Tomonaga-Luttinger liquid in a quasi-one-dimensional
= 1 antiferromagnet observed by specific heat measurements
比熱測定による
=1の準一次元反強磁性鎖における朝永・ラッティンジャー流体的振る舞い
萩原 政幸*; 辻井 宏之*; Rotundu, C. R.*; Andraka, B.*; 高野 安正*; 立岩 尚之
; 小林 達生*; 鈴木 隆史*; 菅 誠一郎*
Hagiwara, Masayuki*; Tsujii, Hiroyuki*; Rotundu, C. R.*; Andraka, B.*; Takano, Yasumasa*; Tateiwa, Naoyuki; Kobayashi, Tatsuo*; Suzuki, Takafumi*; Suga, Seiichiro*
準一次元系磁性物質Ni(C
H
N
)(NO
)(ClO
)(NTENP)の磁場中比熱測定を行った。スピン鎖に並行に磁場を加えると、臨界磁場
以上でスピンギャップが消滅し、磁気秩序転移温度より高温では比熱
が温度
に依存する振る舞いを示すことが明らかとなった。本研究から明らかとなった、朝永-ラッティンジャー流体的振る舞いについて理論モデルを用いて解析する。
Specific-heat experiments on single crystals of the
= 1 quasi-one-dimensional bond-alternating antiferromagnet Ni(C
H
N
)(NO
)(ClO
) (NTENP) have been performed in magnetic fields applied both parallel and perpendicular to the spin chains. We have found for the parallel field configuration that the magnetic specific heat (
) is proportional to temperature (
) above a critical field
, at which the energy gap vanishes, in a temperature region above that of the long-range ordered state. The ratio
=
increases as the magnetic field approaches
from above. The data are in good quantitative agreement with the prediction of the
=1 conformal field theory in conjunction with the velocity of the excitations calculated by a numerical diagonalization, providing conclusive evidence for a Tomonaga-Luttinger liquid.