The $\bf T=0$ $\bf 2k_F$ density wave phase transition in a two dimensional Fermi liquid is first order

dc.creatorAltshuler, B. L.
dc.creatorIoffe, L. B.
dc.creatorMillis, A. J.
dc.date1995-04-06
dc.date.accessioned2026-07-07T03:07:40Z
dc.date.available2026-07-07T03:07:40Z
dc.descriptionWe study $T=0$ spin density wave transitions in two dimensional Fermi liquids in which the ordering wavevector $\bf Q$ is such that the tangents to the Fermi line at the points connected by $\bf Q$ are parallel (e.g. $Q=2p_F$ in a system with a circular Fermi line) and the Fermi line is not flat. We show that the transition is first order if the ordering wave vector $\bf Q$ is not commensurate with a reciprocal lattice vector, $\bf G$, i.e. ${\bf Q} \neq {\bf G}/2$. If $\bf Q$ is close to ${\bf G}/2$ the transition is weakly first order and an intermediate scaling regime exists; in this regime the $2p_F$ susceptibility and observables such as the NMR rates $T_1$ and $T_2$ have scaling forms which we determine.
dc.description11 pages, 8 Postscript figures in a separate file
dc.identifierhttps://arxiv.org/abs/cond-mat/9504024
dc.identifierhttp://arxiv.org/abs/cond-mat/9504024
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/27251
dc.subjectCondensed Matter
dc.titleThe $\bf T=0$ $\bf 2k_F$ density wave phase transition in a two dimensional Fermi liquid is first order
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