2017
DOI: 10.1134/s106377611707024x
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Formation of correlated states and tunneling for a low energy and controlled pulsed action on particles

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Cited by 15 publications
(8 citation statements)
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“…It was shown in [3][4][5][6][7][8][9][10][11][12][13] that the simplest method of excitation of CCS for a particle is associated with a nonstationary deformation of the harmonic potential V(q,t) = Mω 2 (t)q 2 /2, in the field of which this particle is located. In a symmetric nonstationary parabolic potential well for which <q> = 0, <p> = 0, the wave function of the particle, which was in the ground state prior to the deformation, depends on the correlation coefficient and has the form…”
Section: Methods For Formation Of Coherent Correlated States In Real mentioning
confidence: 99%
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“…It was shown in [3][4][5][6][7][8][9][10][11][12][13] that the simplest method of excitation of CCS for a particle is associated with a nonstationary deformation of the harmonic potential V(q,t) = Mω 2 (t)q 2 /2, in the field of which this particle is located. In a symmetric nonstationary parabolic potential well for which <q> = 0, <p> = 0, the wave function of the particle, which was in the ground state prior to the deformation, depends on the correlation coefficient and has the form…”
Section: Methods For Formation Of Coherent Correlated States In Real mentioning
confidence: 99%
“…The mechanism of the formation of a CCS under a pulsed action on a particle [11,13] can be realized, for example, as by the shock deformation of the lattice under the action of shock waves, as under the action of a pulsed magnetic field on free charged particles A typical example of such external action is an electric discharge in a gas or liquid. The current J(t) of the discharge is accompanied by the formation of a pulsed azimuthal magnetic field ( , )…”
Section: Nuclear Physics Universal Mechanism Of Realization Of Nucleamentioning
confidence: 99%
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