82 research outputs found
Asymptotic freedom with discrete spin variables?
We study the critical behaviour of the 2d dodecahedron spin model and
investigate the conjecture that the discrete model describes the same continuum
theory as the O(3) non-linear sigma model. In particular, we found that the
anisotropy of the magnetization A(z) measured in a fixed physical volume
decreases with increasing correlation length, at least up to \xi \approx 1000.Comment: 5 pages, 4 figure
Isospin susceptibility in the O() sigma-model in the delta-regime
We compute the isospin susceptibility in an effective O() scalar field
theory (in dimensions), to third order in chiral perturbation theory
(PT) in the delta--regime using the quantum mechanical rotator picture.
This is done in the presence of an additional coupling, involving a parameter
, describing the effect of a small explicit symmetry breaking term (quark
mass). For the chiral limit we demonstrate consistency with our
previous PT computations of the finite-volume mass gap and isospin
susceptibility. For the massive case by computing the leading mass effect in
the susceptibility using PT with dimensional regularization, we determine
the PT expansion for to third order. The behavior of the shape
coefficients for long tube geometry obtained here might be of broader interest.
The susceptibility calculated from the rotator approximation differs from the
PT result in terms vanishing like for .
We show that this deviation can be described by a correction to the rotator
spectrum proportional to the square of the quadratic Casimir invariant.Comment: 34 page
New fixed point action for SU(3) lattice gauge theory
We present a new fixed point action for SU(3) lattice gauge theory, which has --- compared to earlier published fixed point actions --- shorter interaction range and smaller violations of rotational symmetry in the static q\bar{q}-potential even at shortest distances
Non-trivial \theta-Vacuum Effects in the 2-d O(3) Model
We study \theta-vacua in the 2-d lattice O(3) model using the standard action
and an optimized constraint action with very small cut-off effects, combined
with the geometric topological charge. Remarkably, dislocation lattice
artifacts do not spoil the non-trivial continuum limit at \theta\ non-zero, and
there are different continuum theories for each value of \theta. A very precise
Monte Carlo study of the step scaling function indirectly confirms the exact
S-matrix of the 2-d O(3) model at \theta = \pi.Comment: 4 pages, 3 figure
Casimir squared correction to the standard rotator Hamiltonian for the O() sigma-model in the delta-regime
In a previous paper we found that the isospin susceptibility of the O()
sigma-model calculated in the standard rotator approximation differs from the
next-to-next to leading order chiral perturbation theory result in terms
vanishing like for and further showed that
this deviation could be described by a correction to the rotator spectrum
proportional to the square of the quadratic Casimir invariant. Here we confront
this expectation with analytic nonperturbative results on the spectrum in 2
dimensions, by Balog and Heged\"us for and by Gromov, Kazakov and
Vieira for . We also consider the case of 3 dimensions.Comment: 25 pages, 1 figur
Study of theta-Vacua in the 2-d O(3) Model
We investigate the continuum limit of the step scaling function in the 2-d
O(3) model with different theta-vacua. Since we find a different continuum
value of the step scaling function for each value of theta, we can conclude
that theta indeed is a relevant parameter of the theory and does not get
renormalized non-perturbatively. Furthermore, we confirm the result of the
conjectured exact S-matrix theory, which predicts the continuum value at theta
= pi. To obtain high precision data, we use a modified Hasenbusch improved
estimator and an action with an optimized constraint, which has very small
cut-off effects. The optimized constraint action combines the standard action
of the 2-d O(3) model with a topological action. The topological action
constrains the angle between neighboring spins and is therefore invariant
against small deformations of the field.Comment: 7 pages, 4 figures, The 30 International Symposium on Lattice Field
Theory - Lattice 2012, June 24-29, 2012, Cairns, Australi
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