Difference between revisions of "BEC"
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new areas. We have utilized buffer-gas methods to demonstrate Bose-Einstein condensation of <math>^4</math>He* 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. | new areas. We have utilized buffer-gas methods to demonstrate Bose-Einstein condensation of <math>^4</math>He* 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. <math>^4</math>He* is excited via RF discharge with an efficiency of <math>10^{-5}</math> from a <math>^4</math>He buffer gas and cooled to the refrigerator temperature by collisions with the remaining buffer gas. The buffer gas is cryo-pumped to a charcoal sorb, leaving ,math>\sim 10^{11} ^4</math>He* atoms trapped in the magnetic field. The atom cloud is then evaporatively cooled to 1 mK by surface-induced evaporation and transferred to a tightly confining superconducting quadrupole-Ioffe configuration trap to prevent Majorana losses. Further evaporative cooling using a RF knife leads to the creation of a BEC at a temperature of 5 <math>\mu</math>K with approximately <math>10^6</math> atoms remaining. | ||
| + | Since producing our <math>^4</math>He* BEC we have been exploring | ||
==Recent Publications== | ==Recent Publications== | ||
Revision as of 08:44, 29 July 2009
Buffer-Gas BEC project
People
- Charlie Doret
- Colin Connolly
- Yat Shan Au
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 to molecules is thus an important step towards realizing scientific opportunities in new areas. We have utilized buffer-gas methods to demonstrate Bose-Einstein condensation of <math>^4</math>He* 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. <math>^4</math>He* is excited via RF discharge with an efficiency of <math>10^{-5}</math> from a <math>^4</math>He buffer gas and cooled to the refrigerator temperature by collisions with the remaining buffer gas. The buffer gas is cryo-pumped to a charcoal sorb, leaving ,math>\sim 10^{11} ^4</math>He* atoms trapped in the magnetic field. The atom cloud is then evaporatively cooled to 1 mK by surface-induced evaporation and transferred to a tightly confining superconducting quadrupole-Ioffe configuration trap to prevent Majorana losses. Further evaporative cooling using a RF knife leads to the creation of a BEC at a temperature of 5 <math>\mu</math>K with approximately <math>10^6</math> atoms remaining.
Since producing our <math>^4</math>He* BEC we have been exploring
