491 research outputs found
Critical behaviour of a spin-tube model in a magnetic field
We show that the low-energy physics of the spin-tube model in presence of a
critical magnetic field can be described by a broken SU(3) spin chain. Using
the Lieb-Schultz-Mattis Theorem we characterize the possible magnetization
plateaus and study the critical behavior in the region of transition between
the plateaus m=1/2 and m=3/2 by means of renormalization group calculations
performed on the bosonized effective continuum field theory. We show that in
certain regions of the parameter space of the effective theory the system
remains gapless, and we compute the spin-spin correlation functions in these
regions. We also discuss the possibility of a plateau at m=1, and show that
although there exists in the continuum theory a term that might cause the
appearance of a plateau there, such term is unlikely to be relevant. This
conjecture is proved by DMRG techniques. The modifications of the three-leg
ladder Hamiltonian that might show plateaus at m =1,5/6,7/6 are discussed, and
we give the expected form of correlation functions on the m=1 plateau.Comment: RevTeX, 43 pages, 5 EPS figure
Phase diagram of a 1 dimensional spin-orbital model
We study a 1 dimensional spin-orbital model using both analytical and
numerical methods. Renormalization group calculations are performed in the
vicinity of a special integrable point in the phase diagram with SU(4)
symmetry. These indicate the existence of a gapless phase in an extended region
of the phase diagram, missed in previous studies. This phase is SU(4) invariant
at low energies apart from the presence of different velocities for spin and
orbital degrees of freedom. The phase transition into a gapped dimerized phase
is in a generalized Kosterlitz-Thouless universality class. The phase diagram
of this model is sketched using the density matrix renormalization group
technique.Comment: 11 pages, 5 figures, new references adde
Stability of fixed points in the (4+\epsilon)-dimensional random field O(N) spin model for sufficiently large N
We study the stability of fixed points in the two-loop renormalization group
for the random field O() spin model in dimensions. We solve the
fixed-point equation in the 1/N expansion and expansion. In the
large-N limit, we study the stability of all fixed points. We solve the
eigenvalue equation for the infinitesimal deviation from the fixed points under
physical conditions on the random anisotropy function. We find that the fixed
point corresponding to dimensional reduction is singly unstable and others are
unstable or unphysical. Therefore, one has no choice other than dimensional
reduction in the large-N limit. The two-loop function enables us to
find a compact area in the plane where the dimensional reduction
breaks down. We calculate higher-order corrections in the 1/N and
expansions to the fixed point. Solving the corrected eigenvalue equation
nonperturbatively, we find that this fixed point is singly unstable also for
sufficiently large and the critical exponents show a dimensional reduction.Comment: 9 pages, 2 figure
Function of the Shoulder Muscles during Arm Elevation: An Assessment Using Positron Emission Tomography
On gonihedric loops and quantum gravity
We present an analysis of the gonihedric loop model, a reformulation of the
two dimensional gonihedric spin model, using two different techniques. First,
the usual regular lattice statistical physics problem is mapped onto a height
model and studied analytically. Second, the gravitational version of this loop
model is studied via matrix models techniques. Both methods lead to the
conclusion that the model has for all values of the parameters
of the model. In this way it is possible to understand the absence of a
continuous transition
Antiferromagnetic S=1/2 Heisenberg Chain and the Two-flavor Massless Schwinger Model
An antiferromagnetic S=1/2 Heisenberg chain is mapped to the two-flavor
massless Schwinger model at \theta=\pi. The electromagnetic coupling constant
and velocity of light in the Schwinger model are determined in terms of the
Heisenberg coupling and lattice spacing in the spin chain system.Comment: 3 pages. LaTex2
Arterial bleeding during EUS-guided pseudocyst drainage stopped by placement of a covered self-expandable metal stent
Smooth Paths on Three Dimensional Lattice
A particular class of random walks with a spin factor on a three dimensional
cubic lattice is studied. This three dimensional random walk model is a simple
generalization of random walk for the two dimensional Ising model. All critical
diffusion constants and associated critical exponents are calculated. Continuum
field theories such as Klein-Gordon, Dirac and massive Chern-Simons theories
are constructed near several critical points.Comment: 7 pages,NUP-A-94-
Effect of Hund coupling in the one-dimensional SU(4) Hubbard model
The one-dimensional SU(4) Hubbard model perturbed by Hund coupling is
studied, away from half-filling, by means of renormalization group and
bosonization methods. A spectral gap is always present in the spin-orbital
sector irrespective of the magnitude of the Coulomb repulsion. We further
distinguish between two qualitatively different regimes. At small Hund
coupling, we find that the symmetry of the system is dynamically enlarged to
SU(4) at low energy with the result of {\it coherent} spin-orbital excitations.
When the charge sector is not gapped, a superconducting instability is shown to
exist. At large Hund coupling, the symmetry is no longer enlarged to SU(4) and
the excitations in the spin sector become {\it incoherent}. Furthermore, the
superconductivity can be suppressed in favor of the conventional charge density
wave state.Comment: 10 pages, 1 figur
Charged Black Holes in Two-Dimensional String Theory
We discuss two dimensional string theories containing gauge fields introduced
either via coupling to open strings, in which case we get a Born-Infeld type
action, or via heterotic compactification. The solutions to the modified
background field equations are charged black holes which exhibit interesting
space-time geometries. We also compute their masses and charges.Comment: 39 page
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