1、http:/- 1 -中国科技论文在线高温超导体铜氧面上的电偶极子晶格 AA*作者简介：AAA1969AAAAAAAAAAAAAAAAAAAA. E-mail: dong_（北京应用物理与计算数学研究所,北京，100094）5 摘要：AAA论AAAAAAAAAAAA论AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA。AAAAAAAAAAAAAAAA文AAAAAAAA。AAAAAAAAAAAAAAA在AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA。在AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA
2、AAAAAAAAA10AAAAAAAAAAAAAAAAAAAAAAAAAA。A文AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA。在AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA线AdAAAAAAAAAAAAAAA线AAAAAAAAAAA。15 关键词：AAAAAAAAAAAAAdAAAAAAAAA中图分类号：74.20.-z,74.20.Mn,74.20.Rp,74.72 -hExisting of dipole lattice on CuO2 pl
3、ane of cuprate superconductor20 Dong Hang(Institute of applied physics and computational mathematics,Beijing,100094)Abstract: The existing theory about the cuprate superconductor bases on band theory, all neglects the position difference of Cu-O ions on plane, and assumes that the charge on ions are
4、 averagely distributed. Considering that the nature of conduction is the moving of electrons, carrier 25 means electron in this article. The charge opposite the carriers distributes on fixed ions, and the position difference of Cu-O ions slightly violates average electricity distribution, so the con
5、cept of hole is not suitable. It is proved that, near the optimal doping level, since the density of ions is relatively low, the violations can be treated as a perturbation, and the ion lattice can be seen as a combination of regular lattice and dipole lattice. Considering about that the character o
6、f cuprate 30 superconductor is mainly dominated by the dipole lattice, the pairing mechanism, the d-wave symmetry, and the linear temperature dependence of normal state resistivity is tersely interpreted. Key words: high temperature superconductor; electricity dipole lattice; phase diagram; d-wave s
7、ymmetry; normal state35 0AAAA20AAAAAAAAAAAAAAAAAAAAAAAA1-5: AAAAAAAA在AAAAAAAAAAA线AdAAAAAAAAAAAAAAAAAAAAAA线AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA在AAAA6, AAA在AAAAAAAAAAAA7A40AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA论AAAAAAAAAAAAAA论AAAAAAAAAAAAAAAAAAAAAAAA在AAAAAAAAAAAAAAAAAAAAAAAAAAAAA8,9AAAA论AAAAAAAAAAA
8、AAAAAAAAAAAAAAAAA10Ahttp:/- 2 -中国科技论文在线A文AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA45AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA文中AAAAAAAAAAAAAAA在AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA2Cu12O1Cu22Cu1O21AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA中AAAAAAAAAAAAA1250AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA2u1AAAAAA1AAAAA
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10、A60AAAAAAAAAA线AAAAAAAAAAAAAAAAAAAAAA论AAAAA1AAAAAAAA在AA1AAAAAAAAAAAAAAAAAACu-OAAAbAAAAAAA2CuOAAAAAAAAAAAAAAAA0x0a00/xb65A1 AAAAAAFig.1 Illustration of ion lattice在AAAAAAAAAAAAAAAAAAAAAAAAA1AAAAAE0aA在AAAAAAAAA0.15AAAAAAAAAAAAAAAA在Cu AA0xc0xA O AAAAAAAAAA AAAAAAAAAAAAAAAACuPO12OCuP70AAAAAAAAAAAAAAAAAAA
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12、 AAAAAAAAAAAAAAAAAjAAAAAAAAAAAAAAAA:0a80 (4) jiCuefdipoljiefdipole rPabEraE,32302,02 1414AAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAA0AAAAAAAAAAAAAAAAAAA-AAAAAAAAAAA AAAAAdipoleEAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA在AAAAAAAAAAA AAAAAAAAAAAAA2c dipoleE85AAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAA2CuOAAA
13、AAAAAAAAAAAAAAA4AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAA2CuO90 2AAAAAAAAAA2.1AAAAAAAA2 AAAAAAAFig.2 Illutration of paring mechanismhttp:/- 4 -中国科技论文在线95A2 AAAAAAAAAAAAAAAAAAAAAAAAAA中2R AAAAAAAAAAAAAAb AAA R11AAAAAAAAAAAAAAAAAAAAAAAAAAAAAACu AAAAAAAAO
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18、c14AAAAAAAAAAAAAAAAAA文AAAA)6.(.8c135AAAAAAAAAAAAAAAAAAAA3AAA论A线AAAA线AAAFig.3 Comparing of theoretical and empirical curve140 2.3 AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA论AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA145AAAAAAAAAAA
19、AAAAA在AAAAAAAAAA在,AA在AAAAAAAcTAAAAAAAAAAAAAAAAAAAAAAA在AAAAAAAAAAAAAAAhttp:/- 6 -中国科技论文在线AAAAAAAAAAAAcT2.4 dAAAAAAAAAAA在AAAAAAAAAAAAAAA在Cu-OAAAAAAAAA150AdAAAAAAA5AAAAAAAAA2.5 AAAAAAAAAA线AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA155在AAAAAAAAAAAAAAAAAAAAA, AAAAAAA
20、AAAAcTcBTkAAAAAAAAA在AA, AAAAAAAAAAAAAAAAAAAAcBTk43AAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAANAAAAA15 , AAAAAAAd 2/1NdAAAAAAAAAAAAAAA160A11A2)1(/CureguladipoPTAAAA11AAAAAAAAAAAAAAAAA AAAAAAAAAAAdipoleTA. AA AAAAA AAAAAAAAAAA在AAreguladdipolecT3/ilAAAAAAAAAAAAAAA线AAA16A 165 3A论A文AA论AAAAAAAAAAAAAA在AAAAAAAAAA
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22、AAAAAAAAAAAAAAAAAAAA175A文AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA文AAAarXiv:1201.6435A参考文献 (References)1 T.Kondo, R.Khasanov,J. Karpinski,et al.Dual Character of the Electronic Structure of YBa2Cu4O8: The Conduction Bands of CuO2 Planes and CuO ChainsJ.Phys. Rev. Lett. ,2007,98(1570
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