591 research outputs found
Percolation transition in quantum Ising and rotor models with sub-Ohmic dissipation
We investigate the influence of sub-Ohmic dissipation on randomly diluted
quantum Ising and rotor models. The dissipation causes the quantum dynamics of
sufficiently large percolation clusters to freeze completely. As a result, the
zero-temperature quantum phase transition across the lattice percolation
threshold separates an unusual super-paramagnetic cluster phase from an
inhomogeneous ferromagnetic phase. We determine the low-temperature
thermodynamic behavior in both phases which is dominated by large frozen and
slowly fluctuating percolation clusters. We relate our results to the smeared
transition scenario for disordered quantum phase transitions, and we compare
the cases of sub-Ohmic, Ohmic, and super-Ohmic dissipation.Comment: 9 pages, 2 figure
Transport properties in antiferromagnetic quantum Griffiths phases
We study the electrical resistivity in the quantum Griffiths phase associated
with the antiferromagnetic quantum phase transition in a metal. The resistivity
is calculated by means of the semi-classical Boltzmann equation. We show that
the scattering of electrons by locally ordered rare regions leads to a singular
temperature dependence. The rare-region contribution to the resistivity varies
as with temperature where the is the usual Griffiths
exponent which takes the value zero at the critical point and increases with
distance from criticality. We find similar singular contributions to other
transport properties such as thermal resistivity, thermopower and the Peltier
coefficient. We also compare our results with existing experimental data and
suggest new experiments.Comment: 4 pages, 1 figur
Influence of Generic Scale Invariance on Classical and Quantum Phase Transitions
This review discusses a paradigm that has become of increasing importance in
the theory of quantum phase transitions; namely, the coupling of the
order-parameter fluctuations to other soft modes, and the resulting
impossibility of constructing a simple Landau-Ginzburg-Wilson theory in terms
of the order parameter only. The soft modes in question are manifestations of
generic scale invariance, i.e., the appearance of long-range order in whole
regions in the phase diagram. The concept of generic scale invariance, and its
influence on critical behavior, is explained using various examples, both
classical and quantum mechanical. The peculiarities of quantum phase
transitions are discussed, with emphasis on the fact that they are more
susceptible to the effects of generic scale invariance than their classical
counterparts. Explicit examples include: the quantum ferromagnetic transition
in metals, with or without quenched disorder; the metal-superconductor
transition at zero temperature; and the quantum antiferromagnetic transition.
Analogies with classical phase transitions in liquid crystals and classical
fluids are pointed out, and a unifying conceptual framework is developed for
all transitions that are influenced by generic scale invariance.Comment: 55pp, 25 eps figs; final version, to appear in Rev Mod Phy
Breakdown of Landau-Ginzburg-Wilson theory for certain quantum phase transitions
The quantum ferromagnetic transition of itinerant electrons is considered. It
is shown that the Landau-Ginzburg-Wilson theory described by Hertz and others
breaks down due to a singular coupling between fluctuations of the conserved
order parameter. This coupling induces an effective long-range interaction
between the spins of the form 1/r^{2d-1}. It leads to unusual scaling behavior
at the quantum critical point in dimensions, which is determined
exactly.Comment: 4 pp., REVTeX, no figs, final version as publishe
Superconductivity and Quantum Phase Transitions in Weak Itinerant Ferromagnets
It is argued that the phase transition in low-T_c clean itinerant
ferromagnets is generically of first order, due to correlation effects that
lead to a nonanalytic term in the free energy. A tricritical point separates
the line of first order transitions from Heisenberg critical behavior at higher
temperatures. Sufficiently strong quenched disorder suppresses the first order
transition via the appearance of a critical endpoint. A semi-quantitative
discussion is given in terms of recent experiments on MnSi and UGe_2. It is
then shown that the critical temperature for spin-triplet, p-wave
superconductivity mediated by spin fluctuations is generically much higher in a
Heisenberg ferromagnetic phase than in a paramagnetic one, due to the coupling
of magnons to the longitudinal magnetic susceptibility. This qualitatively
explains the phase diagram recently observed in UGe_2 and ZrZn_2.Comment: 10 pp., LaTeX, 5 ps figs., requires World Scientific style files
(included), Invited contribution to MB1
Quantum critical behavior of clean itinerant ferromagnets
We consider the quantum ferromagnetic transition at zero temperature in clean
itinerant electron systems. We find that the Landau-Ginzburg-Wilson order
parameter field theory breaks down since the electron-electron interaction
leads to singular coupling constants in the Landau-Ginzburg-Wilson functional.
These couplings generate an effective long-range interaction between the spin
or order parameter fluctuations of the form 1/r^{2d-1}, with d the spatial
dimension. This leads to unusual scaling behavior at the quantum critical point
in 1 < d\leq 3, which we determine exactly. We also discuss the
quantum-to-classical crossover at small but finite temperatures, which is
characterized by the appearance of multiple temperature scales. A comparison
with recent results on disordered itinerant ferromagnets is given.Comment: 13 pp., REVTeX, psfig, 3 eps figs, final version as publishe
The quantum phase transition of itinerant helimagnets
We investigate the quantum phase transition of itinerant electrons from a
paramagnet to a state which displays long-period helical structures due to a
Dzyaloshinskii instability of the ferromagnetic state. In particular, we study
how the self-generated effective long-range interaction recently identified in
itinerant quantum ferromagnets is cut-off by the helical ordering. We find that
for a sufficiently strong Dzyaloshinskii instability the helimagnetic quantum
phase transition is of second order with mean-field exponents. In contrast, for
a weak Dzyaloshinskii instability the transition is analogous to that in
itinerant quantum ferromagnets, i.e. it is of first order, as has been observed
in MnSi.Comment: 5 pages RevTe
Percolation quantum phase transitions in diluted magnets
We show that the interplay of geometric criticality and quantum fluctuations
leads to a novel universality class for the percolation quantum phase
transition in diluted magnets. All critical exponents involving dynamical
correlations are different from the classical percolation values, but in two
dimensions they can nonetheless be determined exactly. We develop a complete
scaling theory of this transition, and we relate it to recent experiments in
LaCu(Zn,Mg)O. Our results are also relevant for
disordered interacting boson systems.Comment: 4 pages, 3 eps figures, final version, as publishe
Infinite randomness and quantum Griffiths effects in a classical system: the randomly layered Heisenberg magnet
We investigate the phase transition in a three-dimensional classical
Heisenberg magnet with planar defects, i.e., disorder perfectly correlated in
two dimensions. By applying a strong-disorder renormalization group, we show
that the critical point has exotic infinite-randomness character. It is
accompanied by strong power-law Griffiths singularities. We compute various
thermodynamic observables paying particular attention to finite-size effects
relevant for an experimental verification of our theory. We also study the
critical dynamics within a Langevin equation approach and find it extremely
slow. At the critical point, the autocorrelation function decays only
logarithmically with time while it follows a nonuniversal power-law in the
Griffiths phase.Comment: 10 pages, 2 eps figures included, final version as published
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