Vector-coupling coefficients for space groups based on simple cubic lattices (1980)
Clebsch-Gordan coefficients are calculated for the irreducible representations X x X and M x M of space groups of perovskites and cuprite.
Vector-coupling coefficients for space groups based on simple cubic lattices (1980)
Clebsch-Gordan coefficients are calculated for the irreducible representations X x X and M x M of space groups of perovskites and cuprite.
Vector-coupling coefficients for space groups based on simple cubic lattices (1980)
Clebsch-Gordan coefficients are calculated for the irreducible representations X x X and M x M of space groups of perovskites and cuprite.
Clebsch-Gordan coefficients for M x M in beta tungsten (1979)
The Clebsch-Gordan coefficients are calculated for M x M irreducible representations in the beta tungsten structure.
Clebsch-Gordan coefficients for M x M in beta tungsten (1979)
The Clebsch-Gordan coefficients are calculated for M x M irreducible representations in the beta tungsten structure.
Clebsch-Gordan coefficients for M x M in beta tungsten (1979)
The Clebsch-Gordan coefficients are calculated for M x M irreducible representations in the beta tungsten structure.
Clebsch-Gordan coefficients for X x X and R x R in beta tungsten (1978)
The Clebsch-Gordan coefficients are calculated for irreducible representations X x X and R x R in beta tungsten structure.
Selection rules for the double space group O1h (1978)
Kunert, H., Popenda, J., Suffczynski, M.
The octahedral symmorphic space group O1h is the symmetry group of the simple cubic. the caesium chloride, the perovskites and the rhenium trioxide structures. The direct products of irreducible...
Clebsch-Gordan coefficients for X x X and R x R in beta tungsten (1978)
The Clebsch-Gordan coefficients are calculated for irreducible representations X x X and R x R in beta tungsten structure.
Selection rules for the double space group O1h (1978)
Kunert, H., Popenda, J., Suffczynski, M.
The octahedral symmorphic space group O1h is the symmetry group of the simple cubic. the caesium chloride, the perovskites and the rhenium trioxide structures. The direct products of irreducible...
Clebsch-Gordan coefficients for X x X and R x R in beta tungsten (1978)
The Clebsch-Gordan coefficients are calculated for irreducible representations X x X and R x R in beta tungsten structure.
Selection rules for the double space group O1h (1978)
Kunert, H., Popenda, J., Suffczynski, M.
The octahedral symmorphic space group O1h is the symmetry group of the simple cubic. the caesium chloride, the perovskites and the rhenium trioxide structures. The direct products of irreducible...
Selection rules for the double space group of the beta-Wolfram structure (1977)
The direct products of irreducible representations of the double space group of the beta-wolfram structure are reduced for the four points of highest symmetry of the Brillouin zone.
Selection rules for the double space group of the beta-Wolfram structure (1977)
The direct products of irreducible representations of the double space group of the beta-wolfram structure are reduced for the four points of highest symmetry of the Brillouin zone.
Selection rules for the double space group of the beta-Wolfram structure (1977)
The direct products of irreducible representations of the double space group of the beta-wolfram structure are reduced for the four points of highest symmetry of the Brillouin zone.
Selection rules for the space group of cuprite, the symmetry points and lines (1976)
Olbrychski, K., Kolodziejski, R., Kunert, H.
The paper presents selection rules for the double space group O4 h of cuprite, i.e. decompositions of direct products of the irreducible representations in which one factor refers to a high symmetry...
Selection rules for the space group of cuprite, the symmetry points and lines (1976)
Olbrychski, K., Kolodziejski, R., Kunert, H.
The paper presents selection rules for the double space group O4 h of cuprite, i.e. decompositions of direct products of the irreducible representations in which one factor refers to a high symmetry...
Selection rules for the space group of cuprite, the symmetry points and lines (1976)
Olbrychski, K., Kolodziejski, R., Kunert, H.
The paper presents selection rules for the double space group O4 h of cuprite, i.e. decompositions of direct products of the irreducible representations in which one factor refers to a high symmetry...
Selection rules for the space group of Cu2O, at four symmetry points of the Brillouin zone (1975)
The direct products Dkp × Dmq of irreducible représentations of the double space group O4 h of Cu2O are reduced. The wave vectors k, m run over the four highest symmetry points of the Brillouin...
Selection rules for the space group of Cu2O, at four symmetry points of the Brillouin zone (1975)
The direct products Dkp × Dmq of irreducible représentations of the double space group O4 h of Cu2O are reduced. The wave vectors k, m run over the four highest symmetry points of the Brillouin...
Selection rules for the space group of Cu2O, at four symmetry points of the Brillouin zone (1975)
The direct products Dkp × Dmq of irreducible représentations of the double space group O4 h of Cu2O are reduced. The wave vectors k, m run over the four highest symmetry points of the Brillouin...
Impaired cognitive performance in drug free users of recreational ecstasy (MDMA)
Gouzoulis-Mayfran..., E., Daumann, J., Tuchtenhagen, F., Pelz, S., Becker, S., Kunert, H., ...
OBJECTIVES—Ecstasy (3,4-methylenedioxymethamphetamine (MDMA) and related congerers: MDA, MDEA) is the name given to a group of popular recreational drugs. Animal data raise concern about neurotoxic...