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dc.contributor.authorGraen, Timo
dc.contributor.authorInhester, Ludger
dc.contributor.authorClemens, Maike
dc.contributor.authorGrubmüller, Helmut
dc.contributor.authorGroenhof, Gerrit
dc.date.accessioned2017-01-11T11:08:55Z
dc.date.available2017-01-11T11:08:55Z
dc.date.issued2016
dc.identifier.citationGraen, T., Inhester, L., Clemens, M., Grubmüller, H., & Groenhof, G. (2016). The Low Barrier Hydrogen Bond in the Photoactive Yellow Protein : A Vacuum Artifact Absent in the Crystal and Solution. <i>Journal of the American Chemical Society</i>, <i>138</i>(51), 16620-16631. <a href="https://doi.org/10.1021/jacs.6b05609" target="_blank">https://doi.org/10.1021/jacs.6b05609</a>
dc.identifier.otherCONVID_26396020
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/52698
dc.description.abstractThere has been considerable debate on the existence of a low-barrier hydrogen bond (LBHB) in the photoactive yellow protein (PYP). The debate was initially triggered by the neutron diffraction study of Yamaguchi et al. (Proc. Natl. Acad. Sci., U. S. A., 2009, 106, 440−444) who suggested a model in which a neutral Arg52 residue triggers the formation of the LBHB in PYP. Here, we present an alternative model that is consistent within the error margins of the Yamaguchi structure factors. The model explains an increased hydrogen bond length without nuclear quantum effects and for a protonated Arg52. We tested both models by calculations under crystal, solution, and vacuum conditions. Contrary to the common assumption in the field, we found that a single PYP in vacuum does not provide an accurate description of the crystal conditions but instead introduces strong artifacts, which favor a LBHB and a large 1 H NMR chemical shift. Our model of the crystal environment was found to stabilize the two Arg52 hydrogen bonds and crystal water positions for the protonated Arg52 residue in free MD simulations and predicted an Arg52 pKa upshift with respect to PYP in solution. The crystal and solution environments resulted in almost identical 1 H chemical shifts that agree with NMR solution data. We also calculated the effect of the Arg52 protonation state on the LBHB in 3D nuclear equilibrium density calculations. Only the charged crystal structure in vacuum supports a LBHB if Arg52 is neutral in PYP at the previously reported level of theory (J. Am. Chem. Soc., 2014, 136, 3542−3552). We attribute the anomalies in the interpretation of the neutron data to a shift of the potential minimum, which does not involve nuclear quantum effects and is transferable beyond the Yamaguchi structure.
dc.language.isoeng
dc.publisherAmerican Chemical Society
dc.relation.ispartofseriesJournal of the American Chemical Society
dc.subject.otherphotoactive yellow protein
dc.subject.otherlow-barrier hydrogen bond
dc.titleThe Low Barrier Hydrogen Bond in the Photoactive Yellow Protein : A Vacuum Artifact Absent in the Crystal and Solution
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-201701021004
dc.contributor.laitosKemian laitosfi
dc.contributor.laitosDepartment of Chemistryen
dc.contributor.oppiaineFysikaalinen kemiafi
dc.contributor.oppiaineNanoscience Centerfi
dc.contributor.oppiainePhysical Chemistryen
dc.contributor.oppiaineNanoscience Centeren
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2017-01-02T07:15:11Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.format.pagerange16620-16631
dc.relation.issn0002-7863
dc.relation.numberinseries51
dc.relation.volume138
dc.type.versionpublishedVersion
dc.rights.copyright© 2016 American Chemical Society. This is an open access article published under an ACS AuthorChoice License, which permits copying and redistribution of the article or any adaptations for non-commercial purposes.
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
dc.relation.grantnumber292820
dc.subject.ysovetysidokset
jyx.subject.urihttp://www.yso.fi/onto/yso/p38131
dc.rights.urlhttp://pubs.acs.org/page/policy/authorchoice_termsofuse.html
dc.relation.doi10.1021/jacs.6b05609
dc.relation.funderSuomen Akatemiafi
dc.relation.funderResearch Council of Finlanden
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundinginformationGG is supported by the Academy of Finland grant 292820. TG was supported by the MPG (International Max Planck Research School - Physics of Biological and Complex Systems). LI was supported by the DFG SFB755. MC was supported by the Volkswagen Foundation grant 83940. We thank Dr. Heikki Takala for valuable discussions. We thank Dr. Mehdi Davari for his contributions at the start of the project.
dc.type.okmA1


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Except where otherwise noted, this item's license is described as © 2016 American Chemical Society. This is an open access article published under an ACS AuthorChoice License, which permits copying and redistribution of the article or any adaptations for non-commercial purposes.