab&#x000F3; et al., <xref ref-type="bibr" rid="B39">2014</xref>). In particular, the A4-b (strain: KLAp2) symbiont displayed a higher absolute PSII functional absorption cross section in the light activated state (&#x003C3;<sub>PSII&#x02032;</sub>) relative to the other symbiotic algae, and similar to the results of Szab&#x000F3; et al. (<xref ref-type="bibr" rid="B39">2014</xref>) (albeit in their dark acclimated samples), higher (&#x003C3;<sub>PSII&#x02032;</sub>) in lower excitation wavelengths (447&#x02013;530 nm) which then decreased toward red excitation (Figure <xref ref-type="fig" rid="F2">2A</xref>). In contrast, the light acclimated PSII absorption cross section of the A4-a symbiont steadily decreased as excitation light moved from the blue to the red spectrum. Because the photopigments diadinoxanthin and peridinin have peak absorbance values near 505 and 530 nm, respectively, such divisions in &#x003C3;<sub>PSII&#x02032;</sub> could be driven by different levels of Chl <italic>a</italic>:diadinoxanthin or Chl <italic>a</italic>:peridinin ratios as well as light harvesting protein content. The decline in functional absorption cross section toward the red excitation spectrum is also naturally due to lower light harvesting complex absorption in the higher wavelength range. In corals, this also correlates to a higher scalar irradiance at higher wavelengths (Wangpraseurt et al., <xref ref-type="bibr" rid="B40">2012</xref>), however, it is not known if a similar irradiance pattern exists in a symbiotic sea anemone that lacks a calcium carbonate skeleton.</p>
<p>The significant drop in chlorophyll <italic>a</italic> concentration in the high light acclimated A4-a and B1-a symbionts is a common photoacclimation response which significantly decrease the amount of light captured by the cell, thereby reducing the potential for excess excitation energy under high irradiance levels. Photoacclimation in <italic>Symbiodinium</italic> has been documented among a number of different species and the overall response is well-understood (Iglesias-Prieto and Trench, <xref ref-type="bibr" rid="B14">1994</xref>, <xref ref-type="bibr" rid="B16">1997b</xref>; Hennige et al., <xref ref-type="bibr" rid="B8">2009</xref>; Finney et al., <xref ref-type="bibr" rid="B4">2010</xref>). Similar to that observed during stress conditions, total organism absorbance may also decline, as symbionts reduce the amount of light that is absorbed and channeled toward photosynthesis (Rodriguez-Rom&#x000E1;n et al., <xref ref-type="bibr" rid="B32">2006</xref>; Hoadley et al., <xref ref-type="bibr" rid="B9">2016</xref>). Although absorbance decreased in the high light acclimated anemones harboring the A4-a alga, there was no significant change in absorbance between the two acclimation light levels for the anemones harboring the B1-a symbiont. Despite the decline in Chl <italic>a</italic> cell<sup>&#x02212;1</sup> in the high light acclimated B1-a, this lower absorption difference may have been due, in part, to the alga cell size which also declined during high light acclimation, thus chlorophyll cellular volume<sup>&#x02212;1</sup> and pigment packaging may have remained similar across the two light levels.</p>
<p>Interestingly, acclimation to high light conditions reduced Fq&#x02032;/Fm&#x02032; in both symbiont types, but only when excited with red spectrum (597&#x02013;625 nm) wavelengths. Because photoprotective pigments such as xanthophylls do not absorb at these wavelengths, it is possible that the observed reductions in Fq&#x02032;/Fm&#x02032; are indicative of decoupling between PSII reaction centers and light harvesting proteins. Apart from this reduction in Fq&#x02032;/Fm&#x02032;, the two holobionts showed marked photochemical differences in their patterns of photoacclimation, as the B1-a alga displayed a consistent down-regulation of functional PSII reaction centers (i.e., significant decline in Fv/Fm) (Figure <xref ref-type="fig" rid="F3">3B</xref>), while the A4-a symbiont reduced overall absorbance more and displayed a reduction in antennae-based non-photochemical quenching (Figure <xref ref-type="fig" rid="F4">4A</xref>) while Fv/Fm remained stable (Figure <xref ref-type="fig" rid="F3">3A</xref>). Under high light acclimation, microalgae tend to increase photo-protective mechanisms such as antennae-based non-photochemical quenching (Suggett et al., <xref ref-type="bibr" rid="B36">2007</xref>). The reductions in non-photochemical quenching within the antennae bed observed for A4-a may possibly reflect a difference in optics associated with living inside the host anemone as opposed to free-living as is the case for most microalgal light acclimation studies. Coral tissues contain numerous fluorescent proteins which can substantially change the perceived light field for <italic>in situ</italic> symbionts (Dove, <xref ref-type="bibr" rid="B2">2004</xref>). These host derived proteins may also differ across light and temperature gradients thus potentially also influencing symbiont response to elevated light conditions (Salih et al., <xref ref-type="bibr" rid="B33">2000</xref>). Current efforts in understanding the miroenvironments in which <italic>Symbiodinium</italic> live (Wangpraseurt et al., <xref ref-type="bibr" rid="B40">2012</xref>; Lichtenberg et al., <xref ref-type="bibr" rid="B24">2016</xref>) are critical for improving our knowledge of coral/algal photoprotective mechanisms.</p>
<p>To ground-truth our fluorometer, we compared measurements of the same samples against a single excitation (peak 447 nm) Fluorescence Induction and Relaxation (FIRe) fluorometer (Satlantic Inc.). Both systems reported similar Fv/Fm values and overall trends in response to low and high light acclimation (Figure <xref ref-type="fig" rid="F6">6</xref>). Likewise, a similar response in functional absorption cross section was noted for both instruments, as high light acclimation led to elevated &#x003C3;<sub>PSII</sub> values. The slight reduction in Fv/Fm in the B1-a alga under high light acclimation noted with both systems is consistent with previously published work with most cultured <italic>Symbiodinium</italic> and reef corals (Lesser and Gorbunov, <xref ref-type="bibr" rid="B23">2001</xref>; Hennige et al., <xref ref-type="bibr" rid="B8">2009</xref>), however, the rise in &#x003C3;<sub>PSII</sub> under high light is not as common, and &#x003C3;<sub>PSII</sub> in cultured <italic>Symbiodinium</italic> tend to decrease slightly under high light (see Hennige et al., <xref ref-type="bibr" rid="B8">2009</xref> for one exception to this in a cultured F2 alga).</p>
<p>It is interesting to note that while the symbiont-anemone combinations used in this study contained a similar symbiont density and Chl. <italic>a</italic> algal cell<sup>&#x02212;1</sup> (Table <xref ref-type="table" rid="T2">2</xref>), multispectral active chlorophyll fluorescence revealed clear differences in symbiont photochemical efficiency that would be missed by a conventional fluorometer using a single wavelength band excitation light source. Importantly, symbiont density was normalized to the quantity of total soluble animal protein, and this does not account for possible structural differences between these two anemone populations, symbiont distributions across anemone location (e.g., tentacles vs. oral disc), or light absorbing animal pigments, all of which could significantly alter the photosynthetically usable radiation (PUR) in these animals further.</p>
<p>Different algal populations were separated by their light acclimated photochemical patterns (Figure <xref ref-type="fig" rid="F2">2C</xref>), but were not resolvable from dark acclimated samples alone (not shown). Spectrally dependent differences in algal photochemistry can not only provide more detail of photochemical differences within a single symbiosis, and also may potentially be a powerful tool for resolving genetically (and functionally) different <italic>Symbiodinium</italic> populations across diverse cnidarian hosts, including reef building corals. These results, while limited in scope, are similar to those of a more extensive study by Suggett et al. (<xref ref-type="bibr" rid="B35">2015</xref>) that examined 18 genetically distinct cultured <italic>Symbiodinium</italic> isolates with a single waveband excitation (peak excitation, 450 nm) fast repetition rate fluorometer. Specifically, that work noted that different phylotypes of <italic>Symbiodinium</italic> could be grouped into particular clusters based on the balance of how symbionts used the fraction of open PSII reaction centers (i.e., photochemical quenching or [1-<italic>C</italic>] vs. non-photochemical quenching [1-<italic>Q</italic>]).</p>
<p>There is a growing interest in the field of plant biology to better characterize genomic expression by characterizing specific phenotypic traits in a given environment, also known as phenomics (Furbank and Tester, <xref ref-type="bibr" rid="B5">2011</xref>). Similar to the desire to link genomics to plant function and favorable agricultural traits, there is a growing need to characterize specific physiological traits of symbiotic reef building corals to their environment (Madin et al., <xref ref-type="bibr" rid="B25">2016</xref>; Warner and Suggett, <xref ref-type="bibr" rid="B42">2016</xref>). Active chlorophyll fluorescence is one such tool that has the potential to allow for rapid high throughput screening of photochemical response to different environmental conditions.</p>
<p>This work suggests that low-cost multispectral chlorophyll <italic>a</italic> fluorescence may prove useful in delineating functional traits as well as groups of different symbionts. Open source hardware and software platforms are becoming increasingly popular within the research community as their ease of use and low cost promotes high levels of customization for specific applications and a broad user base that reaches beyond traditional academic research. For example, the MultspeQ is a recently developed fluorometer designed to promote greater utilization across both scientific and community users interested in assessing terrestrial plant physiological responses via a phenomics-based approach (Kuhlgert et al., <xref ref-type="bibr" rid="B19">2016</xref>). By utilizing chlorophyll fluorescence and absorbance based parameters, it is designed to provide a common platform to compare the photochemical traits of plant species worldwide. This device is relatively low cost, in part, due to the utilization and promotion of open access hardware and software platforms. The advantage of a greater user base also allows for higher level interpretation and analysis of the collected data. Although this current study does not offer a fully developed product for other users, it serves as an example of the type of research that can be achieved through the integration of open source platforms with specific research questions in mind and relatively inexpensive hardware. As more advanced hardware platforms adopt the open source concept, it is possible that even more sophisticated and low-cost instrumentation will become more accessible to a larger community of scientific and public community users interested in monitoring the physiological stability of algal-invertebrate symbioses as well.</p>
<p>In conclusion, spectrally dependent characteristics of symbiont photochemistry were effectively quantified using a multispectral chlorophyll-<italic>a</italic> fluorometer. It is likely that the spectrally dependent characteristics observed here correlate with differences in photopigment abundance across symbiont types as has been previously shown using immunoblot and HPLC analyses (Iglesias-Prieto et al., <xref ref-type="bibr" rid="B12">1991</xref>; Iglesias-Prieto and Trench, <xref ref-type="bibr" rid="B16">1997b</xref>; Hennige et al., <xref ref-type="bibr" rid="B8">2009</xref>). With respect to symbiont types A4-a and B1-a, spectrally resolved Fv/Fm and &#x003C3;<sub>PSII</sub> values revealed additional changes in response to high-light acclimation that would not be possible if using more conventional active chlorophyll-<italic>a</italic> fluorometers with a single excitation wavelength centered at 450 nm. Importantly, these spectrally resolved fluorescence measurements were made using a custom built fluorometer using open source hardware and software platforms. Our work serves as an example of the potential for open source platforms to be utilized to construct purpose built and relatively low-cost instruments.</p>
</sec>
<sec id="s5">
<title>Author contributions</title>
<p>All authors listed have made a substantial, direct and intellectual contribution to the work, and approved it for publication.</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>This project was supported by funding from the National Science Foundation (awards 1316055 and 1258065 to MW).</p>
</ack>
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