as pointed out above , the present invention overcomes the problems of size and expense involved in present day laser systems using long chain amplifiers . the invention achieves this by the use of a regenerative amplifier cavity wherein a low energy pulse switched into the cavity is amplified by many passes through an amplification medium within the cavity to achieve the desired gain . the &# 34 ; round trip &# 34 ; path length for the pulse is long ( as for example , 10 - 1000 meters or more ) to allow for possible repetitive pumping of the amplification medium and to allow the plasma formed within the spatial filter pinhole to clear between successive passes . the apparatus provides for long transit times through long path lengths . after the desired gain has been reached , the amplified pulse is switched out of the cavity to a point of use . referring now to the drawings , fig1 illustrates a preferred embodiment of a large injection locked regenerative amplifier laser system which is basically composed of a pair of separated reflector members or mirrors 10 and 11 , a pinhole spatial filter assembly 12 positioned centrally between mirrors 10 and 11 , a polarizer assembly 13 between mirror 10 and filter assembly 12 , a laser amplifier assembly 14 intermediate to mirror 11 and filter assembly 12 , and a pockels cell or switch assembly 15 positioned between amplifier assembly 14 and filter assembly 12 . by way of example , mirrors 10 and 11 are positioned 5 - 1000 meters apart and have a diameter or cross - sectional distance of 0 . 2 - 10 . 0 meters or even more if useful . also , the mirrors could be segmented to simplify fabrication . spatial filter assembly 12 is located at the beam waist in the cavity formed by mirrors 10 and 11 and may be constructed as is known in the art with a central member having a pinhole 16 . the fig1 laser system , if of a short length ( less than 3 meters ) will operate under atmospheric conditions except for the spatial filter assembly . for the long length , large devices ( 3 meters to 1000 meters ) it is necessary to enclose the system in a casing or housing , and evacuate it to a pressure in the 0 . 1 - 10 torr range . a special case of the preferred embodiment of fig1 described in the paragraph above is the concentric resonator wherein the reflector members 10 and 11 form an optical relay . the optical relay concept allows a regenerative amplifier to maintain high fill factors , to suppress diffraction effects , and to minimize phase distortion . the concentric resonator case of fig1 is the only fully relayed stable resonator made up of two identical mirrors . a more general treatment of the optical relay as applied to the regenerative amplifier is disclosed in ser . no . 868 , 642 , &# 34 ; a fully relayed regenerative amplifier &# 34 ; by alexander j . glass , filed on the same day as this application , assigned to the assignee of this application , and incorporated by reference herein . while the fig1 embodiment illustrates a two sided ( ended ) resonator arrangement , it is not intended to limit the invention to such a configuration , since three or four sided resonators will offer much greater flexibility in placement of pockels cells , spatial filters , polarizers , and amplifiers . also , it is understood that another laser amplifier assembly could be utilized on the opposite side of the spatial filter assembly . the spatial filter assembly is located at the beam waist , which is the region of minimum beam diameter between two focusing elements of a resonating cavity . in addition , the location of the pockels cell and polarizer or other switching means may be on the same side of the spatial filter and located in interchanged positions . many - sided resonator configurations with open optical paths are disclosed in ser . no . 868 , 640 , &# 34 ; multiple pass laser amplification for fusion applications with near - field or far - field optical separation &# 34 ; by wilhelm f . hagen , filed on the same day as this application , assigned to the assignee of this application , and incorporated by reference herein . the problems associated with the laser system of fig1 are outlined as follows and individually discussed hereinafter : while not shown , it will be necessary to servo control the mirrors 10 and 11 and possibly the spatial filter assembly 12 . such servo control means are known in the art and thus need not be described herein . the frequency response of the large optical components is very low and thus is little different than on the currently used long chain amplifier systems . as pointed out above , for short length systems , the laser can operate in the atmosphere except at the spatial filter , but for large , long length systems a vacuum enclosure must be utilized for the regenerative cavity . this may be readily accomplished by two methods , graphically illustrated in fig3 and 4 , respectively . the first method or approach ( fig3 ) is to break up the gain medium in transverse direction with appropriate absorbers . for example , in a glass amplifier , one would divide the amplifier disk into small segments as illustrated in fig2 such that disk 20 is composed of a plurality of segments 21 with each segment being about 15 to 30 cm , for a nd : glass disk having an overall disk size of 2 × 4 meters . other composite amplifier designs are disclosed in ser . no . 868 , 641 , &# 34 ; staggered amplifier configuration for laser fusion amplifier chains &# 34 ;, by wilhelm f . hagen , filed on the same day as this application , assigned to the assignee of this application , and incorporated by reference herein . also , the disk segments could be separated along the beam axis , if desired . between the disk segments an absorbing glass 22 , such as those doped with copper oxide , or samarium is used , which also fuses the segments together . this absorbing glass can be about 1 mm thick and functions to suppress parasitic oscillation or amplified fluorescence . such a thickness will intercept less than 1 % of the beam , and thus it will be a small loss . similar approaches could be used with gas laser amplifier systems under certain conditions . the interference pattern arising from this obstruction will diffract away or be eliminated by the spatial filter . one method and apparatus for joining composite amplifier disks is disclosed in ser . no . 868 , 643 &# 34 ; composite solid state laser amplifier discs &# 34 ; by james a . glaze , filed on the same day as this application , assigned to the assignee of this application and incorporated by reference herein . the second approach or method ( fig4 ) is to use the regenerative feature of the system to keep the gain below the parasitic limit naturally and is particularly suited to very long resonators ( like 1 km ) where the round trip transit time can be in the 1 - 15 μsec region . this approach also looks attractive for gas lasers with shorter pump times and shorter resonators , where repumping of the laser medium can occur . it is clear that from the wide variety of resonator configurations that can be designed around the basic concept of this invention , the mirrors , polarizers and amplifiers can be located at positions consistent with their damage limits or saturation fluxes . it is quite clear that there are a wide variety of ways of accomplishing this , such as rotating optics , phase shifting a mirror , evanescent wave coupling , faraday rotators , pockels cells , etc . small systems can easily use pulsed rotators , however , at meter apertures one would have to switch megajoules in microseconds . for a large , long ( 1000 meter ) length system , for example , a pockels cell can be used which is built up as illustrated in fig5 driven with alternating polarity strip transmission lines 30 and 31 positioned between crystal bars 32 . for active material , crystalline quartz or adp ( ammonium di - hydrogen phosphate ) may be used . crystalline electrooptic materials like adp are typically available in pieces up to 10 cm in diameter , so the segmented pockels cell could be composed of such pieces in the array as shown in fig5 . note that there is no need for a large linear or quadratic electro - optic coefficient since one or both switch slowly ( compared to 1 ns ) and use 100 - 200 kv with ease , and thus economical materials can be used . as an example , glasses can be made , which can be heat treated to precipitate crystals and which show linear or quadratic electro - optic effect . the crystals are allowed to reach 50 - 100 a in size and thus will not scatter light . if linear materials are precipitated , they will have to be oriented ( by nucleation in an electric field , stress field , etc .). with quadratic materials ( para electric or ferroelectric ), one only needs to orient the domains by poling the material as is done with ceramics . such materials are described in greater detail in applied physics letter , vol . 7 , no . 5 , sept . 1 , 1965 , &# 34 ; electrooptics effect of ferroelectric microcrystals in a glass matrix &# 34 ;, by n . f . borelli et al . thus , such materials can be made if adp or quartz is too costly or otherwise inappropriate . note again that the spatial filter removes the interference pattern caused by the strip transmission line obscuration . since the joints of the segmented pockels cell of fig5 will require protection from the laser beam , an array of fused silica wires may be utilized as illustrated in fig6 ( only one set shown ) wherein a joint 40 between two transparent members 41 and 42 has a pair of fused silica wires 43 positioned in spaced relation on opposite sides of joint 40 . the wires 43 are shaped in cross - section like a lens and diverge the laser light to lower the flux on the joint 40 . the resulting pattern will diffract away rapidly . the wires 43 , for example , may have a cross - sectional width of about 1 mm and may be located about 1 cm from the joint 40 . the polarizer assembly 13 and the pockels cell 15 function , as is known in the art , to inject a low energy signal or pulse (˜ 1 joule ) from an externally located source , such as a laser oscillator , into the regenerative cavity , as indicated at 17 , wherein the input pulse 17 is amplified by multiple passes through the cavity . after the pulse has reached saturation intensity ( net gain ) it is deflected or switched out of the cavity as indicated at 18 to a point of use . during amplification of the input pulse in the regenerative amplifier cavity , the polarizer and pockels cell are in an inactivated state , such that they pass the pulse through undeviated in direction , or deviated by a fixed and controlled amount , depending on the cavity component configuration . with this pulse switching arrangement , the input signal or pulse may be 10 - 8 to 10 - 11 of the output pulse or stated differently , the gain of the repetitive amplification is 10 8 - 10 11 . accordingly , it is readily seen that the cavity may be switched at high voltages by electro - optical crystals with low electro - optic coefficients . also , due to the length of the resonant cavity , there is a time span of up to 1 μsec for switching time of the pockels cell thus further reducing switch problems . the input signal can be injected as indicated by reflection off the polarizer , or by any other means known in the art , capable of providing a suitable insertion of optical energy in the cavity . other means of switching , such as faraday rotators , can also be adapted to large aperture , segmented systems . the real interest in a long resonator comes from the need to have the plasma formed at the spatial filter completely clear of the aperture before the next pulse . for systems operating at f / 100 to f / 1000 , the pinhole size runs from 0 . 1 to 3 . 0 cm . in addition , the depth of field of the focus is quite long , so we can distribute the spatial filter in such a way that it can be both long in the z direction , as well as segmented in the θ direction if necessary . a helix as illustrated in fig7 may be desired as it could be continuously fed into the filter if shot to shot erosion is excessive . also , the spatial filter may be composed of a multiple series of pinholes as illustrated in fig8 . it has been determined that with a long cavity transit time of a km length cavity , a rotating wheel at an external focus is fast enough to give complete prepulse isolation . also , saturable absorbers can suppress any prepulse emitted by the input signal oscillator or any parasitic pulse issuing from the amplifier . consider a nd : glass amplifier system with a 1 meter beam diameter . assuming use of two disks 100 cm × 200 cm × 10 cm with an index nonlinearity n 2 ≈ 0 . 7 × 10 - 13 esu on each side of the spatial filter ( 4 disks total ), by either method of transverse gain control , we can achieve a stored energy density of 0 . 5 j / cm 3 , and thus have stored 315 kj . since the resonator is long ( 1 km ), the terminal level completely relaxes to the ground state between passes , so almost all of the stored energy is extracted , about 250 kj . if one limits the nonlinear phase distortion to a value of 2 . 5 radians between filters , one has approximately 150 tw ( tw = terawatts ) output power . for a fill factor ( the ratio of illuminated area to total aperture area ) of 0 . 6 , we have 150 kj and 90 tw , which is roughly half the output of the above referenced large , multiple chain amplifier laser system ( shiva / nova ). shiva / nova has an output of 5 . 7 kj and about 5 tw in each chain . note also that only 30 mj or less is required to pump the system . another example is to use the two 30 cm disk output amplifiers ( such as proposed for shiva / nova ) on either side of the spatial filter , as shown in fig1 . again , assuming an n 2 of 0 . 7 × 10 - 13 esu and a gain coefficient 0 . 045 cm - 1 , one has 7 . 2 kj stored energy . of this , one can extract 5 kj at a peak power of 10 . 5 tw . the required pump energy is 900 kj , so that 50 of these will provide 250 kj and over 500 tw , with a 45 mj pump . another choice would be to use 6 nd : glass amplifier disks which would yield 7 . 5 kj and 7 . 5 tw . with 50 devices in parallel , the output would be 375 kj and 375 tw , with a pump requirement of 70 mj . in each case presented , the overall efficiency is 0 . 5 %, much more efficient than present chain designs . it has been shown that a mode matched pulse of as little as 10 - 11 of the output is sufficient to lock the regenerative amplifier . thus the system described herein should operate with a 1 μ ( mj ) drive pulse . by providing at the most a one joule drive pulse , stability of operation could be ensured . while the above description has been primarily directed to nd : glass amplifiers , other amplifiers may use a lasing medium of a vapor or a gas which when excited by means such as electron beam systems produces xebr *, xef *, krf *, krcl *, xe 2 *, kr 2 *, or ar 2 *, with a total gas pressure of typically ˜ 1 atmosphere . this gain medium would be repetitively and synchronously pumped by an electron beam or flashlamp to provide temporary energy storage of narrowband , short wavelength fluorescence energy which is quickly extracted by the laser pulses passing therethrough . the energy storage time need only be of the order of τ r ˜ 30 nanoseconds if the gain medium is pumped immediately before the laser pulse passes therethrough . the gain per single pass through the gain medium may be of the order of 20 db ; after a small number of passes (˜ 2 - 10 ) through the medium , the laser pulse reaches saturation . after this , the circulating laser pulse efficiently extracts optical energy from the amplifier during each pass and thus grows in amplitude . associated gain medium efficiency is of the order of 4 - 10 %. for more information on multiple excitation , see ser . no . 868 , 639 , multiple excitation regenerative amplifier inertial confinement system , by e . victor george et al ., filed on the same day as this application , assigned to the same assignee as this application , and incorporated by reference herein . referring now to the fig9 embodiment of the regenerative amplifier laser system , which is generally similar to the fig1 embodiment except for the positioning of the polarizer and the pockels cell and the addition of a second laser amplifier assembly , each amplifier assembly is composed of a pair of tilted disks , positioned on the opposite side of the spatial filter assembly . accordingly , like components are given similar reference numerals corresponding to the fig1 embodiment . to provide an upper bound to performance of large regenerative amplifier laser systems using nd : glass , the following calculations and values are set forth : the maximum energy storage density e d one can achieve in a large disk is ## equ1 ## where h = planck &# 39 ; s constant the factor 2 is an approximation for ## equ2 ## where n is the index of refraction and t the thickness of an individual disk . n is a factor for a segmented disk which is the ratio of the long axis of the full disk to the maximum dimension of a small segment . thus , the maximum available output energy is ## equ3 ## where a is the fill factor (≦ 1 ) to calculate the maximum power capability , it is assumed that half of the laser glass is on each side of the spatial filter , as illustrated in fig1 . the upper limit for i p is set by the b integral as follows : thus ## equ4 ## assuming that we will have a b = 2 in the laser glass , take ## equ5 ## and b = 0 . 5 for the pockels cell . and makes these normalizations ## equ8 ## one obtains ## equ9 ## where d is in meters . the following are four examples of parameters for laser systems , embodied in this invention , based in part upon the values and calculations set forth above : table 1__________________________________________________________________________ examples a b c d__________________________________________________________________________no . of beams 1 1 6 10e . sub . max ( kj ) 4 14 1 , 000 10 , 000p . sub . max ( tw ) 6 14 300 1 , 000beam diameter ( meters ) 0 . 3 0 . 5 1 . 2 2 . 5n = 1 1 2 4l ( meters ) . 16 0 . 2 0 . 33 0 . 75σ ( cm . sup . 2 ) 2 . 7 × 10 . sup .- 20 1 . 5 × 10 . sup .- 20 1 × 10 . sup .- 20 1 . 4 × 10 . sup .- 20n . sub . 2 ( esu ) 1 . 4 × 10 . sup .- 13 1 . 4 × 10 . sup .- 13 1 . 3 × 10 . sup .- 13 1 . 4 × 10 . sup .- 13gain ( single pass ) 2 . 1 1 . 84 2 . 28 6 . 5max flux density ( surface )( j / cm . sup . 2 ) 4 . 5 5 . 7 11 . 9 16 . 1max flux density ( bulk )( j / cm . sup . 2 ) 5 . 39 6 . 8 14 . 3 19 . 4characteristic pulseduration ( ns ) 0 . 7 1 3 10__________________________________________________________________________ further details of the four examples of this invention presented in table 1 are : a single regenerative amplifier is envisioned , with an output beam diameter of 0 . 3 m . an unsegmented disk amplifier with a single pass gain of 2 . 1 is used to amplify a 0 . 7 ns seed pulse . it is assumed that the four amplifier disks are made of owens - illinois ed - 2 laser glass . up to 4 kj and 6 tw can be extracted from this device . a device similar to example a is envisioned , but with an aperture diameter of 0 . 5 m . an unsegmented amplifier uses an amplifying medium of a glass with the non - linear index coefficient of ed - 2 , but with a lower stimulated emission cross - section . in 1 ns , up to 14 kj and 14 tw can be extracted . a device consisting of six regenerative amplifiers of 1 . 2 m diameter is envisioned . the amplifiers employ disks composed of two segments , using a glass with the nonlinear index of ed - 2 , but a cross - section for stimulated emission of less than half the value for ed - 2 . in a 3 ns pulse , up to 1 mj and 300 tw can be extracted . a device with 10 regenerative amplifiers , each employing disks made up of four segments with a final aperture of 2 . 5 m is envisioned . with the cross - section of stimulated emission about half that of ed - 2 , and the index nonlinearity the same as ed - 2 , an output of up to 10 mj and 1000 tw can be achieved . further development of glasses with a low cross - section for stimulated emission and low index nonlinearity , will allow even further improvements in the performance of regenerative amplifier devices , shown in fig1 , where the parameters , other than σ , are those of example b above . it has thus been shown that the present invention provides a simple high energy laser system using large regenerative amplifier arrangements , while reducing the cost over the currently known chain amplifier laser systems by 10 - 15 %. the laser system may be used for various high energy applications , of which just a few are plasma confinement and heating systems , production of charged particles , production of neutrons , laser fusion systems , communication systems , fabrication systems , and the like . related copending applications which are filed on the same day as this application , assigned to the assignee of the application , and are incorporated by reference herein , are as follows : ser . no . 868 , 633 , tunable , rare earth - doped solid state lasers , by john l . emmett et al ., wherein an excimer pump laser with a rare earth - doped solid matrix utilizes a 5d - 4f radiative transition in a rare earth ion to produce visible and ultra - violet laser radiation with a possible high overall efficiency and a relatively long radiative lifetime . ser . no . 868 , 638 , repetitively pumped electron beam device , by leland g . schlitt , wherein fast , repetitive , electron beam pulses are produced by phased energy storage in a finite length transmission line . while particular embodiments and examples of the invention have been illustrated and described , other possible examples and embodiments as well as modifications and changes will be apparent to those skilled in the art , and the inventor &# 39 ; s intention is to cover in the appended claims all such examples , embodiments , modifications , and changes as come within the spirit and scope of the invention .