Спектроскопические модели для лазерного синтеза и контроля ультрахолодных ансамблей димеров щелочных металлов (1097879), страница 31
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and Softley T.P. Ultracold molecules and ultracold chemistry // Mol.Phys. - 2009. - V.107. - N2. - P.99-1323.[8] Ospelkaus S., Ni K., Wang D., De Miranda M. H. G., Neyenhuis B., Quéméner G.,Julienne P. S., Bohn J. L., Jin D. S., Ye J. Quantum-State Controlled ChemicalReactions of Ultracold Potassium-Rubidium Molecules // Science. - 2010. - V.327. P.853-857.[9] Danzl G. R., Haller E., Gustavsson M., Mark M.
J., Hart R., Bouloufa N., Dulieu O.,Ritsch H.T., and Nagerl H.C. Quantum gas of deeply bound ground state molecules// Science. - 2008. - V.321. - P.1062-1066.[10] Ni K.-K., Ospelkaus S., de Miranda M. H. G., Peer A., Neyenhuis B., Zirbel J. J.,Kotochigova S., Julienne P. S., Jin D. S., and Ye J. A high phase-space-density gas ofpolar molecules // Science. - 2008. - V.322. - P.231-235.[11] Ni K.-K., Ospelkaus S., Wang D., Quéméner G., Neyenhuis B., de Miranda M.
H. G.,Bohn J. L., Ye J., Jin D. S. Dipolar collisions of polar molecules in the quantum regime// Nature -2010. - V.464. - P.1324–1328[12] Abrahamsson E., Tscherbul T. V., and Krems R. V. Inelastic collisions of cold polarmolecules in nonparallel electric and magnetic fields // J. Chem. Phys. - 2007. - V.127.- P.044302-10214[13] Cheng Chin, Flambaum V. V., and Kozlov M. G.
Ultracold molecules: new probes onthe variation of fundamental constants // New Journal of Physics - 2009. - V.11. P.055048-14.[14] Bergmann K., Theuer H., and Shore B. W. Coherent population transfer amongquantum states of atoms and molecules // Reviews of Modern Physics. - 1998. - V.70.- N3. - P.1003-1025.[15] Koch C. P., Luc-Koenig E., and Masnou-Seeuws F.
Making ultracold molecules in atwo-color pump-dump photoassociation scheme using chirped pulses // Phys. Rev. A.- 2006. - V.73. - P.033408-13.[16] Stwalley W.C., Wang He Ultra photoassociative spectroscopy of heteronuclear alkalimetal diatomic molecules // J. Chem. Phys. - 1998.
- V.108. - N14. - P.5767-5771.[17] Sage J.M., Sainis S., Bergeman T., and DeMille D. Optical production of ultracoldpolar molecules // Phys. Rev. Lett. - 2005. - V.94. - P.203001-203004.[18] Deiglmayr J., Grochola A., Repp M., Mörtlbauer K., Glück C., Lange J., DulieuO., Wester R., and Weidemüller M. Formation of ultracold polar molecules in therovibrational ground state // Phys.
Rev. Lett. - 2008. - V.101. - P.133004-133007.[19] DeMille D. Quantum computation with trapped polar molecules // Phys. Rev. Lett.- 2002. - V.88. - P.067901-067904.[20] Micheli A., Brennen G. K., Zoller P. A toolbox for lattice-spin models with polarmolecules // Nature Physics. - 2006.- V.2. - P.341-347.[21] Levy T., Cohen G., Rabani E. Simulating Lattice Spin Models on Graphics ProcessingUnits // J. Chem. Theory Comput. - 2010. - V.6. - P.3293–3301.[22] Vexiau R., Bouloufa N., Aymar M., Danzl J.
G., Mark M.J., Nagerl H.C., and DulieuO. Optimal trapping wavelengths of Cs2 molecules in an optical lattice // Eur. Phys.J. D. - 2011. - V.65. - P.243–250.[23] Bahns J.T., Stwalley W.C., and Gould P.L. Laser cooling of molecules: a sequentialscheme for rotation, translation, and vibration // J. Chem. Phys. - 1996. - V.104. N24.
- P.9689-9697.[24] Viteau M., Chotia A., Allegrini M., Bouloufa N., Dulieu O., Comparat D., and PilletP. Optical pumping and vibrational cooling of molecules // Science. - 2008. - V.321.- P.232-234.[25] Wang H., Gould P.L., and Stwalley W.C. Photoassociative spectroscopy of pure longrange molecules // Z. Phys. D. - 1996. - V.36. - P.317-323.215[26] Kerman A.J., Sage J.M., Sainis S., Bergeman T., and DeMille D.
Production ofultracold, polar RbCs molecules via photoassociation // Phys. Rev. Lett. - 2004. V.92. - P.033004-033007.[27] Stwalley W.C. Efficient conversion of ultracold Feshbach-resonance-related polarmolecules into ultracold ground state X 1 Σ+ (v = 0; J = 0) molecules // Eur. Phys. J.D - 2004. - V.31. - P.
221-225.[28] Pilch K., Lange A. D., Prantner A., Kerner G., Ferlaino F., Nägerl H.-C., and GrimmR. Observation of interspecies Feshbach resonances in an ultracold Rb-Cs mixture //Phys. Rev. A. - 2009. - V.79. - P.042718-7.[29] Takekoshi T., Debatin M., Rameshan R., Ferlaino F., Grimm R., Nägerl H. -C., LeSueur C. R., Hutson J. M., Julienne P. S., Kotochigova S., Tiemann E. Towards theproduction of ultracold ground-state RbCs molecules: Feshbach resonances, weaklybound states, and the coupled-channel model // Phys. Rev. A. - 2012. - V.85. P.032506-14.[30] Pellegrini P., Gacesa M., and Côté R.
Giant formation rates of ultracold molecules viaFeshbach-optimized photoassociation // Phys. Rev. Lett. - 2008. - V.101. - P.053201-4.[31] Junker M., Dries D., Welford C., Hitchcock J., Chen Y. P., and Hulet R. G.Photoassociation of a Bose-Einstein condensate near a Feshbach resonance // Phys.Rev. Lett.
- 2008. - V.101. - P.060406-4.[32] Debatin M., Takekoshi T., Rameshan R., Reichs¨öllner L., Ferlaino F., Grimm R.,Vexiau R., Bouloufa N., Dulieu O., Nägerl H. -C. Molecular spectroscopy for groundstate transfer of ultracold RbCs molecules // Phys. Chem.
Chem. Phys. - 2011. - V.13.- P.18926-18935[33] Bergeman T., Kerman A. J., Sage J., Sainis S., DeMille D. Prospects for productionof ultracold X1 Σ+ RbCs molecules // Eur. Phys. J. D. - 2004.- V.31 - P.179-188.[34] Ghosal S., Doyle R. J., Koch C. P., and Hutson J. M. Stimulating the productionof deeply bound RbCs molecules with laser pulses: the role of spin–orbit coupling informing ultracold molecules // New Journal of Physics - 2009. - V.11.
- P.055011-26.[35] Kuznetsova E., Gacesa M., Pellegrini P., Yelin S. F., and Côté R. Efficient formationof ground-state ultracold molecules via STIRAP from the continuum at a Feshbachresonance // New Journal of Physics - 2009. - V.11. - P.055028-18.[36] Kim J.T., Lee Y., Kim B., Wang D., Stwalley W.C., Gould P.L., and Eyler E.E.
Spectroscopic prescription for optimal stimulated Raman transfer of ultracoldheteronuclear molecules to the lowest rovibronic level // Phys. Rev. A. - 2011. V.84. - P.062511-7.216[37] Pazyuk E.A., Stolyarov A.V., Tamanis M.Ya., and Ferber R.S. Global deperturbationanalysis from energetic, magnetic and radiative measurements: application to Te2 //J. Chem. Phys. - 1993. - V.99. - N10. - P.7873-7887.[38] Jarmola A., Tamanis M., Ferber R., Pazyuk E.A., Stolyarov A.V. LIF intensitydistribution as a deperturbation tool: application to the fully-mixed A1 Σ+ ∼ b3 Πcomplex of NaRb // J. Quant.
Spectr. Rad. Transfer - 2005. - V.95. - N2. - P.165-174.3[39] Xie X., Field R. W. The 6 Li2 A1 Σ+u ∼ b Πu spin-orbit perturbations: sub-Dopplerspectra and steady state kinetic lineshape model // Chem. Phys. - 1985. - V.99. - N.2.- P.337-345.[40] Xie X., Field R. W. Perturbation Facilitated Optical-Optical Double Resonance3333 +spectroscopy of the 6 Li2 33 Σ+g , 2 Πg , 1 ∆g , b Πu , and a Σu states // J.
Mol. Spectrosc.- 1986. - V.117. - N.2.- P.228-244.[41] Linton C., Martin F., Russier I., Ross A. J., Crozet P., Churassy S., Bacis R.6Observation and Analysis of the A1 Σ+u State of Li2 from v = 0 to the DissociationLimit // J. Mol. Spectrosc. - 1996. - V.175.- N.2. - P.340-353.[42] Urbanski K., Antonova S., Lyyra A. M., Yiannopoulous A., Stwalley W.C. All optical7triple resonance spectroscopy of the A1 Σ+u state of Li2 // Chem. Phys. - 1996. - V.104.- N.8. - P.2813-2817.[43] Li L., Lyyra A. M. Triplet states of Na2 and Li2 by perturbation facilitatedoptical–optical double resonance spectroscopy // Spectrochim. Acta A.
- 1999. - V.55.- P.2147–2178.[44] Atkinson J. B., Becker J., Demtröder W. Experimental observation of the a3 Πu stateof Na2 // Chem. Phys. Lett. - 1982. - V.87. - N.1. - P.92–97.[45] Effantin C., Babaky O., Hussein K., d’Incan J., Barrow R. F. Interactions between3A1 Σ+u and b Πu states of Na2 // J. Phys. B. - 1985. - V.18. - N.20.
- P.4077-4087.3[46] Katô H., Otani M., Baba M. Perturbations of the A1 Σ+u and b Πu states of Na2 andthe effects on the transition intensity and the line splitting // J. Chem. Phys. - 1988.- V.89.- N.2. - P.653-659.[47] Whang T. -J. , Stwalley W. C., Li L., Lyyra A. M. Perturbation facilitated all opticaltriple resonance spectroscopy of the Na2 b3 Πu state // J. Chem. Phys.
- 1992. - V.97.N.10. - P.7211-7219.[48] Qi P., Bai J., Ahmed E., Lyyra A. M., Kotochigova S., Ross A. J., Effantin C., ZalickiP., Vigué J., Chawla G., Field R. W., Whang T. -J., Stwalley W. C., Knöckel H.,Tiemann E., Shang J., Li L., Bergeman T. New spectroscopic data, spin-orbit functions,2173and global analysis of data on the A1 Σ+u and b Πu states of Na2 // J. Chem. Phys. 2007. - V.127. - P.044301-17[49] Sun H., Huennekens J. Spin–orbit perturbations between the A(2)1 Σ+ and b(1)3 Π0states of NaK // J.
Chem. Phys. - 1992. - V.97. - N7. - P.4714 -4722.[50] Ross A.J. , Crozet P., Effantin C., d’Incan J., Barrow R. F. Interactions between the3A(1)1 Σ+u and b(1) Πu states of K2 // J. Phys. B. - 1987. - V.20. - N.23. - P.6225-6231.[51] Jong G., Li L., Whang T.
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