Abstract
The vector potential function for a k-mode and λ-polarization photon, with the quantized amplitude α0k(ωk) = ξωk, satisfies the classical wave propagation equation as well as the Schrodinger’s equation with the relativistic massless Hamiltonian and finally an equivalent quantum equation for the vector potential amplitude operator . Thus, behaves as a wave function for the photon within a non-local representation that can be suitably normalized. It is deduced that the probability for detecting a k-mode photon around a point on the propagation axis depends on the square of the angular frequency. Taking into account the left and right circularly polarized states and weighting by we define a six components function as a general function for a k-mode photon. The square of the modulus of the defined general function gives the energy density at a given coordinate which depends on the fourth power of the angular frequency. The amplitudes of the electric and magnetic fields of a single k-mode photon free of cavity are also calculated and it is shown that they are proportional to the square of the angular frequency. In this way, the influence of the photon electric and/or magnetic fields on the energy levels of atoms and molecules might be used for a non-destructive photon detection.
Highlights
The challenging difficulties encountered for establishing a wave function for the photon are well developed in the literature [1,2,3,4,5]
At the same time it revealed the necessity of developing a non-local representation for the photon, through a real wave function, in which new variables are not explicitly excluded
We have seen that the vector potential function with the quantized amplitude
Summary
The challenging difficulties encountered for establishing a wave function for the photon are well developed in the literature [1,2,3,4,5]. In recent years, the experimental evidence of the entangled states with single photons sources has demonstrated the permanent violation of Bell’s inequality entailing that the existence of hidden variables within a local quantum mechanical representation is excluded [6, and references therein]. At the same time it revealed the necessity of developing a non-local representation for the photon, through a real wave function, in which new variables are not explicitly excluded. We analyze the resulting expressions of the intrinsic electric and magnetic fields of a free photon opening perspectives for new experiments that might be used for a nondestructive photon detection method
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