• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The subject of the invention is a system for phasing laser sources with a periodic configuration, comprising: means for collimating and directing the beams coming from the sources onto a periodic phase grating diffractive optical element (1), with an angle of incidence that is different from one beam to another, these angles of incidence being determined as a function of the period of the grating; means for controlling the phases of said sources from a feedback signal from the recombined beams, - means (5) for taking a fraction (12) of the recombined beams, - on the path of this fraction of the beams, a Fourier lens (6), with the recombination optical diffractive element (1) in its object plane, - a matrix of detectors (7) in the image plane of the Fourier lens (6), able to detect intensity distributions, - means (8) for calculating the counter signal -action from these distractions ibutions of intensity.
    公开号:FR3021761A1
    申请号:FR1401222
    申请日:2014-05-28
    公开日:2015-12-04
    发明作者:Jerome Bourderionnet；Arnaud Brignon
    申请人:Thales SA；
    IPC主号:
    专利说明:

    [0001] BACKGROUND OF THE INVENTION 1. Field of the invention is that of the coherent recombination of a large number of elementary laser sources.
    [0002] The coherent recombination of laser sources applies in particular to the production of high power laser sources, and / or high energy in the case of ultra-short pulse sources, for example of pulse width less than one picosecond. Obtaining laser sources of high power (or energies) lo and large luminances is today limited by the flow resistance of the gain materials. One solution to this problem is to spread the amplification over several gain media in parallel. This requires that the laser beams at the output of each gain medium are in phase so as to ensure optimal coherent recombination of all the laser beams. It is therefore necessary to dynamically compensate for the delays introduced on a large number of laser beams M by the propagation through a set of gain media (fiber amplifiers for example) in parallel. Once locked in phase, the M emerging laser beams interfere constructively and thus constitute a source of luminance M times greater than that of an elementary amplifier, while keeping its beam quality (limited by diffraction in the case of monomode fibers by example). It is therefore a question of setting up as many phase locked loops as transmitters. The phasing architectures of laser sources can be classified according to several criteria. The first is the way in which the beams are spatially recombined, or superimposed. Two families can be distinguished: - Tiled aperture: the M laser beams are collimated and have parallel propagation directions.
    [0003] This recombination mode is the optical equivalent of the radar beamforming antenna. The far field then has an intense central lobe, and parasitic secondary lobes. - Close-field recombination ("filled aperture"): the M beams are superimposed in the near field, using polarizers or a diffractive optical element (or "DOE"), the acronym for the Diffractive Optical Element. The advantage of the near-field recombination method is its efficiency, since in this case there are no side lobes in the far field. Then comes the nature of the error signal, and the treatment that will allow to counter-react on the phases between laser sources, and optimize their coherent addition. There are basically 4 methods of coherent recombination of laser beams, classified according to the amount of information contained in the feedback signal: The so-called hill climbing method: the error signal is simply constituted by the sampling of a fraction of the recombined energy, which is maximized by playing on the phases of the M channels (beams) to be recombined. This technique is based on a gradient optimization algorithm with M-1 dimensions. The complexity lies here on the processing algorithm, the error signal, a scalar signal, being extremely simple, and low cost. The disadvantage of this method is the bandwidth of the loop, which evolves in 1 / M. This method therefore lends itself to a small number of recombinant beams typically less than 10. The method known as "OHD" acronym for the English expression "Optical Heterodyne Detection". For this method, the error signal which consists of the measurement of the phase of each transmitter relative to a reference beam, is a vector signal; one detector is used per channel. The M measurements are made in parallel by heterodyne mixing and demodulation. The drawbacks of this method are the use of RF components, which penalizes the cost per channel, the use of a reference beam, the error signal which is measured before recombination and which does not guarantee a quality of data. optimal recombination: it does not make it possible to compensate the phase fluctuations between the phase measurement plane and the recombination plane. A calibration of the system is then required. The so-called "LOCSET" or "Synchronous Multi-Dither" method. As for hill climbing, this method uses a fraction of the recombined energy as an error signal, but in this case, the contributions of the different channels are identified by frequency "marking" each channel by RF modulation. a frequency of its own. The error signal for each beam is then obtained by heterodyne mixing with a reference beam. This method is attractive because it requires only a single detector, and the availability of fast phase modulators makes it possible to envisage a large number of channels. On the other hand, it requires a large number of RF components in the feedback loop (mixers, modulators, etc.), which considerably increases the cost per channel of the system. A similar signal is obtained by sequentially modulating each of the beams sequentially, this time at the same frequency, but at the expense of the system bandwidth. The method for direct measurement of the phases between transmitters, for which the error signal is a mapping of the phases extracted from the interferogram of the recombinant beams interfering with each other or with a reference beam. This method of direct interferometric measurement is collective: the set of phases is obtained by the recording of a single image by a matrix sensor, and thus lends itself perfectly to a large number of emitters. The cost of the imager used is divided by the number of channels and is therefore not critical. The bandwidth of the system can however be limited by the sensor used, especially in the infrared. This is not a fundamental limit.
    [0004] Finally, as for the "OHD" method, the phase measurement is performed before recombination; it does not compensate for phase fluctuations between the phase measurement plane and the recombination plane and therefore does not guarantee an optimal quality of recombination. A calibration of the system is then required.
    [0005] The table below summarizes the state of the art of coherent recombination techniques. The shaded boxes indicate the negative points of each method.
    [0006] 5 Nature of the Scalar Signal Vector Error "Hill" LOCSET "" OHD "Interf. Climbing »direct Number of detectors 1 1 M> 2M (for M sources) Bandwidth Increased in 1 / M> 10kHz> 10kHz Limited per camera (potentially> 1-10kHz) Calibration No No Yes Yes required Need No Yes Yes No RF electronics ( impact the cost) Need a No No Yes Not necessarily reference (QWLSI in [11]) Optical Type Near Field Near Field Far Field Far Field The most suitable recombination There is no architecture at this time coherent recombination of laser beams which satisfies both the conditions of a loop bandwidth> 1 kHz, a number of beams potentially of 100, 1000 or even more, of a non-calibration operation (signal of error in the recombination plane), and low cost.
    [0007] The scope of the invention is that of a system in which the laser beams are spatially recombined using a diffractive optical element (DOE). The system according to the invention is based on an original use of this diffractive element which makes it possible, in addition to ensuring the spatial recombination of the beams, to generate an innovative error signal making it possible to compensate for phase differences between laser sources. . This error signal is calculated from the diffracted intensities on the higher orders of the recombination diffractive element. Such an error signal makes it possible to fulfill all the conditions set out above.
    [0008] More specifically, the subject of the invention is a system for phasing M laser sources of the same wavelength centered around Ivo, having a periodic spatial configuration, M being an integer> 2, which comprises: - means for collimating and directing the M beams from the sources on a periodic phase grating diffractive optical element, with a different incidence angle from one beam to another, these angles of incidence being determined according to the period of the network, and - means for controlling the phases of said sources from a feedback signal from the recombined beams. It is mainly characterized in that it comprises: means for sampling a fraction of the recombined beams, in the path of this fraction of the recombined beams, a Fourier lens having an object plane and an image plane, with the diffractive optical element of recombination in its object plane, a matrix of detectors in the image plane of the Fourier lens, able to detect intensity distributions of the fraction of the recombined beams, means for calculating the counter signal -reaction from these intensity distributions. A vector error signal (of size given by the number of measured higher diffraction orders) is obtained, but without having to use RF components. In addition, the system in principle does not require any calibration, since the optimization does not target the phase locking (cf "OHD" and "direct interferometric measurement" techniques), but directly the recombined intensity (minimizing intensity of higher orders).
    [0009] Thus, the following advantages are grouped together: As for the "LOCSET" and "hill climbing" methods, the error signal is generated in the recombination plane, therefore no calibration is required. The error signal consists of a set of non-redundant measurements that allow simple processing to generate the feedback signal. - The cost of the system per channel (beam) is relatively low since no RF element is involved, and only one detector per channel is needed.
    [0010] The system is compatible with a large number of channels, and with a bandwidth> 1kHz. According to a characteristic of the invention, the means for calculating the feedback signal comprise means for calculating the product of the distribution of the intensities detected in the plane of the matrix of the detectors by the inverse of a matrix of dimension. (2M-1) x (2M-1) if M is odd, and 2M x 2M if M is even, defined by coefficients obtained by Fourier series development of the phase of the diffractive optical element of recombination taken on a period.
    [0011] Typically M> 100. Preferably, the sources are arranged in a one or two dimensional spatial configuration. According to a preferred embodiment of the invention, the beams coming from the laser sources have the same output plane, and the system then comprises another Fourier lens having an object plane in which the output plane of the laser sources is located. and an image plane in which the recombination diffractive optical element is located.
    [0012] Other features and advantages of the invention will become apparent on reading the following detailed description, given by way of nonlimiting example and with reference to the accompanying drawings, in which: FIG. 1 schematically illustrates the use of FIG. a diffractive optical element as means for recombining "M to 1" beams (5 to 1 in the example of the figure), FIG. 2 schematically represents an example of a phasing system according to the invention, the FIGS. 3 schematically show an intensity profile for a diffractive optical element used as a separator from 1 to M (from 1 to 5 in the example of the figure) (FIG. 3a), or used as means for recombining beams of M towards 1 (from 5 to 1 in the example of the figure) with the distribution of intensities diffracted by the diffractive optical element. From one figure to another, the same elements are identified by the same references. The scope of the invention is that of a system which relies firstly on the use of a diffractive optical element 1 (or DOE) as a means of recombining different laser beams 10, as shown in the example Figure 1. The laser beams 10 are incident on the DOE 1 at an angle defined by the spatial period of the DOE. When the beams are locked in phase, and with the optimal phase distribution (imposed by the DOE), then all the beams interfere constructively on the order 0 (= main order) of the DOE 11b, and destructively on the higher orders 11a. . The principle of the invention is to use the intensity distribution 11a diffracted on the higher orders of the DOE as an error signal to optimize the recombination, as represented in the example of FIG. 2. In our approach, as for LOCSET and hill 30 climbing techniques, the error signal is measured at the end of the chain (that is to say after the DOE), which makes it possible to take into account all the disturbances experienced by the beams. Note that if the example of FIG. 2 represents an on-line arrangement of the laser beams, and therefore a 1-dimensional DOE, the proposed solution nevertheless applies equivalently to a 2D arrangement of the laser beams and a 2-dimensional DOE. dimensions.
    [0013] A laser phase matching system according to the invention is described with reference to FIG. 2. The M laser sources have the same wavelength centered around A.sub.o. These laser sources may be pulse sources; the pulse width can also be less than 10-12 s. The system comprises: - M phase modulators: a modulator 4 at the output of each laser source.
    [0014] A phase-specific recombination DOE 1 having a predetermined spatial period, situated in the image plane of a Fourier lens 14: the M beams coming from the modulators are directed on the DOE 1 by this Fourier lens 14. Each beam arrives on the DOE with a specific angle of incidence defined by the spatial period of the DOE. Means for sampling a fraction 12 of the recombined beams 11, which may be a high reflectivity mirror 5 (with a sampling of 1% for example) or a polarization separator cube. A sample <1 / M is preferably chosen. The other fraction of recombined beams constitutes the output beam 13 of the system. A second Fourier lens 6 in the plane of which the recombination DOE 1 is located. A matrix of detectors 7 in the image plane (= plane B) of the second Fourier lens 6, able to detect the distributions 25 intensity 11b, 11a of the fraction of the diffraction orders of the beams recombined by the DOE 1. Means 8 for calculating the feedback signal from these distributions in the plane of the matrix of detectors. These calculation means 8 are connected to the M phase modulators 4 so as to control them. The M beams can be directed to the DOE 1 in different ways. The system comprises, for example, upstream of the DOE: a same master oscillator 2 connected to a coupler 3 "1 to M" so as to generate the M laser sources, possibly M amplifiers 9 respectively connected to the phase modulators 4. The output plane (= plane A) of the M laser beams (from amplifiers or modulators) is located in the object plane of the Fourier lens 14, according to a periodic spatial configuration of pitch P as As an alternative, the M laser sources have a collimation lens associated with each source and are directly positioned in a periodic spatial and angular configuration, so that the beams arrive at the recombinant DOE with a specific angle of incidence defined by the spatial period of the DOE. We now consider the means 8 for calculating the feedback signal. The problem to be solved by these calculation means is thus posited: The problem variable is the spatial distribution of the electromagnetic field consisting of the superposition of the electromagnetic fields from each of the laser sources. The intensity distributions of the electromagnetic field are assumed to be known in two distinct planes: a uniform (or measured) distribution IA in the output plane of the sources (plane A in FIG. 2) and an IB distribution measured after recombination by the DOE (in plane B in Figure 2). We want to calculate the phase distributions cpA and cpB in the planes A and B such that the electromagnetic field giej <PA propagated numerically from A to B gives This problem is similar to that of the measurement of phase aberrations from distortions of intensity images encountered for example in astronomy. Examples of methods of solving this problem can be found in the literature. The following publications can be cited: R. G. Paxman and J. R. Fienup, "Optical Misalignment Sensing and Image Reconstruction Using Phase Diversity," J. Opt. Soc. Am. A 5, 914923 (1988), or J.N.Cederquist, J.R. Fienup, C.C. Wackerman, S.R. Robinson, and D. Kryskowski, "Wave-front phase estimation from Fourier 35 Intensity measurements," J. Opt. Soc. Am. A 6, 1020-1026 (1989), or R.G.
    [0015] Paxman, T. J. Schulz, J. R. Fienup, "Joint estimation of object and aberrations by using phase diversity," J. Opt. Soc. Am. A 9, 1072-1085 (1992). A major disadvantage of this type of method is that they make use of digital Fourier transforms (for type 5 optical propagation calculations from A to B in the search for the solution) which implies a calculation time that can be long (typically much greater than 1s). In the system according to the invention, a major simplification for the phase calculation comes from the fact that the calculation of the electromagnetic field distribution in the plane B from that of the plane A is carried out by a simple product by a matrix known. Indeed, for M laser beams considered in A, the electric field distribution in A can be written, according to the parity of M: + N 2 x EA (X) = e ± (0) * euPk8 (x-kP )) k = -N 15 if M = 2N + 1, or: + N EA (x) = e- (7 x) 2 ei <Pk5 (x- kP) k = -N + 1 if M = 2N. Let: 20 2 akei9k6 (x-kP) k = -oe With: - w the size ("waist" in English) of the beams (supposed Gaussian) in the plane A, 25 - P the period of the positions of the beams in the plane A, - ak the amplitude weighting coefficient of the kth beam (for example here, ak = 1 for k between -N and + N for M = 2N + 1 and k between -N + 1 and + N for M = 2N, and ak = 0 otherwise) - (Pk the optical phase of the kth beam, 3021761 11 - b the Dirac function and the convolution operator The field in the DOE plane is obtained by Fourier transform of EA (x) and multiplication by the in-phase transmission function of the DOE, ei (PDoE (u) ED0E (u) = p e- (iruco) 2 ei4oDoE (u) x (Elio ° 00 akei (pk e-2ircukP ) The field propagated to the measurement plane (plane B) is obtained again by the Fourier transform of ED0E (u): +00 f XE g (X) = [e - (7)) y (ei In addition, the DOE phase being by construction a periodic function, of period 1 / P (u) being considered in the far field), we can write ei <PD0E (1) in the form of its Fourier series: ei (PD0E (u) = Co ck e2itrukP And so - 2 x EB (x) = e-F ( 0) 15 {+.0 +.0 ahei9h 6 (x + hP) * ck 8 (x-kP) 1 h-co k = -. 2 +00 +00 e-UX * ahei`Ph x ck 8 (x - (k - h) P) h = -09 k-co 2 e- (* [I 0r, +00 D x ck + hahei <Ph 8 (x - kP) k = -00 h = -00 +00 (+00 Ck + hcrhei <Ph xe (x- (01eP) 2 k = -00 h = -oo A combination DOE is calculated to combine M beams to 1. On the contrary, 1 single beam diffracted by the same DOE will produce essentially M beams (so-called principal) of intensity of the same order / 1), and infinity of higher orders of intensity / 2 less (/ 2 In other words, this implies the following relations for the coefficients ck: 1412 for k between -N and + N for M = 2N + 1 and k between -N + 1 and + N for M = 2N, 1412 "1 / iii otherwise.
    [0016] The terms ck + hah of the expression of EB (x) above may therefore have non-negligible values for: [-N <k + h __ + N] u [-N h 5 + N] for M = 2N + 1 or [-N + 1k + h + N] u [-N + 1 5 h + N] for M = 2N.
    [0017] Let: k e [-2N, ---, + 2N} for M = 2N + 1 or k e {-2N + 1, ..., + 2N} for M = 2N. In general terms, the expression of EB (x) can therefore be considered to be exact for indices k and h truncated from -2N to + 2N for M = 2N + 1: (x-kp 2 xew) or from -2N + 1 to + 2N for M = 2N: + 2N i + 2N Eg (X) = / k = -2N h 2N) 1 ck + hane "Ph 15 + 2N (x-kP 2 xek (0) ) ck + hahei`Ph + 2N EB (x) = 1 k = -2N + 1 h = -2N + 1 We then recognize the expression of a matrix product, as written below for the case M = 2N + 1: 20 EB, -2N = / C-4N '' 'C-2N .-' 'CO X a -21 ^ 1, -a iP 2N EB, 0 .- - - - r. - C2N - - -2N '' 'Co. Aoeig) 0 - -. EB, + 2N Co --- C2N --- C4N 1 pie + 2N a + 2Ns- Let: EB, -2N EA, -2N EB, 0 = With EA, k (and respectively EB, k) the complex weighting coefficients of the field EA (x) (and respectively EB (x)), such as, for example, neighborhood of x = kP: 5 (x-kP) 2 EA (x) = EA, kxe `&) '(x-kn2 EB (X) = EB, k X e Wj HDoE is the matrix defined by the coefficients ck of Fourier series development of the DOE phase over a period of time. This matrix is therefore known a priori by construction of the DOE.
    [0018] As seen above, in practice, with a DOE calculated to combine M laser beams, with M odd equal to 2N + 1, 2M-1 coefficients are needed in the Fourier series to ensure equality: + 2N eiePDoE ( u) = 1 ck e2inukP k = -2N 15 For M pair equal to 2N, 2M coefficients are then necessary to have: + 2N ei <PD0E (u) = Z Ck e2iirukP k = -2N + 1 This choice, non restrictive, of 2M-1 coefficients in the case M = 2N + 1 is also illustrated in FIGS. 3a and 3b by the fact that only the orders diffracted from order -2N to + 2N (in the plane B in the vicinity of x = kP for k E [-2N, ..., 2N1) have a significant intensity for calculation. The optical propagation of M beams from the plane A to the plane B is thus calculated by the simple product of a matrix of dimension (2M-1) x (2M1) for odd M, and 2M x 2M for M even (the matrix HDOE ) by the vector EA.
    [0019] The Fourier transformations used in the usual methods have been replaced by this HDoE matrix. Thus the calculation of the electromagnetic field distribution in the plane A from that detected in the plane B by the photo detector array, is carried out by a simple product of the inverse of this matrix HDoE by this distribution of The intensity detected in the plane B. From the electromagnetic field distribution thus calculated in the plane A, the phase is calculated in a conventional manner. This simplified calculation of the electromagnetic field distribution in the plane A considerably accelerates the phase calculation algorithms (= calculation of the feedback signal), for example of the maximum or iterative search type, and allows a real-time implementation. of these means for calculating the feedback signal, even for a number of beams of several thousand. As an example of phase calculation by iterations, mention may be made of the calculations described in the publications: J. Markham and JA Conchello, "Parametric blind deconvolution: a robust method for the simultaneous estimation of image and blur," J.Opt.Soc .Am.A 16 (10), 2377-2391 (1999), JR Fienup, "Phase retrieval algorithms: a comparison," Appl. Opt. 21 (15), 2758-2769 (1982). In the examples, the combination DOE operates in transmission, but the system according to the invention remains valid using a DOE in reflection.
    权利要求:
    Claims (8)
    [0001]
    REVENDICATIONS1. A phasing system of M laser sources of the same wavelength centered around A 0, having a periodic spatial configuration, M being an integer> 2, which comprises: means for collimating and directing the M beams from the sources on a periodic phase grating diffractive optical element (1) with an angle of incidence different from one beam to another, these angles of incidence being determined as a function of the period of the grating, and for controlling the phases of said sources from a feedback signal from the recombined beams, characterized in that it comprises: - means (5) for taking a fraction (12) of the recombined beams, on the path of this fraction of the recombined beams, a Fourier lens (6) having an object plane and an image plane, with the recombination diffractive optical element (1) in its object plane, - a matrix of detectors (7) in the picture of the Fourier lens (6), able to detect intensity distributions of the fraction of the recombined beams, - means (8) for calculating the feedback signal from these intensity distributions.
    [0002]
    Laser phase matching system according to the preceding claim, characterized in that the means (8) for calculating the feedback signal comprise means for calculating the product of the distribution of the intensities detected in the plane of the laser. matrix of the detectors by the inverse of a matrix of dimension (2M-1) x (2M-1) for odd M and 2M x 2M for M even, defined by coefficients obtained by Fourier series development of the phase of the diffractive optical element of recombination taken over a period. 3021761 16
    [0003]
    Laser phase sequencing system according to one of the preceding claims, characterized in that the laser sources are pulsed. 5
    [0004]
    4. phasing system laser sources according to the preceding claim, characterized in that the pulse width is less than 10-12s.
    [0005]
    A laser source phasing system according to one of the preceding claims, characterized in that M> 100.
    [0006]
    Laser phase sequencing system according to one of the preceding claims, characterized in that the sample fraction is <1 / M. 15
    [0007]
    Laser phase sequencing system according to one of the preceding claims, characterized in that the sources are arranged in a one or two dimensional spatial configuration. 20
    [0008]
    8. laser phase sequencing system according to one of the preceding claims, characterized in that the beams from the laser sources having the same output plane, it comprises another Fourier lens (14) having an object plane in which is located the output plane of the laser sources and an image plane in which is located the diffractive optical recombination element (1). 30
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    优先权:
    申请号 | 申请日 | 专利标题
    FR1401222|2014-05-28|
    FR1401222A|FR3021761B1|2014-05-28|2014-05-28|SYSTEM FOR CONDITIONING A LARGE NUMBER OF LASER SOURCES|FR1401222A| FR3021761B1|2014-05-28|2014-05-28|SYSTEM FOR CONDITIONING A LARGE NUMBER OF LASER SOURCES|
    JP2016569820A| JP6538084B2|2014-05-28|2015-05-26|Phase matching system for multiple laser sources|
    ES15725588T| ES2704111T3|2014-05-28|2015-05-26|Phasing system of a large number of laser sources|
    HUE15725588A| HUE042506T2|2014-05-28|2015-05-26|System for phasing a large number of laser sources|
    CN201580041454.6A| CN106663913B|2014-05-28|2015-05-26|System for adjusting the phase of a large amount of laser sources|
    KR1020167036621A| KR102272867B1|2014-05-28|2015-05-26|System for phasing a large number of laser sources|
    EP15725588.6A| EP3149813B1|2014-05-28|2015-05-26|System for phasing a large number of laser sources|
    PCT/EP2015/061524| WO2015181130A1|2014-05-28|2015-05-26|System for phasing a large number of laser sources|
    US15/313,542| US9812840B2|2014-05-28|2015-05-26|System for phasing a large number of laser sources|
    IL249158A| IL249158A|2014-05-28|2016-11-23|System for phasing a large number of laser sources|
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