DISTRIBUTION OF K IONS IN INTERMEDIATE KC60

被引:23
作者
FAIGEL, G
BORTEL, G
TEGZE, M
GRANASY, L
PEKKER, S
OSZLANYI, G
CHAUVET, O
BAUMGARTNER, G
FORRO, L
STEPHENS, PW
MIHALY, G
JANOSSY, A
机构
[1] ECOLE POLYTECH FED LAUSANNE, INST GENIE ATOM, DEPT PHYS, PHYS SOLIDES SEMICRISTALLINES LAB, CH-1015 LAUSANNE, SWITZERLAND
[2] SUNY STONY BROOK, DEPT PHYS, STONY BROOK, NY 11794 USA
[3] TECH UNIV BUDAPEST, INST PHYS, H-1521 BUDAPEST, HUNGARY
来源
PHYSICAL REVIEW B | 1995年 / 52卷 / 05期
关键词
D O I
10.1103/PhysRevB.52.3199
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Intermediate KC60 formed from the homogeneous KC60 phase at 400 K is investigated by differential scanning calorimetry, x-ray diffraction, de resistivity, electron-spin resonance (ESR), and magnetic ac susceptibility. We show that in intermediate KC60 the C-60 sublattice is continuous over large distances but the K ions separate into small K3C60 and K-free C-60 regions. ESR shows a large volume fraction of superconducting K3C60 The K3C60 phase is finely distributed and the magnetic-field exclusion is small. K3C60 regions are compressed and K-free regions are expanded with-respect to the corresponding bulk phases. The compression decreases the superconducting critical temperature (T-c) from 19 to 16 K. The expansion of the K-free C-60 regions decreases the orientational ordering transition temperature (at 260 K) by 10 K.
引用
收藏
页码:3199 / 3205
页数:7
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