S1 singlet excited-state absorption of DODCI

1 excited-state absorption cross-section spectrum of DODCI in ethylene glycol is determined in the wavelength range from 500 nm to 750 nm. The S₁ state is populated by amplified femtosecond dye laser pulses (wavelength 592 nm) and the S₁-state absorption and emission behaviour is probed with a femtosecond light continuum. A general analysis procedure is developed to extract absolute excited-state absorption cross-sections from the measured transmissions. For DODCI in ethylene glycol the wavelength regions of saturable absorption (mode-locking application), reverse saturable absorption (optical limiter application), and effective stimulated emission (laser application) are determined. Received: 25 July 1996     

Saturable absorption dynamics of DODCI

The saturable absorption dynamics of DODCI in a femtosecond dye laser is studied theoretically. The N-isomer and P-isomer photoisomerization dynamics is included. The wavelength region between 570 nm and 650 nm is considered where the N-isomer and P-isomer absorption dynamics changes from short-wavelength to long-wavelength s₀-s₁ excitation. The slow saturable absorber DODCI shortens a circulating pulse in a laser oscillator down to femtosecond duration if the gain medium compensates the absorber losses. Fast local relaxation in the S₁ -state in the case of short-wavelength excitation and fast level refilling in the S₀ -state in the case of long-wavelength excitation facilitate the pulse shortening and the background signal suppression.     

Saturable absorption and absorption recovery of indocyanine green J-aggregates in water

Received: 12 May 1997/Revised version: 22 October 1997     

Synchronous pulsed infrared detection in AgGaSe2 crystal using 1.318 μm pump

2 laser by nonlinear upconversion, is reported for the first time in AgGaSe₂ crystal under near noncritical phase-matching, pumped by an electro-optically Q-switched Nd:YAG laser operated at 1.318 μm. The capability for low-level infrared signal detection at room temperature with a fast response was also studied. Received: 15 December 1996/Revised version: 20 February 1997     

Ferroelectric domain inversion in near-stoichiometric lithium niobate for high efficiency blue light generation

LiNbO₃ single crystals with a composition close to stoichiometry ([Li]/[Li+Nb]=0.496), 16 mm in diameter and 40 mm in length were grown by the Czochralski method using K₂O flux. The domain reversal characteristics of near-stoichiometric LiNbO₃ single crystals were investigated. The switching field required for 180° ferroelectric domain reversal in the near-stoichiometric crystal at room temperature was 7.5 KV/mm. This is about one third of the switching field required for conventional LiNbO₃ crystals. Domain reversal (180°) in near-stoichiometric LiNbO₃ samples of 1.0 mm thickness has been achieved. Samples have been evaluated by second harmonic generation and conversion efficiencies of up to 32% have been obtained. Received: 8 November 2000 / Accepted: 29 January 2001 / Published online: 20 June 2001     

Photoluminescence effect of Ru dye on alumina membranes with ordered pore arrays

We have investigated the quenching luminescence and the luminescence mechanisms of self-assembled Ru(II)L₂X₂ (Ru(II)(4,4’-dicarboxyl-2,2’-bipyridyl)₂(SCN)₂) dye in porous anodic alumina. Porous anodic alumina can emit visible light due to numerous oxygen vacancies formed during anodic oxidation. Energy transfer from the porous anodic alumina to the dye molecules causes the quenching and red shift of the PL peak, which gives a fundamental understanding of the PL mechanism in porous anodic alumina. Received: 29 May 2001 / Accepted: 3 August 2001 / Published online: 30 October 2001     

Single-longitudinal-mode selection in a nanosecond-pulsed dye laser

We investigate the dynamics of the excited-state population, the cavity photon number, and the spectrum of an optically pumped nanosecond-pulsed dye laser containing bandwidth-narrowing elements in the cavity. We show that, in order to achieve single-mode operation, the pump-pulse duration has to be long enough and the dye concentration sufficiently high. This is partly due to the frequency shift of the laser spectrum during the decrease of the excited-state population towards its steady-state value. We demonstrate a single-mode dye laser, where single-mode selection is realised with the aid of an intracavity Fox–Smith interferometer. In this way we have obtained 5-ns-long pulses at the wavelength of 590 nm with a pulse energy of 6 mJ and a spectral width of 100 MHz (FWHM). Received: 3 December 2001 / Published online: 14 March 2002     

Self-stabilizing additive-pulse mode-locking due to thermo-optical non-linearity in an optical fiber

16 , 1671 (1991)] described a Nd:YLF APM laser which somehow automatically adjusted the relative resonator phase. We reproduce this behavior and analyse its origin. Thermal effects due to the light power guided in the fiber affect the effective fiber length, which in turn influences the phase and thus the power level; hence a closed servo loop results. We demonstrate this explanation to be correct in quantitative terms. Consequences arise for other systems involving fiber-optic loops or interferometers. Received: 7 April 1997/Revised version: 15 July 1997     

Photoisomer generation and absorption relaxation in the mode-locking dye 3,3'-diethyloxadicarbocyanine iodide

A quantum efficiency of ≈ 0.01 for the generation of the photoisomer of DODCI has been obtained. The establishment of equilibrium concentrations for the two forms of the dye in mode-locked rhodamine dye lasers has been confirmed. The measured saturable absorber recovery times of ≈ 200–250 psec are shown to be consistent with an excited state lifetime of ≈ 300 psec, in agreement with fluorescence measurements.     

Theory and experiment of CW dye laser injection locking and its application to second harmonic generation

High-power single-mode operation of a cw ring dye laser has been obtained by injection of cw single-mode radiation. The intracavity power of this system was used to generate tunable single-mode uv radiation by frequency doubling in a temperature phase-matched ADA crystal: up to 45 W intracavity fundamental power and up to 70 mW extracted uv power have been observed. A theoretical treatment of the injection locked cw ring dye laser system is given for the stationary state. Expressions for the intracavity intensities as a function of the small-signal gain and the saturation intensity are derived.     

Enhanced efficiency and extended wavelength range of dye lasers operated with DCM

It is observed that the efficiency of the DCM dye dissolved in ethylene glycol benzyl alcohol can be enhanced if the dye is preheated at a temperature of 150 °C. Peak powers as high as 1.5 W have been achieved with a single-mode ring dye laser at 640 nm when pumped by 9 W (all lines) from an argon-ion laser. The wavelength region has been also extended beyond both ends of the tuning curve compared to a conventionally prepared DCM dye. Received: 3 September 1999 / Revised version: 9 December 1999 / Published online: 23 February 2000     

Triple mode-locking of Ar+ and dye lasers

We report a new technique of generating highly synchronous simultaneous pulse trains at three wavelengths, two of which are continuously tunable over a moderate range. A series of oscillographs shows the time-resolved Ar⁺ pulses and the effects of varying the two cavity lengths with respect to each other. Preliminary correlation measurements indicate low jitter.     

Photo-stability of laser dye solutions under Copper-vapour-laser excitation

The photo-stability of laser dyes, Rhodamine-6G, Rhodamine-B, and Kiton-Red, under high repetition rate (6.3 kHz) Copper-vapour-laser (CVL) irradiation has been investigated. Exhaustive photo-bleaching of these dyes in different solvents has been carried out to study the extent to which the dye photo-degraded products would interfere with the lasing process in high-power CVL-pumped dye lasers. Our results indicate that the photo-degradation of dyes occurs predominantly through excited-state intermolecular reactions, involving the singlet state, rather than the process of nonlinear optical absorption in individual molecules. Received: 13 March 2000 / Revised version: 2 August 2000 / Published online: 21 March 2001     

Determination of molecular orientation in ultrathin liquid crystal. films on solid substrates using X-ray absorption spectroscopy

42 H₆₀O₆, HBT) deposited on a (111)-oriented Au single crystal and a polycrystalline indium tin oxide (ITO) substrate has been carried out using X-ray absorption spectroscopy. Films of thicknesses between 2 nm and 15 nm were prepared in UHV by evaporation of HBT [which exhibits a discotic liquid crystalline (LC) bulk phase] from a Knudsen cell. Thickness and composition of the HBT films were determined using X-ray photoelectron spectroscopy (XPS). For the thinnest films with thicknesses in the monolayer regime, the orientational analysis reveals a pronounced orientation of the disc-shaped HBT molecules parallel to the Au surface. For thicker films, a significantly reduced anisotropy is observed with the molecular plane oriented more normal to the Au surface. In the case of the ITO-substrates, no significant differences were observed between different thickn esses and the average orientation of the molecular planes was predominantly normal to the surfaces, as for the thicker films on the Au substrate. Received: 1 March 1997/Accepted: 24 April 1997     

Growth and absorption properties of Dy-doped and undoped p-type TlGaSe2

2 and Dy-doped p-TlGaSe₂ (p-TlGaSe₂:Dy)single crystals were grown by the Bridgman–Stockbarger method. Absorption spectra were measured on freshly cleaved (001) surfaces. The freshly cleaved crystals had a mirror-like surface and there was no need for mechanical treatment. The absorption measurements were carried out in p-TlGaSe₂ and p-TlGaSe₂:Dy samples in the temperature range 10–320 K with a step of 10 K. The phonon energies calculated in p-TlGaSe₂ and p-TlGaSe₂:Dy are 23.0 meV and 21.0 meV, respectively. The direct band gaps of p-TlGaSe₂ and p-TlGaSe₂:Dy are 2.279 eV and 2.294 eV at 10 K, respectively. There is an abrupt change for the energy peak for p-TlGaSe₂ in the temperature ranges 105–120 K, 240–250 K, and for p-TlGaSe₂:Dy in the temperature ranges 100–110 K, 240–260 K. Received: 3 December 1997 / Accepted: 5 October 1998     

Optical transient bleaching/absorption of surface-oxidized CuInS2 nanocrystals

2 nanocrystals in a polymer film have been studied with the picosecond pump-probe technique. The oxidized CuInS₂ nanocrystals have an additional absorption band with a peak at 1.03 eV, which is bleached under picosecond excitation. Rapid (∼50 ps) trapping into midgap surface states results in long-lived (≫300 ps) bleaching and induced absorption features. A schematical energy-level diagram for oxidized CuInS₂ nanocrystals is given based on the experimental results. Received: 7 January 1997/Revised version: 16 April 1997     

Laser intracavity absorption spectroscopy

Emission spectra of multimode lasers are very sensitive to spectrally selective extinction in their cavity. This phenomenon allows the quantitative measurement of absorption. The sensitivity of measurements of intracavity absorption grows with the laser pulse duration. The ultimate sensitivity obtained with a cw laser is set by various perturbations of the light coherence, such as quantum noise, Rayleigh scattering, four-wave mixing by population pulsations, and stimulated Brillouin scattering. It depends on the particular laser type used, and on its operative parameters, for example pump power, cavity loss, cavity length, and length of the gain medium. Nonlinear mode-coupling dominates the dynamics of lasers that feature a thin gain medium, such as dye lasers, whereas Rayleigh scattering is more important in lasers with a long gain medium, such as doped fibre lasers, or the Ti:sapphire laser. The highest sensitivity so far has been obtained with a cw dye laser. It corresponds to 70000 km effective length of the absorption path. The ultimate spectral resolution is determined by the spectral width of mode emission, which is 0.7 Hz in this dye laser. High sensitivity and high temporal and spectral resolution allow various practical applications of laser intracavity spectroscopy, such as measurements and simulations of atmospheric absorption, molecular and atomic spectroscopy, process control, isotope separation, study of free radicals and chemical reactions, combustion diagnostics, spectroscopy of excited states and nonlinear processes, measurements of gain and of spectrally narrow light emission. Intracavity absorption in single-mode lasers shows enhanced sensitivity as well, although not as high as in multimode lasers. Received: 10 May 1999 / Published online: 29 July 1999     

Fluorescence dynamics in Tm,Ho:YLF following 800 nm pulsed laser excitation

Received: 19 February 1997/Revised version: 4 April 1997     

Dependence of harmonic signals on sample-gas parameters in wavelength-modulation spectroscopy for precise absorption measurements

4 and N₂O, are given. Received: 4 March 1998/Revised version: 27 July 1998     

Detection of argon and krypton traces in noble gases by diode laser absorption spectrometry

Wavelength modulation, diode laser atomic absorption spectrometry is applied to measure traces of argon and krypton in other noble gases. Strong transitions from long-lived metastable levels highly populated in a low-pressure dc discharge are induced with a standard diode laser in the spectral range around 811 nm. The detection limits achieved are in the lower ppbv range, and the residual concentrations of Kr and Ar traces in the utilized high-purity noble gases are measured. Received: 2 October 2000 / Final version: 3 May 2001 / Published online: 7 June 2001