Electronic transport properties of liquid less-simple metals
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Abstract
Electronic transport properties, namely the electrical resistivity and the thermoelectric power, of liquid less-simple metals, Zn, Cd, Hg, In, Tl, Sn, Pb, Sb, and Bi, are calculated using Ziman's theory. The effective electron-ion and ion-ion interactions are described by the Bretonnet-Silbert model. The static structure factors are evaluated by the self-consistent Variational Modified Hyper-netted Chain (VMHNC) integral equation of liquids. The results for the electrical resistivity are fairly good when compared with experimental data, but the agreement improves significantly when the blurring of the Fermi surface due to the finite electron mean free path is accounted for. The values of the thermoelectric power, for most systems, have the same sign and order of magnitude as the experimental ones. The results for the thermopower also show that the contribution of the energy dependent term of the electron-ion potential is significant for the concerned systems.
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Electronic transport properties of liquid less-simple metals</title><author><name sortKey="Sharmin, S" uniqKey="Sharmin S">S. Sharmin</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, University of Dhaka</s1><s2>Dhaka-1000</s2><s3>BGD</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></inist:fA14><country>Bangladesh</country><wicri:noRegion>Dhaka-1000</wicri:noRegion></affiliation></author><author><name sortKey="Bhuiyan, G M" uniqKey="Bhuiyan G">G. M. Bhuiyan</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, University of Dhaka</s1><s2>Dhaka-1000</s2><s3>BGD</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></inist:fA14><country>Bangladesh</country><wicri:noRegion>Dhaka-1000</wicri:noRegion></affiliation></author><author><name sortKey="Khaleque, M A" uniqKey="Khaleque M">M. A. Khaleque</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, University of Dhaka</s1><s2>Dhaka-1000</s2><s3>BGD</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></inist:fA14><country>Bangladesh</country><wicri:noRegion>Dhaka-1000</wicri:noRegion></affiliation></author><author><name sortKey="Rashid, R I M A" uniqKey="Rashid R">R. I. M. A. Rashid</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, University of Dhaka</s1><s2>Dhaka-1000</s2><s3>BGD</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></inist:fA14><country>Bangladesh</country><wicri:noRegion>Dhaka-1000</wicri:noRegion></affiliation></author><author><name sortKey="Mujibur Rahman, S M" uniqKey="Mujibur Rahman S">S. M. Mujibur Rahman</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Department of Physics, College of Science, Sultan Qaboos University, P.O. Box 36</s1><s2>Al Khod, 123 Muscat</s2><s3>OMN</s3><sZ>5 aut.</sZ></inist:fA14><country>Oman</country><wicri:noRegion>Al Khod, 123 Muscat</wicri:noRegion></affiliation></author></titleStmt><publicationStmt><idno type="inist">02-0485938</idno><date when="2002">2002</date><idno type="stanalyst">PASCAL 02-0485938 INIST</idno><idno type="RBID">Pascal:02-0485938</idno><idno type="wicri:Area/Main/Corpus">00E780</idno><idno type="wicri:Area/Main/Repository">00F467</idno></publicationStmt><seriesStmt><idno type="ISSN">0370-1972</idno><title level="j" type="abbreviated">Phys. status solidi, B, Basic res.</title><title level="j" type="main">Physica status solidi. B. Basic research</title></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Antimony</term><term>Bismuth</term><term>Cadmium</term><term>Electrical conductivity</term><term>Electron ion interaction</term><term>Fermi surface</term><term>Indium</term><term>Integral equations</term><term>Mean free path</term><term>Mercury</term><term>Thermoelectric power</term><term>Tin</term><term>Transport processes</term><term>Ziman theory</term><term>Zinc</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Phénomène transport</term><term>Conductivité électrique</term><term>Pouvoir thermoélectrique</term><term>Interaction électron ion</term><term>Equation intégrale</term><term>Surface Fermi</term><term>Libre parcours moyen</term><term>Zinc</term><term>Cadmium</term><term>Mercure</term><term>Indium</term><term>Etain</term><term>Antimoine</term><term>Bismuth</term><term>Zn</term><term>Cd</term><term>Hg</term><term>In</term><term>7215J</term><term>7215L</term><term>7215C</term><term>Tl</term><term>Sn</term><term>Bi</term><term>Théorie Ziman</term></keywords><keywords scheme="Wicri" type="concept" xml:lang="fr"><term>Zinc</term><term>Cadmium</term><term>Mercure</term><term>Antimoine</term><term>Bismuth</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">Electronic transport properties, namely the electrical resistivity and the thermoelectric power, of liquid less-simple metals, Zn, Cd, Hg, In, Tl, Sn, Pb, Sb, and Bi, are calculated using Ziman's theory. The effective electron-ion and ion-ion interactions are described by the Bretonnet-Silbert model. The static structure factors are evaluated by the self-consistent Variational Modified Hyper-netted Chain (VMHNC) integral equation of liquids. The results for the electrical resistivity are fairly good when compared with experimental data, but the agreement improves significantly when the blurring of the Fermi surface due to the finite electron mean free path is accounted for. The values of the thermoelectric power, for most systems, have the same sign and order of magnitude as the experimental ones. The results for the thermopower also show that the contribution of the energy dependent term of the electron-ion potential is significant for the concerned systems.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0370-1972</s0></fA01><fA02 i1="01"><s0>PSSBBD</s0></fA02><fA03 i2="1"><s0>Phys. status solidi, B, Basic res.</s0></fA03><fA05><s2>232</s2></fA05><fA06><s2>2</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Electronic transport properties of liquid less-simple metals</s1></fA08><fA11 i1="01" i2="1"><s1>SHARMIN (S.)</s1></fA11><fA11 i1="02" i2="1"><s1>BHUIYAN (G. M.)</s1></fA11><fA11 i1="03" i2="1"><s1>KHALEQUE (M. A.)</s1></fA11><fA11 i1="04" i2="1"><s1>RASHID (R. I. M. A.)</s1></fA11><fA11 i1="05" i2="1"><s1>MUJIBUR RAHMAN (S. M.)</s1></fA11><fA14 i1="01"><s1>Department of Physics, University of Dhaka</s1><s2>Dhaka-1000</s2><s3>BGD</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></fA14><fA14 i1="02"><s1>Department of Physics, College of Science, Sultan Qaboos University, P.O. Box 36</s1><s2>Al Khod, 123 Muscat</s2><s3>OMN</s3><sZ>5 aut.</sZ></fA14><fA20><s1>243-253</s1></fA20><fA21><s1>2002</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>10183B</s2><s5>354000104512850060</s5></fA43><fA44><s0>0000</s0><s1>© 2002 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>40 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>02-0485938</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Physica status solidi. B. Basic research</s0></fA64><fA66 i1="01"><s0>DEU</s0></fA66><fC01 i1="01" l="ENG"><s0>Electronic transport properties, namely the electrical resistivity and the thermoelectric power, of liquid less-simple metals, Zn, Cd, Hg, In, Tl, Sn, Pb, Sb, and Bi, are calculated using Ziman's theory. The effective electron-ion and ion-ion interactions are described by the Bretonnet-Silbert model. The static structure factors are evaluated by the self-consistent Variational Modified Hyper-netted Chain (VMHNC) integral equation of liquids. The results for the electrical resistivity are fairly good when compared with experimental data, but the agreement improves significantly when the blurring of the Fermi surface due to the finite electron mean free path is accounted for. The values of the thermoelectric power, for most systems, have the same sign and order of magnitude as the experimental ones. The results for the thermopower also show that the contribution of the energy dependent term of the electron-ion potential is significant for the concerned systems.</s0></fC01><fC02 i1="01" i2="3"><s0>001B70B15J</s0></fC02><fC02 i1="02" i2="3"><s0>001B70B15L</s0></fC02><fC02 i1="03" i2="3"><s0>001B70B15C</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Phénomène transport</s0><s5>01</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Transport processes</s0><s5>01</s5></fC03><fC03 i1="02" i2="3" l="FRE"><s0>Conductivité électrique</s0><s5>02</s5></fC03><fC03 i1="02" i2="3" l="ENG"><s0>Electrical conductivity</s0><s5>02</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Pouvoir thermoélectrique</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Thermoelectric power</s0><s5>03</s5></fC03><fC03 i1="04" i2="X" l="FRE"><s0>Interaction électron ion</s0><s5>04</s5></fC03><fC03 i1="04" i2="X" l="ENG"><s0>Electron ion interaction</s0><s5>04</s5></fC03><fC03 i1="04" i2="X" l="SPA"><s0>Interacción electrón ión</s0><s5>04</s5></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Equation intégrale</s0><s5>05</s5></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Integral equations</s0><s5>05</s5></fC03><fC03 i1="06" i2="3" l="FRE"><s0>Surface Fermi</s0><s5>06</s5></fC03><fC03 i1="06" i2="3" l="ENG"><s0>Fermi surface</s0><s5>06</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Libre parcours moyen</s0><s5>07</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Mean free path</s0><s5>07</s5></fC03><fC03 i1="08" i2="3" l="FRE"><s0>Zinc</s0><s2>NC</s2><s5>15</s5></fC03><fC03 i1="08" i2="3" l="ENG"><s0>Zinc</s0><s2>NC</s2><s5>15</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Cadmium</s0><s2>NC</s2><s5>16</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Cadmium</s0><s2>NC</s2><s5>16</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Mercure</s0><s2>NC</s2><s5>17</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Mercury</s0><s2>NC</s2><s5>17</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Indium</s0><s2>NC</s2><s5>18</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Indium</s0><s2>NC</s2><s5>18</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Etain</s0><s2>NC</s2><s5>19</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Tin</s0><s2>NC</s2><s5>19</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Antimoine</s0><s2>NC</s2><s5>20</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>Antimony</s0><s2>NC</s2><s5>20</s5></fC03><fC03 i1="14" i2="3" l="FRE"><s0>Bismuth</s0><s2>NC</s2><s5>21</s5></fC03><fC03 i1="14" i2="3" l="ENG"><s0>Bismuth</s0><s2>NC</s2><s5>21</s5></fC03><fC03 i1="15" i2="3" l="FRE"><s0>Zn</s0><s4>INC</s4><s5>52</s5></fC03><fC03 i1="16" i2="3" l="FRE"><s0>Cd</s0><s4>INC</s4><s5>53</s5></fC03><fC03 i1="17" i2="3" l="FRE"><s0>Hg</s0><s4>INC</s4><s5>54</s5></fC03><fC03 i1="18" i2="3" l="FRE"><s0>In</s0><s4>INC</s4><s5>55</s5></fC03><fC03 i1="19" i2="3" l="FRE"><s0>7215J</s0><s2>PAC</s2><s4>INC</s4><s5>56</s5></fC03><fC03 i1="20" i2="3" l="FRE"><s0>7215L</s0><s2>PAC</s2><s4>INC</s4><s5>57</s5></fC03><fC03 i1="21" i2="3" l="FRE"><s0>7215C</s0><s2>PAC</s2><s4>INC</s4><s5>58</s5></fC03><fC03 i1="22" i2="3" l="FRE"><s0>Tl</s0><s4>INC</s4><s5>92</s5></fC03><fC03 i1="23" i2="3" l="FRE"><s0>Sn</s0><s4>INC</s4><s5>93</s5></fC03><fC03 i1="24" i2="3" l="FRE"><s0>Bi</s0><s4>INC</s4><s5>94</s5></fC03><fC03 i1="25" i2="3" l="FRE"><s0>Théorie Ziman</s0><s4>CD</s4><s5>96</s5></fC03><fC03 i1="25" i2="3" l="ENG"><s0>Ziman theory</s0><s4>CD</s4><s5>96</s5></fC03><fC07 i1="01" i2="3" l="FRE"><s0>Métal transition</s0><s5>48</s5></fC07><fC07 i1="01" i2="3" l="ENG"><s0>Transition elements</s0><s5>48</s5></fC07><fN21><s1>287</s1></fN21><fN82><s1>PSI</s1></fN82></pA></standard></inist></record>Pour manipuler ce document sous Unix (Dilib)
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