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    • 专利摘要:
    The invention relates to a gas sensor (20) comprising - a substrate (231); an objective (211) located on the substrate (231), adapted to collect a light beam (212, 213) emitted by a light source (210); an eyepiece (250) located on the substrate (231) adapted to collect an incident light beam for focusing on a detector (251); return reflective surfaces (281, 282) facing said substrate; and at least one field lens (221) disposed on an intermediate reflecting surface (222) formed on the substrate (231), and adapted to deflect beams (213) from the light beam emitted by the light source, to bring them closer together the optical axis of the eyepiece (250);
    公开号:FR3016213A1
    申请号:FR1450048
    申请日:2014-01-06
    公开日:2015-07-10
    发明作者:Luc Andre
    申请人:Commissariat a lEnergie Atomique CEA；Commissariat a lEnergie Atomique et aux Energies Alternatives CEA；
    IPC主号:
    专利说明:

    [0001] TECHNICAL FIELD The present invention relates to the field of gas sensors, in particular the field of gas sensors using the absorption of infrared radiation. STATE OF THE PRIOR ART In the prior art, gas sensors using the so-called NDIR technique are known for "Non Dispersive Infra Red". According to this technique, an infrared light beam (wavelength between 1 μm and 10 μm) is emitted inside a cavity receiving a gas to be detected. The light beam is partially absorbed by said gas. The wavelength of absorption depends on the nature of the gas. A light source emitting a light beam is generally used at the absorption wavelength of the gas to be detected. Alternatively, a wavelength filter is used to eliminate spectral contributions that do not belong to a spectral band of interest centered on the wavelength of absorption. A detector makes it possible to measure the light intensity at the absorption wavelength, after partial absorption by said gas. It is thus possible to detect the presence of a specific gas, and even its concentration in the cavity using BeerLambert's law. It is recalled that for a predetermined gas having an absorption wavelength, the Beer-Lambert law relates: - the light intensity to the wavelength of absorption before partial absorption by said gas (1c); the luminous intensity at the absorption wavelength after partial absorption by said gas (I); the length of the optical path traveled in the gaseous medium (eg); the concentration of gas in the medium (C); and the molar absorptivity of said gas (E): ## EQU1 ## In these known gas sensors, the light source may be a light-emitting diode, emitting a beam centered on the desired absorption wavelength. One can also use a filament acting as a black body. In this case, a filter as defined above is advantageously used, as well as a collimation optics. FIG. 1 shows an example of a gas sensor 10 according to the prior art. The light source 11 is formed by a filament, and emits a light beam 12 in the direction of collimation optics 13. A filter 14 eliminates the spectral contributions of the light beam 12 lying outside an associated useful spectral band gas to be detected. Near the detector 16 is a focusing optics 15, adapted to focus the light beam on said detector. The detector 16 makes it possible to translate the light intensity of the incident light beam into an electrical signal. The whole is located inside a cavity 17 receiving said gas to be detected. For a given gas, it is possible to define a minimum length of the optical path traveled by the light beam in the cavity, making it possible to obtain a sufficiently accurate measurement of the gas concentration. Various solutions are known in the prior art for producing a miniaturized gas sensor. For example, US patent document 2003/0136911 proposes to use a cavity whose walls are formed by two parallel flat surfaces connected by a lateral surface orthogonal to the two parallel flat surfaces. Parallel plane surfaces have a truncated ellipse shape. Two lines start from the truncated ends of the ellipse and converge towards the detector. The light source is placed in a first focus of the ellipse, while the detector is placed at the second focus of the ellipse. The light rays emitted by the light source are reflected at least once on the lateral surface of the cavity, before reaching the detector. They thus travel an optical path greater than the distance separating the light source and the detector. A disadvantage of such a cavity is that it must be aligned very precisely with respect to the light source and the detector. In addition, it offers relatively small miniaturization possibilities because most of the light rays only reflect on the lateral surface before reaching the detector. An object of the present invention is to provide a gas sensor having a higher compactness than gas sensors of the prior art, for the same optical path length traversed by a light beam inside the cavity receiving the gas to study. DISCLOSURE OF THE INVENTION This object is achieved with a gas sensor comprising a cavity for receiving a gas, a light source and a detector.
    [0002] The gas sensor according to the invention comprises: a substrate; an objective located on the substrate, adapted to collect a light beam emitted by the light source; an ocular located on the substrate adapted to collect an incident light beam to focus on the detector; so-called return reflective surfaces located opposite said substrate; and at least one relay lens, disposed on a so-called intermediate reflecting surface formed on the substrate, and comprising at least one field lens adapted to deflect rays of the light beam emitted by the light source, to bring them closer to the optical axis of the eyepiece.
    [0003] According to the invention, the objective, the eyepiece, the relay lens, the intermediate reflective surface, and the return reflective surfaces together form an optical system arranged so that the light beam emitted by the light source propagates by reflections. successive lenses from the lens to the eyepiece through the relay lens. The substrate is advantageously a substrate of transparent semiconductor material at an emission wavelength of the light source. Alternatively, the substrate is metal. Preferably, the light source and the detector are disposed on a first face of the substrate, opposite to a second face of the substrate on which the lens, the eyepiece, and the relay lens are arranged. The field lens may be a concave plane lens, a planar face of the field lens being disposed on the intermediate reflective surface and an intermediate focus of the optical system.
    [0004] The relay lens preferably comprises at least one intermediate lens interposed between two field lenses, so that the light beam emitted by the light source is propagated by successive reflections from the lens to the eyepiece through the field lenses. and the intermediate lens.
    [0005] At least one optical element among the relay lens, the lens, and the eyepiece can be of high density polyethylene. At least one optical element among the relay lens, the lens, and the eyepiece may consist of a subwavelength lens.
    [0006] Preferably, the gas sensor according to the invention is such that: the light source comprises a plurality of elementary sources; the objective comprises a plurality of elementary objectives, each adapted to collect a light beam emitted by an elementary source; the eyepiece comprises a plurality of elementary eyepieces each adapted to collect an incident light beam to focus on the detector; and the relay lens comprises a plurality of elementary relay lenses.
    [0007] The light source may comprise a plurality of elementary sources aligned on the same line. Alternatively, the light source may comprise a plurality of elementary sources distributed on either side of the detector and aligned along two parallel lines. According to another variant, the light source comprises a plurality of elementary sources distributed over a circle centered on the detector. At least one of the reflective return surfaces is advantageously inclined relative to the plane of the detector, so that light beams emitted by the elementary sources are focused at one and the same point on the detector. The gas sensor according to the invention may comprise a gas pre-concentrator disposed on a return reflective surface. The gas sensor according to the invention advantageously comprises a cover receiving the return reflective surface and the gas pre-concentrator, the cap being made removable relative to the substrate.
    [0008] Preferably, the light source is made according to MEMS technology. This is for example a microelectronic infrared source, comprising a resistive membrane forming a thermal emitter. The detector is advantageously made according to MEMS technology. This is for example a microelectronic bolometer, comprising an absorbent membrane forming a thermal absorbent. The invention also relates to an alcohol meter comprising a gas sensor according to the invention adapted to receive a gas exhaled by a user.
    [0009] BRIEF DESCRIPTION OF THE DRAWINGS The present invention will be better understood on reading the description of exemplary embodiments given purely by way of indication and in no way limiting, with reference to the appended drawings in which: FIG. 1 schematically illustrates a sensor of FIG. gas according to the prior art; FIG. 2 illustrates a first embodiment of a gas sensor according to the invention; FIG. 3A schematically illustrates a second embodiment of a gas sensor according to the invention; FIG. 3B schematically illustrates the "unfolded" equivalent of the gas sensor of FIG. 3A; FIGS. 4A to 4D schematically illustrate several variants of a third embodiment of a gas sensor according to the invention; FIG. 5 illustrates a fourth embodiment of a gas sensor according to the invention; FIG. 6 illustrates a sixth embodiment of a gas sensor according to the invention; FIG. 7 illustrates a network that can be a sub-wavelength lens used in a gas sensor according to the invention; and Figures 8A and 8B illustrate a detail view of a gas sensor according to the invention in which at least one refractive optic is formed by a subwavelength lens. DETAILED DESCRIPTION OF PARTICULAR EMBODIMENTS A first embodiment of a gas sensor 20 according to the invention will first be described with reference to FIG.
    [0010] The gas sensor 20 according to the invention comprises a cavity 270 for receiving a predetermined gas. This gas may be carbon dioxide, carbon monoxide, a gas for domestic use such as methane, ethane, propane, butane, ammonia. The gas sensor can also be used for the measurement of ethanol in an alcohol meter.
    [0011] A light source 210 emits a light beam in the infrared. A detector 251 receives this light beam after a path in the cavity 270 in which the light beam is partially absorbed by the gas present inside the cavity 270. The cavity comprises two opposite inner faces 230 and 280. typically a cylindrical shape or rectangular parallelepiped, whose faces 230 and 280 form the two bases. On the side of the inner face 230 is a substrate 231, for example of semiconductor material. The substrate 231 is for example derived from a silicon wafer having a thickness of 725 μm. It is transparent to the absorption wavelength of the gas to be detected. On this substrate 231 are arranged the following optical elements (it is refractive optics): an objective 211, adapted to collect a light beam emitted by the light source 210; an eyepiece 250 adapted to focus an incident beam on the detector 251; and a relay lens 221. The light source 210 and the detector 251 are located on the side of the substrate opposite to the refractive optics. The relay lens is disposed on an intermediate reflective surface 222. This intermediate reflecting surface is advantageously located between the substrate 231 and the relay lens 221. On the inside face 280 side there are reflective return surfaces 281, 282. This is for example flat mirrors. Thus, a light beam: is emitted by the light source 210; crosses the lens 211; crosses the cavity 270 a first time; is reflected on the return reflective surface 281; crosses the cavity 270 a second time; crosses the relay lens 221; is reflected on the intermediate reflecting surface 222; crosses the relay lens 221 a second time; crosses the cavity 270 a third time; is reflected on the return reflective surface 282; crosses the cavity 270 a fourth time; crosses the eyepiece 250 which focuses it on the detector 251. In other words, the lens 211, the reflective return surfaces 281, 282, the relay lens 221, the intermediate reflecting surface 222 and the eyepiece 250 form together an optical system arranged so that the light beam emitted by the light source propagates by successive reflections from the lens 211 to the eyepiece 250 through the relay lens 221. The lens 211, the relay lens 221 and the eyepiece 250 together form a lentoscope endoscope, folded thanks to the reflective return and intermediate surfaces. In the example of Figure 1, the relay lens is a convergent plane-concave lens crossed twice: it is equivalent to a biconcave lens. The intermediate reflective surface 222 is located on the plane side of the relay lens 221.
    [0012] The relay lens 221 is more particularly a field lens. It is located in an intermediate focus of the optical system as defined above. In particular, the flat face of the relay lens is located in an intermediate focus of said optical system. This configuration is therefore equivalent to a field lens in a lens endoscope, in the center of which is located an intermediate focus of the endoscope. The field lens 221 makes it possible to reduce light rays located at the edge of the field towards the optical axis of the eyepiece. FIG. 2 shows a beam 212 centered on the optical axis of the eyepiece (coinciding with the optical axis of the objective and the relay lens), and a beam 213 moving away from this optical axis. The beam 212 is shown in solid line, while the beam 213 is shown in phantom. The beam 212 is focused on the flat face of the field lens 221, in the center of this face. The beam 213 is focused on the periphery of this plane face. After crossing this field lens, the beam 212 is not deviated from the optical axis of the eyepiece, because it passes through the center of the biconcave lens equivalent to the field lens. The beam 213, on the contrary, is deflected in the direction of the optical axis of the eyepiece, so that the beams 212 and 213 are focused by the eyepiece 250 at the same point of the detector 251. The field lens allows that the total width of the light beam propagating from the light source to the detector remains limited. It is thus possible to use refractive optics, in particular an eyepiece, which have a reduced diameter. It can thus be seen that a gas sensor with reduced dimensions can be produced in this way while offering a large optical path length inside the cavity. The field sensor has a reduced depth P, thanks to the reflective return and intermediate surfaces which fold the optical path of the light beam emitted by the light source 210. The gas sensor has a reduced height H, thanks to the field lens 221 which limits the spatial widening of the light beam during its propagation. Similarly, the width (not shown) of the field sensor is limited by the field lens 221 which limits the spatial widening of the light beam during its propagation. In addition, the alignment constraints are less severe than if the light source and the detector were to be placed at the centers of an ellipse. It is further noted that all the refractive optics (objective, ocular, relay lens) are made on the same surface, in particular on the same substrate. The source and the detector are located on the side of this substrate opposite the refractive optics. The realization of a gas sensor according to the invention is therefore simplified since all the useful elements of the sensor is located on the substrate. One can even consider making several gas sensors according to the invention from the same substrate plate, then cut the plate after fixing sources, detectors and refractive optics. The focal lengths of the objective, the eyepiece and the relay lens, as well as the distances between these refractive optics will be chosen by those skilled in the art as a function of the desired dimensions of the gas sensor. For example, known optical systems forming a lens endoscope may be adapted. For this purpose, mirrors are interposed between the lenses of the endoscope, and the characteristics of the lenses are adjusted to take into account the double crossing of the relay lens in a gas sensor according to the invention. For example, a biconcave relay lens of radius R1-R1 belonging to a lens endoscope will be equivalent, in the optical system according to the invention, to a plane-concave lens of radius R1.
    [0013] On the same model as the endoscopes with lenses, it will be possible to provide as many relay lenses as necessary, in particular according to a desired depth P of the cavity 270 and a desired optical path length for the light beam propagating from the light source 210 to the detector 251. As illustrated with reference to Figures 3A and 3B, all intermediate lenses are not field lenses. For example, it is desired to obtain an optical path length of 8 cm, to measure a concentration of carbon dioxide. It is desired to obtain a depth P of the cavity equal to 1 cm, ie four trips back and forth inside the cavity.
    [0014] FIG. 3A shows schematically a second embodiment of a gas sensor 30 according to the invention. In this embodiment of the gas sensor 30 according to the invention, the light beam 312 performs four trips back and forth within the cavity, between the substrate 231 and a face 383 receiving return reflective surfaces.
    [0015] The light beam 312 passes successively through the objective 211, a first relay lens 321 formed by a field lens as described above, a second relay lens 322, a third relay lens 321 formed by a field lens, and the eyepiece 250. All relay lenses are located on an intermediate reflecting surface (not shown).
    [0016] The second relay lens 322 is an intermediate lens, sandwiched between two field lenses. FIG. 3B shows the "unfolded" equivalent of the optical system of FIG. 3A. It is recognized that the field lenses 321 are each located in an intermediate focus of the optical system. Between these two field lenses is the intermediate lens 322 which helps to position the intermediate foci on the field lenses. FIGS. 4A to 4D schematically illustrate several variants of a third embodiment of a gas sensor according to the invention. FIGS. 4A to 4D correspond to front views of the substrate 231 receiving the refractive optics. Figures 4A-4D correspond to a gas sensor comprising an objective, a first field lens, an intermediate lens, a second field lens, and an eyepiece.
    [0017] In the third embodiment of the gas sensor according to the invention, the light source is produced using technologies derived from microelectronics. Such a light source generally provides reduced optical power, which is why a plurality of elementary sources are advantageously used to form the light source of the gas sensor. The elementary sources are located in the same plane. By thus increasing the emission surface of a light beam, a desired optical power is obtained. In a first variant of the third embodiment of a gas sensor according to the invention, the objective, the eyepiece, and the relay lenses (field lenses and intermediate lens) are also decomposed into elementary lenses. A plurality of elementary optical systems each associated with an elementary source is thus produced. This first variant is illustrated in FIG. 4A. The light source (not shown) consists of a plurality of elementary sources aligned along the same straight line 41. Each elementary optical system comprises an elementary lens 211, a first elementary field lens 321, an elementary intermediate lens 322, a second elementary field lens 321, and an elemental eyepiece 250 ,. There are N elementary optical systems distributed on a substrate 231 of height H1 and width L1. For example, the substrate has a height H1 of 12 mm, a width L1 of 12 mm, and receives 10 elementary optical systems. The detector may have a bar shape. FIG. 4B illustrates a second variant of the third embodiment of a gas sensor according to the invention. Figure 4B will only be described for its differences with respect to Figure 4A. The plane of the substrate 231 is defined by the orthogonal axes x and y. In FIG. 4B, the elementary optical systems share a single eyepiece 250. Such a characteristic is made possible by the inclination of the return reflective surfaces (not shown in FIGS. 4A to 4D). In particular, an elementary light beam emitted by an elementary source is reflected between the second field lens 321 and the eyepiece 250 on a dedicated reflecting surface. For each elementary light beam (except for any elementary light beam naturally directed on the eyepiece 250), said dedicated reflective surface is inclined about the y-axis so as to deflect the elementary light beam along the x-axis, in the direction of the eyepiece 250. It may be noted that said dedicated reflecting surface can also be inclined around the x axis, in order to deflect the elementary light beam along the y axis, towards the eyepiece 250. It can be seen that the various Elemental beams emitted by each of the elementary sources traverse different optical paths. This factor can be used to calculate the gas concentration. For example, we can determine an average optical path length. Those skilled in the art will easily provide other variants according to this model, without departing from the scope of the present invention. For example, it may be provided to gradually deflect the light beams to a single eyepiece, as and when they spread. For this, we will also use an inclination around the y-axis, reflecting surfaces back. The number of elementary relay lenses can thus be decreasing, considered in the order in which they are traversed by the elementary light beams. It will also be possible to focus the elementary light beams on several oculars, fewer than the elementary sources.
    [0018] An advantage of these variants is that they make it possible to use a reduced surface detector, thus having a good signal-to-noise ratio. FIG. 4C illustrates a third variant of the third embodiment of a gas sensor according to the invention. Figure 4C will only be described for its differences with respect to Figure 4A. In the embodiment of FIG. 4C, the elementary sources are aligned along two lines. A first group of elementary objectives 211A is aligned along a straight line 41A. A second group of elementary goals 2118; is aligned along a line 41B. The straight lines 41A and 41B are parallel to each other and located on either side of the detector located at a height of a row of elementary eyepieces 250,. On one side of this row of elementary oculars 250 are successive rows of first elementary field lenses 321A ,, elementary intermediate lenses 322A ,, and second elementary field lenses 321A ,. We find the configuration of Figure 4A. On the other side of the row of elementary oculars 250 are other successive rows of first elementary field lenses 321B ,, elementary intermediate lenses 322B ,, and second elementary field lenses 321B ,. It can thus be seen that for the same number of elementary sources, this variant makes it possible to distribute the bulk of the refractive optics on the substrate in the direction of its height H2, and not only in the direction of its width L2.
    [0019] FIG. 4D illustrates a fourth variant corresponding to elementary sources distributed in a circle 45 centered on a point detector. The elementary objectives 211 ,, and elementary relay lenses 321 ,, 322 are distributed in concentric circles around a single eyepiece 250. It is thus possible to use a reduced surface detector having a good signal-to-noise ratio. Many additional variants of distribution of the elementary sources relative to the detector can be envisaged, without departing from the scope of the present invention. For example, the distribution of the optical elements on the substrate will be a function of the distribution of the elementary sources relative to the detector. It will also be possible to envisage many variants implementing a light source or a plurality of elementary light sources, and a detector or a plurality of elementary detectors, without departing from the scope of the present invention. FIG. 5 illustrates a fourth embodiment of a gas sensor 50 according to the invention. Figure 5 will only be described for its differences with respect to Figure 2.
    [0020] FIG. 5 shows an opening 51 for the entry of the gas to be detected inside the cavity 270. This opening here has a disc shape with a diameter of 1 cm. Alternatively, the gas enters through a plurality of smaller openings, or by at least two apertures facing each other, on either side of the cavity 270.
    [0021] The light source consists of a plurality of elementary light sources 210, each associated with an elementary lens 211, an elementary relay lens 221, and an elementary eyepiece 250. In a similar manner to the embodiment of FIG. 4A, the elementary light sources are aligned with each other. The gas sensor 50 is shown in a sectional view in the plane (yOz), orthogonal to a line in which the elementary light sources are aligned. FIG. 5 shows the elementary beams 212 and 213 respectively corresponding to the beams 212 and 213 of FIG. 2.
    [0022] The mirror 281 is a plane mirror inclined at an angle of -3.5 ° around the x axis (axis orthogonal to the plane (yOx)). The mirror 282 is a plane mirror inclined at an angle of + 3.5 ° around the x axis. In a variant in which the gas sensor comprises more than one relay lens, for example three, it can be provided that the other return reflective surfaces are flat and parallel to the plane (xOy). We can provide separate plan mirrors for each elementary optical system. Between the elementary source 210, and the objective 211, there is an elementary optical filter 52, as shown above, for selecting a range of 10 useful wavelengths for a predetermined gas concentration measurement. In the example shown in FIG. 5, the elementary optical filter 52 is made on the substrate 231. In FIG. 5, the elementary optical filter 52 is superimposed on the elementary objective 211. Alternatively, it may be superimposed on the elementary eyepiece 250, or superimposed on the elementary relay lens 221, or a combination of these several possibilities. The substrate 231 is thus maximally functionalized, which facilitates the manufacture of the gas sensor according to the invention. The transfer function of the filter (high pass, low pass, pass band) will be different depending on its position. Substrate 231 is covered with a layer of reflective material 53 except for elementary light sources 210 and elementary detectors 251. This layer of reflective material 53 forms an intermediate reflecting surface as defined with reference to FIG. 2. It also makes it possible to prevent the arrival of stray light on the detector. The main steps of producing a gas sensor as shown in FIG. 5 will now be described. The substrate 231, for example made of semiconductor material, comes from a silicon wafer with a thickness of 725 μm. It is therefore transparent to the wavelengths of interest.
    [0023] On this substrate, a layer of reflective material is deposited, for example a metal such as gold or aluminum. Other materials such as silver or copper may also be considered. Holes of about 1 mm in diameter are etched in the layer of reflective material, so as to open the reflective material layer 53 with respect to the elementary light sources 210, and the elementary detectors 251,. This etching is preferably carried out following a photolithography step which makes it possible to define the zones in which to make the opening of the reflective material. Engraving itself may be wet or dry depending on the material. Photolithography includes, for example, steps for depositing a photoresist, superimposing a mask, and etching the resin with exposure to ultraviolet radiation. The etching itself is for example a chemical etching of the layer 53 through the etched resin.
    [0024] A substrate 231 covered with a layer of perforated reflecting material 53 is obtained. Alternatively, the substrate 231 is a non-transparent material at the wavelengths of interest, and perforated with respect to the light source and the detector. This is for example a metal. This metal may be reflective, so that the intermediate reflecting surface receiving the relay lens according to the invention is formed by a face of the substrate. On the layer of perforated reflective material 53, a deposit is produced for forming the elementary optical filters 52,. The elementary optical filter 52 may be formed of a metal-dielectric multilayer stack or of a high index-low index dielectric multilayer stack. For example, an elementary optical filter 52 is formed by a metal-dielectric stack of 5 layers, or by a high index-low index dielectric stack of 12 layers. The deposit is then etched. It is preserved only in the openings of the reflective material layer 53 intended to be placed facing an elementary source. As a variant, it is preserved only in the openings of the reflective material layer 53 intended to be placed facing an elementary detector or an elementary relay lens, or in several of these types of opening (see FIG. above).
    [0025] Elementary objectives 211, elementary relay lenses 221 and elementary eyepieces 250 are then produced. Advantageously, these different refractive optics are produced in the following manner: a nickel mold called "master" is engraved, according to the complementary shape of a shape desired for an optical element; a useful material is poured into the mold. The useful material is, for example, HDPE (high density polyethylene). It will in any case be a sufficiently transparent material in the spectral range referred to, and that can be printed. Its glass transition temperature Tg should be such that by heating it, it can be softened sufficiently to then be able to give it the desired shape. ; the useful material such as HDPE is heated so that it softens and takes the shape of the mold; after the useful material has cooled, the mold is placed at the desired location, against the layer of reflective material 53, or against an elementary optical filter. The useful material adheres to the reflective material layer 53 or the elementary optical filter, and forms an elementary lens 211, an elementary relay lens 221, or an elementary eyepiece 250.
    [0026] Advantageously, all of the elementary objectives 211, elementary relay lenses 221, and elementary eyepieces 250 are produced at the same time, using a single nickel plate. Thus, the different refractive optics are produced at the same time, according to a collective manufacturing process. An advantage of the invention is therefore that the manufacture can be carried out at low cost and on a large scale.
    [0027] For example, the elementary lens 211 is an aspherical lens having a diameter of 700 μm and a height of 200 μm, and the elementary eyepiece 250 is an aspheric lens having a diameter of 2 mm. The relay lens has a diameter at most equal to 2 mm. The aspheric shape of the optics makes it possible to maintain a dense light beam. The objective and the eyepiece must be very open optics, to collect a maximum of luminous flux. Each elementary source 210 is advantageously an elementary infrared source based on a microelectromechanical type (or MEMS) technology. The elementary source 210 comprises a resistive membrane 510, forming a thermal emitter. This membrane is called resistive because it is traversed by metal tracks, arranged in concentric circles. By supplying a current to the resistive membrane 510, it heats up and forms a source of infrared radiation. The resistive membrane 510 is suspended above a crucible 515, made of silicon, and protected by a cap 516, transparent to infrared wavelengths. The cap may be formed of a 725 μm thick silicon substrate sample having a 300 μm deep recess. The cavity formed between the crucible 515, and the cap 516, may have particular pressure conditions. For example, a partial vacuum is achieved between the crucible 515 and the cap 516. The resistive membrane 510 is, for example, a silicon nitride membrane (Si3N4) 100 nm thick and 150 μm in diameter. The skilled person will easily find in the literature all the details necessary for the realization of such an elementary source. The term "source micro-hotplate" is used more frequently to designate such a source. The term "micro filament" can also be used. In the same way, each elementary detector 251 is advantageously an infrared bolometer based on MEMS type technology. The elementary detector 251 comprises a membrane 551, which absorbs heat. Infrared radiation incident on the membrane 551 warms the latter. The heat absorbed by the membrane 551 is converted into an electrical signal, which makes it possible to quantify the light intensity of the incident infrared radiation. The membrane 551 is, for example, a vanadium oxide membrane having a square surface area of 28 μm and a thickness of 1. It can be overcome by a precise stack of additional layers, for example a stack of Si (300 nm), YSZ (40 nm), CeO 2 (10 nm), GBCO (50 nm) and PtOx (200 nm). Those skilled in the art will easily find in the literature all the details necessary for the realization of such an elementary detector. In a variant, each elementary detector 251 may be a thermopile or a pyrometer, also produced using MEMS technology. The elementary sources 210, and the elementary detectors 251, are then deposited and glued in the same plane, on the substrate 231, and on the opposite side to the refractive optics. The repository uses a so-called "pick and place" technique. The assembly is then glued on a printed circuit board 54. The printed circuit board 54 is in particular a PCB (for the English "Printed Board Circuit"), and more particularly an ASIC (for English "Application-Specific Integrated Circuit "). Each elementary source 210 is electrically powered by a connection wire 55 ,, and each elementary detector 251 is connected to the printed circuit 54 by a connection wire 56. The wiring using the connection son 55, and 56, can be achieved by a technique called "wire bonding". In particular, the wiring can be achieved by a so-called "lease bonding" connection. Alternatively, the wiring can be achieved by a connection called TSV (for English "Through Silicon Vias"). A housing, open on one of its faces, is then bonded to the printed circuit 54 to form, between the inside of this housing and the printed circuit 54, the cavity 270 of the gas sensor according to the invention. Reflective return surfaces are made inside the housing. The reflective surfaces of return are flat mirrors, that is why the gluing of the case does not require precise alignment. Various variants can be envisaged for producing the reflective return surfaces, without departing from the scope of the present invention.
    [0028] For example, the bottom of the housing can receive a single plane mirror, or several separate mirrors possibly inclined differently relative to each other, or a single structured mirror so as to form several reflective surfaces inclined differently relative to each other. FIG. 6 illustrates a sixth embodiment of a gas sensor 60 according to the invention. The gas sensor 60 will only be described for its differences with respect to the gas sensor 50 of FIG. 5. The gas sensor 60 comprises an optical filter 61 arranged on the optical path of the light beam, at the output of the elementary objective 211 ,. It replaces the elementary optical filters 52, as described with reference to FIG. 5. An advantage is that the optical filter 61 is then disposed where the light beam is at near-normal incidence, which improves its efficiency. The optical filter 61 has for example an area of 2 × 10 mm 2: it extends at the output of all the elementary objectives 211,. The optical filter 61 is held by a support 62. In a variant, it is conceivable to place the optical filter 61 on a reflective surface of return or under a relay lens. The alignment of the optical filter relative to the other elements of the gas sensor 60 does not need to be accurate, so it can be done by hand.
    [0029] The gas sensor 60 further comprises a gas pre-concentrator 63, also called "gas absorber". A pre-concentrator is a device which will concentrate a large quantity of the gas present in the cavity 270 therein. Thus, by placing a pre-concentrator on the optical path of the light beam inside the cavity 270, it is possible to ensures that said light beam crosses a maximum of the molecules of said gas present in the cavity. The light beam inside the cavity passes through the pre-concentrator 63, is reflected on the return reflective surface 281, then crosses again the preconcentrator 63. The absorption by the gas is therefore maximum. In other words, a preconcentrator allows the gas to be measured to be more present on the optical path of the light beam inside cavity 270. Thus, it is possible to detect the presence of a gas, and to determine its concentration in the cavity, for a reduced length of said optical path. The gas sensor 60 thus produced is also suitable for measuring low concentrations of a gas, or for measuring on a gas having a low absorption cross section. In the example shown in Figure 6, the gas sensor 60 is part of an ethylene 100, but can be considered many other devices that may include such a gas sensor, for example volatile organic compound sensors such as formaldehyde . The pre-concentrator 63 of FIG. 6 therefore makes it possible to concentrate the ethanol, but preconcentrators can be envisaged to concentrate formaldehyde or another volatile organic compound. The pre-concentrator 63 is placed on one of the return reflective surfaces. According to a variant not shown, each return reflective surface is covered by the pre-concentrator or by a dedicated pre-concentrator. In the example shown in Figure 6, the pre-concentrator 63 is placed on the return reflective surface 281.
    [0030] A disadvantage of a pre-concentrator is that it does not release the gas once the latter has been absorbed. It is thus seen that it is necessary to replace the pre-concentrator after each measurement made using the gas sensor 60. The gas sensor 60 has a removable cover 64, receiving the return reflective surfaces and the pre-concentrator 63. Thus, after each use of the breathalyzer 100, the preconcentrator 63 can be easily replaced. As mentioned above, the reflective return surfaces do not require precise alignment with respect to the other elements of the gas sensor 60. therefore consider removing and replacing the removable cover 64, by hand, without damaging the performance of the gas sensor 60. This provides a compact gas sensor, accurate and inexpensive. The gas sensor 60 is connected to a measurement and supply module 65. The measuring and supply module comprises in particular calculation means for measuring an ethanol concentration in the air in the cavity 270, using a calculation of a ratio between the light intensity received by the detector and the light intensity emitted by the light source. The measurement and power module 65 may comprise electronic means and computer and / or software means. It is typically a digital or analog electronic circuit, preferably dedicated, associated with a microprocessor and / or a computer. FIG. 7 shows a network forming a subwavelength lens 70, which can be used as objective, eyepiece and / or relay lens, in a gas sensor according to the invention. In other words, at least one of these refractive optics can be formed by a subwavelength lens 70, also called subwavelength grating, or sub-lambda lens. The subwavelength lens 70 is formed of nanostructures of nanometric dimensions, for example pads 71. The pads may be arranged in square matrix, honeycomb, these two examples are not limiting. Alternatively, these nanostructures may be holes, lines, or any other pattern. It can also be a concentric circle whose pitch is less than the wavelength and whose center corresponds to the optical axis of the sub-wavelength lens 70. This optical axis is then advantageously confused with the optical axis of the light source (or of an elementary light source), corresponding to the optical axis of the detector (or a corresponding elementary detector). The characteristic dimension of these nanostructures is well below the wavelength of the light beam emitted by the light source. For example, these nanostructures are pads whose section is much smaller than said wavelength. For example, the incident light beam has a wavelength between 2 μm and 10 μm, and the section of a pad is of the order of 400 nm. The height of a pad is between 4 μm and 10 μm. The density of the pads varies between the center of the subwavelength lens and the edges of the subwavelength lens. Thus, at the scale of the wavelength of the incident light beam, the subwavelength lens 70 has a gradient index and acts as a refractive optics. The subwavelength lens 70 is advantageously etched in a silicon layer. Preferably, a pre-existing silicon layer of the gas sensor is used for etching a subwavelength lens forming refractive optics. According to a first variant, the subwavelength lens 70 is etched on the face of the silicon substrate 231 opposite the face receiving the source and the detector. Preferably, only the objective and the eyepiece are made by a subwavelength lens. Figure 8A illustrates an example of this first variant. FIG. 8A represents a detail of FIG. 6, and differs from FIG. 6 in that the elementary and elementary ocular objectives are each formed by a subwavelength lens 70 etched on the face of the silicon substrate opposite to the face receiving the source and the detector. According to a second variant, the subwavelength lens 70 is etched on the face of the silicon substrate receiving the source and the detector. FIG. 8B illustrates an example of this second variant. In the example shown in FIG. 8B, the objective, the eyepiece and the relay lens are made by a subwavelength lens. FIG. 8B represents a detail of FIG. 6, and differs from FIG. 6 in that the elementary, elementary ocular and elementary relay lenses are each formed by a subwavelength lens 70 etched on the face of the substrate in silicon receiving the source and the detector. The layer of reflective material 53 is under the relay lens, this time on the side of the substrate receiving the source and the detector. According to a third variant, the sub-wavelength lens 70 is etched on a lower or upper face of the cap protecting the light source or the detector (see description with reference to FIG. 5). An advantage of such a subwavelength lens 70 is that it makes it possible to further reduce the bulk of a gas sensor according to the invention, since at least some of the refractive optics form an integral part of the substrate. Silicon or silicon cap belonging to the source or detector. The invention is not limited to the examples which have just been described, and many variants can be envisaged without departing from the scope of the present invention. In particular, other examples of sources or detectors may be implemented, including sources and detectors adapted to be mounted on a substrate and according to a technology called "wafer-level packaging".
    权利要求:
    Claims (15)
    [0001]
    REVENDICATIONS1. A gas sensor (20; 30; 50; 60) comprising a cavity (270) for receiving a gas, a light source (210) and a detector (251), characterized by: a substrate (231); an objective (211) located on the substrate (231), adapted to collect a light beam (212, 213) emitted by the light source (210); an eyepiece (250) located on the substrate (231), adapted to collect an incident light beam to focus on the detector (251); so-called return reflective surfaces (281, 282) facing said substrate; and at least one relay lens (221, 321, 322) disposed on an intermediate reflecting surface (222) formed on the substrate (231), and comprising at least one field lens (221; 321) adapted to deviate rays (213) of the light beam emitted by the light source, to bring them closer to the optical axis of the eyepiece (250); the objective (211), the eyepiece (250), the relay lens (221; 321, 322), the intermediate reflective surface (222), and the return reflective surfaces (281, 282) together forming an optical system arranged so that the light beam (212, 213) emitted by the light source (210) is propagated by successive reflections from the lens (211) to the eyepiece (250) via the relay lens (221; , 322).
    [0002]
    2. Gas sensor (20; 30; 50; 60) according to claim 1, characterized in that the light source (210) and the detector (251) are arranged on a first face of the substrate (231), opposite to a second face of the substrate (231) on which are disposed the objective (211), the eyepiece (250), and the relay lens (221; 321, 322).
    [0003]
    A gas sensor (20; 30; 50; 60) according to claim 1 or 2, characterized in that the field lens (221; 321) is a concave plane lens, a planar face of the field lens being disposed on the intermediate reflective surface (222) and in an intermediate focus of the optical system.
    [0004]
    4. A gas sensor (30) according to any of claims 1 to 3, characterized in that the relay lens comprises at least one intermediate lens (322) interposed between two field lenses (322), so that the light beam (212, 213) emitted by the light source (210) is propagated by successive reflections from the objective (211) to the eyepiece (250) via the field lenses (321) and the intermediate lens (322). ).
    [0005]
    A gas sensor (20; 30; 50; 60) according to any one of claims 1 to 4, characterized in that at least one optical element among the relay lens (221; 321,322), the lens (211), and the eyepiece (250) consists of a subwavelength lens (70).
    [0006]
    The gas sensor (50; 60) according to any one of claims 1 to 5, characterized in that: the light source comprises a plurality of elementary sources (210; the objective comprises a plurality of elementary objectives (211; 211Ai, 211B;), each adapted to collect a light beam emitted by an elementary source (210;); the eyepiece comprises a plurality of elementary eyepieces (250) each adapted to collect an incident light beam in order to focus it on the detector; andthe relay lens comprises a plurality of elementary relay lenses (212, 321, 322; 321A, 321B, 322A ,, 322B,).
    [0007]
    7. Gas sensor (50; 60) according to any one of claims 1 to 6, characterized in that the light source comprises a plurality of elementary sources (210) aligned on the same line (41).
    [0008]
    8. Gas sensor (50; 60) according to any one of claims 1 to 6, characterized in that the light source comprises a plurality of elementary sources (210,) distributed on either side of the detector and aligned according to two parallel lines (41A, 41B).
    [0009]
    The gas sensor (50; 60) according to any one of claims 1 to 6, characterized in that the light source comprises a plurality of elementary sources (210) distributed over a circle (45) centered on the detector.
    [0010]
    The gas sensor (50; 60) according to any one of claims 6 to 9, characterized in that at least one of the return reflective surfaces (281, 282) is inclined relative to the plane of the detector, so that light beams emitted by the elementary sources (210) are focused at the same point on the detector.
    [0011]
    The gas sensor (60) according to any one of claims 1 to 10, characterized by a gas pre-concentrator (63) disposed on a reflective return surface (281; 282).
    [0012]
    12. Gas sensor (20; 30; 50; 60) according to claim 11, characterized in that it comprises a cover (64) receiving the reflective return surface and the gas pre-concentrator (63), the hood ( 64) being removably made relative to the substrate (231).
    [0013]
    13. Gas sensor (20; 30; 50; 60) according to any one of claims 1 to 12, characterized in that the light source (210; 210) is a microelectronic infrared source comprising a resistive membrane. (510,) forming a heat emitter.
    [0014]
    14. Gas sensor (20; 30; 50; 60) according to any one of claims 1 to 13, characterized in that the detector (251; 251) is a microelectronic bolometer comprising an absorbing membrane (551 ,) forming a thermal absorbent.
    [0015]
    A breathalyzer (100) comprising a gas sensor adapted to receive a breath exhaled by a user, characterized in that the gas sensor is a gas sensor (20; 30; 50; 60) according to any of the claims. 1 to 14.
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    同族专利:
    公开号 | 公开日
    EP2891877A1|2015-07-08|
    US9488577B2|2016-11-08|
    EP2891877B1|2016-07-27|
    FR3016213B1|2016-02-26|
    US20150192517A1|2015-07-09|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    FR2390725A1|1977-05-13|1978-12-08|Commissariat Energie Atomique|PHOTOMETRY DEVICE WITH CONCAVED MIRRORS AND FIELD OPTICS|
    US5468961A|1991-10-08|1995-11-21|Fisher & Paykel Limited|Infrared gas analyser and humidity sensor|
    US5459566A|1994-04-22|1995-10-17|The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration|Multiple pass gas absorption cell utilizing a spherical mirror opposite one or more pair of obliquely disposed flat mirrors|
    WO2011151629A1|2010-06-03|2011-12-08|Duvas Technologies Limited|Optical absorption spectroscopy|
    US4394575A|1980-06-30|1983-07-19|Ophir Corporation|Apparatus for measuring vapor density, gas temperature, and saturation ratio|
    US4933545A|1985-12-30|1990-06-12|Metricor, Inc.|Optical pressure-sensing system using optical resonator cavity|
    DE4434814A1|1994-09-29|1996-04-04|Microparts Gmbh|Infrared spectrometric sensor for gases|
    SE520664C2|2000-04-27|2003-08-05|Senseair Ab|Carbon dioxide-adapted gas cell|
    US7649174B2|2008-02-11|2010-01-19|Flir Systems, Inc.|Thermography camera configured for gas leak detection|DE202015002315U1|2015-03-27|2015-05-06|Infineon Technologies Ag|gas sensor|
    JP6626281B2|2015-07-10|2019-12-25|旭化成エレクトロニクス株式会社|Gas sensor|
    CN105842167A|2016-04-21|2016-08-10|青岛海纳光电环保有限公司|Optical path adjustable gas-absorbing pool|
    DE102016012970A1|2016-10-28|2018-05-03|Drägerwerk AG & Co. KGaA|Device for determining the concentration of at least one gas component in a breathing gas mixture|
    US10837837B2|2016-12-13|2020-11-17|Koninklijke Philips N.V.|Microbolometer focal plane array with integrated multi-spectral mosaic band-pass filter/focusing lens array for simultaneous real-time anesthetic and respiratory gas concentration detection and measurement signal processing|
    DE102016225344A1|2016-12-16|2018-06-21|Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V.|System for analyzing electromagnetic radiation and device for producing the same|
    DE102016125840B4|2016-12-29|2018-11-08|Infineon Technologies Ag|Gas analyzer|
    法律状态:
    2015-02-02| PLFP| Fee payment|Year of fee payment: 2 |
    2016-02-01| PLFP| Fee payment|Year of fee payment: 3 |
    2017-01-31| PLFP| Fee payment|Year of fee payment: 4 |
    2018-01-31| PLFP| Fee payment|Year of fee payment: 5 |
    2019-09-27| ST| Notification of lapse|Effective date: 20190906 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1450048A|FR3016213B1|2014-01-06|2014-01-06|MINIATURE GAS SENSOR.|FR1450048A| FR3016213B1|2014-01-06|2014-01-06|MINIATURE GAS SENSOR.|
    EP14199930.0A| EP2891877B1|2014-01-06|2014-12-23|Miniature gas sensor|
    US14/589,340| US9488577B2|2014-01-06|2015-01-05|Miniature gas sensor|
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