Effect of concentration on laser threshold of organic dye laser

The effect of concentration on laser threshold is examined theoretically and experimentally for Rhodamin B and Rhodamin 6G. Laser action is obtained in the region from 1 · 10^?6 mol to 2.5 · 10^?1 mol. Lasing in organic dye solutions which are excited by a pulslaser is possible in a broad concentration range. For high concentrations laser action is limited by fluorescence quenching and increasing losses (diffraction, thermal effects, and bleaching). For low concentrations the limit is given by the losses of the used experimental set-up. In the present work the influence of the concentration on the exciting intensity at laserthreshold is examined for Rhodamin B and Rhodamin 6G solutions.     

Quantum description of free electrons in the laser

The fully quantum mechanical theory of the free electron laser is formulated in the moving frame introduced by the authors. The laser and wiggler fields are taken to be at their classical limit and quantum effects of the electron motion are considered. The Schrodinger equation is written down and solved for the unsaturated gain and momentum distribution. The results are found to be closely related to the corresponding expressions from a fully classical theory.     

Quantum theory of laser cooling: Statistical description of the process dynamics

A dynamic theory of coherent X-ray radiation generated in a periodic layered medium by a relativistic electron multiply scattered by target atoms has been developed. The expressions describing the spectral–angular characteristics of parametric X-ray radiation and diffracted transition radiation are derived. Numerical calculations based on the derived expressions have been performed.     

Characteristics of a multicolor dye laser

An experimental investigation on the possibility of obtaining tunable, multiple wavelength output in mixture of dyes pumped by a nitrogen laser has been carried out. A great number of binary dye mixtures have been tested. Simultaneous two wavelength operation is generally possible provided the gain profiles of both dyes are neither strongly overlapped nor too widely separated. Three color emission is feasible in many mixtures, but the possible combinations are limited. A simple scheme for multiple, simultaneous wavelength tuning is presented.     

Rapid tuning of a dye laser

An electrooptically tunable Lyot filter was inserted into a dye laser resonator as a first stage element. The laser emission was tuned with a speed of 35 nm/μsec over a wavelength range of 20 nm.     

Infrared dye laser excited by a diode laser

A waveguide dye laser with an inner diameter of 30 μm and a length of 1.0 nm has been excited with a pulsed GaAlAs diode laser. The infrared-absorbing dye 5,5′-dichloro-11-diphenylamino-3,3′-diethyl-10,12-ethylenethiatri- carbocyanine perchlorate was used in tetramethylene sulfoxide solution. By changing dye concentration, laser wavelengths from 950 to 1005 nm were obtained.     

A picosecond dye laser tunable in the 1.1μ m region

We report in this letter the characteristic of a picosecond dye laser, tunable in the 1.08–1.12 μm range. The dye is pumped by the fundamental of a mode-locked Nd-YAG laser. The energy conversion efficiency is higher than 10% and the pulse duration is less than 10 ps.     

Energy transfer dye mixture for argon-pumped dye laser operation in the 700 to 800 nm region

The tunable wavelength region for argon-pumped dye lasers is extended to 805 nm using a binary energy transfer dye mixture. Efficiency as high as 13% was observed at the peak wavelength of 730 nm.     

Quantum theory of dye lasers

A quantum model of dye laser is given. To account for triplet losses a six levels model for the molecular system is assumed. The solution of generalized von Neumann equation in thermodynamical limit leads to a system of kinetic equations. Stationary solutions of this system are discussed. There are two distinct types of dependence of photon number versus pumping parameter. Beside a usual one, a new dependence characteristic for dye lasers only is present. In this case the definition of threshold should be revised.     

Color center laser pumped with a DCM dye laser

A CW, DCM dye laser has been used to pump a RbCl:Li crystal in a color center laser. The DCM dye laser was pumped by the 488 nm and 514.5 nm lines of an argon ion laser. When used in a broad band configuration the dye laser had a power output in the TEM₀₀ mode in excess of 600 mW at a wavelength of 655 nm. An output power in excess of 10 mW at 2.73 μm was possible from the RbCl:Li crystal in a Burleigh FCL for an input power of 600 mW at 655 nm. This method of pumping for the RbCl:Li alleviates the need for both argon ion and krypton ion laser pumps for the Burleigh FCL. All three crystals can be pumped to the specification power levels with a single argon ion laser.     

Quantum threshold group signature

In most situations, the signer is generally a single person. However, when the message is written on behalf of an organization, a valid message may require the approval or consent of several persons. Threshold signature is a solution to this problem. Generally speaking, as an authority which can be trusted by all members does not exist, a threshold signature scheme without a trusted party appears more attractive. Following some ideas of the classical Shamir’s threshold signature scheme, a quantum threshold group signature one is proposed. In the proposed scheme, only t or more of n persons in the group can generate the group signature and any t − 1 or fewer ones cannot do that. In the verification phase, any t or more of n signature receivers can verify the message and any t − 1 or fewer receivers cannot verify the validity of the signature. Supported by the National Basic Research Program of China (973 Program)(Grant No. 2007CB311100), the National High-Technology Research and Development Program of China (Grant Nos. 2006AA01Z419 and 2006AA01Z440), the Major Research Plan of the National Natural Science Foundation of China (Grant No. 90604023), the Scientific Research Common Program of Beijing Municipal Commission of Education (Grant No. KM200810005004), the Scientific Research Foundation for the Youth of Beijing University of Technology (Grant No. 97007016200701), the Doctoral Scientific Research Activation Foundation of Beijing University of Technology (Grant No. 52007016200702), the ISN Open Foundation, and the National Laboratory for Modern Communications Science Foundation of China (Grant No. 9140C1101010601)     

Color center laser pumped by a flashlamp-pumped dye laser

A reliable, pulsed, color center laser is described which provides a pulse energy up to 0.4 mJ in a wavelength range from 2.4 μm to 3.3 μm at a bandwidth below 20 GHz. A simple, broadband, flashlamp-pumped dye laser is used as the pump source. A new transverse pumping scheme of F-centers is described using hydrogenated color center crystal which allows to pump color center lasers with high energy pump pulses.     

Continuous wave dye laser pumped by a HeNe laser

Continuous wave operation of a dye laser pumped at 633 nm by a HeNe laser is reported. A jet of a cooled solution of Oxazine 1 in ethanol was used as the laser medium in an asymmetric spherical cavity. With mirrors of high reflectivity a threshold as low as 10 mW could be achieved.     

Photophysical properties and laser characteristics of a new rigid aminocoumarin dye lasing in the blue-green region

The photophysical properties of a new dye, 7-Diethyl AminoCoumarin with a Rigid substitution in the 3-position (referred to as DARC) have been studied in three solvents: dioxane, DMF and DMSO. The dye has been found to have a fluorescence quantum efficiency (_fl) between 0.40 and 0.80 in these solvents. The dye-laser performance of this dye has also been investigated in dioxane, DMF and DMSO, under nitrogen-laser pumping and compared with that of the commercially available standard laser dye, Coumarin 515 (C-515). A tuning range of nearly 70 nm was obtained in the blue-green region with an efficiency up to 80% of that of the standard dye. The observed characteristics of the dye are explained in terms of the sructural rigidization of the dye in the 3-position which inhibits the formation of the Twisted Intramolecular Charge Transfer (TICT) conformation in the excited state leading to an enhancement of the _fl and a considerable improvement in the laser performance.Research carried out at U.D.C.T., Bombay, India     

Optimization of a long pulse dye laser

The development of the thermal lens in a 60 μs long pulse dye laser is described. The use of a resonator with a spherical mirror permits to obtain reliable output pulses at a conversion efficiency of 0.3%.     

Modeling a distributed feedback dye laser pumped by a Nd-glass laser

A mathematical model has been developed to describe the dynamic emission of a distributed feedback dye laser (DFDL) pumped by a Nd-glass laser. The model is based on the coupled-wave theory. It allows the investigation of the temporal behavior of the Nd-glass pumping laser source and the DFDL pulses. The model allows studying the effect of the variation of the laser input parameters of the Nd-glass laser, such as maximum amplification coefficient, loss coefficient and pumping rate on the characteristics of DFDL pulses regarding the pulse width, delay time and separation time. The feedback process of the DFDL is provided either by changes of the refractive index or by optical gain or by both together. The model estimates the following: temporal behavior of the density of emitted radiation, energy densities of the first excited singlet and triplet states, DFDL output power, cavity decay time and the temperature of the produced grating. The numerical solution of the nonlinear coupled rate equation system predicts the generation of DFDL picosecond pulses. The calculated results are in good agreement with the available experimental data. The calculations were done using rhodamine 6G dissolved in ethanol as the investigated matrix.     

Generation of nearly transform-limited pulses in subnanosecond region with TEA nitrogen-laser-pumped dye laser

A dye laser is transversely pumped by a TEA nitrogen laser with 700 ps duration. The dye laser pulse has a spectral linewidth of 0.007 nm and a pulse width of ≈ 140 ps, giving a time-bandwidth product of 1.5. It is pointed out that the fluorescence lifetime of the laser dye plays an important role in generation of laser emission using a long laser cavity under subnanosecond pulse pumping.     

Dynamics of a random laser above threshold

We have performed enhanced backscattering experiments in a high gain random laser, under circumstances where a stationary theory predicts the laser intensity to diverge. Above the laser threshold the observed backscatter cone changes only gradually, not showing any signs of the divergence. We present measurements and theory-generalized laser equations with a diffusive transport term for pump and laser light-to explain the observed behavior. The population dynamics prevent an indefinite growth of the intensity. Time dependence is essential for a theory of random lasers above the laser threshold.