By I. Ya. Barit, V. A. Sergeev (auth.), Academician D. V. Skobel’tsyn (eds.)
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Additional resources for Nuclear Physics and Interaction of Particles with Matter
Cerenkov Radiation in the Frequency Range Involving Negative Group Velocities When the group-velocity vector is directed to the side of the wave vector, the group velocity is termed positive. , a frequency range can exist in which the phase velocity of light and the velocity of energy propagation are antiparallel. away from it. The direction in which the phase of the emitted waves propagates is important in all radiation processes depending upon the absolute value of the phase velocity of light.
Popov, Report on the 16th Annual Conference on Nuclear Spectroscopy, Moscow, January 1966. 7. A. Lande and G. E. Brown, Nucl. , 75:344 (1966). 8. N. Azziz, Phys. , 23:337 (1966). 9. A. Bohr and B. Mottelson, Dan. Mat. Fys. , Vol. 27, No. 16 (1953). 10. A. M. Lane, Nuclear Structure Study with Neutrons, Proc. Intern. , Antwerpen, July 19-23, 1965. 11. A. E. Green, Proc. Intern. Conf. Nucl. Opt. , 1959. 12. M. E. Lynn, Nucl. , 17:563 (1960). 13. D. Wilkinson, Physica, 22:1039 (1956). RADIATION OF A CHARGED PARTICLE IN THE PRESENCE OF A SEPARATING BOUNDARY V.
Dissipation of electromagnetic energy means that Im E. > 0 and Im J1. > 0. In the frequency range inFig. 8 volving negative group velocities (Re E. < 0, Re J1. I. is negative. Since the square root of a complex quantity whose imaginary part is negative is equal to a complex number having real and imaginary parts with different signs, advancing potentials correspond to a solution with attenuation (for Re ik < 0 we have Re k < 0): Im n 2 < 0, Re n < 0, Im n > 0. ; expansion in the exponent of the exponential function in the integral of Eq.
Nuclear Physics and Interaction of Particles with Matter by I. Ya. Barit, V. A. Sergeev (auth.), Academician D. V. Skobel’tsyn (eds.)