The “Diphoton”: A Two–Photon Bound State in Self–Focusing Media

1992 ◽  
pp. 317-325
Author(s):  
RAYMOND Y. CHIAO ◽  
IVAN H. DEUTSCH ◽  
JOHN C. GARRISON
Keyword(s):  
1991 ◽  
Vol 67 (11) ◽  
pp. 1399-1402 ◽  
Author(s):  
Raymond Y. Chiao ◽  
Ivan H. Deutsch ◽  
John C. Garrison
Keyword(s):  

2018 ◽  
Vol 63 (21) ◽  
pp. 1392-1396 ◽  
Author(s):  
Xiaorui Wang ◽  
Honggang Ye ◽  
Zhicheng Su ◽  
Dapeng Yu ◽  
Shijie Xu

1997 ◽  
Vol 36 (6) ◽  
pp. 1155 ◽  
Author(s):  
Guang S. He ◽  
Makoto Yoshida ◽  
Jayant D. Bhawalkar ◽  
Paras N. Prasad

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
C. F. Lo

AbstractWe have shown that the smallest possible singel-qubit critical coupling strength of the N-qubit two-photon Rabi model is only 1/N times that of the two-photon Rabi model. The spectral collapse can thus occur at a more attainable value of the critical coupling. For both of the two-qubit and three-qubit cases, we have also rigorously demonstrated that at the critical coupling the system not only has a set of discrete eigenenergies but also a continuous energy spectrum. The discrete eigenenergy spectrum can be derived via a simple one-to-one mapping to the bound state problem of a particle of variable effective mass in the presence of a finite potential well and a nonlocal potential. The energy difference of each qubit, which specifies both the depth of the finite potential well and the strength of the nonlocal potential, determines the number of bound states available, implying that the extent of the incomplete spectral collapse can be monitored in a straightforward manner.


2021 ◽  
Author(s):  
Lei Wang ◽  
Zhen Yi ◽  
Li-hui Sun ◽  
Wen-Ju Gu

Abstract We study the nonreciprocal properties of transmitted photons in the chiral waveguide QED system, including single- and two-photon transmissions and second-order correlations. For the single-photon transmission, the nonreciprocity is induced by the effects of chiral coupling and atomic dissipation in the weak coupling region. It vanishes in the strong coupling regime when the effect of atomic dissipation becomes ignorable. In the case of two-photon transmission, there exist two ways of going through the emitter: independently as plane waves and formation of bound state. Besides the nonreciprocal behavior of plane waves, the bound state that differs in two directions also alters transmission probabilities. In addition, the second-order correlation of transmitted photons depends on the interference between plane wave and bound state. The destructive interference leads to the strong antibunching in the weak coupling region, while the effective formation of bound state leads to the strong bunching in the intermediate coupling region. However, the negligible interactions for left-propagating photons hardly change the statistics of the input coherent state.


1993 ◽  
Vol 47 (4) ◽  
pp. 3330-3336 ◽  
Author(s):  
Ivan H. Deutsch ◽  
Raymond Y. Chiao ◽  
John C. Garrison

1980 ◽  
Vol 10 (8) ◽  
pp. 1009-1013 ◽  
Author(s):  
V D Gora ◽  
Yu N Karamzin ◽  
Anatolii P Sukhorukov

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