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1 Introduction: The New Era of High Energy Lasers

1 Introduction: The New Era of High Energy Lasers

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46.6



Prospect of the Laser System Upgrading



389



of our present 6 atm CO2-HPA as well as possibility of increasing its operating

pressure up to 10 atm in order to amplify laser pulses as short as 1 ps (Sect. 2.2).

We are planning to realize these possibilities in te very near future since they do not

demand principal reassembling of present laser system. We also have some other

plans (for longer terms) for our system upgrading:

1. Investigating the possibility of using N2O:CO:N2:He mixtures in our CO2-HPA

instead of traditional CO2:N2:He ones. It should be noted that owing to lower

group of symmetry of N0 molecule if compared with CO2 neighboring

rotational-vibration transitions in the N2O molecule are located twice as close to

each other compared with CO2 molecule. Therefore, it is possible to realize

smooth gain spectrum of N2O molecule owing to pressure broadening of laser

transitions at the pressures of gas mixtures 5–6 atm, thus considerably

decreasing the level of pulsed high-voltage applied to the discharge chamber. It

should be also noted that utilization of such a gas mixture is many orders less

expensive compared with CO2 multiisotopic mixtures. Of course we understand

that it will not be an easy problem. Owing to the substantially higher attachment

of electrons to N2O molecules compared with that of CO2 the kinetics of the

SSVD in N2O mixtures strongly differs from that of CO2. However, we had

already realized SSVD in N2O gas mixtures of 1 atm pressure with record

values of SSVD active volume (20 Â 20 Â 125 cm3), efficiency (6.7%) and

light energy (465 J) [13] and have a good experience in investigation of kinetics

of SSVD in such gas mixtures.

2. We are sure that repetition rates of *60 Hz can be realized in our laser system.

All elements of our present MO scheme can operate at f * 60 Hz with reasonable upgrading. The e-beam gun utilized in our CO2–HPA can also operate

at such repetition rates if we provide more effective evacuation systems for

vacuum diode compared with present one (this necessity is caused by evaporation of graphite into the volume of the diode at each shot of the gun). All

elements of our DPPHVG (capacitors and spark gaps) can also operate at such

repetition rates; moreover, the spark gaps were elaborated to work at f < 100 Hz

in the gas flow mode of operation (in the present laser system, there is no need to

use this option but it can be put into operation easily). The main problem for

60 Hz operation of CO2–HPA is to provide gas flow mode of operation of the

discharge chamber. It will evidently demand its reassembling and modification

or more probable construction of a new one. It should be noted that construction

of TEA-CO2 lasers with f up to 20 Hz and active volumes of 5–10 1 and

TEA-CO2 lasers with f up to 400 Hz and single pulse energy of *1 J.

3. The utilization of e-beam gun in laser systems demands a high vacuum pump

system (to provide 10−5 Torr). The presence of this system evidently substantially increases the weight and dimensions of CO2–HPA as well as making its

operation more complicated. It is also evident that additional problems will

occur when transitioning to high repirates. As such, we are now searching for

alternative systems of gas mixture preionization and one of the possible methods

is pulling electrons out of the barrier close-to-cathode discharge and into the



390



46



Wide Aperture Picosecond CO2 Laser System



discharge gap. We have a wealth of experience in utilizating this type of

preionization in TEA-CO2 discharge units with interelectrode spacing of up to

60 cm and we hope to use this for superatmospheric pressure gas mixtures [14].

If we are successful in this endeavor, this will considerably simplify the construction and operation of our CO2–HPA.



46.7



Conclusions



1. We have put a CO2 laser system in operation with high aperture (5 Â 5 cm2),

6 atm amplifier, that generates a train of subnanosecond laser pulses with sum

energy of up to 5 J.

2. Our estimates based on scaling laws of SSVD stability with pressure indicate

that we can obtain SSVD in our CO2-HPA at P = 10 atm for interelectrode

spacing =4 cm, present gas mixture (CO2:N2:He = 10:5:85) and energy loading

densities >100 J/(l atm). Such a discharge unit can effectively amplify 10 lm

laser pulses as short as 1 ps.

3. There are no principal limits for upgrading our laser system to operate with

repetition rate *60 Hz. However, such a modification of the setup will obviously demand solutions to a number of technical problems.



References

1. V.V. Apollonov, A.I. Artemyev, Yu.L. Kalachev, A.G. Suzdaltsev, A.M. Prokhorov, M.V.

Fedorov, Electrons acceleration by intence laser radiation field in the presence of static

magnetic filed. JETF 97(5), 1498–1510 (1990)

2. J. Amesson, F.K. Kneubuhl, Future laser-driven particle accelerators. Infrared Phys. 25,

121–130 (1985)

3. S.A. Jamison, A.V. Nurmikko, Generation of picosecond pulses of variable duration at

10.6 lm. Appl. Phys. Lett. 33(7), 589–600 (1978)

4. P.B. Corkum, High-power, subpicosecond 10 lm pulse generation. Opt. Lett. 8, 514–516

(1983)

5. P.B. Corkum, Amplification of 10 lm Pulses in Multiatmosphere CO2 Lasers. IEEE,

J. Quantum Electron. QE-21, 216–232, (1985)

6. Z.A. Biglov, V.M. Gordienko, V.T. Platonenko, V.A. Slobodyanyuk, V.D. Taranukhin, SYu.

Ten, Generation and amplification of phazemodulated picosecond pulses of 10 lm range.

Izvestiya AN USSR, Seriya Fizicheskaya 55, 337–341 (1991)

7. P.B. Corkum, C. Roland, High Energy Picosecond 10 lm Pulses. Proc. SPIE 664, 212–216

(1986)

8. V.V. Apollonov, G.G. Baitsur et al., SSVD initiated by UV radiation and electrons of plasma

of spark discharge on the surface of dielectric (in Russian). Pis’ma v zhurnal telhnicheskoi

fiziki 14, 2107–2110 (1988)



References



391



9. A.G. Gordeichik, A.G. Maslennikov, A.A. Kuchinsky, V.A. Rodichkin, V.A. Smirnov, V.

P. Tomashevich, I.V. Shestakov, E.G. Yankin, Pulsed CO2 laser pumped by SSVD and

preionized by soft X-ray (in Russian), Kvantovaya Elektronika 18(10), 173–1175 (1991)

10. A.J. Alcock, P.B. Corkum, Ultra-fast switching of infrared radiation by laser produced

carrirers in semiconductors. Can. J. Phys. 57, 1280–1290 (1979)

11. P.E. Dyer, I.K. Perera, Pulse evolution in injection mode locked TE CO2 lasers. Appl. Phys.

23, 245–251 (1980)

12. P.B. Corkum, A.J. Alcock, Generation and amplification of short 10 pm pulses. in Picosecond

Phenomena, Springer Series in Chemical Physics, ed. by C.V. Shank, E.P. Ippen, S.L.

Shapiro, vol. 4 (1978), p. 308–312

13. V.V. Apollonov et al., N2O laser pumped by SSVD. Kvantovaya Elektronika 16, 1303–1305

(1989)

14. V.V. Apollonov et al, High-power CO2 and N2O lasers with SSVD pumping. J. Opt. Soc. Am.

B 8(2), 220 (1991)



Chapter 47



Lasers for Industrial, Scientific

and Ecological Use



Abstract This chapter is based on a long-term experience of the development and

operation of lasers and contains tested technical solutions on designing separate

units as well on the laser on the whole. The best overall dimensions and operation

characteristics and the prospects of additional chemical pumping put AMT GDL in

the forefront among other powerful industrial lasers. High repetition rate

pulse-periodic regime of high power laser radiation generated by AMT GDL on the

level of >100 kW of average power is the most important step for effective

implementation of many different laser-based technologies of the time. The very

near future will highlight the total potential of high-energy lasers, which will be

used effectively for processing materials and for the solution of other important

challenges faced by future science and technology. However, today it is possible to

say that creation of megawatt high-repetition-rate P–P lasers with a large cross

section of the active medium will open up an avenue for their use in solving the

problems of launching small satellites with lasers, formation of super-long conducting channels in space and atmosphere, and cleaning of the near-Earth space

from space debris, etc. Hopefully, the mono-module disk laser will have a lot of

advantages in comparison with the many other lasers observed in the present

chapter.



47.1



Introduction: The New Era of High Energy Lasers



So, the SDI age is over. The age that was very much influencing research and

development in the area of high power and high energy lasers. These days, we have

extremely strong demand for the development of very powerful lasers (>100 kW)

for civil applications [1]. Now the modern level of laser technology development

makes laser methods of materials treatment more and more competitive. In particular, disregarding the higher price of the equipment applied, laser welding of

metals provides a significant increase in productivity, a higher quality of the weld

practically without any following mechanical processing, and low residual stresses



© Springer International Publishing Switzerland 2016

V.V. Apollonov, High-Energy Molecular Lasers,

Springer Series in Optical Sciences 201, DOI 10.1007/978-3-319-33359-5_47



393



394



47 Lasers for Industrial, Scientific and Ecological Use



in the welded products. The world market of powerful industrial lasers (average

power level 1 Ä 15 kW) applied for cutting and welding of metal structures of

1 Ä 10 mm thick has been actively formed.

At the same time, there are a number of technical problems, the solution for

which is significantly simplified by the application of industrial powerful lasers

(within the range of 50 Ä 100 kW). In particular, the areas of applications for

autonomous mobile technological laser complexes (AMT GDL) are the following:

• Cleaning the coast line from oil products following oil emergency overflow and

cleaning of water surface from oil layer including thin iridescent layer that can

not be effectively removed by any other methods;

• Remote cutting of metal and armored concrete constructions in a course of

demontage and emergency repair on nuclear power plants, oil and gas boring

wells, in a process of emergency work after an earthquake and other natural

disasters; cutting up ships and submarines to metal scrap;

• Remote treatment of large metallurgical chemical, mining equipment in the

course of assembling and repair;

• Special technologies for use at specific conditions of different productions such

as cutting of materials and metal constructions, welding and surface treatment;

• Operative struggle with ice-covering of port equipment, constructions and

special system;

• Laser-based decontamination of surfaces by peeling in a process of emergency

works after natural disasters and different accidents;

The upper level of estimation for output power of laser should be given by:

"





! #

Á 0:75 Á v

pffiffiffi

1

0:53 1

hẳ

1:26 v ỵ 0:126 v ỵ

1 ỵ p

W

G

v



The variables in the expression are given in: h—[cm]; W—[kW]; v—[cm/s];

G—[g/s]. In order to increase cut depth, a simultaneous increase of power and gas

flow rate are required and taking into account the losses, the power needed for

cutting the samples 35 cm thick should be %100 kW (v = 0.3 cm/s; G = 20 g/s).

There are several variants of high-energy laser beams application on removal of

a thin oil film from the water surface, removal of the results of disasters, accidents

and catastrophes. In these cases, price and work expenses do not play the primary

role. The first place is occupied with the requirements for the reliability of high

average power lasers; the overhaul period without putting additional components;

simplicity in service; and operation and ecological safety. More than this, as the

objects of operation are located outside workshops and far away from electric

power sources, one of the basic requirements for a powerful high energy laser for

such application is its mobility and full autonomy. As such, most attention had been

devoted to the discussions and experimental realizations of autonomous mobile

technological gas-dynamic laser (AMT GDL) [2].



47.2



47.2



Comparison of Some Types of Lasers …



395



Comparison of Some Types of Lasers That Can Be

Scaled up to the Average Power Level >100 kW



Among all types of lasers that can be scaled up to the average power level

50 Ä 100 kW, the following lasers can be taken for industrial applications:













Gas-dynamic CO2-laser (CO2 GDL),

Chemical HF/DF-lasers,

Chemical oxygen-iodine laser (COIL);

Gas-discharge CO laser;

Gas-discharge CO2-laser.



Let’s make a short comparison of the above-given lasers.

A CW chemical HF-laser can be rather powerful and effective but it is typical of

low pressure of the active medium (not exceeding several mm Hg) and a toxic

exhaust. Hence, on the ground, this laser can operate only with vacuum vessels,

which doesn’t satisfy the requirements of a long-term operation.

Intensive development in the latest period chemical oxygen-iodine laser (COIL)

does not seem attractive from the point of view of ecology and the exploitation of

SCT lasers satisfying the above-given requirements, although the potential of this

COIL-laser for the creation of other industrial lasers cannot be stressed highly

enough. This laser also has a rather low work pressure; its exhaust gases have

iodine vapors. Chemical means of the production of oxygen delta requires components difficult in application (chlorine, alkali, hydrogen peroxide etc.) and rather

big chemical reactors. Gas-discharge method of the oxygen delta production does

not improve the situation significantly and is yet to be developed perfectly. The

price of application of a COIL of such power is assumed by specialists to be

50 Ä 60 US$ per a kW h of laser, which makes is unprofitable.

A gas-discharge CO laser has a rather high efficiency (of the order of 40%).

However, for a long-term operation of the industrial CO laser with an open working

cycle and output power of 50 Ä 100 kW, a rather high consumption of cryogenically cooled CO and N2 (of the order of 3 Ä 4 tons/h) will take place. In

addition, the bulky store systems of the components, the system of laser

gas-dynamic pat cooling as well as complex high-power electric devices will be

required. The development of a neutralizing system, which provides ecologically,

permitted CO laser exhaust is of a certain difficulty. And the creation of an

industrial CO laser of similar power with the closed cycle in a mobile variant seems

problematic enough because of high consumption of liquid N2 for heat pick up from

its gas-dynamic path.

The application of gas-discharge CO2-lasers is discussed in two variants: open

and closed cycles. Disregarding a much lower efficiency comprised to a CO laser, a

gas-discharge CO2-laser of the closed cycle is simpler technologically than the

analogous CO laser since its gas-dynamic path is not cooled to cryogenic



396



47 Lasers for Industrial, Scientific and Ecological Use



temperature and heat dissipated by the laser can be removed by means of water heat

exchangers. Here the operation of a gas-discharge CO2-laser of the closed cycle is

fulfilled on the mixture of CO2:N2:HE with helium content of up to 50%, and the

mixture should be renewed in the amount of %1% per each one of its rounds over

the gas-dynamic path. Hence the laser with the power of %100 kW will consume

expensive helium for mixture renovation in the amount not less than 35–40 kg/h,

which makes its operation much expensive. This laser is a more complex than the

analogous one with an open cycle and of much higher weight and overall dimension. That’s why it’s more advantageous in operation under stationary conditions

with a long daily operation cycle where in the first place the level of operation

expenses is. At the same time a gas-discharge CO2-laser of the open cycle is more

suitable for the SCT laser creation.

One of the variants of the mobile non-SSVD industrial CO2-laser of an open

cycle developed in Russia with the power of 50 kW, which operates on the mixture

of CO2 and the atmospheric air. This laser is designed for works on recovery after

accidents in oil and gas wells, operates from on-board components for 10 min and

weights 30 tons. For operation, it requires an external power source of ! 600 kW.

Work components of this laser consume:

• CO2 gaseous

• Fuel (aircraft kerosene)

• Cooling water



1260 kg/h

2700 kg/h

15,000 kg/h



The laser is located on two vehicles and requires a powerful electric power

source (in the field—a mobile electric station). As such, such a laser is not

acceptable for many areas of applications.



47.3



Mobile CO2-AMT GDL



The experience of the developments show that the best weight & overall dimensions with power levels 50 Ä 100 kW have gas-dynamic CO2-lasers (GDL). GDL

is not restricted by a stationary power source and does not require intermediate

transformers from heat energy into the electric one, it does not need additional

systems for spent gases exhaust into the atmosphere, it is rate easy in operation, is

highly reliable and has a long service time. All these factors, make GDL most

suitable for the creation of SCT laser of full value with the application of air as an

oxidizer and sowbelly-spread and low-toxica matter as aircraft kerosene (C12H22)

and toluene (C7H8).

Below can see list of technical parameters of AMT GDL based on reconstructed

RD-33 engine.



47.3



Mobile CO2-AMT GDL



397

AMT GDL



AMT CGDL



Output power, kW

Beam diameter, mm

Mode of operation



! 100

100

Continuous



Wavelength, lm

Angular divergence, rad

Fuel consumption

Laser fuel (toluene), kg/h

Engine fuel (kerosene), kg/h

Sucked air flow rate, kg/s

Bled off air flow rate, kg

Compressed air pressure, MPa

Time of continuous operation, min

Total service life, h

Power unit and laser device overall

dimensions, mm3

Setup weight, kg



10.6

3 Á 10−4



! 100

100

Continuous, high

repetitive pulsed

10.6

3 Á 10−4



1000

2800

70

9

20

30

5000

7000 Â 3000 Â 2500



400 Ä 500

2800

70

5

16

30

5000

7000 Â 2000 Â 3000



7500



7500



It follows from the list that the cost of 1 kW h of laser power in such AMT GDL

are not exceeding 15 US$, which is 4 times lower than for COIL.

It should also be noted that there is a possibility of a more complete reconstruction of RD-33 engine, which allows to bled off up to 14 kg/s of compressed air

under the pressure of 2.3 Mpa. Here the output power of AMT GDL with the same

operation expenses may reach 100 kW.

The AMT GDL is a module structure mounted in standard container. During the

development of this scheme the experience of the creation of autonomous electric

stations based on aircraft engines was applied. The container design allows providing its transportation by all types of vehicle as well as comfortable working

conditions for the personnel.

It is well know that the specific output in a GDL Wsp is determined by the

composition of the active medium at the input of the nozzle unit, its stagnation

temperature, T0, and pressure, p0, the dimension of the restricted section of the

nozzle, hcr, as soon as active area width l and optical resonator parameters. All these

parameters depend on each other.

The calculations of the specific power output, Wsp, of the industrial AMT GDL

were made assuming for the application of an unstable optical resonator. Specific

output for kerosene constitutes 5 and 7 kW/kg with the expansion ratio values of 15

and 23, respectively, and for toluene 7 and 9 kW/kg.

Table 47.1 gives output power values W for some variants of GDL creation.



398



47 Lasers for Industrial, Scientific and Ecological Use



Table 47.1 Output power values W for some variants of fuel for GDL

Fuel



Kerosene

Toluene



p0,

MPa



Nozzle unit

parameters

h/hkp

hkp,

mm



L,

m



0.4

0.4



1.5

2.0



15

23



1.7

2.3



T0, K



1300 Ä 1400

1400 Ä 1500



Flow rate

air,

kg/s



fuel, kg/s



10.0

14.0



0.26 Ä 0.28

0.38 Ä 0.40



W, kW



50 Ä 70

100 Ä 130



As it follows from the given data, the operation of industrial GDL requires the

source of compressed air with the pressure %1.7 Ä 2.3 Mpa and the flow rate of

10 Ä 14 kg/s. Such parameters can be provided by a specially designed compressor

driven by the gas-turbine engine (GTE). The advantage of such an approach is in

the possibility of optimization parameters of the air fed to the laser. For powerful

industrial GDL, operating under stationary conditions, the variant of GTE’s feeding

from a natural gas source can be discussed. This cuts the operation expenses in half.

At present, the structure on the basis of a serial aircraft engine appears to be

more prepared for application. Besides its compressor, it is able to give a portion of

the compressed air required for operation of the laser. In such a case, the aircraft

engine should not only be able to allow to be bled off the required air portion but

also to provide required pressure. A comparative analysis of aircraft engines produced in Russia showed that as a gas-turbine compressor unit of an industrial GDL,

a serial RD-33 engine, can be taken. The engine provides sucked airflow rate of up

to 80 kg/s and the degree of complete pressure increase pk % 22. As the studies

show, it is quite possible to bled off up to 9 kg/s of air heated to %700 K under the

pressure of %20 Mpa after a rather simple reconstruction of this engine [3].

An input ejector is positioned at the engine input, behind the low-pressure

turbine an output ejector is situated that provides the external air pumping through a

heat exchanger where heat pick up from the coolant system of units of the laser

module (flow part of optical resonator, diffuser, resonator mirrors etc.). The input

and output ejectors are of a lobe type because these devices simultaneously fulfil the

function of noise suppressors. In a high-pressure compressor, compressed air is fed

to the laser device, which is located behind the engine. The exhaust laser and engine

gases are sent to the common exhaust device.

The possibility of the application of GDL in the form of industrial laser imposes

a number of specific demands on the structure, which were not met by the developers of laser system before. First of all, this concerns the necessity of continuous

operation during 6–8 h under conditions of multiple switching OFF and ON with

the service life of at least a year without the replacing of any parts and units. This is

achieved by the application of materials capable of operation under the temperatures up to 1500 Ä 1600 K and the application of cooled structures.



47.4



47.4



Efficiency Increase of the AMT GDL …



399



Efficiency Increase of the AMT GDL by Additional

Chemical Pumping



The further development of an idea lying in the basis of GDL has yielded

appearance of the so-called chemical GDL. The latter approach is based on the

optimization of the active medium parameters by the burning process control.

Altering the coefficient a (deviation from stoichiometry) in the various stages of the

process, feeding the fuel, other components into corresponding areas of the combustion chamber, one may control the portion of chemical energy supplied in the

rotational levels and simultaneously decrease the temperature of gas immediately

before the nozzle array.

Investigations demonstrated significant growth of specific energy characteristics

(in particular gain) compared with the conventional GDL; expected advantages of

AMT CGDL are also:

• Smaller consumption of gas and fuel components;

• The temperature of the working gas immediately before the nozzle array may be

decreased to 1000 Ä 1200 K, which essentially simplifies the choice of the

materials, cooling of gas flow path; and the entire lifetime of the laser unit

significantly grows;

• Due to essential lowering of working gas temperature, the extension ratio of a

nozzle and switch pressure of the diffuser (at atmospheric exhaust) may be

diminished; hence the blade becomes more manufacturable and of durable;

• Energy consumption, and weight-overall dimension become smaller significantly.



47.5



High Repetitive Pulsed Regime of the AMT GDL



One of the ways of GDL operation mode control and optimization is based on use

of active intracavity optics. It enables modulation of transparency of the resonator

in the frequency range up to many tens of kHz (30–60 kHz) and thus to form the

required temporal modulation of laser radiation. This problem concerns with the

high power GDL is of an essential interest. The possibility to accomplish such a

mode of operation is considered in details [4].



47.6



New Approach to High Energy Lasers—

Mono-Module Disk Laser



The mono-module disk laser concept is an effective design for diode-pumped

solid-state lasers, which allows the realization of lasers with a super-high output

average power, having very good efficiency and excellent beam quality. Since the



400



47 Lasers for Industrial, Scientific and Ecological Use



first demonstration of the principle in 1964, the output power of mono-module disk

lasers has been increased to the level of a few kW in continuous wave (CW) mode.

“Zig-Zag” disk laser geometry is not, in our opinion, promising for scaling up the

laser output. The scaling laws for the mono-module disk laser design show that the

limits for CW mode are far beyond 100 kW for the output power, and the energy

can be higher than 100 J in pulsed mode. Owing to efficient porous cooling technology and possibility of suppressing amplified spontaneous emission (ASE),

mono-module disk lasers can operate in CW and pulse-periodic (P–P) regimes at

extremely high output powers.

It has long been customary that as new technologies emerge into the light,

potential users and experts start wondering whether these new technologies will

replace the old, well-established approaches to the solution of known problems.

When we look back at the time when the first laser was created, it becomes clear

that each new and more advanced technology usually replaces the pre-existing and

well-proven technologies. However, a more differentiated and balanced assessment

of the many innovations in the field of laser shows that there is no such thing as a

perfect design, or an ideal laser. There is always room for improvement and further

development. It is possible that in the near future a laser with disk geometry of the

active medium will become the dominant technology. However, despite this, a

number of existing laser technologies (with some exceptions, of course) will continue to improve for quite a long time. Based on these considerations, we must

continue to develop most types of lasers, each time clearly specifying their undeniable technological niche and knowing well their advantages and disadvantages.

High efficiency and excellent beam quality of disk lasers means that they can be

widely used in modern science and industry for a very large range of applications,

including treatment of the surface of dielectric materials in microelectronics, cutting, drilling, welding, polishing and cleaning of the surface, and other technological operations with superhard and fragile metals and composite materials, etc.

Pulse-periodic Q-switched disk lasers and high-average-power, mode-locked laser

systems ensure optimal conditions for ablation (sublimation) of a material.

A number of advantages of high repetition rate P–P lasers emitting short pulses, as

applied to a wide range of industrial technologies, is the basis of many modern

concepts of disk lasers. High-intensity light with an insignificant thermal lens effect

in the central highly loaded zone of the active medium has led to the lifting of

restrictions on the brightness of the pump diode. This has reduced the cost of laser

sources, and thus has significantly improved the efficiency of electro-optical conversion, especially in the regime of high average powers. The power of the laser

source is varied by scaling the cross sectional area of the generated radiation. It

should be noted that its ratio to the thickness of the active material in disk geometry

is much larger than the ratio of the cross section of typical core elements of the

active medium to their length in any conventional solid-state laser system. This

eliminates the problems associated with nonlinear distortions of the geometry of the

active medium, and enables realization of super high peak and average powers of

laser sources with disk geometry and same parameters of radiation in the far-field

region.



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