TY - JOUR
T1 - Superconducting state of the binary boride Ru 7B 3 with the noncentrosymmetric crystal structure
AU - Kase, Naoki
AU - Akimitsu, Jim
PY - 2009/4
Y1 - 2009/4
N2 - Single crystals of Ru 7B 3 were grown by the Czochralski puling method in a tetra-arc furnace. The compound crystallizes in a Th 7Fe 3-type structure (hexagonal, space group: P6 3, mc), which has no inversion symmetry along the oaxis. Measurements in magnetic fields indicate type-II superconductivity with upper critical fields of H c2(0) ≃ 17.2kOe for H &par [001] and 15.8kOe for H &par [100], respectively. The coherence length ξ(0) GL, penetration depth λ(0)GL, and Ginzburg-Landau (GL) parameter κ(0) obtained from these values are 144Å, 3U0Å, and 21.6 for H ∥ [100], and 138 Å, 3520Å, and 25.5 for H &par [001], respectively. Specific heat measurements reveal that Ru 7B 3 is a weak-coupling superconductor with an isotropic superconducting gap.
AB - Single crystals of Ru 7B 3 were grown by the Czochralski puling method in a tetra-arc furnace. The compound crystallizes in a Th 7Fe 3-type structure (hexagonal, space group: P6 3, mc), which has no inversion symmetry along the oaxis. Measurements in magnetic fields indicate type-II superconductivity with upper critical fields of H c2(0) ≃ 17.2kOe for H &par [001] and 15.8kOe for H &par [100], respectively. The coherence length ξ(0) GL, penetration depth λ(0)GL, and Ginzburg-Landau (GL) parameter κ(0) obtained from these values are 144Å, 3U0Å, and 21.6 for H ∥ [100], and 138 Å, 3520Å, and 25.5 for H &par [001], respectively. Specific heat measurements reveal that Ru 7B 3 is a weak-coupling superconductor with an isotropic superconducting gap.
KW - No inversion symmetry
KW - Ru B
KW - Specific heat
KW - Superconductivity
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U2 - 10.1143/JPSJ.78.044710
DO - 10.1143/JPSJ.78.044710
M3 - Article
AN - SCOPUS:67649204244
SN - 0031-9015
VL - 78
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 4
M1 - 044710
ER -