A quasithermal light source [6], produced by focusing a laser beam on a rotating ground glass is used for optical transforms. Simply examinable conditions about the quality of the ground glass are given.
A quasithermal light source [6], produced by focusing a laser beam on a rotating ground glass is used for optical transforms. Simply examinable conditions about the quality of the ground glass are given.
The differential absorption and reflection coefficients of uniaxially stressed Si and SrTiO3 were determined by rotating the samples in a linearly polarized light beam.
The first direct observation of subsidiary electron bands in bismuth has been made by a study of the Shubnikov-de Haas effect in tellurium-doped crystals.
A possible explanation of the increase of the density in rotating helium II is presented.
Inequivalent representations of the Weyl relations are constructed for an infinite system of harmonic oscillators with linear interaction terms for temperature T = 0 and T ≠ 0, and a theorem on the change of factor type is indicated.
The Gross-Pitaevski equation is generalized to take into account the effects of pressure, both positive and negative, on the structure of vortices. Experiments are suggested which will help determine the density structure inside the vortex core.
The isotopic selection rules are discussed in the framework of a scheme of strong CP-violation proposed by Lee. (According to these scheme the charge conjugation operators Cst and Cγ leaving invariant strong and electromagnetic interactions, respectively, do not coincide with each other.) It is shown that in this scheme CP-noninvariant vertices describing the emission of photons by ordinary hadrons must be necessarily isotopically invariant (ΔI = 0) independent of whether the principle of minimal electromagnetic interaction is applicable to so called a-particles and whether these particles are isottopic singlets.
The representation matrices of finite U3 transformations are explicitly determined.
The polarization of neutrons from the reaction 2H(d,n)3He, at a reaction angle of 46.5° and a deuteron energy of 350 keV, has been determined as (−13.8 ± 1.4)% (phase shifts of Austin et al.).

