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Physical Review A - Atomic, Molecular, and Optical Physics

Volumn 80, Issue 1, 2009, Pages

Strong-field approximation for ionization of a diatomic molecule by a strong laser field. III. High-order above-threshold ionization by an elliptically polarized field

(3) Busuladzic M a Gazibegovic Busuladzic A b Milosevic D B b,c

a UNIVERSITY OF SARAJEVO (Bosnia and Herzegovina)

b UNIVERSITY OF SARAJEVO (Bosnia and Herzegovina)

c MAX BORN INSTITUT (Germany)

Author keywords

[No Author keywords available]

Indexed keywords

DIATOMIC MOLECULES; ELLIPTICALLY POLARIZED FIELD; ELLIPTICALLY POLARIZED LASER FIELD; EMISSION ANGLE; HIGH ENERGY; HIGH-ENERGY ELECTRON; HIGH-ORDER ABOVE-THRESHOLD IONIZATION; INTERFERENCE EFFECTS; IONIZATION SPECTRUM; IONIZED ELECTRONS; LINEARLY POLARIZED FIELD; MAJOR AXIS; MOLECULAR AXIS; PEAK INTENSITY; PHOTOELECTRON SPECTRUM; PLATEAU REGION; POLARIZATION ELLIPSE; STRONG LASER FIELD; STRONG-FIELD APPROXIMATIONS; SYMMETRY PROPERTIES;

EMISSION SPECTROSCOPY; LASER PULSES; LASERS; LIGHT POLARIZATION; PHOTOELECTRON SPECTROSCOPY; PHOTOELECTRONS; PHOTOIONIZATION; PHOTONS;

MOLECULAR ORIENTATION;

EID: 68949107278 PISSN: 10502947 EISSN: 10941622 Source Type: Journal
DOI: 10.1103/PhysRevA.80.013420 Document Type: Article

Times cited : (41)

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- In fact, we fix the number of photons n exchanged with the laser field in HATI process, so that Ep =nω- Ip - Up is approximately equal to 58.5?eV?8.3 Up. Since the ionization energies Ip of N2 and O2 are different, while the laser intensity and wavelength are fixed, the number n is different for N2 and O2.
- In fact, we fix the number of photons n exchanged with the laser field in HATI process, so that Ep =nω- Ip - Up is approximately equal to 58.5?eV?8.3 Up. Since the ionization energies Ip of N2 and O2 are different, while the laser intensity and wavelength are fixed, the number n is different for N2 and O2.

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