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Optical and Quantum Electronics

Azimuthal quantum number dependent two dimensional atom microscopy, via atom cavity coupling

Maha M. A. Lashin, Meraj Ali Khan, Sayed M. Eldin, Aizaz Khan, Zeeshan Ahmad, Sayed Saifullah

Published Sep 10, 2023• 2 citations
Publisher
DOI
10.1007/s11082-023-05231-8

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We present a comprehensive theoretical investigation of two-dimensional (2D) Compton-azimuthal atomic localization in a three-level atomic system interacting with spatially structured light fields. The study focuses on how the azimuthal quantum numbers of the applied standing-wave fields influence the spatial probability distribution of an atom within the 2D plane. By numerically solving the governing equations of motion with realistic atomic parameters, we obtain localization maps that reveal sharp and well-defined probability peaks. The spatial localization arises from the position-dependent Rabi frequencies, which are modulated by the standing-wave interference patterns and the orbital angular momentum carried by the fields. Our results demonstrate a clear transition from multiple sharp localization peaks to a single dominant peak as ℓ1 and ℓ2 are reduced. This peak reduction significantly increases the probability of finding the atom at the remaining high-probability sites, reaching 100% localization probability in the single-peak regime. Physically, this occurs because lower azimuthal mode numbers simplify the spatial interference structure, concentrating the atomic wavefunction in a narrower spatial region. The tunability of localization via ℓ1 and ℓ2 provides a flexible control mechanism for atomic position measurement with subwavelength precision. The findings not only offer new insights into Compton-azimuthal localization mechanisms but also open potential applications in quantum metrology, atom-based nanolithography, and precision quantum control of matter–light interactions in structured optical fields.
We discuss the power dependence of distributed cavity phase errors for cylindrical TE011cavities in laser-cooled atomic fountain clocks. The azimuthally symmetric phase variations produce a surprisingly large distributed cavity phase error for two 2pi, 4pi, and 6pi pulses. This is due to the correlation between the transverse variation of the Rabi frequency over the cavity aperture and a quadratic density variation of the atomic sample, along with the symmetry of the longitudinal phase variation in the cavity. We show that the large azimuthally symmetric fields and phase shifts near the walls of the endcap holes produce very small errors at optimal power for a uniform wall resistance. We also show the power variation for higher order azimuthal variations m=1, 2, and 4. These may be caused by fountain tilts, nonuniform detection of atoms, and asymmetries in the laser trapping and cooling of the atoms. We demonstrate that distributed cavity phase errors in physical cavities may have no variation with the microwave power. A combination of rigorous calculations of cavity losses, measurements of power dependence, the atomic distributions, and fountain tilts, and electrical measurements that show the lower limit of the cavity Q and the cavity symmetry, should provide stringent limits on distributed cavity phase errors for current atomic clocks
As is known, the hydrogen atom energy levels depend on the principal quantum number n only and are independent of the azimuthal quantum number l. One can say (by using the common but not very suitable term) that there is degeneracy (i.e., the multiplicity of the level) with respect to the azimuthal quantum number. On the other hand, there is a general rule according to which the multiplicity of the Schro¨dinger equation eigenvalues relates to the invariance of the equation under a definite group of transformations. So, for example, the invariance under a common rotation group (spherical symmetry) leads to the energy level independence on the magnetic quantum number m. Therefore, it should be expected that the energy level independence of the azimuthal quantum number is explained by the existence of a certain transformation group that is more general than the three-dimensional rotation group. Up to now, this group of transformations for the Schro¨dinger equation has not been found. In the present work, we shall show that this group is equivalent to the rotation group in the four-dimensional Euclidean space.