欢迎登录材料期刊网

材料期刊网

高级检索

采用溶胶-凝胶方法合成了名义组分为Bi2Sr2-xCaxCuO6+δ(x=0.1、0.3、0.5、0.7和0.9)的系列样品,运用 XRD、TEM和四引线法,研究了钙掺杂对Bi-2201相晶体结构、点阵参数、非公度调制结构和超导临界转变开始温度(T C,onset )的影响。研究发现,钙原子已进入到 Bi-2201单胞内部,在整个掺杂体系内,Bi-2201单胞都能够维持正交点阵;随着钙掺杂量增加,正交单胞的c 轴长度逐渐减小,而当x>0.3时,Bi-2201相调制波矢的b 轴分量逐渐减小,而c 轴分量有所上升;电阻随温度变化曲线表明,当x=0.3时,T C,onset 达到最高,之后有所下降,这与调制波矢在b 轴分量的变化相一致,这种变化能够用晶格失配模型很好地解释。

A series of samples with the nominal composition of Bi2Sr2-xCaxCuO6+δ(x=0.1,0.3,0.5,0.7,0.9) were prepared by sol-gel method.By means of XRD,TEM and standard four-probe technique,it was investiga-ted that the effects of Ca doping on lattice types and parameters of Bi-2201 phase,the incommensurate modula-tion structure and the onset temperature of superconducting critical transition (TC,onset ).It was found that Bi-2201 phase with orthorhombic symmetry can be maintained with the introduction of Ca2+ in the whole doping range.With increasing x,lattice parameter c was decreasing gradually.When x>0.3,the b* component of the modulation wave vector was decreasing while the c* component was increasing with increasing x.Experi-mental R-T curves show that TC,onset was the highest when x=0.3,and then has a declining trend with increas-ing x,which was in agreement with the variation of the b* component of the modulation wave vector and can be interpreted by the crystal misfit model.

参考文献

[1] M. C. Boyer;W. D. Wise;Kamalesh Chatterjee;Ming Yi;Takeshi Kondo;T. Takeuchi;H. Ikuta;E. W. Hudson .Imaging the two gaps of the high-temperature superconductor Bi_2Sr_2CuO_(6+x)[J].Nature physics,2007(11):802-806.
[2] Wise WD;Boyer MC;Chatterjee K;Kondo T;Takeuchi T;Ikuta H;Wang YY;Hudson EW .Charge-density-wave origin of cuprate checkerboard visualized by scanning tunnelling microscopy[J].Nature physics,2008(9):696-699.
[3] Arao Y;Tange M;Ikeda H;Koyano T;Yoshizaki R .A new aspect of superconductivity observed (Bi, Pb)(2)(Sr, La)(2)CuO6+delta single crystals[J].Physica, C. Superconductivity and its applications,2006(0):440-442.
[4] Yoshizaki R;Nakajima T;Tange M .Ca substitution effect for Sr upon superconductivity of Bi2.1 Cay Sr1.9-y CuO6+δ[J].Japanese Journal of Applied Physics,2007,46(8-11):L167-L169.
[5] Nakajima T;Tange M;Kizuka T;Ikeda H;Yoshizaki R;Sasaki S .80 K superconductivity in Bi-2201 phase[J].Physica, C. Superconductivity and its applications,2007(0):93-95.
[6] 陈源清,赵高扬,薛人中,严复学,李颖.溶胶-凝胶法制备YBa2Cu3O7-x超导薄膜的研究[J].功能材料,2006(09):1423-1425,1428.
[7] 雷家珩;唐福龙;袁启华 .溶胶-凝胶法制备 YBa2 Cu3 O7-δ超细粉体及其性质[J].功能材料,1994,25(02):127-131.
[8] Torardi C C;Subramanian M A;Calabrese J C et al.Structures of the superconducting oxides Tl2 Ba2 CuO6 and Bi2Sr2CuO6[J].Physical Review B:Condensed Matter,1998,38(01):225-231.
[9] Wongng W.;Rawn CJ.;Roth RS. .PREPARATION AND STRUCTURAL INVESTIGATION OF BI-16(SR,CA)(14)O-38[J].Journal of the American Ceramic Society,1997(2):324-328.
[10] Zandbergen H W;Groen W A;Mijlhoff F C et al.Mod-els for the modulation in A2B2CanCu1+nO6+2n,A,B=Bi,Sr or Tl,Ba and n=0,1,2[J].Physica C,1988,156(03):325-354.
[11] Mao Zhiqiang;Fan Chenggao;Shi Lei et al.Multiple Bi2 Sr2-x Bax CuOy microstructures and the effect of ele-ment doping(Ba,La,Pb)on the 2:2:0:1 phase[J].Physical Review B,1993,47(21):14467-14475.
[12] Van Tendeloo G;Zandbergen H W;Van Landuyt J et al.The defect structure of the high-TC superconductors in the system Bi-Ca-Sr-Cu-O[J].Applied Physics A:Materials Science and Processing,1988,46(02):153-158.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%