0000000000597399

AUTHOR

O.n. Ulenikov

showing 11 related works from this author

On the Study of the Very High Excited Vibrational Levels of the Pyramidal Molecules

2006

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Very High Excited Vibrational Levels[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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Study of Resonance Interactions and Splittings in the PH3 Molecule : v1, v3, v2+v4 and 2v4 Bands

2002

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]PH3HRMS[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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Etude des Etats Vibrationnels Très Excités des Molécules Pyramidales Non Planes.

2006

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Etats Vibrationnels Excités[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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Analysis of high excited "hot" bands of the SO2 molecule

2011

The main goal of the present study is to analyse rotational structures of highly excited "hot" vibrational bands, v1+2v2-v2 and 2v2+v3-v2, v2+3v3-v2 and 2v1+v2+v3-v2, and v2+2v3-v2. All of these bands are located in the region of considerably stronger bands, v1 + v2 and v2 + v3, 3v3 and 2v1+v3, and 2v3, respectively . On that reason, as the first step of analysis, we made assignments of transitions belonging to these strong bands. As the result of analysis, we were able to assign three times more transitions to the bands v1 + v2 , v2 + v3, and 3v3 (3360 transitions with Jmax. = 78 and Kmax.a = 27 to the band v1 + v2, and 2380 transitions with Jmax. = 69 and Kmax.a = 24 to the band v2 + v3, …

High excited levelsHot Bands[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]SO2 molecule[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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Algebraic Hamiltonian Adapted to Strech-Bend Coupling in the Stibine Molecule.

2003

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]XY3 MoleculesVibrational SpectraLie Algebra[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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On the "expanded local mode" approach applied to the methane molecule

2011

Methane (CH4 ) is one of the main prototypical hydrocarbons and is of great importance in a variety of applications ranging from our understanding of the chemical bonding, structure and quantum dynamics, reaction kinetics to geology, astrophysics, atmospheric and environmental science. On that reason, during more than five last decades both the vibrational and ro-vibrational spectra of methane were a subject of numerous studies (see, for example, M.Hippler and M.Quack, J. Chem. Phys. 116 (2002) 6045. and H.M.Niederer, S.Albert, S.Bauerecker, V.Boudon, J.P.Champion and M.Quack, Chimia 62 (2008) 273 where extensive references to spectroscopic and theoretical works can be found, the complete, …

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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High Resolution Study of Some Doubly Excited Vibrational States of PH2D: The v1+v2, v2+v5, v2+v3 and v2+v6 Bands

2003

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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Fermi-type interaction in molecular and atomic Hamiltonians. Application to molecular systems and Bose-Einstein condensates.

2008

International audience; We present a simple prescription to build phenomenological Hamiltonians describing Fermi-type interactions and apply the developed formalism to two distinct physical systems. First, in a very simple way, we derive equations describing time dynamics of two coherently coupled Bose-Einstein condensates. Further, for bent XY2 molecules, we reproduce all the experimental data with an excellent precision.

Condensed Matter::Quantum Gases[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Fermi-type Interaction. XY2. BEC[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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On the ”Expanded” Local Mode Approach and Isotopic Effect (CH2D2/CH3D/CHD3) in the Methane Molecule

2010

Earlier derived, [1] - [3], for the XY2 (C2v and XY3 (C3v molecules) ”expanded local mode model” is applied to the methane-type, XH4, molecules. On the base of using os specially obtained value of the ambiguity parameter, sin gamma , simple value of all transformation coefficients, l_{N \alpha \lambda}, were obtained for the CH4 molecule. It gave us possibility, on the one hand, 1). to derive simple relations between different spectroscopic parameters (harmonic frequencies, anharmonic parameters and vibrational tetrahedral coefficients, rotational-vibrational and rotational tetrahedral coefficients) of the CH4 molecule, and, on the other hand, 2). on the base of the genegal isotopic substit…

[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph][ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Local ModeMethane and Isotopic Species[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]Rovibrational Spectra
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On the SPGF approach in asymmetric top molecules: application to the hydrogen sulfide.

2007

SPGF approach[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph][ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]asymmetric top molecules[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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Study of High Resolution Spectra of the PH2D Molecule in the Regions of the Deformational Vibrational Bands 2v4, v4+v6, 2v6, v3+v4, v3+v6 and 2v3

2005

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]PH2DHRMS[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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