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   <subfield code="a">10.1007/s12043-013-0637-x</subfield>
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   <subfield code="a">High harmonic generation in H2  +  and HD +  by two-colour femtosecond laser pulses</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[FARZANA SHARMIN, SAMIR SAHA, S BHATTACHARYYA]</subfield>
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   <subfield code="a">We have theoretically investigated the high harmonic generation (HHG) spectra of H2  +  and HD +  using a time-dependent wave packet approach for the nuclear motion with combined two-colour (1ω L -3ω L ) pulsed lasers for ω L corresponding to wavelengths 1064nm and 800nm. The 1ω L and 3ω L lasers have peak intensities of I 1 0 = 5.0×1013W/cm2 and I 2 0 = 2.0×1014W/cm2, respectively. We have taken the pulse duration of T = 50fs for both the fields, and the molecular initial vibrational level v 0 = 0. We have argued that for these combinations, the harmonic generation due to transitions in the electronic continuum by tunnelling or multiphoton ionization may be neglected and only the electronic transitions within the two lowest electronic states would be important. Thus, the characteristic features of HHG spectra in the two-colour field are determined, in our model, by the nuclear motions on the two lowest field-coupled electronic states between which interelectronic and intraelectronic (due to the intrinsic dipole moments in case of HD + ) radiative transitions can take place. We have studied the role of relative phase (φ) of the two fields on the HHG spectra of the molecular ions. In case of HD + , the effect of nonadiabatic (NA) nonradiative interaction between the two lowest Born-Oppenheimer (BO) electronic states (1sσ g , 2pσ u ) has been taken into account. Our calculations give realistic HHG spectra which are reasonably efficient and extended for both H2  +  and HD +  in the mixed two-colour field without involving the electronic continuum. The use of two-colour (1ω L -3ω L ) field enables us to generate high harmonics beyond that achievable with a single 1ω L or 3ω L field of the corresponding intensity, frequency and pulse time.</subfield>
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   <subfield code="a">Indian Academy of Sciences, 2013</subfield>
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   <subfield code="a">High harmonic generation</subfield>
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   <subfield code="u">Atomic and Molecular Physics Section, Department of Materials Science, Indian Association for the Cultivation of Science, Jadavpur, 700 032, Kolkata, India</subfield>
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