Patent Description:
Today, pulsed laser transmitters are used in many applications to represent the spatial distribution of particular targets along the propagation direction of the laser beam. Similar to RADAR and SONAR, the backscattering or echo of a pulse is here received and recorded through a medium such as a vacuum, air or water using a corresponding photo receiver installed next to the transmitting station. The distance of the target is then obtained as a product of the runtime to the target and back and of the speed of light in the medium. The very narrow spectral width of a laser additionally allows, similar to RADAR and SONAR, to measure the speed of the target along the beam axis from a frequency shift of the received signal against the optical frequency of the transmission beam - i.e. Doppler shift. Measuring arrangements of this kind are referred to as LIDAR or Light Detection And Ranging.

<CIT> discloses a LIDAR arrangement with a light transmission assembly configured to transmit a plurality of light signals towards a solid target, wherein each of the plurality of light signals has a unique characteristic (for instance wavelength) that differs from the other. Light signals which are backscattered from an object and which have different wavelength are separated according to their wavelength by means of dichroic mirrors. Several photodetectors which all are configured to detect a particular wavelength are used. A laser pulse series comprising laser pulses of different wavelength, may be produced in a cavity with oscillating spacing or by the use of several light sources.

<CIT> discloses a method and system of frequency tagging lidar light signals. A laser source provides a signal to a mixer. A local oscillator also provides a signal to the mixer. Local oscillator can be a radio frequency oscillator, such as a microwave oscillator. The mixer uses non-linear mixing to produce a frequency comb with frequencies which are spaced by the RF frequency. The detection system comprises a plurality of individual sensor elements each of which is sensitive to a particular frequency. RF frequency spacing can be limited by the amount of Doppler shift.

<CIT> discloses a time-of-flight scanner to enable, for example, distance measurements with an increased scanning rate. This is achieved by emitting laser pulse sets having a signature which enable correlation of each detected return pulse set with the corresponding emitted pulse set. Signature could be, for example, a bipulse, but also a different wavelength. Two different wavelengths are produced by two fiber amplified lasers and filtered by the detector by means of a filter or wavelength demultiplexer.

<CIT> discloses a laser radar and 3d scanner. Pulses of two fiber lasers having different wavelengths are bundled together and transmitted to the object. Received light is split in a beam splitter (long wave reflection, short wave transmission) and detected by photodetectors. An average of the signal of the two detectors is made to improve distance measurement accuracy.

The reference <NPL>, discloses a scanning lidar for forest scanning. Two lasers emit simultaneously nanosecond pulses of different wavelength. The receiver includes a dichroic beam splitter. Laser wavelengths are in the IR regime.

<CIT> relates a three-dimensional imaging system with a multi-wavelength pulsed light source. Pulses having different wavelength are separated in space on the transmission side by a frequency-to-space converter (e.g. arrayed waveguide grating) and transmitted to different locations in space. A lens collects reflected light from different locations. The document suggests to solve the range ambiguity problem by reordering the pulses.

<CIT> relates to a lidar sensor for motor vehicle. Three laser diodes produce pulses which are then deflected by a deflection mirror onto the roadway. Intensity of reflected light as a function of frequency gives insight into the surface of the roadway. Solid targets are sensed.

<CIT> relates to a frequency agile LADAR sensor including a transmitter configured to provide laser pulses of different wavelength and receiver with a frequency agile optical filter configured to receive a reflected signal of particular frequency. As an alternative to the optical filter (resonator), the document also suggests to use an optical combiner along with a heterodyne detector. Long range sensor operation requires a high laser pulse energy. The optical frequencies used in the document may be within high atmospheric transmission bands, thus the amount of detected photons backscattered from the atmosphere may be significant. The LADAR may be mounted on an aircraft.

For further prior art concerning LIDAR arrangements, components and advantageous uses thereof, reference is made to <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, and <CIT>.

A particularly preferred use of the invention relates to satellite-based LIDAR arrangements and LIDAR methods, particularly for meteorological purposes such as wind detection. Most relevant prior art in this respect is the WIND-LIDAR "ALADIN" of the company of Astrium used on the satellite Aeolus, see.

The invention is based on the object of providing a LIDAR arrangement and a LIDAR method with a higher laser repetition rate, preferably also of a kind that permits scanning transversely to the motion direction of the LIDAR arrangement and/or enables a compact design.

This object is achieved by a LIDAR arrangement and a LIDAR method comprising the features or steps of the attached independent claims.

Advantageous embodiments of the invention are the subject of the subclaims.

In a first aspect, the invention provides a LIDAR arrangement configured for atmospheric measurements, comprising a laser transmitter for transmitting pulses of a laser radiation to a measurement object, and a receiver for receiving pulses of the laser radiation backscattered from the measurement object, wherein the laser transmitter is configured to transmit a pulse sequence in which successive pulses respectively comprise a specific frequency shift to each other and wherein the receiver includes a dispersive element for the spatial separation of the pulses depending on the optical frequency by a frequency-dependent deflection, and a spatial resolution optical matrix sensor on which the pulses spatially separated by the dispersive element are mapped (direct reception), wherein the receiver between the dispersive element and the matrix sensor comprises an interferometer configured for mapping at least partially spatially separated interferograms to the individual pulses of the pulse sequence on the matrix sensor.

Hence, the invention provides a LIDAR arrangement comprising a laser transmitter for transmitting pulses of a laser radiation to a measurement object, and a receiver for receiving pulses of the laser radiation backscattered from the measurement object, wherein the laser transmitter is designed for transmitting a pulse sequence in which successive pulses respectively comprise a specific frequency shift to each other and wherein the receiver includes a dispersive element for a spatial separation of the pulses depending on the optical frequency by a frequency-based deflection, and a spatial resolution matrix sensor on which the pulses spatially separated by the dispersive element are mapped.

Preferably, the laser transmitter is configured to transmit pulses with a pulse frequency of <NUM> to <NUM>, preferably of <NUM> to <NUM>, even more preferably of <NUM> to <NUM>.

Preferably, the laser transmitter includes a master oscillator including a number of lasers, in particular diode lasers or micro solid-state lasers of different wavelengths; a master laser that can be directly modulated in its wavelength; or a combination of a master laser and a downstream modulator for modulating the wavelength of the master laser.

Preferably, the laser transmitter includes one or more optical amplifiers for amplifying a signal from a master oscillator.

Preferably, the laser transmitter includes one or more optical amplifiers for amplifying a signal from a master oscillator preferably composed of one or more fiber amplifiers.

Preferably, the laser transmitter includes a frequency multiplier preferably arranged downstream of the amplifier or fiber laser.

Preferably, the laser transmitter includes a transmission telescope.

Preferably, the laser transmitter includes a scanner for scanning an angular range with the radiation from the laser transmitter.

Preferably, the dispersive element includes one or several elements from the group comprising a grating, a prism, a Fabry-Pérot interferometer, a fiber-optical de-multiplexer, a reconfigurable fiber-optical multiplexer, and an arrayed waveguide grating.

Preferably, the matrix sensor is selected from the group comprising a one-dimensional matrix sensor, a two-dimensional matrix sensor, a photo detector array, a one-dimensional photo detector array, a two-dimensional photo detector array, a CCD array, a one-dimensional CCD array, a two-dimensional CCD array, a PIN detector array, a one-dimensional PIN detector array, a two-dimensional PIN detector array, a CMOS array, a one-dimensional CMOS array, a two-dimensional CMOS array, a CMOS APD array, a one-dimensional CMOS APD array, a two-dimensional CMOS APD array, an ICCD detector, a one-dimensional ICCD detector, a two-dimensional ICCD detector, an EMCCD array, a one-dimensional EMCCD array, a two-dimensional EMCCD array, an IBCCD array, a one-dimensional IBCCD array, a two-dimensional IBCCD array, an EMCMOS array, a one-dimensional EMCMOS array, a two-dimensional EMCMOS array, an IBCMOS array, a one-dimensional IBCMOS array, and a two-dimensional IBCMOS array.

Preferably, the receiver comprises an A/D converter for converting signals from pixels of the matrix sensor.

Preferably, the receiver comprises an intermediate register for buffering signals from pixels of the matrix sensor.

Preferably, the receiver comprises a synchronization device for synchronizing the reading and/or for further processing signals to be assigned to different pulses of the received signals over time.

Preferably, the receiver comprises a receive telescope.

Preferably, the receiver comprises a light guide device for receiving radiation from different directions from the measurement object and for introducing the radiation into the dispersive element from different directions at different angles or at spatially offset locations.

In a further aspect, the invention relates to a LIDAR method for measuring the location and/or velocity of a measurement object, comprising:.

Preferably, the pulses are transmitted with a pulse frequency of <NUM> to <NUM>, preferably of <NUM> to <NUM>, even more preferably of <NUM> to <NUM>.

Preferably, the pulses having a different frequency are generated in a master oscillator and are subsequently amplified by means of at least one fiber amplifier.

Preferably, after being amplified, the pulses are converted with respect to their optical frequency and are especially multiplied with respect to their optical frequency, particularly by optically non-linear media.

Preferably, the method comprises scanning the transmitted pulses over an angular range and receiving the backscattered pulses within an angular range and spatially separated mapping of pulses received from different angles on the matrix sensor.

Particularly, the invention relates to a method and an arrangement for the separate measurement of LIDAR signals superimposed in time.

The invention and/or advantageous embodiments of the invention create an improvement of the LIDAR technology which makes it possible to separate and individually measure reception signals of a pulsed transmission radiation of very high transmission frequency in the receiver - despite their overlap in time which occurs as a consequence of a long pulse transit time through the scanned medium, for example at the measurement of the earth's atmosphere from a satellite.

According to the invention, a method and an arrangement for LIDAR detection at high repetition rates are provided.

The invention is particularly suitable for applications in air and space travel, especially for an improved satellite-based wind LIDAR.

Satellite LIDARS as previously implemented in the field, achieve only a low repetition rate of <NUM>, typically about <NUM>, at maximum.

LIDARs with high repetition rates such as enabled by the present invention, allow the use of the very compact and stable fiber laser technology. Unfortunately, this interesting fiber technology only permits a low pulse power and hence only a relatively low pulse energy. This can be compensated by a higher repetition rate. On the other hand, a higher repetition rate may lead to ambiguities in the pulse detection, which in turn lead to that high repetition rates cannot be used for very long measuring ranges, as it would be the case in altitudes above the atmosphere. The advantageous embodiments of the invention herein described also allow the use of fiber lasers for space LIDARs such as satellite-based LIDARs.

In current atmospheric LIDAR systems, which detect wind speeds in the atmosphere from satellites, a laser beam is sent to the atmosphere and is backscattered, and the backscattered light, which is frequency shifted due to the Doppler effect, is received by the satellite. Due to the runtime, the atmospheric height of the backscatter can be resolved. Two main principles can be applied:.

As the atmosphere has a height in the range of <NUM>, the laser pulse runtime through the atmosphere is about <NUM>. In case the pulse repetition frequency of the measurement is above <NUM>, the height at which a particular backscattering signal strength is achieved cannot be resolved anymore due to ambiguity of overlapping pulses.

Concerning the basic principle for example, embodiments of the invention work in the same way as the current LIDAR systems and are therefore able to detect wind speeds or speeds of other measurement objects via a measurement of the Doppler shift according to one of the above-mentioned main principles <NUM>) or <NUM>) when designed as a Doppler LIDAR. According to embodiments of the invention, to achieve unambiguity at atmospheric wind LIDAR detections, the pulses emitted by the laser are additionally wavelength coded or frequency coded. For example, successive pulses are modulated in such a manner that they have different wavelengths (wavelength division multiplexing - WDM) or different frequencies.

Particularly preferably, in the case of WDM, the received pulses are not separated by a wavelength splitter, as usual in communication and measurement techniques, but are delivered in a manner identical with a Fabry-Pérot interferometer (briefly referred to as FP interferometer or FPI, or alternatively also a different interferometer, e.g. of the type Fizeau), which is used for the determination of the Doppler shift induced by the wind speed. The Fabry-Pérot interferometer is preferably designed in such a manner that the free spectral range is greater than the Doppler frequency shift plus n times the wavelength shift of the multiplex pulse channels (n being the number of the multiplex channels).

When using interference fringe technologies, it is possible not only to determine a fringe displacement corresponding to the Doppler shift, but also to additionally sort the pulses by time, which - due to the run length that corresponds to the light speed - corresponds to atmospheric heights, and therefore the pulses are sorted according to the atmospheric height.

In this manner, the problem of ambiguity in high repetition atmospheric LIDAR wind speed detection without additional channel splitting at the receiving end (which would require a separate receiver for each wavelength channel) can be solved with a single Fabry-Pérot receiver that is anyway needed for the determination of the Doppler shift of an individual channel. The only additional effort is the right design of the Fabry-Pérot receiver as described above.

Similarly, when using the frequency multiplex technique, subsequent pulses are shifted in frequency by an amount greater than the Doppler-shifted reception signal. Using a Fast Fourier Transform (FFT) or a filtering process after a coherent receiver again enables sorting of the pulses according to time and hence according to the atmospheric heights.

Accordingly, the above-described configuration of the receiver and the use of a shift in wavelength or frequency of successive pulses make it possible for the first time to employ fiber lasers or fiber amplifiers having a high repetition rate for LIDAR systems at repetition rates substantially above <NUM>, which currently is the measuring limit for space LIDAR arrangements or methods involving atmospheric height resolution.

The use of fiber lasers and/or fiber amplifiers is a key factor for enabling future LIDAR systems in space, which are extremely stable, efficient and miniaturized and which allow height-resolved wind speed measurements for greatly improved meteorological forecasts.

One idea relates to a method and/or an arrangement for separating LIDAR signals having a high transmission pulse frequency with an overlap in time of the reception signals due to the long runtime through the scanned medium.

Preferably, a periodic optical frequency shift (wavelength shift) of adjacent transmission pules is performed.

Preferably, in case of a direct reception technique, a spatial separation takes place on the receiver side by a dispersive element depending on the wavelength of the different individual laser pulses.

Preferably, the laser pulses are then mapped on a suitable one or two-dimensional photo detector array at at least partially different locations.

Preferably, the spatially separated signals are supplied to an interferometer at different positions and/or different angles such that at the output of the interferometer at least partially separated interferograms to the individual spatially separated frequency-shifted laser pulses are produced which are recorded by means of a one or two-dimensional photo detector array.

Preferably, the photo detector signals of the individual pixels are read into an intermediate register via an analog-to-digital converter, and buffering and read-out thereof for further digital processing are synchronized in the timing of the incoming signals.

Preferably, a number of lasers (array) of different wavelengths (for example laser diodes), which are coupled into a common optical fiber, are used as a master laser.

Preferably, the radiation of the master laser is amplified in power by a common fiber amplifier.

Preferably, the amplified laser radiation is frequency converted by using non-linear optical media for example.

Preferably, the wavelengths of the master lasers correspond to a portion of the internationally standardized wavelengths for use in wavelength division multiplexing systems.

Preferably, a master laser is used that can be directly modulated in its emission wavelength.

Further preferably, in this case, the master laser is modulated in its emission wavelength by a current modulation, a temperature modulation or the change of a frequency-selective element of the same (e.g. a Bragg reflector), by an introduction of stress onto the laser crystal or a combination thereof.

Preferably, the output radiation of the master laser is changed by means of a downstream electro-optical or acousto-optical modulator.

Preferably, a grating, a prism, a Fabry-Pérot interferometer, a fiber-optical de-multiplexer (OADM), a reconfigurable fiber-optical multiplexer (ROADM) or an arrayed waveguide grating (AWG) are used as a dispersive element for spatially separating the individual laser wavelengths of the emitted laser pulses.

Preferably, a Fabry-Pérot interferometer or a Fizeau interferometer are used as an interferometer.

Preferably, the coupling of the spatially separated wavelengths of the received laser radiation into the dispersive element takes place in an arrangement of a line, a circle or in any other two-dimensional arrangement of light rays.

Preferably, the image position of the optical radiation of the individual laser pulses behind the interferometer corresponds to a circular pattern in the case of a Fabry-Pérot interferometer or to a line pattern in the case of a Fizeau interferometer.

Preferably, a linear or two-dimensional arrangement of photo detectors is used as a detector array.

Preferably, an array from the group comprising a one or two-dimensional CCD array, a PIN detector array, a CMOS array, a CMOS APD array, an ICCD detector, an EMCCD array, an IBCCD array, an EMCMOS array or an IBCMOS array is used as a photo detector array.

Preferably, the LIDAR reception signals read into the intermediate register are read-out in parallel or serially in a time cycle with the timing of the LIDAR reception signals for further electronic processing.

Another method and/or arrangement relates to the measurement of high rate and/or time-overlapped multiple LIDAR signals by means of a detector system having a low readout rate, the laser repetition rate Flaser of the LIDAR system being clearly greater than the inverse of the runtime of the laser pulses through the medium to be measured.

In this case, it is preferred that the laser repetition rate Flaser of the LIDAR system is as high that the resulting backscattering overlaps in time and does not permit an unambiguous assignment in time of the received signal to the number of the emitted laser pulses, wherein the laser pulses emitted within the time T are respectively assigned to different laser frequencies using suitable frequency modulation methods, wherein further, in the case of direct reception, the signals overlapping in time are spatially separated and are detected by a detector array or in the case of a heterodyne reception the signal is, after the reception of the backscattered laser pulses by a photo detector, subsequently subjected to a frequency analysis such that the individual laser pulses are separated in frequency at this frequency analysis such that the fast pulse sequence of the laser pulses can be unambiguously assigned by means of frequency-based separation in the frequency analyzer and the unambiguous overlap of the received signals can be unambiguously resolved.

In this case, it is preferred to use a master laser that can be directly modulated in its emission wavelength.

Further preferably, the master laser is modulated in its emission wavelength using a current modulation, a temperature modulation or by the change of a frequency-selective element of the same (e.g. a Bragg reflector) or a combination thereof.

Preferably, a PIN diode, an APD diode or a receiver composed of several such diodes is used as a photo detector.

Preferably, the frequency-based separation of the signals takes place using a Fourier analysis (e.g. FFT) or one or several filters.

Preferably, the LIDAR signals are received from an angle that is fixed with respect to the LIDAR system.

Preferably, the LIDAR signals are received from several angles or angle ranges that can be switched in terms of time or can be continuously changed (scan).

Embodiments of the invention will now be described in more detail with reference to the attached drawings. In the drawings it is shown by:.

The Figures <NUM> through <NUM> show different embodiments of LIDAR arrangements <NUM>, the basic functions and advantages of which will first be described in more detail with reference to the <FIG> and <FIG>. The LIDAR arrangements <NUM> can be used in many applications to represent the spatial distribution of particular targets along the propagation direction of a laser beam. Particular attention is paid to the suitability of the LIDAR arrangement <NUM> for atmospheric LIDAR measurements, especially for meteorological measurements of the atmosphere. In particular, the LIDAR arrangement <NUM> is designed for use on or in satellites or space stations or other aerospace objects.

A sectional image can be obtained using single-axle scanning of the transmission and receiving axes of a stationary LIDAR during the emission of a laser pulse series. This sectional image is also created without scanning, if the LIDAR device is in a smooth motion on the plane or in a satellite. Here the LIDAR leaves a series of parallel scanning tracks with measurement recordings in the direction toward the ground. By additionally scanning the transmission and receiving axis over a fixed angle transversely to the moving direction, the ground or the atmosphere can be scanned over a particular angular range even two-dimensionally or three-dimensionally.

LIDARs are used for various measurement tasks using laser wavelengths in the entire wavelength range from UV through IR. These tasks are generally divided into two categories: LIDAR measurements to solid targets or to soft targets. Distance, profile and area measurements to solid objects belong to the first category. Some examples are: LIDAR scanning in autonomous driving of a vehicle for recording obstacles; LIDAR scanning from the aircraft, which enables a sight with the focused laser beam through gaps in the forest cover to the ground, in the service of vegetation research and archaeology; LIDAR measurements from the satellite, which produce accurate height profiles of the surface of the planets Mars, Mercury and the moon, for planetary research.

To the second category of soft targets belong LIDAR measurements of the distribution of air aerosols in clear weather, mist, fog, cloud and individual gas constituents and of their motion from their Doppler shift in the reception signal, for meteorological observation and atmospheric research. Such measurements are respectively made from ground stations, aircrafts or satellites. In contrast to solid targets, where exclusively the sharp echoes are important and reflect the contours of and the distance from objects, in soft targets the continuous intensity profile of backscatter is recorded to derive the concentration of the atmosphere constituents along the beam axis from this profile. In Doppler LIDARs, wind speeds are recorded by additionally measuring the progress of the Doppler frequency shift in the projection onto the beam axis.

"Snapshots on one axis" are taken with individual transmission pulses during the short period of their runtime. Today, the airplane or the satellite uses a pulse frequency about <NUM> to obtain in a series of vertical snapshots a sectional image along the trajectory through the atmosphere.

On the other hand, transmission frequencies higher than <NUM> enable a better spatial resolution in the sectional images and last but not least scanning transversely to the trajectory. However, at a higher pulse frequency, account has to be taken that when a single photo receiver is used for all signals there may be caused an overlap in time of the received measurement signals of different pulses meaning that each received signal can no longer be unambiguously assigned to individually emitted transmission pulses in the pulse series.

The limit of the measurement frequency until such overlap occurs is determined by the ratio of the runtime of the transmission pulse to the expanse of the measuring section L in both solid and soft targets. When the distance in time of the transmission pulse Ts of the frequency Fs = <NUM>/Ts is considerably greater than the runtime TL = <NUM>/c there and back, with c being the light speed, i.e. Ts >> TL, the echoes from solid discrete objects of category <NUM> in different unknown distances on the measuring section of a particular transmission pulse Pn can still be unambiguously differentiated from those of a subsequent transmission pulse Pn+<NUM> because their distance in time will then always be <MAT> i.e. all measurement signals of Pn+<NUM> on the measuring section arise completely separate from the measurement signals of Pn in terms of time.

However, this is not the case when the time interval of the pulses is equal to the pulse runtime over the expanse of the measuring section, i.e. <MAT>.

Because in this case, the echo of an object as it is received by the photo receiver can be either interpreted as an echo of the pulse Pn of an object at the end of the measuring section or of a subsequent pulse Pn+<NUM> at the beginning of the measuring section, because both arrive at the receiver at the same time. This means that an overlap is produced at the receiver which also applies to each pair of adjacent transmission pulses in the pulse series.

Now, if the time interval of adjacent pulses is shorter than the measured expanse, i.e. <MAT> the overlapping region of these two pulses shifts from the edge towards the center of the measuring range and there are produced around its center intervals of this overlap of more distant pulses and closer pulses.

If the time interval is <MAT> the ambiguity range even extends to the pulses Pn-<NUM> and Pn+<NUM>, meaning that it leads to an overlap in time over an increasing number of adjacent pulses if the pulse spacing further decreases.

The above description relates to the possible overlap of echoes of several discrete solid targets at a high transmission frequency. The same also applies to measurements to soft targets, because these can be regarded as a tight juxtaposition of discrete semipermeable targets. With soft targets such as the earth atmosphere, this overlap of the received signals leads to a serious problem in a single receiver which has not been solved up to present. Namely, in this case, unambiguous recording of the relative intensity of the backscatter from the atmosphere or, in the case of the Doppler LIDAR, of the frequency shift in any position along the measuring section is desired.

The overlap in time of the signal components of the backscatter of several adjacent transmission pulses occurring at a high transmission frequency here leads to a radical distortion of the measurement results.

The LIDAR arrangements <NUM> as proposed and the LIDAR methods that can be carried out using these arrangements shall enable a separation of the received signals, i.e. a recovery of their correct assignment to the individual transmission pulses and thus their measurement despite this overlap.

The limit of the pulse spacing of the transmitter beyond which the ambiguity of the measurement occurs is different for different LIDAR applications. This is due to the different measured expanses. For example, in ground measurements or in measurements of the atmosphere from the aircraft with the measured expanse being L = <NUM>, the limit of the pulse spacing <MAT> and the limit frequency then is <MAT>.

Further, at typical measured expanses of the atmosphere from a satellite of L = <NUM>, for example, the limit frequency is <MAT>.

<FIG> shows this effect for use of atmospheric measurements from the satellite, which is in the foreground here as an application of the LIDAR arrangement <NUM>.

<FIG> shows the measured signal I of a receiver of a satellite atmospheric LIDAR in the case where a) the transmission frequency is only half of the measurement frequency (<FIG>), b) the transmission frequency is equal to the measurement frequency (<FIG>) and c) the transmission frequency two times higher than the measurement frequency (<FIG>).

In <FIG>, in all the time periods, n = <NUM>, <NUM>, <NUM>, <NUM>. Tn,n+<NUM> = TL = <NUM>/c with the measurement frequency FL = <NUM>/TL, where L indicates the level above the ground. The various sub-<FIG> illustrate the above-discussed cases where a) the transmission frequency is lower by one half, b) is equal to and c) is twice the measurement frequency.

In satellite measurements of the atmosphere it may be advantageous or in some cases even necessary to measure for example on the dayside of the earth the reflection of the sun over the same time period as the backscatter signal of the laser pulses from the atmosphere to deduce it mathematically at a later time as a natural base rate from the backscatter signal of each of the laser pulses from the atmosphere.

For such cases, there should be introduced between the times of the measurements of the atmospheric signal an equally long time interval, which exclusively serves for the measurement of the background, while the transmission pulse has not yet entered the atmosphere. By these additional measurement intervals prior to each pulse measurement, the limit frequency FGrenze in satellite measurements of <NUM> is cut by half or reduced to <NUM>. This case is shown in <FIG>.

The intention is that the LIDAR arrangements herein described are particularly suitable for enabling improved satellite-based measurements. For this reason, there will be first discussed known LIDAR arrangements intended for a similar use.

The satellite ADM (Atmospheric Dynamic Monitoring) - Aeolus of the European Space Agency, ESA, carries a Doppler LIDAR: ALADIN (Atmospheric Laser Doppler Instrument), and the satellite EarthCare (Earth Clouds, Aerosols and Radiation Explorer) of ESA and of the Japanese Space Agency JAXA carries the atmospheric backscatter LIDAR ATLID (atmospheric Lidar). Both LIDAR devices are forerunners of a series of further atmospheric satellite LIDAR devices which are envisaged and which are based on an increasingly improved technology. In both missions, the transmitter is a frequency-tripled Nd:YAG crystal laser having a transmission pulse frequency of <NUM> or <NUM>, respectively. With this low transmission pulse frequency, the above-discussed problem of overlap does not yet occur. In ATLID, the measurement object is the height distribution of the aerosol concentration and in ALADIN the height distribution of wind speeds in the east-west direction. In this case, the aim is to provide a LIDAR arrangement <NUM> capable of delivering more complex and higher resolution sectional images of the atmosphere with a larger surface covering than in the case of known LIDAR arrangements.

Backscattering of the atmosphere partially takes place from the air molecules, the so-called Rayleigh scattering, or from its air particles and water droplets, the so-called Mie scattering. For characterizing said backscattering, one uses the backscattering coefficient β of the relative scattering intensity per meter (m-<NUM>) and steradian (sr-<NUM>). As the backscattering coefficient for the Rayleigh scattering in dependence on the wavelength of the transmission beam λ is proportional to λ-<NUM> and proportional to λ-<NUM> for the Mie scattering, preferably short transmission wavelengths are used for Rayleigh LIDARS - in the case of ATLID and ALADIN the frequency-tripled <NUM> wavelength of the Nd:YAG laser (<NUM>) in the UV range. However, at a constant transmission power, the number of laser photons is also reduced proportionally to λ-<NUM> due to frequency multiplication. Moreover, considerable optical losses have to be expected in frequency multiplication.

In the measurement and further processing of the received signal in the frequency space, attention should be paid to that the optical frequency bandwidth of the transmission signal ΔfL is generally dependent on the pulse duration ΔtL according to the Fourier relation ΔfL, ΔtL = <NUM>, i.e. with a pulse duration of ΔtL = <NUM> ns, the frequency bandwidth is ΔfL = <NUM> and with a pulse duration of ΔtL = <NUM> ns, the frequency bandwidth ΔfL = <NUM>. To avoid a considerable impact of this spread on the measurement signal, the pulse durations with ALADIN and ATLID are <NUM> ns and <NUM> ns, respectively, with a bandwidth of <NUM> and <NUM>, respectively.

A further effect that should be taken into account for measurements in the frequency space is the Doppler Spread of the received signals due to the statistical own motion of particles and molecules of the atmosphere. In Mie scattering, i.e. scattering from aerosols, this Doppler frequency spread of the received signal compared to the transmission signal is negligibly small due to the their inertia. On the other hand, this spread is considerable in LIDAR measurements of the Rayleigh scattering and is described as a standard deviation of the Doppler profile from the central frequency in dependence of the temperature: δfD = fL/C (kT/m)<NUM>/<NUM>, where k stands for the Boltzmann constant, T stands for the temperature in Kelvin, and m stands for the mass of the molecule. At room temperature and at an average mass of the air molecules, it can be assumed that δfD = <NUM>-<NUM>, i.e. at a UV radiation of λ = <NUM> with the transmission frequency of <NUM><NUM> Hz, δfD = <NUM>.

<FIG> shows a relative frequency shift of the Mie and Rayleigh scattering in the atmosphere due to LIDAR measurement.

<FIG> schematically shows the reception signal progression as a function of the frequency deviation from the central transmission frequency due to both scatter operations. In both satellites, ALADIN and ATLID, the two scatter components are separated from each other using complex filtering techniques and are individually measured.

The measured single-sided Doppler frequency sweep due to wind in the atmosphere is <MAT> where fL is the frequency of the laser and v is the wind speed projected in the direction of the receiving axis of the LIDAR. In ALADIN, this is inclined by <NUM>° against nadir. The Doppler frequency shift at a smallest resolved speed of a horizontal wind of u = <NUM>/s then is ΔfD = <NUM> fL v/c cos (<NUM>°-<NUM>°) = <NUM> v/λ cos (<NUM>°-<NUM>°) = <NUM>. The frequency range for the measurement of wind speeds of +/-<NUM>/s then is <NUM>.

The LIDAR arrangements <NUM> herein described enable measurements with considerably higher repetition rates, i.e. in a range of several Kilohertz to a range of hundred Kilohertz, compared to the satellite missions ALADIN and ATLID. This offers the following advantages:.

Advantageous embodiments of the invention enable considerably higher measurement frequencies FMessung in LIDARs and particularly in satellite LIDARs as result of the benefits of technological improvements both in the transmission and receiving techniques, despite the above-described problems of a reception signal overlap in individual photo receiver systems and the related limit frequency FGrenze.

Some preferred embodiments of the LIDAR arrangement and of the LIDAR method provide for:.

In the embodiments shown in the Figures <NUM> through <NUM>, a laser transmitter <NUM> is provided which is constructed in such a manner that it periodically emits in its continuous pulse series over a particular number M of adjacent laser pulses at a measurement frequency (which corresponds to the repetition rate of the laser) FMessung, which is desirably higher than the above-stated limit frequency FGrenze, at different optical frequencies f<NUM>, f<NUM>, f<NUM>,. fM (i.e. colors) at a frequency spacing Δfn. Preferably, it is provided at the same time for the overall duration of the period of the emission of said M pulses being longer than the duration between pulses at the limit frequency, i.e. M/FMessung ≥ <NUM>/FGrenze. This provides for the advantage that the received signals of these M adjacent transmission pulses are always different from each other by their different optical frequency (color) in addition to their mutual time delay (phase difference).

From the basic principle, the receiver <NUM> and the LIDAR arrangement <NUM> operate in the same manner as generally described above for LIDAR arrangements; i.e. the receiver <NUM> operates for example in a clocked manner with an exposure time (period) and receives impinging backscattered pulses within the exposure time to measure the distance from the measurement object via the runtime of the individual pulses or to measure a speed of the measurement object via a measurement of the Doppler shift. In addition to this functionality, the receiver <NUM> is designed for example to spatially separate pulses overlapping during the measurement, e.g. incoming pulses per exposure time/clock.

In some illustrated embodiments of the LIDAR arrangement <NUM>, for separating the pulses according to their frequency coding (color), an optical receiving device <NUM> of the receiver <NUM> is designed in such a manner that the receiver is equipped with a dispersive optical element <NUM> (e.g. prism or grating) alone and/or with an interferometer <NUM> (e.g. Fizeau or Fabry-Pérot), which maps the received signals having a different frequency in a spatially separated manner on a matrix sensor such as a photo detector array <NUM> (1D or 2D).

Optical reception signals, which overlap in time due to the short time interval of the transmission pulses, are spatially unbundled through this measure and can then be converted in their pixels first in an analog-to-digital (a/d) manner after their mapping on the photo detector array <NUM> (1D or 2D) to be then read individually into an intermediate register for example, where they are available for further serial/digital signal processing.

After a period of the frequency shift of the pulses (i.e. after M pulses), received signals arise in the subsequent period in the same frequency series and are therefore spatially deflected in the same manner onto the photo detector array <NUM> by the dispersive element <NUM>. However, in this case there is a time difference M/FMessung greater than <NUM>/FGrenze between the signals of the individual pixels of these first and second series. After an analog-to-digital conversion, this second pulse series can be read-in and further processed in the intermediate register <NUM> separated in time from the first pulse series. Separate serial or parallel processing of all received signals can only take place in the conventional manner. In this case, the readout rate of the receiver is at least M/FMessung.

In the past years, lasers have been developed which are very well suited for serving as transmission lasers for the laser transmitter <NUM>. These are preferably fiber lasers or master-oscillator-amplifier combinations, preferably with fiber-optical amplifiers having a higher pulse frequency allowing in an efficient manner to obtain an advantageous average beam power in the range of hundreds of Watts. One example is the glass fiber laser or glass fiber amplifier doped with ytterbium, Yb, with amplifying wavelengths between <NUM> and <NUM>, or doped with erbium with amplifying wavelengths of about <NUM>. An additional advantage of these fiber-lasers and amplifiers over former crystal lasers and crystal amplifiers is their compact integral construction. Due to connections of the subsystems to light guides, the usual common optical bench of all optical components and subsystems of a LIDAR which impedes operation thereof in a satellite, may be omitted.

A rather attractive system architecture for the laser transmitter <NUM> is the design of frequency-stable and easy modulating master oscillators <NUM> with a fiber pre-amplifier <NUM> and a fiber final amplifier <NUM>, a so-called MOPA <NUM> (master-oscillator power amplifier) for generating the pulsed radiation with a low spectral bandwidth. A low spectral bandwidth of the transmission radiation is advantageous both for measurements of the intensity of the atmospheric backscattering and of the wind force by means of Doppler LIDARs; in the first case for separating frequency-shifted pulses in pulse series and in the second case for obtaining the required Doppler measurement resolution in the frequency range.

Here, a diode laser or micro solid-state laser of suitable wavelength in the IR in the low power range can be used for providing a pulsed emission of a low spectral bandwidth and high radiation quality which are both substantially maintained during a subsequent amplification. The good radiation quality obtained after amplification by means of fiber amplifiers <NUM>, <NUM> is advantageous for a possible further frequency multiplication of the original infrared wavelength to obtain the UV wavelength preferred for atmospheric LIDARs.

An important step forward in the art has been made in recent years in the field of photo receivers and signal evaluation techniques and makes it possible to measure the very weak backscattering signals of individual pulses from the earth atmosphere. This applies to both different techniques as used today in LIDAR and based on the one hand on the property of light as a particle stream, i.e. direct reception involving intensity detection or single photon count, and on a wave action through coherence reception involving signal superimposition on the other hand. Advantageous embodiments of the receiving device <NUM> and of a signal evaluation device <NUM> utilize the progress of at least one of these two technologies.

Embodiments for direct reception as shown for example in the <FIG>, use a photo detector <NUM> with high signal dynamics in the reception channel - receiver <NUM>, the photo detector <NUM> being capable of detecting individual photon events in the reception signal of the broadband Rayleigh and the narrowband Mie scattering and of counting up to a high rate or integrating in analogous manner. In configurations of the LIDAR arrangement <NUM> and of the LIDAR method, the frequency coding task is solved and the separation of the optical signals achieved in that in the direct reception (as shown for example in <FIG>) on the transmission side of the LIDAR arrangement <NUM> the optical frequency of the pulses along the transmission pulse series is successively shifted by a small amount. Upon reception, the dispersive element <NUM> is added to spatially separate the frequency of the received signals before these signals meet a matrix sensor <NUM>, in particular the photo detector array <NUM> - which may happen in some circumstances also via an optional wavelength analyzer for differentiating minor frequency shifts of the laser signal in the measurement medium (e.g. Doppler shift) - in order to assign the signals to the related transmission pulses.

First of all, possible constructions for the direct reception technology are described in detail with reference to the illustrations of the <FIG>. In the following there will be particularly discussed the signal unbundling in relation to the direct reception technique.

In a preferred embodiment of the LIDAR arrangement <NUM> there is provided that the entire laser transmitter <NUM> is composed of an oscillator <NUM>, a pre-amplifier <NUM> and a final amplifier <NUM> (master oscillator power amplifier, MOPA <NUM>) comprising an optional frequency multiplication device <NUM> for a subsequent frequency multiplication. Further, the embodiments of the LIDAR arrangement <NUM> and the LIDAR method provide that the frequency shift proposed here is carried out in the oscillator stage in a distributed reflection bragg (DRB) laser diode or in a micro crystal laser resonator. The amplification of each frequency-shifted signal then takes place in subsequent one or two-fiber amplifiers followed by an optional frequency multiplication up to the target power in a stage suitable therefor.

For the fast shifting of the transmission frequency from pulse to pulse, embodiments of the LIDAR arrangement <NUM> and of the LIDAR method first provide a fast direct shift of the optical frequency of the oscillator <NUM> or the use of several chronologically pulsed lasers L1, L2, L3. LM of different fixed emission wavelengths. There can be used for example several laser diodes of emission wavelengths in the range of fiber amplification (in the range of about <NUM> or other wavelength ranges), for example corresponding to the frequency spacing used in fibers in frequency division multiplexing, which offers the advantage that the usual dispersive elements in the field of fiber optics common for WDM can be used on the receiving side.

A second method is the direct change of the resonator frequency of the laser resonator by a stepwise shift of the optical spacing of the resonator mirrors. This method is particularly attractive for short resonators with a broad frequency spacing of the longitudinal modes, i.e. of a micro laser. Because here only one mode is within the amplification band width, which is <NUM> or <NUM> in a Nd:YAG material for example and has a similar width in semiconductor diodes. The change of the emission frequency, i.e. of the optical spacing of the final mirrors in the resonator, can then be made for both kinds of the laser with fast temperature changes of the semiconductor material by introducing stress via a piezoelectric element for example or by moving an external resonator mirror with piezoelectric elements for example.

A third method of frequency modulation of a laser is the use of an internal or external electro-optical or acousto-optical modulator.

As discussed above, it is proposed to design M pulses in such a manner that their optical frequency is different by a particular amount Δfn, wherein M is chosen such that: M/FMessung ≥ <NUM>/FGrenze in order to avoid ambiguity at the reception. Hence the entire frequency deviation Δfp passed through in each period on the transmission side is Δfp = M Δfn. This frequency deviation Δfp is chosen such that it lies within the frequency band width of the band width of the fiber amplifier <NUM>, <NUM> on the transmission side of the LIDAR. On the receiving side, Δfn is predetermined such that it is sufficiently large to be resolved if necessary together with the Doppler frequency shift by the dispersive element <NUM>.

In the first case, embodiments of the LIDAR arrangement <NUM> and the LIDAR method provide that after the reception of signal backscattered from the atmosphere with a telescope, the pulses of different wavelength are supplied separated in space to a detector array by means of a dispersive element <NUM>, e.g. a prism, a grating or a fiber-optical de-multiplexer, a reconfigurable de-multiplexer or an arrayed waveguide grating, and are then optionally coupled under different angles and/or different positions into an interferometer <NUM> such as a Fabry-Pérot interferometer or alternatively a Fizeau interferometer, if small frequency shifts of the received LIDAR signal such as a Doppler shift shall be measured, so that at the output of the interferometer several ring systems (interferograms) are produced at least partially separated in space so that the individual backscattering pulses can also be separated in space and analyzed. In this case, there is performed, so to speak, a first rough separation of the individual reception signals depending on the wavelength of the transmission pulses by means of a dispersive element <NUM> and a further separation and analysis of these signals (optionally along with the Doppler shift with respect to each of the pulses of different wavelength) with the aid of the interferometer <NUM>. In this process, the optical signals of the interferograms are converted into electrical signals using a 1D or 2D matrix sensor <NUM>.

Embodiments of the LIDAR arrangement <NUM> and the LIDAR method additionally provide that, if needed, a small portion of the radiation of the laser transmitter <NUM> is directly supplied to the dispersive element <NUM> as a frequency or wavelength reference for the Doppler-shifted signals by means of a switch in order to serve as a reference signal. In the Figures, this switch is shown as a part of a reference signal line <NUM>.

Two embodiments of the LIDAR arrangement <NUM> for these tasks are schematically represented in <FIG> and <FIG>. Both Figures show on the left side thereof the master oscillator <NUM> that can be switched in several frequency steps and comprises several lasers L1, L2,. LM emitting a pulse series f<NUM>, f<NUM>,. fm of a suitable pulse frequency and comprising a suitable frequency shift between the individual pulses, and a beam combiner <NUM> for coupling the outputs of the lasers L1, L2,. LM to a common output (especially fiber). Further, embodiments of the LIDAR arrangement <NUM> show a pre-amplifier <NUM> and a post-amplifier <NUM> (booster) for amplifying the pulse energy at the primary wavelength, which mostly is in the IR wavelength range, and an optional frequency multiplying device <NUM> for an optional frequency tripling up to the UV wavelength range. Further shown in <FIG> and <FIG> is the emission of the pulse series to a remote soft target <NUM> - one example of a measurement object - and the reception thereof by the receiver <NUM>.

<FIG> shows an embodiment of the LIDAR arrangement <NUM> designed as a backscatter LIDAR arrangement for the direct reception comprising a series-switchable laser array as a master oscillator <NUM> and comprising downstream fiber amplifiers <NUM>, <NUM>, an optional frequency multiplier <NUM> on the transmission side, and a dispersive element <NUM> for resolving the reception signal into a point spectrum, and a 1D matrix sensor <NUM> (especially a matrix sensor comprising an A7D converter) (and an intermediate register <NUM>) on the receiving side.

<FIG> shows an embodiment of the LIDAR arrangement <NUM> designed as a Doppler LIDAR arrangement for direct reception and comprising a series of lasers L1, L2,. LM including a beam combiner <NUM> as a master oscillator <NUM>, fiber amplifiers <NUM>, <NUM>, optional frequency multipliers <NUM>, a dispersive element <NUM>, a Fabry-Pérot interferometer frequency analyzer <NUM> comprising an interferometer designed as a Fabry-Pérot interferometer, a 2D matrix detector with an A/D converter - one further example of the matrix sensor <NUM> - and an intermediate register <NUM> for recording the measurement data <NUM>.

Both embodiments of the arrangement according to <FIG> and <FIG> are different from each other with regard to the spectral resolution, i.e. whether the LIDAR is a pure backscattering LIDAR or a Doppler LIDAR. In both cases, the backscattering signal is received by means of reception electrodes <NUM> and is transmitted to the dispersive element <NUM>, i.e. in the present case to a prism or to a different one of the aforementioned dispersive elements, for a rough separation of the reception signals of the individual transmission frequencies. In a backscattering LIDAR, in which the signals are only separated by frequency, the reception signals can then be recorded at this point as point spectra <NUM> of the laser sources using a linear 1D photo detector array <NUM> as shown in <FIG>.

For a finer frequency separation, such as in the Doppler LIDAR, a Fabry-Pérot interferometer is used as a frequency analyzer for example, with subsequent imaging of its interferograms on a suitable 2D matrix detector <NUM> as shown in <FIG>.

The free spectral range of the Fabry-Pérot interferometer (FPI) is ΔfFP = c/<NUM>FP, wherein LFP describes the plate spacing of the interferometer <NUM>. Accordingly, the free spectral range at a plate spacing of LFP = <NUM> is ΔfFP = <NUM> for example. This is set in such a manner that it is sufficient for covering at least the greatest Doppler frequency shift in the Doppler LIDAR plus M times the frequency shift.

Avalanche CMOS or CDD photo detector arrays and MCP (multichannel plates) image intensifiers for example are suitable as a linear photo detector <NUM> or matrix photo detector (matrix sensor <NUM>) for the single photon detection.

In embodiments of the LIDAR arrangement <NUM> and of the LIDAR method, the point spectra <NUM> and interferograms <NUM> are charged side by side over a fixed time interval after the photo detector <NUM>, <NUM> and after an analog-to-digital conversion and can then be read out in parallel at a considerably lower frequency than the pulse frequency used, and their further signal processing involving electronic processing can be performed in the conventional manner.

A further possible embodiment of the LIDAR arrangement <NUM> is shown in <FIG>. In this case, it is assumed that a single master laser <NUM> is used as a master oscillator <NUM> with a switchable modulator <NUM> for producing the optical frequency series previously described.

<FIG> shows as a signal on the matrix detector array <NUM> an image of concentrated interference rings <NUM>, which are either generated using a single interferometer <NUM> as previously described or an arrangement of two successive interferometers as a so-called tandem interferometer <NUM> with a different free spectral range and/or frequency, hence a new variant of frequency separation and analysis for both a backscattering and Doppler LIDAR.

Such a tandem interferometer <NUM> comprises for instance two serial FP interferometers with a different plate spacing: one with a short plate spacing in order to achieve a longer overall free spectral range at a spectral resolution of the second FP interferometer with the larger plate spacing. In this case, the first Fabry-Pérot interferometer with a large free spectral range takes over the role of the dispersive element <NUM>. Other than in the previous case, the interferometers <NUM> are not laterally offset, but are concentrically arranged so that a different ring radius corresponds to a different frequency of each laser pulse. In this case, the second Fabry-Pérot interferometer again serves for the measurement of a Doppler shift that may be required.

<FIG> shows a single laser <NUM> as a master oscillator <NUM> comprising an external frequency modulator <NUM>, fiber amplifiers <NUM>, <NUM>, a tandem Fabry-Pérot interferometer <NUM>, a matrix sensor <NUM> including an A/D converter, and an intermediate register <NUM> for recording the measurement data. In this case, the interferograms <NUM> are individual concentric ring systems with a radial distance of the free spectral range of the FPI corresponding to the small plate spacing that covers the whole range of the Doppler shift to be measured. Other combinations are also possible.

Besides a prism as shown in <FIG> and <FIG> and an FPI as shown in <FIG>, also a "fiber-optical de-multiplexer (OADM)", a "reconfigurable fiber-optical de-multiplexer (ROADM)" or an "arrayed waveguide grating (AWF)" can be used as a dispersive element <NUM>.

Some embodiments of the LIDAR arrangement <NUM> and of the LIDAR method further provide scanning of the measurement object for instance transversely to the moving direction of an aircraft or satellite using a scanner <NUM> upstream of transmission telescope <NUM> over discrete angular positions within a small angular range and receiving the backscatter by means of a receive telescope <NUM> that covers the whole angle transmission range as shown in <FIG>.

<FIG> shows the scanning of a small angular range with the transmission beam in discrete steps (A, B, C) and the receipt of the backscatter within the fixed same angular range of a receive telescope <NUM>.

In this case, the different receiving axes within the FOV (field of view) of the receive telescope <NUM> can be defined by an array of glass fibers <NUM> in its focal plane as this is shown in more detail in <FIG> and <FIG>.

<FIG> shows the forwarding of the backscattering signals from several directions by means of glass fibers <NUM>, for a separation by means of a dispersive element <NUM> (e.g. prism) and the mapping as parallel rows of the measurements from different directions and with different transmission frequencies.

<FIG> accordingly shows a first case analogous to the arrangement shown in <FIG>, but with the receiving fiber array arranged perpendicular to the plane of refraction of the prism as the dispersive element <NUM>. In this case, the dot patterns <NUM> of the different transmission frequencies would be mapped on the photo detector array (matrix sensor <NUM>) in parallel rows of the different directions - see reference number <NUM>.

<FIG> shows a second case indicating an analogous extension of the functions of the arrangements of <FIG>, wherein the arrangement according to <FIG> uses a Fabry-Pérot interferometer <NUM> after a prism. According to <FIG>, the signal from the various receiving directions can be separately mapped on the photo detector array <NUM> as parallel rows of interferograms <NUM> - at pos. <NUM>, read separately into the intermediate register <NUM> and then further processed in the conventional manner.

Claim 1:
LIDAR arrangement (<NUM>) configured for atmospheric measurements, comprising a laser transmitter (<NUM>) for transmitting pulses of a laser radiation to a measurement object (<NUM>), and a receiver (<NUM>) for receiving pulses of the laser radiation backscattered from the measurement object (<NUM>),
wherein the laser transmitter (<NUM>) is designed for transmitting a pulse series in which successive pulses respectively comprise a particular optical frequency shift to each other and
wherein the receiver (<NUM>) includes a dispersive element (<NUM>) for spatially separating the pulses depending on the optical frequency by a frequency-dependent deflection, and a local resolution optical matrix sensor (<NUM>) on which the pulses spatially separated by the dispersive element are mapped, characterized in that the receiver (<NUM>) between the dispersive element (<NUM>) and the matrix sensor (<NUM>) comprises an interferometer (<NUM>) configured for mapping at least partially spatially separated interferograms (<NUM>) to the individual pulses of the pulse sequence on the matrix sensor (<NUM>).