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Irradiation of EPDM PP blend ISpenadel, 1979

Irradiation of furoxans 34a-c

Irradiation of Glycosylimides 114.

Irradiation of PS-tBVK

Irradiation of spiro oxaziridines to cyclic lactams

Irradiation of Starch—Acrylonitrile and Starch—Vinyl Acetate Mixtures

Irradiation parameters

Irradiation temperatures and dose rates for RPV surveillance

Irradiation Time Required for 50 Decomposition of Sevin, 1-Naphthol, Baygon, Pyrolan, and Dimetilan

Irradiation-Induced Optical Absorption Bands in Alkali Azides and Proposed Defect Models

Irreducible basis sets TL,m for various spin interactions.

Irreducible Cartesian Compound Tensor Operators Resulting from a Product of Two First-Rank Tensor Operators 3 and jT

Irreducible components of the optical activity tensor for the noncentrosymmetric crystallographic point groups.

Irreducible representation matrix B0

Irreducible representations and allowed transitions in Djd symmetries.

Irreducible representations and basis fiuictions for point group Almmm.

Irreducible representations and basis functions for the symmetry point X in the BZ of the sc Bravais lattice.

Irreducible representations for R

Irreducible representations for the generators

Irreducible representations of the allowed Raman tensors in both orthorhombic

Irreducible representations of the lowest excited electronic states of 2 resulting from excitations to the lowest excited molecular orbital. Electric dipole transitions are only allowed from the ground state Ajg to Ai , respectively

Irreducible representations of the point group Oh 0 8 C, and their Cartesian tensor bases .

Irreducible representations, energies, and compositions of the FMOs of . nSTDO S calculations were performed on the corresponding DFT

Irreducible Spherical Compound Tensor Operators Resulting from a Product of Two First-Rank Tensor Operators J T and. 9.T

Irreducihle standard matrix representations of the point group Ds



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