EP2275998B1 - Dispositif de verification de documents de valeur - Google Patents
Dispositif de verification de documents de valeur Download PDFInfo
- Publication number
- EP2275998B1 EP2275998B1 EP10011629.2A EP10011629A EP2275998B1 EP 2275998 B1 EP2275998 B1 EP 2275998B1 EP 10011629 A EP10011629 A EP 10011629A EP 2275998 B1 EP2275998 B1 EP 2275998B1
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- European Patent Office
- Prior art keywords
- luminescence
- previous
- luminescence sensor
- detector
- radiation
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- 229910052710 silicon Inorganic materials 0.000 claims description 10
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Images
Classifications
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- G—PHYSICS
- G07—CHECKING-DEVICES
- G07D—HANDLING OF COINS OR VALUABLE PAPERS, e.g. TESTING, SORTING BY DENOMINATIONS, COUNTING, DISPENSING, CHANGING OR DEPOSITING
- G07D7/00—Testing specially adapted to determine the identity or genuineness of valuable papers or for segregating those which are unacceptable, e.g. banknotes that are alien to a currency
- G07D7/06—Testing specially adapted to determine the identity or genuineness of valuable papers or for segregating those which are unacceptable, e.g. banknotes that are alien to a currency using wave or particle radiation
- G07D7/12—Visible light, infrared or ultraviolet radiation
- G07D7/121—Apparatus characterised by sensor details
-
- G—PHYSICS
- G07—CHECKING-DEVICES
- G07D—HANDLING OF COINS OR VALUABLE PAPERS, e.g. TESTING, SORTING BY DENOMINATIONS, COUNTING, DISPENSING, CHANGING OR DEPOSITING
- G07D7/00—Testing specially adapted to determine the identity or genuineness of valuable papers or for segregating those which are unacceptable, e.g. banknotes that are alien to a currency
- G07D7/06—Testing specially adapted to determine the identity or genuineness of valuable papers or for segregating those which are unacceptable, e.g. banknotes that are alien to a currency using wave or particle radiation
- G07D7/12—Visible light, infrared or ultraviolet radiation
-
- G—PHYSICS
- G07—CHECKING-DEVICES
- G07D—HANDLING OF COINS OR VALUABLE PAPERS, e.g. TESTING, SORTING BY DENOMINATIONS, COUNTING, DISPENSING, CHANGING OR DEPOSITING
- G07D7/00—Testing specially adapted to determine the identity or genuineness of valuable papers or for segregating those which are unacceptable, e.g. banknotes that are alien to a currency
- G07D7/06—Testing specially adapted to determine the identity or genuineness of valuable papers or for segregating those which are unacceptable, e.g. banknotes that are alien to a currency using wave or particle radiation
- G07D7/12—Visible light, infrared or ultraviolet radiation
- G07D7/1205—Testing spectral properties
Definitions
- a device for determining the emission spectra in securities with fluorescent security features, which has a high-resolution spectrophotometer, a suitable excitation energy source and optionally serving as a dispersion element narrow-band interference filter.
- the devices can be used in all types of devices in which optical radiation, in particular luminescence radiation, is tested. Although not limited thereto, the following describes as a preferred variant the checking of banknotes in banknote processing devices, which can serve, for example, for counting and / or sorting and / or depositing and / or paying out banknotes.
- the banknote sorting device 1 in this case has an input compartment 3 for banknotes BN in a housing 2, into which banknotes to be processed BN can either be input manually from the outside or banknotes bundles can be fed automatically, if necessary after a preceding debrapping.
- the banknotes BN entered into the input compartment 3 are separated from the stack by a singler 4 and transported through a sensor device 6 by means of a transport device 5.
- the sensor device 6 can have one or more sensor modules integrated in a common housing or mounted in separate housings. The sensor modules can serve, for example, to check the authenticity and / or the state and / or the nominal value of the banknotes BN being tested.
- the light sources 14 can emit light of a plurality of different wavelengths or wavelength ranges, it can be provided that the individual wavelengths or wavelength ranges can be selectively activated.
- the light emanating from the laser diode 14 is irradiated by means of an imaging optical system 15, 16, 17 on a banknote to be tested.
- the imaging optics comprises a collimator lens 15, a deflection mirror as a beam splitter 16, in particular a dichroic beam splitter 16, which emanating from the laser diode 14 and through the collimator lens 15 deflects laser beam formed by 90 °, and a condenser lens 17 with a large opening angle, which images the deflected laser beam through a front glass 18 preferably perpendicular to the conveyed by the transport system 5 in the direction T to be examined banknote BN and thus the banknote BN for emission stimulated by luminescence radiation
- the optics for imaging the luminescence radiation onto a photosensitive detector unit 21 likewise comprises the front glass 18, the condenser lens 17 and the mirror 16 at least partially transparent to the luminescence radiation to be measured.
- the optic subsequently has another condenser lens 19 with a large opening, followed by a filter 20, which is designed to block the illumination wavelength of the light source 14 and other wavelengths not to be measured, and a deflection mirror 23.
- the deflecting mirror 23 serves to fold the beam path and to redirect the luminescence radiation to be measured to an imaging grating 24 or another device for spectral decomposition 24.
- the deflection mirror is advantageously mounted parallel or nearly parallel to the image plane of the spectrometer for an extremely compact design (angle ⁇ 15 degrees).
- the imaging grating 24 in this case has a wavelength-dispersing element with concave mirror 26, which preferably images the luminescence radiation of first order or minus first order onto the detector unit 21.
- the detector unit 21 preferably has a detector row 22 of a plurality of photosensitive pixels arranged in series, ie pixels, as they are z. B. in relation to the FIGS. 6 or 7 will be described below by way of example.
- the deflecting mirror 23 is positioned with respect to the imaging grating 24 so that the entrance slit AS falls onto the region of the deflecting mirror 23. Since in this way the beam cross section of the radiation to be deflected on the deflection mirror 23 is particularly small, the deflection mirror 23 itself can also have particularly small dimensions. If the deflecting mirror 23 is a component of the detector unit 21, the deflecting mirror 23 can thereby not only according to FIG FIG. 2 above, but also adjacent to the photosensitive areas of the detector unit 21 are attached.
- the light source 14 for the excitation of luminescence radiation generates an elongated illumination surface 35 extending in the transport direction T on the banknote BN to be checked.
- This variant has the advantage that the luminescent, in particular phosphorescent feature substances present in the banknotes BN are usually pumped up longer by the illumination surface extending in the transport direction during the onward transport at the luminescence sensor 12 and, in particular, the radiation intensity of the luminescent phosphorescent feature substances is increased ,
- FIG. 5 illustrates a related snapshot.
- An elongated illumination surface 35 extending in the transport direction T can be understood to mean that the illumination radiation at any given time irradiates an arbitrarily shaped surface, in particular a rectangular track on the banknote, which is significantly larger in the transport direction T than perpendicular to the transport direction T.
- the extent of the illumination surface 35 in the transport direction T at least twice, especially preferably be at least three times, four times or five times as long as the extension perpendicular to the transport direction T.
- Fig. 5 With another hatching also the image surface 36, ie the entrance hatch 36 of the spectrometer 30 is illustrated, ie that region of the banknote BN which is imaged on the spectrometer 30 at the given time in accordance with the dimensions of the entry slit AS. It can be seen that the length and width of the entrance hatch 36 of the spectrometer 30 are preferably smaller than the corresponding dimensions of the illumination surface 35 of the laser diode 14. This allows greater adjustment tolerances for the individual sensor components.
- the illumination surface 35 extends substantially further in the transport direction T as compared to the transport direction T compared to the image surface 36. This is particularly advantageous for exploiting the increased inflation effect.
- the illumination surface 35 and the image surface 36 overlap only partially in the transport direction T.
- the luminescence sensor 6 can be used both in devices 1 in which the banknotes BN are transported in the illustrated transport direction T and in devices 1 in which the banknotes BN be transported in opposite direction -T.
- different detector units 21, 27 are used for detecting the luminescence radiation, in particular the luminescence radiation emanating from the device for spectral decomposition 24, ie the imaging grating 24.
- a filter may be provided to only one or more given wavelengths or regions to be measured, wherein the measurable spectral regions of the different detector units 21, 27 are preferably different and, for example, only partially or not overlap.
- a plurality of further detector units 27 may be present, which measure in different wavelengths or ranges.
- the plurality of further detector units 27 may be spaced apart from each other or may be in a sandwich structure, as shown in FIG DE 1 0127 837 A1 is described by way of example
- this further detector unit 27 in particular when it is designed for measuring zeroth order of the spectrometer 30, tilted with respect to the imaging grating 24 and the detector line 22 may be arranged to avoid a disturbing back reflection on the concave mirror 26 ,
- a radiation-absorbing light trap such as a black-colored surface at the end of the beam path of the outgoing radiation from the further detector unit 27 may be present.
- the reference sample 32 can therefore also be mounted outside of the housing 13, in particular on the side opposite to the banknote BN to be measured, and e.g. be integrated in a counter element, such as a plate 28.
- an additional detector unit 33 may be present as a separate component or integrated in the plate 28.
- the additional detector unit 33 may be e.g. one or more photocells for measuring the radiation of the laser diode 14 and / or the luminescence radiation of the banknote BN which has passed through the front glass 18 and possibly through the banknote BN.
- the plate 28 may be slidably mounted in a guide in the direction P, so that either either the reference sample 32 or the photocell 33 can be brought into alignment with the illumination radiation of the laser diode 14.
- the light source 14 has two laser diodes 51, 52 arranged perpendicular to one another which emit at different wavelengths, the radiation of the individual laser diodes 51, 52 being e.g. can be coupled by a further dichroic beam splitter 53, so that the same illumination surface 35 or overlapping or spaced illumination surfaces 35 can be irradiated on the banknote BN.
- the radiation of the individual laser diodes 51, 52 being e.g. can be coupled by a further dichroic beam splitter 53, so that the same illumination surface 35 or overlapping or spaced illumination surfaces 35 can be irradiated on the banknote BN.
- the luminescence sensor 6 preferably has in the housing 13 itself a control unit 50 which serves for signal processing of the measured values of the spectrometer 30 and / or for power control of the individual components of the luminescence sensor 6.
- a conventional detector line 22 is shown in sections, which usually has more than 100 juxtaposed photosensitive picture elements (referred to as pixels 40 for short) (of which FIG Fig. 6 only the first seven left pixels 40 are shown) which are of equal size and spaced apart on or in a substrate 41 which is approximately equal to the width of the pixels 40
- individual pixels 40 have different dimensions, in particular in the direction of dispersion of the luminescence radiation to be measured, as described in US Pat Fig. 7 is shown. Since usually not all wavelengths of the spectrum, but specifically only individual wavelengths or wavelength ranges are evaluated, the pixels 40 can be constructed adapted to the respective wavelengths (ranges) to be evaluated.
- the detector line 22 may consist of a different material in the cases mentioned.
- detectors made of silicon which are sensitive below about 1100 nm, and particularly suitable for measurement in the infrared spectral range detector array 22 of InGaAs, which are sensitive above 900 nm.
- Such an InGaAs detector array 22 will be deposited directly on a silicon substrate 42 having an amplifier stage made in silicon technology for amplifying the analog signals of the pixels 40 of the InGaAs detector array 22. This also provides a particularly compact design with short signal paths and increased signal-to-noise ratio.
- the detector line 22 with a few pixels 40 (eg after Fig. 7 ), preferably only a relatively small spectral range of less than 500 nm, more preferably less than or of about 300 nm is detected. It can also be provided that the detector line 22 has at least one pixel 40 which is photosensitive outside the luminescence spectrum of the banknotes BN to be measured in order to carry out normalizations such as baseline determination in the evaluation of the measured luminescence spectrum.
- the imaging grating 24 is preferably more than about 300, more preferably more than about 500 lines / mm, i. Have diffraction elements in order to still allow a sufficient dispersion of the luminescence radiation on the detector element 21 despite the compact construction of the luminescence sensors 6 according to the invention.
- the distance between the imaging grating 24 and the detector element 21 may preferably be less than approximately 70 mm, particularly preferably less than approximately 50 mm.
- a readout of the individual pixels 40 of the detector line 22 may be z. B. using a shift register serial. According to the invention, however, a parallel readout of individual pixels 40 and / or pixel groups of the detector row 22 will take place.
- the three left-hand pixels 40 are read out one at a time by measuring the measuring signals of these pixels 40 with the aid of one amplifier stage 45 each. Component of the silicon substrate 42 after Fig. 7 , amplified and each supplied to an analog / digital converter 46.
- the two right-hand pixels in the schematic representation of Fig. 9 in turn, first amplified by separate amplifier stages 45, then a common multiplexing unit 47, which may optionally include a sample & hold circuit, and then a common analog / digital converter 46 is supplied, which is connected to the multiplexing unit 47
- the parallel readout of a plurality of pixels 40 or pixel groups thereby made possible short integration times and a synchronized measurement of the banknote BN. This measure also contributes to an increase in the signal-to-noise ratio.
- Deflection mirror 23 for deflecting the luminescence radiation to be detected on the spectrometer 30 may be connected directly to the detector unit 21, as for example in Fig. 2 is shown.
- Fig. 7 shows a modified variant in which the deflection mirror 23 is applied directly on a common carrier with the detector line 22, that is, in particular on the silicon substrate 42.
- the deflecting mirror 23 may also be mounted on a cover glass of the detector unit 21, for example.
- a photodetector such as a photocell 56
- a photocell 56 may be present below the deflecting mirror 23 below the deflecting mirror 23 .
- This preferred variant is exemplary in the FIG. 8 pictured, which is a cross section along the line II of FIG. 7 shows.
- the deflecting mirror 23 applied to the photocell 56 is at least partially transparent to the wavelengths to be measured by the photocell 56.
- the photocell 56 can in turn be used for calibration purposes and / or for evaluating other properties of the luminescence radiation.
- the detector array 22 preferably asymmetrically on the support, that is applied to the silicon substrate 42.
- this can also be done by an active mechanical adjustment of the optical components of the luminescence sensor 12, the adjustment depending on measured values of the luminescence sensor 12 e.g. by an external control unit 11 or preferably by an internal control unit 50 can be controlled.
- the component of the imaging grating 24 can be displaceably mounted in the direction S.
- a mechanical adjustment of other optical components such. B. the detector 21 can be achieved, the z. B. in the direction of arrow D in Fig. 2 actively controlled can be displaced. It is also possible to perform an adjustment of the optical components in more than one direction.
- an evaluation of the measured values of the luminescence sensor 12 is carried out and in the presence of deviations of the measured values (eg the detector row 22, the further detector unit 27 or the photocell 33) or of quantities derived therefrom
- Reference values or areas an active mechanical adjustment of one or more of the optical components of the luminescence sensor 12 are performed to achieve increased signal efficiency and compensation of undesirable changes, for example due to caused by the lighting or electronics temperature fluctuations or aging phenomena of optical components. This is particularly important for a detector unit 21 with few pixels 40.
- the laser diode 14 is driven only with high power when a bill BN just in the field of the measuring window, d. H. of the front glass 18 is located
- a Plangitter can be used.
- the structure of such a luminescence sensor 12 is exemplary in the FIG. 10 illustrated.
- the radiation emitted by the banknote BN to be tested and detected by an entrance window 18 also falls in this case through a collimating lens 17 onto a beam splitter 16, from which the light is deflected by 90 °, via a lens 19 and a filter 20 for illumination suppression on a first spherical collimator mirror 70 falls. From this mirror 70, the radiation is deflected onto a screen grid 71.
- the spectrally dispersed light is then directed to a detector array 21 via a second spherical collimator mirror 72 and a cylindrical lens 73.
- the luminescence sensor 12 of FIG. 10 is further characterized in that the illumination light is coupled by means of a fiber optic coupling.
- the light generated by a laser light source 68 is irradiated via a light guide 69, a beam shaping optics 66, the beam splitter 16, the collimating lens 17 and the entrance window 18 on the bill to be tested. Since light guides 69 are flexible and deformable and thus the illumination beam path can (largely) run as desired, it is only possible, for example, to fasten the light source in a particularly space-saving location in the housing 13.
- FIG. 11 shows an associated schematic example in which a light source 68 radiates into a light guide 69, which leads into the housing 13 of a luminescence sensor 12.
- the housing 13 may be constructed as an example of how the FIG. 10 with the only difference that the light source 68 is thus outside of the housing 13 and the light guide 69 thus also extends outside of the housing 13.
- FIG. 11 Another special feature of the light coupling, for example FIG. 11 it is that the light source 69 and the housing 13 connecting optical fiber 69 in a in the FIG. 11 schematically shown in a cross-sectional view middle portion 70 is spirally wound.
- the light source 68 radiates into the light guide 69, a series of total reflections occurs in the light guide 69.
- the beam cross section of the coupled-in laser radiation of the light source 68 is spatially homogenized.
- the optical fiber does not necessarily have to be spirally wound in a plane for this purpose. Rather, it is only important that the light guide has a certain length
- the light guide 69 is preferably at a fiber cross section of 50 microns to 200 microns have a length of 1 m to 20 m.
- the irradiation of the banknote to be checked exclusively via outside of the housing 13 existing Components takes place and the luminescence sensor 12 inside the housing 13 includes only the optical components, which are used for the measurement of emanating from the illuminated banknote radiation.
- a grating spectrometer i. a spectrometer 30 with imaging grating 24
- a grating spectrometer 30 with prism for spectral dispersion can be used or a measurement with the aid of different filters for filtering out different wavelengths to be detected or wavelength ranges of the luminescence radiation can be carried out. This can be used in particular for a multi-track or a high-sensitivity measurement.
- FIG. 12 An example of a luminescence sensor 1 without a grating spectrometer is shown in FIG. 12 illustrated.
- FIG. 12 shows in a schematic way only the detection part of a luminescence sensor. All other components such as the housing, the lighting and the imaging optics are omitted for the sake of clarity.
- the outgoing from the banknote to be tested BN beam is deflected via a pivotable about a rotation axis 58 deflecting mirror 57 selectively to individual detectors 59, which are sensitive to different wavelengths or wavelength ranges. This can be done by the choice of photosensitive in different wavelength ranges Detector surfaces of the detectors 59 take place.
- filters 60 for different wavelength ranges upstream of the detectors 59 and preferably also be attached to these themselves.
- a detector 61 is depicted in a very schematic manner according to yet another example.
- the detector has a row or an array of similar photosensitive pixels 63 on a substrate 62.
- a filter 64 is mounted above the pixels 63, which has a direction indicated by the arrow gradient of the filter wavelength. This means that as seen in the direction of the arrow at different points of the filter 64 different wavelengths are filtered out.
- the use of such a filter with wavelength gradients filter 64 has the advantage that the light to be tested are irradiated directly to the detector 61 and on wavelength dispersing elements such as the grating 24 or the deflecting mirrors 23, 57 can be omitted.
- the structure of the luminescence sensor 1 can thereby be designed particularly simple and with fewer components.
- the active optical adjustment of individual components can be used not only in the particularly preferred example of a luminescence sensor, but also in other, in particular other optical sensors with advantage.
- the special design of the spectrometer is also advantageous if the luminescence sensor itself has no light source for exciting luminescent radiation
- the test can be carried out, for example, by generating a light having a first wavelength with a predetermined intensity by means of the light source 14 for a specific time period 0-t P for the excitation of the feature substance.
- the feature substance of the banknote BN to be checked and which has been transported past the front glass 18 in the direction T is excited, whereupon the feature substance emits luminescent light of a second wavelength.
- the intensity of the emitted luminescent light increases during the time period 0-t P of the excitation according to a certain law.
- the manner of increase and decrease in the intensity of the emitted luminescent light depends on the feature substance used and on the exciting light source 14, ie its intensity and wavelength or wavelength distribution. After completion of the excitation at time t P , the intensity of the emitted luminescent light decreases according to a certain law.
- the spectrometer 30 With the help of the spectrometer 30 is now the perpendicular, ie parallel to the excitation light, from the banknotes. BN outgoing luminescence detected and evaluated.
- evaluating the signal of the detector unit 21 at one or more specific times t 2 , t 3 it is possible to check particularly reliably whether a genuine banknote. BN is present, since only the feature substance used for the banknote BN or the combination of feature substances used has such a decay behavior.
- the verification of the decay behavior can take place by means of the above-described comparison of the intensity of the luminescence light at one or more specific times with given intensities for genuine banknotes BN. It can also be provided that the course of the intensity of the luminescence light is compared with predetermined progressions for known banknotes BN.
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- Health & Medical Sciences (AREA)
- General Health & Medical Sciences (AREA)
- Toxicology (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Inspection Of Paper Currency And Valuable Securities (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
- Apparatus For Radiation Diagnosis (AREA)
Claims (24)
- Dispositif (1) de contrôle de documents de valeur (BN) luminescents, comprenant une source de lumière (14, 51, 52, 68) destinée à une excitation de rayonnement luminescent et un capteur de luminescence (12) afin de saisir avec résolution spectrale le rayonnement luminescent émanant du document de valeur (BN),
caractérisé en ce que
le capteur de luminescence (12) comporte une ligne de détecteurs (22) comportant des pixels (49) réalisés directement sur un substrat en silicium (41, 42),
en ce que des pixels (40) individuels et/ou des groupes de pixels de la ligne de détecteurs (22) peuvent être lus parallèlement et
en ce que les pixels (40) individuels et/ou les groupes de pixels de la ligne de détecteurs (22) sont respectivement reliés avec un propre étage amplificateur qui fait partie du substrat en silicium (41, 42) et avec un convertisseur analogique/numérique situé après. - Dispositif (1) selon la revendication 1, caractérisé en ce que la source de lumière (14, 51, 52, 68) génère sur le document de valeur (BN) transporté dans une direction de transport (T) en passant par le capteur de luminescence (12) une surface d'éclairage (35) qui s'étend en direction du transport (T), et en ce que, de préférence, l'extension de la surface d'éclairage (35) en direction du transport (T) est au moins deux fois, de préférence au moins trois fois, quatre fois et particulièrement de préférence au moins cinq fois plus longue que l'extension perpendiculairement à la direction du transport (T).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce qu'une surface d'image (36) du capteur de luminescence (12) s'étend en direction du transport (T) du document de valeur (BN) transporté en passant par le capteur de luminescence (12).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que la longueur et/ou la largeur de la surface d'image (36) sont inférieures aux dimensions correspondantes de la surface d'éclairage (35) de la source de lumière (14, 51, 52, 68), et/ou en ce que, à un moment donné, la surface d'image (36) et surface d'éclairage (35) sur le document de valeur (BN) se chevauchent au moins partiellement ou complètement.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte une ou plusieurs sources de lumière (14, 51, 52, 68) qui émettent à différentes longueurs d'ondes, cependant que, de préférence, des longueurs d'ondes individuelles peuvent être activées de manière sélective.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte au moins une ligne de détecteurs (22) ayant un faible nombre de pixels (40), de préférence de 10 à 32 pixels (40), particulièrement de préférence de 10 à 20 pixels (40).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte au moins un élément de détecteur (40) afin de mesurer du rayonnement à l'extérieur du spectre de luminescence du document de valeur (BN).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte au moins une ligne de détecteurs (22) à pixels (40) de différentes dimensions, en particulier en direction de la dispersion du rayonnement luminescent de différentes dimensions à mesurer.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte une ligne de détecteurs InGaAs (22) en tant que ligne de détecteurs sur le substrat en silicium (42), le substrat en silicium (42) comportant un ou plusieurs étages amplificateurs (45) pour l'amplification des signaux de mesure analogiques de pixels (40) de la ligne de détecteurs InGaAs (22).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce qu'une unité de détecteur (21) du capteur de luminescence (6) saisit un domaine spectral inférieur à 500 nm, de préférence inférieur à ou environ égal à 300 nm, et/ou en ce que le réseau (24) formateur d'image du capteur de luminescence (6) comporte davantage qu'environ 300, de préférence davantage qu'environ 500 lignes/mm et/ou en ce que l'écart entre le réseau (24) formateur d'image et l'unité de détecteur (21) est inférieur à 70 mm, de préférence inférieur à 50 mm.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que la source de lumière (14) et/ou le capteur de luminescence (12) et/ou une unité de commande (50) sont, pour le traitement de signal des valeurs mesurées du capteur de luminescence (6) et/ou pour la commande de puissance de composantes du capteur de luminescence (6), intégrés dans un boîtier (13) commun ou dans des boîtiers (13, 68) séparés.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que la source de lumière (14) éclaire verticalement le document de valeur (BN) à contrôler et en ce que le capteur de luminescence (12) saisit le rayonnement luminescent émanant verticalement du document de valeur (BN) éclairé et/ou en ce que le rayonnement généré par la source de lumière (68) rayonne par l'intermédiaire d'un conduit de lumière (69) sur le document de valeur à contrôler, et/ou en ce que le capteur de luminescence (12) comporte un miroir de renvoi (23) pour le pliage du trajet de rayonnement du rayonnement luminescent à mesurer et/ou pour un renvoi du rayonnement luminescent à mesurer vers une autre unité optique telle qu'un équipement de décomposition spectrale (24).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte un photodétecteur (56) ayant un miroir de renvoi (23) qui se trouve sur ou au-dessus de sa surface et qui est au moins partiellement transparent pour les longueurs d'ondes devant être mesurées par le photodétecteur (56), et en ce que le capteur de luminescence (12) comporte de préférence un filtre (60, 64) qui, dans le trajet de rayonnement du rayonnement à mesurer, est disposé en amont du photodétecteur (56, 59, 63), en particulier un filtre (64) à gradients de longueurs d'ondes de filtrage.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte un composant (21) qui comporte tant une unité de détecteur (22) photosensible pour rayonnement luminescent que des composantes (23) pour la formation d'image du rayonnement luminescent sur l'unité de détecteur (22) photosensible.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte une ligne de détecteurs (22) qui est placée asymétriquement sur un substrat (42).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte plusieurs unités de détecteur (21, 27) pour la saisie de différentes propriétés du rayonnement luminescent qui, de préférence, mesurent dans différents domaines spectraux et/ou à différentes résolutions spectrales.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que les différentes unités de détecteur (21, 27) sont conçues pour le contrôle de différentes substances caractéristiques du document de valeur (BN).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce qu'une unité de détecteur (21) est conçue pour la mesure à résolution spectrale du rayonnement luminescent et en ce qu'une autre unité de détecteur (27) est conçue pour la mesure sans résolution spectrale du rayonnement luminescent.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce qu'une unité de détecteur (21) est conçue pour la mesure intégrée dans le temps du rayonnement luminescent, et une autre unité de détecteur (27) est conçue pour la mesure résolue dans le temps du rayonnement luminescent.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce qu'une unité de détecteur (27) est conçue pour la mesure de l'ordre zéro du rayonnement luminescent spectralement décomposé et une autre unité de détecteur (21) est conçue pour la mesure d'un autre ordre du rayonnement luminescent spectralement décomposé.
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce qu'une unité de détecteur (27) est agencée de manière basculée par rapport à un équipement (24) de décomposition spectrale afin d'éviter une rétroréflexion sur l'équipement (24).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte un échantillon de référence (32) ayant une substance caractéristique luminescente et de préférence une source supplémentaire de lumière (31) pour l'éclairage de l'échantillon de référence (32).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que le capteur de luminescence (12) comporte des moyens (25) de réglage mécanique actif de composants optiques (21, 24) du capteur de luminescence (12), et en ce que, de préférence, un réglage mécanique actif de composants optiques (21, 24) du capteur de luminescence (12) est commandable par une unité de commande (11, 50) en fonction de valeurs mesurées du capteur de luminescence (12).
- Dispositif (1) selon au moins une des revendications précédentes, caractérisé en ce que les valeurs mesurées du capteur de luminescence (12) relatives à un document de valeur (BN) sont encore évaluées pendant que, en même temps, déjà des valeurs mesurées d'un document de valeur (BN) suivant sont enregistrées.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102004035494A DE102004035494A1 (de) | 2004-07-22 | 2004-07-22 | Vorrichtung und Verfahren zur Prüfung von Wertdokumenten |
EP05770995A EP1784795A1 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procede de verification de documents de valeur |
Related Parent Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP05770995.8 Division | 2005-07-19 | ||
EP05770995A Division EP1784795A1 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procede de verification de documents de valeur |
Publications (3)
Publication Number | Publication Date |
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EP2275998A2 EP2275998A2 (fr) | 2011-01-19 |
EP2275998A3 EP2275998A3 (fr) | 2012-01-25 |
EP2275998B1 true EP2275998B1 (fr) | 2016-09-07 |
Family
ID=35094077
Family Applications (6)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP10011626A Ceased EP2278557A3 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
EP10011627.6A Active EP2278558B1 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
EP10011628A Ceased EP2282298A3 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
EP10011629.2A Active EP2275998B1 (fr) | 2004-07-22 | 2005-07-19 | Dispositif de verification de documents de valeur |
EP10011625A Ceased EP2278556A3 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
EP05770995A Ceased EP1784795A1 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procede de verification de documents de valeur |
Family Applications Before (3)
Application Number | Title | Priority Date | Filing Date |
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EP10011626A Ceased EP2278557A3 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
EP10011627.6A Active EP2278558B1 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
EP10011628A Ceased EP2282298A3 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
Family Applications After (2)
Application Number | Title | Priority Date | Filing Date |
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EP10011625A Ceased EP2278556A3 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procédé de vérification de documents de valeur |
EP05770995A Ceased EP1784795A1 (fr) | 2004-07-22 | 2005-07-19 | Dispositif et procede de verification de documents de valeur |
Country Status (11)
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US (1) | US7737417B2 (fr) |
EP (6) | EP2278557A3 (fr) |
JP (1) | JP4919355B2 (fr) |
KR (4) | KR101277932B1 (fr) |
CN (2) | CN102169607B (fr) |
AU (2) | AU2005266522B2 (fr) |
DE (1) | DE102004035494A1 (fr) |
ES (2) | ES2923700T3 (fr) |
IL (1) | IL180847A (fr) |
RU (4) | RU2375751C2 (fr) |
WO (1) | WO2006010537A1 (fr) |
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DE102006045626A1 (de) * | 2006-09-27 | 2008-04-03 | Giesecke & Devrient Gmbh | Vorrichtung und Verfahren zur optischen Untersuchung von Wertdokumenten |
RU2358882C1 (ru) | 2008-04-18 | 2009-06-20 | Общество С Ограниченной Ответственностью "Новые Энергетические Технологии" | Устройство проверки подлинности документов |
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DE102008028689A1 (de) * | 2008-06-17 | 2009-12-24 | Giesecke & Devrient Gmbh | Sensoreinrichtung zur spektral aufgelösten Erfassung von Wertdokumenten und ein diese betreffendes Verfahren |
KR100882396B1 (ko) * | 2008-10-01 | 2009-02-05 | 한국조폐공사 | 진위 식별기 |
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2004
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2005
- 2005-07-19 JP JP2007521891A patent/JP4919355B2/ja active Active
- 2005-07-19 US US11/658,005 patent/US7737417B2/en active Active
- 2005-07-19 EP EP10011626A patent/EP2278557A3/fr not_active Ceased
- 2005-07-19 EP EP10011627.6A patent/EP2278558B1/fr active Active
- 2005-07-19 AU AU2005266522A patent/AU2005266522B2/en active Active
- 2005-07-19 KR KR1020117030777A patent/KR101277932B1/ko active IP Right Grant
- 2005-07-19 ES ES10011627T patent/ES2923700T3/es active Active
- 2005-07-19 EP EP10011628A patent/EP2282298A3/fr not_active Ceased
- 2005-07-19 EP EP10011629.2A patent/EP2275998B1/fr active Active
- 2005-07-19 ES ES10011629.2T patent/ES2598357T3/es active Active
- 2005-07-19 CN CN2011100236010A patent/CN102169607B/zh active Active
- 2005-07-19 WO PCT/EP2005/007872 patent/WO2006010537A1/fr active Application Filing
- 2005-07-19 KR KR1020077003654A patent/KR101224255B1/ko active IP Right Grant
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- 2005-07-19 EP EP10011625A patent/EP2278556A3/fr not_active Ceased
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- 2011-05-11 RU RU2011118715/08A patent/RU2451339C1/ru active
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