Difference between revisions of "BEC"
m (→Recent Publications) |
m (→Metastable Helium BEC) |
||
| Line 9: | Line 9: | ||
=Metastable Helium BEC= | =Metastable Helium BEC= | ||
[[image:BEC_cell.jpg|thumb|left|The G-10 cell and trapping magnets.]] [[image:He_BEC_formation.jpg|thumb|right|Phase-contrast images of 4He* in 1 ms TOF, showing BEC formation. (a) a thermal cloud slightly above Tc. (b) onset of BEC. (c) a nearly pure BEC after further evaporative cooling.]] | [[image:BEC_cell.jpg|thumb|left|The G-10 cell and trapping magnets.]] [[image:He_BEC_formation.jpg|thumb|right|Phase-contrast images of 4He* in 1 ms TOF, showing BEC formation. (a) a thermal cloud slightly above Tc. (b) onset of BEC. (c) a nearly pure BEC after further evaporative cooling.]] | ||
| − | We have utilized buffer-gas methods to demonstrate Bose-Einstein condensation of 4He* without the use of laser pre-cooling. These methods are readily extendable to any paramagnetic species with typical collisional parameters that allow for efficient evaporative cooling, significantly extending the scope of ultracold atom/molecule research. The experiment takes place in a G-10 cell, coaxially inside the bore of a 4 T deep superconducting anti-Helmholtz magnetic trap and thermally anchored to a dilution refrigerator. 4He* is excited via RF discharge with an efficiency of 10^-5 | + | We have utilized buffer-gas methods to demonstrate Bose-Einstein condensation of 4He* without the use of laser pre-cooling. These methods are readily extendable to any paramagnetic species with typical collisional parameters that allow for efficient evaporative cooling, significantly extending the scope of ultracold atom/molecule research. The experiment takes place in a G-10 cell, coaxially inside the bore of a 4 T deep superconducting anti-Helmholtz magnetic trap and thermally anchored to a dilution refrigerator. 4He* is excited via RF discharge from a 4He buffer gas with an efficiency of 10^-5 and cooled to the refrigerator temperature by collisions with the remaining buffer gas. The buffer gas is cryo-pumped to a charcoal sorb, leaving approximately 10^11 4He* atoms trapped in the magnetic field. The atom cloud is then evaporatively cooled to 1 mK by surface-induced evaporation, forced by asymmetrically reducing the currents to the anti-Helmholtz coils. Atoms are then transferred to a tightly confining, superconducting quadrupole-Ioffe configuration (QUIC) trap to prevent Majorana losses. After transferring the atoms evaporative cooling continues, now using an RF knife. In the present apparatus we observe BEC formation at a temperature of 5 uK with approximately 10^6 atoms remaining, while further evaporative cooling create nearly-pure condensates of 2-300,000 atoms. Geometric constraints currently limit the transfer of atoms to the QUIC trap to 5% efficiency; straightforward improvements should produce condensates of 10^7 atoms. |
Click here for 2009 GRC poster:[http://cua.harvard.edu/pub/talks_and_posters/He_BEC_GRC_2009.pdf He_BEC_GRC_2009_poster.pdf] | Click here for 2009 GRC poster:[http://cua.harvard.edu/pub/talks_and_posters/He_BEC_GRC_2009.pdf He_BEC_GRC_2009_poster.pdf] | ||
Revision as of 14:25, 29 July 2009
Contents
Overview
Despite innumerable experimental advances, research with degenerate Bose and Fermi gases has remained limited to only a handful of atomic species since its inception due to the field's reliance on laser pre-cooling as the first step towards quantum degeneracy. Developmening new cooling methods applicable to a wider range of atoms and also to molecules and extendable to the ultracold regime is thus important for taking full advantage of scientific opportunities in new areas.
People
- Charlie Doret
- Colin Connolly
- Yat Shan Au
Metastable Helium BEC
We have utilized buffer-gas methods to demonstrate Bose-Einstein condensation of 4He* without the use of laser pre-cooling. These methods are readily extendable to any paramagnetic species with typical collisional parameters that allow for efficient evaporative cooling, significantly extending the scope of ultracold atom/molecule research. The experiment takes place in a G-10 cell, coaxially inside the bore of a 4 T deep superconducting anti-Helmholtz magnetic trap and thermally anchored to a dilution refrigerator. 4He* is excited via RF discharge from a 4He buffer gas with an efficiency of 10^-5 and cooled to the refrigerator temperature by collisions with the remaining buffer gas. The buffer gas is cryo-pumped to a charcoal sorb, leaving approximately 10^11 4He* atoms trapped in the magnetic field. The atom cloud is then evaporatively cooled to 1 mK by surface-induced evaporation, forced by asymmetrically reducing the currents to the anti-Helmholtz coils. Atoms are then transferred to a tightly confining, superconducting quadrupole-Ioffe configuration (QUIC) trap to prevent Majorana losses. After transferring the atoms evaporative cooling continues, now using an RF knife. In the present apparatus we observe BEC formation at a temperature of 5 uK with approximately 10^6 atoms remaining, while further evaporative cooling create nearly-pure condensates of 2-300,000 atoms. Geometric constraints currently limit the transfer of atoms to the QUIC trap to 5% efficiency; straightforward improvements should produce condensates of 10^7 atoms.
Click here for 2009 GRC poster:He_BEC_GRC_2009_poster.pdf
Two-body collisions in thulium and erbium
Since producing our 4He* BEC we have been investigating two-body atom-atom collisional properties of the "submerged-shell" rare-earth atoms thulium and erbium using the same apparatus. Previous research in our lab indicated that the submerged-shell nature of these atoms gives rise to strong suppression of inelastic processes during atom-helium collisions. Similar suppression of inelastic collisions in atom-atom collisions would permit efficient evaporative cooling and make these atoms excellent candidates for new quantum degenerate gases, accessible using our new buffer-gas BEC approach.
Recent Publications
- A buffer-gas cooled Bose-Einstein condensate, S. C. Doret, C. B. Connolly, W. Ketterle, and J. M. Doyle, to be published by Phys. Rev. Lett. (2009).
- Spin-exchange collisions of submerged shell atoms below 1 kelvin, J.G.E. Harris, S.V. Nguyen, S.C. Doret, W. Ketterle, and J.M. Doyle. Physical Review Letters, 99, 223201 (2007).
- Evaporative cooling of metastable helium in the multi-partial-wave regime, S.V. Nguyen, S.C. Doret, C.B. Connolly, R.A. Michniak, W. Ketterle, and J.M. Doyle. Phys. Rev. A, 72, 060703(R) (2005).
