We show how decimated Gibbs measures which have an unbroken continuous symmetry due to the Mermin-Wagner theorem, although their discrete equivalents have a phase transition, still can become non-Gibbsian. The mechanism rests on the occurrence of a spin-flop transition with a broken discrete symmetry, once the model is constrained by the decimated spins in a suitably chosen "bad" configuration.Comment: 16 pages, 1 figure (updated
We reconsider the conceptual foundations of the renormalization-group (RG) formalism, and prove some...
We study the decimation to a sublattice of half the sites of the one-dimensional Dyson-Ising ferroma...
We consider disordered lattice spin models with finite volume Gibbs measures μ Λ[η](dσ). Here σ deno...
We show how decimated Gibbs measures having unbroken continuous symmetry due to the Mermin-Wagner th...
We extend proofs of non-Gibbsianness of decimated Gibbs measures at low temperatures to include long...
International audienceWe extend proofs of non-Gibbsianness of decimated Gibbs measures at low temper...
We generalize a result of Lebowitz and Maes, that projections of massless Gaussian measures onto Isi...
It is known that the joint measures on the product of spin-space and disorder space are very often n...
We consider Ising-spin systems starting from an initial Gibbs measure 1) and evolving under a spin-f...
The finite-volume microscopic behaviour of a system in equilibrium is de¬termined by the Boltzmann-G...
Abstract: We consider Ising-spin systems starting from an initial Gibbs measure ν and evolving under...
We generalize a result of Lebowitz and Maes, that projections of massless Gaussian measures onto Isi...
We consider Ising-spin systems starting from an initial Gibbs measure ν and evolving under a spin-fl...
We reconsider the conceptual foundations of the renormalization-group (RG) formalism, and prove some...
In numerical calculations of a quantity Λ(T)≡-∂lnχEA′/∂T, where χEA′≡Σ(〈σiσj〉T2)J for finite L×L Edw...
We reconsider the conceptual foundations of the renormalization-group (RG) formalism, and prove some...
We study the decimation to a sublattice of half the sites of the one-dimensional Dyson-Ising ferroma...
We consider disordered lattice spin models with finite volume Gibbs measures μ Λ[η](dσ). Here σ deno...
We show how decimated Gibbs measures having unbroken continuous symmetry due to the Mermin-Wagner th...
We extend proofs of non-Gibbsianness of decimated Gibbs measures at low temperatures to include long...
International audienceWe extend proofs of non-Gibbsianness of decimated Gibbs measures at low temper...
We generalize a result of Lebowitz and Maes, that projections of massless Gaussian measures onto Isi...
It is known that the joint measures on the product of spin-space and disorder space are very often n...
We consider Ising-spin systems starting from an initial Gibbs measure 1) and evolving under a spin-f...
The finite-volume microscopic behaviour of a system in equilibrium is de¬termined by the Boltzmann-G...
Abstract: We consider Ising-spin systems starting from an initial Gibbs measure ν and evolving under...
We generalize a result of Lebowitz and Maes, that projections of massless Gaussian measures onto Isi...
We consider Ising-spin systems starting from an initial Gibbs measure ν and evolving under a spin-fl...
We reconsider the conceptual foundations of the renormalization-group (RG) formalism, and prove some...
In numerical calculations of a quantity Λ(T)≡-∂lnχEA′/∂T, where χEA′≡Σ(〈σiσj〉T2)J for finite L×L Edw...
We reconsider the conceptual foundations of the renormalization-group (RG) formalism, and prove some...
We study the decimation to a sublattice of half the sites of the one-dimensional Dyson-Ising ferroma...
We consider disordered lattice spin models with finite volume Gibbs measures μ Λ[η](dσ). Here σ deno...