Magnetization in the Ultraquantum Limit
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Abstract
The magnetization below and far above the quantum limit for small Fermi surface orbits has been measured in the metallic compound LaRhIn5 . The magnetization due to a pocket of Fermi surface that comprises less than 1 part in 104 of the total Brillouin zone volume, and for which the quantum limit is approximately 7 T , leads to the appearance of an overall sample magnetic moment at fields between 7 and 32 T . This moment arises from diamagnetic currents produced by electrons in the ultraquantum limit. A model calculation of the origin and magnitude of the effect is in excellent agreement with the measured field dependence of the induced magnetization.
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Magnetization in the Ultraquantum Limit</title><author><name sortKey="Goodrich, R G" uniqKey="Goodrich R">R. G. Goodrich</name><affiliation wicri:level="2"><inist:fA14 i1="01"><s1>Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70802</s1><sZ>1 aut.</sZ></inist:fA14><country xml:lang="fr">États-Unis</country><placeName><region type="state">Louisiane</region></placeName><wicri:cityArea>Department of Physics and Astronomy, Louisiana State University, Baton Rouge</wicri:cityArea></affiliation></author><author><name sortKey="Maslov, D L" uniqKey="Maslov D">D. L. Maslov</name><affiliation wicri:level="2"><inist:fA14 i1="02"><s1>Department of Physics, University of Florida, Gainesville, Florida 32611</s1><sZ>2 aut.</sZ><sZ>3 aut.</sZ></inist:fA14><country xml:lang="fr">États-Unis</country><placeName><region type="state">Floride</region></placeName><wicri:cityArea>Department of Physics, University of Florida, Gainesville</wicri:cityArea></affiliation></author><author><name sortKey="Hebard, A F" uniqKey="Hebard A">A. F. Hebard</name><affiliation wicri:level="2"><inist:fA14 i1="02"><s1>Department of Physics, University of Florida, Gainesville, Florida 32611</s1><sZ>2 aut.</sZ><sZ>3 aut.</sZ></inist:fA14><country xml:lang="fr">États-Unis</country><placeName><region type="state">Floride</region></placeName><wicri:cityArea>Department of Physics, University of Florida, Gainesville</wicri:cityArea></affiliation></author><author><name sortKey="Sarrao, J L" uniqKey="Sarrao J">J. L. Sarrao</name><affiliation wicri:level="2"><inist:fA14 i1="03"><s1>Los Alamos National Laboratory, MST-10, Los Alamos, New Mexico 87545</s1><sZ>4 aut.</sZ></inist:fA14><country xml:lang="fr">États-Unis</country><placeName><region type="state">Nouveau-Mexique</region></placeName><wicri:cityArea>Los Alamos National Laboratory, MST-10, Los Alamos</wicri:cityArea></affiliation></author><author><name sortKey="Hall, D" uniqKey="Hall D">D. Hall</name><affiliation wicri:level="2"><inist:fA14 i1="04"><s1>National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310</s1><sZ>5 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country xml:lang="fr">États-Unis</country><placeName><region type="state">Floride</region></placeName><wicri:cityArea>National High Magnetic Field Laboratory, Florida State University, Tallahassee</wicri:cityArea></affiliation></author><author><name sortKey="Fisk, Z" uniqKey="Fisk Z">Z. Fisk</name><affiliation wicri:level="2"><inist:fA14 i1="04"><s1>National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310</s1><sZ>5 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country xml:lang="fr">États-Unis</country><placeName><region type="state">Floride</region></placeName><wicri:cityArea>National High Magnetic Field Laboratory, Florida State University, Tallahassee</wicri:cityArea></affiliation></author></titleStmt><publicationStmt><idno type="inist">02-0342096</idno><date when="2002-07-08">2002-07-08</date><idno type="stanalyst">PASCAL 02-0342096 AIP</idno><idno type="RBID">Pascal:02-0342096</idno><idno type="wicri:Area/Main/Corpus">00F067</idno><idno type="wicri:Area/Main/Repository">00E036</idno></publicationStmt><seriesStmt><idno type="ISSN">0031-9007</idno><title level="j" type="abbreviated">Phys. rev. lett.</title><title level="j" type="main">Physical review letters</title></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Brillouin zones</term><term>Experimental study</term><term>Fermi liquid</term><term>Fermi surface</term><term>Indium compounds</term><term>Lanthanum compounds</term><term>Magnetic moments</term><term>Magnetization</term><term>Rhenium compounds</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>7118</term><term>7127</term><term>Etude expérimentale</term><term>Lanthane composé</term><term>Rhénium composé</term><term>Indium composé</term><term>Aimantation</term><term>Surface Fermi</term><term>Zone Brillouin</term><term>Moment magnétique</term><term>Liquide Fermi</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">The magnetization below and far above the quantum limit for small Fermi surface orbits has been measured in the metallic compound LaRhIn<sub>5</sub> . The magnetization due to a pocket of Fermi surface that comprises less than 1 part in 10<sup>4</sup> of the total Brillouin zone volume, and for which the quantum limit is approximately 7 T , leads to the appearance of an overall sample magnetic moment at fields between 7 and 32 T . This moment arises from diamagnetic currents produced by electrons in the ultraquantum limit. A model calculation of the origin and magnitude of the effect is in excellent agreement with the measured field dependence of the induced magnetization.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0031-9007</s0></fA01><fA02 i1="01"><s0>PRLTAO</s0></fA02><fA03 i2="1"><s0>Phys. rev. lett.</s0></fA03><fA05><s2>89</s2></fA05><fA06><s2>2</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Magnetization in the Ultraquantum Limit</s1></fA08><fA11 i1="01" i2="1"><s1>GOODRICH (R. G.)</s1></fA11><fA11 i1="02" i2="1"><s1>MASLOV (D. L.)</s1></fA11><fA11 i1="03" i2="1"><s1>HEBARD (A. F.)</s1></fA11><fA11 i1="04" i2="1"><s1>SARRAO (J. L.)</s1></fA11><fA11 i1="05" i2="1"><s1>HALL (D.)</s1></fA11><fA11 i1="06" i2="1"><s1>FISK (Z.)</s1></fA11><fA14 i1="01"><s1>Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70802</s1><sZ>1 aut.</sZ></fA14><fA14 i1="02"><s1>Department of Physics, University of Florida, Gainesville, Florida 32611</s1><sZ>2 aut.</sZ><sZ>3 aut.</sZ></fA14><fA14 i1="03"><s1>Los Alamos National Laboratory, MST-10, Los Alamos, New Mexico 87545</s1><sZ>4 aut.</sZ></fA14><fA14 i1="04"><s1>National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310</s1><sZ>5 aut.</sZ><sZ>6 aut.</sZ></fA14><fA20><s2>026401-026401-4</s2></fA20><fA21><s1>2002-07-08</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>8895</s2></fA43><fA44><s0>8100</s0><s1>© 2002 American Institute of Physics. All rights reserved.</s1></fA44><fA47 i1="01" i2="1"><s0>02-0342096</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Physical review letters</s0></fA64><fA66 i1="01"><s0>USA</s0></fA66><fC01 i1="01" l="ENG"><s0>The magnetization below and far above the quantum limit for small Fermi surface orbits has been measured in the metallic compound LaRhIn<sub>5</sub> . The magnetization due to a pocket of Fermi surface that comprises less than 1 part in 10<sup>4</sup> of the total Brillouin zone volume, and for which the quantum limit is approximately 7 T , leads to the appearance of an overall sample magnetic moment at fields between 7 and 32 T . This moment arises from diamagnetic currents produced by electrons in the ultraquantum limit. A model calculation of the origin and magnitude of the effect is in excellent agreement with the measured field dependence of the induced magnetization.</s0></fC01><fC02 i1="01" i2="3"><s0>001B70A18</s0></fC02><fC02 i1="02" i2="3"><s0>001B70A27</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>7118</s0><s2>PAC</s2><s4>INC</s4></fC03><fC03 i1="02" i2="3" l="FRE"><s0>7127</s0><s2>PAC</s2><s4>INC</s4></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Etude expérimentale</s0></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Experimental study</s0></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Lanthane composé</s0></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Lanthanum compounds</s0></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Rhénium composé</s0></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Rhenium compounds</s0></fC03><fC03 i1="06" i2="3" l="FRE"><s0>Indium composé</s0></fC03><fC03 i1="06" i2="3" l="ENG"><s0>Indium compounds</s0></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Aimantation</s0></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Magnetization</s0></fC03><fC03 i1="08" i2="3" l="FRE"><s0>Surface Fermi</s0></fC03><fC03 i1="08" i2="3" l="ENG"><s0>Fermi surface</s0></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Zone Brillouin</s0></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Brillouin zones</s0></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Moment magnétique</s0></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Magnetic moments</s0></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Liquide Fermi</s0></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Fermi liquid</s0></fC03><fN21><s1>182</s1></fN21><fN47 i1="01" i2="1"><s0>0226M000481</s0></fN47></pA></standard></inist></record>Pour manipuler ce document sous Unix (Dilib)
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