Fourier Description of Optical Cavity Modes

Author(s):  
J. Scott Tyo ◽  
Andrey Alenin
Keyword(s):  
2020 ◽  
Vol 124 (3) ◽  
Author(s):  
Joshua Feis ◽  
Dominik Beutel ◽  
Julian Köpfler ◽  
Xavier Garcia-Santiago ◽  
Carsten Rockstuhl ◽  
...  

2009 ◽  
Vol 80 (4) ◽  
Author(s):  
A. Dantan ◽  
M. Albert ◽  
J. P. Marler ◽  
P. F. Herskind ◽  
M. Drewsen

1993 ◽  
Vol 140 (12) ◽  
pp. 3492-3494 ◽  
Author(s):  
Corrine L. Curtis ◽  
Vincent V. Doan ◽  
Grace M. Credo ◽  
Michael J. Sailor

2016 ◽  
Vol 28 (14) ◽  
pp. 1529-1532 ◽  
Author(s):  
Jing Chen ◽  
Tao Zhang ◽  
Chaojun Tang ◽  
Peng Mao ◽  
Yuanjian Liu ◽  
...  

2010 ◽  
Vol 114 (3) ◽  
pp. 1241-1246 ◽  
Author(s):  
Brian P. Mehl ◽  
Ralph L. House ◽  
Abhineet Uppal ◽  
Amanda J. Reams ◽  
Chuan Zhang ◽  
...  

1965 ◽  
Vol 4 (S1) ◽  
pp. 58 ◽  
Author(s):  
A. G. Fox
Keyword(s):  

2011 ◽  
Vol 09 (supp01) ◽  
pp. 83-92 ◽  
Author(s):  
MATTEO BINA ◽  
FEDERICO CASAGRANDE ◽  
ALFREDO LULLI ◽  
MARCO G. GENONI ◽  
MATTEO G. A. PARIS

We describe the dynamics of tripartite state mapping and entanglement transfer from qubit-like radiation states to two-level atoms via optical cavity modes. When the entangled radiation is carried to the cavities by single-mode fibers, optimal pure and mixed state transfer is predicted for perfect mirror transmittance, and entanglement sudden death (and birth) is demonstrated for Werner input states. The general case of multi-mode fiber coupling is also discussed. The dynamics is finally investigated under various dissipative effects.


2019 ◽  
Vol 5 (4) ◽  
pp. eaav0582 ◽  
Author(s):  
Prashanta Kharel ◽  
Glen I. Harris ◽  
Eric A. Kittlaus ◽  
William H. Renninger ◽  
Nils T. Otterstrom ◽  
...  

To date, microscale and nanoscale optomechanical systems have enabled many proof-of-principle quantum operations through access to high-frequency (gigahertz) phonon modes that are readily cooled to their thermal ground state. However, minuscule amounts of absorbed light produce excessive heating that can jeopardize robust ground-state operation within these microstructures. In contrast, we demonstrate an alternative strategy for accessing high-frequency (13 GHz) phonons within macroscopic systems (centimeter scale) using phase-matched Brillouin interactions between two distinct optical cavity modes. Counterintuitively, we show that these macroscopic systems, with motional masses that are 1 million to 100 million times larger than those of microscale counterparts, offer a complementary path toward robust ground-state operation. We perform both optomechanically induced amplification/transparency measurements and demonstrate parametric instability of bulk phonon modes. This is an important step toward using these beam splitter and two-mode squeezing interactions within bulk acoustic systems for applications ranging from quantum memories and microwave-to-optical conversion to high-power laser oscillators.


1998 ◽  
Vol 536 ◽  
Author(s):  
Keiki-Pua S. Dancil ◽  
Douglas P. Greiner ◽  
Michael J. Sailor

AbstractIn this paper we demonstrate that porous silicon (PS) can be used as an immobilization matrix and a transducer for biosensor applications. Thin layers of PS were fabricated showing fine structure in their reflection spectra, characteristic of longitudinal optical cavity modes, or Fabry-Perot interference fringes. The PS surface was modified by covalently bonding streptavidin to a heterobifunctional linker immobilized to the surface using common silane chemistry. The mode spacing and wavelength in the interference spectrum was modified, by displacing buffer and introducing proteins into the PS layer. Protein-protein interactions between immobilized Streptavidin and biotinylated Protein A followed by Protein A and IgG were detected. The surface was regenerated during the course of the experiment showing reversibility of the sensor at the third layer.


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