The structure of the title complex, [Mg(H(2)O)(6)](C(10)H(15)O(4)S)(2), consists of regular octa-hedral [Mg(H(2)O)(6)](2+) cations and d-camphor-10-sulfonate anions. A three-dimensional supra-molecular architecture is formed via hydrogen-bond inter-actions [O-H⋯O = 2.723 (2)-2.833 (2) Å] to give alternating layers of [Mg(H(2)O)(6)](2+) cations and d-camphor-10-sulfonate anions. The title compou...

Gauge unification in a five dimensional supersymmetric SO(10) model compactified on an orbifold S/(Z2 × Z ′ 2) is studied. One orbifolding reduces N = 2 supersymmetry to N = 1, and the other breaks SO(10) to the Pati-Salam gauge group SU(4)C × SU(2)L × SU(2)R. Further breaking to the standard model gauge group is made through the Higgs mechanism on one of the branes. The differences of the thre...

Several numerical computations, including the Fast Fourier Transform 0, require that the data is ordered according to a bit-reversed permutation. In fact, for several standard FIT programs, this pre or post computation is claimed to take 10-50 percent of the computation time [l]. In this paper, a linear sequential bit-reversal algorithm is presented. This is an improvement by a factor of logzn ...

Superfield equations of motion for D = 10 type IIB Dirichlet super-9-brane are obtained from the generalized action principle. The geometric equations containing fermionic superembedding equations and constraints on the generalized field strength of Abelian gauge field are separated from the proper dynamical equations and are found to contain these dynamical equations among their consequences. ...

The existence of maximally supersymmetric solutions to heterotic string theory that are not toroidal compactifications of the ten-dimensional superstring is established. We construct an exact fermionic realization of an N=1 supersymmetric string theory in D=8 with non-simply-laced gauge group Sp(20). Toroidal compactification to six and four dimensions gives maximally extended supersymmetric th...