Observation of Stimulated Emission in Short Wavelength Band from Silica-Based Superstructure Films

2009 ◽  
Vol E92-C (12) ◽  
pp. 1454-1459 ◽  
Author(s):  
Takehiko UNO ◽  
Satoru NOGE ◽  
Kei KASAHARA
2014 ◽  
Vol 176 (3-4) ◽  
pp. 363-369 ◽  
Author(s):  
P. Khosropanah ◽  
T. Suzuki ◽  
R. A. Hijmering ◽  
M. L. Ridder ◽  
M. A. Lindeman ◽  
...  

2000 ◽  
Vol 2 (1) ◽  
pp. 23-30 ◽  
Author(s):  
A. S. Tatikolov ◽  
Zh. A. Krasnaya ◽  
L. A. Shvedova ◽  
V. A. Kuzmin

Spectral and fluorescent properties of ketocyanine dyes (polyenic bis-ω,ω′-aminoketones) and cation-anionic polymethine dyes of various structures were studied. The symmetric ketocyanines were shown to have a long-wavelength absorption band bathochromically shifted in comparison with that of the asymmetric ketocyanines with the same total length of the polyenic chain. The nonlinear ketocyanines exhibit the additional short-wavelength band in their absorption spectra, which can be more intense than the longwavelength band. The absorption spectra of ion pairs of cation-anionic dyes with overlapping cation and anion bands contain a new intense short-wavelength band inactive in fluorescence excitation. These spectral peculiarities are explained on the basis of chromophore interaction model. It has also been shown that theT1levels of ketocyanine chromophores do not essentially interact with each other in a ketocyanine molecule in nonpolar solvents; in polar solvents this interaction becomes appreciable due to lowering the potential barrier for conjugation.


2012 ◽  
Author(s):  
P. Khosropanah ◽  
R. Hijmering ◽  
M. Ridder ◽  
J. R. Gao ◽  
D. Morozov ◽  
...  

1978 ◽  
Vol 8 (9) ◽  
pp. 1115-1118 ◽  
Author(s):  
G A Abakumov ◽  
M M Mestechkin ◽  
V N Poltavets ◽  
A P Simonov

1994 ◽  
Vol 339 ◽  
Author(s):  
I. Akasaki ◽  
H. Amano

ABSTRACTHigh-quality AlGaN/GaN and AlGaN/GalnN DHs were fabricated by MOVPE using low-temperature deposited AlN buffer layer. We applied the newly designed dual-flow-channel reactor, by which high-quality and well-controlled AlGaN and GalnN alloys and their heterostructures have been grown. AlGaN/GaN-DH shows low-threshold stimulated emission by optical pumping at room temperature for both edge and surface modes. The peak wavelength of stimulated emission for edge mode was 369.5nm. The peak wavelength of stimulated emission was affected by the strain due to heterostructure as well as the many body effect under high excitation. The wavelength for stimulated emission can be widely changed by using GalnN as the active layer. AlGaN/GalnN DH with InN molar fraction of the active layer of 0.09 shows room temperature low-threshold stimulated emission for edge mode by optical pumping with peak wavelength of 402.5nm. A few mW-class symmetrical AlGaN/GaN DH LED and anti symmetrical AlGaN/GalnN/GaN DH LED using low energy electron beam irradiation (LEEB1) treated Mg-doped P-AlGaN cladding layer were fabricated. These results show that column-Ill nitrides are promising for the realization of practical short wavelength LED and LD.


2006 ◽  
Vol 15 (03) ◽  
pp. 309-313 ◽  
Author(s):  
SULAIMAN WADI HARUN ◽  
CHENG XIAU SAN ◽  
HARITH AHMAD

A multi-wavelength Brillouin erbium fiber laser (BEFL) which operates in a short wavelength band (S-Band) is demonstrated using a depressed cladding erbium-doped fiber (EDF). Two 80/20 couplers were used in the system for internal feedback of generated stokes signal in order to produce cascaded Brillouin stokes for multi-wavelength operation. It generates an optical wavelength comb with spacing of approximately 0.084 m. A stable output laser of up to 7 lines was obtained with a Brillouin pump of 3.5 mW, a 980 nm pump laser of 200 mW and an EDF length of 20 m. The BEFL has the potential to be used in the future dense wavelength division multiplexing (DWDM) communication system.


2003 ◽  
Vol 58 (2-3) ◽  
pp. 109-117 ◽  
Author(s):  
V. I. Tomin ◽  
J. Heldt

The luminescence spectrum of laurdan in glycerol consists of two bands with maxima at 425 and 500 nm. The strong dependence of this spectrum on the energy of the excitation quanta is demonstrated. When, excited on the red-edge slope of the absorption band, it is investigated at various temperatures. The biggest red shift (about 10 nm) of λmax is found for the long wavelength band at low temperature, where the solvent forms a rigid matrix. A small shift, about 3 - 4 nm, and a change of the luminescence band shape occurs on increasing the temperature to 370 K. Simultaneously, intensity changes occur in the excitation spectra when the maximum intensity of the two emission bands is recorded. From the received data, the differential excitation spectrum has been determined. The additional absorption contributes to the luminescence of the short wavelength band. The deconvolution of the luminescence decay data obtained separately for the luminescence bands results in common components in the sub- and nanosecond time range with different participation. The experimental data testify the presence of an additional mechanism, responsible for the heterogeneity of the solution, which differs from the well-known solvent molecule reorientation. Torsion oscillation of the N(CH3)2 functional group in the laurdan molecule is necessary to take into account as well as the statistical properties of the laurdan solvate shells. The observed luminescence properties are explained taking into account the simultaneous existence of local-excited and charge transfer states in the solute molecules.


Sign in / Sign up

Export Citation Format

Share Document