Multi-output chirped amplification chain

Abstract

An M-output, where M>1, chirped pulse amplification chain that includes a stretcher of stretching factor tx_stretch, M amplifiers in cascade, M output compressors respectively placed at the output of each amplifier, wherein it comprises: a partially compressing device placed between the stretcher and the first amplifier, this partially compressing device having at least one partial compression factor, the one (or more than one) partial compression factor(s) being lower than tx_stretch, and an optical switch configured to receive a beam output from the stretcher and to direct it directly to the first amplifier of the cascade or to the partially compressing device depending on the output compressor chosen among the output compressors.

Claims

1. An M-output, where M>1, chirped pulse amplification chain that comprises: a stretcher of stretching factor tx stretch, M amplifiers in cascade, M output compressors respectively placed at the output of each of the M amplifiers, further comprising: a partially compressing device placed between the stretcher and a first amplifier of the M amplifiers, said partially compressing device having at least one partial compression factor, one or more of said at least one partial compression factor(s) being lower than tx_stretch, and an optical switch configured to receive a beam output from the stretcher and to direct said beam output directly to the first amplifier of the cascade or to the partially compressing device depending on an output compressor chosen among the M output compressors.

2. The amplification chain as claimed in claim 1, wherein M>2, and wherein the partially compressing device includes a partial compressor of adjustable compression factor.

3. The amplification chain as claimed in claim 2, wherein the partial compressor includes at least one translationally motorized diffraction grating.

4. The amplification chain as claimed in claim 1, wherein M>2, and wherein the partially compressing device includes L diffraction-grating-comprising partial compressors, 1<L<M, each partial compressor having a constant compression factor.

5. The amplification chain as claimed in claim 1, configured to amplify a pulse of duration shorter than 100 fs.

6. A method for using a pulse amplification chain as claimed in claim 1, the method comprising the following steps: stretching a pulse with the stretcher, depending on a chosen output compressor chosen among said M output compressors, sending the pulse to the partially compressing device via the optical switch or passing directly to the following step, sending the pulse through the cascade of M amplifiers from the first amplifier to one of the M amplifiers associated with the chosen output compressor, sending the pulse to said chosen output compressor.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) Other features and advantages of the invention will become apparent on reading the following detailed description, which is given by way of nonlimiting example with reference to the appended drawings, in which:

(2) FIG. 1, which has already been described, schematically shows a single-output chirped amplification chain according to the prior art,

(3) FIG. 2, which has already been described, schematically shows a multi-output chirped amplification chain according to the prior art,

(4) FIG. 3, which has already been described, schematically shows an example of a prior-art stretcher,

(5) FIG. 4 schematically shows an example of a prior-art compressor,

(6) FIG. 5 schematically shows a multi-output chirped amplification chain according to the invention,

(7) FIG. 6 schematically shows an example of a constant-factor partial compressor of an amplification chain according to the invention,

(8) FIG. 7 schematically shows a first example of an adjustable-factor partial compressor comprising a folding dihedron, of an amplification chain according to the invention,

(9) FIG. 8 schematically shows a second example of an adjustable-factor partial compressor comprising two pairs of diffraction gratings, of an amplification chain according to the invention.

DETAILED DESCRIPTION

(10) In all the figures, elements that are the same have been referenced with the same references.

(11) As indicated in the preamble, an amplification chain essentially includes a stretcher, an amplifier and a compressor. A stretcher and compressors that comprise diffraction gratings are considered.

(12) Stretchers and compressors are similar: a stretcher is a compressor with a negative equivalent distance between its diffraction gratings, which distance is produced by an optical system of −1 magnification, hence the convention mentioned in the preamble.

(13) An example of a stretcher 10 comprising two diffraction gratings 11, 12 is shown in FIG. 2. It is also possible to use a stretcher comprising a single diffraction grating. The principle of a stretcher comprising a single diffraction grating is the same, but the single grating is placed far away from the center of curvature of the Offner triplet.

(14) The stretcher 10 is characterized by the following geometric parameters:

(15) The distance between the 2 gratings: G_ETR. In the case of a stretcher with a single diffraction grating, G_ETR is two times the distance between the diffraction grating and the center of curvature of the Offner triplet.

(16) The angle of incidence on the 1 st grating 12 (or on the single grating): θ_ETR.

(17) The groove density of each grating: N_ETR.

(18) As already indicated, it is possible to achieve 1 or more passages through the stretcher.

(19) The stretching factor is:

(20) $\mathrm{tx\_stretch}=\frac{2.Math.\mathrm{G\_ETR}.Math.\lambda 0.Math.{\mathrm{N\_ETR}}^2.Math.\mathrm{nbre\_pass}\mathrm{\_ETR}}{c.Math.{\cos }^3\left(\theta \mathrm{d\_ETR}\right)}$
where:
λ0=the average wavelength of the spectrum of the pulse,
c=the speed of light,
θd_ETR=the 1st-order angle diffracted by the first grating 12 (or the single grating) for the wavelength λ0, which is given by the formula:
sin(θd_ETR)+sin(θ_ETR)=λ0N_ETR

(21) A diagram of a compressor 30.sub.i is shown in FIG. 4. This compressor includes two pairs of diffraction gratings 31.sub.i, 32.sub.i, and 33.sub.i, 34.sub.i. The four gratings all have the same number of grooves per mm. The gratings 31.sub.i and 34.sub.i have the same dimensions; likewise for the gratings 32.sub.i and 33.sub.i, but the dimensions of the latter may be larger than those of the gratings 31.sub.i and 34.sub.i. The pulse 5 incident on the first grating 31.sub.i is diffracted toward the second grating 32.sub.i parallel to the first. It is diffracted by this second grating, which sends it to a third grating 33.sub.i, which diffracts it toward a fourth grating 34.sub.i. At the exit of this 4th grating 34.sub.i, the duration of the pulse 5 has been compressed.

(22) The geometric parameters of a compressor are: the distance between the 2 gratings of each pair: G_CPR, the angle of incidence on the 1st grating: θ_CPR, the groove density of the gratings: N_CPR.

(23) The compression factor is:

(24) $\mathrm{tx\_compression}=\frac{2.Math.\mathrm{G\_CPR}.Math.\lambda 0.Math.{\mathrm{N\_CPR}}^2}{c.Math.{\cos }^3\left(\theta \mathrm{d\_CPR}\right)}$ θd_CPR, the angle diffracted by the first grating for the wavelength λ0, is given by the formula:
sin(θd_CPR)+sin(θ_CPR)=λ0N_CPR

(25) The spectral phase of the stretcher and of the compressor are exactly opposite if:
G_CPR=G_ETR×nbre_pass_ETR
θ_CPR=θ_ETR
N_CPR=N_ETR.

(26) In the ideal case where no dispersive material is placed in the amplification chain the spectral phase is zero and the laser pulse is transform-limited, i.e. its duration is the shortest theoretically possible. Of course, the laser beam of an amplification chain passes through dispersive materials, amplification crystals for example. However, the stretching factor of such dispersive elements is negligible with respect to the stretching factor of the stretcher or of the compressors; the stretching factor (or equivalently the spectral phase) introduced by these dispersive elements is therefore neglected here.

(27) According to the invention, a partially compressing device 50 is placed between the stretcher 10 and amplifier No. 1 (20.sub.1).

(28) An example of an M-output chirped amplification chain 100 according to the invention is described with reference to FIG. 5.

(29) It comprises:

(30) a stretcher 10, connected to an

(31) optical switch 40, connected to

(32) a partially compressing device 50 the function of which is to be able to match the stretching factor to the compression factor of each output compressor, and

(33) to a first amplifier 20.sub.1 associated with a first output compressor 30.sub.1, other amplifiers 20.sub.2, . . . , 20.sub.M, all the amplifiers 20.sub.2, . . . , 20.sub.M being placed in cascade, each other amplifier 20.sub.2, . . . , 20.sub.M being associated with one other output compressor 30.sub.2, . . . , 30.sub.M. The compression factors of the output compressors increase with rank, the last compressor, compressor M, having the highest compression factor.

(34) Depending on the chosen output, the laser pulse output from an amplifier 20.sub.1, . . . , 20.sub.M−1 is directed either to the compressor associated with this amplifier, or to the following amplifier, via an optical switch (not shown in the figure) placed at the output of each amplifier except the last one.

(35) The optical switch 40 (and optionally the switches at the outputs of the amplifiers) is an optical invariant. It may be a retractable system of mirrors that comprises two parallel mirrors mounted on one and the same motorized translatable element, or a mirror mounted on a rotatable stage in order to address the partial compressor or to avoid it. Thus the partially compressing device may be selected or avoided depending on the position of this system of mirrors.

(36) A plurality of configurations are envisioned for the partially compressing device 50, depending on the compression factors of the output compressors.

(37) The following are defined:

(38) tx_stretch_resist_flux: minimum stretching factor of the stretcher 10 required

(39) for the optics of the laser amplification chain to withstand the flux. tx_stretch(i) the stretching factor of the stretcher 10 required to both limit vignetting in compressor No. i (compressor 30.sub.i) and to guarantee that the optics of the laser amplification chain upstream of this compressor, i.e. compressor No. i, are able to withstand the flux; therefore:
tx_stretch(i)>tx_stretch_resist_flux
and as the energy received by compressor No. i is higher than the energy received by compressor No. i−1 (compressor 30.sub.i−1):
tx_stretch(i)>tx_stretch(i−1).

(40) Regarding compressor No. M, it is vignetting that constrains the distance between the gratings of this compressor, compressor No. M (i.e. compressor 30.sub.M) rather than the flux resistance of the optics of the various laser amplifiers 20.sub.1 to 20.sub.M.
tx_stretch_max=max[tx_stretch(i)]=tx_stretch(M).
The stretching factor of the stretcher 10 is tx_stretch_max.
tx_compression_partial, the compression factor of the partially compressing device 50, which is a parameter to be optimized.

(41) For outputs i that respect:
tx_stretch(i)<tx_stretch_max−tx_compression_partial
the laser beam output from the stretcher 10 is directed to the partially compressing device 50 by the optical switch 40.

(42) For the other outputs (such that tx_stretch(i)>tx_stretch_max−tx_compression_partial), the laser beam output from the stretcher 10 is deviated by the optical switch 40 in order to avoid the partially compressing device 50; the beam is deviated directly to amplifier No. 1. This is in particular the case for the last output (=output of compressor No. M).

(43) Thus, the laser pulse passes firstly through the stretcher 10. Depending on the No. i output used, i varying from 1 to M, either the pulse is sent to the partially compressing device 50, or it is sent directly to the following stage.

(44) The laser pulse then passes through the series of amplifiers 20.sub.1 to 20.sub.i. It is then deviated toward the compressor 30.sub.i. It does not pass through the amplifier 20.sub.i+1.

(45) The various compressors of the various outputs have geometric parameters equivalent to those of the stretcher: θ_CPR(i) and N_CPR(i) are close to the parameters θ_ETR and N_ETR of the stretcher. They are equal in theory but close in practice on account of the dispersive materials (the amplification crystals for example) between the stretcher and compressors. Their inter-grating distance G_CPR(i) is set depending on the desired compression factor.

(46) The partially compressing device is for example a Treacy compressor 50a described with reference to FIG. 6 with geometric parameters equivalent to those of the other compressors 30.sub.i and of the stretcher 10: same θ_CPR, same N_CPR. It comprises:

(47) A first diffraction grating 51a, a second diffraction grating 52a. The gratings 51a and 52a have the same number of grooves, they are parallel and their grooves are parallel to one another. They may be of different size, typically the width of 52a is larger than that of 51a. A dihedron 60a allows the laser rays to be redirected toward 52a and their height to be changed. The laser rays therefore pass in order through sur 51a, 52a, 60a, 52a and 51a.

(48) The distance G_CPR_partial(i) is about:
G_CPR_partial(i)=G_ETR×nbre_pass_ETR−G_CPR(i).
The compression factor of the partial compressor, i.e. tx_compression_partial, may be deduced therefrom. It is also possible to write: tx_compression_partial (i)=tx_stretch(M)−tx_stretch(i).

(49) When intermediate output compressors Nos. 1 to M−1 (compressors 30.sub.1 to 30.sub.M−1) all have the same compression factor, the partially compressing device 50 typically includes a single partial compressor 50a of constant compression factor, one example of which is shown in FIG. 6.

(50) When compressors Nos. 1 to M−1 do not have the same compression factor (compressors with increasing compression factors), the partially compressing device 50 may include a plurality of partial compressors, typically as many partial compressors as there are compressors 30.sub.i of different compression factors. The partial compression factor of each of these partial compressors is constant and set depending on the one (or more than one) output compressor(s) that correspond thereto. These partial compressors are arranged in parallel.

(51) According to one alternative, the partially compressing device 50 includes one (or more than one) partial compressor(s) the compression factor of which is adjustable depending on the corresponding output compressor. This adjustable factor is for example obtained using a compressor: the second diffraction grating 52a of which is translationally motorized in the direction of the middle ray corresponding to the wavelength of the center of the spectrum between 51a and 52a in the case of a compressor 50a comprising two gratings+a folding dihedron, one example of which is shown in FIG. 7, the dihedron 60a then being over-dimensioned for the same reasons as the stretcher shown in FIG. 2, or the second and third diffraction gratings 52b, 53b of which are translationally motorized in the direction of the middle ray corresponding to the wavelength of the center of the spectrum between 52b and 53b in the case of a compressor 50b comprising two pairs of gratings 51b, 52b, 53b, 54b as shown in FIG. 8.

(52) This amplification chain according to the invention makes it possible both to avoid having to motorize a diffractive component of the stretcher and to use intermediate compressors (compressors 30.sub.1 to 30.sub.M−1) that are as compact as possible.

(53) An example embodiment having the following specifications is described below:

(54) Gaussian spectrum centered on 800 nm, of full width at half maximum of 60 nm.

(55) The vignetting of the 720-890 nm spectrum must be minimized.

(56) 3 laser amplifiers with Ti:Sa crystals pumped with lasers at 532 nm.

(57) 3 output compressors (one after each laser amplifier).

(58) minimum stretching factor: tx_stretch_resist_flux=9.58 ps/nm. This stretching factor allows damage to the optics of the laser amplifiers to be prevented.

(59) Parameters of the amplifiers:

(60) TABLE-US-00001 ampli output CPR output energy (J) energy (J) output 1 3.6 2.5 output 2 35.7 25 output 3 357.1 250

(61) It is chosen to work with compressors based on conventional holographic gratings, with 1480 grooves/mm.

(62) The angle of incidence is chosen in the vicinity of 56° (compromise between effectiveness of diffraction in the useful spectral band, and limitation of vignetting).

(63) The maximum fluence for the holographic diffraction gratings is in the vicinity of 110 mJ/cm.sup.2.

(64) The following diameters at the input of the 3 compressors are obtained:

(65) TABLE-US-00002 CPR input diameter (mm) area (cm.sup.2) compressor 1 48 18 compressor 2 152 182 compressor 3 481 1816

(66) The distance G_CPR(3)=980 mm is set to limit vignetting in compressor No. 3.

(67) The compression factor of compressor No. 3 is 14.1 ps/nm. It is therefore higher than necessary to merely ensure flux resistance, i.e. higher than tx_stretch_resist_flux=9.58 ps/nm.

(68) According to the invention, the stretcher is designed to have the same stretching factor as the compressor M at the end of the chain, in the present case compressor No. 3.

(69) When output 1 or 2 is used, the laser pulse is sent from the stretcher to a partially compressing device in order that the stretching factor of the stretcher (14.1 ps/nm) minus the factor of the partially compressing device (4.52 ps/nm) is equal to tx_stretch_resist_flux (9.58 ps/nm).

(70) The parameters of the various elements are:

(71) TABLE-US-00003 Nbre stretching θ_ETR N_ETR G_ETR pass factor (ps/nm) Stretcher 56° 1480 grooves/mm 490 mm 2 14.10 Compression θ_CPR N_CPR G_CPR factor (ps/nm) Partial CPR 56° 1480 grooves/mm 314 mm 4.52 CPR1 56° 1480 grooves/mm 666 mm 9.58 CPR2 56° 1480 grooves/mm 666 mm 9.58 CPR3 56° 1480 grooves/mm 980 mm 14.10
Compressor 3 is therefore clearly the most voluminous.

(72) In this example, compressors 1 and 2 have the same compression factor; the partially compressing device then includes a single compressor of constant factor.