High-resolution angle-resolved photoemission study of Pb-substituted Bi2201
We have performed a systematic doping-dependent angle-resolved photoemission spectroscopy (ARPES) of Pb-substituted Bi2201 (Bi 1.80Pb 0.38Sr 2.01CuO 6− δ ) with high energy (7–11 meV) and momentum (0.01 Å −1) resolutions. We found that all the samples show a large hole-like Fermi surface centered at...
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Veröffentlicht in: | The Journal of physics and chemistry of solids 2001, Vol.62 (1), p.157-161 |
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creator | Sato, T. Naitoh, Y. Kamiyama, T. Takahashi, T. Yokoya, T. Mesot, J. Kaminski, A. Fretwell, H. Campuzano, J.C. Ding, H. Chong, I. Terashima, T. Takano, M. Kadowaki, K. |
description | We have performed a systematic doping-dependent angle-resolved photoemission spectroscopy (ARPES) of Pb-substituted Bi2201 (Bi
1.80Pb
0.38Sr
2.01CuO
6−
δ
) with high energy (7–11
meV) and momentum (0.01
Å
−1) resolutions. We found that all the samples show a large hole-like Fermi surface centered at (π,π), whose volume changes systematically as a function of doping. The superconducting gap exhibits a d
x
2−
y
2
-like anisotropy with a typical gap value of 10–15
meV near (π,0). By comparing with Bi
2Sr
2CaCu
2O
8 (Bi2212), we found that the size of superconducting gap is well scaled with the maximum
T
c (
T
c
max). Doping-dependence of spectral line shape at (π,0) is very similar between Bi2201 and Bi2212, while its energy scale is different by a factor of 4, corresponding to the ratio of
T
c
max between the two compounds. These indicate that the superconducting and pseudogap properties are characterized by
T
c
max irrespective of the number of CuO
2 layers or the BiO superstructure. |
doi_str_mv | 10.1016/S0022-3697(00)00119-0 |
format | Article |
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1.80Pb
0.38Sr
2.01CuO
6−
δ
) with high energy (7–11
meV) and momentum (0.01
Å
−1) resolutions. We found that all the samples show a large hole-like Fermi surface centered at (π,π), whose volume changes systematically as a function of doping. The superconducting gap exhibits a d
x
2−
y
2
-like anisotropy with a typical gap value of 10–15
meV near (π,0). By comparing with Bi
2Sr
2CaCu
2O
8 (Bi2212), we found that the size of superconducting gap is well scaled with the maximum
T
c (
T
c
max). Doping-dependence of spectral line shape at (π,0) is very similar between Bi2201 and Bi2212, while its energy scale is different by a factor of 4, corresponding to the ratio of
T
c
max between the two compounds. These indicate that the superconducting and pseudogap properties are characterized by
T
c
max irrespective of the number of CuO
2 layers or the BiO superstructure.</description><identifier>ISSN: 0022-3697</identifier><identifier>EISSN: 1879-2553</identifier><identifier>DOI: 10.1016/S0022-3697(00)00119-0</identifier><language>eng</language><publisher>United States: Elsevier Ltd</publisher><subject>A. Oxides ; ANISOTROPY ; C. Photoelectron spectroscopy ; D. Superconductivity ; FERMI LEVEL ; INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY ; PHOTOEMISSION ; RESOLUTION ; SHAPE ; SPECTROSCOPY</subject><ispartof>The Journal of physics and chemistry of solids, 2001, Vol.62 (1), p.157-161</ispartof><rights>2000 Elsevier Science Ltd</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c380t-cf4151f33cb70b6740318eccbe249f7b69add5ab0bb15880f1f17250fa556ed93</citedby><cites>FETCH-LOGICAL-c380t-cf4151f33cb70b6740318eccbe249f7b69add5ab0bb15880f1f17250fa556ed93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/S0022-3697(00)00119-0$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>230,315,781,785,886,3551,4025,27927,27928,27929,45999</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/949481$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Sato, T.</creatorcontrib><creatorcontrib>Naitoh, Y.</creatorcontrib><creatorcontrib>Kamiyama, T.</creatorcontrib><creatorcontrib>Takahashi, T.</creatorcontrib><creatorcontrib>Yokoya, T.</creatorcontrib><creatorcontrib>Mesot, J.</creatorcontrib><creatorcontrib>Kaminski, A.</creatorcontrib><creatorcontrib>Fretwell, H.</creatorcontrib><creatorcontrib>Campuzano, J.C.</creatorcontrib><creatorcontrib>Ding, H.</creatorcontrib><creatorcontrib>Chong, I.</creatorcontrib><creatorcontrib>Terashima, T.</creatorcontrib><creatorcontrib>Takano, M.</creatorcontrib><creatorcontrib>Kadowaki, K.</creatorcontrib><creatorcontrib>Argonne National Lab. (ANL), Argonne, IL (United States)</creatorcontrib><title>High-resolution angle-resolved photoemission study of Pb-substituted Bi2201</title><title>The Journal of physics and chemistry of solids</title><description>We have performed a systematic doping-dependent angle-resolved photoemission spectroscopy (ARPES) of Pb-substituted Bi2201 (Bi
1.80Pb
0.38Sr
2.01CuO
6−
δ
) with high energy (7–11
meV) and momentum (0.01
Å
−1) resolutions. We found that all the samples show a large hole-like Fermi surface centered at (π,π), whose volume changes systematically as a function of doping. The superconducting gap exhibits a d
x
2−
y
2
-like anisotropy with a typical gap value of 10–15
meV near (π,0). By comparing with Bi
2Sr
2CaCu
2O
8 (Bi2212), we found that the size of superconducting gap is well scaled with the maximum
T
c (
T
c
max). Doping-dependence of spectral line shape at (π,0) is very similar between Bi2201 and Bi2212, while its energy scale is different by a factor of 4, corresponding to the ratio of
T
c
max between the two compounds. These indicate that the superconducting and pseudogap properties are characterized by
T
c
max irrespective of the number of CuO
2 layers or the BiO superstructure.</description><subject>A. Oxides</subject><subject>ANISOTROPY</subject><subject>C. Photoelectron spectroscopy</subject><subject>D. Superconductivity</subject><subject>FERMI LEVEL</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>PHOTOEMISSION</subject><subject>RESOLUTION</subject><subject>SHAPE</subject><subject>SPECTROSCOPY</subject><issn>0022-3697</issn><issn>1879-2553</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><recordid>eNqFkE1LxDAQhoMouK7-BKHe9BCdaZu2OYkufuGCgnoOTZrsRnabJUkX9t_bbsWrp4GZZx5mXkLOEa4RsLj5AEhTmhW8vAS4AkDkFA7IBKuS05Sx7JBM_pBjchLCNwAw5Dghr892saReB7fqonVtUreLlR4bW90km6WLTq9tCMMwxK7ZJc4k75KGToZoYxd76t6mKeApOTL1Kuiz3zolX48Pn7NnOn97epndzanKKohUmRwZmixTsgRZlDlkWGmlpE5zbkpZ8LppWC1BSmRVBQYNlikDUzNW6IZnU3Ixel1_gAjKRq2WyrWtVlHwnOcV9gwbGeVdCF4bsfF2XfudQBBDamKfmhgiEQBin5qAfu923NP9A1ur_eDXrdKN9YO-cfYfww9Y0XQ1</recordid><startdate>2001</startdate><enddate>2001</enddate><creator>Sato, T.</creator><creator>Naitoh, Y.</creator><creator>Kamiyama, T.</creator><creator>Takahashi, T.</creator><creator>Yokoya, T.</creator><creator>Mesot, J.</creator><creator>Kaminski, A.</creator><creator>Fretwell, H.</creator><creator>Campuzano, J.C.</creator><creator>Ding, H.</creator><creator>Chong, I.</creator><creator>Terashima, T.</creator><creator>Takano, M.</creator><creator>Kadowaki, K.</creator><general>Elsevier Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>2001</creationdate><title>High-resolution angle-resolved photoemission study of Pb-substituted Bi2201</title><author>Sato, T. ; Naitoh, Y. ; Kamiyama, T. ; Takahashi, T. ; Yokoya, T. ; Mesot, J. ; Kaminski, A. ; Fretwell, H. ; Campuzano, J.C. ; Ding, H. ; Chong, I. ; Terashima, T. ; Takano, M. ; Kadowaki, K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c380t-cf4151f33cb70b6740318eccbe249f7b69add5ab0bb15880f1f17250fa556ed93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2001</creationdate><topic>A. Oxides</topic><topic>ANISOTROPY</topic><topic>C. Photoelectron spectroscopy</topic><topic>D. Superconductivity</topic><topic>FERMI LEVEL</topic><topic>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</topic><topic>PHOTOEMISSION</topic><topic>RESOLUTION</topic><topic>SHAPE</topic><topic>SPECTROSCOPY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sato, T.</creatorcontrib><creatorcontrib>Naitoh, Y.</creatorcontrib><creatorcontrib>Kamiyama, T.</creatorcontrib><creatorcontrib>Takahashi, T.</creatorcontrib><creatorcontrib>Yokoya, T.</creatorcontrib><creatorcontrib>Mesot, J.</creatorcontrib><creatorcontrib>Kaminski, A.</creatorcontrib><creatorcontrib>Fretwell, H.</creatorcontrib><creatorcontrib>Campuzano, J.C.</creatorcontrib><creatorcontrib>Ding, H.</creatorcontrib><creatorcontrib>Chong, I.</creatorcontrib><creatorcontrib>Terashima, T.</creatorcontrib><creatorcontrib>Takano, M.</creatorcontrib><creatorcontrib>Kadowaki, K.</creatorcontrib><creatorcontrib>Argonne National Lab. (ANL), Argonne, IL (United States)</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>The Journal of physics and chemistry of solids</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sato, T.</au><au>Naitoh, Y.</au><au>Kamiyama, T.</au><au>Takahashi, T.</au><au>Yokoya, T.</au><au>Mesot, J.</au><au>Kaminski, A.</au><au>Fretwell, H.</au><au>Campuzano, J.C.</au><au>Ding, H.</au><au>Chong, I.</au><au>Terashima, T.</au><au>Takano, M.</au><au>Kadowaki, K.</au><aucorp>Argonne National Lab. (ANL), Argonne, IL (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>High-resolution angle-resolved photoemission study of Pb-substituted Bi2201</atitle><jtitle>The Journal of physics and chemistry of solids</jtitle><date>2001</date><risdate>2001</risdate><volume>62</volume><issue>1</issue><spage>157</spage><epage>161</epage><pages>157-161</pages><issn>0022-3697</issn><eissn>1879-2553</eissn><abstract>We have performed a systematic doping-dependent angle-resolved photoemission spectroscopy (ARPES) of Pb-substituted Bi2201 (Bi
1.80Pb
0.38Sr
2.01CuO
6−
δ
) with high energy (7–11
meV) and momentum (0.01
Å
−1) resolutions. We found that all the samples show a large hole-like Fermi surface centered at (π,π), whose volume changes systematically as a function of doping. The superconducting gap exhibits a d
x
2−
y
2
-like anisotropy with a typical gap value of 10–15
meV near (π,0). By comparing with Bi
2Sr
2CaCu
2O
8 (Bi2212), we found that the size of superconducting gap is well scaled with the maximum
T
c (
T
c
max). Doping-dependence of spectral line shape at (π,0) is very similar between Bi2201 and Bi2212, while its energy scale is different by a factor of 4, corresponding to the ratio of
T
c
max between the two compounds. These indicate that the superconducting and pseudogap properties are characterized by
T
c
max irrespective of the number of CuO
2 layers or the BiO superstructure.</abstract><cop>United States</cop><pub>Elsevier Ltd</pub><doi>10.1016/S0022-3697(00)00119-0</doi><tpages>5</tpages><oa>free_for_read</oa></addata></record> |
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subjects | A. Oxides ANISOTROPY C. Photoelectron spectroscopy D. Superconductivity FERMI LEVEL INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY PHOTOEMISSION RESOLUTION SHAPE SPECTROSCOPY |
title | High-resolution angle-resolved photoemission study of Pb-substituted Bi2201 |
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