Idoeta R, Legarda F (1992) Review and calculation of Mott scat- tering cross section by unscreened point nuclei. Nucl Instrum Meth B 71:116-125Idoeta R. and Legarda F., "Review and Calculation of Mott Scattering Cross Section by Unscreened Point Nuclei" Nucl. Instrum. Methods, B71:...
The formulas required for the calculation of the Mott cross section for scattering of electrons by an unscreened nuclear charge and the GoudsmitSaunderson angular multiple-scattering distribution for electrons are summarized, and a FORTRAN-IV code which performs these calculations is given, The ...
The increase in the scattering cross section is caused by the electron scattering to the unoccupied states at colli sions with phonons (Fig. 1). The calculations of the electron–phonon interac tion in metals discussed in this paper demonstrate that relation (2) is indeed approximately met in ...
Mezei flippers were placed before the sample to allow the measurement of neutron SF and NSF scattering cross-sections. A 5-coil Helmholtz assembly was used to control the neutron spin orientation at the sample position by producing a magnetic field of the order of 10 G. The orientation of ...
3—which is substantially less than the 30 meV shift reported in the Rh-doped samples12,13), and the presence of quasiparticle peaks, which are absent in Sr2Ir1−xRhxO4, are both consistent with lower disorder scattering, in the absence of substitutional disorder directly in the IrO2 ...
distributionelectronsmott scatteringmultiple scatteringtransport electrons/transport of, evaluation of mott cross section and goudsmit--saunderson multiple-scattering distribution for, (tdoi:10.13182/NSE70-A19505FelderR. M.Nuclear Science and Engineering...
Application of a strong electric field, depicted as strong band tilt c, accelerates these carriers causing Joule heating due to scattering. In a system with defects b, a moderate electric field promotes carriers from in-gap states into the UHB d resulting in collapse of the Mott insulator ...