Patent Description:
Document <CIT> describes a test instrument including a radiation source with a black body radiation source for providing energy in the infrared portion of the spectrum, and a Fabry-Perot etalon with at least first and second etalon plates, wherein the Fabry-Perot etalon is arranged to receive output from the radiation source. One or both of the etalon plates are associated with a wavelength scanning mechanism, comprising a piezoelectric or other actuator for translating the etalon plates with respect to one another.

Document <CIT> discloses an optical system comprising a telescope coupled to a spectrograph and a focal plane array, wherein a calibration source contains an optical frequency comb which provides for an absolute, repeatable frequency scale defined by a series of laser modes which are equally spaced across the frequency spectrum, and wherein an atomic clock is coupled to the optical frequency comb in order to stabilize the latter. A beam splitter allows coupling of the optical signal from the optical frequency comb with that of a continuous-wave laser which is locked to one comb line and simultaneously fed to a wavemeter, and a Fabry-Perot cavity is provided in the calibration source in order to filter out unwanted modes from the optical frequency comb spectrum.

In document <CIT>, a light supplying apparatus generating a highresolution comb for spectrometer calibration is described. A broadband light source emits light having a continuous spectrum, a collimating device collimates the light form the light source and conveys it to a Fabry-Perot-etalon which transmits narrow band light.

Spectrographs are generally used for determining the intensity of electromagnetic radiation as a function of wavelength or frequency. Specifically, to analyze the spectrum of the electromagnetic radiation such as light by a spectrograph, the light is directed onto a spectral separator of the spectrograph, which separates the light so that its spectral components propagate out of the spectral separator in different directions depending on their respective wavelengths. This spatially separated light is detected by a photodetector comprising a matrix of pixels (i.e., pixel segments) which can individually detect the light. By simultaneously recording the photosignal from each pixel segment receiving its corresponding spatially separated light, the spectrum of the incoming light is determined, the spectrum of the light incident on the spectral separator can be determined.

Especially in spectroscopic applications requiring high precision, such as in astronomical spectroscopy, the spectrograph needs to be accurately calibrated, in order to be able to draw conclusions on the actual wavelength dependent intensity I(λ) of the electromagnetic radiation. Such calibration comprises, in particular, ascertaining the so-called spectral sensitivity of the spectrograph, which is also known as the instrument spectral response function. The spectral sensitivity, S(λ), is wavelength dependent and is proportional to the quotient of the electrical signal and the corresponding intensity of light. Vice versa, from the amplitude A(λ) of the electrical signal transmitted by the photodetector upon which electromagnetic radiation with wavelength λ and intensity I(λ) is incident and the spectral sensitivity S(λ), the wavelength dependent intensity I(λ) of the electromagnetic radiation can be calculated by the following mathematical equation (<NUM>): <MAT>.

The spectral sensitivity can be determined by suitably irradiating the spectrograph by a laser beam whose wavelength can be tuned, such as by means of an optical parametric oscillator (OPO). In practice, the laser light tuned to a specific wavelength λ<NUM> and having a determined intensity I(λ<NUM>) propagates through the spectral separator, is diffracted thereby, and is then detected by the corresponding photodetector pixel segment which generates a photoelectrical signal with amplitude A(λ<NUM>). From these values, the spectral sensitivity value for λ<NUM> is determined. Subsequently, the laser is tuned to another wavelength λ<NUM>, and, from the corresponding intensity I(λ<NUM>) and the corresponding photoelectrical signal with amplitude A(λ<NUM>), the spectral sensitivity value for λ<NUM> is determined analogously. This process is repeated for all wavelengths to which the spectrograph is sensitive, to obtain the total spectral sensitivity of the instrument (i.e., the spectrograph). Against this background, it is an object of the present invention to provide a system and a method for more efficiently determining the spectral sensitivity of a spectrograph.

This object may be achieved by a system for and a method of determining the spectral sensitivity of a spectrograph according to claims <NUM> and <NUM>, respectively.

The system comprises an irradiation device configured to emit first electromagnetic radiation with a first spectrum including at least three substantially simultaneously emitted spectral lines, and a spectrograph comprising a spectral separator and a photodetector with a matrix of pixels. The spectral separator is arranged so as to receive the first electromagnetic radiation and to separate the first electromagnetic radiation so that the at least three spectral lines are assigned to different pixel segments from among the matrix of pixels. Herein, "substantially" simultaneously may mean that a possible time difference between the emission of the different spectral lines may be negligibly small as compared to the overall duration of the determining of the spectral sensitivity. Furthermore, the spectral separator as used herein may be a spatial spectral separator spatially separating the spectral lines, preferably, by at least one of diffraction and diffusion.

In the context of the present disclosure, the first electromagnetic radiation and/or the second electromagnetic radiation described below may include light with wavelengths above the X-ray band and below the radio frequency band, in particular, in one or more of the following spectral bands: ultraviolet (UV; from <NUM> - <NUM>), in particular, extreme ultraviolet (EUV; from <NUM> - <NUM>), and/or near ultraviolet (NUV; <NUM> - <NUM>); visible (VIS; <NUM> - <NUM>); and infrared (<NUM> - <NUM>), in particular, near infrared (NIR; <NUM> - <NUM>), mid infrared (MIR; <NUM> - <NUM>), and/or far infrared (FIR; <NUM> - <NUM>). , in this context, the term "light" may refer to electromagnetic waves with a wavelength spectrum within any of these bands. Insofar, the spectroscopy discussed herein may be understood as optical spectroscopy. It goes without saying that optical spectroscopy with respect to the spectral band to be analyzed may extend beyond the spectroscopy of visible light. Preferably, the first spectrum wave may extend, in wavelength, over a band from <NUM> to <NUM>, <NUM> to <NUM>, or <NUM> to <NUM>.

The system allows for calibrating the spectrograph in regard of its spectral sensitivity more quickly and easily. In particular, since the spectral lines are simultaneously emitted by the Irradiation device, and can be simultaneously detected by the photodetector upon being dispersed and/or diffracted by the spectrograph, tuning an irradiation device such as an OPO laser is unnecessary. Thus, the spectral sensitivity / spectral response function of the entire instrument (i.e., the spectrograph) may be determined significantly more quickly. Since the spectral lines are assigned to different pixels of the photodetector, the irradiation device and spectrograph may synergistically provide these advantages. In other words, the simultaneous emission of the spectral lines can be appropriately utilized by the photodetector with the matrix of pixels, since the pixels can be read out relatively quickly. In addition, the system may have a relatively simple and compact design, since optical components required for laser wavelength detuning, such as an OPO, may be avoided. This compact design is particularly advantageous for applications in space, such as astronomical spectroscopy.

The spectral lines may be distinct and/or separate from each other. Specifically, in a spectral diagram showing the intensity of the first electromagnetic radiation over wavelength, the spectral lines may be represented as separate peaks. For two neighboring spectral lines to be understood as being separate, their respective maxima may be spaced apart in wavelength at least by their full width at half maximum. For example, the at least three spectral lines may be spaced apart from each other by at least <NUM>, at least <NUM> or at least <NUM> or at least <NUM> or at least <NUM> or at least <NUM> or at least <NUM>. The respective maxima of neighboring spectral lines of the at least three spectral lines may be spaced apart by at most <NUM> or at most <NUM> or at most <NUM> or at most <NUM> or at most <NUM> or at most <NUM>. Furthermore, the number of the at least three spectral lines of the first spectrum may be at least <NUM>, at least <NUM>, at least <NUM>, at least <NUM>, at least <NUM>, or at least <NUM>.

The irradiation device comprises an irradiation source, which generates and emits a second electromagnetic radiation with a second spectrum which is a broadband or continuous spectrum and includes the at least three spectral lines as well as one or more further bands of the electromagnetic spectrum. It is noted that generating the second electromagnetic radiation may comprise converting electrical energy or further electromagnetic radiation other than the first or second electromagnetic radiation to the second electromagnetic radiation. The at least three spectral lines may form part of the further bands, i.e., lie within the further bands. It is noted that, herein, a broadband spectrum is generally understood as a spectrum which extends over a broader wavelength range than each of the spectral lines of the first spectrum. In a variant, the further bands may be one continuous band, comprising all of the at least three spectral lines. , the second spectrum may continuously extend over the first spectrum. In other words, the output power values of the irradiation source may be above <NUM> throughout the continuous spectrum. Each of the further bands or the continuous spectrum may extend over a wavelength range that is at least <NUM> or at least <NUM> or at least <NUM> or at least <NUM> or at least <NUM> wide. The Irradiation source may be SuperK EVO, by NKT Photonics INC.

Preferably, the irradiation source comprises a light source configured to output the second electromagnetic radiation. The light source may be, in particular, a broadband light source and/or a white light source. More specifically, the light source may comprise one or more of a laser, a semiconductor laser, a supercontinuum laser, a supercontinuum fiber laser, and a gas discharge lamp. In particular, it is preferred that the first electromagnetic radiation is not generated and/or emitted by a comb laser, to provide that the system is comparably compact. Accordingly, the first spectrum may be free of a frequency comb as generated by a comb laser.

Furthermore, the electromagnetic radiation may be pulsed or continuous wave. In particular, if the light source is a laser, the laser may be a pulsed laser, a modelocked laser or a continuous wave laser. Most preferably, the laser has a pulse repetition rate in the range of Megahertz or Gigahertz, in particular, between <NUM> and <NUM>. Further, the light source may comprise one or more waveguides such as optical fibers. Specifically, the second electromagnetic radiation, when exiting the irradiation source may be coupled to an optical fiber or fiber bundle. The light source may provide the second electromagnetic radiation with a total power of more than <NUM> mW or more than <NUM> W. The light source's average output power may be between <NUM> and <NUM> mW/nm.

Furthermore, the irradiation device may comprise an irradiation conversion device arranged to convert the second electromagnetic radiation to the first electromagnetic radiation before the first electromagnetic radiation is emitted by the irradiation device. The irradiation conversion device may be interposed between the irradiation source and the spectrograph. In particular, along the propagation direction or axis of the first and/or the second radiation, the irradiation conversion device may be arranged proximate to the irradiation source so that the second spectrum of the second electromagnetic radiation arrives at an entrance of the irradiation conversion device. In other words, the system for determining the spectral sensitivity of the spectrograph may be free of any element suitable for substantially modifying the second spectrum, such as an optical filter, between the irradiation source and the irradiation conversion device.

In particular, the irradiation conversion device may be a filter. The filter may be configured to filter out every portion of the second spectrum other than the at least three spectral lines. In a variant, the irradiation conversion device may be or may comprise a Fabry-Perot resonator having a resonator length, L. When the second electromagnetic radiation with the second spectrum is incident on the Fabry-Perot resonator, this resonator may be configured to transmit only the first spectrum including only the at least three spectral lines. The Fabry-Perot resonator may comprise a plurality of semi-transparent mirrors spaced apart by a distance. A cavity may be formed between the mirrors. The distance may be equal to the resonator length, L. The following equation (<NUM>) may be valid for the wavelengths, λn, of the at least three spectral lines: <MAT>.

Herein, the parameter n is an integer. The length, L, may be between <NUM> and <NUM>, in particular, between <NUM>,<NUM> and <NUM>. Furthermore, the Fabry-Perot resonator may have a free spectral range between <NUM> and <NUM>, preferably between <NUM> and <NUM>, and, more preferably, between <NUM> and <NUM>. For example, the free spectral range may be between <NUM> and <NUM>. Moreover, the Fabry-Perot resonator may have a finesse value between <NUM> and <NUM>, between <NUM> and <NUM>, or between <NUM> and <NUM>.

Moreover, it is conceivable that the resonator length, L, of the Fabry-Perot resonator is variable. Specifically, the Fabry-Perot resonator may be configured so that its resonator length, L, may be varied at most by such an extent that the at least three spectral lines remain assigned to the aforementioned different pixels from among the matrix of pixels. Preferably, varying the Fabry-Perot resonator length, L, does not shift any of the at least three spectral lines to another one of the pixels. Alternatively, it is conceivable that the resonator length, L, is changed to such an extent that the at least three spectral lines are shifted from one pixel to another. Specifically, the resonator length, L, may be varied by less than <NUM>% or less than <NUM>% or less than <NUM>% of the minimum value of the resonator length, in particular within the above mentioned boundaries from the length, L. For varying the length, the Fabry-Perot resonator may comprise a piezo element, which may be configured to set the resonator length, L, in dependence of a voltage applied to the piezo element.

In a variant, the Fabry-Perot resonator may be a fiber Fabry-Perot resonator. This configuration is particularly advantageous when the irradiation source is fibercoupled, i.e., when the second electromagnetic radiation is emitted by the irradiation source through an optical fiber. In this case, the optical fiber coupled to the irradiation source is preferably likewise coupled to an input port of the fiber Fabry-Perot resonator, so that aligning these optical components is unnecessary. In further detail, the fiber Fabry-Perot resonator may be lensless, and may consist of a single mode optical fiber arranged between two highly reflective multilayer mirrors. In particular, the fiber Fabry-Perot resonator may be enclosed in a housing, comprising the inlet port and an outlet port. It is noted that not only the inlet port, but also the outlet port may be configured for coupling a connector of an input optical fiber and output optical fiber, respectively, thereto. On the side of the output optical fiber opposite of the Fabry-Perot resonator, the output optical fiber may be configured to be coupled to the spectrograph. Except of the inlet and outlet ports, the housing may be closed, in order to block external radiation from being coupled to the Fabry-Perot resonator. The fiber Fabry-Perot resonator may be the product FFP-TF <NUM>-<NUM>-<NUM>-<NUM>-<NUM>-<NUM> of Micron Optics Inc.

In an example not falling under the scope of the invention, the irradiation source may be arranged outside of the Fabry-Perot resonator (i.e., outside of the cavity), in particular, on a side of the Fabry-Perot resonator opposite of the spectrograph with respect to the axis along which the first and/or second electromagnetic radiation propagates (propagation path). Note that the word "axis" is not meant as a straight axis herein. Rather, the direction of the axis may change between the irradiation source and the spectral separator. Preferably, the irradiation source is then configured to emit the second electromagnetic radiation towards the irradiation conversion device, so that the second electromagnetic radiation enters the Fabry Perot resonator by propagating through a mirror of the Fabry Perot resonator arranged opposite of the spectrograph, and the first electromagnetic radiation is output out of the Fabry Perot resonator through the mirror facing the spectral separator.

According to the invention, the irradiation source is arranged inside of the Fabry-Perot resonator, in particular, in the cavity located between the mirrors. Other than in the configuration, in which the irradiation source is arranged outside of the resonator, the second electromagnetic radiation may be emitted in the cavity, so that it does not propagate through any of the mirrors of the Fabry-Perot resonator. In this case, the irradiation source may comprise a laser medium, such as, in the form of a (doped) crystal, a (doped) glass, a semiconductor (e.g., gallium arsenide (GaAs), indium gallium arsenide (InGaAs), or gallium nitride (GaN)), or a liquid with a die. By this configuration, the degree of compactness of the system may be further increased.

The at least three substantially simultaneously emitted spectral lines may be equidistant, i.e. uniformly spaced, in frequency or wavelength. The spectral separator may be provided with a prism and/or a grating, in particular, an Echelle-grating, and may be arranged so that the first electromagnetic radiation propagates into the spectrograph such that the entire first spectrum may arrive at the spectral separator and may be separated thereby.

The photodetector may be a CCD chip. The CCD chip may be a linear (1D) chip or a 2D chip. If the CCD chip is a 1D chip, the number of pixels of the photodetector/the CCD chip may essentially corresponds to the number of the at least three spectral lines or may exceed the number of the at least three spectral lines by at most <NUM> % or at most <NUM> % or at most <NUM> %. Preferably, the photodetector is arranged such that each of the spectral lines is detected by another pixel of the chip. Specifically, if the photodetector is a CCD chip, a part of the first electromagnetic radiation corresponding to a first one of the at least three spectral lines is incident on a first pixel, another part of the first electromagnetic radiation corresponding to a second one of the at least three spectral lines is incident on a second pixel, a yet further part of the first electromagnetic radiation corresponding to a third one of the at least three spectral lines is incident on a third pixel, etc.. If the CCD chip is a 2D chip, the first, second, and third pixels may be arranged along a main direction, in particular, an edge of the chip.

Furthermore, some or all of the pixels may respectively comprise a plurality of sub-pixels. In this case, it is preferred that the irradiation conversion device comprises a Fabry-Perot resonator with variable length. The resonator may be configured such that changing the resonator length from a first length to a second length causes each of the at least three spectral lines to shift in wavelength, and to become assigned to a different sub-pixel of the respective pixel assigned to the respective spectral line. In further detail, when the resonator has a first length, the first spectral line may be assigned to a first sub-pixel of the first pixel, the second spectral line may be assigned to a first sub-pixel of the second pixel, and the third spectral line may be assigned to a first sub-pixel off the third pixel. When the resonator has the second length, which may be larger than the first length, the spectral lines may be shifted in wavelength according to above equation (<NUM>), so that the first spectral line may be assigned to a second sub-pixel of the first pixel, the second spectral line may be assigned to a second sub-pixel of the second pixel, and the third spectral line may be assigned to a second sub-pixel of the third pixel. The first sub-pixels may be different from the second sub-pixels, and may be arranged on the CCD chip adjacent to one another.

The system may further comprise a controller configured for controlling the irradiation device and the spectrograph as well as all of their above described components. The controller may comprise a storage section in which predetermined intensity data of the first electromagnetic radiation incident on the spectral separator is stored. The intensity data may comprise a power spectrum of the first electromagnetic radiation, comprising power values (I(λn)) for each of the wavelengths λn detectable by the spectrograph. The controller is further configured to determine the spectral sensitivity based on an electrical signal output by the photodetector and above equation (<NUM>).

The method of determining the spectral sensitivity of a spectrograph may comprise emitting a first electromagnetic radiation with a first spectrum including at least three substantially simultaneously emitted, equidistant spectral lines by an irradiation device; receiving the electromagnetic radiation by a spectral separator of a spectrograph; separating the electromagnetic radiation; detecting the separated electromagnetic radiation by a photodetector of the spectrograph, wherein the photodetector comprises a matrix of pixels, wherein the at least three spectral lines are assigned to different pixels from among the matrix of pixels; and determining the spectral sensitivity of the spectrograph based on an (electrical) photodetector signal intensity of the pixels.

The method may be carried out on ground or in space, in particular, in Earth orbit, and/or may further comprise method steps corresponding to any of the above described properties or functions of the system for determining the spectral sensitivity of a spectrograph.

Preferred embodiments of a system for determining the spectral sensitivity of a spectrograph are now described in further detail by referring to the enclosed schematic drawings, wherein.

<FIG> show a system <NUM> for determining the spectral sensitivity of a spectrograph <NUM>, which comprises an irradiation device <NUM> with an irradiation source <NUM> and an irradiation conversion device <NUM>, herein, formed as a Fabry-Perot resonator, in particular, a fiber Fabry-Perot resonator in this variant. The spectrograph <NUM> comprises a separator <NUM> and a photodetector <NUM> with a plurality of pixels forming a matrix of pixels P1-Pm. Herein, the photodetector <NUM> is a linear array CCD photodetector, in which the pixels P1-Pm are arranged vertically in a column in the view of <FIG>.

Alternatively, the photodetector <NUM> may be a 2D array CCD photodetector with further pixels arranged in rows perpendicular to the column of pixels and extending from the pixels P1-Pm. The spectral separator <NUM> is a prism or grating and is arranged so as to receive the first electromagnetic radiation <NUM> and to separate the first electromagnetic radiation <NUM> so that the at least three spectral lines S1-Sk are assigned to, i.e., incident on and detected by different pixels from among the matrix of pixels P1-Pm.

The irradiation device <NUM> is configured to generate and emit first electromagnetic radiation <NUM> having a first spectrum including k equidistant spectral lines S1-Sk, wherein, in this variant, k equals <NUM>. In <FIG> and the remaining drawings, only <NUM> of these spectral lines are shown for clear illustration. The number of pixels m is chosen to be <NUM> times the number of spectral lines, namely <NUM>, wherein only the first five and the last pixel are shown in the drawings for clarity. In the intensity over wavelength diagram I(λ), the spectral lines are separate equidistant peaks, again for illustration purposes, all having the same amplitude. The free spectral range of the Fabry-Perot resonator is, in this case, approximately <NUM>. Note that the amplitudes of the peaks may differ. Since the first spectrum characterizes the first electromagnetic radiation, all spectral lines S1-Sk, i.e. peaks, are simultaneously emitted by the irradiation device <NUM>.

As shown in <FIG>, the first electromagnetic radiation <NUM> has the first spectrum not only at the site where it is output from the Fabry-Perot resonator (irradiation conversion device <NUM>), but also where it enters the spectrograph <NUM>. In other words, the portion of the first electromagnetic radiation corresponding to any of the spectral lines S1 to Sk is not hindered from propagating from the irradiation conversion device <NUM> to the spectrograph <NUM>. Nevertheless, it is conceivable that optical elements such as one or more mirrors or one or more lenses are arranged between the irradiation device <NUM> and the spectrograph <NUM> for guiding the first electromagnetic radiation.

The irradiation source <NUM> of the irradiation device <NUM> is a white light source configured to emit second electromagnetic radiation <NUM> with a second (broadband) spectrum which is continuous and includes all spectral lines S1-Sk. Herein, the second spectrum extends over a wavelength band of <NUM> width, specifically from <NUM> to <NUM>. In particular, the irradiation source <NUM> is a supercontinuum laser which is fiber coupled such that the second electromagnetic radiation is output from the irradiation source <NUM> through an optical fiber or fiber bundle.

The irradiation conversion device <NUM> (i.e., the Fabry-Perot resonator) is arranged to convert the second electromagnetic radiation <NUM> to the first electromagnetic radiation <NUM> to be emitted by the irradiation device <NUM>. In further detail, the second electromagnetic radiation <NUM> emitted by the irradiation source <NUM> outside of the Fabry-Perot resonator is incident on a first semitransparent mirror <NUM> of the Fabry-Perot resonator. A second semitransparent mirror <NUM> is arranged on the side of the first semitransparent mirror <NUM> opposite of the irradiation device at a distance corresponding to the resonator length L of the Fabry-Perot resonator from the first semitransparent mirror <NUM>.

The Fabry-Perot resonator has a finesse on the order of <NUM> and is configured to transmit only the electromagnetic waves of the second spectrum which are resonating between the mirrors <NUM> and <NUM>, i.e., for which the equation λn=<NUM>/n is valid, wherein n is an integer. Assuming that λn are equal to the wavelengths at which the peaks/spectral lines S1-Sk are present in the first spectrum, the Fabry-Perot resonator filters out all of the second spectrum except of the first spectrum (i.e., the first spectral lines). Accordingly, the first electromagnetic radiation <NUM> with the first spectrum including the at least three spectral lines S1-Sk is transmitted through the irradiation conversion device <NUM> to the spectrograph <NUM>.

<FIG> shows an irradiation device <NUM> of a further system <NUM> for determining the spectral sensitivity of a spectrograph <NUM>. This irradiation device <NUM> differentiates from the irradiation device <NUM> of the system <NUM> of <FIG> by its irradiation source <NUM> being arranged inside the cavity of the Fabry-Perot resonator, in particular, between the semi-transparent mirrors <NUM>, <NUM>, rather than outside of the cavity. The irradiation source <NUM> may comprise a laser medium or gain medium, so that the irradiation source <NUM> in combination with the Fabry-Perot resonator form a Fabry-Perot laser. Otherwise, the irradiation device <NUM> of <FIG> and the system <NUM> of which this irradiation device <NUM> forms part may comprise any of the features of the irradiation device <NUM> and the system <NUM> of <FIG>, respectively.

<FIG> shows a yet further system <NUM> for determining the spectral sensitivity of a spectrograph <NUM>. This system <NUM> differentiates from the system <NUM> of <FIG> by the Fabry-Perot resonator having a variable length. Herein, the Fabry-Perot resonator is configured for varying the resonator length between a first length at which the spectral line S1 is assigned to a first pixel, e.g., P1 and a second length at which the spectral line S1 is assigned to a second pixel, e.g., P2, which may in a further variant not be adjacent to the first pixel. Accordingly, when the Fabry-Perot resonator has the first length, the portion of the first electromagnetic radiation <NUM> corresponding to the first spectral line S1 may be detected by the first pixel P1, the portion of the first electromagnetic radiation corresponding to the second spectral line S2 may be detected by a second pixel P3, the portion of the first electromagnetic radiation <NUM> corresponding to the third spectral line S3 may be detected by a third pixel P5, etc., and the portion of the first electromagnetic radiation <NUM> corresponding to the k-th spectral line Sk may be detected by the (m-<NUM>)-th pixel.

Vice versa, when the Fabry-Perot resonator has the second length, the portion of the first electromagnetic radiation <NUM> corresponding to the first spectral line S1 may be detected by pixel P2 adjacent to the first pixel P1, the portion of the first electromagnetic radiation <NUM> corresponding to the second spectral line S2 may be detected by pixel P4 adjacent to the second pixel P3, the portion of the first electromagnetic radiation <NUM> corresponding to the third spectral line S3 may be detected by a pixel adjacent to the third pixel P5, etc., and the portion of the first electromagnetic radiation corresponding to the k-th spectral line Sk may be detected by the pixel Pm adjacent to the (m-<NUM>)-th pixel (not shown in the drawings). Note that additional pixels may be located between pixels P2 and P3, between pixels P4 and P5, etc., i.e., between pixels not specified above to be adjacent to each other. On the other hand, adjacent pixels may be directly adjacent to each other without any pixel interposed between them.

Otherwise, the system <NUM> of <FIG> may comprise any of the features of the systems <NUM> of <FIG>, respectively.

Claim 1:
A system (<NUM>) for determining the spectral sensitivity of a spectrograph (<NUM>),
comprising
an irradiation device (<NUM>) configured to emit first electromagnetic radiation (<NUM>) with a first spectrum including at least three simultaneously emitted, spectral lines (S1-Sk) equidistant in wavelength, and
a spectrograph (<NUM>) comprising a spectral separator (<NUM>) and a photodetector (<NUM>) with a plurality of pixels (P1-Pm), wherein the spectral separator (<NUM>) is arranged so as to receive the first electromagnetic radiation (<NUM>) and to separate the first electromagnetic radiation (<NUM>) so that the at least three spectral lines (S1-Sk) are assigned to different pixels from among the plurality of pixels (P1-Pm), wherein the irradiation device (<NUM>) comprises
an irradiation source (<NUM>) configured to emit second electromagnetic radiation (<NUM>) with a second spectrum which is broadband or continuous and includes the at least three spectral lines (S1-Sk), and
an irradiation conversion device (<NUM>) arranged to convert the second electromagnetic radiation (<NUM>) to the first electromagnetic radiation (<NUM>) to be emitted by the irradiation device (<NUM>), wherein the irradiation conversion device (<NUM>) comprises a Fabry-Perot resonator having a resonator length, L, and being configured to transmit the first electromagnetic radiation (<NUM>) including the at least three spectral lines (S1-Sk), wherein the irradiation source (<NUM>) is arranged inside of the Fabry-Perot resonator.