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P. Mistark

Publications and source records attributed to P. Mistark.

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Entropic Origin of Pseudogap Physics and a Mott-Slater Transition in Cuprates

We propose a new approach to understand the origin of the pseudogap in the cuprates, in terms of bosonic entropy. The near-simultaneous softening of a large number of different $q$-bosons yields an extended range of short-range order, wherein the growth of magnetic correlations with decreasing temperature $T$ is anomalously slow. These entropic effects cause the spectral weight associated with the Van Hove singularity (VHS) to shift rapidly and nearly linearly toward half filling at higher $T$, consistent with a picture of the VHS driving the pseudogap transition at a temperature $\sim T^*$. As a byproduct, we develop an order-parameter classification scheme that predicts supertransitions between families of order parameters. As one example, we find that by tuning the hopping parameters, it is possible to drive the cuprates across a {\it transition between Mott and Slater physics}, where a spin-frustrated state emerges at the crossover.

cond-mat.str-el

Van Hove Singularity as the Driver of Pseudogap Physics in Cuprate High-$T$ Superconductors

We propose a new approach to the pseudogap problem in cuprates. Hole-doped cuprates display a broad plateau in the susceptibility centered near $(\pi,\pi)$. Competition between the softening of different $q$-modes on this plateau leads to anomalously slow growth of magnetic correlations with reducing temperature -- i.e., extended ranges of short-range correlations. The plateau arises from competition between Fermi- surface nesting and a `hidden' Van Hove singularity (VHS) nesting, associated with a bulk contribution to the susceptibility. As such, the VHS contribution is not tied to the Fermi level but rather turns on near $T_{VHS}=(E_F-E_{VHS})/k_B$ [where $E_F$ is the Fermi energy and $E_{VHS}$ the energy of the VHS peak]. Identifying $T^*\simeq T_{VHS}$ can explain many characteristic features of the pseudogap, including the transport anomalies and the termination of the pseudogap when $E_{VHS}$ crosses the Fermi level.

cond-mat.supr-con