Detailed Structure of a CDW in a Quenched Random Field
Using high resolution x-ray scattering, we have measured the structure of the Q_1 CDW in Ta-doped NbSe_3. Detailed line shape analysis of the data demonstrates that two length scales are required to describe the phase-phase correlation function. Phase fluctuations with wavelengths less than a new le...
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creator | Brock, J. D Finnefrock, A. C Ringland, K. L Sweetland, E |
description | Using high resolution x-ray scattering, we have measured the structure of the
Q_1 CDW in Ta-doped NbSe_3. Detailed line shape analysis of the data
demonstrates that two length scales are required to describe the phase-phase
correlation function. Phase fluctuations with wavelengths less than a new
length scale $a$ are suppressed and this $a$ is identified with the amplitude
coherence length. We find that xi_a* = 34.4 \pm 10.3 angstroms. Implications
for the physical mechanisms responsible for pinning are discussed. |
doi_str_mv | 10.48550/arxiv.cond-mat/9411123 |
format | Article |
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Q_1 CDW in Ta-doped NbSe_3. Detailed line shape analysis of the data
demonstrates that two length scales are required to describe the phase-phase
correlation function. Phase fluctuations with wavelengths less than a new
length scale $a$ are suppressed and this $a$ is identified with the amplitude
coherence length. We find that xi_a* = 34.4 \pm 10.3 angstroms. Implications
for the physical mechanisms responsible for pinning are discussed.</description><identifier>DOI: 10.48550/arxiv.cond-mat/9411123</identifier><language>eng</language><subject>Physics - Disordered Systems and Neural Networks ; Physics - Materials Science ; Physics - Mesoscale and Nanoscale Physics ; Physics - Other Condensed Matter ; Physics - Quantum Gases ; Physics - Soft Condensed Matter ; Physics - Statistical Mechanics ; Physics - Strongly Correlated Electrons ; Physics - Superconductivity</subject><creationdate>1994-11</creationdate><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/cond-mat/9411123$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.1103/PhysRevLett.73.3588$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.cond-mat/9411123$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Brock, J. D</creatorcontrib><creatorcontrib>Finnefrock, A. C</creatorcontrib><creatorcontrib>Ringland, K. L</creatorcontrib><creatorcontrib>Sweetland, E</creatorcontrib><title>Detailed Structure of a CDW in a Quenched Random Field</title><description>Using high resolution x-ray scattering, we have measured the structure of the
Q_1 CDW in Ta-doped NbSe_3. Detailed line shape analysis of the data
demonstrates that two length scales are required to describe the phase-phase
correlation function. Phase fluctuations with wavelengths less than a new
length scale $a$ are suppressed and this $a$ is identified with the amplitude
coherence length. We find that xi_a* = 34.4 \pm 10.3 angstroms. Implications
for the physical mechanisms responsible for pinning are discussed.</description><subject>Physics - Disordered Systems and Neural Networks</subject><subject>Physics - Materials Science</subject><subject>Physics - Mesoscale and Nanoscale Physics</subject><subject>Physics - Other Condensed Matter</subject><subject>Physics - Quantum Gases</subject><subject>Physics - Soft Condensed Matter</subject><subject>Physics - Statistical Mechanics</subject><subject>Physics - Strongly Correlated Electrons</subject><subject>Physics - Superconductivity</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1994</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNpjYJA3NNAzsTA1NdBPLKrILNNLzs9L0c1NLNG3NDE0NDQy5mQwc0ktSczMSU1RCC4pKk0uKS1KVchPU0hUcHYJV8jMAzICS1PzkjOACoIS81LycxXcMlNzUngYWNMSc4pTeaE0N4Oqm2uIs4cu2J74gqLM3MSiyniQffFA--Kh9hkTqw4AnP86BA</recordid><startdate>19941128</startdate><enddate>19941128</enddate><creator>Brock, J. D</creator><creator>Finnefrock, A. C</creator><creator>Ringland, K. L</creator><creator>Sweetland, E</creator><scope>GOX</scope></search><sort><creationdate>19941128</creationdate><title>Detailed Structure of a CDW in a Quenched Random Field</title><author>Brock, J. D ; Finnefrock, A. C ; Ringland, K. L ; Sweetland, E</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_cond_mat_94111233</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1994</creationdate><topic>Physics - Disordered Systems and Neural Networks</topic><topic>Physics - Materials Science</topic><topic>Physics - Mesoscale and Nanoscale Physics</topic><topic>Physics - Other Condensed Matter</topic><topic>Physics - Quantum Gases</topic><topic>Physics - Soft Condensed Matter</topic><topic>Physics - Statistical Mechanics</topic><topic>Physics - Strongly Correlated Electrons</topic><topic>Physics - Superconductivity</topic><toplevel>online_resources</toplevel><creatorcontrib>Brock, J. D</creatorcontrib><creatorcontrib>Finnefrock, A. C</creatorcontrib><creatorcontrib>Ringland, K. L</creatorcontrib><creatorcontrib>Sweetland, E</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Brock, J. D</au><au>Finnefrock, A. C</au><au>Ringland, K. L</au><au>Sweetland, E</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Detailed Structure of a CDW in a Quenched Random Field</atitle><date>1994-11-28</date><risdate>1994</risdate><abstract>Using high resolution x-ray scattering, we have measured the structure of the
Q_1 CDW in Ta-doped NbSe_3. Detailed line shape analysis of the data
demonstrates that two length scales are required to describe the phase-phase
correlation function. Phase fluctuations with wavelengths less than a new
length scale $a$ are suppressed and this $a$ is identified with the amplitude
coherence length. We find that xi_a* = 34.4 \pm 10.3 angstroms. Implications
for the physical mechanisms responsible for pinning are discussed.</abstract><doi>10.48550/arxiv.cond-mat/9411123</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - Disordered Systems and Neural Networks Physics - Materials Science Physics - Mesoscale and Nanoscale Physics Physics - Other Condensed Matter Physics - Quantum Gases Physics - Soft Condensed Matter Physics - Statistical Mechanics Physics - Strongly Correlated Electrons Physics - Superconductivity |
title | Detailed Structure of a CDW in a Quenched Random Field |
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