5,625 research outputs found
Does HBT Measure the Freeze-out Source Distribution?
It is generally assumed that as a result of multiple scattering, the source
distribution measured in HBT interferometry corresponds to a chaotic source at
freeze-out. This assumption is subject to question as effects of multiple
scattering in HBT measurements must be investigated within a quantum-mechanical
framework. Applying the Glauber multiple scattering theory at high energies and
the optical model at lower energies, we find that multiple scattering leads to
an effective HBT density distribution that depends on the initial chaotic
source distribution with an absorption.Comment: 4 pages, talk presented at QM2004 Conference, January 11-17, 2004,
Oakland, California, USA, to be published in the Proceeding
Ordering in the dilute weakly-anisotropic antiferromagnet Mn(0.35)Zn(0.65)F2
The highly diluted antiferromagnet Mn(0.35)Zn(0.65)F2 has been investigated
by neutron scattering in zero field. The Bragg peaks observed below the Neel
temperature TN (approximately 10.9 K) indicate stable antiferromagnetic
long-range ordering at low temperature. The critical behavior is governed by
random-exchange Ising model critical exponents (nu approximately 0.69 and gamma
approximately 1.31), as reported for Mn(x)Zn(1-x)F2 with higher x and for the
isostructural compound Fe(x)Zn(1-x)F2. However, in addition to the Bragg peaks,
unusual scattering behavior appears for |q|>0 below a glassy temperature Tg
approximately 7.0 K. The glassy region T<Tg corresponds to that of noticeable
frequency dependence in earlier zero-field ac susceptibility measurements on
this sample. These results indicate that long-range order coexists with
short-range nonequilibrium clusters in this highly diluted magnet.Comment: 7 pages, 5 figure
Ground state properties of a one-dimensional strongly-interacting Bose-Fermi mixture in a double-well potential
We calculate the reduced single-particle density matrix (RSPDM), momentum
distributions, natural orbitals and their occupancies, for a strongly
interacting one-dimensional Bose-Fermi mixture in a double-well potential with
a large central barrier. For mesoscopic systems, we find that the ground state
properties qualitatively differ for mixtures with even number of particles
(both odd-odd and even-even mixtures) in comparison to mixtures with odd
particle numbers (odd-even and even-odd mixtures). For even mixtures the
momentum distribution is smooth, whereas the momentum distribution of odd
mixtures possesses distinct modulations; the differences are observed also in
the off-diagonal correlations of the RSPDM, and in the occupancies of natural
orbitals. The calculation is based on a derived formula which enables efficient
calculation of the RSPDM for mesoscopic mixtures in various potentials.Comment: 10 figure
Tropicalization of Canonical Curves: the Planar Case
We study a topological version of the tropical lifting problem for canonical
curves. This leads us to a tropical analogue of the notion of graph curves that
we refer to as tropical graph curves. We study the analogous tropical lifting
problem for graph curves and use this as a tool to show that every three
regular, three edge connected planar graph of a given genus can be realized as
the tropicalization of a canonical curve of the same genus.Comment: 26 pages, 14 Figures. This Is a revised version of our preprint
"Tropical Graph Curves". We have completely rewritten the introduction,
revised the body of the paper including several proofs and added a new
section "Conclusion and Future Work
A generalisation of the fractional Brownian field based on non-Euclidean norms
We explore a generalisation of the L\'evy fractional Brownian field on the
Euclidean space based on replacing the Euclidean norm with another norm. A
characterisation result for admissible norms yields a complete description of
all self-similar Gaussian random fields with stationary increments. Several
integral representations of the introduced random fields are derived. In a
similar vein, several non-Euclidean variants of the fractional Poisson field
are introduced and it is shown that they share the covariance structure with
the fractional Brownian field and converge to it. The shape parameters of the
Poisson and Brownian variants are related by convex geometry transforms, namely
the radial th mean body and the polar projection transforms.Comment: 28 pages, To appear in J. Math. Anal. App
Effective and Asymptotic Critical Exponents of Weakly Diluted Quenched Ising Model: 3d Approach Versus -Expansion
We present a field-theoretical treatment of the critical behavior of
three-dimensional weakly diluted quenched Ising model. To this end we analyse
in a replica limit n=0 5-loop renormalization group functions of the
-theory with O(n)-symmetric and cubic interactions (H.Kleinert and
V.Schulte-Frohlinde, Phys.Lett. B342, 284 (1995)). The minimal subtraction
scheme allows to develop either the -expansion series or to
proceed in the 3d approach, performing expansions in terms of renormalized
couplings. Doing so, we compare both perturbation approaches and discuss their
convergence and possible Borel summability. To study the crossover effect we
calculate the effective critical exponents providing a local measure for the
degree of singularity of different physical quantities in the critical region.
We report resummed numerical values for the effective and asymptotic critical
exponents. Obtained within the 3d approach results agree pretty well with
recent Monte Carlo simulations. -expansion does not allow
reliable estimates for d=3.Comment: 35 pages, Latex, 9 eps-figures included. The reference list is
refreshed and typos are corrected in the 2nd versio
d=3 random field behavior near percolation
The highly diluted antiferromagnet Mn(0.35)Zn(0.65)F2 has been investigated
by neutron scattering for H>0. A low-temperature (T<11K), low-field (H<1T)
pseudophase transition boundary separates a partially antiferromagnetically
ordered phase from the paramagnetic one. For 1<H<7T at low temperatures, a
region of antiferromagnetic order is field induced but is not enclosed within a
transition boundary.Comment: 9 pages, 4 figure
F-Theory on all Toric Hypersurface Fibrations and its Higgs Branches
We consider F-theory compactifications on genus-one fibered Calabi-Yau
manifolds with their fibers realized as hypersurfaces in the toric varieties
associated to the 16 reflexive 2D polyhedra. We present a base-independent
analysis of the codimension one, two and three singularities of these
fibrations. We use these geometric results to determine the gauge groups,
matter representations, 6D matter multiplicities and 4D Yukawa couplings of the
corresponding effective theories. All these theories have a non-trivial gauge
group and matter content. We explore the network of Higgsings relating these
theories. Such Higgsings geometrically correspond to extremal transitions
induced by blow-ups in the 2D toric varieties. We recover the 6D effective
theories of all 16 toric hypersurface fibrations by repeatedly Higgsing the
theories that exhibit Mordell-Weil torsion. We find that the three Calabi-Yau
manifolds without section, whose fibers are given by the toric hypersurfaces in
P^2, P^1x P^1 and the recently studied P^2(1,1,2), yield F-theory realizations
of SUGRA theories with discrete gauge groups Z_3, Z_2 and Z_4. This opens up a
whole new arena for model building with discrete global symmetries in F-theory.
In these three manifolds, we also find codimension two I_2-fibers supporting
matter charged only under these discrete gauge groups. Their 6D matter
multiplicities are computed employing ideal techniques and the associated
Jacobian fibrations. We also show that the Jacobian of the biquadric fibration
has one rational section, yielding one U(1)-gauge field in F-theory.
Furthermore, the elliptically fibered Calabi-Yau manifold based on dP_1 has a
U(1)-gauge field induced by a non-toric rational section. In this model, we
find the first F-theory realization of matter with U(1)-charge q=3.Comment: 129 pages, 32 figures, 44 tables v2: minor changes, references adde
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