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Scattering Length for Atom-Diatom Scattering at Ultra-Low Energies. E.A. Kolganova (JINR Dubna). In collaboration with A.K.Motovilov (JINR Dubna) W.Sandhas (PI Bonn). Two-body, experiment. 4 He - 4 He. First observation by Luo et al (1993) and Schollkopf, Toennies (1994).
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Scattering Length for Atom-Diatom Scattering at Ultra-Low Energies E.A. Kolganova (JINR Dubna) In collaboration with A.K.Motovilov (JINR Dubna) W.Sandhas (PI Bonn)
Two-body, experiment 4He - 4He First observation by Luo et al (1993) and Schollkopf, Toennies (1994) First measurement of the bond length by Grisenti (2000) Estimation of the binding energy and scattering length
Two-body, theory 4He - 4He Potential models: Aziz et al. – HFD-B (1987), LM2M2 (1991) Tang et al. – TTY (1995) where and
Three-body, experiment and theory bound state 4He- 4He - 4He Experiment – Toennies et al. 1996 , 2002 Theory – Variational methods Pandharipande(1983), Barnett(1993), Lewerenz(1997), Nakaishi-Maeda(1983) Hyperspherical approachEsry(1996), Jensen (1998), Greene(2000) Kievsky (2001) Faddeev equations Momentum spaceGloeckle (1986) Configuration spaceCarbonell (1993), Kolganova (1997), Motovilov(2001), Roudnev (2002)
Three-body, theory scattering 4He2 - 4He Phase shifts calculations usingFaddeev differential equations Roudnev (2003) Kolganova,Motovilov(1998,2001) Zero-range model model - Hammer et al. (1999,2003), Penkov(2003)
Three-body, theory formalizm 4He2 - 4He Faddeev integro-differential equationsafter angular partial-wave analysis At L=0 the partial angular momentum corresponds both to the dimer and an additional atom. Stand to the standard Jacobi variables. Function - L.D.Faddeev,Merkuriev, 1993.
Three-body, theory formalizm 4He2 - 4He Boundary conditions Here, is the dimer w.f., stands for the scattering energy given by
Three-body, theory scattering 4He2 - 4He Phase shifts calculations usingFaddeev differential equations Blume,Greene (2000) Roudnev (2003) Penkov (2003) Braaten,Hammer (2003) 2004 2001 Motovilov,Kolganova,Sandhas
Three-body, theory scattering 4He2 - 4He Efimov-type properties of exited state
Three-body, theory scattering 4He2 - 4He Efimov-type properties of exited state