跳转到内容

铁基超导体

维基百科,自由的百科全书
LnFePnO的晶体结构,它是ferropnictide化合物之一。

铁基超导体是指化合物中含有,在低温时具有超导现象,且扮演形成超导的主体的材料。2006年日本东京工业大学细野秀雄教授的团队发现第一个以为超导主体的化合物LaFeOP[1],打破以往普遍认定元素不利形成超导迷思。

根据BCS理论,产生超导性的必要条件是材料中的电子必须配对,这样配对的电子称为库柏对库柏对中的两个电子自旋相反,所以总自旋为零,因而科学家认为超导性铁磁性可能无法共存,材料中如果加入磁性元素(如)会大大降低超导性。铁基超导体虽然含有元素且是产生超导的主体,但是和其他元素(如)形成铁基平面后,已不再具有铁磁性

2008年1月9日,细野秀雄教授的团队再度发现铁基层状材料La[O1-xFx]FeAs(x = 0.05 – 0.12)在绝对温度26K时存在超导性[2]。2008年2月26日,细野团队又发现其在绝对温度43 K的超导性[3]。2008年3月28日,中国科学院物理研究所赵忠贤领导的科研小组报告,氟掺杂镨氧铁砷化合物的高温超导临界温度可达52 K(-221.15 ℃)。4月13日该科研小组又有新发现:氟掺杂钐氧铁砷化合物假如在压力环境下产生作用,其超导临界温度可进一步提升至55 K(-218.15 ℃)。此外,中科院物理所闻海虎领导的科研小组还报告,锶掺杂镧氧铁砷化合物的超导临界温度为25 K(-248.15 ℃)[4],从此研究铁基超导体便在世界上形成一股热潮。引起许多科学家的兴趣的重要原因之一在于铁基超导体的结构与高温超导的铜氧平面类似,超导性发生在铁基平面上,属于二维的超导材料。因此尽管铁基超导体的临界温度只有数十开尔文,研究铁基超导体可能有助于了解高温超导的机制。

晶格结构

[编辑]

现有的铁基超导体从结构上可分为四类:(1111)、(122)、(111) 和 (11)。

氮磷族氧化物
(oxypnictide)
临界温度 (K)
LaO0.89F0.11FeAs 26[5]
LaO0.9F0.2FeAs 28.5[6]
CeFeAsO0.84F0.16 41[5]
SmFeAsO0.9F0.1 43[5]
La0.5Y0.5FeAsO0.6 43.1[7]
NdFeAsO0.89F0.11 52[5]
PrFeAsO0.89F0.11 52[8]
ErFeAsO1-y 45[9]
Al-32522 (CaAlOFeAs) 30(As), 16.6 (P)[10]
Al-42622 (CaAlOFeAs) 28.3(As), 17.2 (P)[11]
GdFeAsO0.85 53.5[12]
BaFe1.8Co0.2As2 25.3[13]
SmFeAsO~0.85 55[14]
氮磷族氧化物
(non-oxypnictide)
临界温度 (K)
Ba0.6K0.4Fe2As2 38[15]
Ca0.6Na0.4Fe2As2 26[16]
CaFe0.9Co0.1AsF 22[17]
Sr0.5Sm0.5FeAsF 56[18]
LiFeAs <18 [19] [20][21]
NaFeAs 9–25[22][23]
FeSe <27[24][25]

参见

[编辑]

参考文献

[编辑]
  1. ^ Yoichi Kamihara, Hidenori Hiramatsu, Masahiro Hirano, Ryuto Kawamura, Hiroshi Yanagi, Toshio Kamiya, and Hideo Hosono. Iron-Based Layered Superconductor: LaOFeP. Journal of American Chemical Society. 2006, 128 (31): 10012–10013. doi:10.1021/ja063355c. 
  2. ^ Iron-Based Layered Superconductor La〔O1-xFx〕FeAs (x = 0.05−0.12) with Tc = 26 K - Journal of the American Chemical Society (ACS Publications). [2015-04-06]. (原始内容存档于2014-07-10). 
  3. ^ Access : Superconductivity at 43|〔thinsp〕|K in an iron-based layered compound LaO1-xFxFeAs : Nature. [2015-04-06]. (原始内容存档于2010-01-05). 
  4. ^ Yoichi Kamihara, Takumi Watanabe, Masahiro Hirano, and Hideo Hosono. Iron-Based Layered Superconductor La[O1-xFx]FeAs (x = 0.05-0.12) with Tc = 26 K. Journal of American Chemical Society. 2008, 130 (11): 3296–3297. doi:10.1021/ja800073m. 
  5. ^ 5.0 5.1 5.2 5.3 K. Ishida; et al. To What Extent Iron-Pnictide New Superconductors Have Been Clarified: A Progress Report. J. Phys. Soc. Jpn. 2009, 78 (6): 062001. Bibcode:2009JPSJ...78f2001I. arXiv:0906.2045可免费查阅. doi:10.1143/JPSJ.78.062001. 
  6. ^ Prakash, J.; Singh, S. J.; Samal, S. L.; Patnaik, S.; Ganguli, A. K. Potassium fluoride doped LaOFeAs multi-band superconductor: Evidence of extremely high upper critical field. EPL (Europhysics Letters). 2008, 84 (5): 57003. Bibcode:2008EL.....8457003P. doi:10.1209/0295-5075/84/57003. 
  7. ^ Shirage, Parasharam M.; Miyazawa, Kiichi; Kito, Hijiri; Eisaki, Hiroshi; Iyo, Akira. Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1‑xYxFeAsOy. Physical Review B. 2008, 78 (17): 172503. Bibcode:2008PhRvB..78q2503S. doi:10.1103/PhysRevB.78.172503. 
  8. ^ Ren, Z. A.; Yang, J.; Lu, W.; Yi, W.; Che, G. C.; Dong, X. L.; Sun, L. L.; Zhao, Z. X. Superconductivity at 52 K in iron based F doped layered quaternary compound Pr[O1–xFx]FeAs. Materials Research Innovations. 2008, 12 (3): 105. doi:10.1179/143307508X333686. 
  9. ^ Shirage, Parasharam M.; Miyazawa, Kiichi; Kihou, Kunihiro; Lee, Chul-Ho; Kito, Hijiri; Tokiwa, Kazuyasu; Tanaka, Yasumoto; Eisaki, Hiroshi; Iyo, Akira. Synthesis of ErFeAsO-based superconductors by the hydrogen doping method. EPL (Europhysics Letters). 2010, 92 (5): 57011. Bibcode:2010EL.....9257011S. arXiv:1011.5022可免费查阅. doi:10.1209/0295-5075/92/57011. 
  10. ^ Shirage, Parasharam M.; Kihou, Kunihiro; Lee, Chul-Ho; Kito, Hijiri; Eisaki, Hiroshi; Iyo, Akira. Emergence of Superconductivity in "32522" Structure of (Ca3Al2O5–y)(Fe2Pn2) (Pn = As and P). Journal of the American Chemical Society. 2011, 133 (25): 9630–3. PMID 21627302. doi:10.1021/ja110729m. 
  11. ^ Shirage, Parasharam M.; Kihou, Kunihiro; Lee, Chul-Ho; Kito, Hijiri; Eisaki, Hiroshi; Iyo, Akira. Superconductivity at 28.3 and 17.1 K in (Ca[sub 4]Al[sub 2]O[sub 6−y])(Fe[sub 2]Pn[sub 2]) (Pn=As and P). Applied Physics Letters. 2010, 97 (17): 172506. Bibcode:2010ApPhL..97q2506S. arXiv:1008.2586可免费查阅. doi:10.1063/1.3508957. 
  12. ^ Yang, Jie; Li, Zheng-Cai; Lu, Wei; Yi, Wei; Shen, Xiao-Li; Ren, Zhi-An; Che, Guang-Can; Dong, Xiao-Li; Sun, Li-Ling. Superconductivity at 53.5 K in GdFeAsO1−δ. Superconductor Science and Technology. 2008, 21 (8): 082001. Bibcode:2008SuScT..21h2001Y. doi:10.1088/0953-2048/21/8/082001. 
  13. ^ Yin, Yi; Zech, M.; Williams, T. L.; Wang, X. F.; Wu, G.; Chen, X. H.; Hoffman, J. E. Scanning Tunneling Spectroscopy and Vortex Imaging in the Iron Pnictide Superconductor BaFe_{1.8}Co_{0.2}As_{2}. Physical Review Letters. 2009, 102 (9). Bibcode:2009PhRvL.102i7002Y. arXiv:0810.1048v2可免费查阅. doi:10.1103/PhysRevLett.102.097002. 
  14. ^ Ren, Zhi-An; Che, Guang-Can; Dong, Xiao-Li; Yang, Jie; Lu, Wei; Yi, Wei; Shen, Xiao-Li; Li, Zheng-Cai; Sun, Li-Ling. Superconductivity and phase diagram in iron-based arsenic-oxides ReFeAsO1−δ (Re = rare-earth metal) without fluorine doping. EPL (Europhysics Letters). 2008, 83: 17002. Bibcode:2008EL.....8317002R. arXiv:0804.2582可免费查阅. doi:10.1209/0295-5075/83/17002. 
  15. ^ Marianne Rotter, Marcus Tegel, and Dirk Johrendt. Superconductivity at 38 K in the Iron Arsenide (Ba1-xKx)Fe2As2. Physical Review Letters. 2008, 101 (10): 107006. Bibcode:2008PhRvL.101j7006R. PMID 18851249. arXiv:0805.4630可免费查阅. doi:10.1103/PhysRevLett.101.107006. 
  16. ^ Shirage, Parasharam Maruti; Miyazawa, Kiichi; Kito, Hijiri; Eisaki, Hiroshi; Iyo, Akira. Superconductivity at 26 K in (Ca1-xNax)Fe2As2. Applied Physics Express. 2008, 1: 081702. doi:10.1143/APEX.1.081702. 
  17. ^ Satoru Matsuishi, Yasunori Inoue, Takatoshi Nomura, Hiroshi Yanagi, Masahiro Hirano and Hideo Hosono. Superconductivity Induced by Co-Doping in Quaternary Fluoroarsenide CaFeAsF. J. Am. Chem. Soc. 2008, 2008 (44): 14428–14429 [2013-09-27]. PMID 18842039. doi:10.1021/ja806357j. (原始内容存档于2020-08-11). 
  18. ^ G. Wu, Y. L. Xie, H. Chen, M. Zhong, R. H. Liu, B. C. Shi, Q. J. Li, X. F. Wang, T. Wu, Y. J. Yan, J. J. Ying, and X. H. Chen. Superconductivity at 56 K in Samarium-doped SrFeAsF. Journal of Physics: Condensed Matter , (2009). 2008, 21 (3). Bibcode:2008arXiv0811.0761W. arXiv:0811.0761可免费查阅. 
  19. ^ X. C. Wang, Q. Q. Liu, Y. X. Lv, W. B. Gao, L. X. Yang, R.C. Yu, F. Y. Li, and C. Q. Jin. The superconductivity at 18 K in LiFeAs system. Solid State Commun. 2008, 148: 538. arXiv:0806.4688可免费查阅. 
  20. ^ Michael J. Pitcher; et al. Structure and superconductivity of LiFeAs. Chem. Commun. 2008, 2008 (45): 5918–5920. PMID 19030538. doi:10.1039/b813153h. 
  21. ^ Joshua H. Tapp; et al. LiFeAs: An intrinsic FeAs-based superconductor with Tc=18 K. Physical Review B. 2008, 78 (6): 060505(R). Bibcode:2008PhRvB..78f0505T. arXiv:0807.2274可免费查阅. doi:10.1103/PhysRevB.78.060505. 
  22. ^ C. W. Chu; et al. The Synthesis and Characterization of LiFeAs and NaFeAs. 2009. arXiv:0902.0806可免费查阅 [cond-mat.supr-con]. 
  23. ^ Dinah R. Parker, Michael J. Pitcher, and Simon J. Clarke. Structure and superconductivity of the layered iron arsenide NaFeAs. Chemical Communications. 2008, 2189 (16): 2189. arXiv:0810.3214可免费查阅. doi:10.1039/B818911K. 
  24. ^ Fong-Chi Hsu; et al. Superconductivity in the PbO-type structure α-FeSe. PNAS. 2008, 105 (38): 14262–14264. Bibcode:2008PNAS..10514262H. PMC 2531064可免费查阅. PMID 18776050. doi:10.1073/pnas.0807325105. 
  25. ^ Yoshikazu Mizuguchi, Fumiaki Tomioka, Shunsuke Tsuda, Takahide Yamaguchi, and Yoshihiko Takano. Superconductivity at 27 K in tetragonal FeSe under high pressure. Appl. Phys. Lett. 2008, 93 (15): 152505. Bibcode:2008ApPhL..93o2505M. arXiv:0807.4315可免费查阅. doi:10.1063/1.3000616.