Evidence that all high-temperature superconductors are p-type

被引:30
作者
Blackstead, HA [1 ]
Dow, JD [1 ]
机构
[1] ARIZONA STATE UNIV,DEPT PHYS,TEMPE,AZ 85287
来源
PHYSICAL REVIEW B | 1997年 / 55卷 / 10期
关键词
D O I
10.1103/PhysRevB.55.6605
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The ground charge state of Ce substituting for Nd+3 in Nd2CuO4 is usually assumed to be Ce+4, indicating that Ce is a donor which causes Nd2-zCezCuO4 to be an n-type superconductor. Using the self-consistent bond/charge method, we show that the Ce ground state is Ce+3, not Ce+4, in ideal Nd2CuO4, implying that monatomic Ce dopants are isoelectronic centers, not n-type donors. The observed Ce doping of Nd2-zCezCuO4 can be understood if an interstitial oxygen binds to the Ce, elevating its charge state to Ce+4. This is a paired defect of Ce and oxygen, which dopes the host p-type, not n-type, because of oxygen's 2p holes. The condition that the interstitial oxygen does dope the hostp-type translates into an approximate steric constraint that the ionic radius of the rare-earth ion R(+3) must exceed that of Tb+3 for Ra2-zCezCuO4 to superconduct. A similar situation occurs for the infinite-layer material Sr1-vNdvCuO2, where the Nd dopant is isoelectronic Nd+2, not donor Nd+3 as assumed, unless an extra oxygen is adjacent to the Nd. The data are reviewed in light of these results, and show no convincing evidence either of particle-hole symmetry in doping, or of n-type doping of any high-temperature superconductor. Instead they hint that the superconductivity is associated with oxygen, rather than with any particle-hole-symmetric cuprate-plane phenomenon.
引用
收藏
页码:6605 / 6611
页数:7
相关论文
共 58 条
[1]   EFFECT OF CE DOPING ON THE CU CHARGE IN THE ELECTRON SUPERCONDUCTOR ND2-XCEXCUO4 [J].
ALP, EE ;
MINI, SM ;
RAMANATHAN, M ;
DABROWSKI, B ;
RICHARDS, DR ;
HINKS, DG .
PHYSICAL REVIEW B, 1989, 40 (04) :2617-2619
[2]   POSSIBLE HIGH-TC SUPERCONDUCTIVITY IN THE BA-LA-CU-O SYSTEM [J].
BEDNORZ, JG ;
MULLER, KA .
ZEITSCHRIFT FUR PHYSIK B-CONDENSED MATTER, 1986, 64 (02) :189-193
[3]   CHARGE-DISTRIBUTION IN YUPR1-UBA2CU3OX [J].
BLACKSTEAD, HA ;
DOW, JD ;
FEDERICI, JF ;
PACKARD, WE ;
PULLING, DB .
PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 1994, 235 :2161-2162
[4]   Charge-transfer and the location of superconducting holes in La2-beta Sr beta CuO4 [J].
Blackstead, HA ;
Dow, JD .
JOURNAL OF PHYSICS AND CHEMISTRY OF SOLIDS, 1995, 56 (12) :1697-1698
[5]  
BLACKSTEAD HA, 1994, JETP LETT+, V59, P283
[6]   LOCATION OF THE ROOT OF SUPERCONDUCTIVITY IN LA2-BETA-SR-BETA-CUOX AND ND2-ZCEZCUOX [J].
BLACKSTEAD, HA ;
DOW, JD .
PHILOSOPHICAL MAGAZINE B-PHYSICS OF CONDENSED MATTER STATISTICAL MECHANICS ELECTRONIC OPTICAL AND MAGNETIC PROPERTIES, 1995, 72 (05) :529-534
[7]   Anomalous charge-transfer in La2-beta Sr beta CuO4 and in Nd2-zCezCuO4 [J].
Blackstead, HA ;
Dow, JD .
JOURNAL OF APPLIED PHYSICS, 1995, 78 (12) :7175-7180
[8]  
BLACKSTEAD HA, 1995, P SOC PHOTO-OPT INS, V2397, P617, DOI 10.1117/12.206908
[9]  
Brown I. D., 1980, STRUCTURE BONDING CR, VII, P1
[10]   EMPIRICAL PARAMETERS FOR CALCULATING CATION-OXYGEN BOND VALENCES [J].
BROWN, ID ;
WU, KK .
ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL SCIENCE, 1976, 32 (JUL15) :1957-1959