Add to ORKGBoth the nonzero structure constant fkμν and the symmetric invariant tensor dkμν one calculated. We also bring out a new representation of SU(4) in terms of Pauli matrices constructed. Finally, the weight of the first fundamental representation of SU(4) is also obtained
AbstractThe structure of the tensor product representation Vλ1(x)⊗Vλ2(y) of Uq(sl̂2) is investigated...
We give a brief introduction to structure theory of Lie algebras , followed by representation theor...
physical conditions, K3 and K4 are real diagonal operators represent-ing energy, K2 = K 1, and the H...
In this master thesis I have looked on two different kinds of representations of the Lie algebras su...
The mathematical derivation of the general mass formula of SU4 is given. The derivation is preceded ...
We build an integrity basis for the SU(2) × SU(2) scalars belonging to the enveloping algebra of SU(...
It is known how to find minimal dimension matrix representations for fourdimensional complex Lie alg...
We develop graphical calculation methods. Jones-Wenzl projectors for U_q(sl(2,C)) are very ...
A representation of the exceptional Lie algebras is presented. It reflects a simple unifying view an...
We propose an algorithm for the numerical calculation of matrix elements of general U(4) group eleme...
Starting from the defining transformations of complex matrices for the SO(4) group, we construct the...
So far in this course we have given a very general theory of compact Lie groups and their representa...
We give an elementary treatment of the defining representation and Lie algebra of the three-dimensio...
First, we develop a result using multilinear algebra to prove, in an elementary way, a useful identi...
We present a new proof of the representation theorem for fourth-order isotropic tensors that does no...
AbstractThe structure of the tensor product representation Vλ1(x)⊗Vλ2(y) of Uq(sl̂2) is investigated...
We give a brief introduction to structure theory of Lie algebras , followed by representation theor...
physical conditions, K3 and K4 are real diagonal operators represent-ing energy, K2 = K 1, and the H...
In this master thesis I have looked on two different kinds of representations of the Lie algebras su...
The mathematical derivation of the general mass formula of SU4 is given. The derivation is preceded ...
We build an integrity basis for the SU(2) × SU(2) scalars belonging to the enveloping algebra of SU(...
It is known how to find minimal dimension matrix representations for fourdimensional complex Lie alg...
We develop graphical calculation methods. Jones-Wenzl projectors for U_q(sl(2,C)) are very ...
A representation of the exceptional Lie algebras is presented. It reflects a simple unifying view an...
We propose an algorithm for the numerical calculation of matrix elements of general U(4) group eleme...
Starting from the defining transformations of complex matrices for the SO(4) group, we construct the...
So far in this course we have given a very general theory of compact Lie groups and their representa...
We give an elementary treatment of the defining representation and Lie algebra of the three-dimensio...
First, we develop a result using multilinear algebra to prove, in an elementary way, a useful identi...
We present a new proof of the representation theorem for fourth-order isotropic tensors that does no...
AbstractThe structure of the tensor product representation Vλ1(x)⊗Vλ2(y) of Uq(sl̂2) is investigated...
We give a brief introduction to structure theory of Lie algebras , followed by representation theor...
physical conditions, K3 and K4 are real diagonal operators represent-ing energy, K2 = K 1, and the H...