Modifying hydrogen-bonded structures by physical vapor deposition: 4-methyl-3-heptanol
We prepared films of 4-methyl-3-heptanol by vapor depositing onto substrates held at temperatures between T dep = 0.6T g and T g, where T g is the glass transition temperature. Using deposition rates between 0.9 and 6.0 nm/s, we prepared films about 5 μm thick and measured the dielectric properties...
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Veröffentlicht in: | The Journal of chemical physics 2017-11, Vol.147 (19), p.194504-194504 |
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container_title | The Journal of chemical physics |
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creator | Young-Gonzales, A. R. Guiseppi-Elie, A. Ediger, M. D. Richert, R. |
description | We prepared films of 4-methyl-3-heptanol by vapor depositing onto substrates held at temperatures between T
dep = 0.6T
g and T
g, where T
g is the glass transition temperature. Using deposition rates between 0.9 and 6.0 nm/s, we prepared films about 5 μm thick and measured the dielectric properties via an interdigitated electrode cell onto which films were deposited. Samples prepared at T
dep = T
g display the dielectric behavior of the ordinary supercooled liquid. Films deposited at lower deposition temperatures show a high dielectric loss upon heating toward T
g, which decreases by a factor of about 12 by annealing at T
g = 162 K. This change is consistent with either a drop of the Kirkwood correlation factor, g
k
, by a factor of about 10, or an increase in the dielectric relaxation times, both being indicative of changes toward ring-like hydrogen-bonded structure characteristic of the ordinary liquid. We rationalize the high dielectric relaxation amplitude in the vapor deposited glass by suggesting that depositions at low temperature provide insufficient time for molecules to form ring-like supramolecular structures for which dipole moments cancel. Surprisingly, above T
g of the ordinary liquid, these vapor deposited films fail to completely recover the dielectric properties of the liquid obtained by supercooling. Instead, the dielectric relaxation remains slower and its amplitude much higher than that of the equilibrium liquid state, indicative of a structure that differs from the equilibrium liquid up to at least T
g + 40 K. |
doi_str_mv | 10.1063/1.4999300 |
format | Article |
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dep = 0.6T
g and T
g, where T
g is the glass transition temperature. Using deposition rates between 0.9 and 6.0 nm/s, we prepared films about 5 μm thick and measured the dielectric properties via an interdigitated electrode cell onto which films were deposited. Samples prepared at T
dep = T
g display the dielectric behavior of the ordinary supercooled liquid. Films deposited at lower deposition temperatures show a high dielectric loss upon heating toward T
g, which decreases by a factor of about 12 by annealing at T
g = 162 K. This change is consistent with either a drop of the Kirkwood correlation factor, g
k
, by a factor of about 10, or an increase in the dielectric relaxation times, both being indicative of changes toward ring-like hydrogen-bonded structure characteristic of the ordinary liquid. We rationalize the high dielectric relaxation amplitude in the vapor deposited glass by suggesting that depositions at low temperature provide insufficient time for molecules to form ring-like supramolecular structures for which dipole moments cancel. Surprisingly, above T
g of the ordinary liquid, these vapor deposited films fail to completely recover the dielectric properties of the liquid obtained by supercooling. Instead, the dielectric relaxation remains slower and its amplitude much higher than that of the equilibrium liquid state, indicative of a structure that differs from the equilibrium liquid up to at least T
g + 40 K.</description><identifier>ISSN: 0021-9606</identifier><identifier>EISSN: 1089-7690</identifier><identifier>DOI: 10.1063/1.4999300</identifier><identifier>PMID: 29166100</identifier><identifier>CODEN: JCPSA6</identifier><language>eng</language><publisher>United States: American Institute of Physics</publisher><subject>Amplitudes ; Correlation coefficients ; Dielectric loss ; Dielectric properties ; Dielectric relaxation ; Dipole moments ; Glass transition temperature ; Hydrogen bonding ; Physical vapor deposition ; Physics ; Substrates ; Supercooling ; Thick films ; Vapor deposited films</subject><ispartof>The Journal of chemical physics, 2017-11, Vol.147 (19), p.194504-194504</ispartof><rights>Author(s)</rights><rights>2017 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c383t-8ec1f4126caa273bf4447441f570cf2598ab2504ac9ca3b0bbffb1c902f1cfc63</citedby><cites>FETCH-LOGICAL-c383t-8ec1f4126caa273bf4447441f570cf2598ab2504ac9ca3b0bbffb1c902f1cfc63</cites><orcidid>0000-0003-4715-8473 ; 0000-0001-8503-3175 ; 0000000347158473 ; 0000000185033175</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jcp/article-lookup/doi/10.1063/1.4999300$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,777,781,791,4498,27905,27906,76133</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/29166100$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Young-Gonzales, A. R.</creatorcontrib><creatorcontrib>Guiseppi-Elie, A.</creatorcontrib><creatorcontrib>Ediger, M. D.</creatorcontrib><creatorcontrib>Richert, R.</creatorcontrib><title>Modifying hydrogen-bonded structures by physical vapor deposition: 4-methyl-3-heptanol</title><title>The Journal of chemical physics</title><addtitle>J Chem Phys</addtitle><description>We prepared films of 4-methyl-3-heptanol by vapor depositing onto substrates held at temperatures between T
dep = 0.6T
g and T
g, where T
g is the glass transition temperature. Using deposition rates between 0.9 and 6.0 nm/s, we prepared films about 5 μm thick and measured the dielectric properties via an interdigitated electrode cell onto which films were deposited. Samples prepared at T
dep = T
g display the dielectric behavior of the ordinary supercooled liquid. Films deposited at lower deposition temperatures show a high dielectric loss upon heating toward T
g, which decreases by a factor of about 12 by annealing at T
g = 162 K. This change is consistent with either a drop of the Kirkwood correlation factor, g
k
, by a factor of about 10, or an increase in the dielectric relaxation times, both being indicative of changes toward ring-like hydrogen-bonded structure characteristic of the ordinary liquid. We rationalize the high dielectric relaxation amplitude in the vapor deposited glass by suggesting that depositions at low temperature provide insufficient time for molecules to form ring-like supramolecular structures for which dipole moments cancel. Surprisingly, above T
g of the ordinary liquid, these vapor deposited films fail to completely recover the dielectric properties of the liquid obtained by supercooling. Instead, the dielectric relaxation remains slower and its amplitude much higher than that of the equilibrium liquid state, indicative of a structure that differs from the equilibrium liquid up to at least T
g + 40 K.</description><subject>Amplitudes</subject><subject>Correlation coefficients</subject><subject>Dielectric loss</subject><subject>Dielectric properties</subject><subject>Dielectric relaxation</subject><subject>Dipole moments</subject><subject>Glass transition temperature</subject><subject>Hydrogen bonding</subject><subject>Physical vapor deposition</subject><subject>Physics</subject><subject>Substrates</subject><subject>Supercooling</subject><subject>Thick films</subject><subject>Vapor deposited films</subject><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp90EtLxDAUhuEgio6XhX9ACm5UiJ6TpmnjTgZvoLhRtyVJE6fSaWrSCv33VmZ04cLV2Tx8HF5CDhHOEUR6gedcSpkCbJAZQiFpLiRskhkAQyoFiB2yG-M7AGDO-DbZYRKFQIAZeX30Ve3Gun1LFmMV_JttqfZtZask9mEw_RBsTPSYdIsx1kY1yafqfEgq2_lY97VvLxNOl7ZfjA1N6cJ2vWp9s0-2nGqiPVjfPfJyc_08v6MPT7f386sHatIi7WlhDTqOTBilWJ5qxznPOUeX5WAcy2ShNMuAKyONSjVo7ZxGI4E5NM6IdI-crHa74D8GG_tyWUdjm0a11g-xRCnyQjABfKLHf-i7H0I7fVcyRAGMZVk2qdOVMsHHGKwru1AvVRhLhPI7donlOvZkj9aLg17a6lf-1J3A2QpEU_fqO9Y_a1-zGYaQ</recordid><startdate>20171121</startdate><enddate>20171121</enddate><creator>Young-Gonzales, A. R.</creator><creator>Guiseppi-Elie, A.</creator><creator>Ediger, M. D.</creator><creator>Richert, R.</creator><general>American Institute of Physics</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0003-4715-8473</orcidid><orcidid>https://orcid.org/0000-0001-8503-3175</orcidid><orcidid>https://orcid.org/0000000347158473</orcidid><orcidid>https://orcid.org/0000000185033175</orcidid></search><sort><creationdate>20171121</creationdate><title>Modifying hydrogen-bonded structures by physical vapor deposition: 4-methyl-3-heptanol</title><author>Young-Gonzales, A. R. ; Guiseppi-Elie, A. ; Ediger, M. D. ; Richert, R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c383t-8ec1f4126caa273bf4447441f570cf2598ab2504ac9ca3b0bbffb1c902f1cfc63</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Amplitudes</topic><topic>Correlation coefficients</topic><topic>Dielectric loss</topic><topic>Dielectric properties</topic><topic>Dielectric relaxation</topic><topic>Dipole moments</topic><topic>Glass transition temperature</topic><topic>Hydrogen bonding</topic><topic>Physical vapor deposition</topic><topic>Physics</topic><topic>Substrates</topic><topic>Supercooling</topic><topic>Thick films</topic><topic>Vapor deposited films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Young-Gonzales, A. R.</creatorcontrib><creatorcontrib>Guiseppi-Elie, A.</creatorcontrib><creatorcontrib>Ediger, M. D.</creatorcontrib><creatorcontrib>Richert, R.</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Young-Gonzales, A. R.</au><au>Guiseppi-Elie, A.</au><au>Ediger, M. D.</au><au>Richert, R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Modifying hydrogen-bonded structures by physical vapor deposition: 4-methyl-3-heptanol</atitle><jtitle>The Journal of chemical physics</jtitle><addtitle>J Chem Phys</addtitle><date>2017-11-21</date><risdate>2017</risdate><volume>147</volume><issue>19</issue><spage>194504</spage><epage>194504</epage><pages>194504-194504</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><coden>JCPSA6</coden><abstract>We prepared films of 4-methyl-3-heptanol by vapor depositing onto substrates held at temperatures between T
dep = 0.6T
g and T
g, where T
g is the glass transition temperature. Using deposition rates between 0.9 and 6.0 nm/s, we prepared films about 5 μm thick and measured the dielectric properties via an interdigitated electrode cell onto which films were deposited. Samples prepared at T
dep = T
g display the dielectric behavior of the ordinary supercooled liquid. Films deposited at lower deposition temperatures show a high dielectric loss upon heating toward T
g, which decreases by a factor of about 12 by annealing at T
g = 162 K. This change is consistent with either a drop of the Kirkwood correlation factor, g
k
, by a factor of about 10, or an increase in the dielectric relaxation times, both being indicative of changes toward ring-like hydrogen-bonded structure characteristic of the ordinary liquid. We rationalize the high dielectric relaxation amplitude in the vapor deposited glass by suggesting that depositions at low temperature provide insufficient time for molecules to form ring-like supramolecular structures for which dipole moments cancel. Surprisingly, above T
g of the ordinary liquid, these vapor deposited films fail to completely recover the dielectric properties of the liquid obtained by supercooling. Instead, the dielectric relaxation remains slower and its amplitude much higher than that of the equilibrium liquid state, indicative of a structure that differs from the equilibrium liquid up to at least T
g + 40 K.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>29166100</pmid><doi>10.1063/1.4999300</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0003-4715-8473</orcidid><orcidid>https://orcid.org/0000-0001-8503-3175</orcidid><orcidid>https://orcid.org/0000000347158473</orcidid><orcidid>https://orcid.org/0000000185033175</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Amplitudes Correlation coefficients Dielectric loss Dielectric properties Dielectric relaxation Dipole moments Glass transition temperature Hydrogen bonding Physical vapor deposition Physics Substrates Supercooling Thick films Vapor deposited films |
title | Modifying hydrogen-bonded structures by physical vapor deposition: 4-methyl-3-heptanol |
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