Modeling of static K and Rb diode pumped alkali lasers (DPAL) and ion-electron recombination processes in these lasers is reported. The cases of He/CH4 and pure He buffer gases are investigated and the output power and optical efficiency calculated for various pump powers, mole fractions of methane, buffer gas pressures and flow velocities. The model considers the processes of excitation of high levels of K and Rb, ionization, ion-electron recombination and heating of electrons which affect the diffusion coefficient of K and Rb ions. It explains the experimentally observed sharp increase in power in static K DPAL caused by the addition of a few percent of methane to He buffer gas and its decrease with further increase in the methane percentage [B.V. Zhdanov et al, Opt. Exp. 25, 30793 (2017)]. The predictions of the model for different He/CH4 mixtures are presented and verified by comparing them with experimental results for K flowing-gas DPAL [A. J. Wallerstein, Ph.D. dissertation (Air Force Institute of Technology, 2018)] and with the calculated results obtained using a simplified three-level model based on one-dimensional gas dynamics approach reported by A. Gavrielides et al [J. Opt. Soc. Am. B 35, 2202 (2018)]. Calculations of potential energy curves of the 2 K + and 2 Rb + molecular ions and of the diabatic 1ε+, 3ε+, 1Δ, 3Δ, 1 Π 3Π, 1Φ and 3Φ valence states of 2 K + and 2 Rb + that provide the routes for dissociative recombination (DR of the ions are performed. These curves are required for subsequent calculations of DR rate constants. The excited states of K atoms produced by DR are 42P and 52P. Most of the Rb atoms produced by DR are in the 62P excited state. This conclusion contradicts the kinetic scheme for K and Rb DPAL proposed elsewhere, and thus the kinetic schemes of these DPALs should be modified according to the present results.
A comprehensive three-dimensional modeling of static K diode pumped alkali laser (DPAL) and flowing-gas K and Rb DPALs is carried out. The cases of He/CH4 and pure He buffer gases are investigated and the output power and optical efficiency calculated for various pump powers, mole fractions of methane, buffer gas pressures and flow velocities. The model considers the processes of excitation of high levels of K and Rb, ionization, ion-electron recombination and heating of electrons which affect the diffusion coefficient of K and Rb ions. It explains the experimentally observed sharp increase in power in static K DPAL caused by the addition of a few percent of methane to He buffer gas and its decrease with further increase in the methane percentage [B.V. Zhdanov et al, Opt. Exp. 25, 30793 (2017)]. The predictions of the model for different He/CH4 mixtures are presented and verified by comparing them with experimental results for K flowing-gas DPAL [A. J. Wallerstein, Ph.D. dissertation (Air Force Institute of Technology, 2018)] and with the calculated results obtained using a simplified three-level model based on one-dimensional gas dynamics approach reported by A. Gavrielides et al [J. Opt. Soc. Am. B 35, 2202 (2018)].
Comprehensive analysis of the performance and beam quality of subsonic flowing-gas K diode-pumped alkali lasers (DPALs) with different pumping geometries, using 3D computational fluid dynamics model, is reported. The model is first applied to a K DPAL with transverse pumping and parameters similar to those of the 1.5 kW K DPAL [Pitz et al, Proc. SPIE 9729, 972902 (2016)] and the calculated results are in satisfactory agreement with the measurements. To study the possibility of scaling up the K DPAL the model is then applied to 100-kW class device with transverse and end pumping geometry. Dependence of the output power on the flow velocity and the pumping geometry is studied. Comparison between end and transverse pumping schemes shows that the output power is almost unaffected by the pumping geometry. However, the spatial intensity distribution of the output laser beam depends on the pumping geometry: it is uniform for the end pumping, whereas for the transverse pumping it is strongly non-uniform at high gas temperature (corresponding to large density of K atoms), becoming more uniform with temperature reduction. The model is applied to evaluation of the beam quality of flowing-gas K DPALs which strongly depends on the refractive index distribution in the gain medium. The beam divergence and the width of the intensity profile in the far field for the end pumping appear to be much smaller than for the transverse pumping. Wave front corrections of the transversely pumped device using cylindrical lens results in substantial reduction of the laser beam divergence and improvement of its quality which becomes comparable with that of the end pumped laser.
Analysis of beam propagation, kinetic and fluid dynamic processes in Cs diode pumped alkali lasers (DPALs), using wave optics model and gasdynamic code, is reported. The analysis is based on a three-dimensional, time-dependent computational fluid dynamics (3D CFD) model. The Navier-Stokes equations for momentum, heat and mass transfer are solved by a commercial Ansys FLUENT solver based on the finite volume discretization technique. The CFD code which solves the gas conservation equations includes effects of natural convection and temperature diffusion of the species in the DPAL mixture. The DPAL kinetic processes in the Cs/He/C2H6 gas mixture dealt with in this paper involve the three lowest energy levels of Cs, (1) 62S1/2, (2) 62P1/2 and (3) 62P3/2. The kinetic processes include absorption due to the 1→3 D2 transition followed by relaxation the 3 to 2 fine structure levels and stimulated emission due to the 2→1 D1 transition. Collisional quenching of levels 2 and 3 and spontaneous emission from these levels are also considered. The gas flow conservation equations are coupled to fast-Fourier-transform algorithm for transverse mode propagation to obtain a solution of the scalar paraxial propagation equation for the laser beam. The wave propagation equation is solved by the split-step beam propagation method where the gain and refractive index in the DPAL medium affect the wave amplitude and phase. Using the CFD and beam propagation models, the gas flow pattern and spatial distributions of the pump and laser intensities in the resonator were calculated for end-pumped Cs DPAL. The laser power, DPAL medium temperature and the laser beam quality were calculated as a function of pump power. The results of the theoretical model for laser power were compared to experimental results of Cs DPAL.
Scaling-up flowing-gas diode pumped alkali lasers (DPALs) to megawatt class power is studied using accurate three-dimensional computational fluid dynamics model, taking into account the effects of temperature rise and losses of alkali atoms due to ionization. Both the maximum achievable power and laser beam quality are estimated for Cs and K lasers. We examined the influence of the flow velocity and Mach number M on the maximum achievable power of subsonic and supersonic lasers. For Cs DPAL devices with M = 0.2 - 3 the output power increases with increasing M by only ~20%, implying that supersonic operation mode has only small advantage over subsonic. In contrast, the power achievable in K DPALs strongly depends on M. The output power increases by ~100% when M increases from 0.2 to 4, showing a considerable advantage of supersonic device over subsonic. The reason for the increase of the power with M in both Cs and K DPALs is the decrease of the temperature due to the gas expansion in the flow system. However, the power increase for K lasers is much larger than for the Cs devices mainly due to the much smaller fine-structure splitting of the 2P states (~58 cm-1 for K and ~554 cm-1 for Cs), which results in a much stronger effect of the temperature decrease in K DPALs. For pumping by beams of the same rectangular cross section, comparison between end-pumping and transverse-pumping shows that the output power is not affected by the pump geometry. However, the intensity of the output laser beam in the case of transverse-pumped DPALs is strongly non-uniform in the laser beam cross section resulting in higher brightness and better beam quality in the far field for the end-pumping geometry where the intensity of the output beam is uniform.
Modeling of static and flowing-gas subsonic, transonic and supersonic Cs and K Ti:Sapphire and diode pumped alkali lasers (DPALs) is reported. A simple optical model applied to the static K and Cs lasers shows good agreement between the calculated and measured dependence of the laser power on the incident pump power. The model reproduces the observed threshold pump power in K DPAL which is much higher than that predicted by standard models of the DPAL. Scaling up flowing-gas DPALs to megawatt class power is studied using accurate three-dimensional computational fluid dynamics model, taking into account the effects of temperature rise and losses of alkali atoms due to ionization. Both the maximum achievable power and laser beam quality are estimated for Cs and K lasers. The performance of subsonic and, in particular, supersonic DPALs is compared with that of transonic, where supersonic nozzle and diffuser are spared and high power mechanical pump (needed for recovery of the gas total pressure which strongly drops in the diffuser), is not required for continuous closed cycle operation. For pumping by beams of the same rectangular cross section, comparison between end-pumping and transverse-pumping shows that the output power is not affected by the pump geometry, however, the intensity of the output laser beam in the case of transverse-pumped DPALs is strongly non-uniform in the laser beam cross section resulting in higher brightness and better beam quality in the far field for the end-pumping geometry where the intensity of the output beam is uniform.
An analysis of radiation, kinetic and fluid dynamic processes in diode pumped alkali lasers (DPALs) is reported. The
analysis is based on a three-dimensional, time-dependent computational fluid dynamics (3D CFD) model. The CFD code
which solves the gas conservation equations includes effects of natural convection and temperature diffusion of the species
in the DPAL mixture. The gas flow conservation equations are coupled to the equations for DPAL kinetics and to the
Beer-Lambert equations for pump and laser beams propagation. The DPAL kinetic processes in the Cs/CH4 (K/He) gas
mixtures considered involve the three low energy levels, (1) n2S1/2, (2) n2P3/2 and (3) n2P1/2 (where n=4,6 for K and Cs,
respectively), three excited alkali states and two alkali ionic states. Using the CFD model, the gas flow pattern and spatial
distributions of the pump and laser intensities in the resonator were calculated for end-pumped CW and pulsed Cs and K
DPALs. The DPAL power and medium temperature were calculated as a function of pump power and pump pulse duration.
The CFD model results were compared to experimental results of Cs and K DPALs.
We report on recent progress on our three-dimensional computational fluid dynamics (3D CFD) modeling of supersonic
diode pumped alkali lasers (DPALs), taking into account fluid dynamics and kinetic processes in the lasing medium. For
a supersonic Cs DPAL with laser section geometry and resonator parameters similar to those of the 1-kW flowing-gas
subsonic Cs DPAL [A.V. Bogachev et al., Quantum Electron. 42, 95 (2012)] the maximum achievable output power, ~ 7
kW, is 25% higher than that achievable in the subsonic case. Comparison between semi-analytical and 3D CFD models
for Cs shows that the latter predicts much higher maximum achievable output power than the former. Optimization of the
laser parameters using 3D CFD modeling shows that very high power and optical-to-optical efficiency, 35 kW and 82%,
respectively, can be achieved in a Cs supersonic device pumped by a collimated cylindrical (0.5 cm diameter) beam.
Application of end- or transverse-pumping by collimated rectangular (large cross section ~ 2 - 4 cm2) beam makes it
possible to obtain even higher output power, > 250 kW, for ~ 350 kW pumping power. The main processes limiting the
power of Cs supersonic DPAL are saturation of the D2 transition and large ~ 40% losses of alkali atoms due to
ionization, whereas the influence of gas heating is negligibly small. For supersonic K DPAL both gas heating and
ionization effects are shown to be unimportant and the maximum achievable power, ~ 40 kW and 350 kW, for pumping
by ~ 100 kW cylindrical and ~ 700 kW rectangular beam, respectively, are higher than those achievable in the Cs
supersonic laser. The power achieved in the supersonic K DPAL is two times higher than for the subsonic version with
the same resonator and K density at the gas inlet, the maximum optical-to-optical efficiency being 82%.
Application of two- and-three dimensional computational fluid dynamics (2D and 3D CFD) models to subsonic flowing-gas DPALs is reported. The 2D model is applied to a DPAL with optical resonator-flow field coaxial configuration and the 3D model is applied to an optical axis transverse to the flow configuration. The models take into account effects of temperature rise and losses of alkali atoms due to ionization. The 2D CFD model is applied to 1 kW flowing-gas Cs DPAL [A.V. Bogachev et al., Quantum Electron. 42, 95 (2012)] and the calculated results are in good agreement with the measurements. Comparison of the 2D CFD to semi-analytical model [B. D. Barmashenko and S. Rosenwaks, J. Opt. Soc. Am. B 30, 1118 (2013)] shows that for low pump power both models predict very close values of the laser power; however, at higher pump power, corresponding to saturation of the absorption of the pump transition, the laser power calculated using the 2D CFD model is much higher than that obtained using the semi-analytical model. At high pump power, the heat convection out of the laser resonator is more efficient for the transverse case than the coaxial case, the beam temperature is lower and consequently the calculated laser power is higher. Optimization of the Cs DPAL parameters, using 3D CFD modeling, shows that applying high flow velocity and narrowband pumping, maximum lasing power as high as 40 kW can be obtained at pump power of 80 kW for transverse flow configuration in a pumped volume of ~ 0.7 cm3.
Comparison between a semi-analytical and two- and-three dimensional computational fluid dynamics (2D and 3D CFD)
models is reported. The models take into account effects of temperature rise and losses of alkali atoms due to ionization
and chemical reactions, resulting in a decrease of the slope efficiency and lasing power. Effects of natural convection in
static DPALs are also taken into account. Both models are applied to Cs DPALs and the results are in good agreement
with measurements in a static [B.V. Zhdanov, J. Sell and R.J. Knize, Electron. Lett. 44, 582 (2008)] and 1-kW flowinggas
[A.V. Bogachev et al., Quantum Electron. 42, 95 (2012)] DPALs. Comparison of the models applied to the flowinggas
DPAL shows that for low pump power both models predict very close values of the laser power; however, at higher
pump power, corresponding to saturation of the absorption of the pump transition, the values of the laser power
calculated using the 2D CFD model are much higher than those obtained using the semi-analytical model.
Comprehensive analysis of kinetic and fluid dynamic processes in flowing-gas diode pumped alkali lasers (DPALs)
using two- and three-dimensional computational fluid dynamics (2D and 3D CFD) models is reported for Cs DPALs.
The models take into account effects of temperature rise and losses of alkali atoms due to ionization. Various gas flow
regimes and transverse and parallel flow-optics directions configurations are studied. Optimization of the Cs DPAL
parameters, using 3D CFD modeling, shows that applying high flow velocity and narrowband pumping, maximum lasing
power as high as 40 kW can be obtained at pump power of 80 kW for transverse flow configuration in a pumped volume
of ~ 0.7 cm3. At high pump power the calculated laser power is higher for the transverse scheme than for the parallel
scheme because of a more efficient heat convection from the beam volume in the transverse configuration. The CFD
models are applied to experimental devices and the calculated results are in good agreement with the measurements.
Results of recent semi-analytical and three dimensional computational fluid dynamics (3D CFD) modeling of supersonic
diode pumped alkali lasers (DPALs), as well as summary of work in progress, are reported. DPALs have been
extensively studied in the past few years and static and flowing-gas devices have been investigated. Modeling of these
devices has been conducted as well and fluid dynamics and kinetic processes have been taken into account, but until
recently only flowing-gas DPALs with subsonic velocity of the gas were considered. Following our previous work on
supersonic DPALs we further explore in the present study the feasibility of operating DPALs with supersonic expansion
of the gaseous laser mixture, consisting of alkali atoms, He atoms and (frequently) hydrocarbon molecules. The
motivation for this exploration stems from the possibility of fast and efficient cooling of the mixture by the supersonic
expansion. In a recent paper (S. Rosenwaks et al, Proc. SPIE 8962, 896209 (2014)) we have reported on semi-analytical
modeling for a supersonic Cs DPAL with parameters similar to those of the 1-kW flowing-gas subsonic Cs DPAL (A.V.
Bogachev et al, Quantum Electron. 42, 95 (2012)); the maximum power, Plase, for the former was found to be higher than
for the latter by 25%. Optimization of the He/CH4 buffer gas composition and flow parameters using 3D CFD modeling
shows that for Bogachev et al resonator parameters, extremely high lasing power and optical-to-optical efficiency, 33
kW and 82%, respectively, are achievable in the Cs supersonic device. Comparison between the semi-analytical and the
3D CFD models for Cs shows that the latter predicts much higher maximum achievable laser power than the former. For
a supersonic K DPAL the semi-analytical model predicts Plase = 43 kW, 70% higher than for subsonic with the same
resonator and K density at the inlet, the maximum optical-to-optical efficiency being 82%. The paper also includes
estimates for closed cycle supersonic systems.
The feasibility of operating diode pumped alkali lasers (DPALs) with supersonic expansion of the gaseous laser mixture, consisting of alkali atoms, He atoms and (frequently) hydrocarbon molecules, is explored. Taking into account fluid dynamics and kinetic processes, both semi-analytical and three-dimensional (3D) computational fluid dynamics (CFD) modeling of supersonic DPALs is reported. Using the semi-analytical model, the operation of supersonic DPALs is compared with that measured and modeled in subsonic lasers for both Cs and K. The maximum power of supersonic Cs and K lasers is found to be higher than that of subsonic lasers with the same resonator and alkali density at the laser inlet by 25% and 70%, respectively. Using the 3D CFD model, the flow pattern and spatial distributions of the pump and laser intensities in the resonator are calculated for Cs DPALs. Comparison between the semi-analytical and 3D CFD models for Cs shows that the latter predicts much larger maximum achievable laser power than the former. These results indicate that for scaling-up the power of DPALs, supersonic expansion should be considered.
In the last four years, a few research groups worked on the feasibility of compressive sampling (CS) in ultrasound medical imaging and several attempts of applying the CS theory may be found in the recent literature. In particular, it was shown that using iotap-norm minimization with p different from 1 provides interesting RF signal reconstruction results. In this paper, we propose to further improve this technique by processing the reconstruction in the Fourier domain. In addition, alpha -stable distributions are used to model the Fourier transforms of the RF lines. The parameter p used in the optimization process is related to the parameter alpha obtained by modelling the data (in the Fourier domain) as an alpha -stable distribution. The results obtained on experimental US images show significant reconstruction improvement compared to the previously published approach where the reconstruction was performed in the spatial domain.
Kinetic and fluid dynamic processes in diode pumped alkali lasers (DPALs) are analyzed in detail using a semianalytical model, applicable to both static and flowing-gas devices. The model takes into account effects of temperature rise, excitation of neutral alkali atoms to high lying electronic states and their losses due to ionization and chemical reactions, resulting in a decrease of the pump absorption, slope efficiency and lasing power. Effects of natural convection in static DPALs are also taken into account. The model is applied to Cs DPALs and the results are in good agreement with measurements in a static [B.V. Zhdanov, J. Sell and R.J. Knize, Electron. Lett. 44, 582 (2008)] and 1-kW flowing-gas [A.V. Bogachev et al., Quantum Electron. 42, 95 (2012)] DPALs. It predicts the dependence of power on the flow velocity in flowing-gas DPALs and on the buffer gas composition. The maximum values of the laser power can be substantially increased by optimization of the flowing-gas DPAL parameters. In particular for the aforementioned 1 kW DPAL, 6 kW maximum power is achievable just by increasing the pump power and the temperature of the wall and the gas at the flow inlet (resulting in increase of the alkali saturated vapor density). Dependence of the lasing power on the pump power is non-monotonic: the power first increases, achieves its maximum and then decreases. The decrease of the lasing power with increasing pump power at large values of the latter is due to the rise of the aforementioned losses of the alkali atoms as a result of ionization. Work in progress applying two-dimensional computational fluid dynamics modeling of flowing-gas DPALs is also reported.
We explore the feasibility of supersonic operation of diode pumped alkali lasers (DPALs) applying model calculations. The power and efficiency of Cs and K atoms DPALs are estimated based on a semi-analytical model previously used for studying static and subsonic flow DPALs. The operation of supersonic lasers is compared with that measured and modeled in subsonic lasers. The maximum power of supersonic Cs and K lasers is found to be higher than that of subsonic lasers with the same resonator and alkali density at the laser inlet by 25% and 70%, respectively. These results indicate that for scaling-up the power of DPALs, supersonic expansion should be considered. Work in progress applying three-dimensional computational fluid dynamics modeling of supersonic DPALs is also reported.
KEYWORDS: Resonators, Mirrors, Chemical lasers, 3D modeling, Lawrencium, Geometrical optics, Laser resonators, Chemical oxygen iodine lasers, Data modeling, Near field optics
Simple models are developed, describing the power extraction in chemical oxygen-iodine lasers (COILs) with stable and
unstable resonators. For stable resonators the model is applied to the ejector high pressure COIL and the results are
compared with the experimental data (see also a preceding paper by Rosenwaks et al.). The positive and negative branch
unstable resonators with cylindrical mirrors that have been recently used in COILs are studied theoretically using a
geometrical optics model. The optical extraction efficiency, spatial distributions of the intracavity radiation intensity in
the flow direction and the intensity in the far field are calculated for both kinds of resonators as a function of both the
resonator and COIL parameters. The optimal resonator magnifications corresponding to the maximum intensity in the far
field are found.
The kinetics of the chemical oxygen-iodine laser (COIL) has been studied alongside the technological efforts in COIL
development. In particular, many efforts have been devoted to the study of the mechanism of I2 dissociation in the COIL
medium. Since O2(a) is the energy reservoir of the COIL, it must be involved in the dissociation of I2. Therefore,
understanding the dissociation mechanism may help in finding ways of minimizing the O2(a) consumption for
dissociation and increasing the chemical efficiency of the laser. In the present paper previously suggested mechanisms
of I2 dissociation are briefly overviewed and recent measurements and modeling of the gain and the power in supersonic
COILs carried out in our laboratory are presented. Our studies employ both an analytical model and numerical
calculations which are outlined in the present paper, with more details on the models given in a following paper by
Barmashenko et al. To unravel the I2 dissociation mechanism we utilize kinetic-fluid dynamics three-dimensional
modeling, where pathways involving the excited species I2(X, 10 ≤ v < 25), I2(X, 25 ≤ v ≤ 47), I2(A, A'), O2(X, v), O2(a,
v), O2(b, v) and I(2P1/2) as intermediate reactants are included. Both the gain and the power studies show good agreement
between calculations and experiments. We believe that future modeling should include the above pathways and
additional pathways should be considered when additional kinetic data is available.
The results of three-dimensional computational fluid dynamics model calculations are reported in detail and compared to
available experimental results [Nikolaev et al., IEEE J. Quantum Electron. 38, 421 (2002)]. It is shown that the model is
applicable to high pressure, ejector type chemical oxygen-iodine laser (COIL), reasonably reproducing the measured
gain, temperature, static pressure and gas velocity. A previous model which included I2(A' 3Pi2u), I2(A 3Pi1u) and O2(a 1Deltag,
v) as significant intermediates in the dissociation of I2 [Waichman et al., J. Appl. Phys. 102, 013108 (2007)] reproduced
the measured gain and temperature of a low pressure supersonic COIL. The previous model is complemented here by
adding the effects of turbulence, which play an important role in high pressure COILs.
KEYWORDS: 3D modeling, Chemical oxygen iodine lasers, Oxygen, Chemical lasers, Computational fluid dynamics, Mirrors, Iodine, Chlorine, Modeling, Systems modeling
Experimental and theoretical work in progress on supersonic COILs at Ben-Gurion University is reported. Following the
achievement of a record value (40%) for the chemical efficiency of a supersonic 5-cm gain length COIL in our lab, a 10-
cm gain length device was experimentally studied. Maximum output power exceeding 0.6 kW with chemical efficiency
of 35% was obtained for 1% total mirror transmission in preliminary studies. Comparing the results of three-dimensional
computational fluid dynamics model calculations to available experimental results [Nikolaev et al., IEEE J. Quantum
Electron. 38, 421 (2002)], we show that the model is applicable to high pressure, ejector type chemical oxygen-iodine
laser (COIL), reasonably reproducing the measured gain and temperature.
KEYWORDS: 3D modeling, Chemical lasers, Chemical oxygen iodine lasers, Iodine, Computational fluid dynamics, Molecules, 3D metrology, Computer simulations, Optical simulations, Chemical reactions
The dissociation of I2 molecules at the optical axis of a supersonic chemical oxygen-iodine laser (COIL) was studied via detailed measurements and three dimensional computational fluid dynamics calculations. Comparing the measurements and the calculations enabled critical examination of previously proposed dissociation mechanisms and suggestion of a mechanism consistent with the experimental and theoretical results. The gain, I2 dissociation fraction and temperature at the optical axis, calculated using Heidner's model (R.F. Heidner III et al., J. Phys. Chem. 87, 2348 (1983)), are much lower than those measured experimentally. Agreement with the experimental results was reached by using Heidner's model supplemented by Azyazov-Heaven's model (V.N. Azyazov and M.C. Heaven, AIAA J. 44, 1593 (2006)) where I2(A') and vibrationally excited O2(a1&Dgr;) are significant dissociation intermediates.
KEYWORDS: Iodine, Chemical oxygen iodine lasers, Chemical lasers, Molecules, Chemical analysis, Oxygen, Chemical species, Absorption, Resonators, Diagnostics
The dissociation of I2 molecules at the optical axis of a supersonic chemical oxygen-iodine laser (COIL) was studied
experimentally as a function of I2 flow rate. The measurements revealed that the number of consumed O2(1&Dgr;) molecules
per dissociated I2 molecule depends on the experimental conditions: it is 4.2 ± 0.4 for typical conditions and I2 densities
applied for the operation of the COIL, but increases at lower I2 densities. In addition, a new method for dissociating I2
prior to its mixing with O2(1&Dgr;) and thus reducing the loss of O2(1&Dgr;) is reported. The method is based on applying
corona/glow electrical discharge in the transonic section of the secondary flow in the COIL supersonic nozzle. 1.7% of I2
is dissociated by the discharge resulting in 70% power enhancement at rather high I2/O2 ratio, 1.6%, close to the optimal
value (~ 2.5%) for operation of COILs with supersonic mixing.
We investigated the operation of a diode-pumped Yb:YAG laser passively Q-switched, by Cr4+:YAG, Cr4+:LuAG, and Cr4+:GSGG saturable absorbers. The results presented here are focused towards the design of a passively Q-switched Yb:YAG microlaser. The free-running performance of both rod and a disk Yb:YAG is characterized, and experimental parameters such as gain and loss are evaluated. These values, together with the value of the stimulated emission cross section, e.g. (sigma) emequals3.3x10-20 cm2 were found to fit between our experimental results and an existing numerical model which relates the experimental and physical parameters to the minimal threshold pumping power. Q-switched pulses with maximum peak power of approximately equals 10.4-kW, and energy of approximately equals 0.5 mJ/pulse were extracted with 30% extraction efficiency.
We report the operation of a passively Q-switched diode end pumped Nd3+:KGW laser, which was obtained by using a Cr4+:YAG or Cr4+:GGG saturable absorbers in the multi-kHz frequency domain. The free-running (with maximum slope efficiency of 46%), and the passively Q-switched characteristics of Nd:KGW were investigated and the use of Nd:KGW as microlasers will be discussed.
The performance (in terms of output power and slope efficiency) of the passively Q-switched Nd:YAG and Nd:YVO4 lasers, both side pumped and end-pumped, will be reported and compared to our theoretical model. Passive Q- switch operation by a Cr4+:GGG element as a saturable absorber was studied in terms of pulse frequency as a function of pump power.
Laser performance of an electric discharge, plasma cathode preionized, atmospheric pressure HF chemical laser was investigated and geometrically optimized. The preionization electron density was measured at atmospheric pressure in helium and in a mixture of SF6 + H2 diluted by helium. The measured preionization density is ne approximately equals 6.7 X 106 - 2 X 107 cm-3, which is higher than the minimum critical density required for a self-sustained, homogeneous discharge of atmospheric-pressure electro-negative gasses. We have found improvement in laser specific energy for a diluted gas mixture of SF6 + H2 due to reduction in SF6 concentration. The effects of inter-electrode gap height and plasma cathode grid width on laser performance were also investigated and will be reported.
An experimental study of velocity and thermal turbulence generation is presented. These studies are directed to simple and compact laboratory simulation of atmospheric turbulence. The velocity and temperature turbulence was produced by injection of heated air into a main uniform flow of air. The turbulence velocity and temperature flow field was mapped and the one dimensional energy spectra and integral scales were measured. Homogeneous and isotropic turbulence with 18.5 percent streamwise velocity fluctuation intensity was achieved 8 mesh sizes downstream of the injector. At this location the turbulence was homogeneous within 5 percent and the ratio between the longitudinal and the perpendicular fluctuation components was 1.26. The average integral scale of the streamwise velocity turbulence was 18 mm, 0.18 units of mesh size, and the ratio between the velocity and temperature integral scales was 1.04.
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