It is demonstrated that within the framework of the second quantization, the quantum Hamiltonian operator for a free transverse field reveals an alternative set of states satisfying the eigenstate functional equations. The construction is based on extensions of the quadratic form of the transverse Laplace operator, which are used as a source of spherical basis functions with singularity at the origin. This basis naturally replaces the basis of plane or spherical waves, which is used to separate variables with the help of the Fourier transform or transition to spherical coordinates.
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Translated from Zapiski Nauchnykh Seminarov POMI, Vol. 487, 2019, pp. 78–99.
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Bolokhov, T.A. Quantum Hamiltonian Eigenstates for a Free Transverse Field. J Math Sci 257, 476–490 (2021). https://doi.org/10.1007/s10958-021-05496-y
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DOI: https://doi.org/10.1007/s10958-021-05496-y