1,122 research outputs found
Modelling the gluon propagator
Scaling of the Landau gauge gluon propagator calculated at beta=6.0 and at
beta=6.2 is demonstrated. A variety of functional forms for the gluon
propagator calculated on a large (32^3x64) lattice at beta=6.0 are
investigated.Comment: LATTICE98(confine), 3 pages, 2 figure
Electronic nematicity and its relation to quantum criticality in Sr_3Ru_2O_7 studied by thermal expansion
We report high-resolution measurements of the in-plane thermal expansion
anisotropy in the vicinity of the electronic nematic phase in SrRuO
down to very low temperatures and in varying magnetic field orientation. For
fields applied along the c-direction, a clear second-order phase transition is
found at the nematic phase, with critical behavior compatible with the
two-dimensional Ising universality class (although this is not fully
conclusive). Measurements in a slightly tilted magnetic field reveal a broken
four-fold in-plane rotational symmetry, not only within the nematic phase, but
extending towards slightly larger fields. We also analyze the universal scaling
behavior expected for a metamagnetic quantum critical point, which is realized
outside the nematic region. The contours of the magnetostriction suggest a
relation between quantum criticality and the nematic phase.Comment: 8 pages, 12 Figures, invited paper at QCNP 2012 conferenc
Symmetry-breaking lattice distortion in Sr_3Ru_2O_7
The electronic nematic phase of SrRuO is investigated by
high-resolution in-plane thermal expansion measurements in magnetic fields
close to 8 T applied at various angles off the c-axis. At
we observe a very small () lattice distortion which
breaks the four-fold in-plane symmetry, resulting in nematic domains with
interchanged - and b-axis. At the domains are
almost fully aligned and thermal expansion indicates an area-preserving lattice
distortion of order which is likely related to orbital
ordering. Since the system is located in the immediate vicinity to a
metamagnetic quantum critical end point, the results represent the first
observation of a structural relaxation driven by quantum criticality.Comment: 4 pages, 5 figures, PRL accepte
Anisotropy of the low-temperature magnetostriction of Sr3Ru2O7
We use high-resolution capacitive dilatometry to study the low-temperature
linear magnetostriction of the bilayer ruthenate SrRuO as a
function of magnetic field applied perpendicular to the ruthenium-oxide planes
(). The relative length change is detected either
parallel or perpendicular to the c-axis close to the metamagnetic region near
B=8 T. In both cases, clear peaks in the coefficient at three subsequent metamagnetic transitions are observed. For , the third transition at 8.1 T bifurcates at temperatures below 0.5
K. This is ascribed to the effect of an in-plane uniaxial pressure of about 15
bar, unavoidable in the dilatometer, which breaks the original fourfold
in-plane symmetry.Comment: 3 pages, 3 Figures, Manuscript for Proceedings of the International
Conference on Quantum Criticality and Novel Phases (QCNP09, Dresden
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The Gluon Propagator in Momentum Space
We give preliminary numerical results for the gluon propagator evaluated both
in coordinate and momentum space on a 16^3X40 quenched lattice at beta=6.0. Our
findings are compared with earlier results in the literature at zero momentum.
In addition, by considering nonzero momenta we attempt to extract the form of
the propagator and compare it to continuum predictions formulated by Gribov and
others. latex, file espcrc2.sty needed (appended at the end: search for
espcrc2.sty).Comment: 4 page
Uniaxial stress tuning of geometrical frustration in a Kondo lattice
Hexagonal CeRhSn with paramagnetic moments on a distorted Kagome lattice
displays zero-field quantum critical behavior related to geometrical
frustration. We report high-resolution thermal expansion and magnetostriction
measurements under multiextreme conditions such as uniaxial stress up to 200
MPa, temperatures down to 0.1 K and magnetic fields up to 10 T. Under uniaxial
stress along the -direction, quantum criticality disappears and a complex
magnetic phase diagram arises with a sequence of phases below 1.2 K and fields
between 0 and 3 T (). Since the Kondo coupling increases with
stress, which alone would stabilize paramagnetic behavior in CeRhSn, the
observed order arises from the release of geometrical frustration by in-plane
stress.Comment: Accepted in PRB Rapid Com
Deciding Robust Feasibility and Infeasibility Using a Set Containment Approach: An Application to Stationary Passive Gas Network Operations
In this paper we study feasibility and infeasibility of nonlinear two-stage
fully adjustable robust feasibility problems with an empty first stage. This is
equivalent to deciding whether the uncertainty set is contained within the
projection of the feasible region onto the uncertainty-space. Moreover, the
considered sets are assumed to be described by polynomials. For answering this
question, two very general approaches using methods from polynomial
optimization are presented - one for showing feasibility and one for showing
infeasibility. The developed methods are approximated through sum of squares
polynomials and solved using semidefinite programs. Deciding robust feasibility
and infeasibility is important for gas network operations, which is a nonconvex
feasibility problem where the feasible set is described by a composition of
polynomials with the absolute value function. Concerning the gas network
problem, different topologies are considered. It is shown that a tree
structured network can be decided exactly using linear programming.
Furthermore, a method is presented to reduce a tree network with one additional
arc to a single cycle network. In this case, the problem can be decided by
eliminating the absolute value functions and solving the resulting linearly
many polynomial optimization problems. Lastly, the effectivity of the methods
is tested on a variety of small cyclic networks. It turns out that for
instances where robust feasibility or infeasibility can be decided
successfully, level 2 or level 3 of the Lasserre relaxation hierarchy typically
is sufficient
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