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首页> 外文期刊>Physical Review, B. Condensed Matter >Scaling exponents in the incommensurate phase of the sine-Gordon and U(1) Thirring models - art. no. 085109
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Scaling exponents in the incommensurate phase of the sine-Gordon and U(1) Thirring models - art. no. 085109

机译:正弦Gordon模型和U(1)Thirring模型的不相称阶段的缩放指数-艺术。没有。 085109

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摘要

In this paper we study the critical exponents of the quantum sine-Gordon model and U(1) Thirring models in the incommensurate phase. This phase appears when the chemical potential h exceeds a critical value and is characterized by a finite density of solitons. The low-energy sector of this phase is critical and is described by the Gaussian model (Tomonaga-Luttinger liquid) with the compactification radius dependent on the soliton density and the sine-Gordon model coupling constant beta. For a fixed value of beta, we find that the Luttinger parameter K is equal to 1/2 at the commensurate-incommensurate transition point and approaches the asymptotic value beta (2)/8 pi away from it. We describe a possible phase diagram of the model consisting of an array of weakly coupled chains. The possible phases are Fermi liquid, spin density wave, spin-Peierls, and Wigner crystal. [References: 15]
机译:在本文中,我们研究了处于不相称阶段的量子正弦戈登模型和U(1)三次模型的临界指数。当化学势h超过临界值时出现此阶段,并以有限的孤子密度为特征。该阶段的低能级至关重要,由高斯模型(Tomonaga-Luttinger液体)描述,其压实半径取决于孤子密度和耦合常数β的正弦-戈登模型。对于固定的β值,我们发现Luttinger参数K在相称-不相称的过渡点等于1/2,并且渐近渐近值β(2)/ 8 pi。我们描述了模型的可能相图,该模型由一系列弱耦合链组成。可能的相为费米液体,自旋密度波,自旋Peierls和维格纳晶体。 [参考:15]

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