手征对称性动力学破缺和铜氧化物超导体相变的三维量子电动力学研究

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利用三维量子电动力学理论中的Dyson-Schwinger方程方法,研究了零温情况下平面铜氧化合物超导体的反铁磁相和d波超导相之间的相变.通过在朗道规范下近似解析求解和数值求解完全耦合的Dyson-Schwinger方程、并将所得结果与1/N展开方法的结果相比较,发现在半填充准费密子味道数约小于等于4的情况下,通过手征对称性自发破缺,d波超导相可以演化到反铁磁相,并且反铁磁相有可能与d波超导相共存.通过进一步比较不同相的压强,还说明反铁磁与d波超导共存相为稳定相,从而反铁磁相确实可以与d波超导相共存.
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