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Cooling and trapping of ultracold strontium isotopic mixtures

N. Poli, R. E. Drullinger, G. Ferrari, J. Léonard, F. Sorrentino, and G. M. Tino
Phys. Rev. A 71, 061403(R) – Published 13 June 2005

Abstract

We present the simultaneous cooling and trapping of an isotopic mixture in a magneto-optical trap and describe the transfer of the mixture into a conservative, far-off-resonant dipole trap. The mixture is prepared with a technique that applies to intermediate and heavy alkaline-earth-metal-like atoms. In this work, Sr88 and Sr86 are simultaneously loaded first into the magneto-optical trap operated on the S01P13 spin-forbidden line at 689 nm, and then transferred into the dipole trap. We observe fast interspecies thermalization in the dipole trap which allows one to set a lower bound on the Sr88Sr86 elastic cross section.

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  • Received 8 March 2005

DOI:https://doi.org/10.1103/PhysRevA.71.061403

©2005 American Physical Society

Authors & Affiliations

N. Poli, R. E. Drullinger, G. Ferrari, J. Léonard*, F. Sorrentino, and G. M. Tino

  • Dipartimento di Fisica—LENS, Università di Firenze, Istituto Nazionale di Fisica Nucleare—Sezione di Firenze, Istituto Nazionale di Fisica della Materia—Unità di Firenze, Polo Scientifico, 50019 Sesto Fiorentino, Italy

  • *Present address: Van der Waals-Zeeman Institute, Amsterdam, The Netherlands. Permanent address: IPCMS, Strasbourg, France.
  • Electronic address: guglielmo.tino@fi.infn.it

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Issue

Vol. 71, Iss. 6 — June 2005

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Images

  • Figure 1
    Figure 1
    Relevant energy levels and optical transitions for laser cooling and trapping of strontium.Reuse & Permissions
  • Figure 2
    Figure 2
    Metastable P23 state decay when trapped in a 56Gcm magnetic quadrupole. The data are taken for the individual isotopes with the S01P11 MOT switched off (circles: Sr86, lifetime τ=4.7s. Squares: Sr88, τ=6.6s), and with the S01P11 MOT operating on the undetected isotope (diamonds: Sr86 with Sr88 MOT, τ=4.7s. Triangles: Sr88 with Sr86 MOT, τ=4.9s). The measurements are taken after red MOT recapture and the e1 lifetimes are reported.Reuse & Permissions
  • Figure 3
    Figure 3
    Time sequence for simultaneous trapping of Sr88 and Sr86 in an optical dipole trap. MOT: magneto-optical trap. ToF: time of flight.Reuse & Permissions
  • Figure 4
    Figure 4
    Transfer from the intercombination red MOT to the optical dipole trap with different overlap time between the final red MOT and the FORT. The Sr86 and Sr88 mixture was prepared in order to load about twice Sr88 than Sr86atoms in the final red MOT.Reuse & Permissions
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