• Tidak ada hasil yang ditemukan

sigma11-053. 1793KB Jun 04 2011 12:10:53 AM

N/A
N/A
Protected

Academic year: 2017

Membagikan "sigma11-053. 1793KB Jun 04 2011 12:10:53 AM"

Copied!
18
0
0

Teks penuh

Loading

Gambar

Figure 1. Action of the Fourier group on the sphere (from [21]).
Figure 2.Cartesian eigenvalues following the asignments of position and energy generators in (4.2)within the algebra so(4)
Figure 4. Polar eigenvalues following the asignments of radius and angle in (reduction4.17) within the algebra so(4) ⊃ so(3) ⊃ so(2) in (4.14)
Figure 5.Basis of mode-angular momentum eigenstates on the polar array of radius and angle,Ψn,m◦(ρ, φk) in (4.19).
+5

Referensi

Dokumen terkait

The aim of this paper is to show that it is possible to tackle the problem of quantizing an extension of the PU oscillator within a Lagrangian and a canonical ormulation, using

In other words, the transformation of phase superspace coordinates to super-Darboux form is canonical when restricted to physical variables, and hence quantization in the new

Surprisingly, the on-shell actions, with all auxiliary fields eliminated, admit a direct extension to the gauge group SU(N) and general self-dual backgrounds [ 19 , 20 , 21 ].. It

The first is to give an orbital description of the decomposition of τ into irreducibles, in the case when G is a connected, simply connected one-parameter metabelian nilpotent

In Section 5 we investigate the symmetric and antisymmetric vector-valued Jack polynomials in relation with connectivity of the Yang–Baxter graph whose affine edges have been

On the other hand, it is important to remember that the first-order transformations induced in the new potential a delta term with an opposite sign compared with the initial

By considering the fact that several of the translations on the lattice of connection preserving deformations present equivalent evolution equations, we recover an automorphism

It is suggested by our method that most of the quadratic algebras for all St¨ ackel equivalence classes of 3D second order quantum superintegrable systems on conformally flat