30 research outputs found

    Scaling limit of virtual states of triatomic systems

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    For a system with three identical atoms, the dependence of the ss-wave virtual state energy on the weakly bound dimer and trimer binding energies is calculated in a form of a universal scaling function. The scaling function is obtained from a renormalizable three-body model with a pairwise Dirac-delta interaction. It was also discussed the threshold condition for the appearance of the trimer virtual state.Comment: 9 pages, 3 figure

    Weakly bound atomic trimers in ultracold traps

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    The experimental three-atom recombination coefficients of the atomic states 23^{23}NaF=1,mF=1>|F=1,m_F=-1>, 87^{87}RbF=1,mF=1>|F=1,m_F=-1> and 85^{85}RbF=2,mF=2>|F=2,m_F=-2>, together with the corresponding two-body scattering lengths, allow predictions of the trimer bound state energies for such systems in a trap. The recombination parameter is given as a function of the weakly bound trimer energies, which are in the interval 1<m(a/)2E3<6.9 1<m(a/\hbar)^2 E_3< 6.9 for large positive scattering lengths, aa. The contribution of a deep-bound state to our prediction, in the case of 85^{85}RbF=2,mF=2>|F=2,m_F=-2>, for a particular trap, is shown to be relatively small.Comment: 5 pages, 1 figur

    Ultracold scattering processes in three-atomic helium systems

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    We review results on scattering observables for 4^4He--4^4He2_2 and 3^3He--4^4He2_2 collisions. We also study the effect of varying the coupling constant of the atom-atom interaction on the scattering length

    Scaling predictions for radii of weakly bound triatomic molecules

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    The mean-square radii of the molecules 4^4He3_3, 4^4He26_2-^6Li, 4^4He27_2-^7Li and 4^4He223_2-^{23}Na are calculated using a three-body model with contact interactions. They are obtained from a universal scaling function calculated within a renormalized scheme for three particles interacting through pairwise Dirac-delta interaction. The root-mean-square distance between two atoms of mass mAm_A in a triatomic molecule are estimated to be of de order of C2/[mA(E3E2)]{\cal C}\sqrt{\hbar^2/[m_A(E_3-E_2)]}, where E2E_2 is the dimer and E3E_3 the trimer binding energies, and C{\cal C} is a constant (varying from 0.6\sim 0.6 to 1\sim 1) that depends on the ratio between E2E_2 and E3E_3. Considering previous estimates for the trimer energies, we also predict the sizes of Rubidium and Sodium trimers in atomic traps.Comment: 7 pages, 2 figure

    The ^4He trimer as an Efimov system

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    We review the results obtained in the last four decades which demonstrate the Efimov nature of the 4^4He three-atomic system.Comment: Review article for a special issue of the Few-Body Systems journal devoted to Efimov physic

    Stability of the trapped nonconservative Gross-Pitaevskii equation with attractive two-body interaction

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    The dynamics of a nonconservative Gross-Pitaevskii equation for trapped atomic systems with attractive two-body interaction is numerically investigated, considering wide variations of the nonconservative parameters, related to atomic feeding and dissipation. We study the possible limitations of the mean field description for an atomic condensate with attractive two-body interaction, by defining the parameter regions where stable or unstable formation can be found. The present study is useful and timely considering the possibility of large variations of attractive two-body scattering lengths, which may be feasible in recent experiments.Comment: 6 pages, 5 figures, submitted to Physical Review

    Q2Q^2 Independence of QF2/F1QF_2/F_1, Poincare Invariance and the Non-Conservation of Helicity

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    A relativistic constituent quark model is found to reproduce the recent data regarding the ratio of proton form factors, F2(Q2)/F1(Q2)F_2(Q^2)/F_1(Q^2). We show that imposing Poincare invariance leads to substantial violation of the helicity conservation rule, as well as an analytic result that the ratio F2(Q2)/F1(Q2)1/QF_2(Q^2)/F_1(Q^2)\sim 1/Q for intermediate values of Q2Q^2.Comment: 13 pages, 7 figures, to be submitted to Phys. Rev. C typos corrected, references added, 1 new figure to show very high Q^2 behavio

    Stability of trapped Bose-Einstein condensates

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    In three-dimensional trapped Bose-Einstein condensate (BEC), described by the time-dependent Gross-Pitaevskii-Ginzburg equation, we study the effect of initial conditions on stability using a Gaussian variational approach and exact numerical simulations. We also discuss the validity of the criterion for stability suggested by Vakhitov and Kolokolov. The maximum initial chirp (initial focusing defocusing of cloud) that can lead a stable condensate to collapse even before the number of atoms reaches its critical limit is obtained for several specific cases. When we consider two- and three-body nonlinear terms, with negative cubic and positive quintic terms, we have the conditions for the existence of two phases in the condensate. In this case, the magnitude of the oscillations between the two phases are studied considering sufficient large initial chirps. The occurrence of collapse in a BEC with repulsive two-body interaction is also shown to be possible.Comment: 15 pages, 11 figure
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