<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-04-13T13:22:19Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2099.1/16864" metadataPrefix="marc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2099.1/16864</identifier><datestamp>2026-01-20T11:05:32Z</datestamp><setSpec>com_2072_1033</setSpec><setSpec>col_2072_452951</setSpec></header><metadata><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
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      <subfield code="a">López Pérez, Daniel Ernesto</subfield>
      <subfield code="e">author</subfield>
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   <datafield ind2=" " ind1=" " tag="260">
      <subfield code="c">2012-06</subfield>
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      <subfield code="a">The helical peptide Cys-Ala-Lys-(Glu-Ala-Ala-Ala-Lys)2-Ala-NH-(CH2)2-SH has been organized forming a self-assembled monolayer on gold (0.602 peptides per nm2), its conductance behavior at stretching conditions being studied using scanning tunnelling microscopy and current sensing atomic force microscopy. The helical conformation of the peptide has been found to play a fundamental role in the conductance. Moreover, variation of the current upon molecular stretching indicates that peptides can be significantly elongated before the conductance drops to zero, the critical elongation being 1.22 ± 0.47 nm. Molecular dynamics simulations of a single peptide in the free state and of a variable number of peptides tethered to a gold surface (i.e. densities ranging from 10.026 to 1.295 peptides per nm2) have indicated that the helical conformation is intrinsically favored in solvated environments while in desolvated environments it is retained because of the fundamental role played by peptide–peptide intermolecular interactions. The structure obtained for the system with 24 tethered peptides, with a density of 0.634 peptides per nm2 is the closest to the experimental one, is in excellent agreement with experimental observations. On the other hand, simulations in which a single molecule is submitted to different compression and stretching processes while the rest remain in the equilibrium have been used to mimic the variation of the tip–substrate distance in experimental measures. Results allowed us to identify the existence, and in some cases coexistence, of intermolecular and intramolecular ionic ladders, suggesting that peptide-mediated electron transfer occurs through the hopping mechanism. Finally, quantum mechanical calculations have been used to investigate the variation of the electronic structure upon compression and stretching deformations.</subfield>
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      <subfield code="a">Àrees temàtiques de la UPC::Enginyeria química::Química física::Estructura molecular</subfield>
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      <subfield code="a">Àrees temàtiques de la UPC::Enginyeria química::Química orgànica::Bioquímica</subfield>
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      <subfield code="a">Peptides –- Metabolism</subfield>
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      <subfield code="a">Molecular dynamics -- Simulation methods</subfield>
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      <subfield code="a">Pèptids -- Metabolisme</subfield>
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      <subfield code="a">Dinàmica molecular -- Mètodes de simulació</subfield>
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      <subfield code="a">Intermolecular interactions in Electron Transfer through Stretched Helical Peptides</subfield>
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