Search

The focused beam of a pulsed CO/sub 2/ TEA laser was used to photodissociate ethylene gas at total pressures of 100 to 300 torr. The laser pulse induces molecular hydrogen elimination to yield primarily C/sub 2/H/sub 2/ and H/sub 2/ in a large excess of helium to eliminate heating. An investigation was made of the dependence of product yield on wavelength, inert gas pressure, ethylene pressure and intensity. Photochemical yield was followed over a 10,000 fold range. Its dependence was investigated employing alternate methods of focusing the laser beam, one of which results in a constant volume geometry. A photometric method of characterizing this focal zone is described. A ''structureless'' computer model of the laser pumping process involving coupled rate equations and phenomenological absorption and stimulated emission coefficients is described. The model assumes rapid intramolecular energy transfer between the various vibrational modes throughout the entire vibrational manifold, and rapid equilibration of rotational states. The model includes stimulated emission and deactivating collisions, and predicts a product yield versus intensity dependence that does not exhibit threshold behavior in agreement with experiment. Calculated dependences of product yield on laser power for various parameters are given in order to relate the model to variousmore » photolysis experiments.« less

The investigation results of TEA – Xe laser operating at pulse repetition rates up to 2 kHz are presented. The influence of macro- and microinhomogeneities of the volume discharge plasma and gas-dynamic processes in the near-electrode layers on the ignition frequency of the volume discharge and the average radiation power level was determined. In TEA-Xe laser with an active volume of V A = 42×1,8×0.5 cm3 at a pulse repetition rate of 1.2 kHz the maximum value of the average radiation power of 2.8 W was reached.

In this paper different stage of pulse charging circuit (Blumlein circuit) was design. The laser system consist of different dimension printed board act as capacitor, fast spark gap switch and two parallel electrode made of Brass. TEA Nitrogen laser produce UV radiation with 337.1nm. the basic design contain two capacitor with one spark gap while, fourth design consist of four spark gap with five capacitor. As the number of stage rise the overvoltage required for breakdown increase so we can obtain gas discharge and excitation of Nitrogen molecules at lower voltage. The maximum energy obtained for OSBC was 1.02 mJ at 25 KV with laser pulse width around 8 ns. The last design with four stage blumlein circuit the energy raised to higher value more than for last design, the maximum energy was 19.01mJ at 25 kv with pulse width around 4.6 ns.

In this work, we estimate the potential of a cryogenic far IR radiation detector for registering the energy release by the amount of a substance desorbed upon its exposure to far IR quanta. The temperature invariability of the system at the first-order phase transition excludes the diffusion character of heat transfer processes, which contributes to the detector’s speed of operation and, according to our estimates, enables its use in pulsed location systems based on a CO2 TEA laser. As an example of another cryogenic detector, we consider an antiferromagnetic, where the speed of operation is provided by the resonance transfer of far IR quantum energy to the spin system, the sublevels of which are split by a strong (∼1,000 T) exchange field. The magnetic response arising in this case is registered by a quantum magnetometer based on the Josephson effect.

Ge15Se77Sb8 chalcogenide thin films having thickness 300 nm were grown on glass/Si wafer by vacuum evaporation technique and induced by Transverse Electrical Excitation (TEA) laser for 10, 20 and 30 min. The synthesized Ge15Se77Sb8 chalcogenide exhibited the glassy as well as amorphous nature, as evidenced in differential scanning calorimetry measurements. TEA laser irradiation on Ge15Se77Sb8 thin films showed the polycrystalline nature while the as-prepared thin films were in amorphous nature. The optical band gap of as-prepared and laser irradiated films were determined by measuring the optical absorbance with photon energy. An increase in absorption coefficient and extinction coefficient was observed while the decrease in optical band gaps with laser irradiation time was demonstrated.

George Stout investigated radiation ablation as a means of erasing white paint stripes (applied to facilitate realignment) from Philae Temple sandstone blocks after their reassembly on the island of Agilkia. Forty-two years ago state-of-the-art laser technology offered very few options in terms of diversity in wavelengths and pulse lengths. Laser divestment in art conservation had only been demonstrated for black sulfate encrustations on white calcareous stones. However, a CO2 IR (10.6 µm) TEA laser from an inertial-confinement thermonuclear fusion program was available and had been employed to ablate white tufa deposits from brown Cyprian pottery shards. Consequently, Stout adapted the heat-transfer analytical modeling of a concurrent laser divestment project in Venice to white paint upon brown sandstone, characterizing the Philae situation to guide TEA-laser divestment tests on the white-striped Isis stones. In contrast to results obtained with radiation from Nd:YAG, Nd:glass, and ruby lasers, the mid-i...

The design, development and operational characteristics of a compact corona pre-ionized helium-free TEA CO2 laser is discussed. Remarkably high efficiency of about 19% was obtained in this laser, which is attributed to the optimum concentration of CO2 and N2 gas, reduction in energy dissipation in the pre-ionization loop and the switch, minimizing the diffraction losses and finally optimization of the output coupler reflectivity. The helium-free TEA CO2 laser has also been analysed using a comprehensive theoretical model, developed based on the Boltzmann transport equations and the discharge excitation circuit equations. The voltage and current waveforms of the pulsed discharge were simulated and used as input to the laser rate equations to estimate the laser pulse energies and the pulse shapes. The theoretical estimations of the laser pulse energy agree fairly well with the experimental results. The accuracy of our theoretical model becomes evident from the numerically evaluated laser pulse shapes, which show remarkable resemblance with the experimentally measured pulse shapes. A detailed comparison with the helium-rich case is included to highlight the key aspects of a suitably designed helium-free TEA laser.

A carbon dioxide (CO2) transverse electrical breakdown in atmosphere (TEA), pulsed laser was used to enhance the laser-induced breakdown spectroscopy (LIBS) spectral signatures of uranium under nanosecond (ns) and femtosecond (fs) ablation. The peak areas of both ionic and neutral species increased by one order of magnitude for ns-ablation and two orders of magnitude for fs-ablation over LIBS when the CO2 TEA laser was used with samples of dried solutions of uranyl nitrate hexahydrate (UO2(NO3)2·6H2O) on silicon wafers. Electron temperature and density measurements show that the spectral emission improvement from using the TEA laser comes from plasma reheating.

The ablation of coatings (paint, varnish, oxides, etc.) using a pulsed laser beam is a process that has a number of major benefits compared with conventional cleaning techniques (mechanical and chemical), the main advantage being the possibility of removing the surface layer without any risk of damaging the substrate. Another benefit, and certainly not the least, is the non-use of toxic solvents or chemical products that are difficult to eliminate and, in any case, will be banned from use in the near future. However, it must be stressed that, notwithstanding the above benefits, laser ablation of painted surfaces can only give good quality results if the process is properly controlled. The procedure discussed in this paper has two aims: the first involves establishing a thermal model of the interaction, applied to the ablation of paint from metal surfaces by infra-red laser. The second involves proposing an optimised paint removal process validated by experimental measurements. This second objective will be based on an analysis method of the acoustic signal transmitted by the ablation plasma beam.

Laser Ultrasonic Testing (UT) is an important technique for the non-destructive inspection of composite parts in the aerospace industry. In laser UT a high power, short pulse probe laser is scanned across the material surface, generating ultrasound waves which can be detected by a second low power laser system and are used to draw a defect map of the part. We report on the design and testing of a transversely excited atmospheric pressure (TEA) CO 2 laser system specifically optimised for laser UT. The laser is excited by a novel solid-state switched pulsing system and utilises either spark or corona preionisation. It provides short output pulses of less than 100 ns at repetition rates of up to 1 kHz, optimised for efficient ultrasonic wave generation. The system has been designed for highly reliable operation under industrial conditions and a long term test with total pulse counts in excess of 5 billion laser pulses is reported.

We constructed a TEA laser which consists of spark gap, pulse type high voltage power supply, Blumlein transmission line circuit, laser tube with Ernst electrode. We observed the self-preionization with an optical fiber in the spark gap and laser tube. The higher voltage power supplied to the Blumlein transmission line circuit, the better preionization was. An U-type transformer yielded better stability and output power than an I-type transformer. The discharge time after triggering a spark gap for the U-type transformer was also short. We obtained the stability of and output power of when the optimum conditions of the laser operation were spark gap distance of 6.0 mm, electrode distance in laser tube of 5.0 mm, gas flow rate in spark gap of 1500 cc/min, gas flow rate in laser tube of 4 /min, output window reflectivity of and repetition rate of 10 Hz.

A reliable procedure for remote high-accuracy laser detection of N 2 O as one of the principal destroyers of the protective ozone layer of the Earth has been developed. The procedure is based on using a CO 2 -laser system emitting efficiently in the ∼4.5 μm range. In this case lasing from isotopic modification 12 C 18 O 2 of carbon dioxide with its subsequent frequency doubling by a nonlinear crystal is used. With the object of reducing the price the composition of the active medium (both for TEA laser and low-pressure longitudinal-discharge-excitation laser) has been optimized. New high-efficiency intracavity frequency doubling schemes based on nonlinear AgGaSe 2 crystals have been developed for CO 2 -lasers of both types. Low concentrations of N 2 O and concentrations of the principal background gases CO and H 2 O have been measured under real atmosphere conditions with the aid of the lidar complex built around these lasers.

The experimental results on the laser-supported directed-energy "air spike" (DEAS) in hypersonic flow are presented. A CO 2 TEA laser has been used in conjunction with the IEAv 0.3-m Hypersonic Shock Tunnel to demonstratethe laser-supported DEAS concept. A single laser pulse generated during the tunnel useful test time was focused through a NaCI lens ahead of an aluminum hemisphere-cylinder model fitted with a piezoelectric pressure transducer at the stagnation point. In the more recent experiments, a double Apollo disk model fitted with seven piezoelectric pressure transducers substituted the simple hemisphere-cylinder model. The objective of the present research is to corroborate the past results as well as to obtain additional pressure distribution information.

The infrared multiphoton dissociation (IRMPD) of pure SiF4 and in mixtures with different gases was studied using a tunable CO2 TEA laser. The initial dissociation step of the IRMPD of SiF4 was found to be the decomposition into SiF3 and F. The gas phase reactions of trifluorosilyl, SiF3, with F and H2 was investigated. A kinetic scheme was proposed to explain the experimental results. The set of coupled differential equations associated to this scheme was numerically solved. The rate constants of the SiF3+F→SiF4 and SiF3+H 2→SiF3H+H reactions were determined. Fil: Alcaraz, A. N.. Universidad de Buenos Aires. Facultad de Ingeniería. Departamento de Física; Argentina Fil: Codnia, Jorge. Consejo Nacional de Investigaciones Científicas y Técnicas. Instituto de Investigaciones Científicas y Técnicas para la Defensa. Centro de Investigación en Láseres y Aplicaciones; Argentina Fil: Azcárate, María Laura. Consejo Nacional de Investigaciones Científicas y Técnicas. Instituto de Investigaciones Científicas y Técnicas para la Defensa. Centro de Investigación en Láseres y Aplicaciones; Argentina

An extra-cavity CO2-TEA laser pulse clipper for high spatial resolution atmospheric monitoring is presented. The clipper uses pulsed high voltageto facilitate the breakdown of the gas within the clipper cell. Complete extinction of the nitrogen tail, that degrades the range resolution of LIDARS, is obtained at pressures from 375 up to 1500 Torr for nitrogen and argon gases whereas an attenuation coefficient of almost 102 is achieved for helium. Excellent energy stability and pulse width repeatability were achieved using high voltage pre-ionized gas technique.

Laser induced breakdown spectroscopy (LIBS) was used for the analysis of Ca in a soil depth profile of Patagonia (Argentina), using a CO 2 TEA Laser and solid pellets of the soil in a BaCl 2 matrix. The experimental set-up allowed for the simultaneous observation of the emission lines in the range 390–420 nm, corresponding to Ca(II) and Ba(II), so that the intensity ratio I (Ca)/ I (Ba) could be measured to obtain a calibration curve, rather than I (Ca) alone. The results of the ablation could be interpreted with an evaporation model and non-stoichiometric conditions. The experimental variables such as laser energy, number of pulses averaged, and Ca concentration in the pellet were evaluated in order to find the best conditions for the analysis. The samples were obtained at variable depths (from 0 to 18 m) and analyzed to measure the total Ca and the acid soluble Ca. These results were compared with those obtained with the standard techniques.

Laser ablation of Upilex-S polyimide films 80 μm thick was performed in air using a pulse TEA CO 2 laser with wavelength 9.3 μm. A halo surrounding the hole was observed, which is covered with sub-micro particles. Pieces of ablation products protrude from the ablated surface, leading to considerable roughness of the ablated area. Chemical and structural changes of Upilex-S polyimide film surface irradiated by the pulse TEA CO 2 laser in air were analyzed by X-ray photoelectron spectroscopy (XPS). Relative C content in the ablated area was found to be higher, whilst both O and N contents were lower than in the untreated area. This means that TEA CO 2 laser ablation released both the O and N atoms. Also, the peak areas corresponding with carbonyl group (CO) in the imide system were reduced much more and a new component at 287.0 eV assigned to the amide structure (NCO) was detected after laser ablation. These suggest that the pyrolysis of the Upilex-S polyimide was the decomposition of the imide ring between the nitrogen/aromatic carbon atom and carbonyl carbon atom. In addition, another new component arising from >CO groups was also detected for higher fluence (7.83 J/cm 2 ), and its peak areas is very small. This result indicates that the slight oxidation may take place with higher fluence during laser ablation in air. Based on above-mentioned experimental results, a possible thermally-induced decomposition path of Upilex-S polyimide ablated by TEA CO 2 laser is presented.

This paper describes numerical and analytical studies on the optimization of the ultra-broadband infrared (IR) source, a novel high average-power device. The main objective of current studies was the reduction of weight, size, and cost of the system by devising a scheme to generate the two closely spaced radiation lines with a single laser driver instead of the two CO/sub 2/ transversely excited atmospheric pressure (TEA) lasers envisioned in the initial work. By inducing the modulation instability in nonlinear media, we have obtained as good or better results as in our previous studies but with one of the TEA lasers replaced by a very low-power driver that provides the seed radiation for the excitation of the instability. Even more importantly, we have demonstrated that the second high peak-power TEA laser can be replaced by a compact, light weight, low peak-power driver by focusing the radiation to a tighter spot. The average power of the source is maintained at the previous level by operating at higher duty factor. In the new low-peak-power operating regime, the output spectrum is very similar to that of the high-power regime, provided that the ratio of the peak power to the nonlinear length that scales proportionally to the area of the laser spot remains fixed.

The pulsed laser deposition (PLD) technique is frequently applied to synthesize carbon nitride coatings having a general formula CNx. In previous experiments, the polycrystalline CNx films were deposited with the use of a CO2 TEA laser in a remote nitrogen atmosphere [1] . The x value was found to be approximately 0.6 and the grains, observed with SEM, were typically of a few hundreds of nanometers of size. This phenomenon was tentatively explained by the abundance of vapors generated by the action of the laser. It can be, in turn, related to the thermal fields in the graphite target. The numerical code ‘Fusion-2D’, describing laser/target interaction, was applied to model the temperature in two dimensions. The optical absorption data were taken for the wavelengths that corresponded to the typical lasers used in PLD processes, i.e. excimer, YAG and CO2. The evolutions in the graphite target temperature at the pulses generated by these lasers were then calculated for a given power density. The differences in these evolutions were related to the volume of produced vapors and helped to explain the morphology of the synthesized films.

Quasi-simultaneous laser action in the UV (0.337 μm ) and the IR (10.6 μm ) was observed from a pulsed laser with a sliding discharge plasma cathode. The laser operates at atmospheric pressure, with a gas mixture of CO2/N2/He, at a 0.26/0.50/4.0 l min −1 flow rate. Output energies of 30 mJ in the IR and 0.35 mJ in the UV were obtained, from a laser discharge volume of 38.0×1.0×2.8 cm 3 . The optimum gas mixtures have been determined and the temporal behavior of the discharge parameters, the performance characteristics of the laser and the beam spatial distributions were investigated.

13C-Selective infrared multiple photon decomposition of lactone compounds has been studied using a CO2 TEA (transversely excited atmospheric) laser. The main decomposition products were ethylene and CO2 in β-propiolactone. We obtained CO2 with a 13C atomic fraction of 55% in the irradiation of 2 Torr (1 Torr = 1 mmHg = 133.322 Pa) β-propiolactone at 1035.47 cm-1. The addition of 100 Torr of N2 to 2 Torr of β-propiolactone resulted in a remarkable increase in selectivity, i.e., 75% 13C in CO2, while the yield was considerably decreased. Respective olefinic products were propylene and allene in the multiple photon decompositions of β-butyrolactone and diketene. The common product CO2 was also found to be significantly enriched with 13C in these lactone compounds.

Dehydrochlorination of 1,2-dichloropropane (DCP) was conducted by thermal elimination and CO2 laser-induced dielectric breakdown, which was induced by focusing the 10.6 μm lines of a CO2 TEA laser. Thermal dehydrochlorination proceeded by a four-centered mechanism at > 425 °C and by a surface-catalyzed radical process at 2000 °C.

Five and six-temperature models for the CO 2 –N 2 –He system are used to describe the process of the dynamic emission in the TEA CO 2 laser. All physical constants and relaxation rates related to these models are examined to estimate the output pulse parameters as a function of the input parameters. The two pumping processes implemented; empirical function and differential equation show a good agreement with the experimental data.

The operation characteristics of a two-stage Blumlein circuit (TSBC), which can increase the output energy of a TEA- laser by 100% without embarking on spark-gap miniaturization, are investigated using a discharge-coupled circuit model. This circuit model predicts that a TSBC can produce a laser-channel breakdown voltage of up to , as compared with computed for a one-stage Blumlein circuit (OSBC), where is the charging voltage. Although the gain in the breakdown voltage is only 25%, it significantly increases the laser-channel current and input power which, when compared with computed values for an OSBC, are enhanced by 2.3 and 2.6 times respectively. The computed input power, as a function of , is correlated to that of the measured laser output.

X-ray photoelectron spectrometry (XPS) has been used to observe the changes in surface chemistry during the removal of paint from a zinc coated steel substrate by means of TEA-CO2 laser ablation. Laser ablation at both plasma and sub-plasma fluences is investigated and their relative merits are discussed. The laser is shown to be an effective tool for removal of the bulk of the paint layer and is not impaired by evidence of ageing in the paint. Evidence for a very thin layer of organic compounds present on the surface after cleaning at sub-plasma fluences has been found, although these can be removed at plasma fluences.

For the removal of material with pulsed laser radiation the distance travelled by the shock or blast wave and the amount of energy released in the plasma state due to the absorption of laser radiation are determined experimentally and theoretically. The distance travelled by the blast wave is detected by schlieren photography, the released energy by monitoring the transmitted laser radiation during the removal process. The theoretical evaluation is performed by numerical simulation using a model incorporating the laser-induced vaporization process and the dynamics of the plasma state. The results obtained from the experiments and the model are compared with that of the Sedov - Taylor scaling. The removal of the oxide layer from austenitic steel is investigated with laser radiation produced by a TEA and a high-power laser device. For the TEA laser with fluences of 5 and 10 J 50 - 80% of the pulse energy is released into the plasma state and the Sedov - Taylor scaling describes the distance travelled by the blast wave in agreement with data from the experiments and the simulation. For the high-power laser with a fluence of 50 J , 6% of the pulse energy is released into the plasma state and the Sedov - Taylor scaling does not describe the data of the simulation. The process of removal of copper and aluminium material is simulated for excimer laser radiation with fluences of 15 and 30 J . For copper 15 - 30% of the pulse energy is released into the plasma state and the Sedov - Taylor scaling is applicable. For aluminium, less than 2% of the pulse energy is released into the plasma state and the Sedov - Taylor scaling is only applicable for the higher fluence.

Simultaneous laser action from HF and N/sub 2/ is obtained, from a plasma cathode TEA laser, for the first time. The sliding discharge along the surface of a dielectric is used as a plasma cathode, for the main volumetric discharge. The laser operates at atmospheric pressure, with a gas mixture of SF/sub 6/:C/sub 3/H/sub 8/:N/sub 2/:He. For a typical flow rate ratio of 0.27:0.024:0.2:19.8 1 min/sup -1/, it produces simultaneously 160 mJ HF and 0.6 mJ N/sub 2/ laser outputs at 0.43% and 1.4/spl times/10/sup -3/% efficiencies respectively, at the moderate charging voltage of 28.5 kV. These output characteristics are obtained from a small active discharge volume and length of 10/sup 6/ cm/sup 3/ and 38 cm respectively. These values extend the performance, recently reported in the literature, of a sliding discharge HF/N/sub 2/ laser with corresponding simultaneous energy outputs of 12 mJ HF and 1.1 mJ N/sub 2/, to a higher energy output level, thus making the device suitable for a broader range of applications. This novel dual wavelength HF/N/sub 2/ laser system presented, can be particularly convenient for medical experiments, where the IR beam can be used for tissue ablation, while the UV beam can be used as the excitation source for fluorescence spectroscopic measurements, for the evaluation of the ablation process. Details are presented on the dependence of the laser performance parameters, such as output energy, discharge voltage and current and structure of the laser output pulses on the mixture composition and the circuit parameters.

We report an experimental investigation of the absorption and ablation characteristics of the high-temperature polymer Upilex polyimide, using a line-tunable TEA laser. It is demonstrated that excellent quality through-holes (vias) can be produced in thin films of Upilex when the laser is tuned to a strongly absorbed wavelength as a result of thermal decomposition produced by laser heating of the bulk polymer. For weakly absorbed wavelengths, transmission and probe beam deflection measurements reveal an incubation effect in the ablation which is thought to be related to particulate contamination in the film.

The capacity of the CO2 TEA laser beam to ablate caries in dentistry is discussed. We conducted in vitro and in vivo tests on dogs and primates, respectively, to determine the efficacy of ...

Construction of powerful and efficient laser sources, lasing in various IR ranges, is of importance for further development of a number of trends, e.g., spectroscopy, laser chemistry, sounding of the atmosphere, and metrology. The most natural way to solve this problem is to use unconventional (nontraditional) transitions to produce lasing in commonly used CO2 lasers. The spectral range of CO 2 lasers is greatly increased in lasing on transitions of the so-called "hot" band 0111-1110, whose P-branch is in the range of 10.9-11.3 µm. Thorough investigations of gain, vibrational temperatures (T1, T2, T3), and output parameters on lines of the hot band made it possible to achieve efficient lasing both for pulse TEA and for cw longitudinal-discharge CO2 lasers. In studying the lasing spectrum of hot transitions in TEA CO2 lasers some lines not belonging to the 0111-1110 band. We suggested, that these lasing lines belong to higher level transitions, e.g., 1001-2000 (0400), which were called "doubly hot," i.e., transitions in which compared to hot transitions two deformation quanta or one symmetric quantum rather than one deformation quantum is added both to the upper and to the lower energy level. In the present work lasing in both a TEA laser and a low-pressure laser with longitudinal discharge on some transitions of the CO2 molecule in the range of 11.0-11.6 µm is reported. The rather high resolution of the spectral equipment used and calculation of transition frequencies on the basis of recent spectroscopic constants made it possible to identify definitively the lasing lines obtained as belonging to the doubly hot bands 0221-1220 and 100l-2000 and the sequence hot band 0112-1111. To find optimum conditions for lasing on the aforementioned bands experimental studies of vibrational temperatures in active media of a TEA CO2 laser and a low-pressure laser with long itudinal discharge were carried out. Earlier the lasing on the 0200(1000)-0110 band of the CO 2 molecule has been obtained in the specific systems at cryogenic temperatures under the lowest efficiency. The optimization of the active medium and its electrical discharge pumping conditions based on the original technique of the temperature model allowed to obtain in the simple TE CO2 laser with UV preionization the powerful lasing on the 0200-0110 band at room temperature. The dependencies of the output and spectral performances of the 16 (14) micrometers lasing vs. a content of the active medium, pumping parameters and cavity characteristics have been carried out. To increase the power performances of the 16 (14) microns CO2 laser the possibility of lasing on the 0201(1001)-0111 band have been experimentally and theoretically investigated under the combined (electrical + optical) excitation of the active medium. The conditions for

HfO2 and Y2O3 films for optical applications are prepared by excimer laser ablation and CO2 TEA laser evaporation, respectively. The growing films are bombarded with oxygen ions of 150 to 550 eV energy and several 10 to 250 μA/cm2 ion current density. Films of both materials deposited at relatively low ion bombardment possess high refractive indexes approaching those of the corresponding bulk. These films are of amorphous structure and have a high packing density with low porosity. Increasing ion bombardment, i.e. increasing ion energy and current density, leads to a marked decrease in refractive index and hence in the packing density due to increasing crystallization within the films. In the case of hafnia, for example, the refractive index at 600 nm wavelength decreases from 2.15 down to 1.80. Using appropriate deposition parameters hafnia and yttria films, with both high and low refractive index, showing low absorption and high laser damage thresholds at 1.06 μm wavelength can be prepared.

Stable and repetitive single-longitudinal-mode output from a pulsed TEA carbon dioxide laser has been achieved using a time-gated gain cell. The gain cell is operated as an oscillator for the time periods between the laser pulses. Before the TEA laser is triggered, the gain cell is rapidly switched below threshold to avoid saturation of the gain-switched spike in the TEA laser pulse. Standard dither-stabilization techniques can be used during the CW operation of the gain cell to position the output coupler for single-mode operation. This method for obtaining single-mode output from a pulsed TEA laser is completely automatic and very straightforward to implement.

Using controlled feedback and coincident far infrared absorption, we have shown that the superradiant emission process in NH 3 pumped by the 9R16 line of a CO 2 TEA laser has a marked effect on the absorption of laser energy and vibrational heating of the gas. Since many polyatomic molecules pumped by IR laser are efficient superradiant far infrared sources, the effect is important for laser induced fluorescence studies in these polyatomics.

The potential of InSb as a material for limiters for CO 2 laser pulses is explored. A model of the nonlinearity is presented and material parameters estimated from Z-Scans and ring-scans. This is then used to model the performance of a basic thin-sample defocussing limiter and find optimum conditions. A simple practical device for removing the gain switched peak from a TEA laser pulse is also described.

Quadrupole mass analyzers (QMAs) are receiving increasing attention for applications in time-of-flight (TOF) studies of laser-induced desorption, ablation and surface reactions in order to extend the information attainable from these experiments. With such a complicated detection device, however, it is easily possible to inadvertantly manipulate the real time-of-flight distribution, for example by missing fast or slow particles. In this work a systematic investigation of the influence of the different QMA parameters on the signal and their interplay was undertaken in laser-induced desorption experiments. The particle pulses were generated by resonant vibrational excitation of condensed benzene films with a TEA CO2 laser. Our investigations give the optimized configuratioin and setting of potentials for the instrument studied, in terms of sensitivity and energy resolution, and an accurate procedure to determine the drift time of ions in the quadrupole. This makes it possible to detect undistorted time-of-flight distributions with a time resolution of about 5 μs for a range of incident kinetic energies of at least 0–3 eV.

A theoretical analysis of the N 2 Blumlein laser circuit based on the distributed parameter model is carried out. Some typical parametric dependences are presented and compared with the well known lumped parameter model. The results indicate the validity of the distributed parameter model over a wider range of parametric studies. The analysis is quite general and can be easily extended to study other fast discharge laser systems such as TEA CO 2 , excimer and metal vapour lasers.

Electrostatic plasma waves are excited in a laboratory plasma by means of the ponderomotive force of a high‐power, power‐modulated transversely excited atmosphere (TEA) CO2 laser beam [W. W. Duley, CO2 Lasers (Academic, New York, 1976), Chap. 2.5]. The strengths of the magnetic field, for which the plasma waves are excited selectively, and the group velocity of the excited plasma waves are consistent with the dispersion relation of the electrostatic ion cyclotron wave. This wave‐excitation experiment gives proof to the principles of the driven scattering plasma diagnostics which has been proposed as a method for the ion temperature measurement of high‐temperature plasmas.

A simple method for the generation of short, single-mode CO2 laser pulses produced by applying two voltage gates (of amplitude 3Uλ/4 and Uλ/4) to an electro-optic Q-switch placed in a three-mirror cavity is proposed. Single, single-mode, well-synchronizable pulses of 3 ns duration and of 3 mJ energy have been experimentally achieved from a TEA CO2 laser with an intracavity Pockels cell with 3 ns switching time. Using a numerical simulation it is shown that with shorter switching time (≈1 ns) the method enables one to obtain, from such a laser, a single, megawatt pulse of 1 ns duration.

A four-channel nanosecond transversely excited atmospheric (TEA) N2 laser controlled by a simple and cost effective multistage spark gap which offers a high flexibility in varying the time sequence of the laser pulses from over 100 ns to as low as 5 ns is described. The delays between these laser pulses depend mainly on two important spark gap breakdown parameters: the charging voltage and their respective gap separations. The jitters between these laser pulses are observed to be independent of the initial ignition of the multistage spark gap-hence a precision and very fast triggering technique that is usually crucial for such work can be dispensed with.

The long-term operation of a 1 kHz, 500 W transversely excited atmospheric CO2 laser has been realized by using an all-solid-state exciter. The laser system consisted of a fast-gas-flow tunnel containing a discharge head, a pulsed power supply made of an all-solid-state exciter, and a gas regenerator with a gas analyser. The energy transfer efficiency of the exciter was 65% and an overall laser efficiency of 5.2% was obtained. Continuous operation of more than 107 shots has been achieved for sealed-off conditions.

Bone ablation using different pulse parameters and four emission lines of 9.3, 9.6, 10.3, and 10.6 μm of the CO2 laser exhibits effects which are caused by the thermal properties and the absorption spectrum of bone material. The ablation mechanism was investigated with light- and electron-microscopy at short laser-pulse durations of 0.9 and 1.8 μs and a long pulse of 250 μs. It is shown that different processes are responsible for the ablation mechanism either using the short or the long pulse durations. In the case of short pulse durations it is shown that, although the mineral components are the main absorber for CO2 radiation, water is the driving force for the ablation process. The destruction of material is based on explosive evaporation of water with an ablation energy of 1.3 kJ/cm3. Histological examination revealed a minimal zone of 10–15 μm of thermally altered material at the bottom of the laser drilled hole. Within the investigated spectral range we found that the ablation threshold at 9.3 and 9.6 μm is lower than at 10.3 and 10.6 μm. In comparison the ablation with a long pulse duration is determined by two processes. On the one side, the heat lost by heat conduction leads to carbonization of a surface layer, and the absorption of the CO2 radiation in this carbonized layer is the driving force of the ablation process. On the other side, it is shown that up to 60% of the pulse energy is absorbed in the ablation plume. Therefore, a long pulse duration results in an eight-times higher specific ablation energy of 10 kJ/cm3.

The performance of a pulsed CO2 laser using the capacitor transfer circuit is generally known to improve with an optimum peaking‐to‐storage capacitor ratio Cp/Cs which varies from around 0.1 to almost 0.5. There has been no reported attempt to account for precisely the origin of this optimum ratio and the large difference amongst them with different experimental setups. In this paper, the optimum capacitor ratio is shown to depend uniquely on the distributed circuit inductances. This may be understood from a simple consideration of the impedance matching for achieving an optimum power transfer at a quasiconstant E/N ratio into the main discharge.

The practical application of the narrow-band transversely excited atmosphere CO(2) laser, which uses a double-grating cavity, is demonstrated by pumping spectrally pure farinfrared lines in a CH(2)OH laser.

We communicate results of the stable operation of a TEA CO(2) oscillator-amplifiers system, producing pulses of 10(14) W/cm(2) at best focus, furnished with a simple provision for retropulse isolation.

Trifluoromethyl iodide, CF(3)I, has been shown to be an efficient optical filter for TEA CO(2) laser pumped several mid IR molecular lasers. Its absorption characteristics and effectiveness of filtering capacity were examined using a pump TEA CO(2) laser and a 12.08-microm NH(3) laser.