216 research outputs found
Detailed Phase Transition Study at M_H <= 70 GeV in a 3-dimensional --Higgs Model
We study the electroweak phase transition in an effective 3-dimensional
theory for a Higgs mass of about 70 GeV by Monte Carlo simulations. The
transition temperature and jumps of order parameters are obtained and
extrapolated to the continuum using multi-histogram techniques and finite size
analysis.Comment: Talk presented at LATTICE96(electroweak), 4 pages, 5 figure
Physics of the Electroweak Phase Transition at M_H <= 70 GeV in a 3-dimensional SU(2)-Higgs Model
Physical parameters of the electroweak phase transition in a 3d effective
lattice SU(2)-Higgs model are presented. The phase transition temperatures,
latent heats and continuum condensate discontinuities are measured at Higgs
masses of about 70 and 35 GeV. Masses and Higgs condensates are compared to
perturbation theory in the broken phase. In the symmetric phase bound states
and the static force are determined.Comment: Talk presented at LATTICE96(electroweak), 4 pages, 5 figure
3-D lattice simulation of the electroweak phase transition at small Higgs mass
We study the electroweak phase transition by lattice simulations of an
effective 3-dimensional theory, for a Higgs mass of about . In the
broken symmetry phase our results on masses and the Higgs condensate are
consistent with 2-loop perturbative results. However, we find a
non-perturbative lowering of the transition temperature, similar to the one
previously found at . For the symmetric phase, bound state masses
and the static force are determined and compared with results for pure
theory.Comment: 11 pages, uuencoded ps-file, 5 postscript figures include
--Dimensional Approach to Hot Electroweak Matter for GeV
We study the electroweak phase transition by lattice simulations of an
effective 3-dimensional theory, for a Higgs mass of about GeV. Exploiting
a variant of the equal weight criterion of phase equilibrium, we obtain
transition temperature, latent heat and surface tension and compare with GeV. For the symmetric phase, bound state masses and the static
force are determined and compared with results for pure theory.Comment: 6 pages with 4 figures, latex,postscript figures and uuencode
Phase transitions in two dimensions - the case of Sn adsorbed on Ge(111) surfaces
Accurate atomic coordinates of the room-temperature (root3xroot3)R30degree
and low-temperature (3x3) phases of 1/3 ML Sn on Ge(111) have been established
by grazing-incidence x-ray diffraction with synchrotron radiation. The Sn atoms
are located solely at T4-sites in the (root3xroot3)R30degree structure. In the
low temperature phase one of the three Sn atoms per (3x3) unit cell is
displaced outwards by 0.26 +/- 0.04 A relative to the other two. This
displacement is accompanied by an increase in the first to second double-layer
spacing in the Ge substrate.Comment: RevTeX, 5 pages including 2 figure
Determination of the (3x3)-Sn/Ge(111) structure by photoelectron diffraction
At a coverage of about 1/3 monolayer, Sn deposited on Ge(111) below 550 forms
a metastable (sqrt3 x sqrt3)R30 phase. This phase continuously and reversibly
transforms into a (3x3) one, upon cooling below 200 K. The photoemission
spectra of the Sn 4d electrons from the (3x3)-Sn/Ge(111) surface present two
components which are attributed to inequivalent Sn atoms in T4 bonding sites.
This structure has been explored by photoelectron diffraction experiments
performed at the ALOISA beamline of the Elettra storage ring in Trieste
(Italy). The modulation of the intensities of the two Sn components, caused by
the backscattering of the underneath Ge atoms, has been measured as a function
of the emission angle at fixed kinetic energies and viceversa. The bond angle
between Sn and its nearest neighbour atoms in the first Ge layer (Sn-Ge1) has
been measured by taking polar scans along the main symmetry directions and it
was found almost equivalent for the two components. The corresponding bond
lengths are also quite similar, as obtained by studying the dependence on the
photoelectron kinetic energy, while keeping the photon polarization and the
collection direction parallel to the Sn-Ge1 bond orientation (bond emission). A
clear difference between the two bonding sites is observed when studying the
energy dependence at normal emission, where the sensitivity to the Sn height
above the Ge atom in the second layer is enhanced. This vertical distance is
found to be 0.3 Angstroms larger for one Sn atom out of the three contained in
the lattice unit cell. The (3x3)-Sn/Ge(111) is thus characterized by a
structure where the Sn atom and its three nearest neighbour Ge atoms form a
rather rigid unit that presents a strong vertical distortion with respect to
the underneath atom of the second Ge layer.Comment: 10 pages with 9 figures, added reference
Surface Phase Transitions Induced by Electron Mediated Adatom-Adatom Interaction
We propose that the indirect adatom-adatom interaction mediated by the
conduction electrons of a metallic surface is responsible for the
structural phase transitions
observed in Sn/Ge (111) and Pb/Ge (111). When the indirect interaction
overwhelms the local stress field imposed by the substrate registry, the system
suffers a phonon instability, resulting in a structural phase transition in the
adlayer. Our theory is capable of explaining all the salient features of the
transitions observed in
Sn/Ge (111) and Pb/Ge (111), and is in principle applicable to a wide class of
systems whose surfaces are metallic before the transition.Comment: 4 pages, 5 figure
The Growth of Bubbles in Cosmological Phase Transitions
We study how bubbles grow after the initial nucleation event in generic
first-order cosmological phase transitions characterised by the values of
latent heat, interface tension and correlation length, and driven by a scalar
order parameter . Equations coupling and the fluid variables
and and depending on a dissipative constant are derived and solved
numerically in the 1+1 dimensional case starting from a slightly deformed
critical bubble configuration. Parameters corresponding to QCD and electroweak
phase transitions are chosen and the whole history of the bubble with formation
of combustion and shock fronts is computed as a function of . Both
deflagrations and detonations can appear depending on the values of the
parameters. Reheating due to collisions of bubbles is also computed.Comment: 24 LaTeX-pages with 20 figures not included. The complete PostScript
file, including figures, is available by anonymous ftp from
fltxc.helsinki.fi, as /pub/bubble.ps, or as a hardcopy by airmail (a
dublicate lies at nic.funet.fi:/pub/sci/physics/papers/bubble.ps). Helsinki
Preprint HU-TFT-93-4
Inhomogeneous Field Configurations and the Electroweak Phase Transition
We investigate the effects of inhomogeneous scalar field configurations on
the electroweak phase transition. For this purpose we calculate the leading
perturbative correction to the wave function correction term Z(\vph,T), i.e.,
the kinetic term in the effective action, for the electroweak Standard Model at
finite temperature and the top quark self--mass. Our finding for the fermionic
contribution to Z(\vph,T) is infra--red finite and disagrees with other
recent results. In general, neither the order of the phase transition nor the
temperature at which it occurs change, once Z(\vph,T) is included. But a
non--vanishing, positive (negative) Z(\vph,T) enhances (decreases) the
critical droplet surface tension and the strength of the phase transition. We
find that in the range of parameter space, which allows for a first--order
phase transition, the wave function correction term is negative --- indicating
a weaker phase transition --- and especially for small field values so large
that perturbation theory becomes unreliable.Comment: 23 pages of LaTeX + 3 PostScript figures included in uuencoded form,
FERMI-PUB-93/253-
Maximal variance reduction for stochastic propagators with applications to the static quark spectrum
We study a new method -- maximal variance reduction -- for reducing the
variance of stochastic estimators for quark propagators. We find that while
this method is comparable to usual iterative inversion for light-light mesons,
a considerable improvement is achieved for systems containing at least one
infinitely heavy quark. Such systems are needed for heavy quark effective
theory. As an illustration of the effectiveness of the method we present
results for the masses of the ground state and excited states of
mesons and baryons. We compare these results with the experimental
spectra involving quarks.Comment: 31 pages with 7 postscript file
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