Search results for "Continuous symmetry"

showing 4 items of 4 documents

Reinforced cyclam derivatives functionalized on the bridging unit

2016

International audience; A new synthetic method has been developed for the preparation of reinforced cyclams (1,4,8,11-tetraazacyclotetradecane) C-functionalized on the bridging unit, by using a "one pot" reaction starting from the appropriate bis-aminal cyclam intermediate. The high reactivity of quaternized aminal moiety toward nucleophilic agent has been used to elaborate a new class of cross-bridged and side-bridged cyclam derivatives containing cyanide group on the ethylene bridge. Several chelators and corresponding copper(II) complexes have been prepared and characterized by X-ray diffraction. These new constrained polyazamacrocycles are valuable precursors of bifunctional chelating a…

CyanideRadiometals010402 general chemistry01 natural sciencesCatalysisCopper(ii) complexesCoordination complexContinuous symmetry measureschemistry.chemical_compoundNucleophileBifunctional chelator[SDV.IDA]Life Sciences [q-bio]/Food engineeringCyclamMaterials ChemistryOrganic chemistryMoietyChelationBifunctionalPolyhedrachemistry.chemical_classification010405 organic chemistry[ SDV.IDA ] Life Sciences [q-bio]/Food engineeringGeneral ChemistryCombinatorial chemistry0104 chemical sciencesCoordination chemistrychemistryAminalTherapyStability
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Asymptotic structure factor and power-law tails for phase ordering in systems with continuous symmetry.

1991

We compute the asymptotic structure factor ${\mathit{S}}_{\mathbf{k}}$(t) [=L(t${)}^{\mathit{d}}$g(kL(t)), where L(t) is a time-dependent characteristic length scale and d is the dimensionality] for a system with a nonconserved n-component vector order parameter quenched into the ordered phase. The well-known Ohta-Jasnow-Kawasaki-Yalabik-Gunton result is recovered for n=1. The scaling function g(x) has the large-x behavior g(x)\ensuremath{\sim}${\mathit{x}}^{\mathrm{\ensuremath{-}}(\mathit{d}+\mathit{n})}$, which includes Porod's law (for n=1) as a special case.

PhysicsContinuous symmetryPhase (matter)Phase orderingGeneral Physics and AstronomyOrder (ring theory)Function (mathematics)Structure factorPower lawScalingMathematical physicsPhysical review letters
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Finite-size scaling for a first-order transition where a continuous symmetry is broken: The spin-flop transition in the three-dimensional XXZ Heisenb…

2019

Finite-size scaling for a first-order phase transition where a continuous symmetry is broken is developed using an approximation of Gaussian probability distributions with a phenomenological ``degeneracy'' factor included. Predictions are compared with data from Monte Carlo simulations of the three-dimensional, $XXZ$ Heisenberg antiferromagnet in a field in order to study the finite-size behavior on a $L\ifmmode\times\else\texttimes\fi{}L\ifmmode\times\else\texttimes\fi{}L$ simple cubic lattice for the first-order ``spin-flop'' transition between the Ising-like antiferromagnetic state and the canted, $XY$-like state. Our theory predicts that for large linear dimension $L$ the field dependen…

PhysicsPhase transitionInverse01 natural sciences010305 fluids & plasmasUniversality (dynamical systems)Transition pointContinuous symmetry0103 physical sciencesFlop-transitionProbability distribution010306 general physicsScalingMathematical physicsPhysical Review E
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Asymptotic structure factor for the two-component Ginzburg-Landau equation

1992

We derive an analytic form for the asymptotic time-dependent structure factor for the two-component Ginzburg-Landau equation in arbitrary dimensions. This form is in reasonable agreement with results from numerical simulations in two dimensions. A striking feature of our analytic form is the absence of Porod's law in the tail. This is a consequence of the continuous symmetry of the Hamiltonian, which inhibits the formation of sharp domain walls.

Physicssymbols.namesakeContinuous symmetryDynamic structure factorsymbolsGinzburg landau equationGeneral Physics and AstronomyStructure factorHamiltonian (quantum mechanics)Mathematical physicsPhysics Letters A
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