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 A. Chakrabarti Mathematics , 1996, Abstract: A two-parametric generalization of the Jordanian deformation $U_h (sl(2))$ of $sl(2)$ is presented. This involves Jacobian elliptic functions. In our deformation $U_{(h,k)}(sl(2))$, for $k^2=1$ one gets back $U_h(sl(2))$. The constuction is presented via a nonlinear map on $sl(2)$. This invertible map directly furnishes the highest weight irreducible representations of $U_{(h,k)}(sl(2))$. This map also provides two distinct induced Hopf stuctures, which are exhibited. One is induced by the classical $sl(2)$ and the other by the distinct one of $U_h(sl(2))$. Automorphisms related to the two periods of the elliptic functions involved are constructed. Translations of one generator by half and quarter periods lead to interesting results in this context. Possibilities of applications are discussed briefly.
 Physics , 1993, DOI: 10.1007/BF00805857 Abstract: When the parameter of deformation q is a m-th root of unity, the centre of U_q(sl(N))$contains, besides the usual q-deformed Casimirs, a set of new generators, which are basically the m-th powers of all the Cartan generators of U_q(sl(N)). All these central elements are however not independent. In this letter, generalising the well-known case of U_q(sl(2)), we explicitly write polynomial relations satisfied by the generators of the centre. Application to the parametrization of irreducible representations and to fusion rules are sketched.  L. D. Faddeev Mathematics , 2007, Abstract: Modular double of quantum group U_q (sl(2)) with deformation parameter q=e^{i\pi\tau} is a natural object explicitly taking into account the duality \tau -> 1/\tau. The use of the modular double in CFT allows to consider the region 1  Physics , 1995, DOI: 10.1016/0550-3213(95)00361-U Abstract: A class of second order difference (discrete) operators with a partial algebraization of the spectrum is introduced. The eigenfuncions of the algebraized part of the spectrum are polinomials (discrete polinomials). Such difference operators can be constructed by means of$U_q(sl_2)$, the quantum deformation of the$sl_2$algebra. The roots of polinomials determine the spectrum and obey the Bethe Ansatz equations. A particular case of difference equations for$q$-hypergeometric and Askey-Wilson polinomials is discussed. Applications to the problem of Bloch electrons in magnetic field are outlined. {abstract}  Azizollah Shafiekhani Physics , 1994, DOI: 10.1142/S0217732394003099 Abstract: A unified and systematic scheme for constraction of differential opreator realization of any irreducible representation of$sl(n)$is developed. The$q$-analogue of this unified scheme is used to constract$q$-difference operator realization of any irreducible representation of$U_q(sl(n))$. Explicit results for$U_q(sl(2))$,$U_q(sl(3))$and$U_q(sl(n))$are given.  Mathematics , 2001, Abstract: We study relations between the two-parameter$\U_q(sl(n))$-invariant deformation quantization on$sl^*(n)$and the reflection equation algebra. The latter is described by a quantum permutation on$\End(\C^n)$given explicitly. The reflection equation algebra is used for constructing the one-parameter quantization on coadjoint orbits, including symmetric and certain bisymmetric and nilpotent ones. Our approach is based on embedding the quantized function algebras on the orbits into the algebra of functions on the quantum group$SL_q(n)$via reflection equation algebra characters.  A. Morozov Physics , 1993, Abstract: Non-abelian coordinate ring of$U_q(SL(N))$(quantum deformation of the algebra of functions) for$N=2,3$is represented in terms of conventional creation and annihilation operators. This allows to construct explicitly representations of this algebra, which were earlier described in somewhat more abstract algebraic fashion. Generalizations to$N>3$and Kac-Moody algebras are not discussed but look straightforward.  Mathematics , 1995, DOI: 10.1088/0305-4470/29/21/009 Abstract: We propose a new structure${\cal U}^{r}_{\displaystyle{q}}(sl(2)) $. This is realized by multiplying$\delta$($q=e^{\delta}$,$\delta\in \CC$) by$\theta$, where$\theta$is a real nilpotent -paragrassmannian- variable of order$r$($\theta^{r+1}=0$) that we call the order of deformation, the limit$r\rightarrow \infty$giving back the standard${\cal U}_{\displaystyle {q}}(sl(2))$. In particular we show that, for$r=1$, there exists a new${\cal R}$-matrix associated with$sl(2)$. We also proof that the restriction of the values of the parameters of deformation give nonlinear algebras as particular cases.  A. Matsuo Physics , 1992, Abstract: The$q$-vertex operators of Frenkel and Reshetikhin are studied by means of a$q$-deformation of the Wakimoto module for the quantum affine algebra$U_q(\widehat{\sl}_2)$at an arbitrary level$k\ne 0,-2$. A Fock module version of the$q$-deformed primary field of spin$j$is introduced, as well as the screening operators which (anti-)commute with the action of$U_q(\widehat{\sl}_2)$up to a total difference of a field. A proof of the intertwining property is given for the$q$-vertex operators corresponding to the primary fields of spin$j\notin {1 \over2}\Z_{\geq0}$, which is enough to treat a general case. A sample calculation of the correlation function is also given.  Mathematics , 2011, DOI: 10.1007/s11005-011-0538-1 Abstract: We consider the class of quantum spin chains with arbitrary$U_q(\mathfrak{sl}_2)$-invariant nearest neighbor interactions, sometimes called$\textrm{SU}_q(2)$for the quantum deformation of$\textrm{SU}(2)$, for$q>0$. We derive sufficient conditions for the Hamiltonian to satisfy the property we call {\em Ferromagnetic Ordering of Energy Levels}. This is the property that the ground state energy restricted to a fixed total spin subspace is a decreasing function of the total spin. Using the Perron-Frobenius theorem, we show sufficient conditions are positivity of all interactions in the dual canonical basis of Lusztig. We characterize the cone of positive interactions, showing that it is a simplicial cone consisting of all non-positive linear combinations of "cascade operators," a special new basis of$U_q(\mathfrak{sl}_2)\$ intertwiners we define. We also state applications to interacting particle processes.