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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Oncol.</journal-id>
<journal-title>Frontiers in Oncology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Oncol.</abbrev-journal-title>
<issn pub-type="epub">2234-943X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fonc.2021.671431</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Oncology</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>USP9X Is Required to Maintain Cell Survival in Response to High-LET Radiation</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Nickson</surname>
<given-names>Catherine M.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn002">
<sup>&#x2020;</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Fabbrizi</surname>
<given-names>Maria Rita</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn002">
<sup>&#x2020;</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1245245"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Carter</surname>
<given-names>Rachel J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hughes</surname>
<given-names>Jonathan R.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Kacperek</surname>
<given-names>Andrzej</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hill</surname>
<given-names>Mark A.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/767712"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Parsons</surname>
<given-names>Jason L.</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>*</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/125192"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Cancer Research Centre, Department of Molecular and Clinical Cancer Medicine, University of Liverpool</institution>, <addr-line>Liverpool</addr-line>, <country>United Kingdom</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Clatterbridge Cancer Centre NHS Foundation Trust</institution>, <addr-line>Bebington</addr-line>, <country>United Kingdom</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Department of Oncology, CRUK/MRC Oxford Institute for Radiation Oncology, University of Oxford, Gray Laboratories</institution>, <addr-line>Oxford</addr-line>, <country>United Kingdom</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Pankaj Chaudhary, Queen&#x2019;s University Belfast, United Kingdom</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Rupak Pathak, University of Arkansas for Medical Sciences, United States; Paul F. Wilson, University of California, Davis, United States</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Jason L. Parsons, <email xlink:href="mailto:j.parsons@liverpool.ac.uk">j.parsons@liverpool.ac.uk</email>
</p>
</fn>
<fn fn-type="equal" id="fn002">
<p>&#x2020;These authors have contributed equally to this work</p>
</fn>
<fn fn-type="other" id="fn003">
<p>This article was submitted to Radiation Oncology, a section of the journal Frontiers in Oncology</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>01</day>
<month>07</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>11</volume>
<elocation-id>671431</elocation-id>
<history>
<date date-type="received">
<day>23</day>
<month>02</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>15</day>
<month>06</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2021 Nickson, Fabbrizi, Carter, Hughes, Kacperek, Hill and Parsons</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Nickson, Fabbrizi, Carter, Hughes, Kacperek, Hill and Parsons</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) and the copyright owner(s) 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>Ionizing radiation (IR) principally acts through induction of DNA damage that promotes cell death, although the biological effects of IR are more broad ranging. In fact, the impact of IR of higher-linear energy transfer (LET) on cell biology is generally not well understood. Critically, therefore, the cellular enzymes and mechanisms responsible for enhancing cell survival following high-LET IR are unclear. To this effect, we have recently performed siRNA screening to identify deubiquitylating enzymes that control cell survival specifically in response to high-LET &#x3b1;-particles and protons, in comparison to low-LET X-rays and protons. From this screening, we have now thoroughly validated that depletion of the ubiquitin-specific protease 9X (USP9X) in HeLa and oropharyngeal squamous cell carcinoma (UMSCC74A) cells using small interfering RNA (siRNA), leads to significantly decreased survival of cells after high-LET radiation. We consequently investigated the mechanism through which this occurs, and demonstrate that an absence of USP9X has no impact on DNA damage repair post-irradiation nor on apoptosis, autophagy, or senescence. We discovered that USP9X is required to stabilize key proteins (CEP55 and CEP131) involved in centrosome and cilia formation and plays an important role in controlling pericentrin-rich foci, particularly in response to high-LET protons. This was also confirmed directly by demonstrating that depletion of CEP55/CEP131 led to both enhanced radiosensitivity of cells to high-LET protons and amplification of pericentrin-rich foci. Our evidence supports the importance of USP9X in maintaining centrosome function and biogenesis and which is crucial particularly in the cellular response to high-LET radiation.</p>
</abstract>
<kwd-group>
<kwd>centrosome</kwd>
<kwd>DNA damage</kwd>
<kwd>DNA repair</kwd>
<kwd>ionizing radiation</kwd>
<kwd>protons</kwd>
<kwd>ubiquitin</kwd>
<kwd>USP9X</kwd>
</kwd-group>
<contract-sponsor id="cn001">Medical Research Council<named-content content-type="fundref-id">10.13039/501100000265</named-content>
</contract-sponsor>
<contract-sponsor id="cn002">North West Cancer Research Fund<named-content content-type="fundref-id">10.13039/501100000357</named-content>
</contract-sponsor>
<counts>
<fig-count count="7"/>
<table-count count="2"/>
<equation-count count="0"/>
<ref-count count="48"/>
<page-count count="12"/>
<word-count count="7011"/>
</counts>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<title>Introduction</title>
<p>Ionizing radiation (IR) is a major cancer treatment modality for primary and metastatic cancers. Although conventional radiotherapy (e.g. X-rays) is largely employed, there is an increase in the utilization of precision proton beam therapy (PBT) that can more accurately deliver the radiation dose to the tumor, thus limiting any adverse side effects. In particular, PBT is used for the treatment of solid tumors, such as head and neck squamous cell carcinoma (<xref ref-type="bibr" rid="B1">1</xref>). The therapeutic effect of IR is predominantly through the induction of DNA damage that ultimately drives cancer cell death. As well as DNA double strand breaks (DSBs), IR causes the formation of complex DNA damage (CDD), which is defined as two or more DNA lesions within one or two DNA helical turns, that contribute to the cell killing effects of the radiation (<xref ref-type="bibr" rid="B2">2</xref>&#x2013;<xref ref-type="bibr" rid="B4">4</xref>). This is particularly relevant following high-linear energy transfer (LET) radiation that generates increased quantities and complexity of CDD. Indeed, PBT displays increases in LET at the Bragg peak and at the distal edge where the majority of the radiation dose is delivered, which creates uncertainty in the treatment because of the different biological effects (<xref ref-type="bibr" rid="B5">5</xref>). Specifically within cultured cells, CDD has been shown to persist for several hours post-irradiation (<xref ref-type="bibr" rid="B6">6</xref>, <xref ref-type="bibr" rid="B7">7</xref>), and therefore, its importance in promoting genome instability and cell death following IR is recognized (<xref ref-type="bibr" rid="B5">5</xref>, <xref ref-type="bibr" rid="B8">8</xref>). Although the biological impact of high-LET radiation is largely associated with the direct effects of irreparable CDD induction, this has also been demonstrated to promote disruption and persistent changes to chromatin structure (<xref ref-type="bibr" rid="B9">9</xref>, <xref ref-type="bibr" rid="B10">10</xref>), enhance cellular senescence (<xref ref-type="bibr" rid="B11">11</xref>), and to increase apoptotic signaling (<xref ref-type="bibr" rid="B12">12</xref>). This reflects, to some degree, the potentially diverse mechanisms through which high-LET radiation may act.</p>
<p>The ubiquitin proteasome pathway, catalyzed by E3 ubiquitin ligases and deubiquitylation enzymes (DUBs), is known to be important in the regulation of several DNA repair pathways where it acts to control the cellular levels of key proteins that co-ordinate the repair of the DNA damage (<xref ref-type="bibr" rid="B13">13</xref>&#x2013;<xref ref-type="bibr" rid="B15">15</xref>). Recently, we discovered that ubiquitylation is a key factor in the cellular response to high-LET radiation, including high-LET &#x3b1;-particles and protons. Specifically, we identified that histone H2B ubiquitylation on lysine 120, which is catalyzed by the E3 ubiquitin ligases ring finger protein 20/40 (RNF20/40) and male-specific lethal-2 homolog (MSL2), is induced following high-LET radiation. Induction of histone H2B ubiquitylation in turn promotes the repair of CDD required for cell survival (<xref ref-type="bibr" rid="B6">6</xref>). Subsequently, we utilized an siRNA screening strategy to identify that ubiquitin specific protease 6 (USP6) is important for maintaining levels of the DNA repair protein poly (ADP-ribose) polymerase-1 (PARP-1), which is similarly essential for efficient repair of CDD and thus survival of cells following irradiation with high-LET &#x3b1;-particles and protons (<xref ref-type="bibr" rid="B7">7</xref>). Our findings also highlighted the involvement of other DUBs in controlling cell survival under these conditions, although their precise roles and mechanisms of action in response to high-LET radiation are yet to be determined.</p>
<p>The ubiquitin-specific protease 9X (USP9X) is a highly conserved DUB, which has been suggested to play several important roles, particularly in maintaining cell survival, development, and polarity, as well as in protein trafficking (<xref ref-type="bibr" rid="B16">16</xref>). Specifically, USP9X has been shown to regulate apoptosis by initiating the apoptotic c-Jun N-terminal kinase (JNK) signaling cascade in neurons and embryonic kidney cells (<xref ref-type="bibr" rid="B17">17</xref>, <xref ref-type="bibr" rid="B18">18</xref>). Conversely, USP9X is also proposed to be involved in the stabilization of the anti-apoptotic protein Mcl-1 by protecting it from ubiquitylation-dependent proteasomal degradation (<xref ref-type="bibr" rid="B19">19</xref>, <xref ref-type="bibr" rid="B20">20</xref>), indicating that the role of USP9X in cell death regulation may be cell-type and disease specific. In fact, a role for USP9X in cancer development is not yet clear, having been found to act both as an oncogene and a tumor suppressor, depending on the type and stage of cancer (<xref ref-type="bibr" rid="B16">16</xref>). More recently, there has been accumulating evidence identifying USP9X as a major player in the maintenance and stability of key centriolar satellite proteins, consequently involved in promoting centrosome duplication (<xref ref-type="bibr" rid="B21">21</xref>&#x2013;<xref ref-type="bibr" rid="B24">24</xref>). However, a role for USP9X in the cellular response to IR, and specifically the impact of the enzyme following high-LET radiation, has not been previously reported.</p>
<p>In this study, we have now further examined the roles of other DUBs that are required to promote cell survival specifically in response to high-LET radiation, with a focus on PBT that generates increasing LET particularly at the Bragg peak distal end. We demonstrate that an siRNA knockdown of USP9X leads to increased cell death specifically in response to high-LET protons and &#x3b1;-particle irradiation, but not to low-LET protons and X-rays. We further show that this reduction in cell survival in USP9X-depleted cells does not correlate with alterations in the efficiency of CDD repair or with the activation of cell death pathways, but is in fact mediated by centriolar satellite accumulation.</p>
</sec>
<sec id="s2" sec-type="materials|methods">
<title>Materials And Methods</title>
<sec id="s2_1">
<title>Antibodies and siRNA</title>
<p>The DUB siRNA library (ON-TARGETplus), USP9X siRNA pool and individual siRNA targeting USP9X (USP9X_6 5&#x2032;-AGAAAUCGCUGGUAUAAAU-3&#x2032; and USP9X_8 5&#x2032;-GUACGACGAUGUAUUCUCA-3&#x2032;) were from Horizon Discovery (Cambridge, UK). The non-targeting control siRNA (AllStars Negative Control siRNA) was from Qiagen (Manchester, UK). The following antibodies were used: PARP-1 (sc-53643) and Mcl-1 (sc-819; both Santa Cruz Biotechnology, Heidelberg, Germany), &#x3b3;H2AX (05-636; Merck-Millipore, Watford, UK), USP9X (A301-350A) and 53BP1 (A300-272A; both Bethyl Labs, Montgomery, AL), LC3B (2775) and &#x3b2;-Galactosidase (9860; both Cell Signaling Technology, London, UK), Pericentrin (ab4448; Abcam, Cambridge, UK), CEP55 (23891-1-AP) and CEP131 (25735-1-AP; both Proteintech, Manchester, UK) and tubulin (T6199; Sigma-Aldrich, Gillingham, UK). Goat anti-mouse Alexa Fluor 555 (A21422) or goat anti-rabbit Alexa Fluor 488 (A11008) secondary antibodies for immunofluorescence were from Life Technologies (Paisley, UK).</p>
</sec>
<sec id="s2_2">
<title>Cell Culture and Irradiation Sources</title>
<p>Oropharyngeal squamous cell carcinoma cells (UMSCC74A) were kindly provided by Prof T. Carey, University of Michigan, USA. HeLa and UMSCC74A cells were routinely cultured as monolayers in Dulbecco&#x2019;s Modified Eagle Medium (DMEM) supplemented with 10% fetal bovine serum, 2 mM <sc>l</sc>-glutamine, 1&#xd7; penicillin-streptomycin and 1&#xd7; non-essential amino acids. siRNA knockdowns were performed for 48&#xa0;h using Lipofectamine RNAiMAX (Life Technologies, Paisley, UK). Irradiation sources are as previously described (<xref ref-type="bibr" rid="B6">6</xref>). In brief, cells were exposed to either low-LET X-rays (100 kV; CellRad X-ray irradiator, Faxitron Bioptics, Tucson, USA; dose rate of ~3 Gy/min), or with a horizontal, passive-scattered proton beam line of 60 MeV maximal energy at the Clatterbridge Cancer Centre. These low-energy X-rays will generate higher LET photoelectrons and therefore a raised RBE when compared to higher energy photon sources (<xref ref-type="bibr" rid="B25">25</xref>, <xref ref-type="bibr" rid="B26">26</xref>). For low-LET proton irradiations, cells were irradiated directly by a ~1 keV/&#xb5;m pristine beam of 58 MeV effective energy (dose rate of ~5 Gy/min). For high-LET proton irradiations, a modulator was utilized to generate a 27-mm spread-out Bragg peak and a 24.4-mm absorber was used to position the cells at the distal edge, corresponding to a mean proton energy of 11 MeV at a dose averaged LET of 12 keV/&#xb5;m (dose rate of ~5 Gy/min). The LET was an estimation based on previous work utilizing the Clatterbridge beam (<xref ref-type="bibr" rid="B27">27</xref>) and considering the proton stopping power at this range. RBE values of 1.67 &#xb1; 0.14 (Hela) and 1.85 &#xb1; 0.15 (UMSCC74A), comparing high-LET <italic>versus</italic> low-LET protons, have been previously determined (<xref ref-type="bibr" rid="B6">6</xref>). High-LET &#x3b1;-particle irradiations (3.26 MeV, 121 keV/&#xb5;m) were performed on cells grown on Mylar sealed on glass cylinders using a <sup>238</sup>Pu irradiator at the CRUK/MRC Oxford Institute for Radiation Oncology, as previously described (<xref ref-type="bibr" rid="B28">28</xref>, <xref ref-type="bibr" rid="B29">29</xref>). Assuming a typical cross-sectional nuclear area of an attached Hela and UMSCC74A cell of ~150 &#xb5;m<sup>2</sup>, these irradiations correspond to a mean of ~940, 78, and 7.7 nuclear traversals per Gy for low-LET protons, high-LET protons, and &#x3b1;-particle irradiations, respectively (<xref ref-type="bibr" rid="B29">29</xref>), with the number following a Poisson distribution and dependent on the natural variation in nuclear cross-sectional area with the cell cycle.</p>
</sec>
<sec id="s2_3">
<title>Clonogenic Assays</title>
<p>Clonogenic assays were performed as recently described (<xref ref-type="bibr" rid="B6">6</xref>, <xref ref-type="bibr" rid="B7">7</xref>). In brief, following siRNA treatments, cells were irradiated in 35-mm dishes, harvested and a defined number seeded in triplicate into 6-well plates. Plating efficiencies for the untreated cells were as follows: HeLa (~40%), UMSCC74A (~10%). Plating efficiencies for USP9X siRNA-treated cells were as follows: HeLa (~30%), UMSCC74A (~4%). Increasing cell numbers were plated for increasing IR doses to allow for reductions in plating efficiencies. Colonies were allowed to grow for 7 to 10 days prior to fixing and staining with 6% glutaraldehyde and 0.5% crystal violet for 30&#xa0;min. Dishes were washed, left to air dry overnight and colonies counted using the GelCount colony analyzer (Oxford Optronics, Oxford, UK). Colony counting settings were optimized for both cell lines, based on inclusion of distinct colonies of specific size and intensity, although the same settings were used across the various treatments. A colony is defined as containing 50 or more cells. Relative colony formation (surviving fraction) was expressed as colonies per treatment level <italic>versus</italic> colonies that appeared in the untreated control. Results were accumulated from at least three independent biological experiments, apart from the siRNA screen which was from a single experiment (but containing triplicate samples).</p>
</sec>
<sec id="s2_4">
<title>Cell Cycle Analysis and Immunoblotting</title>
<p>For cell cycle analysis, cells were trypsinized, washed twice with ice-cold PBS (100 &#xd7; <italic>g</italic> for 5&#xa0;min at 4&#xb0;C), fixed with ice cold 70% ethanol and kept at 4&#xb0;C until analysis. Fixed cells were centrifuged (200 &#xd7; <italic>g</italic> for 5&#xa0;min at 4&#xb0;C), washed with PBS containing 0.05% Tween-20, and then resuspended in PBS containing 0.05% Tween-20, 10 &#xb5;g/ml propidium iodide and 0.1 mg/ml RNase A for 1&#xa0;h at room temperature. Analysis was performed using the Attune NxT Flow Cytometer (Life Technologies, Paisley, UK). Whole-cell extracts were prepared, separated by SDS-PAGE electrophoresis, and analyzed by quantitative immunoblotting using the Odyssey image analysis system (Li-cor Biosciences, Cambridge, UK), as previously described (<xref ref-type="bibr" rid="B30">30</xref>, <xref ref-type="bibr" rid="B31">31</xref>).</p>
</sec>
<sec id="s2_5">
<title>Enzyme-Modified Neutral Comet Assay</title>
<p>Detection of CDD was achieved using enzyme treatment of DNA originally described by Sutherland et&#xa0;al. (<xref ref-type="bibr" rid="B32">32</xref>, <xref ref-type="bibr" rid="B33">33</xref>), but which has been employed in development of the enzyme-modified neutral comet assay, as recently described (<xref ref-type="bibr" rid="B34">34</xref>). In brief, cells were trypsinized, diluted to 1 &#xd7; 10<sup>5</sup> cells/ml and 250-&#xb5;l aliquots of the cell suspension placed into the wells of a 24-well plate, which was placed on ice. Cells were irradiated (4 Gy) and embedded on a microscope slide in low melting agarose (Bio-Rad, Hemel Hempstead, UK). The slides were incubated for up to 4&#xa0;h at 37&#xb0;C in a humidified chamber to allow for DNA repair, prior to cell lysis in buffer containing 2.5 M NaCl, 100 mM EDTA, 10 mM Tris-HCl pH 10.5, 1% N-lauroylsarcosine, 1% DMSO, and 1% (v/v) Triton X-100. Slides were washed three times with enzyme reaction buffer (40 mM HEPES-KOH, 100 mM KCl, 0.5 mM EDTA and 0.2 mg/ml BSA, pH 8.0), and then incubated with either buffer alone (mock-treated; revealing levels of DNA DSBs) or with buffer containing 5 pmol OGG1, 6 pmol NTH1, and 0.6 pmol APE1 (enzyme-treated; revealing levels of DNA DSBs plus CDD) for 1&#xa0;h at 37&#xb0;C in a humidified chamber. Following treatment, slides were placed in cold electrophoresis buffer [1 &#xd7; TBE buffer (pH 8.3)] in the dark for 25&#xa0;min to allow the DNA to unwind, prior to electrophoresis at 25&#xa0;V, ~20 mA for 25&#xa0;min. Slides were washed three times with 1&#xd7; PBS before allowing to dry overnight. Slides were rehydrated for 30&#xa0;min in water (pH 8.0), stained for 30&#xa0;min with SYBR Gold (Life Technologies, Paisley, UK), diluted 1:10,000 in water (pH 8.0), and again dried overnight. Cells (50 per slide, in duplicate) were analyzed from the dried slides using the Komet 6.0 image analysis software (Andor Technology, Belfast, Northern Ireland) and % tail DNA values averaged from at least three independent biological experiments.</p>
</sec>
<sec id="s2_6">
<title>Immunofluorescence and &#x3b2;-Galactosidase Staining</title>
<p>Measurement of DNA repair protein foci (&#x3b3;H2AX and 53BP1) was examined as previously described (<xref ref-type="bibr" rid="B30">30</xref>). In brief, cells were grown on 13-mm coverslips until ~70% to 80% confluent, irradiated at 4 Gy and incubated for up to 8&#xa0;h in 5% CO<sub>2</sub> at 37&#xb0;C to allow for DNA repair. Cells were washed with PBS at room temperature for 5&#xa0;min, before being fixed using 4% paraformaldehyde for 10&#xa0;min. Cells were permeabilized with 0.2% Triton X-100 in PBS for 10&#xa0;min, washed three times with 0.1% Tween-20 for 10&#xa0;min, and blocked to avoid non-specific staining <italic>via</italic> incubation with 2% BSA for 30&#xa0;min at room temperature on a rocking platform. &#x3b3;H2AX or 53BP1 antibodies in 2% BSA were subsequently added and coverslips incubated overnight at 4&#xb0;C. Following three washes with PBS, coverslips were incubated with either goat anti-mouse Alexa Fluor 555 or goat anti-rabbit Alexa Fluor 488 secondary antibodies in 2% BSA for 1&#xa0;h at room temperature in the dark. Finally, samples were washed with PBS for 10&#xa0;min on a rocking platform and mounted on a microscope slide using Fluoroshield containing DAPI (Sigma-Aldrich, Gillingham, UK). Cells were examined using an Olympus BX61 fluorescent microscope with a Photometrics CoolSNAP HQ2 CCD camera. MicroManager software was used to capture images (~20 images/cell line/antibody). Similarly, cells were fixed on coverslips post-irradiation (4 Gy) and incubation (48&#xa0;h), but then stained using Pericentrin antibodies prior to incubation with AlexaFluor488 secondary antibodies, and pericentrin-rich foci scored using fluorescence microscopy. Analysis of senescence was carried out using the &#x3b2;-Galactosidase Staining kit (Cell Signaling Technology, London, UK) and where hydrogen peroxide (100 &#xb5;M for 2&#xa0;h) was used as a positive control.</p>
</sec>
<sec id="s2_7">
<title>Statistical Analysis</title>
<p>All experiments (unless defined above) were performed in at least triplicate as separate independent, biological experiments. Statistical analysis of clonogenic survival data was performed using a one-way ANOVA and comparing surviving fractions at 2 Gy (SF2) or 4 Gy (SF4). Statistical analysis of DNA damage quantified through neutral comet assays and pericentrin-rich foci through immunofluorescence staining was performed using either a one-sample or two-sample <italic>t</italic> test.</p>
</sec>
</sec>
<sec id="s3" sec-type="results">
<title>Results</title>
<sec id="s3_1">
<title>Screening for DUBs Involved in Response to High-LET IR</title>
<p>In our recent work, we performed an siRNA screen of 84 DUBs analyzing the survival of HeLa cells after a single dose of IR, with a particular focus on high-LET IR, which generates increased levels and complexity of CDD consisting of two or more DNA lesions within one or two helical turns of the DNA (<xref ref-type="bibr" rid="B7">7</xref>). We have now further interrogated these data, which demonstrates the wide range of changes in HeLa cell survival in response to a single dose of high-LET &#x3b1;-particles (121 keV/&#xb5;m) <italic>versus</italic> low-LET X-rays following individual DUB knockdowns (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1A</bold>
</xref>). Similarly, a variability in cell survival in the absence of the DUBs is observed in response to relatively high-LET protons (12 keV/&#xb5;m) generated at the Bragg peak distal edge, <italic>versus</italic> low-LET protons (1 keV/&#xb5;m) at the entrance dose of a pristine beam (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1B</bold>
</xref>). Survival was normalized to the irradiated mock-treated control sample (generating ~40% cell survival), which was set to 1.0, and the data subsequently plotted (on a log<sub>2</sub> scale). The top 10 DUB candidates reducing cell survival in response to high-LET &#x3b1;-particles (<xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>) and relatively high-LET protons (<xref ref-type="table" rid="T2">
<bold>Table&#xa0;2</bold>
</xref>), in addition to their impact on survival following low-LET protons and X-rays, are shown. We focused our attention on candidate enzymes whose depletion led to a specific reduction in cell survival following high-LET radiation. This led us to identify that depletion of USP9X caused no reduction in cell survival after low-LET X-ray or proton irradiation, whereas survival after high-LET &#x3b1;-particles and protons was reduced by ~20% and&#xa0;~40%, respectively (<xref ref-type="table" rid="T1">
<bold>Tables&#xa0;1</bold>
</xref>, <xref ref-type="table" rid="T2">
<bold>2</bold>
</xref>).</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>siRNA screen of DUBs modulating cell survival following high and low LET radiation. HeLa cells were transfected with siRNA (pool of 4 oligonucleotides) targeting individual DUBs for 48&#xa0;h, and irradiated with either <bold>(A)</bold> 0.5 Gy &#x3b1;-particles or 1 Gy X-rays, or <bold>(B)</bold> 2 Gy relatively high-LET protons or 2 Gy low-LET protons. Clonogenic survival was analyzed from a single experiment (using triplicate samples) and normalized against the mock-treated control. Results are shown as a log<sub>2</sub> plot, and indicated is the clonogenic survival following USP9X depletion. Data has been adapted from (<xref ref-type="bibr" rid="B7">7</xref>).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fonc-11-671431-g001.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>Candidate DUBs whose siRNA-mediated depletion enhance radiosensitivity of cells in response to &#x3b1;-particle radiation.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left">DUB enzyme</th>
<th valign="top" align="center">&#x3b1;-particles</th>
<th valign="top" align="center">X-rays</th>
<th valign="top" align="center">High-LET protons</th>
<th valign="top" align="center">Low-LET protons</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">USP6</td>
<td valign="top" align="center">0.39</td>
<td valign="top" align="center">0.51<sup>*</sup>
</td>
<td valign="top" align="center">0.60</td>
<td valign="top" align="center">1.32</td>
</tr>
<tr>
<td valign="top" align="left">USP21</td>
<td valign="top" align="center">0.41</td>
<td valign="top" align="center">0.52</td>
<td valign="top" align="center">1.06</td>
<td valign="top" align="center">0.82</td>
</tr>
<tr>
<td valign="top" align="left">USP36</td>
<td valign="top" align="center">0.41</td>
<td valign="top" align="center">1.45</td>
<td valign="top" align="center">0.66</td>
<td valign="top" align="center">0.11</td>
</tr>
<tr>
<td valign="top" align="left">DUB3</td>
<td valign="top" align="center">0.49</td>
<td valign="top" align="center">2.00</td>
<td valign="top" align="center">0.90</td>
<td valign="top" align="center">1.89</td>
</tr>
<tr>
<td valign="top" align="left">STAMBPL1</td>
<td valign="top" align="center">0.52</td>
<td valign="top" align="center">0.67</td>
<td valign="top" align="center">0.72</td>
<td valign="top" align="center">0.31</td>
</tr>
<tr>
<td valign="top" align="left">UCHL3</td>
<td valign="top" align="center">0.56</td>
<td valign="top" align="center">0.59</td>
<td valign="top" align="center">1.69</td>
<td valign="top" align="center">0.33</td>
</tr>
<tr>
<td valign="top" align="left">AMSH</td>
<td valign="top" align="center">0.57</td>
<td valign="top" align="center">0.37</td>
<td valign="top" align="center">1.47</td>
<td valign="top" align="center">1.59</td>
</tr>
<tr>
<td valign="top" align="left">CYLD</td>
<td valign="top" align="center">0.57</td>
<td valign="top" align="center">0.79</td>
<td valign="top" align="center">0.47</td>
<td valign="top" align="center">1.76</td>
</tr>
<tr>
<td valign="top" align="left">UCHL5</td>
<td valign="top" align="center">0.57</td>
<td valign="top" align="center">0.64</td>
<td valign="top" align="center">1.51</td>
<td valign="top" align="center">0.54</td>
</tr>
<tr>
<td valign="top" align="left">OTUB1</td>
<td valign="top" align="center">0.58</td>
<td valign="top" align="center">1.55</td>
<td valign="top" align="center">1.99</td>
<td valign="top" align="center">0.61</td>
</tr>
<tr>
<td valign="top" align="left">
<bold>USP9X</bold>
</td>
<td valign="top" align="center">
<bold>0.80</bold>
</td>
<td valign="top" align="center">
<bold>0.90</bold>
</td>
<td valign="top" align="center">
<bold>0.60</bold>
</td>
<td valign="top" align="center">
<bold>1.50</bold>
</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>Surviving fractions from a single experiment containing triplicate samples were normalized against the mock-treated control, which was set to 1.0. Survival data acquired in response to USP9X depletion is highlighted in bold. <sup>*</sup>Previously identified as a false positive result, data adapted from (<xref ref-type="bibr" rid="B7">7</xref>).</p>
</fn>
</table-wrap-foot>
</table-wrap>
<table-wrap id="T2" position="float">
<label>Table&#xa0;2</label>
<caption>
<p>Candidate DUBs whose siRNA-mediated depletion enhance radiosensitivity of cells in response to high-LET protons.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left">DUB enzyme</th>
<th valign="top" align="center">High-LET protons</th>
<th valign="top" align="center">Low-LET protons </th>
<th valign="top" align="center">&#x3b1;-particles </th>
<th valign="top" align="center">X-rays</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">CYLD</td>
<td valign="top" align="center">0.47</td>
<td valign="top" align="center">1.76</td>
<td valign="top" align="center">0.57</td>
<td valign="top" align="center">0.79</td>
</tr>
<tr>
<td valign="top" align="left">USP7</td>
<td valign="top" align="center">0.50</td>
<td valign="top" align="center">0.21</td>
<td valign="top" align="center">1.30</td>
<td valign="top" align="center">1.02</td>
</tr>
<tr>
<td valign="top" align="left">USP31</td>
<td valign="top" align="center">0.59</td>
<td valign="top" align="center">0.38</td>
<td valign="top" align="center">n.d.</td>
<td valign="top" align="center">n.d.</td>
</tr>
<tr>
<td valign="top" align="left">
<bold>USP9X</bold>
</td>
<td valign="top" align="center">
<bold>0.60</bold>
</td>
<td valign="top" align="center">
<bold>1.50</bold>
</td>
<td valign="top" align="center">
<bold>0.80</bold>
</td>
<td valign="top" align="center">
<bold>0.90</bold>
</td>
</tr>
<tr>
<td valign="top" align="left">USP6</td>
<td valign="top" align="center">0.60</td>
<td valign="top" align="center">1.32</td>
<td valign="top" align="center">0.39</td>
<td valign="top" align="center">0.51<sup>*</sup>
</td>
</tr>
<tr>
<td valign="top" align="left">USP36</td>
<td valign="top" align="center">0.66</td>
<td valign="top" align="center">0.11</td>
<td valign="top" align="center">0.41</td>
<td valign="top" align="center">1.45</td>
</tr>
<tr>
<td valign="top" align="left">USP39</td>
<td valign="top" align="center">0.67</td>
<td valign="top" align="center">0.04</td>
<td valign="top" align="center">n.d.</td>
<td valign="top" align="center">2.64</td>
</tr>
<tr>
<td valign="top" align="left">STAMBPL1</td>
<td valign="top" align="center">0.72</td>
<td valign="top" align="center">0.31</td>
<td valign="top" align="center">0.52</td>
<td valign="top" align="center">0.67</td>
</tr>
<tr>
<td valign="top" align="left">USP43</td>
<td valign="top" align="center">0.74</td>
<td valign="top" align="center">0.11</td>
<td valign="top" align="center">n.d.</td>
<td valign="top" align="center">n.d.</td>
</tr>
<tr>
<td valign="top" align="left">YOD1</td>
<td valign="top" align="center">0.77</td>
<td valign="top" align="center">0.22</td>
<td valign="top" align="center">0.78</td>
<td valign="top" align="center">0.90</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>Surviving fractions from a single experiment containing triplicate samples were normalized against the mock-treated control, which was set to 1.0. n.d. indicates not determined. Survival data acquired in response to USP9X depletion is highlighted in bold. <sup>*</sup>Previously identified as a false positive result, data adapted from (<xref ref-type="bibr" rid="B7">7</xref>).</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
<sec id="s3_2">
<title>USP9X Modulates Cell Survival in Response to High-LET IR</title>
<p>Following siRNA screening, we aimed to validate that depletion of USP9X caused a decrease in cell survival following high-LET radiation, but had no impact in response to low-LET protons, in both HeLa cells and also cells derived from head and neck squamous cell carcinoma. In response to USP9X siRNA (pool of 4 siRNAs utilized in the screen), there was no impact on cell survival following a dose titration of low-LET X-rays (<xref ref-type="fig" rid="f2">
<bold>Figures&#xa0;2A, B</bold>
</xref>) or low-LET protons (<xref ref-type="fig" rid="f2">
<bold>Figures&#xa0;2E, F</bold>
</xref>) in comparison to non-targeting (NT) control siRNA-treated cells. In fact, depletion of USP9X appeared to cause a mild increase in radioresistance following low-LET protons. However, in contrast to low-LET radiation, USP9X siRNA led to reduced survival in response to high-LET &#x3b1;-particles (<xref ref-type="fig" rid="f2">
<bold>Figures&#xa0;2C, D</bold>
</xref>), and more dramatically in response to relatively high-LET protons (<xref ref-type="fig" rid="f2">
<bold>Figures&#xa0;2G, H</bold>
</xref>). To further validate that our observations were specific, we utilized two single siRNA sequences (USP9X_6 and USP9X_8) that were demonstrated to be effective in suppressing USP9X protein levels in both HeLa (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3A</bold>
</xref>) and UMSCC74A oropharyngeal squamous cell carcinoma cells (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3B</bold>
</xref>). We focused on the impact of protons, particularly as PBT is employed clinically for the treatment of tumors, including head and neck squamous cell carcinoma. We confirmed that targeting USP9X had no effect on the survival of HeLa cells (<xref ref-type="fig" rid="f3">
<bold>Figures&#xa0;3C, D</bold>
</xref>) or UMSCC74 cells (<xref ref-type="fig" rid="f3">
<bold>Figures&#xa0;3G, H</bold>
</xref>) following low-LET protons, in comparison to NT control siRNA-treated cells. However, significantly reduced survival of HeLa (<xref ref-type="fig" rid="f3">
<bold>Figures&#xa0;3E, F</bold>
</xref>) and UMSCC74A (<xref ref-type="fig" rid="f3">
<bold>Figures&#xa0;3I, J</bold>
</xref>) cells was observed following USP9X depletion in response to high-LET protons, compared with NT control siRNA cells. These data confirmed the importance of USP9X in maintaining cell survival following treatment with relatively high-LET protons.</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>Validation of USP9X in enhancing cellular radiosensitivity in response to high-LET &#x3b1;-particles and protons. HeLa cells were treated with USP9X siRNA (pool of 4 oligonucleotides) or a non-targeting (NT) control siRNA for 48&#xa0;h and irradiated with increasing doses of <bold>(A, B)</bold> X-rays, <bold>(C, D)</bold> &#x3b1;-particles, <bold>(E, F)</bold> low-LET protons, or <bold>(G, H)</bold> relatively high-LET protons. Clonogenic survival of cells was analyzed from 2 independent experiments, and shown is the mean surviving fraction &#xb1; S.E. (<bold>B, D, F, H</bold>) Shown are representative images of colonies in non-irradiated and irradiated plates, the latter of which contained four times the number of cells seeded.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fonc-11-671431-g002.tif"/>
</fig>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>Specific targeting of USP9X leads to enhanced cellular radiosensitivity after relatively high-LET protons. <bold>(A&#x2013;J)</bold> Cells were treated with individual USP9X siRNAs (USP9X_6 and USP9X_8) or a non-targeting (NT) control siRNA for 48&#xa0;h. Whole cell extracts prepared from <bold>(A)</bold> HeLa or <bold>(B)</bold> UMSCC74A cells were analyzed by immunoblotting using USP9X or tubulin antibodies. HeLa cells were subsequently irradiated with increasing doses of <bold>(C, D)</bold> low-LET protons or <bold>(E, F)</bold> relatively high-LET protons. UMSCC74A cells were also treated with increasing doses of <bold>(G, H)</bold> low-LET protons or <bold>(I, J)</bold> relatively high-LET protons. Clonogenic survival of cells was analyzed from 3 independent experiments, and shown is the mean surviving fraction &#xb1; S.E. Shown are representative images of colonies from <bold>(D, F)</bold> HeLa cells or <bold>(H, J)</bold> UMSCC74A cells in non-irradiated and irradiated plates, the latter of which contained four times the number of cells seeded. A comparison of the surviving fractions at 2 Gy (SF2) by one-way ANOVA in HeLa cells reveals p &lt; 0.05 (NT siRNA <italic>vs</italic> USP9X_6), p &lt; 0.001 (NT siRNA <italic>vs</italic> USP9X_8) and in UMSCC74A cells, p &lt; 0.05 (NT siRNA <italic>vs</italic> USP9X_6 and NT siRNA <italic>vs</italic> USP9X_8). At 4 Gy (SF4), one-way ANOVA values in HeLa cells are p &lt; 0.01 (NT siRNA <italic>vs</italic> USP9X_6), p &lt; 0.005 (NT siRNA <italic>vs</italic> USP9X_8) and in UMSCC74A cells, p &lt; 0.05 (NT siRNA <italic>vs</italic> USP9X_6 and NT siRNA <italic>vs</italic> USP9X_8).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fonc-11-671431-g003.tif"/>
</fig>
</sec>
<sec id="s3_3">
<title>USP9X Does Not Interfere With CDD Repair or Cell Cycle Progression Following High-LET Protons</title>
<p>Given our demonstration that USP9X is required for maintaining cell survival specifically in response to relatively high-LET protons, we sought to define its mechanism of action. In the first instance, and given the propensity for high-LET radiation to cause increases in the levels of CDD, we utilized an enzyme-modified neutral comet assay (<xref ref-type="bibr" rid="B34">34</xref>) to monitor the levels and kinetics of repair of CDD. This assay also has the added advantage of revealing the levels and repair of DNA DSBs (in the absence of modifying enzymes). We demonstrate that DNA DSB levels are not significantly different in USP9X siRNA <italic>versus</italic> NT control siRNA-treated cells in response to relatively high-LET protons at any time points (0-4&#xa0;h) post-irradiation (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4A</bold>
</xref>; compare black and red, and <xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4B</bold>
</xref>). We were able to confirm that relatively high-LET protons caused a significant increase in the levels of CDD in NT control siRNA-treated cells immediately post-irradiation, followed by significantly slower kinetics of repair from 1 to 4&#xa0;h post-irradiation (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4A</bold>
</xref>; compare black and grey bars, and <xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4B</bold>
</xref>), consistent with our previously published data (<xref ref-type="bibr" rid="B6">6</xref>, <xref ref-type="bibr" rid="B7">7</xref>). Following depletion of USP9X, we observed that the efficiency of CDD repair in comparison to NT control siRNA-treated cells was not significantly different, at least at 1 to 4&#xa0;h post-irradiation (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4A</bold>
</xref>; compare grey and orange bars, and <xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4B</bold>
</xref>). Data, demonstrating a lack of effect of USP9X depletion on the repair of DNA DSBs induced by relatively high-LET protons, were supported by an absence of any differences in the induction and resolution of &#x3b3;H2AX and 53BP1 foci, as surrogate markers, up to 8&#xa0;h post-irradiation relative to NT control siRNA-treated cells (<xref ref-type="fig" rid="f4">
<bold>Figures&#xa0;4C, D</bold>
</xref>
<bold>)</bold>. We also analyzed the progression of cells through the cell cycle post-irradiation. Similarly, this revealed no significant differences in G2/M accumulation in USP9X siRNA-treated cells either before or after high-LET proton irradiation compared to NT control siRNA-treated cells (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4E</bold>
</xref>), or in the overall cell cycle profiles (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4G</bold>
</xref>). Similar numbers of cells in G2/M phase (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4F</bold>
</xref>) and in cell cycle profiles (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4H</bold>
</xref>) were also observed in USP9X-depleted and NT control siRNA-treated cells in response to low-LET protons. These data suggest that there is no significantly different checkpoint activation or cell cycle arrest in USP9X-depleted cells following either relatively high- or low-LET protons.</p>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>USP9X depletion does not affect the repair of CDD or cell cycle progression in response to relatively high-LET protons. HeLa cells were treated with USP9X or a non-targeting (NT) control siRNA for 48&#xa0;h. <bold>(A)</bold> Cells were irradiated with 4 Gy relatively high-LET protons, and DNA damage measured at various time points post-irradiation using the enzyme-modified neutral comet assay in the absence (revealing DSBs) or presence (revealing CDD; as indicated by mod) of the recombinant enzymes APE1, NTH1, and OGG1. Shown is the mean percentage tail DNA &#xb1; S.D plus <bold>(B)</bold> representative images of comets. *p &lt; 0.02, **p &lt; 0.005, ***p &lt; 0.002 as analyzed by a one-sample <italic>t</italic>-test. <bold>(C)</bold> &#x3b3;H2AX or <bold>(D)</bold> 53BP1 foci were analyzed by immunofluorescence staining at various time points post-irradiation. Shown is the mean number of foci/nucleus &#xb1; S.D. <bold>(E&#x2013;H)</bold> Cell cycle profiles were determined by flow cytometry analysis post-irradiation with <bold>(E, G)</bold> high-LET or <bold>(F, H)</bold> low-LET protons. C refers to control, unirradiated cells. <bold>(E, F)</bold> Shown is the mean percentage of cells in G2/M phase &#xb1; S.E.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fonc-11-671431-g004.tif"/>
</fig>
</sec>
<sec id="s3_4">
<title>USP9X Does Not Impact Apoptosis, Autophagy or Senescence Following High-LET Protons</title>
<p>To examine the potential impact of USP9X on triggering apoptosis post-irradiation with relatively high-LET protons, we analyzed the cellular protein levels of PARP-1 (including cleaved PARP-1) and Mcl-1. However, we did not observe any differences in these proteins 1 to 24&#xa0;h post-irradiation, nor in the accumulation of cleaved PARP-1, in USP9X siRNA-treated cells compared to NT control siRNA-treated cells (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5A</bold>
</xref>), suggesting that apoptosis does not play a role in the differential cellular response. We also compared the expression of LC3B (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5B</bold>
</xref>; red text refers to time following relatively high-LET protons) and &#x3b2;-Galactosidase by both microscopy (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5C</bold>
</xref>; utilizing H2O2 as a positive control) and immunoblotting (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5D</bold>
</xref>), as markers of autophagy and senescence, respectively. Similarly, we observed no obvious differences in LC3B or &#x3b2;-galactosidase levels between USP9X-depleted and NT control siRNA-treated cells post-irradiation with either relatively high- or low-LET protons, suggesting that neither autophagy nor senescence are responsible for decreased cell survival specifically following relatively high-LET protons.</p>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>USP9X depletion does not affect cellular levels of apoptosis, autophagy and senescence in response to relatively high-LET protons. HeLa cells were treated with USP9X or a non-targeting (NT) control siRNA for 48&#xa0;h, and unirradiated (designated C) or irradiated with 4 Gy relatively high-LET or low-LET protons and allowed to repair for the time points indicated post-irradiation. <bold>(A, B, D)</bold> Whole cell extracts were analyzed by immunoblotting using the indicated antibodies. <bold>(C)</bold> Cells were fixed 48&#xa0;h post-irradiation and stained for &#x3b2;-Galactosidase, with 100 &#xb5;M H<sub>2</sub>O<sub>2</sub> used as a positive control.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fonc-11-671431-g005.tif"/>
</fig>
</sec>
<sec id="s3_5">
<title>USP9X Inhibition Causes Amplification of Pericentrin-Rich Bodies After High-LET Protons</title>
<p>Since recent data have shown that USP9X is an integral component of centrosomal protein maintenance, we analyzed the impact of USP9X depletion on stabilization of centrosomal proteins. We observed that an absence of USP9X alone in HeLa cells caused reduced levels of the centrosome proteins CEP55 (~60%) and CEP131 (~40%) in comparison to NT control siRNA-treated cells (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6A</bold>
</xref>; compare lanes 1 and 4). Reduced levels of CEP55 and CEP131 (by ~50&#x2013;60%) were maintained in USP9X-depleted cells 24&#xa0;h post-irradiation with both low- and high-LET protons (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6A</bold>
</xref>; compare lanes 2&#x2013;3 and 5&#x2013;6). Similar observations were seen in UMSCC74A cells, whereby CEP55 and CEP131 protein levels were reduced by 50% and 30%, respectively, in USP9X-depleted cells (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6B</bold>
</xref>; compare lanes 1 and 4). CEP55 and CEP131 protein levels were further reduced (by ~60&#x2013;90%) in USP9X-depleted cells compared to NT control siRNA-treated cells 24&#xa0;h post-irradiation with both low- and high-LET protons (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6B</bold>
</xref>; compare lanes 2&#x2013;3 and 5&#x2013;6). In addition to reduced centrosome protein stability, we discovered a ~2.6- to 2.9-fold increase in pericentrin-rich foci in NT control siRNA-treated HeLa cells 48&#xa0;h post-irradiation with both low and high LET protons (<xref ref-type="fig" rid="f6">
<bold>Figures&#xa0;6C, D</bold>
</xref>
<bold>)</bold>. However, we observed that there was an additional ~1.9-fold statistically significant increase in foci in USP9X-depleted cells specifically in response to high-LET protons, but not following low-LET protons (<xref ref-type="fig" rid="f6">
<bold>Figures&#xa0;6C, D</bold>
</xref>
<bold>)</bold>. Similarly, in UMSCC74A cells, there was a ~1.8-fold increase in pericentrin-rich foci in NT control siRNA-treated HeLa cells 48&#xa0;h post-irradiation with both low- and high-LET protons, but this further increased by ~2.2-fold in USP9X-depleted cells (<xref ref-type="fig" rid="f6">
<bold>Figures&#xa0;6E, F</bold>
</xref>
<bold>)</bold>. Amplification of pericentrin-foci was consequently ~6.7-fold (HeLa) and ~4.9-fold (UMSCC74A) higher in USP9X-depleted cells irradiated with high-LET protons compared with unirradiated cells.</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>USP9X depletion destabilizes centrosomal proteins, and induces pericentrin-rich foci amplification in response to relatively high-LET protons. <bold>(A, C, D)</bold> HeLa or <bold>(B, E, F)</bold> UMSCC74A cells were treated with USP9X or a non-targeting (NT) control siRNA for 48&#xa0;h, and unirradiated designated <bold>(C)</bold> or irradiated with 4 Gy relatively high-LET or low-LET protons and allowed to repair for the time points indicated post-irradiation. <bold>(A, B)</bold> Whole cell extracts were analyzed by immunoblotting using the indicated antibodies. Red and black text refers to time post-irradiation following relatively high-LET and low-LET protons, respectively. Protein levels of CEP131 and CEP55 relative to tubulin and normalized to the unirradiated NT siRNA control treated cells which was set to 1.0 are shown. <bold>(C, E)</bold> Analysis of pericentrin was performed by immunofluorescence 48&#xa0;h post-irradiation. Shown is the mean percentage of cells with &gt;2 pericentrin-rich foci/nucleus &#xb1; S.D. *p &lt; 0.03 as analyzed by a two-sample <italic>t</italic>-test. <bold>(D, F)</bold> Representative images of pericentrin staining (green stain) and nuclei (blue stain; DAPI).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fonc-11-671431-g006.tif"/>
</fig>
<p>To recapitulate the impact of USP9X in controlling sensitivity of cells to high-LET protons mediated <italic>via</italic> centrosomal protein maintenance, we specifically targeted CEP55 and CEP131 using siRNA. We identified conditions that led to ~50% reduced CEP55 and CEP131 protein levels in HeLa cells (<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7A</bold>
</xref>; lanes 4 and 8), which mimic those of USP9X depletion (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6A</bold>
</xref>). We observed under these conditions that cells do not display any increase in radiosensitivity to low-LET protons (<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7B</bold>
</xref>), but that there is reduced survival to relatively high-LET protons (<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7C</bold>
</xref>). Additionally, we discovered that there was an a ~1.4-fold statistically significant increase in pericentrin-rich foci in USP9X-depleted cells <italic>versus</italic> NT control siRNA-treated cells specifically in response to high-LET protons, but not following low-LET protons (<xref ref-type="fig" rid="f7">
<bold>Figures&#xa0;7D, E</bold>
</xref>
<bold>)</bold>. This suggests that USP9X is required for maintenance of centrosomal proteins and for controlling pericentrin-rich foci, which is important for cell survival particularly in response to high-LET radiation.</p>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>
<p>CEP55 and CEP131 depletion induces pericentrin-rich foci amplification and reduces cell survival in response to relatively high-LET protons. <bold>(A)</bold> HeLa cells were treated with CEP55 or CEP131 siRNA (0.01, 0.1 and 1 nM) or a non-targeting (NT) control siRNA for 48&#xa0;h, and whole cell extracts were analyzed by immunoblotting using the indicated antibodies. Protein levels of CEP131 and CEP55 relative to tubulin and normalized to the NT siRNA control-treated cells which was set to 1.0 are shown. <bold>(B&#x2013;E)</bold> HeLa cells were treated with CEP55 and CEP131 siRNA (0.01 nM) or a non-targeting (NT) control siRNA for 48&#xa0;h. Cells were irradiated with increasing doses of <bold>(B)</bold> low-LET protons or <bold>(C)</bold> relatively high-LET protons. Clonogenic survival of cells was analyzed from 2 independent experiments, and shown is the mean surviving fraction &#xb1; S.E. <bold>(D, E)</bold> Alternatively, analysis of pericentrin was performed by immunofluorescence 48&#xa0;h post-irradiation (with 4 Gy). <bold>(D)</bold> Shown is the mean percentage of cells with &gt;2 pericentrin-rich foci/nucleus &#xb1; S.D. *p &lt; 0.05 as analyzed by a two-sample <italic>t</italic>-test. <bold>(E)</bold> Representative images of pericentrin staining (green stain) and nuclei (blue stain; DAPI).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fonc-11-671431-g007.tif"/>
</fig>
</sec>
</sec>
<sec id="s4" sec-type="discussion">
<title>Discussion</title>
<p>IR, particularly at high-LET, can generate CDD known to compromise genome integrity and to contribute to cell death due to the inability of the cellular DNA repair machinery to accurately repair the damage. However, high-LET radiation has also been shown to promote persistent alterations to the structure of chromatin (<xref ref-type="bibr" rid="B9">9</xref>, <xref ref-type="bibr" rid="B10">10</xref>), and to enhance senescence and apoptosis (<xref ref-type="bibr" rid="B11">11</xref>, <xref ref-type="bibr" rid="B12">12</xref>). We recently demonstrated using a DUB siRNA screen, that depletion of USP6 causes significantly increased radiosensitivity to high-LET IR (relatively high-LET protons and &#x3b1;-particles) but not low-LET IR (protons or X-rays), which was mediated by instability of PARP-1 required for CDD repair (<xref ref-type="bibr" rid="B7">7</xref>). In the current study, we discovered that another DUB enzyme, USP9X, is similarly required for maintaining cell survival specifically in response to high-LET IR, particularly high-LET protons. We demonstrated that this phenotype was not caused by interference with CDD repair, cell cycle progression, apoptosis, autophagy or senescence. In fact, we discovered that an absence of USP9X caused destabilization of centrosomal proteins, and enhanced amplification of pericentrin-rich foci in response to relatively high-LET protons. This suggests that maintenance of CEP55 and CEP131 is the major factor contributing to reduced cell survival following relatively high-LET protons in the absence of USP9X.</p>
<p>Our findings that USP9X does not affect cell cycle progression is in agreement with a previous study, which demonstrated that USP9X depletion was linked to an increased loss of anaphase-promoting complex/cyclosome (APC/C) substrates, in particular cyclin A, but also cyclin B and NEK2A, and that cells consequently failed to arrest mitosis after microtubule poisoning in HeLa cells and U2OS cells (<xref ref-type="bibr" rid="B35">35</xref>). USP9X has been shown to promote Mcl-1 stabilization and to increase tumor cell survival in response to radiation and chemotherapy in several tumor types (<xref ref-type="bibr" rid="B19">19</xref>, <xref ref-type="bibr" rid="B36">36</xref>&#x2013;<xref ref-type="bibr" rid="B39">39</xref>). This is in contrast to our findings, where we observed no evidence of a role for Mcl-1, and therefore apoptosis through lack of PARP-1 cleavage, in the USP9X-dependent radiosensitisation of HeLa and UMSCC74A cells following relatively high-LET protons. Indeed, in certain glioblastoma cell lines, it has been demonstrated that USP9X loss regulates radiosensitivity by Mcl-1-independent mechanisms (<xref ref-type="bibr" rid="B40">40</xref>). USP9X interacts with VMP1, indicating that there is a close cooperation between the autophagy pathway and the ubiquitin recognition machinery required for selective autophagosome formation (<xref ref-type="bibr" rid="B41">41</xref>). On analysis of the levels of LC3B, as a marker of autophagy, after relatively high-LET <italic>versus</italic> low-LET protons, we did not find any evidence indicating that autophagy plays a significant role in cell survival in response to these conditions. USP9X has recently been suggested to stabilize the breast cancer protein-1 (BRCA1) required for DSB repair by homologous recombination through its DUB enzymatic activity, and which is required for resistance to the PARP inhibitor olaparib in HeLa and breast cancer cells (<xref ref-type="bibr" rid="B42">42</xref>). These data are supported by another study, although it was proposed that USP9X actually regulates BRCA1 (and RAD51) at the transcriptional level in U2OS cells, which was independent of its catalytic activity (<xref ref-type="bibr" rid="B43">43</xref>). This study also presented limited data showing increased levels of 53BP1 foci both in the absence and presence of IR (1&#xa0;h post-irradiation), in USP9X-depleted cells. Despite this evidence, we observed that an absence of USP9X did not cause any significant differences in the repair of DSBs, using &#x3b3;H2AX and 53BP1 foci analysis, or in the kinetics of DSB or CDD repair after relatively high-LET protons. This would indicate that the ability of the cells, at least the ones utilized in our study (HeLa and UMSCC74A), to repair DNA damage was not heavily compromised.</p>
<p>USP9X has more recently been observed in U2OS and HeLa cells to localize to centrosomes in association with PCM1, CEP55 and CEP131, where the enzyme antagonizes proteosomal degradation of these key centriolar satellite proteins to promote centrosome duplication (<xref ref-type="bibr" rid="B21">21</xref>&#x2013;<xref ref-type="bibr" rid="B23">23</xref>). Interestingly, in MRXS99F fibroblasts USP9X was also found to localize to the centrosome, but had no impact on controlling the protein levels of PCM1 or CEP131 (<xref ref-type="bibr" rid="B24">24</xref>). This suggests that there are cell-type&#x2013;specific roles and targets for USP9X. Here, we observed that USP9X-depleted HeLa and UMSCC74A oropharyngeal squamous cell carcinoma cells have reduced levels of CEP55 and CEP131. Furthermore, we observed an increased number of pericentrin-rich foci after proton irradiation in both non-targeting and USP9X-depleted cells, but that this phenotype was further exacerbated specifically after high-LET protons in USP9X-depleted cells. We also targeted CEP55 and CEP131 directly and demonstrated that their moderate depletion (by&#xa0;~50%, consistent with effects seen following USP9X depletion) also led to amplification of pericentrin-rich foci and enhanced sensitivity of cells specifically to high LET protons. Pericentrin is not only a component of centrosomes but also a feature of centriolar satellites and cilia, which are associated with centrosome biology. Our data therefore indicate that USP9X could play a role in centriolar satellite generation, which ultimately maintains centrosome stability. Centriolar satellites are small, granular structures that cluster around centrosomes and are thought to play important roles in both centrosome assembly and in cilia formation (<xref ref-type="bibr" rid="B44">44</xref>, <xref ref-type="bibr" rid="B45">45</xref>). There is also evidence demonstrating that cellular stresses, such as UV radiation, disrupt centriolar satellites and stimulate ciliogenesis (<xref ref-type="bibr" rid="B46">46</xref>). Furthermore, and consistent with our data, DNA damage induction by IR and bleomycin has been shown to lead to excessive formation of centriolar satellites, which is a prerequisite for centrosome amplification (<xref ref-type="bibr" rid="B47">47</xref>). It is possible, therefore, that following high-LET protons, which is more densely ionizing leading to increased protein as well as DNA damage, there is uncontrolled centrosome biogenesis, which is likely to contribute to increased genome instability through chromosomal aberrations and therefore reduced cell survival. It is important to note that the UMSCC74A cells employed in our study contain wild type p53 tumor suppressor protein, whereas HeLa cells have significantly reduced levels of p53 due to human papillomavirus type 18 infection that ultimately leads to p53 degradation. The phenotype of increased radiosensitivity and elevated levels of pericentrin-rich foci in cells in response to high-LET radiation therefore does not appear to be dependent on loss of p53. Given that p53 is frequently mutated in human cancers, and particularly in head and neck squamous cell carcinoma (<xref ref-type="bibr" rid="B48">48</xref>), more expansive studies using cells containing different p53 status are required to fully investigate this. Nevertheless, and at this stage, the precise mechanism underlying the impact of USP9X in regulating centrosome biology specifically in response to relatively high-LET protons is unclear. Further ongoing experiments are necessary to fully understand centrosome biology (&gt;100 centrosome proteins exist) in multiple cell lines lacking USP9X pre- and post-irradiation, particularly those originating from head and neck cancers, which is our research and clinical focus. We also aim to analyze more the impact of low- <italic>versus</italic> high-LET radiation at the chromosome level, and the dependence on USP9X, which is likely to be contributing to the increased radiosensitivity of cells lacking USP9X specifically in response high-LET radiation. Nevertheless, our data suggest that USP9X is essential for maintaining cell survival, particularly following high-LET radiation.</p>
</sec>
<sec id="s5">
<title>Data Availability Statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>JP conceptualized and designed the project. AK, MH, and JP designed the experimental setup. CN, MF, RC, and JH performed experiments. CN, MF, RC, and JP performed data analysis and validation. CN, MF, RC, and JP wrote the manuscript and all authors contributed to reviewing and editing. JP and MH coordinated funding acquisition. All authors contributed to the article and approved the submitted version.</p>
</sec>
<sec id="s7" sec-type="funding-information">
<title>Funding</title>
<p>This research was funded by North West Cancer Research (CR1074 and CR1197) and by the Medical Research Council <italic>via</italic> a New Investigator Research Grant (MR/M000354/1) awarded to JP. Funding from Medical Research Council Strategic Partnership Funding (MC-PC-12004) for the CRUK/MRC Oxford Institute for Radiation Oncology is also gratefully acknowledged.</p>
</sec>
<sec id="s8" sec-type="COI-statement">
<title>Conflict of Interest</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>
</body>
<back>
<ack>
<title>Acknowledgments</title>
<p>The authors thank Prof T. Carey for providing the UMSCC74A cells and Prof G. Dianov for providing APE1, NTH1, and OGG1 bacterial expression plasmids. The authors also thank Brian Marsland and Ian Taylor at the Clatterbridge Cancer Centre for technical assistance with proton irradiation of cells, and Dr Urszula McClurg for critically reviewing the manuscript.</p>
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