Search arXiv⌕ Search

arXiv · physics/0012049

Cooling gases with Levy flights: using the generalized central limit theorem in physics

Abstract

In the last ten years, the generalized central limit theorem established by Paul Levy in the thirties has been found more and more relevant in physics. Physicists call 'Levy flights' random walks for which the probability density of the jump lenghts $x$ decays as $1/x^{1+α}$ with $α<2$ for large $x$. We give here a glimpse of Levy flights in physics through two examples, without going into technical details. We first introduce a simple toy model, the Arrhenius cascade. We then present an important physical process, subrecoil laser cooling of atomic gases, in which Levy flights play an essential role.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

F. Bardou. 2000-12-20. Cooling gases with Levy flights: using the generalized central limit theorem in physics. https://arxiv.org/abs/physics/0012049

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Energies and lifetimes of the 9p and 10p excited states in atomic francium

We present the first measurement of 9p 2P1/2,3/2 and 10p 2P1/2,3/2 excited levels absolute wavenumbers and radiative lifetime in francium. We used the Collinear Resonance Ionization Spectroscopy (CRIS) technique, applied on a beam of 221Fr atoms. Prior to this work, no experimental data existed for francium p-states with n > 8. The results provide a precision experimental test of relativistic coupled-cluster theory for the heaviest alkali, showing good agreement for lifetimes and relative excitation energies, despite a residual global offset in absolute energies.

physics.atom-ph↗

Switching off a high-harmonic polarization channel by anti-unitary symmetry

We study polarization-resolved high-harmonic generation in a laser-driven two-leg Su--Schrieffer--Heeger ladder with asymmetric dimerization under periodic boundary conditions. A field linearly polarized along the ladder can generate both longitudinal and transverse radiation, whose harmonic content is controlled by lattice symmetry and electronic filling. Using symmetry analysis of the time-dependent density matrix, we show that reflection symmetry enforces odd-order harmonics in the longitudinal response and, when the transverse response is nonzero, even-order harmonics in the transverse direction. At half filling, an additional anti-unitary symmetry relating the occupied and empty bands suppresses the transverse current completely. A unitary chiral symmetry in the clean ladder relates the same bands but fails to enforce this cancellation, showing that band swapping alone is insufficient: the suppression requires both a density-matrix constraint that persists during the driven evolution and the appropriate transformation of the transverse-current operator. Moving away from half filling lifts this cancellation and allows transverse emission, while the reflection selection rule remains whenever reflection symmetry is preserved. Numerical calculations at quarter and half filling, combined with onsite potentials that selectively break the relevant symmetries, confirm these two distinct mechanisms. Thus, reflection symmetry determines which harmonic orders occur, whereas the interplay of anti-unitary symmetry and filling controls whether the transverse HHG channel is present at all.

physics.atom-ph↗

Bringing Dark States to Light after Frustrated Tunneling Ionization

High-harmonic generation (HHG) in gases is typically regarded as a sub-laser-cycle process, well described by the semiclassical three-step model. In this work, we report the extreme-ultraviolet (XUV) emission observed in an HHG experiment arising from a longer temporal process associated with dark states populated through frustrated tunneling ionization. The emission exhibits a larger spatial divergence than typical high-order harmonics, resembling the polarization decay of optically bright states. Supported by the time-frequency analysis of the theoretical calculations, we show that the emission originates from the nonradiative capture of the tunneling electrons into excited dark states of the neutral atom, followed by Floquet-like laser-dressing effects induced by the extended tail of the driving pulse. Our results reveal a largely unexplored pathway for XUV generation through laser-dressed dark states, thereby enabling the enhancement of coherent XUV emission at targeted wavelengths with high repetition rates.

physics.atom-ph↗