{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/23961"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/23961","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"A theory of the electrical resistivity of liquid metals","abstract":"A new technique for the calculation of electron scatter~ng in metals is proposed and developed. The method is considered valid both for crystals, at temperatures well above the Debye temperature, and for liquids, at temperatures well below the critical point. It is based on the use of ~ero-order wave functions which closely resemble Bloch functions, with perturbations depending primarily upon the short~range disorder parameters .. Although the method is similar to the one proposed and developed by GUbanov, there is one important distinction: the present approach uses zero-order wave functions that are discontinuous at the primitive cell boundaries. This allows the inclusion of terms in the scattering matrix element that were neglected by Gubanov and, furthermore, gives a straightforward procedure for calculation of all terms in the matrix element.. The perturbation procedure using dis~ continuous wave functions is justified, not rigorously perhaps, hut very plausibly. The quasi-Bloch technique is limited only by the necessity for the existence of a local structure closely resembling that of crystals, and, should therefore be valid for any liquid metal at temperatures well below the critical point 0 This is in contrast to the pseudopotential method of Ziman and others$ which is valid only when the effective electron-ion interaction is smallo The pseudopotential method is probably val,i<;i also in the very high temperature region (near the critical pOint), so the two theories may be considered as cornplementary~ each having its own region of validity, with very little overlap bet,ween regionso The perturbation matrix element in the present theory contains two types of termso One is a contribution due to long=range disorder, which may be estimated in various wayso Since this term is dominant in sodium~ its value for other metals may be obtained from the experimentally determined resistivity of sodium, and from the assumption that the ratio o'f the nearest=neighbor distance to the mean free path due to long-range disorder is the same for all metals 'at their melting pointso This was Zimanis procedure for estimating his plasma resistance, and the sarne procedure was used hereo The second type of term involves a product of the short= range disorder parameters and various derivatives of the periodic part of the Bloch functions, integrated over the cell boundarieso To avoid the need for a computer in the calculations, the zero-order wave functions were written as solutions of a three=dimensional Kronig=Penn~y mode19 the strength of the potential being related to the band gaps in the solidso It eventually became necessary to approximate these wave functions, so the numerical calculations were of limited validityo They were intended9 however~ as illustrations of the use of the method and do not exhaust its potentialitieso Numerical values of the electron mean free paths were obtained for the liquid alkali and noble metals at the melting pointo The calculated values differed from experimental values by a maximum of ~O percento The agreement was better than that of any previous calculations and was considered satisfactory in view of the uncertainties both in the parameters and in the approximations used in the calculations.","abstract_html":"A new technique for the calculation of electron scatter~ng in metals is proposed and developed. The method is considered valid both for crystals, at temperatures well above the Debye temperature, and for liquids, at temperatures well below the critical point. It is based on the use of ~ero-order wave functions which closely resemble Bloch functions, with perturbations depending primarily upon the short~range disorder parameters .. Although the method is similar to the one proposed and developed by GUbanov, there is one important distinction: the present approach uses zero-order wave functions that are discontinuous at the primitive cell boundaries. This allows the inclusion of terms in the scattering matrix element that were neglected by Gubanov and, furthermore, gives a straightforward procedure for calculation of all terms in the matrix element.. The perturbation procedure using dis~ continuous wave functions is justified, not rigorously perhaps, hut very plausibly. The quasi-Bloch technique is limited only by the necessity for the existence of a local structure closely resembling that of crystals, and, should therefore be valid for any liquid metal at temperatures well below the critical point 0 This is in contrast to the pseudopotential method of Ziman and others$ which is valid only when the effective electron-ion interaction is smallo The pseudopotential method is probably val,i&lt;;i also in the very high temperature region (near the critical pOint), so the two theories may be considered as cornplementary~ each having its own region of validity, with very little overlap bet,ween regionso The perturbation matrix element in the present theory contains two types of termso One is a contribution due to long=range disorder, which may be estimated in various wayso Since this term is dominant in sodium~ its value for other metals may be obtained from the experimentally determined resistivity of sodium, and from the assumption that the ratio o&#x27;f the nearest=neighbor distance to the mean free path due to long-range disorder is the same for all metals &#x27;at their melting pointso This was Zimanis procedure for estimating his plasma resistance, and the sarne procedure was used hereo The second type of term involves a product of the short= range disorder parameters and various derivatives of the periodic part of the Bloch functions, integrated over the cell boundarieso To avoid the need for a computer in the calculations, the zero-order wave functions were written as solutions of a three=dimensional Kronig=Penn~y mode19 the strength of the potential being related to the band gaps in the solidso It eventually became necessary to approximate these wave functions, so the numerical calculations were of limited validityo They were intended9 however~ as illustrations of the use of the method and do not exhaust its potentialitieso Numerical values of the electron mean free paths were obtained for the liquid alkali and noble metals at the melting pointo The calculated values differed from experimental values by a maximum of ~O percento The agreement was better than that of any previous calculations and was considered satisfactory in view of the uncertainties both in the parameters and in the approximations used in the calculations.","abstract_has_math":false,"creators":["Tefft, Wayne Earl"],"institution":"University of Illinois at Urbana-Champaign","degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Physics","degree_department":null,"school":null,"contributors":["Bardeen, John"],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2011,"date_issued":"2011-05-19T14:58:04Z","date_published":"2011-05-19T14:58:04Z","updated_at":"2026-07-22T22:25:23Z","subjects":["electrical resistivity","liquid metals","electron scattering in metals","zero-order wave functions","Bloch functions","short-range disorder parameters"],"languages":["en"],"rights":["Copyright 1964 Wayne Earl Tefft"],"rights_urls":[],"identifier_entries":[{"key":"dc:identifier","label":"Identifier","values":["6137277"],"render_values":[{"text":"6137277","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/2142/23961","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Bardeen, John"]},{"key":"dc:creator","label":"Author","values":["Tefft, Wayne Earl"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2011-05-19T14:58:04Z","10000-01-01","1964"]},{"key":"dc:type","label":"Dc Type","values":["Dissertation / Thesis","text"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Physics"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Dissertation"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Ph.D."]},{"key":"thesis:institution_name","label":"Thesis Institution Name","values":["University of Illinois at Urbana-Champaign"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["electrical resistivity","liquid metals","electron scattering in metals","zero-order wave functions","Bloch functions","short-range disorder parameters"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["en"]},{"key":"dc:rights","label":"Dc Rights","values":["Copyright 1964 Wayne Earl Tefft"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["6137277","http://hdl.handle.net/2142/23961"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["A new technique for the calculation of electron scatter~ng in metals is proposed and developed. The method is considered valid both for crystals, at temperatures well above the Debye temperature, and for liquids, at temperatures well below the critical point. It is based on the use of ~ero-order wave functions which closely resemble Bloch functions, with perturbations depending primarily upon the short~range disorder parameters .. Although the method is similar to the one proposed and developed by GUbanov, there is one important distinction: the present approach uses zero-order wave functions that are discontinuous at the primitive cell boundaries. This allows the inclusion of terms in the scattering matrix element that were neglected by Gubanov and, furthermore, gives a straightforward procedure for calculation of all terms in the matrix element.. The perturbation procedure using dis~ continuous wave functions is justified, not rigorously perhaps, hut very plausibly. The quasi-Bloch technique is limited only by the necessity for the existence of a local structure closely resembling that of crystals, and, should therefore be valid for any liquid metal at temperatures well below the critical point 0 This is in contrast to the pseudopotential method of Ziman and others$ which is valid only when the effective electron-ion interaction is smallo The pseudopotential method is probably val,i<;i also in the very high temperature region (near the critical pOint), so the two theories may be considered as cornplementary~ each having its own region of validity, with very little overlap bet,ween regionso The perturbation matrix element in the present theory contains two types of termso One is a contribution due to long=range disorder, which may be estimated in various wayso Since this term is dominant in sodium~ its value for other metals may be obtained from the experimentally determined resistivity of sodium, and from the assumption that the ratio o'f the nearest=neighbor distance to the mean free path due to long-range disorder is the same for all metals 'at their melting pointso This was Zimanis procedure for estimating his plasma resistance, and the sarne procedure was used hereo The second type of term involves a product of the short= range disorder parameters and various derivatives of the periodic part of the Bloch functions, integrated over the cell boundarieso To avoid the need for a computer in the calculations, the zero-order wave functions were written as solutions of a three=dimensional Kronig=Penn~y mode19 the strength of the potential being related to the band gaps in the solidso It eventually became necessary to approximate these wave functions, so the numerical calculations were of limited validityo They were intended9 however~ as illustrations of the use of the method and do not exhaust its potentialitieso Numerical values of the electron mean free paths were obtained for the liquid alkali and noble metals at the melting pointo The calculated values differed from experimental values by a maximum of ~O percento The agreement was better than that of any previous calculations and was considered satisfactory in view of the uncertainties both in the parameters and in the approximations used in the calculations.","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-05-19T14:58:04Z No. of bitstreams: 1 1964_tefft.pdf: 5567515 bytes, checksum: c22da737bc7d7375e03532f71bf6207f (MD5)","Made available in DSpace on 2011-05-19T14:58:04Z (GMT). No. of bitstreams: 1 1964_tefft.pdf: 5567515 bytes, checksum: c22da737bc7d7375e03532f71bf6207f (MD5) Previous issue date: 1964","Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-05-19T14:58:04Z Item is restricted indefinitely.","Restriction data tranferred 2014-07-01T11:13:27-05:00 Original Data Group with Access UIUC Users [automated] Release Date: none Reason: Thesis","Thesis","U of I Only"]},{"key":"dc:title","label":"Title","values":["A theory of the electrical resistivity of liquid metals"]}]}],"canonical_facts":{"dc:contributor":["Bardeen, John"],"dc:creator":["Tefft, Wayne Earl"],"dc:date":["2011-05-19T14:58:04Z","10000-01-01","1964"],"dc:description":["A new technique for the calculation of electron scatter~ng in metals is proposed and developed. The method is considered valid both for crystals, at temperatures well above the Debye temperature, and for liquids, at temperatures well below the critical point. It is based on the use of ~ero-order wave functions which closely resemble Bloch functions, with perturbations depending primarily upon the short~range disorder parameters .. Although the method is similar to the one proposed and developed by GUbanov, there is one important distinction: the present approach uses zero-order wave functions that are discontinuous at the primitive cell boundaries. This allows the inclusion of terms in the scattering matrix element that were neglected by Gubanov and, furthermore, gives a straightforward procedure for calculation of all terms in the matrix element.. The perturbation procedure using dis~ continuous wave functions is justified, not rigorously perhaps, hut very plausibly. The quasi-Bloch technique is limited only by the necessity for the existence of a local structure closely resembling that of crystals, and, should therefore be valid for any liquid metal at temperatures well below the critical point 0 This is in contrast to the pseudopotential method of Ziman and others$ which is valid only when the effective electron-ion interaction is smallo The pseudopotential method is probably val,i<;i also in the very high temperature region (near the critical pOint), so the two theories may be considered as cornplementary~ each having its own region of validity, with very little overlap bet,ween regionso The perturbation matrix element in the present theory contains two types of termso One is a contribution due to long=range disorder, which may be estimated in various wayso Since this term is dominant in sodium~ its value for other metals may be obtained from the experimentally determined resistivity of sodium, and from the assumption that the ratio o'f the nearest=neighbor distance to the mean free path due to long-range disorder is the same for all metals 'at their melting pointso This was Zimanis procedure for estimating his plasma resistance, and the sarne procedure was used hereo The second type of term involves a product of the short= range disorder parameters and various derivatives of the periodic part of the Bloch functions, integrated over the cell boundarieso To avoid the need for a computer in the calculations, the zero-order wave functions were written as solutions of a three=dimensional Kronig=Penn~y mode19 the strength of the potential being related to the band gaps in the solidso It eventually became necessary to approximate these wave functions, so the numerical calculations were of limited validityo They were intended9 however~ as illustrations of the use of the method and do not exhaust its potentialitieso Numerical values of the electron mean free paths were obtained for the liquid alkali and noble metals at the melting pointo The calculated values differed from experimental values by a maximum of ~O percento The agreement was better than that of any previous calculations and was considered satisfactory in view of the uncertainties both in the parameters and in the approximations used in the calculations.","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-05-19T14:58:04Z No. of bitstreams: 1 1964_tefft.pdf: 5567515 bytes, checksum: c22da737bc7d7375e03532f71bf6207f (MD5)","Made available in DSpace on 2011-05-19T14:58:04Z (GMT). No. of bitstreams: 1 1964_tefft.pdf: 5567515 bytes, checksum: c22da737bc7d7375e03532f71bf6207f (MD5) Previous issue date: 1964","Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-05-19T14:58:04Z Item is restricted indefinitely.","Restriction data tranferred 2014-07-01T11:13:27-05:00 Original Data Group with Access UIUC Users [automated] Release Date: none Reason: Thesis","Thesis","U of I Only"],"dc:identifier":["6137277","http://hdl.handle.net/2142/23961"],"dc:language":["en"],"dc:rights":["Copyright 1964 Wayne Earl Tefft"],"dc:subject":["electrical resistivity","liquid metals","electron scattering in metals","zero-order wave functions","Bloch functions","short-range disorder parameters"],"dc:title":["A theory of the electrical resistivity of liquid metals"],"dc:type":["Dissertation / Thesis","text"],"thesis:degree_discipline":["Physics"],"thesis:degree_level":["Dissertation"],"thesis:degree_name":["Ph.D."],"thesis:institution_name":["University of Illinois at Urbana-Champaign"]},"updated_at":"2026-07-22T22:25:23Z"}