2017
DOI: 10.1103/physreva.95.013609
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All-optical production of a large Bose-Einstein condensate in a double compressible crossed dipole trap

Abstract: We report on an all-optical production of a 87 Rb Bose-Einstein condensate (BEC) of 10 6 atoms. We construct a double compressible crossed dipole trap (d-CDT) formed by a high-power multimode fiber laser (m-CDT) and a single-mode fiber amplifier (s-CDT), which are both operated at 1.06 µm. A very cold, dense gas is first cooled by polarization gradient cooling in a 3D optical lattice. More than 2×10 7 atoms are loaded into the enlarged d-CDT. Both CDTs are then simultaneously compressed to significantly differ… Show more

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Cited by 14 publications
(9 citation statements)
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“…[59], where = 2 /m Cs (a CsCs −ā) 2 withā = 95.5 a 0 for Cs. We also cannot rule out any heating effects due to the broadband, multi-mode nature of the trapping laser [62][63][64][65] which may inflate the value ofṪ Cs,Heat above the simple estimate of 60 nK/s based upon off-resonant scattering of photons. We find that varying the value of the total trap heating rateṪ Cs,Heat over a large range changes the extracted cross section by less than its error.…”
Section: Analysis Of Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…[59], where = 2 /m Cs (a CsCs −ā) 2 withā = 95.5 a 0 for Cs. We also cannot rule out any heating effects due to the broadband, multi-mode nature of the trapping laser [62][63][64][65] which may inflate the value ofṪ Cs,Heat above the simple estimate of 60 nK/s based upon off-resonant scattering of photons. We find that varying the value of the total trap heating rateṪ Cs,Heat over a large range changes the extracted cross section by less than its error.…”
Section: Analysis Of Resultsmentioning
confidence: 99%
“…The Cs three-body loss coefficient is measured to be K Cs,3 = 1 +1 −0.9 × 10 −26 cm 6 /s at the bias field used in the measurements. In addition to the above terms, T i,ODT is added as an independent heating term to account for any heating from the trapping potential, such as off-resonant photon scattering [61] or additional heating effects due to the multi-mode nature of the trapping laser [62][63][64][65]. The heating rate for Yb alone is found to be zero within experimental error, soṪ Yb,ODT is fixed at 1 nK/s, which is the predicted heating rate due to offresonant photon scattering.…”
Section: Rate Equations For Thermalizationmentioning
confidence: 99%
“…[126], where = 2 /m Cs (a CsCs −ā) 2 withā = 95.5 a 0 for Cs. We also cannot rule out any heating effects due to the broadband nature of the trapping laser [275,277,286,287] which may inflate the value ofṪ Cs,Heat above the simple estimate of 60 nK/s based upon off-resonant scattering of photons. We find that varying the value of the total trap heating rateṪ Cs,Heat over a large range changes the extracted cross section by less than its error.…”
Section: Measuring the Elastic Cross Sectionmentioning
confidence: 87%
“…The Cs three-body loss coefficient is measured to be K Cs,3 = 1 +1 −0.9 × 10 −26 cm 6 /s at the bias field used in the measurements. In addition to the above terms,Ṫ i,dimple is added as an independent heating term to account for any heating from the trapping potential, such as off-resonant photon scattering 1 or additional heating effects due to the broadband nature of the trapping laser [275,277,286,287]. The heating rate for Yb alone is found to be zero within experimental error, soṪ Yb,dimple is fixed at 1 nK/s, which is the predicted heating rate due to off-resonant photon scattering.…”
Section: Interspecies Interactionsmentioning
confidence: 99%
“…One way to achieve that is to use atomic Bose-Einstein condensates (BEC) 26 . The fastest and easiest way to produce an atomic BEC is an all-optical method of condensation 27,28 , where thermal atoms are evaporatively cooled in an optical dipole trap. Such a BEC can be prepared in a free space next to the atom chip in a superposition of a standard magneto-optical trap (MOT) and an optical dipole trap.…”
mentioning
confidence: 99%