Second-order coherence g (2) (τ) and its frequency-dependent characteristics of a two-longitudinal-mode laser

1996 ◽  
Vol 64 (1) ◽  
pp. 65-72
Author(s):  
Jianping Yin ◽  
Shiqun Zhu ◽  
Weijian Gao ◽  
Yuzhu Wang
1995 ◽  
Vol 117 (22) ◽  
pp. 6101-6108 ◽  
Author(s):  
Marianna Fanti ◽  
Giorgio Orlandi ◽  
Francesco Zerbetto

2019 ◽  
Vol 19 (12) ◽  
pp. 4386-4392 ◽  
Author(s):  
Yunkun Zhao ◽  
Junfeng Zhou ◽  
Chenchen Wang ◽  
Youze Chen ◽  
Liang Lu

1959 ◽  
Vol 31 (11) ◽  
pp. 1457-1462 ◽  
Author(s):  
Eric Rule ◽  
Fred J. Suellentrop ◽  
Thomas A. Perls

1994 ◽  
Vol 351 ◽  
Author(s):  
Shlomo Yitzchaik ◽  
Paul M. Lundquist ◽  
Weiping Lin ◽  
David R. Kanis ◽  
Mark A. Ratner ◽  
...  

ABSTRACTAn attractive and challenging approach to the construction of robust, thin film materials with large second-order optical nonlinearities is the covalent self-assembly of aligned arrays of high-β molecular chromophores into multilayer superlattices. In this paper, we describe the dispersion of second harmonic generation (SHG) in a self-assembled (SA) monolayer containing a stilbazolium chromophore. The frequency-dependent measurements were performed on 25 Å thick monolayers on glass using a tunable (0.4–2 μm) light source based on optical parametric amplification (OPA). The SHG spectrum contains a clear two-photon resonance at hω = 1.3eV. The maximum in the second-order susceptibility coincides with a low energy chromophore-centered charge-transfer excitation at 480 nm. The experimental SHG dispersion values compare favorably with theoretical results computed using a sum-over-states (SOS) formalism. However, the measured values exhibit a somewhat broader band response than the theoretical curve, and the origin of this behavior is discussed.


2013 ◽  
Vol 21 (7) ◽  
pp. 8916 ◽  
Author(s):  
B. Q. Yao ◽  
X. Yu ◽  
X. L. Liu ◽  
X. M. Duan ◽  
Y. L. Ju ◽  
...  

Sign in / Sign up

Export Citation Format

Share Document