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Deutsche Physikalische Gessellschaft IOP Institute of Physics

Electron wavepacket control with elliptically polarized laser light in high harmonic generation from aligned molecules

Focus on Attosecond Physics

Y Mairesse1,2,5, N Dudovich1,3, J Levesque1,4, M Yu Ivanov1, P B Corkum1 and D M Villeneuve1

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Part of Focus on Attosecond Physics

We study experimentally and theoretically the high harmonic emission from aligned samples of nitrogen and carbon dioxide, in an elliptically polarized laser field. The ellipticity induces a lateral shift of the recombining electron wavepacket in the generation process. We show that this effect, which is well known from high harmonic generation (HHG) in atoms, can be useful to maintain the plane wave approximation in the case of HHG from molecules whose orbitals contain nodal planes. The study of the harmonic signal as a function of molecular alignment also reveals the role of the ellipticity on the recollision angle of the electron wavepacket, which can be used to accurately track the position of resonances in harmonic spectra.


 

GENERAL SCIENTIFIC SUMMARY
Introduction and background. When an atom or molecule is exposed to an intense femtosecond laser pulse, the electric field of the laser is stronger than the binding potential which holds electrons to the atoms. Once it is free of the atomic potential, the electron is at the mercy of the laser field. The field pulls the electron far from the ion, then drives it back within the optical period of the laser, a few femtoseconds. Although it is improbable, the electron can recombine with the parent ion, and will give up its kinetic energy in the form of a photon in the soft x-ray portion of the spectrum. This process is called high harmonic generation, and results in a coherent beam of photons consisting of one or more attosecond-duration pulses. The recombination process is a quantum transition between a continuum state (the free electron) and the bound state, and so it contains information about the bound state wave function. It has been shown that the high harmonic spectrum from molecules which are aligned in space can be used to form an image of a single molecular orbital wave function.

Main results. The main difficulty in using high harmonic emission to measure orbital wave functions is that the orbitals of most molecules have nodal planes in which the wave function is zero. Since the continuum wave function is derived from the bound state orbital, it too will have nodes for certain molecular angles. To get around this problem, we used elliptically polarized laser light to push the continuum wave function laterally, thereby pushing the nodal plane away from the molecule.

Wider implications. Since the continuum wave function can be manipulated by the laser field, it is possible to decouple the ionization and recombination processes. This approach can be generalized to other means of modifying the laser electric field on a sub-cycle time scale. For example, the combination of a laser field with its second harmonic at an orthogonal polarization allows the recolliding electron to be directed into the side of the molecule, giving another view of the orbital wave function.

PACS

33.80.-b Photon interactions with molecules

Subjects

Atomic and molecular physics

Dates

Issue 2 (February 2008)

Received 22 September 2007

Published 29 February 2008



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