1,304 research outputs found

    Quantum depletion of collapsing Bose-Einstein condensates

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    We perform the first numerical three-dimensional studies of quantum field effects in the Bosenova experiment on collapsing condensates by E. Donley et al. [Nature 415, 39 (2002)] using the exact experimental geometry. In a stochastic truncated Wigner simulation of the collapse, the collapse times are larger than the experimentally measured values. We find that a finite temperature initial state leads to an increased creation rate of uncondensed atoms, but not to a reduction of the collapse time. A comparison of the time-dependent Hartree-Fock-Bogoliubov and Wigner methods for the more tractable spherical trap shows excellent agreement between the uncondensed populations. We conclude that the discrepancy between the experimental and theoretical values of the collapse time cannot be explained by Gaussian quantum fluctuations or finite temperature effects.Comment: 9 pages, 4 figures, replaced with published versio

    Quantum-field dynamics of expanding and contracting Bose-Einstein condensates

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    We analyze the dynamics of quantum statistics in a harmonically trapped Bose-Einstein condensate, whose two-body interaction strength is controlled via a Feshbach resonance. From an initially non-interacting coherent state, the quantum field undergoes Kerr squeezing, which can be qualitatively described with a single mode model. To render the effect experimentally accessible, we propose a homodyne scheme, based on two hyperfine components, which converts the quadrature squeezing into number squeezing. The scheme is numerically demonstrated using a two-component Hartree-Fock-Bogoliubov formalism.Comment: 9 pages, 4 figure

    Cannabinoid receptors expression in bone marrow trephine biopsy of chronic lymphocytic leukaemia patients treated with purine analogues

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    Background: Cannabinoid receptors CB1 and CB2 are part the endocannabinoid system that plays an important role in the process of proliferation and apoptosis of different neoplastic cells. B-cell chronic lymphocytic leukaemia is one of the diseases in which these processes are altered. Aim: The aim of our study was the assessment of cannabinoid receptor expression on the B-lymphocytes in bone marrow trephine biopsy from leukaemic patients at diagnosis and after purine analogue treatment. Methods: The biopsy was taken routinely and standard immunohistochemical staining procedure for paraffin embedded sections was applied. The cannabinoid receptors were detected using specific primary polyclonal antibody anti-CB1 and anti-CB2. Additionally, an existence of cannabinoid receptors was confirmed by flow cytometry. Results: The results showed that the expression of CB1 receptor on the surface of neoplastic cells was lower than that of CB2 (17.0 Β± 3.1% and 92.1 Β± 1.7% respectively, p < 0.001). Nine of the patients responded to applied treatment with a reduction in leukaemic infiltration (77.2 Β± 6.9% to 30.2 Β± 6.5%, p = 0.007) and CB1 receptor expression (24.4 Β± 4.8% to 8.6 Β± 2.9%, p = 0.01), but there was no change in CB2 expression (91.7 Β± 2.7% vs 90.9 Β± 2.8%, p = 0.69). Four patients without remission expressed even greater number of the receptors. In all of the cases both cannabinoid receptor types antibodies gave positive reaction. Furthermore, the existence of cannabinoid receptors on neoplastic lymphocytes was confirmed by flow cytometry. Conclusion: The study provides original evidence for the existence of cannabinoid receptors on B-lymphocytes in chronic lymphocytic leukaemia patients. The receptors are thought to be a new structure that can modify the course of the disease and may be considered as a new target in leukaemia treatment.ОбоснованиС: Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Ρ‹ ΠΊΠ°Π½Π½Π°Π±ΠΈΠ½ΠΎΠΈΠ΄ΠΎΠ² CB1 ΠΈ CB2 яв Π»ΡΡŽΡ‚ΡΡ Ρ‡Π°ΡΡ‚ΡŒΡŽ систСмы эндоканнабиноидов, которая ΠΈΠ³Ρ€Π°Π΅Ρ‚ Π²Π°ΠΆΠ½ΡƒΡŽ Ρ€ΠΎΠ»ΡŒ Π² процСссах ΠΏΡ€ΠΎΠ»ΠΈΡ„Π΅Ρ€Π°Ρ†ΠΈΠΈ ΠΈ Π°ΠΏΠΎΠΏΡ‚ΠΎΠ·Π° Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… нСопластичСских ΠΊΠ»Π΅Ρ‚ΠΎΠΊ. Одним ΠΈΠ· Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ, ΠΏΡ€ΠΈ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… происходит Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΠ΅ этих процСссов, являСтся Π’-ΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½Ρ‹ΠΉ хроничСский Π»ΠΈΠΌΡ„Π»Π΅ΠΉΠΊΠΎΠ·. ЦСль: ΠΎΡ†Π΅Π½ΠΊΠ° экспрСссии Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€ΠΎΠ² ΠΊΠ°Π½Π½Π°Π±ΠΈΠ½ΠΎΠΈΠ΄ΠΎΠ² Π½Π° Π’-Π»ΠΈΠΌΡ„ΠΎΡ†ΠΈΡ‚Π°Ρ… Π² Ρ‚Ρ€Π΅ΠΏΠ°Π½ΠΎΠ±ΠΈΠΎΠΏΡ‚Π°Ρ‚Π°Ρ… Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… Π»Π΅ΠΉΠΊΠΎΠ·ΠΎΠΌ Π΄ΠΎ ΠΈ послС провСдСния лСчСния с использованиСм ΠΏΡƒΡ€ΠΈΠ½ΠΎΠ²Ρ‹Ρ… Π°Π½Π°Π»ΠΎΠ³ΠΎΠ². ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: Π±ΠΈΠΎΠΏΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠ»ΡƒΡ‡ΠΈΠ»ΠΈ Ρ€ΡƒΡ‚ΠΈΠ½Π½Ρ‹ΠΌΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ; иммуногистохимичСскоС исслСдованиС Π΄Π΅ΠΏΠ°Ρ€Π°Ρ„ΠΈΠ½ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… срСзов ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΏΠΎ стандартной ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€Π΅. Π Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Ρ‹ ΠΊΠ°Π½Π½Π°Π±ΠΈΠ½ΠΎΠΈΠ΄ΠΎΠ² опрСдСляли с использованиСм спСцифичСских ΠΌΠΎΠ½ΠΎΠΊΠ»ΠΎΠ½Π°Π»ΡŒΠ½Ρ‹Ρ… Π°Π½Ρ‚ΠΈΡ‚Π΅Π» Π°Π½Ρ‚ΠΈ-CB1 ΠΈ Π°Π½Ρ‚ΠΈ-CB2. ΠšΡ€ΠΎΠΌΠ΅ Ρ‚ΠΎΠ³ΠΎ, Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€ΠΎΠ² ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½ΠΎ ΠΏΡ€ΠΈ ΠΏΠΎ- ΠΌΠΎΡ‰ΠΈ ΠΏΡ€ΠΎΡ‚ΠΎΡ‡Π½ΠΎΠΉ Ρ†ΠΈΡ‚ΠΎΡ„Π»ΡƒΠΎΡ€ΠΈΠΌΠ΅Ρ‚Ρ€ΠΈΠΈ. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ экспрСссия Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Π° CB1 Π½Π° повСрхности ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ Π½ΠΈΠΆΠ΅, Ρ‡Π΅ΠΌ экспрСссия CB2 (17,0Β  Β± 3,1% ΠΈ 92,1 1,7% Ρ‚Π²Π΅Π½Π½ΠΎ, p < 0,001). ПослС ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠ³ΠΎ лСчСния Ρƒ 9 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΎΡΡŒ ΡƒΠΌΠ΅Π½ΡŒΡˆΠ΅Π½ΠΈΠ΅ Π»Π΅ΠΉΠΊΠΎΠ·Π½ΠΎΠ³ΠΎ ΠΈΠ½Ρ„ΠΈΠ»ΡŒΡ‚Ρ€Π°Ρ‚Π° (77,2 6,9% Π΄ΠΎ 30,2 6,5%, p = 0,007) ΠΈ сниТСниС экспрСссии Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Π° CB1 (24,4 4,8% Π΄ΠΎ 8,6 2,9%, p = 0,01), ΠΎΠ΄Π½Π°ΠΊΠΎ Ρ€Π°Π·Π»ΠΈΡ‡ΠΈΠΉ Π² экспрСссии CB2 Π½Π΅ ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΈ (91,7 2,7% ΠΏΡ€ΠΎΡ‚ΠΈΠ² 90,9 2,8%, p = 0,69). Π£ 4 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ², Ρƒ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π½Π΅ ΡƒΠ΄Π°Π»ΠΎΡΡŒ Π΄ΠΎΡΡ‚ΠΈΡ‡ΡŒ рСмиссии, опрСдСляли Π΄Π°ΠΆΠ΅ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΠ΅ экспрСссии Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€ΠΎΠ². Π’ΠΎ всСх случаях ΠΌΠ°Ρ€ΠΊΠΈΡ€ΠΎΠ²ΠΊΠΈ Π°Π½Ρ‚ΠΈΡ‚Π΅Π»Π°ΠΌΠΈ ΠΊ ΠΎΠ±ΠΎΠΈΠΌ Ρ‚ΠΈΠΏΠ°ΠΌ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€ΠΎΠ² ΠΊΠ°Π½Π½Π°Π±ΠΈΠ½ΠΎΠΈΠ΄ΠΎΠ² ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΈ ΠΏΠΎΠ»ΠΎ- ΠΆΠΈΡ‚Π΅Π»ΡŒΠ½ΡƒΡŽ Ρ€Π΅Π°ΠΊΡ†ΠΈΡŽ. Π‘ΠΎΠ»Π΅Π΅ Ρ‚ΠΎΠ³ΠΎ, присутствиС Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€ΠΎΠ² ΠΊΠ°Π½Π½Π°Π±ΠΈΠ½ΠΎΠΈΠ΄ΠΎΠ² Π½Π° злокачСствСнных ΠΊΠ»Π΅Ρ‚ΠΊΠ°Ρ… ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π°Π»ΠΈ ΠΏΡ€ΠΈ ΠΏΠΎΠΌΠΎΡ‰ΠΈ ΠΏΡ€ΠΎΡ‚ΠΎΡ‡Π½ΠΎΠΉ Ρ†ΠΈΡ‚ΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΠΈ. Π’Ρ‹Π²ΠΎΠ΄Ρ‹: Π² Ρ…ΠΎΠ΄Π΅ исслСдования ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ ΠΈΠ·Π½Π°Ρ‡Π°Π»ΡŒΠ½ΠΎΠ΅ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€ΠΎΠ² ΠΊΠ°Π½Π½Π°Π±ΠΈΠ½ΠΎΠΈΠ΄ΠΎΠ² Π½Π° Π’-Π»ΠΈΠΌΡ„ΠΎΡ†ΠΈΡ‚Π°Ρ… Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… хроничСским Π»ΠΈΠΌΡ„ΠΎΠ»Π΅ΠΉΠΊΠΎΠ·ΠΎΠΌ. Π£ΠΊΠ°Π·Π°Π½Π½Ρ‹Π΅ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΎΡ€Ρ‹ ΠΌΠΎΠ³ΡƒΡ‚ Π±Ρ‹Ρ‚ΡŒ Π½ΠΎΠ²ΠΎΠΉ структурой, которая ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ ΠΌΠΎΠ΄ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π° Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ Π±ΠΎΠ»Π΅Π·Π½ΠΈ, ΠΈ ΠΌΠΎΠ³ΡƒΡ‚ ΡΡ‡ΠΈΡ‚Π°Ρ‚ΡŒΡΡ Π½ΠΎΠ²ΠΎΠΉ мишСнью ΠΏΡ€ΠΈ Π»Π΅Ρ‡Π΅Π½ΠΈΠΈ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… Π»Π΅ΠΉΠΊΠΎΠ·ΠΎΠΌ

    Zipf's law in Multifragmentation

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    We discuss the meaning of Zipf's law in nuclear multifragmentation. We remark that Zipf's law is a consequence of a power law fragment size distribution with exponent τ≃2\tau \simeq 2. We also recall why the presence of such distribution is not a reliable signal of a liquid-gas phase transition

    A search on Dirac equation

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    The solutions, in terms of orthogonal polynomials, of Dirac equation with analytically solvable potentials are investigated within a novel formalism by transforming the relativistic equation into a Schrodinger like one. Earlier results are discussed in a unified framework and certain solutions of a large class of potentials are given.Comment: 9 page

    New Shape Invariant Potentials in Supersymmetric Quantum Mechanics

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    Quantum mechanical potentials satisfying the property of shape invariance are well known to be algebraically solvable. Using a scaling ansatz for the change of parameters, we obtain a large class of new shape invariant potentials which are reflectionless and possess an infinite number of bound states. They can be viewed as q-deformations of the single soliton solution corresponding to the Rosen-Morse potential. Explicit expressions for energy eigenvalues, eigenfunctions and transmission coefficients are given. Included in our potentials as a special case is the self-similar potential recently discussed by Shabat and Spiridonov.Comment: 8pages, Te

    Supersonic optical tunnels for Bose-Einstein condensates

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    We propose a method for the stabilisation of a stack of parallel vortex rings in a Bose-Einstein condensate. The method makes use of a hollow laser beam containing an optical vortex. Using realistic experimental parameters we demonstrate numerically that our method can stabilise up to 9 vortex rings. Furthermore we point out that the condensate flow through the tunnel formed by the core of the optical vortex can be made supersonic by inserting a laser-generated hump potential. We show that long-living immobile condensate solitons generated in the tunnel exhibit sonic horizons. Finally, we discuss prospects of using these solitons for analogue gravity experiments.Comment: 14 pages, 3 figures, published versio
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