1 / 9

Physics 551 Presentation: Doppler Cooling

Physics 551 Presentation: Doppler Cooling. Zane Shi Princeton University November 6 th , 2007. Photon Recoil. Sodium Levels. Absorbed photon reduces the atom’s velocity by ∆v = ћ k/m Emitted photon is in a random direction, and the time average of the momentum transfer is zero.

hammett-douglas
Download Presentation

Physics 551 Presentation: Doppler Cooling

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Physics 551 Presentation: Doppler Cooling Zane Shi Princeton University November 6th, 2007

  2. Photon Recoil Sodium Levels Absorbed photon reduces the atom’s velocity by ∆v = ћk/m Emitted photon is in a random direction, and the time average of the momentum transfer is zero

  3. Doppler Effect Due to the Doppler Effect, the laser must be tuned to a frequency ω=ω0-kvz As the atom slows down, the driving frequency must be adjusted accordingly so that the atom still absorbs the photon Two ways to experimentally achieve this: Zeeman Tuning Chirp Cooling

  4. Zeeman Tuning F’=3 ħω F”=2 The tapered solenoid creates a variable magnetic field such that the transition frequency shift due to Zeeman splitting matches the frequency shift due to the Doppler effect

  5. Chirp Cooling Another method of Doppler cooling is to rapidly sweep the driving laser frequency If the frequency is swept fast enough, each atom will interact with the “right” photon; for sodium atoms, a sweep of 1GHz in a few milliseconds is required The name comes from the fact that the driving frequency sweeps sounds like birds chirping

  6. Optical Molasses Six Laser beams from the three coordinate axis intersect at the origin to form a “trap” Each atom with velocity v can absorb a frequency of where g is the natural line width Due to the Doppler Effect, the force on the atom in the trap is F = -av, i.e., the atom is always pulled back in to the trap

  7. Optical Molasses

  8. Doppler Limit The frequency of the six laser beams in the optical molasses can be gradually reduced so that only the slowest atoms are confined However, since the emission of a photon from an excited atom is in a random direction, the atom can gain momentum from this emission When the cooling effect from the laser balances the heating from emission, the Doppler Cooling Limit is reached:

  9. 1997 Nobel Prize in Physics William Phillips - Developed the Zeeman slowing technique First to slow atoms to an average velocity of zero in 1985 Steven Chu – Used chirp cooling to slow down atoms and was the first to confine atoms using an optical molasses trap Claude Cohen-Tannoudji - Developed Sisyphus cooling

More Related