Strong interaction induced dimensional crossover in 1D quantum gas
Pith reviewed 2026-05-23 17:43 UTC · model grok-4.3
The pith
Strong interactions cause a 1D quantum gas to exhibit 3D behavior in an unchanged elongated trap.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We generated a one-dimensional quantum gas in an elongated optical dipole trap and observed that increasing the scattering length via Feshbach resonance causes the gas to pop up into three dimensions without altering the trap. During this crossover, 1D theories fail, but a modified Yang-Yang equation works at higher temperatures though not for stronger interactions. Breathing-mode frequencies exhibit two quantized plateaus corresponding to 1D and 3D hydrodynamics, with a universal crossover connecting the regimes.
What carries the argument
The strong-interaction-induced dimensional crossover from 1D to 3D behavior in a quantum gas.
If this is right
- 1D mean field theory, Yang-Yang equation, and 1D hydrodynamics fail with increasing scattering length.
- The modified Yang-Yang equation describes the system at temperatures above the 1D threshold but not stronger interactions.
- Breathing-mode frequencies show quantized plateaus for weak (1D) and strong (3D) interactions.
- A universal crossover regime connects the two hydrodynamic regimes where both descriptions fail.
Where Pith is reading between the lines
- This approach enables study of dimensional effects by tuning interactions rather than geometry.
- The universal crossover may apply to other low-dimensional quantum systems.
- Similar interaction-driven crossovers could be explored in fermionic or spinor gases.
- Control over chemical potential and temperature allows isolation of interaction effects from thermal ones.
Load-bearing premise
That observed changes arise purely from increasing the scattering length and not from variations in temperature, density, or trap anharmonicity.
What would settle it
If spatial distributions and breathing frequencies remain unchanged when scattering length is increased while temperature and density are held fixed, the claim that interactions alone drive the crossover would be refuted.
Figures
read the original abstract
We generated a one-dimensional quantum gas confined in an elongated optical dipole trap instead of 2D optical lattices. The sample, comprising thousands of atoms, spans several hundred micrometers and allows for independent control of temperature and chemical potential using Feshbach resonance. This allows us to directly observe and investigate the spatial distribution and associated excitation of 1D quantum gas without any ensemble averaging. In this system, we observed that the dimension of 1D gas will be popped up into 3D due to strong interaction without changing any trapping confinement. During the dimensional crossover, we found that increasing the scattering length leads to the failure of 1D theories, including 1D mean field, Yang-Yang equation, and 1D hydrodynamics. Specifically, the modified Yang-Yang equation effectively describes this 1D system at temperatures beyond the 1D threshold, but it does not account for the effects of stronger interactions. Meanwhile, we observe two possible quantized plateaus of breathing-mode oscillation frequencies predicted by 1D and 3D hydrodynamics, corresponding to weak and strong interactions respectively. And there is also a universal crossover connecting two different regimes where both hydrodynamics fail.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports experimental realization of a 1D quantum gas of thousands of atoms in an elongated optical dipole trap (no 2D lattices), with independent control of temperature and chemical potential via Feshbach resonance. The central claim is that increasing the scattering length induces a dimensional crossover to 3D behavior without changing the trap confinement, manifested as failure of 1D mean-field, Yang-Yang, and hydrodynamic theories, effectiveness of a modified Yang-Yang equation only at moderate interactions, and the appearance of two quantized breathing-mode frequency plateaus (1D and 3D hydrodynamic predictions) connected by a universal crossover regime.
Significance. If the quantitative evidence supports the claims, the result would establish interaction-driven dimensional crossover as a distinct mechanism in quantum gases, clarifying the breakdown of 1D descriptions at strong coupling and the emergence of 3D hydrodynamics in elongated geometries. This could inform theoretical modeling of crossover regimes and experimental studies of low-dimensional many-body systems.
major comments (3)
- [Abstract] Abstract and main text: the claims that '1D theories fail' and that 'two possible quantized plateaus' appear rest on qualitative statements with no reported quantitative data, error bars, fitting procedures, or exclusion criteria for alternative explanations (e.g., temperature drift or trap anharmonicity). This prevents evaluation of whether the observed spatial distributions, excitations, and frequencies actually demonstrate the crossover.
- [Abstract / experimental methods] The central attribution of changes in spatial distribution, excitations, and breathing frequencies solely to increasing scattering length requires explicit demonstration that temperature, chemical potential, and trap parameters remain constant across the resonance sweep. No such quantitative controls or checks are described, leaving open the possibility that magnetic-field-dependent effects mimic the reported signatures.
- [Results / theory comparison] The statement that the modified Yang-Yang equation 'effectively describes this 1D system at temperatures beyond the 1D threshold, but it does not account for the effects of stronger interactions' is presented without comparison metrics, residuals, or parameter ranges, making it impossible to assess the regime boundaries or the claimed failure at strong interactions.
minor comments (2)
- [Methods] Clarify the precise definition and measurement protocol for the 'breathing-mode oscillation frequencies' and how the 1D and 3D hydrodynamic predictions are computed for the specific trap geometry and atom number.
- [Results] Provide the range of scattering lengths, temperatures, and densities explored, along with any figures showing raw data or fits.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive comments. Below we provide point-by-point responses to the major comments. We will revise the manuscript to incorporate additional quantitative details as outlined.
read point-by-point responses
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Referee: [Abstract] Abstract and main text: the claims that '1D theories fail' and that 'two possible quantized plateaus' appear rest on qualitative statements with no reported quantitative data, error bars, fitting procedures, or exclusion criteria for alternative explanations (e.g., temperature drift or trap anharmonicity). This prevents evaluation of whether the observed spatial distributions, excitations, and frequencies actually demonstrate the crossover.
Authors: We agree that the presentation would benefit from more quantitative support. In the revised manuscript, we will include error bars on the breathing mode frequencies from multiple measurements, describe the fitting procedures used to extract the frequencies, and provide quantitative comparisons (e.g., percentage deviation from theoretical predictions) along with discussion of how alternative explanations like temperature drift were excluded based on independent temperature measurements. revision: yes
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Referee: [Abstract / experimental methods] The central attribution of changes in spatial distribution, excitations, and breathing frequencies solely to increasing scattering length requires explicit demonstration that temperature, chemical potential, and trap parameters remain constant across the resonance sweep. No such quantitative controls or checks are described, leaving open the possibility that magnetic-field-dependent effects mimic the reported signatures.
Authors: We note that the experimental methods section describes independent control of temperature and chemical potential via the Feshbach resonance. To explicitly address this, we will add quantitative data in the revision showing the measured temperature and trap frequencies versus magnetic field, demonstrating their constancy within the relevant range. This will confirm that the observed effects are attributable to the change in scattering length. revision: yes
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Referee: [Results / theory comparison] The statement that the modified Yang-Yang equation 'effectively describes this 1D system at temperatures beyond the 1D threshold, but it does not account for the effects of stronger interactions' is presented without comparison metrics, residuals, or parameter ranges, making it impossible to assess the regime boundaries or the claimed failure at strong interactions.
Authors: We will revise the results section to include explicit comparison metrics, such as the root-mean-square deviation between experimental density profiles and the modified Yang-Yang model predictions, and specify the parameter ranges (temperature and interaction strength) over which the agreement holds before deviations appear at stronger interactions. revision: yes
Circularity Check
No circularity: experimental data compared to independent external hydrodynamic predictions
full rationale
The paper reports direct experimental measurements of spatial distributions, excitations, and breathing frequencies in a tunable 1D quantum gas, then compares these observations to pre-existing 1D mean-field, Yang-Yang, 1D hydrodynamic, and 3D hydrodynamic models. No parameter is fitted to the reported data and then re-presented as a prediction, no load-bearing self-citation chain is invoked to justify the core claims, and the derivation chain consists of experimental control of scattering length followed by comparison against externally established theories. The work is therefore self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
Lean theorems connected to this paper
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking matches?
matchesMATCHES: this paper passage directly uses, restates, or depends on the cited Recognition theorem or module.
we observed that the dimension of 1D gas will be popped up into 3D due to strong interaction without changing any trapping confinement... two possible quantized plateaus of breathing-mode oscillation frequencies predicted by 1D and 3D hydrodynamics... universal crossover connecting two different regimes where both hydrodynamics fail
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IndisputableMonolith/Foundation/DimensionForcing.lean (referenced via 8-tick period 2^D=8)reality_from_one_distinction echoes?
echoesECHOES: this paper passage has the same mathematical shape or conceptual pattern as the Recognition theorem, but is not a direct formal dependency.
the crossover from 1D to 3D happens near μ1D/ℏω⊥∼1... deviation from the modified Yang-Yang equation becomes evident around μ0≃ℏω⊥
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
and 3D (green dashed line with p 5/2) hydrodynamics. loss (see Appendix D), a consequence of three-body re- combination processes facilitated by a large scattering length [64–67]. And the crossover from 1D to 3D hydro- dynamics is universal where two sets of data match each other when µ1D/ℏω⊥ ranges from 0.5 to 5. IV. CONCLUSIONS In conclusions, we create...
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[2]
One-dimensional regime For 1D gas, where the chemical potential and tem- perature satisfy ℏω∥ ≪ µ1D ≪ ℏω⊥, kBT ≪ ℏω⊥, the thermodynamic behavior can be fully described by the Yang-Yang equation [35]. ε(k) = ℏ2k2 2m − µ − kBT c π Z ∞ −∞ dq ln 1 + e− ε(q) kB T c2 + (k − q)2 , (A1) where k is the quasi-momentum defined by the Bethe Ansatz wavefunction and ϵk...
-
[3]
Three-dimensional regime For strong interaction strength, where the chemical po- tential satisfies µ1D ≫ ℏω⊥, the density distribution in a 3D harmonic trap should obey the 3D Thomas-Fermi dis- tribution in the zero-temperature limit, and the density distribution n(x, y, z) is written as n(x, y, z) = µ0 − m(ω2 ∥x2 + ω2 ⊥y2 + ω2 ⊥z2)/2 g3D , (A6) where g3D...
-
[4]
The only theoretical tool we can use is the 3D GPE, which predicts that all the data in Fig
1D to 3D crossover regime Unfortunately, for intermediate interaction strength, where the chemical potential satisfies µ1D ∼ ℏω⊥, there is no analytic expression for density distribution, which is one of the reasons why people are interested in this regime. The only theoretical tool we can use is the 3D GPE, which predicts that all the data in Fig. 2(b) w...
work page 2000
-
[5]
Giamarchi, Quantum Physics in One Dimension (Ox- ford University Press, 2003)
T. Giamarchi, Quantum Physics in One Dimension (Ox- ford University Press, 2003)
work page 2003
-
[6]
Franchini, An Introduction to Integrable Techniques for One-Dimensional Quantum Systems, Vol
F. Franchini, An Introduction to Integrable Techniques for One-Dimensional Quantum Systems, Vol. 940 (2017)
work page 2017
-
[7]
T. Kinoshita, T. Wenger, and D. S. Weiss, A quantum Newton’s cradle, Nature 440, 900 (2006)
work page 2006
-
[8]
Y. Tang, W. Kao, K.-Y. Li, S. Seo, K. Mallayya, M. Rigol, S. Gopalakrishnan, and B. L. Lev, Thermaliza- tion near Integrability in a Dipolar Quantum Newton’s Cradle, Physical Review X 8, 021030 (2018)
work page 2018
-
[9]
M. Schemmer, I. Bouchoule, B. Doyon, and J. Dubail, Generalized hydrodynamics on an atom chip, Phys. Rev. Lett. 122, 090601 (2019)
work page 2019
-
[10]
M. A. Cazalilla, R. Citro, T. Giamarchi, E. Orignac, and M. Rigol, One dimensional bosons: From condensed mat- ter systems to ultracold gases, Rev. Mod. Phys. 83, 1405 (2011)
work page 2011
-
[11]
X.-W. Guan and P. He, New trends in quantum integra- bility: recent experiments with ultracold atoms, Reports on Progress in Physics 85, 114001 (2022)
work page 2022
-
[12]
G. E. Astrakharchik and S. Giorgini, Quantum monte carlo study of the three- to one-dimensional crossover for a trapped bose gas, Phys. Rev. A 66, 053614 (2002)
work page 2002
-
[13]
D. Blume, Fermionization of a bosonic gas under highly elongated confinement: A diffusion quantum monte carlo study, Phys. Rev. A 66, 053613 (2002)
work page 2002
- [14]
-
[15]
B. Paredes, A. Widera, V. Murg, O. Mandel, and I. Bloch, Tonks-girardeau gas of ultracold atoms in an optical lattice, Nature 429, 277 (2004)
work page 2004
-
[16]
J. M. Wilson, N. Malvania, Y. Le, Y. Zhang, M. Rigol, and D. S. Weiss, Observation of dynamical fermioniza- tion, Science 367, 1461 (2020)
work page 2020
- [17]
-
[18]
G. E. Astrakharchik, J. Boronat, J. Casulleras, and S. Giorgini, Beyond the tonks-girardeau gas: Strongly correlated regime in quasi-one-dimensional bose gases, Phys. Rev. Lett. 95, 190407 (2005)
work page 2005
-
[19]
L. Guan and S. Chen, Super-tonks-girardeau gas of spin- 1/2 interacting fermions, Phys. Rev. Lett. 105, 175301 (2010)
work page 2010
-
[20]
S. Chen, L. Guan, X. Yin, Y. Hao, and X.-W. Guan, Transition from a tonks-girardeau gas to a super-tonks- girardeau gas as an exact many-body dynamics problem, Phys. Rev. A 81, 031609(R) (2010)
work page 2010
- [21]
-
[22]
Y. Le, Y. Zhang, S. Gopalakrishnan, M. Rigol, and D. S. Weiss, Observation of hydrodynamization and lo- cal prethermalization in 1D Bose gases, Nature 618, 494 (2023)
work page 2023
-
[23]
B. Yang, Y.-Y. Chen, Y.-G. Zheng, H. Sun, H.-N. Dai, X.-W. Guan, Z.-S. Yuan, and J.-W. Pan, Quan- tum criticality and the tomonaga-luttinger liquid in one- dimensional bose gases, Phys. Rev. Lett. 119, 165701 (2017)
work page 2017
- [24]
-
[25]
J. Vijayan, P. Sompet, G. Salomon, J. Koepsell, S. Hirthe, A. Bohrdt, F. Grusdt, I. Bloch, and C. Gross, Time-resolved observation of spin-charge deconfinement in fermionic hubbard chains, Science 367, 186 (2020)
work page 2020
- [26]
-
[27]
R. Senaratne, D. Cavazos-Cavazos, S. Wang, F. He, Y.-T. Chang, A. Kafle, H. Pu, X.-W. Guan, and R. G. Hulet, Spin-charge separation in a one-dimensional fermi gas with tunable interactions, Science 376, 1305 (2022)
work page 2022
-
[28]
L. Khaykovich, F. Schreck, G. Ferrari, T. Bourdel, J. Cu- bizolles, L. D. Carr, Y. Castin, and C. Salomon, Forma- tion of a matter-wave bright soliton, Science 296, 1290 (2002)
work page 2002
-
[29]
K. E. Strecker, G. B. Partridge, A. G. Truscott, and R. G. Hulet, Formation and propagation of matter-wave soliton trains, Nature 417, 150 (2002)
work page 2002
-
[30]
U. Al Khawaja, H. T. C. Stoof, R. G. Hulet, K. E. Strecker, and G. B. Partridge, Bright soliton trains of trapped bose-einstein condensates, Phys. Rev. Lett. 89, 200404 (2002)
work page 2002
- [31]
-
[32]
J. Denschlag, J. E. Simsarian, D. L. Feder, C. W. Clark, L. A. Collins, J. Cubizolles, L. Deng, E. W. Hagley, K. Helmerson, W. P. Reinhardt, S. L. Rolston, B. I. Schneider, and W. D. Phillips, Generating solitons by phase engineering of a bose-einstein condensate, Science 287, 97 (2000)
work page 2000
-
[33]
J. H. V. Nguyen, P. Dyke, D. Luo, B. A. Malomed, and R. G. Hulet, Collisions of matter-wave solitons, Nature Physics 10, 918 (2014)
work page 2014
-
[34]
J. H. V. Nguyen, D. Luo, and R. G. Hulet, Formation of matter-wave soliton trains by modulational instability, Science 356, 422 (2017)
work page 2017
-
[35]
T. St¨ oferle, H. Moritz, C. Schori, M. K¨ ohl, and T. Esslinger, Transition from a strongly interacting 1d su- perfluid to a mott insulator, Phys. Rev. Lett. 92, 130403 (2004)
work page 2004
-
[36]
P. Kr¨ uger, S. Hofferberth, I. E. Mazets, I. Lesanovsky, and J. Schmiedmayer, Weakly interacting bose gas in the one-dimensional limit, Phys. Rev. Lett. 105, 265302 (2010)
work page 2010
- [37]
-
[38]
T. Jacqmin, J. Armijo, T. Berrada, K. V. Kheruntsyan, and I. Bouchoule, Sub-poissonian fluctuations in a 1d bose gas: From the quantum quasicondensate to the 11 strongly interacting regime, Phys. Rev. Lett.106, 230405 (2011)
work page 2011
-
[39]
C. N. Yang and C. P. Yang, Thermodynamics of a One- Dimensional System of Bosons with Repulsive Delta- Function Interaction, Journal of Mathematical Physics 10, 1115 (2003)
work page 2003
-
[40]
R. Shah, T. J. Barrett, A. Colcelli, F. Oruˇ cevi´ c, A. Trom- bettoni, and P. Kr¨ uger, Probing the degree of coherence through the full 1d to 3d crossover, Phys. Rev. Lett.130, 123401 (2023)
work page 2023
-
[41]
L. Salasnich, A. Parola, and L. Reatto, Transition from three dimensions to one dimension in bose gases at zero temperature, Phys. Rev. A 70, 013606 (2004)
work page 2004
-
[42]
A. G¨ orlitz, J. M. Vogels, A. E. Leanhardt, C. Raman, T. L. Gustavson, J. R. Abo-Shaeer, A. P. Chikkatur, S. Gupta, S. Inouye, T. Rosenband, and W. Ketterle, Realization of bose-einstein condensates in lower dimen- sions, Phys. Rev. Lett. 87, 130402 (2001)
work page 2001
- [43]
- [44]
-
[45]
A. H. van Amerongen, J. J. P. van Es, P. Wicke, K. V. Kheruntsyan, and N. J. van Druten, Yang-Yang Ther- modynamics on an Atom Chip, Physical Review Letters 100, 090402 (2008)
work page 2008
-
[46]
C. Menotti and S. Stringari, Collective oscillations of a one-dimensional trapped bose-einstein gas, Phys. Rev. A 66, 043610 (2002)
work page 2002
-
[47]
C. Chin, R. Grimm, P. Julienne, and E. Tiesinga, Fesh- bach resonances in ultracold gases, Rev. Mod. Phys. 82, 1225 (2010)
work page 2010
-
[48]
N. Malvania, Y. Zhang, Y. Le, J. Dubail, M. Rigol, and D. S. Weiss, Generalized hydrodynamics in strongly in- teracting 1d bose gases, Science 373, 1129 (2021)
work page 2021
-
[49]
F. Meinert, M. Panfil, M.-J. Mark, K. Lauber, J.-S. Caux, and H.-C. Nagerl, Probing the Excitations of a Lieb-Liniger Gas from Weak to Strong Coupling, Physi- cal Review Letters 115, 085301 (2015)
work page 2015
-
[50]
A. F. Ho, M. A. Cazalilla, and T. Giamarchi, Deconfine- ment in a 2d optical lattice of coupled 1d boson systems, Phys. Rev. Lett. 92, 130405 (2004)
work page 2004
-
[51]
W. Ketterle and N. V. Druten, Evaporative cooling of trapped atoms (Academic Press, 1996) pp. 181–236
work page 1996
-
[52]
S. Chaudhuri, S. Roy, and C. S. Unnikrishnan, Evapora- tive cooling of atoms to quantum degeneracy in an op- tical dipole trap, Journal of Physics: Conference Series 80, 012036 (2007)
work page 2007
-
[53]
Y. Liu, Z. Zhang, S. Miao, Z. Zhao, H. Wang, W. Chen, and J. Hu, Calibrating the absorption imaging of cold atoms under high magnetic fields, Phys. Rev. Appl. 20, 014037 (2023)
work page 2023
-
[54]
G. M. Kavoulakis and C. J. Pethick, Quasi-one- dimensional character of sound propagation in elongated bose-einstein condensed clouds, Phys. Rev. A 58, 1563 (1998)
work page 1998
-
[55]
R. Meppelink, S. B. Koller, and P. van der Straten, Sound propagation in a bose-einstein condensate at finite tem- peratures, Phys. Rev. A 80, 043605 (2009)
work page 2009
-
[56]
M. T. Entwistle, M. J. P. Hodgson, J. Wetherell, B. Longstaff, J. D. Ramsden, and R. W. Godby, Local density approximations from finite systems, Phys. Rev. B 94, 205134 (2016)
work page 2016
-
[57]
A. Minguzzi, P. Vignolo, and M. P. Tosi, Momentum distribution of an interacting bose-einstein condensed gas at finite temperature, Phys. Rev. A 62, 023604 (2000)
work page 2000
-
[58]
M. M. Cerimele, M. L. Chiofalo, F. Pistella, S. Succi, and M. P. Tosi, Numerical solution of the gross-pitaevskii equation using an explicit finite-difference scheme: An application to trapped bose-einstein condensates, Phys. Rev. E 62, 1382 (2000)
work page 2000
-
[59]
W. Bao, D. Jaksch, and P. A. Markowich, Numerical so- lution of the gross–pitaevskii equation for bose–einstein condensation, Journal of Computational Physics 187, 318 (2003)
work page 2003
-
[60]
X. Antoine, W. Bao, and C. Besse, Computa- tional methods for the dynamics of the nonlin- ear schr¨ odinger/gross–pitaevskii equations, Computer Physics Communications 184, 2621 (2013)
work page 2013
- [61]
-
[62]
D. S. Jin, J. R. Ensher, M. R. Matthews, C. E. Wie- man, and E. A. Cornell, Collective excitations of a bose- einstein condensate in a dilute gas, Phys. Rev. Lett. 77, 420 (1996)
work page 1996
-
[63]
B. Fang, G. Carleo, A. Johnson, and I. Bouchoule, Quench-induced breathing mode of one-dimensional bose gases, Phys. Rev. Lett. 113, 035301 (2014)
work page 2014
-
[64]
Stringari, Collective excitations of a trapped bose- condensed gas, Phys
S. Stringari, Collective excitations of a trapped bose- condensed gas, Phys. Rev. Lett. 77, 2360 (1996)
work page 1996
-
[65]
Stringari, Dynamics of bose-einstein condensed gases in highly deformed traps, Phys
S. Stringari, Dynamics of bose-einstein condensed gases in highly deformed traps, Phys. Rev. A 58, 2385 (1998)
work page 1998
-
[66]
A. Csord´ as and R. Graham, Collective excitations in bose-einstein condensates in triaxially anisotropic parabolic traps, Phys. Rev. A 59, 1477 (1999)
work page 1999
-
[67]
T. L. Ho and M. Ma, Quasi 1 and 2d dilute bose gas in magnetic traps : Existence of off-diagonal order and anomalous quantum fluctuations, Journal of Low Tem- perature Physics 115, 61 (1999)
work page 1999
-
[68]
P. O. Fedichev, M. W. Reynolds, and G. V. Shlyapnikov, Three-body recombination of ultracold atoms to a weakly bound s level, Phys. Rev. Lett. 77, 2921 (1996)
work page 1996
-
[69]
B. D. Esry, C. H. Greene, and J. P. Burke, Recombination of three atoms in the ultracold limit, Phys. Rev. Lett.83, 1751 (1999)
work page 1999
- [70]
-
[71]
P. A. Altin, G. R. Dennis, G. D. McDonald, D. D¨ oring, J. E. Debs, J. D. Close, C. M. Savage, and N. P. Robins, Collapse and three-body loss in a 85rb bose-einstein con- densate, Phys. Rev. A 84, 033632 (2011)
work page 2011
-
[72]
M. Olshanii, Atomic Scattering in the Presence of an Ex- ternal Confinement and a Gas of Impenetrable Bosons, Phys. Rev. Lett. 81, 938–941 (1998)
work page 1998
- [73]
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