2011
DOI: 10.1103/physreva.84.043641
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Optimized Bose-Einstein-condensate production in a dipole trap based on a 1070-nm multifrequency laser: Influence of enhanced two-body loss on the evaporation process

Abstract: We present an optimized strategy for the production of tightly confined Bose-Einstein condensates (BEC) of 87 Rb in a crossed dipole trap with direct loading from a magneto-optical trap. The dipole trap is created with light of a multifrequency fiber laser with a center wavelength of 1070 nm. Evaporative cooling is performed by ramping down the laser power only. A comparison of the resulting atom number in an almost pure BEC to the initial atom number and the value for the gain in phase space density per atom … Show more

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Cited by 29 publications
(30 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%
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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%
“…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%
“…For our typical atom number density of ∼10 13 atoms/cm 3 , achieved after the dipole trap loading, this corresponds to an initial loss rate of ∼ 1 Hz. We have attributed these twobody losses to light-assisted inelastic collisions, enhanced by the multimode spectrum of our laser [31][32][33]. The second is a residual loading from the quadrupole.…”
Section: Loading Of the Optical Dipole Trapmentioning
confidence: 95%
“…Our numerical simulations are based in the following loading process: the BEC is created in a cross-dipole trap, see e.g. [213], and loaded into the red-detuned sheet of light. We consider that both the cross-dipole trap and the red-detuned sheet of light lie in a common plane orthogonal to the gravity field.…”
Section: Numerical Simulations Of a Bec Of 87 Rb Atomsmentioning
confidence: 99%