[PDF] Top 20 sigma08-029. 411KB Jun 04 2011 12:10:14 AM
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sigma08-029. 411KB Jun 04 2011 12:10:14 AM
... of the MMKdV Q(x, t). Some of these facts have been discussed in more details in [10], others had to be modified and extended so that they adequately take into account the peculiarities of the DIII type symmetric ... Lihat dokumen lengkap
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sigma08-025. 269KB Jun 04 2011 12:10:14 AM
... In the rational models of CFT with boundary the singular vectors problem appears again when we try to construct the Ishibashi and boundary states because we need to introduce an orthonormal basis for each irreducible ... Lihat dokumen lengkap
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sigma08-028. 226KB Jun 04 2011 12:10:14 AM
... depends on the tangent vector ˙ γ to the transporting curve γ ). Thus the effect of additional noncommutative “Lorentz-like” force is an infinitesimal rotation of actual velocity that precedes the next “commutative” ... Lihat dokumen lengkap
9
sigma08-027. 279KB Jun 04 2011 12:10:14 AM
... [13] Popovych H.V., On SO(3)-partially invariant solutions of the Euler equations, in Proceedings of Third International Conference “Symmetry in Nonlinear Mathematical Physics” (June 12–18, 1999, Kyiv), Editors ... Lihat dokumen lengkap
19
sigma08-026. 691KB Jun 04 2011 12:10:14 AM
... also particle models with non-commutative gauge theory were explored [3] (see also [4]), [5, 6]. On the other hand the present intensive research has been triggered by the natural realiza- tion of non-commutativity of ... Lihat dokumen lengkap
26
sigma08-023. 357KB Jun 04 2011 12:10:14 AM
... There are much motivations to explore the SUSY QHE. With the developments of string theory, it was found that the non-anti-commutative geometry is naturally realized on D-brane in gravi- photon background [12, 13, ... Lihat dokumen lengkap
21
sigma08-021. 467KB Jun 04 2011 12:10:14 AM
... Several simplest solutions of these unitarity equations have been found: three 2-parametric subgroups G1, G2, G3 – each of subgroups consists of two commuting Abelian unitary groups; 4-[r] ... Lihat dokumen lengkap
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sigma08-022. 404KB Jun 04 2011 12:10:14 AM
... At the same time we have to point out that the manifestly covariant Lagrangian approach to duality-symmetric theories [8], which is in the focus of the paper, is not the only way to construct the least action principle ... Lihat dokumen lengkap
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sigma08-024. 350KB Jun 04 2011 12:10:14 AM
... quark interaction [13]. Their inclusion leads to a scalar effective potential which is globally stable and to a full equivalence between the stationary phase approach (SPA) and the mean field (MF) approximation methods ... Lihat dokumen lengkap
14
sigma11-029. 396KB Jun 04 2011 12:10:50 AM
... The study of one-dimensional Hamiltonians with a point interaction has received renewed atten- tion during the past two decades [1, 2, 3, 4, 5, 6, 7]. In general, a point interaction is described by a potential ... Lihat dokumen lengkap
14
sigma08-012. 425KB Jun 04 2011 12:10:13 AM
... It is not easy to guess how Nature can choose its path from the SM to the Planck scale. Different paths essentially depend on the fact whether the intermediate symmetry groups show asymp- totically free or asymptotically ... Lihat dokumen lengkap
15
sigma08-001. 230KB Jun 04 2011 12:10:11 AM
... but also in certain equations employed in quantum cosmology [13], in non-Hermitian but PT - symmetric coupled-channel problems [14] and, unexpectedly, even in classical magnetohydro- dynamics [15] and ... Lihat dokumen lengkap
9
sigma08-011. 301KB Jun 04 2011 12:10:13 AM
... In the present paper we generalize the method of [3, 10] of producing soliton equations and their U -V pairs, filling the gap described above, i.e. making the method to include all known soliton equations, and ... Lihat dokumen lengkap
19
sigma08-014. 190KB Jun 04 2011 12:10:13 AM
... [11, 12, 13], Nasiri [9] has shown that in the Wigner representation of phase space quantum mechanics [14] the quantum potential is removed from the dynamical equation of a particle in linear and harmonic ... Lihat dokumen lengkap
7
sigma08-013. 333KB Jun 04 2011 12:10:13 AM
... | Φ i = (φ + φ µ α µ † + φ µν α µ † α † ν + φ µνρ α † µ α † ν α † ρ + · · · ) | 0 i . (2.3) This yields a concrete calculational scheme and one could hope to be able to rig some kind of kinetic operator K which when ... Lihat dokumen lengkap
23
sigma08-015. 293KB Jun 04 2011 12:10:13 AM
... Further simple analysis of the relation (8.6) allows to obtain explicit expressions for A(s) and B(s). It appears (we omit technical details) that corresponding operator H coincides with the difference Askey–Wilson ... Lihat dokumen lengkap
22
sigma09-029. 321KB Jun 04 2011 12:10:25 AM
... explicitly the procedure to define, in the quantum Gaudin algebras, a set of generators that reduce in the classical case to the usual traces of powers of the Lax matrix.. Besides the fu[r] ... Lihat dokumen lengkap
17
sigma10-029. 272KB Jun 04 2011 12:10:38 AM
... In [7, 8] the solutions of Yang–Baxter relation have been constructed and studied with restriction to cyclic representations of sℓqn+ 1 and with the algebra relations modified for applic[r] ... Lihat dokumen lengkap
16
sigma08-003. 179KB Jun 04 2011 12:10:12 AM
... 5 Duality From the general theory of Poisson–Lie symmetry presented in Section 2, we know that both symmetry Lie algebras GL = Lie LG and GR = Lie ¯B act on the phase space P∞ of the [r] ... Lihat dokumen lengkap
5
sigma07-029. 237KB Jun 04 2011 12:10:00 AM
... We shall now give a weight to a ribbon ζ/µ. Number boxes of the diagram of ζ uniformly in each diagonal, by 1, 2, 3, . . ., starting from the top leftmost box. For each box of ζ/µ, denote c( ) this number (this is a ... Lihat dokumen lengkap
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