1 / 23

Optimal Pulse sequences for efficient population transfer in lower (n<10) Rydberg states

Optimal Pulse sequences for efficient population transfer in lower (n<10) Rydberg states. Mudessar Shah How Camp Marc Trachy. Supervisor: Brett DePaola. Application. Need for a system to be in a specified quantum state Laser control of chemical reactions Atom optics

kobe
Download Presentation

Optimal Pulse sequences for efficient population transfer in lower (n<10) Rydberg states

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. Optimal Pulse sequences for efficient population transfer in lower (n<10) Rydberg states Mudessar Shah How Camp Marc Trachy Supervisor: Brett DePaola

  2. Application Need for a system to be in a specified quantum state • Laser control of chemical reactions • Atom optics • Quantum information

  3. Absorp. k E=ћω P=ћK J= ћ E=0 P=0 J= 0 E=ћω P=ћK J= ћ Two level system 1.0 adiab. coh. exc. Exci. population 0.5 incoh. exc. Pe(t)=1/2[1-e-F(T)] F(T)= I(t)dt Pe(t)=1/2[1-cosΩt] when radiation varies in amplitude cosine argument is replaced by so-called pulse area 0.0 time

  4. Advantages • Excitation between state of same parity can be produced, for which single photon transition are forbidden for electric dipole radiation, or between magnetic sublevels. (for 3 and higher) • Excitation efficiency can be made insensitive to many of experimental details (pulse area, Shape etc). • 100% population transfer between same parity state is possible

  5. |3> 4d 2 |2> 5p  1 |1> 5s Ladder Theoratical prediction For three level systems

  6. |4> 3 9f 4d Delay2 Delay1 |3> 2 2 5p L3 L1 L2 |2> 1 1 |1> 5s Ladder Adiabatic population transfer using sequential pulses (Three photon transition)

  7. Equation of motion

  8. Delay2 Delay1 L2 L3 L1 Delay1 Vs %f population

  9. Delay2 Delay1 L2 L3 L1 Delay2 Vs %f population

  10. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder L1 vs %f

  11. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder L3 vs %9f

  12. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder L2 vs %f

  13. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder Detuning1 vs %f

  14. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder Detuning2 vs %f

  15. General Apparatus Design

  16. Q-Value Spectra Q-Value Spectra 5s-3p 4d-3d 5s-3s

  17. 5p-3p 4d-3s 4d-3d 2D Spectrum 2.5 2D Spectrum 5s-3p 5p-3p 5s-3s 2.0 1.5 Time (ms) 1.0 0.5 0.0 50 100 150 Q-Value (Channel)

  18. Time Evolution of Population

  19. TAC spectra for 9f

  20. Thanks!

  21. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder %5p vs %9f

  22. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder %5s vs %9f

  23. |4> 3 |3> 2 2 |2> 1 1 |1> Ladder %4d vs %9f

More Related