96 research outputs found
Finite-size scaling corrections in two-dimensional Ising and Potts ferromagnets
Finite-size corrections to scaling of critical correlation lengths and free
energies of Ising and three-state Potts ferromagnets are analysed by numerical
methods, on strips of width sites of square, triangular and honeycomb
lattices. Strong evidence is given that the amplitudes of the ``analytical''
correction terms, , are identically zero for triangular-- and honeycomb
Ising systems. For Potts spins, our results are broadly consistent with this
lattice-dependent pattern of cancellations, though for correlation lengths
non-vanishing (albeit rather small) amplitudes cannot be entirely ruled out.Comment: 11 pages, LaTeX with Institute of Physics macros, 2 EPS figures; to
appear in Journal of Physics
Bifurcation at the c=3/2 Takhtajan-Babujian point to the c=1 critical lines
We study the S=1 quantum spin chains with bilinear, biquadratic, plus bond
alternation in the vicinity of the S=1 Takhtajan-Babujian model. Transition
line between the Haldane and the dimer phases are determined numerically. To
see the crossover behavior from c=3/2 (k=2 SU(2) WZW model) at the
Takhtajan-Babujian point to c=1 (k=1 SU(2) WZW model), we calculate the
conformal anomaly c and scaling dimensions of the primary fields on the
transition line.Comment: 10 pages, 8 figure
Renormalization group analysis of the spin-gap phase in the one-dimensional t-J model
We study the spin-gap phase in the one-dimensional t-J model, assuming that
it is caused by the backward scattering process. Based on the renormalization
group analysis and symmetry, we can determine the transition point between the
Tomonaga-Luttinger liquid and the spin-gap phases, by the level crossing of the
singlet and the triplet excitations. In contrast to the previous works, the
obtained spin-gap region is unexpectedly large.
We also check that the universality class of the transition belongs to the
SU(2) Wess-Zumino-Witten model.Comment: 4 pages(RevTeX), 5 figures(EPS), TITCMT-97-10, to appear in Phys.
Rev. Let
Global public policy, transnational policy communities, and their networks
Public policy has been a prisoner of the word "state." Yet, the state is reconfigured by globalization. Through "global public–private partnerships" and "transnational executive networks," new forms of authority are emerging through global and regional policy processes that coexist alongside nation-state policy processes. Accordingly, this article asks what is "global public policy"? The first part of the article identifies new public spaces where global policies occur. These spaces are multiple in character and variety and will be collectively referred to as the "global agora." The second section adapts the conventional policy cycle heuristic by conceptually stretching it to the global and regional levels to reveal the higher degree of pluralization of actors and multiple-authority structures than is the case at national levels. The third section asks: who is involved in the delivery of global public policy? The focus is on transnational policy communities. The global agora is a public space of policymaking and administration, although it is one where authority is more diffuse, decision making is dispersed and sovereignty muddled. Trapped by methodological nationalism and an intellectual agoraphobia of globalization, public policy scholars have yet to examine fully global policy processes and new managerial modes of transnational public administration
Tricritical Behavior in the Extended Hubbard Chains
Phase diagrams of the one-dimensional extended Hubbard model (including
nearest-neighbor interaction ) at half- and quarter-filling are studied by
observing level crossings of excitation spectra using the exact
diagonalization. This method is based on the Tomonaga-Luttinger liquid theory
including logarithmic corrections which stem from the renormalization of the
Umklapp- and the backward-scattering effects.
Using this approach, the phase boundaries are determined with high accuracy,
and then the structure of the phase diagram is clarified. At half-filling, the
phase diagram consists of two
Berezinskii-Kosterlitz-Thouless (BKT) transition lines and one Gaussian
transition line in the charge sector, and one spin-gap transition line.
This structure reflects the U(1) SU(2) symmetry of the electron
system. Near the line, the Gaussian and the spin-gap transitions take
place independently from the weak- to the intermediate-coupling region, but
these two transition lines are coupled in the strong-coupling region. This
result demonstrates existence of a tricritical point and a
bond-charge-density-wave (BCDW) phase between charge- and spin-density-wave
(CDW, SDW) phases. To clarify this mechanism of the transition, we also
investigate effect of a correlated hopping term which plays a role to enlarge
BCDW and bond-spin-density-wave (BSDW) phases. At quarter-filling, a similar
crossover phenomenon also takes place in the large- region involving
spin-gap and BKT-type metal-insulator transitions.Comment: 18 pages(REVTeX), 17 figures(EPS(color)), 3 tables, Detailed paper of
JPSJ 68 (1999) 3123 (cond-mat/9903227), see also cond-mat/000341
Spin-Gap Phases in Tomonaga-Luttinger Liquids
We give the details of the analysis for critical properties of spin-gap
phases in one-dimensional lattice electron models. In the Tomonaga-Luttinger
(TL) liquid theory, the spin-gap instability occurs when the backward
scattering changes from repulsive to attractive.
This transition point is shown to be equivalent to that of the level-crossing
of the singlet and the triplet excitation spectra, using the c=1 conformal
field theory and the renormalization group. Based on this notion, the
transition point between the TL liquid and the spin-gap phases can be
determined with high-accuracy from the numerical data of finite-size clusters.
We also discuss the boundary conditions and discrete symmetries to extract
these excitation spectra. This technique is applied to the extended Hubbard
model, the t-J model, and the t-J-J' model, and their phase diagrams are
obtained. We also discuss the relation between our results and analytical
solutions in weak-coupling and low-density limits.Comment: 14 pages(REVTeX), 9 figures(EPS), 1 table, To appear in PRB, Detailed
paper of PRL 79 (1997) 3214 and JPSJ 67 (1998) 71
Expression of the Salmonella Spp. Virulence Factor SifA in Yeast Alters Rho1 Activity on Peroxisomes
SifA is a virulence protein required for assembly and tubulation of a modified phagosome that promotes Salmonella replication. We show that SifA expressed in yeast induces membrane invagination during peroxisome proliferation and requires functional Rho1p. This is consistent with SifA ability to interact with RhoA and the fact that it is a GEF structural homologue
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