Role of helicity in DNA hairping folding dynamics
We study hairpin folding dynamics by means of extensive computer simulations, with particular attention paid to the influence of helicity on the folding time \(\tau\). We find that the dynamical exponent \(\alpha\) of the anomalous scaling \(\tau \sim N^\alpha\) for a hairpin with length N changes f...
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description | We study hairpin folding dynamics by means of extensive computer simulations, with particular attention paid to the influence of helicity on the folding time \(\tau\). We find that the dynamical exponent \(\alpha\) of the anomalous scaling \(\tau \sim N^\alpha\) for a hairpin with length N changes from 1.6 (\(1+\nu\)) to 1.2 (\(2\nu\)) in three dimensions, when duplex helicity is removed. The relation \(\alpha = 2\nu\) in rotationless hairpin folding is further verified in two dimensions (\(\nu = 0.75\)), and for a ghost-chain (\(\nu = 0.5\)). This, to our knowledge, is the first observation of the theoretical lower bound on \(\alpha\), which was predicted earlier on the basis of energy conservation for polymer translocation through a pore. Our findings suggest that the folding dynamics in long helical chains is governed by the duplex dynamics, contrasting the earlier understanding based on the stem-flower picture of unpaired segments. We propose a scaling argument for \(\alpha = 1+\nu\) in helical chains, assuming that duplex relaxation required for orientational positioning of the next pair of bases is the rate-limiting process. |
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We find that the dynamical exponent \(\alpha\) of the anomalous scaling \(\tau \sim N^\alpha\) for a hairpin with length N changes from 1.6 (\(1+\nu\)) to 1.2 (\(2\nu\)) in three dimensions, when duplex helicity is removed. The relation \(\alpha = 2\nu\) in rotationless hairpin folding is further verified in two dimensions (\(\nu = 0.75\)), and for a ghost-chain (\(\nu = 0.5\)). This, to our knowledge, is the first observation of the theoretical lower bound on \(\alpha\), which was predicted earlier on the basis of energy conservation for polymer translocation through a pore. Our findings suggest that the folding dynamics in long helical chains is governed by the duplex dynamics, contrasting the earlier understanding based on the stem-flower picture of unpaired segments. We propose a scaling argument for \(\alpha = 1+\nu\) in helical chains, assuming that duplex relaxation required for orientational positioning of the next pair of bases is the rate-limiting process.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1806.08609</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Computer simulation ; Deoxyribonucleic acid ; DNA ; Dynamics ; Energy conservation ; Folding ; Helicity ; Lower bounds ; Physics - Biological Physics ; Quantitative Biology - Biomolecules ; Scaling</subject><ispartof>arXiv.org, 2018-06</ispartof><rights>2018. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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We propose a scaling argument for \(\alpha = 1+\nu\) in helical chains, assuming that duplex relaxation required for orientational positioning of the next pair of bases is the rate-limiting process.</description><subject>Computer simulation</subject><subject>Deoxyribonucleic acid</subject><subject>DNA</subject><subject>Dynamics</subject><subject>Energy conservation</subject><subject>Folding</subject><subject>Helicity</subject><subject>Lower bounds</subject><subject>Physics - Biological Physics</subject><subject>Quantitative Biology - Biomolecules</subject><subject>Scaling</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj11rwjAYRsNgMHH-AK8W2HW7N59NLsV9OJANxPuSNMmM1LZLdaz_flV3dW4OD89BaE4g50oIeDLpN_7kRIHMQUnQN2hCGSOZ4pTeoVnf7wGAyoIKwSaIbNra4zbgna9jFY8Djg1-_ljgnYmpi80XDm3tznRDYw6x6u_RbTB172f_nKLt68t2ucrWn2_vy8U6M4LqTFrLJRNEWuKCogqs0lpyVnjCOA8EnJBgubYuFIpxWSkvHLdVYNaOFcCm6OE6e-kpuxQPJg3luau8dI3G49XoUvt98v2x3Len1IyfSgoFEwXnWrM_ZOxOAA</recordid><startdate>20180622</startdate><enddate>20180622</enddate><creator>Li, Huaping</creator><creator>Alkan Kabakcioglu</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>ALC</scope><scope>GOX</scope></search><sort><creationdate>20180622</creationdate><title>Role of helicity in DNA hairping folding dynamics</title><author>Li, Huaping ; Alkan Kabakcioglu</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a529-6bb463516b1df8280b8996437e1344f10d560b49bdf78346c8e5d4bcf3bb55003</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Computer simulation</topic><topic>Deoxyribonucleic acid</topic><topic>DNA</topic><topic>Dynamics</topic><topic>Energy conservation</topic><topic>Folding</topic><topic>Helicity</topic><topic>Lower bounds</topic><topic>Physics - Biological Physics</topic><topic>Quantitative Biology - Biomolecules</topic><topic>Scaling</topic><toplevel>online_resources</toplevel><creatorcontrib>Li, Huaping</creatorcontrib><creatorcontrib>Alkan Kabakcioglu</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Access via ProQuest (Open Access)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv Quantitative Biology</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Li, Huaping</au><au>Alkan Kabakcioglu</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Role of helicity in DNA hairping folding dynamics</atitle><jtitle>arXiv.org</jtitle><date>2018-06-22</date><risdate>2018</risdate><eissn>2331-8422</eissn><abstract>We study hairpin folding dynamics by means of extensive computer simulations, with particular attention paid to the influence of helicity on the folding time \(\tau\). We find that the dynamical exponent \(\alpha\) of the anomalous scaling \(\tau \sim N^\alpha\) for a hairpin with length N changes from 1.6 (\(1+\nu\)) to 1.2 (\(2\nu\)) in three dimensions, when duplex helicity is removed. The relation \(\alpha = 2\nu\) in rotationless hairpin folding is further verified in two dimensions (\(\nu = 0.75\)), and for a ghost-chain (\(\nu = 0.5\)). This, to our knowledge, is the first observation of the theoretical lower bound on \(\alpha\), which was predicted earlier on the basis of energy conservation for polymer translocation through a pore. Our findings suggest that the folding dynamics in long helical chains is governed by the duplex dynamics, contrasting the earlier understanding based on the stem-flower picture of unpaired segments. We propose a scaling argument for \(\alpha = 1+\nu\) in helical chains, assuming that duplex relaxation required for orientational positioning of the next pair of bases is the rate-limiting process.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1806.08609</doi><oa>free_for_read</oa></addata></record> |
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subjects | Computer simulation Deoxyribonucleic acid DNA Dynamics Energy conservation Folding Helicity Lower bounds Physics - Biological Physics Quantitative Biology - Biomolecules Scaling |
title | Role of helicity in DNA hairping folding dynamics |
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