{"title":"用交流磁化率测定Bi(Pb)-Sr-Ca-Cu-O超导体中Ni取代Cu的研究","authors":"N. Pathmanathan, A. Thomson","doi":"10.4038/SLJP.V3I0.185","DOIUrl":null,"url":null,"abstract":"st1\\:*{behavior:url(#ieooui) } \n /* Style Definitions */ \n table.MsoNormalTable \n {mso-style-name:\"Table Normal\"; \n mso-tstyle-rowband-size:0; \n mso-tstyle-colband-size:0; \n mso-style-noshow:yes; \n mso-style-parent:\"\"; \n mso-padding-alt:0cm 5.4pt 0cm 5.4pt; \n mso-para-margin:0cm; \n mso-para-margin-bottom:.0001pt; \n mso-pagination:widow-orphan; \n font-size:10.0pt; \n font-family:\"Times New Roman\"; \n mso-ansi-language:#0400; \n mso-fareast-language:#0400; \n mso-bidi-language:#0400;} \n In this work we have investigated the effect of doping of magnetic element Ni for copper into the copper site of Bi(Pb)-Sr-Ca-Cu-O superconductor by means of AC magnetic susceptibility measurements. Three samples with composition Bi 1.6 Pb 0.4 Sr 2 Ca 2 Ni x Cu 3-x O y with x=0, x=0.05 and x=0.1 were prepared using sol-gel method and the measurements of χ'(T) and χ''(T) were carried out on these samples in zero and in applied d.c magnetic fields. The χ'(T) data for the samples in zero d.c field show single drops indicating that the samples had one superconducting phases and the superconducting transition temperatures of the samples were determined to be 108.7 K, 98.9 K and 56.7 K respectively. Obviously superconducting transition temperatures of the samples decrease with increasing Ni concentration. The χ' (T) data for the samples in d.c magnetic fields show broad superconducting transitions indicating that the magnetic fields quenched superconductivity of the samples. The χ''(T) data in d.c magnetic fields show broad intergrain peaks associated with energy dissipation inside the samples. In low d.c magnetic fields χ' (T) data for the x=0 and x=0.05 samples show two drops associated with inter and intragrain regions of the samples. In high magnetic fields χ' (T) data show single transitions indicating that the magnetic fields simultaneously penetrated into the superconducting grains and the weak links. The χ' (T) data for the x=0.1 sample shows single drops in low and in high d.c. magnetic fields. The high d.c magnetic fields pushed the superconducting transition temperatures of the samples to lower temperatures and the intergrain peaks in χ''(T) shifted to lower temperatures with increasing applied d.c magnetic fields. doi:10.4038/sljp.v3i0.185 Sri Lankan Journal of Physics, Vol.3 (2002) 53-61","PeriodicalId":21880,"journal":{"name":"Sri Lankan Journal of Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2002-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Investigation of Ni Substitution for Cu in Bi(Pb)-Sr-Ca-Cu-O Superconductor by AC Magnetic Susceptibility Measurements\",\"authors\":\"N. Pathmanathan, A. Thomson\",\"doi\":\"10.4038/SLJP.V3I0.185\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"st1\\\\:*{behavior:url(#ieooui) } \\n /* Style Definitions */ \\n table.MsoNormalTable \\n {mso-style-name:\\\"Table Normal\\\"; \\n mso-tstyle-rowband-size:0; \\n mso-tstyle-colband-size:0; \\n mso-style-noshow:yes; \\n mso-style-parent:\\\"\\\"; \\n mso-padding-alt:0cm 5.4pt 0cm 5.4pt; \\n mso-para-margin:0cm; \\n mso-para-margin-bottom:.0001pt; \\n mso-pagination:widow-orphan; \\n font-size:10.0pt; \\n font-family:\\\"Times New Roman\\\"; \\n mso-ansi-language:#0400; \\n mso-fareast-language:#0400; \\n mso-bidi-language:#0400;} \\n In this work we have investigated the effect of doping of magnetic element Ni for copper into the copper site of Bi(Pb)-Sr-Ca-Cu-O superconductor by means of AC magnetic susceptibility measurements. Three samples with composition Bi 1.6 Pb 0.4 Sr 2 Ca 2 Ni x Cu 3-x O y with x=0, x=0.05 and x=0.1 were prepared using sol-gel method and the measurements of χ'(T) and χ''(T) were carried out on these samples in zero and in applied d.c magnetic fields. The χ'(T) data for the samples in zero d.c field show single drops indicating that the samples had one superconducting phases and the superconducting transition temperatures of the samples were determined to be 108.7 K, 98.9 K and 56.7 K respectively. Obviously superconducting transition temperatures of the samples decrease with increasing Ni concentration. The χ' (T) data for the samples in d.c magnetic fields show broad superconducting transitions indicating that the magnetic fields quenched superconductivity of the samples. The χ''(T) data in d.c magnetic fields show broad intergrain peaks associated with energy dissipation inside the samples. In low d.c magnetic fields χ' (T) data for the x=0 and x=0.05 samples show two drops associated with inter and intragrain regions of the samples. In high magnetic fields χ' (T) data show single transitions indicating that the magnetic fields simultaneously penetrated into the superconducting grains and the weak links. The χ' (T) data for the x=0.1 sample shows single drops in low and in high d.c. magnetic fields. The high d.c magnetic fields pushed the superconducting transition temperatures of the samples to lower temperatures and the intergrain peaks in χ''(T) shifted to lower temperatures with increasing applied d.c magnetic fields. doi:10.4038/sljp.v3i0.185 Sri Lankan Journal of Physics, Vol.3 (2002) 53-61\",\"PeriodicalId\":21880,\"journal\":{\"name\":\"Sri Lankan Journal of Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2002-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Sri Lankan Journal of Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.4038/SLJP.V3I0.185\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Sri Lankan Journal of Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.4038/SLJP.V3I0.185","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
摘要
st1\:*{behavior:url(# ieoui)} /*样式定义*/表。mso-style-name:"Table Normal";mso-tstyle-rowband-size: 0;mso-tstyle-colband-size: 0;mso-style-noshow:是的;mso-style-parent:“”;Mso-padding-alt:0cm 5.4pt;mso-para-margin: 0厘米;mso-para-margin-bottom: .0001pt;mso-pagination: widow-orphan;字体大小:10.0分;font-family:宋体;mso-ansi-language: # 0400;mso-fareast-language: # 0400;本文采用交流磁化率测量的方法,研究了在Bi(Pb)-Sr-Ca-Cu-O超导体的铜位中掺杂磁性元素Ni对铜的影响。采用溶胶-凝胶法制备了3种成分为Bi 1.6 Pb 0.4 Sr 2 Ca 2 Ni x Cu 3-x oy、x=0、x=0.05和x=0.1的样品,分别在零磁场和外加直流磁场下对样品进行了χ’(T)和χ’(T)测量。在零直流场中,样品的χ’(T)数据显示为单滴,表明样品具有一个超导相,样品的超导转变温度分别为108.7 K、98.9 K和56.7 K。随着Ni浓度的增加,样品的超导转变温度明显降低。直流磁场下样品的χ′(T)数据显示出广泛的超导跃迁,表明磁场淬灭了样品的超导性。直流磁场下的χ”(T)数据显示出与样品内部能量耗散有关的宽晶粒间峰。在低直流磁场下,x=0和x=0.05样品的χ' (T)数据显示样品的内部和内部区域有两个下降。在强磁场下,χ’(T)数据显示单跃迁,表明磁场同时穿透超导晶粒和薄弱环节。x=0.1样品的χ’(T)数据显示在低直流磁场和高直流磁场中都有单次下降。高直流磁场使样品的超导转变温度降低,且随着外加直流磁场的增大,晶间峰χ”(T)向低温方向移动。doi:10.4038/sljp.v3i0.185斯里兰卡物理学报Vol.3 (2002) 53-61
Investigation of Ni Substitution for Cu in Bi(Pb)-Sr-Ca-Cu-O Superconductor by AC Magnetic Susceptibility Measurements
st1\:*{behavior:url(#ieooui) }
/* Style Definitions */
table.MsoNormalTable
{mso-style-name:"Table Normal";
mso-tstyle-rowband-size:0;
mso-tstyle-colband-size:0;
mso-style-noshow:yes;
mso-style-parent:"";
mso-padding-alt:0cm 5.4pt 0cm 5.4pt;
mso-para-margin:0cm;
mso-para-margin-bottom:.0001pt;
mso-pagination:widow-orphan;
font-size:10.0pt;
font-family:"Times New Roman";
mso-ansi-language:#0400;
mso-fareast-language:#0400;
mso-bidi-language:#0400;}
In this work we have investigated the effect of doping of magnetic element Ni for copper into the copper site of Bi(Pb)-Sr-Ca-Cu-O superconductor by means of AC magnetic susceptibility measurements. Three samples with composition Bi 1.6 Pb 0.4 Sr 2 Ca 2 Ni x Cu 3-x O y with x=0, x=0.05 and x=0.1 were prepared using sol-gel method and the measurements of χ'(T) and χ''(T) were carried out on these samples in zero and in applied d.c magnetic fields. The χ'(T) data for the samples in zero d.c field show single drops indicating that the samples had one superconducting phases and the superconducting transition temperatures of the samples were determined to be 108.7 K, 98.9 K and 56.7 K respectively. Obviously superconducting transition temperatures of the samples decrease with increasing Ni concentration. The χ' (T) data for the samples in d.c magnetic fields show broad superconducting transitions indicating that the magnetic fields quenched superconductivity of the samples. The χ''(T) data in d.c magnetic fields show broad intergrain peaks associated with energy dissipation inside the samples. In low d.c magnetic fields χ' (T) data for the x=0 and x=0.05 samples show two drops associated with inter and intragrain regions of the samples. In high magnetic fields χ' (T) data show single transitions indicating that the magnetic fields simultaneously penetrated into the superconducting grains and the weak links. The χ' (T) data for the x=0.1 sample shows single drops in low and in high d.c. magnetic fields. The high d.c magnetic fields pushed the superconducting transition temperatures of the samples to lower temperatures and the intergrain peaks in χ''(T) shifted to lower temperatures with increasing applied d.c magnetic fields. doi:10.4038/sljp.v3i0.185 Sri Lankan Journal of Physics, Vol.3 (2002) 53-61