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arxiv: 1905.02117 · v2 · pith:JMY3AN25new · submitted 2019-05-06 · ❄️ cond-mat.str-el · cond-mat.stat-mech

Ground State Phases of Distorted S=1 Diamond Chains

classification ❄️ cond-mat.str-el cond-mat.stat-mech
keywords phasesferrimagneticdistortionhaldanelambdaphasequantizedtype
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The ground states of distorted $S=1$ diamond chains are investigated for two types of distortion called type A and B [J. Phys. Soc. Jpn. 79 (2010) 114703]. For the type A distortion, Haldane phases with and without spontaneous translational symmetry breakdown are present for large values of parameter $\lambda$ that parametrize the strength of frustration. For small $\lambda$, the Haldane phase and two quantized ferrimagnetic phases in the undistorted chain remain stable even for strong distortion. In contrast, for the type B distortion, the quantized ferrimagnetic phases with and without spontaneous translational symmetry breakdown are present for large $\lambda$. The partial ferrimagnetic phases emerge between them. For small $\lambda$, two quantized ferrimagnetic phases remain and the partial ferrimagnetic phases also emerge between them. The Haldane phase between the two kinds of ferrimagnetic phases turns into a topologically trivial double Haldane phase for strong distortion.

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