Competing phases in the high field phase diagram of (TMTSF)(2)ClO(4).
Identifieur interne : 000125 ( PubMed/Checkpoint ); précédent : 000124; suivant : 000126Competing phases in the high field phase diagram of (TMTSF)(2)ClO(4).
Auteurs : S. Haddad [Tunisie] ; S. Charfi-Kaddour ; C. Nickel ; M. Héritier ; R. BennaceurSource :
- Physical review letters [ 0031-9007 ] ; 2002.
Abstract
A model is presented for the high field phase diagram of (TMTSF)(2)ClO(4), taking into account the anion ordering, which splits the Fermi surface into two bands. For strong enough field, the largest metal spin density wave critical temperature corresponds to the N=0 phase, which originates from two intraband nesting processes. At lower temperature, the competition between these processes puts at disadvantage the N=0 phase vs the N=1 phase, which is due to interband nesting. A first order transition then takes place from the N=0 to N=1 phase. We ascribe to this effect the experimentally observed phase diagrams.
DOI: 10.1103/PhysRevLett.89.087001
PubMed: 12190492
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A first order transition then takes place from the N=0 to N=1 phase. We ascribe to this effect the experimentally observed phase diagrams.</div></front></TEI><pubmed><MedlineCitation Status="PubMed-not-MEDLINE" Owner="NLM"><PMID Version="1">12190492</PMID><DateCreated><Year>2002</Year><Month>08</Month><Day>22</Day></DateCreated><DateCompleted><Year>2002</Year><Month>10</Month><Day>04</Day></DateCompleted><DateRevised><Year>2003</Year><Month>11</Month><Day>03</Day></DateRevised><Article PubModel="Print-Electronic"><Journal><ISSN IssnType="Print">0031-9007</ISSN><JournalIssue CitedMedium="Print"><Volume>89</Volume><Issue>8</Issue><PubDate><Year>2002</Year><Month>Aug</Month><Day>19</Day></PubDate></JournalIssue><Title>Physical review letters</Title><ISOAbbreviation>Phys. Rev. Lett.</ISOAbbreviation></Journal><ArticleTitle>Competing phases in the high field phase diagram of (TMTSF)(2)ClO(4).</ArticleTitle><Pagination><MedlinePgn>087001</MedlinePgn></Pagination><Abstract><AbstractText>A model is presented for the high field phase diagram of (TMTSF)(2)ClO(4), taking into account the anion ordering, which splits the Fermi surface into two bands. For strong enough field, the largest metal spin density wave critical temperature corresponds to the N=0 phase, which originates from two intraband nesting processes. At lower temperature, the competition between these processes puts at disadvantage the N=0 phase vs the N=1 phase, which is due to interband nesting. A first order transition then takes place from the N=0 to N=1 phase. We ascribe to this effect the experimentally observed phase diagrams.</AbstractText></Abstract><AuthorList CompleteYN="Y"><Author ValidYN="Y"><LastName>Haddad</LastName><ForeName>S</ForeName><Initials>S</Initials><AffiliationInfo><Affiliation>Laboratoire de Physique de la Matière Condensée, Département de Physique, Faculté des Sciences de Tunis, Campus universitaire, 1060 Tunis, Tunisia.</Affiliation></AffiliationInfo></Author><Author ValidYN="Y"><LastName>Charfi-Kaddour</LastName><ForeName>S</ForeName><Initials>S</Initials></Author><Author ValidYN="Y"><LastName>Nickel</LastName><ForeName>C</ForeName><Initials>C</Initials></Author><Author ValidYN="Y"><LastName>Héritier</LastName><ForeName>M</ForeName><Initials>M</Initials></Author><Author ValidYN="Y"><LastName>Bennaceur</LastName><ForeName>R</ForeName><Initials>R</Initials></Author></AuthorList><Language>eng</Language><PublicationTypeList><PublicationType UI="D016428">Journal Article</PublicationType></PublicationTypeList><ArticleDate DateType="Electronic"><Year>2002</Year><Month>08</Month><Day>01</Day></ArticleDate></Article><MedlineJournalInfo><Country>United States</Country><MedlineTA>Phys Rev Lett</MedlineTA><NlmUniqueID>0401141</NlmUniqueID><ISSNLinking>0031-9007</ISSNLinking></MedlineJournalInfo></MedlineCitation><PubmedData><History><PubMedPubDate PubStatus="received"><Year>2001</Year><Month>08</Month><Day>30</Day></PubMedPubDate><PubMedPubDate PubStatus="pubmed"><Year>2002</Year><Month>8</Month><Day>23</Day><Hour>10</Hour><Minute>0</Minute></PubMedPubDate><PubMedPubDate PubStatus="medline"><Year>2002</Year><Month>8</Month><Day>23</Day><Hour>10</Hour><Minute>1</Minute></PubMedPubDate><PubMedPubDate PubStatus="entrez"><Year>2002</Year><Month>8</Month><Day>23</Day><Hour>10</Hour><Minute>0</Minute></PubMedPubDate></History><PublicationStatus>ppublish</PublicationStatus><ArticleIdList><ArticleId IdType="pubmed">12190492</ArticleId><ArticleId IdType="doi">10.1103/PhysRevLett.89.087001</ArticleId></ArticleIdList></PubmedData></pubmed><affiliations><list><country><li>Tunisie</li></country><region><li>Gouvernorat de Tunis</li></region><settlement><li>Tunis</li></settlement></list><tree><noCountry><name sortKey="Bennaceur, R" sort="Bennaceur, R" uniqKey="Bennaceur R" first="R" last="Bennaceur">R. Bennaceur</name><name sortKey="Charfi Kaddour, S" sort="Charfi Kaddour, S" uniqKey="Charfi Kaddour S" first="S" last="Charfi-Kaddour">S. Charfi-Kaddour</name><name sortKey="Heritier, M" sort="Heritier, M" uniqKey="Heritier M" first="M" last="Héritier">M. Héritier</name><name sortKey="Nickel, C" sort="Nickel, C" uniqKey="Nickel C" first="C" last="Nickel">C. Nickel</name></noCountry><country name="Tunisie"><region name="Gouvernorat de Tunis"><name sortKey="Haddad, S" sort="Haddad, S" uniqKey="Haddad S" first="S" last="Haddad">S. Haddad</name></region></country></tree></affiliations></record>Pour manipuler ce document sous Unix (Dilib)
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