Toggle menu
288
405
15
3.9K
QCLab
Toggle preferences menu
Toggle personal menu
Not logged in
Your IP address will be publicly visible if you make any edits.

Antibunching in an optomechanical oscillator.: Difference between revisions

From QCLab
LeeMyeongwon (talk | contribs)
No edit summary
LeeMyeongwon (talk | contribs)
No edit summary
 
(3 intermediate revisions by the same user not shown)
Line 3: Line 3:
* Date: Wednesday, March 29, 2017, at 17:00
* Date: Wednesday, March 29, 2017, at 17:00
* Place: BK Seminar Room
* Place: BK Seminar Room
Special Condensed Matter Seminar invited by Prof. [[Lee, Donghun|Donghun Lee]]




Line 8: Line 10:




{{Media/Button|S-HY2017d.pdf|Talk slides}}
{{Media/Button|S-HJ2017d.pdf|Talk slides}}
 


It will be uploaded after seminar.


[[Category:Condensed Matter Seminars]]
[[Category:Condensed Matter Seminars]]
[[Category:Seminars]]
[[Category:Seminars]]

Latest revision as of 04:30, 5 April 2017

Prof. HyoJun Seok (Kongju Nat. Univ.)
  • Speaker: Prof. HyoJun Seok (Kongju Nat. Univ.)
  • Date: Wednesday, March 29, 2017, at 17:00
  • Place: BK Seminar Room

Special Condensed Matter Seminar invited by Prof. Donghun Lee


We theoretically analyze antibunching of the phonon field in an optomechanical oscillator employing the membrane-in-the-middle geometry. More specifically, a single-mode mechanical oscillator is quadratically coupled to a single-mode cavity field in the regime in which the cavity dissipation is a dominant source of damping, and adiabatic elimination of the cavity field leads to an effective cubic nonlinearity for the mechanics. We show analytically in the weak coupling regime that the mechanics displays a chaotic phonon field for small optomechanical cooperativity, whereas an antibunched single-phonon field appears for large optomechanical cooperativity. This opens the door to control of the second-order correlation function of a mechanical oscillator in the weak coupling regime.