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The method of secondary quantization in the strong bond approximation that in the elaborated method it is not necessary to spread out nuclear charges over the crystal as it is done
The method of secondary quantization in the strong bond approximation that in the elaborated method it is not necessary to spread out nuclear charges over the crystal as it is done
Double gauge invariance and covariantly-constant vector fields in Weyl geometry by the ordinary Lienard-Wiechert field, in particular, by the Coulomb distribution for a charge at rest. Unlike
Effective connections and fields associated with shear-free null congruences, and the electric charge for bounded singularities of this field turns to be "self-quantized." Two invariant
Heating of Electrons in Pure Ge in a Quantum Magnetic Field Upon the Thermal Excitation of Charge CarriersHeating of Electrons in Pure Ge in a Quantum Magnetic Field Upon the Thermal Excitation of Charge
Heating of electrons in pure Ge in a quantum magnetic field at thermal excitation of charge carriersThe results of an experimental study on charge carriers heating by an electric field (E) in pure Ge
QUANTUM ENERGY LEVELS OF BOUND STATES OF THREE CHARGED PARTICLESQUANTUM ENERGY LEVELS OF BOUND STATES OF THREE CHARGED PARTICLES
Influence of a Quantum Magnetic Field on the Heating of Charge Carriers in Pure GermaniumAbstract: The results of an experimental study of charge-carrier heating by an electric field E
Compressing a convolution neural network based on quantization. The results showing the efficiency of quantization of the model while maintaining high accuracy are obtained.
Vacuum polarization of a quantized scalar field in the thermal state in a long throatVacuum polarization of a quantized scalar field in the thermal state in a long throat
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