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IEEE Lasers and Electro-Optics Society Annual Meeting (LEOS)

Super-dressed two-level atom: Very high harmonic generation and related phenomena

A. E. Kaplan, P. L. Shkolnikov

Published Dec 30, 2002• 0 citations
Publisher

Abstract

We present here a two-level model that not only reproduces experimentally observed plateau, but also allows us to evaluate its characteristics in explicit analytic form and predict new dramatic effects. Rare gases and rare-gas like ions in which high order odd harmonic generation (HHG) has been observed so far, may not be inconsistent with two-level description as far as HHG is concerned.>

DOI
10.1109/leos.1993.379035

Related papers

Super-Dressed Two-Level Atom: Very High Harmonic Generation and Multi-Resonances

A. E. Kaplan, P. L. Shkolnikov

We show that a simple nonperturbative two-level model of an atom driven by a very strong periodic field, results in a rich picture of very high harmonic generation and related phenomena. It reproduces experimentally observed plateau, yields for the first time simple analytic formulas for the plateau cutoff frequency, critical driving intensity, and saturation, and predicts intensity-induced multi-resonances. One of the most fascinating phenomenon discovered recently in nonlinear interaction of light with atoms and ions, is very high-order (up to 135) odd harmonic generation (HHG) by intense (∼ 1013 W/cm2 and higher) optical laser radiation in rare gasses and some ions [1], The spectra of generated harmonics drasticly deviate from the perturbation theory predictions [2], In particular, intensity of harmonics, falling monotonically with their orders only up to a certain point, levels off forming a so-called “plateau", and falls monotonically again beyond it. Generally, harmonte generation depends on phase-matching conditions and nonlinear response of individual atoms. It has recently become clear however [3,4] that the major features of HHG, in particular the plateau, result mainly from general properties of atomic nonlinear response. The most direct and apparently successful way so far to approach the problem theoretically has been numerical simulation of the Schrödinger [2,5-7] (including an empiric rule [6]) for many-electron atoms using Hartry-Slater approximation. This approach requires, however, tremendous amount of calculations and involves many processes, making it difficult to gain simple insights. An interesting simplified model [8] based on 3-D delta-potential with a single (ground) level [9] produces results in integration form. The idea of retaining a single energy scale (ionization energy) brings one close to an even simpler system: a two-level model atom. A two-level model of HHG [10], however, due to various complications introduced into it, failed to generate simple results, whereas an analytic solution [11] holds for a virtually degenerate two-level model only (see below) which is unapplicable to the experimental conditions [1-4,7,9]; besides, no relaxation was considered in [10,11].

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We show that a simple nonperturbative two-level model of an atom driven by a very strong periodic field results in a rich picture of very high harmonic generation and related phenomena. It reproduces the experimentally observed plateau, yields simple analytic formulas for the plateau cutoff frequency, critical driving intensity, and saturation, and predicts intensity-induced multiresonances.

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On the basis of our new theory of very-high-harmonic generation (HHG) in a superdriven two-level atom (see our paper for poster session), we have derived, for the first time to our knowledge (considering here all the existing models,1 including a numerical simulation of a two-level model driven by short pulses2), an amazingly simple analytic formula for one of the most important characteristics of the phenomenon: the size of the so-called plateau, or its cutoff frequency ωcut.

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Adiabatic theory for high-order harmonic generation in a two-level atom

Luis Plaja, L. Roso

Coherent high-order harmonic generation by an isolated two-level system is studied. A perturbative theory for the adiabatic regime is presented; the theory describes the plateau structure found experimentally in noble gases. Numerical results, without the rotating-wave approximation, are used to check the analytical predictions.

Journal of the Optical Society of America B•Dec 1, 1992•55 citations
We present here a two-level model that not only reproduces experimentally observed plateau, but also allows us to evaluate its characteristics in explicit analytic form and predict new dramatic effects. Rare gases and rare-gas like ions in which high order odd harmonic generation (HHG) has been observed so far, may not be inconsistent with two-level description as far as HHG is concerned.>
We show that a simple nonperturbative two-level model of an atom driven by a very strong periodic field, results in a rich picture of very high harmonic generation and related phenomena. It reproduces experimentally observed plateau, yields for the first time simple analytic formulas for the plateau cutoff frequency, critical driving intensity, and saturation, and predicts intensity-induced multi-resonances. One of the most fascinating phenomenon discovered recently in nonlinear interaction of light with atoms and ions, is very high-order (up to 135) odd harmonic generation (HHG) by intense (∼ 1013 W/cm2 and higher) optical laser radiation in rare gasses and some ions [1], The spectra of generated harmonics drasticly deviate from the perturbation theory predictions [2], In particular, intensity of harmonics, falling monotonically with their orders only up to a certain point, levels off forming a so-called “plateau", and falls monotonically again beyond it. Generally, harmonte generation depends on phase-matching conditions and nonlinear response of individual atoms. It has recently become clear however [3,4] that the major features of HHG, in particular the plateau, result mainly from general properties of atomic nonlinear response. The most direct and apparently successful way so far to approach the problem theoretically has been numerical simulation of the Schrödinger [2,5-7] (including an empiric rule [6]) for many-electron atoms using Hartry-Slater approximation. This approach requires, however, tremendous amount of calculations and involves many processes, making it difficult to gain simple insights. An interesting simplified model [8] based on 3-D delta-potential with a single (ground) level [9] produces results in integration form. The idea of retaining a single energy scale (ionization energy) brings one close to an even simpler system: a two-level model atom. A two-level model of HHG [10], however, due to various complications introduced into it, failed to generate simple results, whereas an analytic solution [11] holds for a virtually degenerate two-level model only (see below) which is unapplicable to the experimental conditions [1-4,7,9]; besides, no relaxation was considered in [10,11].