Difference between revisions of "LaserCooling"

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(Overview)
(Overview)
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Currently, our group is working with the radical CaF. We have produced a slow, cryogenic beam of CaF with rotational cooling, and have demonstrated cycling of over 1000 photons (and up to 10^5) using the state-of-the-art laser cooling scheme demonstrated by Shuman et al. [3-4] Current work is ongoing to measure longitudinal slowing.  
 
Currently, our group is working with the radical CaF. We have produced a slow, cryogenic beam of CaF with rotational cooling, and have demonstrated cycling of over 1000 photons (and up to 10^5) using the state-of-the-art laser cooling scheme demonstrated by Shuman et al. [3-4] Current work is ongoing to measure longitudinal slowing.  
  
'''Laser Cooling of Atoms (Yb & Tm)'''
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'''Laser Cooling of Atoms (Yb, Tm, & Ho)'''
 
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We first investigated laser cooling and trapping of atoms from a buffer-gas beam. We made the first buffer-gas loaded MOT, using Yb atoms as our species of interest. This MOT, which used no slowing of any kind (Zeeman, laser, etc.), demonstrated the power of our very-slow beam technology, which we plan to use for a molecular MOT. Furthermore, this MOT demonstrated that, in principle, buffer-gas beam technology is compatible with 3D magneto-optical trapping. Owing to the universal nature of this source, we also implemented a MOT of Thulium atoms with only a change of doubling crystal in our optics set-up. MOTs of Thulium, a refractory element, have low loading rates due to the difficulties with oven sources. Our buffer-gas loaded MOT circumvents these high temperature oven sources and allows loading rates over 10^8 /sec/shot, or over 10^9/sec cumulative. This technology could be used to co-load multiple species with little technological overhead (no multiple zeeman slowers).
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We first investigated laser cooling and trapping of atoms from a buffer-gas beam. We made the first buffer-gas loaded MOT, using Yb atoms as our species of interest. This MOT, which used no slowing of any kind (Zeeman, laser, etc.), demonstrated the power of our very-slow beam technology, which we plan to use for a molecular MOT. Furthermore, this MOT demonstrated that, in principle, buffer-gas beam technology is compatible with 3D magneto-optical trapping. Owing to the universal nature of this source, we also implemented MOTs of Thulium and Holmium atoms with only a change of doubling crystal in our optics set-up. Thulium and Holmium are highly magnetic species that are of interest for quantum simulation and quantum computation. These are refractory elements and have low loading rates due to the difficulties with oven sources. Our buffer-gas loaded MOTs circumvent these high temperature oven sources and allows loading rates over 10^8 /sec/shot, or over 10^9/sec cumulative. This technology could be used to co-load multiple species with little technological overhead (no multiple zeeman slowers).
  
 
== References ==
 
== References ==

Revision as of 10:17, 11 July 2013

People

Post Docs

  • Boerge Hemmerling

Grad Students

  • Garrett Drayna
  • Eunmi Chae
  • Aakash Ravi

Collaborators(JILA)

  • Jun Ye (PI), Matthew Hummon, Mark Yeo, Benjamin Stuhl, Alejandra Collopy, Yong Xia

Ye Group Ultracold Molecules Website

Yb blue MOT in our experiment. We have loaded a MOT from a slow buffer-gas beam source. We also can test the effects of a cold buffer-gas beam on MOTs.

Overview

Schematic in experimental plan for laser cooling of atoms and molecules

This experiment is investigating laser cooling and trapping methods as a route towards ultracold molecules. We first cool our species of interest to ~1K using buffer-gas cooling. After buffer-gas cooling, our species is extracted into a very slow beam, where laser cooling can proceed and stationary, 3D traps can be loaded. We are working to demonstrate the compatibility of buffer-gas cooling and laser cooling using atomic species, and we are working to demonstrate novel laser cooling methods in molecules.

Two-stage cryogenic buffer-gas cooled beams are an excellent precursors to laser cooling experiments as the thermal velocities of the atoms or molecules being cooled are comparable to the depth of traps (e.g., magneto-optical traps) [1-2]. In molecular systems, the buffer-gas cooled beams are relevant as well because they quench internal degrees of freedom (e.g., rotational) and thus create a large number of molecules in the ground state.

Laser Cooling and Trapping of Diatomic Radicals (CaF)


We are investigating magneto-optical trapping and cooling of diatomic molecules. Laser cooling of molecules requires buffer-gas cooling to produce samples of ground-state molecules which have necessary rotational phase space densities for current molecular laser cooling schemes. We use slow beam technology developed in our group [1] to reduce the amount of kinetic energy and number of cycled photons needed to bring molecules to rest in a 3D trap.

Currently, our group is working with the radical CaF. We have produced a slow, cryogenic beam of CaF with rotational cooling, and have demonstrated cycling of over 1000 photons (and up to 10^5) using the state-of-the-art laser cooling scheme demonstrated by Shuman et al. [3-4] Current work is ongoing to measure longitudinal slowing.

Laser Cooling of Atoms (Yb, Tm, & Ho)


We first investigated laser cooling and trapping of atoms from a buffer-gas beam. We made the first buffer-gas loaded MOT, using Yb atoms as our species of interest. This MOT, which used no slowing of any kind (Zeeman, laser, etc.), demonstrated the power of our very-slow beam technology, which we plan to use for a molecular MOT. Furthermore, this MOT demonstrated that, in principle, buffer-gas beam technology is compatible with 3D magneto-optical trapping. Owing to the universal nature of this source, we also implemented MOTs of Thulium and Holmium atoms with only a change of doubling crystal in our optics set-up. Thulium and Holmium are highly magnetic species that are of interest for quantum simulation and quantum computation. These are refractory elements and have low loading rates due to the difficulties with oven sources. Our buffer-gas loaded MOTs circumvent these high temperature oven sources and allows loading rates over 10^8 /sec/shot, or over 10^9/sec cumulative. This technology could be used to co-load multiple species with little technological overhead (no multiple zeeman slowers).

References

  • [1] Hsin-I Lu, Julia Rasmussen, Matthew J. Wright, Dave Patterson, and John M. Doyle. Phys. Chem. Chem. Phys., 2011, DOI: 10.1039/c1cp21206k.
  • [2] D. Patterson and J.M. Doyle. J of Chem Phys 126, 154307 (2007).
  • [3] E. S. Shuman, J. F. Barry, D. R. Glenn, and D. DeMille, Phys. Rev. Lett. 103, 223001 (2009).
  • [4] E. S. Shuman, J. F. Barry, and D. DeMille. Nature 467, 820 (2010).
  • [5] M. T. Hummon, M. Yeo, B. K. Stuhl, A. L. Collopy, Y. Xia, and J. Ye, “2D Magneto-Optical Trapping of Diatomic Molecules”, Physical Review Letters, vol. 110, no. 14, pp. 143001/1-5, 2013.