TY - JOUR
T1 - Coexistence of S = 1/2 antiferromagnetic chains and dimers on hole-doped CuO2 chains in Ca1-xCuO2
AU - Hiroi, Zenji
AU - Okumura, Makoto
AU - Yamada, Takahiro
AU - Takano, Mikio
PY - 2000/6
Y1 - 2000/6
N2 - Quasi-one-dimensional cupric oxide Ca1-xCuO2+δ, comprising 25-50% hole-doped edge-sharing CuO2 chains, is studied by uniform magnetic susceptibility and specific heat measurements on a series of polycrystalline samples with controlled metal and oxygen contents. Because the Cu-O-Cu bonds are nearly orthogonal, holes are almost localized, and only spin degrees of freedom survive at low temperature. The results reveal that antiferromagnetic chains made of 50% spins per formula unit always exist, independent of spin density, and the remainder of spins mostly form dimers of variable density. A two-sublattice model is proposed by considering that the nearest-neighbor couplings are negligibly small, due to both geometrical frustration and the special Cu-O-Cu bond angle of ~95°. Thus next-nearest-neighbor interactions dominate, and give rise to a charge-ordered state on one sublattice, which behaves as a Heisenberg antiferromagnetic chain. The rest of the spins tend to form dimers on the other sublattice with low spin density. Long-range antiferromagnetic ordering appears to occur at 12 K.
AB - Quasi-one-dimensional cupric oxide Ca1-xCuO2+δ, comprising 25-50% hole-doped edge-sharing CuO2 chains, is studied by uniform magnetic susceptibility and specific heat measurements on a series of polycrystalline samples with controlled metal and oxygen contents. Because the Cu-O-Cu bonds are nearly orthogonal, holes are almost localized, and only spin degrees of freedom survive at low temperature. The results reveal that antiferromagnetic chains made of 50% spins per formula unit always exist, independent of spin density, and the remainder of spins mostly form dimers of variable density. A two-sublattice model is proposed by considering that the nearest-neighbor couplings are negligibly small, due to both geometrical frustration and the special Cu-O-Cu bond angle of ~95°. Thus next-nearest-neighbor interactions dominate, and give rise to a charge-ordered state on one sublattice, which behaves as a Heisenberg antiferromagnetic chain. The rest of the spins tend to form dimers on the other sublattice with low spin density. Long-range antiferromagnetic ordering appears to occur at 12 K.
KW - CuO chain
KW - Hole-doping
KW - Magnetic susceptibility
KW - Quantum spin system
KW - Specific heat
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U2 - 10.1143/JPSJ.69.1824
DO - 10.1143/JPSJ.69.1824
M3 - Article
AN - SCOPUS:0034397644
VL - 69
SP - 1824
EP - 1833
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
SN - 0031-9015
IS - 6
ER -