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Roger Ding Dr. Daniel S. Elliott John Lorenz July 29, 2010

Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

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Page 1: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Roger DingDr. Daniel S. Elliott

John LorenzJuly 29, 2010

Page 2: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Overall Project Goal:• Photoassociation of Li and Rb

My REU Goals:◦ Work on electronics to help control the dual-

species magneto-optical trap (MOT) Laser locking circuits Timing Controls

Page 3: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Rb Repump Laser

Locking Circuit

Li Trapping and Repump Laser

Rb Trapping Laser

Locking Circuit

Locking Circuit

Timing Control

Timing Control

Timing Control

Dual-Species Magneto-Optical Trap (MOT)

Page 4: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Using light to form molecules from atoms

J. M. Sage et al. “Optical Production of Ultracold Polar Molecules”

Page 5: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Why LiRb?◦ Polar molecule ◦ More complicated than atoms

Potential applications:◦ Quantum computing

D. DeMille. “Quantum Computation with Trapped Polar Molecules”

Page 6: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Magneto-Optical Trap◦ Used to trap and cool

atoms Requirements to trap

atoms:1. Velocity-dependent

force2. Position-dependent

force

Page 7: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Principle ideas:◦ Photons carry momentum◦ Atoms can absorb photons◦ Conservation of momentum◦ Doppler shift

Page 8: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

85Rb~780nm

85Rb

J. Lorenz

3035.73 MHz

361.58 MHz

63.40 MHz

120.65 MHz

D2780.241 nm

85Rb2

3

3

2

2

3

4

22S1/2

22P1/2

22P3/2

29.37 MHz1

D1794.979 nm

Conservation of Momentum

v

p=hf/c

Page 9: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Atom at rest:

Atom moving towards the right:

85Rb fL,RfL,L

v85Rb fL,R + fDfL,L - fD

Page 10: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Red-detune the laser from the transition frequency by

Slow moving atoms

Fast moving atoms

85Rb fL,RfL,L

fL,L - fD fL,R + fD85RbvFnet

L R

fL

=fD=fD

L R

fL

Page 11: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM
Page 12: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Principle Ideas:◦ Slow moving atoms◦ Zeeman effect◦ Selection rules

Page 13: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Zeeman Effect Used to shift atomic

energy levels onto resonance

Slow Moving Atoms Too slow to

Doppler shift laser onto resonance

fD

fL

fL

fD

E=gL�BmFB

Page 14: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Selection Rules In a magnetic field, atoms preferentially

absorb light depending on its polarization

University of Colorado. “Advanced Optics Lab: Laser Cooling and Trapping”

Page 15: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

A. Mills. “Nonlinear Ground-state Pump-probe Spectroscopy in Ultracold Rubidium: Raman-coupled Dressed State

Spectroscopy”

Page 16: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

+-

I

I

Page 17: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Lasers must be tuned and kept at specific frequencies

Stabilizing lasers:◦ Temperature control◦ Current control◦ Electronic feedback

Page 18: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Peak Locking

Small capture range:◦ Accurate ◦ Sensitive to

disturbances

Dichroic Atomic Vapor Laser Lock (DAVLL)

Large capture range:◦ Robust◦ Tendency to drift

f

V

Page 19: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Idea: take the “derivative” of the Doppler-free saturated absorption signal

Page 20: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Rb Cell Rb Cell

Doppler broadening “Hole burning”

87RbF=2

85RbF=3

85RbF=2

87RbF=1

87RbF=2

85RbF=3

85RbF=2

87RbF=1

Page 21: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Rb Cell

Doppler-free saturated absorption

87RbF=2

85RbF=3

85RbF=2

87RbF=1

Physical implementation of Doppler-free saturated absorption

Page 22: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

F=3

2-3 C.O.

2-4 C.O.

F=4

3-4 C.O.

Close-up of 85Rb hyperfine peaks

F=2

Doppler-free saturated absorption87Rb

F=285RbF=3

85RbF=2

87RbF=1

Look at 85Rb F=3 ground state

Page 23: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Hyperfine Peaks Crossover Resonances

F=3

F=2

F=3

F=3

F=2

F=3

-fD

+fD

Page 24: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

1. Apply a dither to the Doppler-free saturated absorption signal

2. Use a lock-in amplifier and low-pass filter to convert amplitude of dither on signal to voltage

Dither

Lock-in +Low-pass

f

Abs.

f

Abs.

f

Abs.

f

V

Page 25: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Idea: in a magnetic field, atoms absorb light differently depending on its polarization

Page 26: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

f

Abs.

f

Abs.

Rb Cell+

-

B

Page 27: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

A. Mills. “Nonlinear Ground-state Pump-probe Spectroscopy in Ultracold Rubidium: Raman-coupled Dressed State

Spectroscopy”

Page 28: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Want benefits of both peak locking and DAVLL schemes◦ Accurate◦ Robust

Brute force approach

Peak Locking

DAVLL +

_ Error Signal

Page 29: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Have not yet had the chance to do extensive testing

Appears to be somewhat quirky:◦ Does not yet lock as well as we had hoped

Improvements:◦ Tweak component values◦ Adjust error signals◦ Better method of combining signals

Page 30: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Need method of controlling multiple acousto-optic modulators for the dual-species MOT

Interface with National Instruments data acquisition card

Page 31: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

AOMs are used for:◦ Frequency shifting◦ Fast shutters

RP Photonics “Acousto-optic Modulators”

Page 32: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Voltage Controlled Oscillator

(VCO)

RF Switch

Voltage Controlled Attenuator

National Instruments Card

AmplifierAcousto-Optic

Modulator (AOM)

Voltage Controlled Oscillator

(VCO)

AmplifierAcousto-Optic

Modulator (AOM)

x6

x2

Page 33: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM
Page 34: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM
Page 35: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

My projects involved working on control mechanisms for the dual-species MOT◦ Laser locking circuits◦ AOM controller board

Page 36: Ding - Final PresentationMicrosoft PowerPoint - Ding - Final Presentation.pptx Author: sergei Created Date: 5/29/2013 6:58:40 PM

Dr. Daniel S. Elliott Dr. Sergei Savikhin John Lorenz Adeel Altaf Dionysios Antypas