1,406 research outputs found
Dynamical Generation of Yukawa Interactions in Intersecting D-brane Models
We construct a supersymmetric composite model in type IIA T^6/(Z_2 x Z_2)
orientifold with intersecting D6-branes. Four generations of quarks and leptons
are naturally emerged as composite fields at low energies. Two pairs of light
electroweak Higgs doublets are also naturally obtained. The hierarchical Yukawa
couplings for the quark-lepton masses can be generated by the interplay between
the string-level higher dimensional interactions among "preons" and the
dynamics of the confinement of "preons". Besides having four generations of
quarks and leptons, the model is not realistic in some points: some exotic
particles, one additional U(1) gauge symmetry, no explicit mechanism for
supersymmetry breaking, and so on. This model is a toy model to illustrate a
new mechanism of dynamical generation of Yukawa couplings for the masses and
mixings of quarks and leptons.Comment: 18 pages, 6 figure
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Improved polyurethane and epoxy resins for use as adhesives at cryogenic temperature
Finite-Field Ground State of the S=1 Antiferromagnetic-Ferromagnetic Bond-Alternating Chain
We investigate the finite-field ground state of the S=1
antiferromagnetic-ferromagnetic bond-alternating chain described by the
Hamiltonian
{\calH}=\sum\nolimits_{\ell}\bigl\{\vecS_{2\ell-1}\cdot\vecS_{2\ell}
+J\vecS_{2\ell}\cdot\vecS_{2\ell+1}\bigr\} +D\sum\nolimits_{\ell}
\bigl(S_{\ell}^z)^2 -H\textstyle\sum\nolimits_\ell S_\ell^z, where
\hbox{} and \hbox{}. We find that two kinds of
magnetization plateaux at a half of the saturation magnetization, the
1/2-plateaux, appear in the ground-state magnetization curve; one of them is of
the Haldane type and the other is of the large--type. We determine the
1/2-plateau phase diagram on the versus plane, applying the
twisted-boundary-condition level spectroscopy methods developed by Kitazawa and
Nomura. We also calculate the ground-state magnetization curves and the
magnetization phase diagrams by means of the density-matrix
renormalization-group method
N=4 Supersymmetric Yang-Mills on S^3 in Plane Wave Matrix Model at Finite Temperature
We investigate the large N reduced model of gauge theory on a curved
spacetime through the plane wave matrix model. We formally derive the action of
the N=4 supersymmetric Yang-Mills theory on R \times S^3 from the plane wave
matrix model in the large N limit. Furthermore, we evaluate the effective
action of the plane wave matrix model up to the two-loop level at finite
temperature. We find that the effective action is consistent with the free
energy of the N=4 supersymmetric Yang-Mills theory on S^3 at high temperature
limit where the planar contributions dominate. We conclude that the plane wave
matrix model can be used as a large N reduced model to investigate
nonperturbative aspects of the N=4 supersymmetric Yang-Mills theory on R \times
S^3.Comment: 31pages: added comments and reference
Phase diagram of S=1 XXZ chain with next-nearest neighbor interaction
The one dimensional S=1 XXZ model with next-nearest-neighbor interaction
and Ising-type anisotropy is studied by using a numerical
diagonalization technique. We discuss the ground state phase diagram of this
model numerically by the twisted-boundary-condition level spectroscopy method
and the phenomenological renormalization group method, and analytically by the
spin wave theory. We determine the phase boundaries among the XY phase, the
Haldane phase, the ferromagnetic phase and the N\'{e}el phase, and then we
confirm the universality class. Moreover, we map this model onto the non-linear
model and analyze the phase diagram in the -1 and
1 region by using the renormalization group method.Comment: 18 pages, 10 figure
Scaling Behavior of Ricci Curvature at Short Distance near Two Dimensions
We study the renormalization of the Ricci curvature as an example of
generally covariant operators in quantum gravity near two dimensions. We find
that it scales with a definite scaling dimension at short distance. The Ricci
curvature singularity at the big bang can be viewed as such a scaling
phenomenon. The problem of the spacetime singularity may be resolved by the
scale invariance of the spacetime at short distance.Comment: 9pages, LaTe
Magnetization-plateau state of the S=3/2 spin chain with single ion anisotropy
We reexamine the numerical study of the magnetized state of the S=3/2 spin
chain with single ion anisotropy D(> 0) for the magnetization M=M_{S}/3, where
M_{S} is the saturation magnetization. We find at this magnetization that for
D<D_{c1}=0.387 the system is critical and the magnetization plateau does not
appear. For D > D_{c1}, the parameter region is divided into two parts D_{c1} <
D < D_{c2}=0.943 and D_{c2} < D. In each region, the system is gapful and the
M=M_{S}/3 magnetization plateau appears in the magnetization process. From our
numerical calculation, the intermediate region D_{c1} < D < D_{c2} should be
characterized by a magnetized valence-bond-solid state.Comment: 6 pages, 8 figure
BCS theory of hadronic matter at high densities
The equilibrium between the so-called 2SC and CFL phases of strange quark
matter at high densities is investigated in the framework of a simple schematic
model of the NJL type. Equal densities are assumed for quarks and .
The 2SC phase is here described by a color-flavor symmetric state, in which the
quark numbers are independent of the color-flavor combination. In the CFL phase
the quark numbers depend on the color-flavor combination, that is, the number
of quarks associated with the color-flavor combinations is different
from the number of quarks associated with the color flavor combinations
. We find that the 2SC phase is stable for a chemical
potential below GeV, while the CFL phase is stable above,
the equilibrium pressure being GeV. We have used a 3-momentum
regularizing cutoff GeV, which is somewhat larger than is usual
in NJL type models. This should be adequate if the relevant chemical potential
does not exceed 0.6 GeV.Comment: 6 figures, 13 page
Magnetic properties of the distorted diamond chain at T=0
We explore, at T=0, the magnetic properties of the antiferromagnetic
distorted diamond chain described by the Hamiltonian {\cal H}
= \sum_{j=1}^{N/3}{J_1 ({\bi S}_{3j-1} \cdot {\bi S}_{3j}
+ {\bi S}_{3j} \cdot {\bi S}_{3j+1})
+ J_2 {\bi S}_{3j+1} \cdot {\bi S}_{3j+2}
+ J_3 ({\bi S}_{3j-2} \cdot {\bi S}_{3j}
+ {\bi S}_{3j} \cdot {\bi S}_{3j+2})}
\allowbreak - H \sum_{l=1}^{N} S_l^z with , which well
models with , and azurite . We employ the physical
consideration, the degenerate perturbation theory, the level spectroscopy
analysis of the numerical diagonalization data obtained by the Lanczos method
and also the density matrix renormalization group (DMRG) method. We investigate
the mechanisms of the magnetization plateaux at and , and
also show the precise phase diagrams on the plane
concerning with these magnetization plateaux, where
and is the saturation magnetization. We also calculate the magnetization
curves and the magnetization phase diagrams by means of the DMRG method.Comment: 21 pages, 29 figure
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