Charge-density-wave order with momentum (2Q,0)(2Q, 0) and (0,2Q)(0, 2Q) within the spin-fermion model: continuous and discrete symmetry breaking, preemptive composite order, and relation to pseudogap in hole-doped cuprates

preprint2014arXivOpen access

Abstract

We analyze charge order within the the spin-fermion model. We show that magnetically-mediated interaction gives rise to charge order ΔkQ=⟨ck+Q†ck−Q⟩Δ_k^Q = \langle c^\dagger_{{\bf k}+{\bf Q}} c_{{\bf k}-{\bf Q}}\rangle with momenta Q=Qx=(2Q,0){\bf Q}=Q_x =(2Q,0) and Q=Qy=(0,2Q){\bf Q}=Q_y =(0,2Q), if the magnetic correlation length ξξ exceeds some critical value. We argue that ΔkQΔ_k^Q and Δ−kQΔ_{-k}^Q are not equivalent, and their symmetric and antisymmetric combinations describe density modulations and bond current. We derive GL functional for four-component U(1)U(1) order parameters Δ±kQΔ^Q_{\pm k} with Q=Qx{\bf Q} = Q_x or QyQ_y. Within mean-field we find two types of CDW states, I and II, depending on system parameters. In state I density and current modulations emerge with the same Q=Qx{\bf Q} = Q_x or QyQ_y, breaking Z2Z_2 lattice rotational symmetry, and differ in phase by ±π/2\pmπ/2. The selection of π/2π/2 or −π/2-π/2 additionally breaks Z2Z_2 time-reversal symmetry, such that the total order parameter manifold is U(1)×Z2×Z2U(1) \times Z_2 \times Z_2. In state II density and current modulations emerge with different Q\bf Q and the order parameter manifold is U(1)×U(1)×Z2U(1) \times U (1) \times Z_2. We go beyond mean-field and show that discrete symmetries get broken before long-range charge order sets in. For state I, the system first breaks Z2Z_2 lattice rotational symmetry (C4→C2C_4 \to C_2) at T=TnT= T_n and develops a nematic order, then breaks Z2Z_2 time-reversal symmetry at Tt<TnT_t < T_n, and finally breaks U(1)U(1) symmetry of a common phase of even and odd components of ΔkQΔ^Q_{k} at T=Tcdw<Tt<TnT= T_{\rm cdw} < T_t < T_n and develops a true charge order. We argue that the preemptive orders lift TcdwT_{\rm cdw} and reduces TscT_{\rm sc} such that at large ξξ charge order may develop prior to superconductivity. We obtain the phase diagram and present quantitative comparison with ARPES data for hole-doped cuprates.

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