• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to an optical sensor (1000) comprising: an optical device (100) comprising a micro-resonator (120), arranged to guide a light beam along a closed-loop optical path, and an injection waveguide and / or extraction (110), optically coupled to the microresonator; a photo-detector (150) disposed at the exit of the injection and / or extraction waveguide; and - an analysis device (160), receiving a signal provided by the photodetector, and deriving information relating to a displacement. According to the invention, the micro-resonator consists of a plurality of elementary waveguides (121) spaced apart from each other and arranged one after the other in a loop-shaped arrangement. The optical sensor according to the invention offers an increased sensitivity to the measurement of nanometric displacements.
    公开号:FR3068778A1
    申请号:FR1756293
    申请日:2017-07-04
    公开日:2019-01-11
    发明作者:Boris TAUREL；Salim BOUTAMI；Laurent Duraffourg
    申请人:Commissariat a lEnergie Atomique CEA；Commissariat a lEnergie Atomique et aux Energies Alternatives CEA；
    IPC主号:
    专利说明:

    DISPLACEMENT SENSOR WITH SEGMENTED RING MICRO-RESONATOR
    DESCRIPTION
    TECHNICAL AREA
    The invention relates to the field of waveguide micro-resonators, and their use for detecting or even measuring, a deformation of the micro-resonator or a displacement in the near field of this micro-resonator.
    PRIOR STATE OF THE ART
    The article "Optical racetrack resonator transduction of nanomechanical cantilevers", by V.T.K. Sauer & al., Nanotechnology, vol. 25 (2014), describes the measurement of the displacement of a nanobeam, near a waveguide micro-resonator.
    The waveguide micro-resonator consists of a curved ring-shaped waveguide, called a ring micro-resonator.
    The ring micro-resonator does not have a sheath. It is the surrounding environment which acts as a sheath.
    This micro-resonator is coupled to an injection and extraction waveguide, by evanescent coupling.
    The evanescent coupling corresponds to an interaction between a guided mode of the injection and extraction waveguide, and a guided mode of the micro-resonator, which results in an energy transfer between these two modes.
    This energy transfer is maximum at the resonance wavelengths of the microresonator. A resonance wavelength of the micro-resonator is a wavelength for which the phase shift provided by a revolution in the ring is a multiple of 2π.
    In operation, a light beam, called an analysis beam, is sent to the input of the injection and extraction waveguide. Part of the analysis laser beam escapes to the micro-resonator, where it performs one or more turns before returning to the injection and extraction waveguide.
    The part of the analysis beam passing through the micro-resonator undergoes optical losses there, due in particular to absorption by the surrounding medium.
    A movable nanobeam is placed in the near field of the micro-resonator. It approaches or moves away from the micro-resonator, depending on external conditions.
    The position of the nanobeam locally defines the composition of a sheath for the micro-resonator. This position therefore influences the value of the effective index N e ^ of the guided mode in the micro-resonator, and consequently the values of resonance wavelength λ.
    These quantities, effective index N e ^ and resonance wavelengths λ, are indeed linked to each other. For a circular optical path of radius R in the micro-resonator, we have in particular:
    (D with m an integer greater than or equal to unity.
    The analysis of a variation in light, at the output of the injection and extraction waveguide, therefore makes it possible to detect and measure a variation in the position of the nanobeam, relative to the ring micro-resonator.
    The influence of the nanobeam on the resonant wavelengths remains however quite limited, which limits the sensitivity of the sensor.
    An objective of the present invention is to provide an optical sensor comprising a waveguide micro-resonator, offering improved sensitivity to the detection of a displacement in the near field of this micro-resonator.
    STATEMENT OF THE INVENTION
    This objective is achieved with an optical sensor comprising:
    an optical device, which comprises:
    - a waveguide micro-resonator, arranged to guide a light beam along an optical path in a closed loop; and
    an injection and extraction waveguide, or an injection waveguide and an extraction waveguide, optically coupled to the microresonator for the injection and extraction of said light beam;
    a photo-detector, disposed at the outlet of the injection and extraction waveguide, respectively at the outlet of the extraction waveguide; and an analysis device, receiving as input a signal supplied by the photo-detector, arranged to compare this signal with reference data, and to deduce therefrom information relating to a movement within the optical device.
    According to the invention, the micro-resonator consists of a plurality of elementary waveguides, spaced from one another, and arranged one after the other in a loop-shaped arrangement.
    Thus, an additional mobile element such as a nano-beam, can move close to the micro-resonator, until it is between two elementary waveguides.
    When the additional mobile element is between two elementary waveguides, it cuts the optical path of the light beam propagating in the micro-resonator, which results in a large increase in losses at the resonance wavelengths of the micro-resonator and / or a strong phase change in the micro-resonator.
    Thus, a displacement of the movable element between two positions, one located between two elementary waveguides of the micro-resonator, and the other not, results in a strong variation of the light leaving the guide injection and extraction wave (respectively at the output of the extraction waveguide).
    The sensitivity to the detection of this displacement is therefore greatly increased, in comparison with the prior art where only the evanescent part of a wave circulating in the micro-resonator is sensitive to this displacement.
    The constitution of the micro-resonator in elementary waveguides spaced from each other has other advantages, some of which are detailed below.
    A waveguide micro-resonator can, in particular when it is arranged suspended, contract and extend radially. This movement is called "microresonator breathing".
    The article "A monolithic radiation-pressure driven, lowphase noise silicon nitride optomechanical oscillator", by Siddharth Tallur & al., Optics Express, Vol. 19, No. 24, describes a ring micro-resonator, according to the prior art, as well as its movement of radial contraction and extension.
    This movement changes the curvilinear length of the micro-resonator, which results in a change in its resonant wavelengths.
    With a micro-resonator according to the invention, this movement also modifies the length of gap between two neighboring elementary waveguides, and therefore the effective index of a mode guided in the micro-resonator.
    However, the resonance length is also a function of this effective index. In comparison with the prior art, the variation in resonance wavelength is therefore higher, for the same amplitude of radial movement.
    This increases the sensitivity of detection, or even measurement, of the mechanical deformation of the micro-resonator.
    Since the micro-resonator consists of separate elementary waveguides, it is possible to release the movement of some of them, relative to the others.
    Mechanical stresses, which in the prior art were not capable of deforming the micro-resonator, can then cause the displacement of one or more elementary waveguides relative to the others. This displacement results in a variation of a signal having passed through the micro-resonator. This increases the sensitivity of the micro-resonator to external mechanical stresses.
    The movement within the optical device, mentioned above, designates in particular a deformation of the micro-resonator itself, and / or the movement of a mobile element relative to the micro-resonator.
    The analysis device can in particular be arranged to compare a wavelength spectrum, supplied by the photo-detector at a current instant t1, and a reference spectrum.
    The reference spectrum can be a wavelength spectrum, supplied by the photodetector at an instant t0 preceding the instant tl.
    The comparison of spectra, which is then implemented by the analysis device, may include a comparison of intensity values, in local minima of these spectra, and / or a comparison of wavelength values, associated to these local minima.
    The invention is based on the interaction between a mechanical displacement and an optical phenomenon of resonance. The optical sensor according to the invention therefore forms an opto-mechanical sensor, with improved sensitivity. The improvement is linked to an opto-mechanical coupling exacerbated between the mechanical displacement and the optical phenomenon of resonance, or in other words between a mechanical oscillator and an optical oscillator.
    The optical sensor according to the invention offers increased sensitivity to the measurement of nanometric displacements.
    The optical device comprising the micro-resonator is described in detail, and protected as such, in patent application FR 16 57222, filed on July 27, 2016. This patent application, on the other hand, does not describe an optical sensor comprising an analysis device as described above, and does not identify the specific advantages of using said optical device to obtain information relating to a movement.
    The optical sensor according to the invention may further comprise an annex mobile element, adapted to move relative to the micro-resonator so as to cross partially or totally a free space between two neighboring elementary waveguides.
    The elementary waveguides of the micro-resonator can be suspended above a substrate, and around a pedestal.
    Preferably, the pedestal has a cylinder shape, the base of the cylinder having a diameter between 0.25 and 0.75 times the diameter of the micro-resonator.
    According to an advantageous embodiment, the elementary waveguides of the microresonator are mounted integral with a support plate, itself bearing on the pedestal.
    The support plate may have one or more trenches, each of these trenches extending from a peripheral region of the support plate, located between two neighboring elementary waveguides, up to a central region of the support plate.
    The support plate can have at least one pair of trenches, each pair delimiting a so-called area on the support plate, receiving one or more elementary waveguides.
    The support plate can have a single pair of trenches.
    As a variant, the support plate may have two pairs of trenches, arranged symmetrical to one another.
    According to another variant, the support plate can have a plurality of trenches together delimiting a plurality of symmetrical isolated zones two by two.
    According to another advantageous embodiment, the elementary waveguides are suspended around the pedestal, by means of arms which extend in a plane parallel to the plane of the micro-resonator.
    The elementary waveguides can also be supported on a substrate, without lever arms.
    The elementary waveguides of the micro-resonator are advantageously distributed periodically one after the other, according to a regular pitch called the distribution pitch.
    Preferably, the distribution pitch (P) is less than:
    λ
    2n h with λ a resonance wavelength of the micro-resonator; and n h the average refractive index of the elementary waveguides.
    BRIEF DESCRIPTION OF THE DRAWINGS
    The present invention will be better understood on reading the description of exemplary embodiments given purely by way of non-limiting indication, with reference to the appended drawings in which:
    Figures IA and IB schematically illustrate a first embodiment of an optical sensor according to the invention, respectively in a top view and in a sectional view;
    Figure 2 illustrates transmission spectra obtained using the sensor of Figures IA and IB;
    Figure 3 schematically illustrates a first variant of the embodiment of Figures IA and IB;
    Figure 4 schematically illustrates a second variant of the embodiment of Figures IA and IB;
    FIG. 5 schematically illustrates a second embodiment of an optical sensor according to the invention;
    FIGS. 6A and 6B illustrate a comparison of the variation in transmission spectrum obtained using a sensor according to the prior art, and using a sensor according to the invention;
    FIGS. 7A and 7B schematically illustrate a first variant of the suspended arrangement of the micro-resonator according to the invention;
    FIGS. 8A and 8B schematically illustrate a second variant of the suspended arrangement of the micro-resonator according to the invention;
    FIGS. 9A to 9D illustrate different variants of the micro-resonator of a third embodiment of an optical sensor according to the invention;
    FIGS. 10A and 10B illustrate two variants of a coupling zone of an injection and extraction waveguide according to the invention; and FIG. 11 schematically illustrates a method of manufacturing an optical device according to the invention.
    DETAILED PRESENTATION OF PARTICULAR EMBODIMENTS
    FIGS. 1A and 1B illustrate a first embodiment of an optical device 100 and an optical sensor 1000 according to the invention, respectively according to a top view, in the plane (xOy) of an orthonormal reference frame, and according to a view in section, in the plane (yOz) of the same coordinate system. In Figure IA, there is shown the section plane AA 'corresponding to Figure IB.
    The optical device 100 comprises:
    - An injection and extraction waveguide 110, configured to guide a light beam called the analysis beam; and
    - A waveguide micro-resonator 120, configured to guide at least a portion of the analysis beam along an optical path 123 in closed loop.
    According to the invention, the waveguide micro-resonator 120 consists of a plurality of waveguide sections, called elementary waveguides 121.
    The elementary waveguides 121 together define the optical path 123 traveled by the light in the micro-resonator, here a circular optical path 123 (shown in dotted lines in FIG. IA). In other words, they are arranged one after the other in a ring-shaped arrangement.
    The several elementary waveguides are spaced from each other. In other words, the input of an elementary waveguide is not in direct physical contact with the output of a neighboring elementary waveguide. The elementary waveguides are separated two by two by a respective free space 122.
    Each of the elementary waveguides 121 is devoid of sheath, so that in operation, a surrounding medium around the micro-resonator 120 acts as sheath.
    Each elementary waveguide 121 is advantageously made of the same single material (or alloy). This material is the same for all the elementary waveguides 121.
    The elementary waveguides are advantageously made of silicon or of silicon nitride.
    They are for example made of silicon, to guide a light beam in the infrared (wavelength greater than 1 μm, in particular between 1 μm and 10 μm).
    As a variant, the elementary waveguides 121 are made of nitride, in particular silicon nitride (SisIXk), to guide a light beam in the visible range (wavelength strictly less than 1 μm, in particular between 0.4 pm and 0.8 pm).
    It can be considered that the micro-resonator 120 forms a segmented ring micro-resonator, that is to say a micro-resonator as described in the introduction, in which only certain sections of the curved waveguide are preserved, and form the elementary waveguides.
    The micro-resonator 120 is placed near the injection and extraction waveguide 110.
    At the micro-resonator 120, the injection and extraction waveguide 110 extends in a straight line, parallel to a tangent to the micro-resonator.
    The injection and extraction waveguide 110 extends outside the microresonator 120, without necessarily having direct physical contact with the latter.
    In the following, an example is illustrated, but not limited to, in which the injection and extraction waveguide 110 is spaced from the micro-resonator 120.
    Preferably, the injection and extraction waveguide 110 is made, like the elementary waveguides 121, of a single material (or alloy), the surrounding medium acting as a sheath. This single material is advantageously the same as that constituting the elementary waveguides.
    In the example described with reference to Figures IA and IB, the injection and extraction waveguide is advantageously formed unsprung, mechanically stable relative to the micro-resonator.
    The micro-resonator 120 and the injection and extraction waveguide 110 are optically coupled to each other by evanescent coupling.
    In operation, the injection and extraction waveguide 110 receives at the input a light beam 111 called the analysis beam.
    At least part of the analysis beam is transferred into the micro-resonator 120, by evanescent coupling. This part of the analysis beam is a signal at a resonant wavelength of the micro-resonator 120. It can be all or part of the analysis beam.
    A resonance wavelength of the micro-resonator is a wavelength for which the phase shift provided by a revolution in the micro-resonator is a multiple of 2π.
    This part of the analysis beam, transferred from the injection and extraction waveguide 110 to the micro-resonator 120, performs several turns in the microresonator 120 before returning to the same injection and extraction waveguide 110 .
    All the light does not return in the injection and extraction waveguide 110, due to losses during propagation in the micro-resonator 120. These losses can even be 100%.
    As shown in FIG. 1B, all the elementary waveguides 121, of thickness h lt are arranged here on the same plane support 140, of thickness H.
    The thicknesses H and h r are measured along the axis (Oz), orthogonal to the plane of the microresonator.
    In FIG. 1B, but in a nonlimiting manner, the thickness H is greater than or equal to the thickness h ± .
    The flat support 140 extends under all of the elementary waveguides 121, between these elementary waveguides 121 and a substrate 172.
    The planar support 140 is in direct physical contact, on one side with each of the elementary waveguides 121, and on the other with said substrate 172.
    Thus, the micro-resonator 120 is not suspended above this substrate 172. In other words, the support points of an elementary waveguide 121 on the substrate 172 are aligned with said guide d elementary wave, along the axis (Oz). In other words, the elementary waveguides 121 are supported on the substrate 172, without a lever arm.
    The elementary waveguides are therefore mechanically stable, relative to each other, and relative to the substrate 172.
    Many variants of an arrangement of the micro-resonator 120 not suspended above the substrate 172 can be implemented, for example without the intermediate planar support 140.
    According to the first embodiment of the invention, the optical device 100 also comprises an annex mobile element 130, which can move relative to the micro-resonator 120, preferably in an oscillating movement.
    In FIG. 1B, elementary waveguides 121 of reduced width are shown, for a better illustration of the movable annex element 130. Nevertheless, the elementary waveguides 121 are preferably wider than tall (dimension according to (Oz)).
    The mobile arrangement of the element 130 can be achieved by a suspended fixing, one end of the element 130 being able to be left free.
    The annex mobile element 130 is located in the near field of the micro-resonator, spaced from the latter by a distance less than a few hundred nanometers, for example less than 600 nm and even less than 300 nm.
    At least one of the dimensions of the movable annex element is less than 0.5 μm, preferably between 10 nm and 300 nm.
    The annex mobile element 130 is here a nanobeam, of width L1 between 100 nm and 200 nm, and of length L2 being worth approximately 1 μm.
    Here, the thickness of the nanobeam 130 (along the axis (Oz)) is less than that of the elementary waveguides 121, without this example being limiting.
    The nanobeam is movable between two extreme positions. In Figures IA and IB, the nanobeam 130 is shown twice, in each of these two extreme positions.
    The path 131 followed by the nanobeam, between these two extreme positions, is represented by a dotted arrow.
    The path 131 extends here in a plane parallel to the plane of the micro-resonator 120. It here defines a radius of the micro-resonator 120.
    Throughout the text, the plane of the micro-resonator is a plane receiving the upper faces of the elementary waveguides 121, parallel to the plane (Oxy).
    In a first of said extreme positions, the nano-beam 130 is oriented towards the center of the micro-resonator, but located entirely outside of it.
    In this case, the optical losses in the micro-resonator remain limited. The nanobeam only interacts with the evanescent part of the beam circulating in the microresonator, as in the prior art.
    In the other of said extreme positions, the nanobeam 130 has been translated along the path 131, and partly extends in a free space 122, between two neighboring elementary waveguides 121.
    It then cuts the path of the light beam in the micro-resonator 120, which causes high optical losses (by optical leaks in the nano-beam, by reflections, diffraction, or even disturbance of a condition on the step of the guides elementary waves that can cancel a guidance condition, etc.).
    The optical losses increase with an occupancy rate, by the nano-beam, of a free space 122 between two elementary waveguides.
    The nanobeam can move in an oscillating movement, during which it enters and leaves a free space 122, between two neighboring elementary waveguides 121.
    By following the evolution over time, of the spectrum of the light beam 112 at the output of the injection and extraction waveguide 110, it is possible to detect, with good sensitivity, a nanometric displacement of the nano-beam relative to the microresonator 120 (for example a displacement less than 20 nm).
    According to the invention, the optical device 100 is part of an optical sensor 1000 further comprising:
    - A photo-detector 150, disposed at the output of the injection and extraction waveguide 110, on the side opposite to an input end of the analysis beam 111 in the injection and extraction waveguide 110; and
    - an analysis device 160, connected to the photo-detector 150.
    The photodetector 150 comprises at least one photodiode. It may further comprise spectral dispersion means such as a prism or an array, or a simple filter, for distributing the different spectral components of a broad spectrum beam over the different photodiodes of a photodiodes array.
    It is arranged at one end of the injection and extraction waveguide, to receive the beam 112 emerging from the injection and extraction waveguide 110, and resulting from the coupling between the micro-resonator 120 and the injection and extraction waveguide 110.
    The analysis device 160 comprises electronic and / or computer means, in particular a processor.
    It receives as input a signal supplied by the photo-detector 150.
    This signal is advantageously, but not limited to, in the form of a wavelength spectrum of the beam 112, emerging from the injection and extraction waveguide 110.
    The analysis device 160 comprises in particular a comparator, electronic or computer, to compare the signal supplied by the photo-detector 150 with reference data, and to deduce therefrom information Id relating to a movement within the optical device 100 .
    The information Id is supplied at the output of the analysis device 160.
    Here, the analysis device 160 implements in particular a comparison between a first wavelength spectrum, supplied by the photo-detector 150 at an initial instant t0, and a second wavelength spectrum, supplied by the photodetector 150 at a time tl subsequent to tO. The wavelength spectrum, supplied at the initial instant t0, then forms the reference data.
    Figure 2 illustrates:
    - the wavelength spectrum 20 (in solid lines), supplied by the photo-detector 150 at an initial instant t0, when the nano-beam 130 is outside a free space between two guides elementary waves 121 neighbors; and
    - The wavelength spectrum 21 (in dotted lines), provided by the photo-detector 150 at time tl, when the nanobeam 130 crosses such a free space.
    The abscissa axis is a wavelength, in pm. The ordinate axis is a transmission rate from one end to the other of the injection and extraction waveguide 110.
    The micro-resonator 120 consists of 500 elementary silicon guides 121, bathed in air. The distribution step of the elementary guides 121 is 40 nm. They are distributed in a ring with a median radius equal to 5 μm. The injection and extraction waveguide has a section of 500 nm by 220 nm. The gap between the injection and extraction waveguide 110 and the micro-resonator 120 is 300 nm. The nanobeam is a rectangular parallelepiped of dimensions 1000 nm x 220 nm x 30 nm.
    The spectra 20 and 21 each correspond to the analysis beam, minus the losses in the micro-resonator 120. These losses are localized at the resonance wavelengths of the micro-resonator 120. These losses form transmission minima 20i, 202 ... 20i, respectively 21ι, 2I2 ... 21 ,, on spectra 20, respectively 21.
    As expected, the losses are much higher when the nanobeam 130 intersects the optical path of the beam passing through the micro-resonator. In particular, the transmission rate at the smallest resonant wavelength is reduced by approximately 8%, when the nanobeam 130 intersects the optical path of the beam passing through the microresonator.
    Thus, the evolution over time of the spectrum of the signal at the output of the injection and extraction waveguide, makes it possible to detect with very good sensitivity that the nanobeam enters or leaves a free space between two guides neighboring elementary waves.
    In particular, the aim here is to follow the evolution over time of the intensity values at the level of the transmission minima.
    The information, la, relating to a displacement within the optical device 100, can consist of the simple detection of a displacement greater than a predetermined threshold.
    According to an advantageous variant, the analysis device 160 uses the result of the comparison, here a comparison of spectra, to calculate the value of this displacement (in unit of length).
    The information, la, then includes this value of this displacement.
    The calculations implemented to calculate this displacement will not be described here further, and will not present any difficulty in itself for the skilled person, specialist in the use of micro-resonators to measure a displacement.
    Each displacement can be considered as a sum of two displacements, a first displacement where the nano-beam remains entirely outside the microresonator, and a second displacement where the nano-beam crosses an increasingly large portion of a space free between two elementary waveguides.
    The first movement can resume calculations implemented in the prior art. The second displacement involves original calculations, based on simulations or on a theoretical model of the micro-resonator.
    Many variants can be implemented without departing from the scope of the invention.
    For example, the nanobeam 130 can move along a vertical path 331, orthogonal to the plane of the micro-resonator 120, as illustrated in FIG. 3. Again, the width of the elementary waveguides is not representative, the latter preferably being wider than tall.
    Other paths can combine components according to (Oz) and according to (Oxy).
    According to a variant not shown, the annex mobile element is a membrane.
    According to another variant, the injection and extraction waveguide 110 is replaced by an injection waveguide 110A, for injecting the analysis beam 111 into the microresonator, and an extraction waveguide 110B separate from the extraction waveguide, to receive what remains of the analysis beam after transit through the micro-resonator 120.
    This variant is illustrated by the optical device 100 ′ and the optical sensor 1000 ′ in FIG. 4. In FIG. 4, the nanobeam is not shown.
    In this case, the analysis beam 111 can be a monochromatic beam, at a resonance wavelength of the micro-resonator 120, and the photo-detector 150 can consist of a simple photodiode, sensitive to this length d 'wave.
    Thus, the signal supplied by the photo-detector 150, to the analysis device 160, is not a spectrum but a single value of light intensity.
    The comparison implemented within the analysis device is then a comparison between an intensity value measured at time tl, and a reference value. Said reference value can be constituted by an intensity value measured at an instant t0, preceding the instant tl.
    This variant has the advantage that the photo-detector 150 receives only the wavelength affected by a displacement. It therefore offers increased sensitivity to this displacement, provided that the resonant wavelength is known, and little affected by the displacement.
    According to another variant, the optical device according to the invention does not include an additional mobile element, and the displacement of the injection waveguide and extraction, respectively of the injection waveguide and / or of the extraction waveguide. Said waveguide is then advantageously arranged suspended, bearing on at least two pillars.
    According to another variant, the optical device according to the invention comprises, on the contrary, several additional mobile elements such as nanobeams. These several elements move together, and together have a greater influence on the signal variations at the output of the injection and extraction waveguide. This increases the sensitivity to a stress causing these displacements.
    According to another variant, the micro-resonator is arranged suspended, but its modes of vibration are unlikely to modify the signal passing through the micro-resonator.
    In each variant of the invention, the reference data are advantageously data previously measured by the photo-detector 150. It can also be data previously calculated, obtained in a completely theoretical manner, or from experimental measurements compiled during a preliminary calibration step.
    The optical device according to the invention can be placed inside a hermetic cavity evacuated. It can also be placed inside a cryostat, to limit the Brownian thermal noise of movement. However, it is preferably subjected to atmospheric pressure.
    The optical sensor according to the invention can comprise the light source adapted to the emission of the analysis beam 111.
    According to a variant not shown, the elementary waveguides may have the shape of a rectangular parallelepiped. The distribution pitch of the elementary waveguides 121 being reduced, preferably less than 2 μm, the optical path of the light guided in the micro-resonator 120 can be assimilated to a circular path.
    The advantageous rules for sizing the optical device according to the invention are detailed below. Reference is made to FIG. 1A for illustration of the quantities mentioned.
    The micro-resonator, here in the form of a ring, advantageously has an external radius less than or equal to 10 μm, in particular less than or equal to 5 μm.
    Preferably, all the elementary waveguides have the same shape and the same dimensions. The shape of an elementary waveguide 121 is here a portion of a straight cylinder with an annular base, this portion being delimited by two planes 124 receiving the generatrix of the cylinder and defining together an angle a.
    Each elementary waveguide 121 is characterized by a height, a width w and a length l (here l is a curvilinear length, measured at the center of the elementary waveguide).
    The different elementary waveguides 121 are distributed periodically one after the other, according to a regular pitch P, called the distribution pitch.
    Here, the pitch P designates a curvilinear length, corresponding to the curvilinear length of an elementary waveguide 121 and of a free space 122. It is in other words the curvilinear length of a portion of the optical path 123, followed by light in the center of an elementary waveguide 121 and in the adjacent free space 122.
    So that the structure in independent elementary waveguides does not affect the light beam guided in the micro-resonator, the pitch P is less than the central wavelength of this light beam.
    On this scale, light is only sensitive to an average refractive index between the index of elementary waveguides 121 and the index in free spaces 122, and is not diffracted. In other words, the core of the micro-resonator 120 behaves like a material with an average refractive index:
    (2) with:
    l the curvilinear length of an elementary waveguide;
    P the distribution pitch of the elementary waveguides;
    n h the average refractive index in an elementary waveguide; and n b the average refractive index between two elementary waveguides, that is to say the average refractive index of the medium surrounding the elementary waveguides (this medium being able to include an additional mobile element such as described above).
    The moy n mean refractive index is an equivalent refractive index of the micro-resonator according to the invention.
    Preferably, the step P checks in particular:
    (3) with:
    λ the central wavelength of the light beam which propagates in the microresonator, or in other words a resonance wavelength of the micro-resonator, or in other words the resonance wavelength exploited by micro-resonator.
    We even have advantageously:
    (4) with:
    n h the average refractive index in an elementary waveguide.
    Here, the elementary waveguides are made of one and the same material, therefore n h is the refractive index of the elementary waveguides.
    In practice, the distribution pitch P is advantageously less than 3 μm, and even less than 2 μm, or even 1 μm.
    According to the invention, the micro-resonator 120 has a guided mode of effective index substantially equal to the effective index of a guided mode of the injection and extraction waveguide 110, preferably exactly equal. By substantially equal is meant equal to plus or minus 1% close, or even to plus or minus 5% close or even to plus or minus 10% close.
    As a reminder, the effective index of a mode, in particular the effective index of a mode guided by a waveguide, is defined as follows:
    (5) with:
    N e ff the effective index of the mode considered;
    λ the wavelength of the light beam propagating in the waveguide; and β the phase constant of the waveguide.
    The phase constant β depends on the wavelength and on the mode of the light beam propagating in the waveguide, as well as on the properties of this waveguide (in particular refractive indices and geometry).
    The phase constant β is defined by: A (z) = A (0) exp (yz), where z is an abscissa along a propagation path in the waveguide, A (z) is the complex amplitude in function of z of a light beam propagating in the waveguide, and β is the imaginary part of y.
    We can sometimes consider that the effective index designates the average optical index of the medium as it is "seen" by a mode of the light beam propagating in the waveguide.
    Preferably, the mode guided in the micro-resonator, respectively in the injection and extraction waveguide, is a zero order mode.
    The injection and extraction waveguide 110 being formed in one piece, and the micro-resonator 120 being formed segmented, the above condition on the effective indices of the guided modes advantageously results in a condition on the widths respective of the injection and extraction waveguide 110 and of the elementary waveguides 121.
    Advantageously, we have:
    w> W (6) with:
    w the width of an elementary waveguide 121, measured in a plane orthogonal to the optical path 123 traversed by the light in the micro-resonator 120; and
    IV the width of the injection and extraction waveguide 110, measured in a plane orthogonal to the optical path traveled by the light in the injection and extraction waveguide 110.
    In practice, each elementary waveguide 121 preferably has a rectangular section of height / q and width w, in planes orthogonal to the optical path 123 traversed by the light in the micro-resonator 120. In the same way, the injection and extraction waveguide 110 advantageously has a rectangular section of height = h 2 and of width W, in planes orthogonal to the optical path traveled by the light in the injection and extraction waveguide 110.
    Equation (6) is notably verified when the injection and extraction waveguide 110 is made of the same material as the elementary waveguides 121, and therefore has the same refractive index.
    The widths w and IV making it possible to verify the above condition on the effective indices of the guided modes, can be calculated with precision using electromagnetic simulation tools known to those skilled in the art. These simulation tools can be used to adjust the various parameters of the optical device according to the invention, so as to verify said condition. These parameters are in particular geometric parameters (no distribution P, curvilinear length l of an elementary waveguide), and refractive index values (refractive indices of the injection and extraction waveguide and index elementary waveguides).
    In particular, an optimal value of the ratio between the widths w and IV can be determined.
    The ratio of the width w divided by the width IV is substantially equal to 2, advantageously between 1.9 and 2.1, and even between 1.8 and 2.2.
    Preferably, the ratio between the curvilinear length Z of an elementary waveguide and the distribution pitch P is substantially equal to 0.5. In particular, this ratio is advantageously between 0.4 and 0.6, or even between 0.45 and 0.55, or even exactly equal to 0.5.
    In other words, the free spaces have approximately the same curvilinear length as the elementary waveguides, which corresponds to the best technological compromise since neither the elementary waveguides nor the free spaces have to present dimensions too reduced.
    Preferably, there is both a ratio of about 0.5 between the curvilinear length l and the pitch P, and a ratio of the width w divided by the width IV substantially equal to 2.
    FIG. 5 schematically illustrates a second embodiment of an optical device 500 and an optical sensor 5000 according to the invention.
    This second embodiment will only be described for its differences with respect to the first embodiment described above.
    Here, the micro-resonator 520 is arranged suspended above a substrate, bearing on a central pillar, or pedestal, 570. In other words, the support points of the elementary waveguides on the substrate are located under the pedestal 570. In other words, the elementary waveguides are supported on the substrate by means of a lever arm.
    Here, the optical device 500 does not include an annex mobile element.
    The displacement detected using the invention is then a displacement of the elementary waveguides relative to one another.
    The suspended arrangement in particular releases a movement of radial contraction and extension of the micro-resonator 520, corresponding to breathing modes of the micro-resonator.
    For purposes of illustration, the microresonator 520 has been shown simultaneously in FIG. 5 in a position of radial contraction (radius RI of the micro-resonator), and in a position of radial extension (radius R2> R1 of the micro- resonator).
    As in the prior art, the movement of radial contraction and extension modifies the curvilinear length L of the optical path of a light beam making a turn in the micro-resonator, which modifies the resonance wavelengths λ of the microresonator since these two quantities are linked by:
    „NeffL λ = (7) m
    with:
    N ef f I 'effective index of the mode guided in the micro-resonator; and m an integer greater than or equal to unity (see also equation (1)).
    Said contraction and extension movement also modifies the distance between the micro-resonator and the injection and extraction waveguide, and therefore an optical coupling rate between these two elements. It also changes the confinement of light in the micro-resonator.
    In addition, due to the constitution of the micro-resonator 520 in a plurality of elementary waveguides 521, this movement also results in a bringing together and then a distancing of the elementary waveguides relative to each other (without change of significant dimension for elementary waveguides).
    The ratio between the length l of an elementary waveguide (constant) and the distribution pitch P of said waveguides (modified) is therefore modified.
    This results in a variation of the average refractive index n av of the microresonator (see equation (2)), and therefore of the effective index N eff of the mode guided in the microresonator.
    This variation in the effective index N eff also participates in modifying the resonance wavelengths of the micro-resonator. The variation in resonance length, linked to the movement of radial contraction and extension, is therefore increased.
    The variation in resonance wavelength is detected by the analysis device 560, which can deduce therefrom an amplitude of contraction and radial extension of the microresonator.
    FIGS. 6A and 6B illustrate a comparison of the variation in transmission spectrum obtained using a sensor according to the prior art (FIG. 6A), and using a sensor according to the invention (FIG. 6B ).
    In the two figures, the abscissa axis is a wavelength, in pm. The ordinate axis is a transmission rate from one end to the other of the injection and extraction waveguide.
    In FIG. 6A, the spectra 60A and 61A each correspond to an analysis beam, minus the losses in a micro-resonator according to the prior art.
    The spectrum 60A is associated with an extension position of said micro-resonator. The spectrum 61A is associated with a contraction position of said micro-resonator. The corresponding variation in resonance wavelength, δΛ Α , is 7.7 nm.
    In FIG. 6B, the spectra 60B and 61B each correspond to an analysis beam, minus the losses in a micro-resonator according to the invention.
    The micro-resonator associated with FIG. 6B differs from that associated with FIG. 6A only in that it consists of several elementary waveguides spaced from one another. In both cases, the contraction position of the micro-resonator corresponds to an average radius of 5.00 pm, and the extension position corresponds to an average radius of 5.05 pm (the average radius being the average of the internal radius and the external radius of the microresonator).
    The spectrum 60B is associated with an extension position of said micro-resonator. The spectrum 61B is associated with a contraction position of said micro-resonator. The corresponding variation in resonance wavelength, δΛ Β , is 9.1 nm, an improvement of 18% in the sensitivity to the breathing modes of the micro-resonator.
    FIGS. 7A and 7B schematically illustrate a first variant of the suspended arrangement of the micro-resonator according to the invention, respectively in a top view in a horizontal plane, and in a sectional view in a vertical plane.
    FIG. 7A shows the section plane BB ', corresponding to the view in FIG. 7B. Again, the width of the elementary waveguides is undersized.
    The micro-resonator 720 is arranged suspended above a substrate 772, resting on a pedestal 770.
    The 770 pedestal is centered on the geometric center of the micro-resonator 720.
    The pedestal 770 preferably has the shape of a cylinder, the base of which has a diameter Dl of between 0.25 and 0.75 times the average diameter D2 of the micro-resonator (average of the internal diameter and the external diameter), preferably between 0.25 and 0.5 times this diameter D2.
    The pedestal is preferably, but not limited to, a cylinder of revolution. It can also be a cylinder with a non-circular base, for example with an oval base. The diameter D1 is then the largest width of the base of the cylinder.
    The elementary waveguides 721 making up the elementary waveguide are all mounted integral with the same support plate 771.
    They extend here adjacent to said support plate 771, along a peripheral edge thereof.
    In practice, the assembly consisting of the elementary waveguides 721 and the support plate 771 can be formed by etching a single layer of material, so that there is physically no interface between a guide. elementary wave 721 and the support plate 771.
    According to a variant not shown, the elementary waveguides are located on the top of the support plate 771.
    The support plate 771 has a reduced thickness, at least three times less than the thickness of the elementary waveguides, or even at least ten times less, so that it does not influence the optical guidance in the micro-resonator .
    It extends along a plane parallel to the plane of the micro-resonator.
    Preferably, it does not protrude outside an area delimited by the elementary waveguides.
    Here it presents a form of full disc.
    Alternatively, it may have other shapes, for example a ring shape, suspended around the pedestal by means of internal arms.
    FIGS. 8A and 8B illustrate a second variant of the suspended arrangement of the micro-resonator according to the invention, respectively in a top view in a horizontal plane, and in a sectional view in a vertical plane.
    FIG. 8A shows the section plane CC ′, corresponding to the view in FIG. 8B. Again, the width of the elementary waveguides is undersized.
    In FIG. 8A, a smaller number of elementary waveguides has been shown for the sake of readability of the figures, without this prefiguring any limitation relating to this variant.
    According to this variant, the elementary waveguides are kept suspended around the pedestal 870 by means of arms which extend parallel to the plane of the micro-resonator. In particular, the upper faces of the arms extend in a plane parallel to the plane of the micro-resonator.
    The arms here comprise so-called peripheral arms, 875, which each extend between an elementary waveguide 821 and the neighboring elementary waveguide, and so-called internal arms, 876, which each extend between a guide of elementary wave 821 and pedestal 870.
    Here, the arms, in particular the peripheral arms, 875, each have a width LB much less than that of the elementary waveguides, for example at least 3 times less, and even at least 4 times or 5 times less.
    In the example shown in FIG. 8A, all the elementary waveguides 821 are connected two by two by peripheral arms 875, and four internal arms 876 extend in a cross and meet above the pedestal 870.
    Here, the arms 875 and 876 are formed with the elementary waveguides in the same layer, and have the same thickness h r as the latter (see FIG. 8B).
    FIGS. 9A to 9D illustrate different variants of a micro-resonator in a third embodiment of an optical device and an optical sensor according to the invention.
    According to this third embodiment, the micro-resonator is arranged suspended above the pedestal, by means of a support plate of the type described with reference to FIGS. 7A and 7B.
    For the sake of clarity, FIGS. 9A to 9D represent only the micro-resonator, according to a top view.
    According to this third embodiment, the support plate is traversed according to its thickness by trenches 925, or grooves, or slots.
    Each trench 925 extends from an outer edge of the support plate, to a central region of the plate, and passes between two neighboring elementary waveguides 921.
    Here, the trenches each extend to the pedestal.
    Preferably, each trench 925 crosses the support plate along its entire thickness, forming a through opening in said plate.
    Each trench 925 here extends along a radius of the ring micro-resonator.
    In FIG. 9A, the support plate 971A comprises two trenches 925. These two trenches delimit laterally, on the support plate 971, a so-called isolated area 9711A.
    The isolated area 9711A here receives a single elementary waveguide 921, called an isolated waveguide, the movement of which relative to the other elementary waveguides is released.
    In particular, the isolated waveguide can move horizontally in the plane of the micro-resonator 920A, according to a rotational movement around an axis parallel to (Oz).
    It can also move vertically, passing above then below the plane of the micro-resonator, according to a rotational movement around an axis located in the plane (xOy)
    It can also move in a rotational movement around the median axis of the isolated area 9711A, this axis also being located in the plane (xOy).
    Each of these rotations results in an increase in losses at the resonant wavelengths of the micro-resonator, or in a shift in the resonant wavelength, the guiding condition even being lost when the displacement of the guide d the isolated wave no longer makes it possible to verify the condition on the step P given in equation (3).
    This increase in losses is detected by the analysis device, which can deduce therefrom an amplitude of the movement of the isolated waveguide.
    This produces a micro-resonator, and therefore an optical device and sensor according to the invention, sensitive to a greater variety of external stresses, in comparison with the prior art.
    The micro-resonator 920B of FIG. 9B differs from that of FIG. 9A only in that the isolated zone 9711B receives several neighboring elementary waveguides 921.
    The micro-resonator 920C of FIG. 9C differs from that of FIG. 9A only in that the support plate 971C comprises two isolated zones 9711C, each being delimited laterally by a couple of two trenches.
    Each isolated zone 9711C here receives a single elementary wave guide.
    The two pairs of trenches are arranged here symmetrical to one another, according to a planar symmetry relative to a plane orthogonal to the plane of the micro-resonator.
    The micro-resonator 920D of FIG. 9D differs from that of FIG. 9A only in that the support plate 971D comprises a plurality of trenches defining a plurality of isolated zones 9711D. The isolated zones 9711D are symmetrical two by two, according to planar symmetries relative to a respective plane, orthogonal to the plane of the micro-resonator 920D.
    Each isolated zone 9711D here receives several elementary waveguides.
    Many other variants can be implemented without departing from the scope of the invention, comprising more or less trenches, with or without symmetries, etc.
    The distribution of the trenches makes it possible to favor one or the other movement of the elementary waveguides.
    Many other variants can be used to cut the support plate so as to isolate different elementary waveguides, neighboring or not.
    It is also possible to release the movement of one or more elementary waveguides, in a suspended arrangement as described with reference to FIGS. 8A and
    8B, for example by removing certain peripheral arms.
    FIGS. 10A and 10B illustrate two variants of a coupling zone of an injection and extraction waveguide according to the invention.
    Said coupling zone is located near the micro-resonator, where the evanescent coupling takes place between the injection and extraction waveguide and the microresonator. In order to promote this coupling, the phase agreement between the respective modes propagated in the injection and extraction waveguide and in the microresonator can be improved.
    The phase agreement is respected when the respective effective indices of the injection and extraction waveguide and of the micro-resonator are identical.
    Two solutions are described below to obtain this equality of the effective indices.
    In FIG. 10A, the width of the injection and extraction waveguide 1010A progressively decreases and then increases again, as we get closer to and then move away from the micro-resonator 1020.
    The injection and extraction waveguide 1010A then comprises a zone 10101 of reduced width, adjacent to the micro-resonator, two zones 10102 of adiabatic coupling (tapers), of decreasing width, respectively increasing, and two zones 10103 of greater width, on both sides of zone 10101.
    As a variant, coupling can be encouraged using an injection and extraction waveguide 1010B whose shape varies gradually until it approaches the segmented shape of the micro-resonator (see FIG. 10B).
    The injection and extraction waveguide 1010B is segmented, in a region adjacent to the micro-resonator. The transition from straight guide to segmented guide is done using a solid central zone 10104 (tap), the width of which decreases as it approaches the micro-resonator.
    The shape of the injection and extraction waveguide 1010B is delimited by an external envelope whose width increases as it approaches the micro-resonator.
    Inside this outer envelope, segments, 10105, are distributed in a periodic pitch on either side of the central zone 10104. The segments 10105 each extend from the central zone 10104 to the envelope external. At the micro-resonator, the injection and extraction waveguide 1010B now only has segments 10105, which each extend from one edge to the other of the external envelope.
    The distribution pitch of the segments 10105 is substantially equal to the distribution pitch of the elementary waveguides of the micro-resonator.
    The various embodiments described above can be combined together. For example, it is possible to combine the suspended arrangement of the micro-resonator and the detection of a displacement of an annexed mobile element.
    These embodiments each time include a micro-resonator coupled to a mechanical oscillator, or itself forming a mechanical oscillator. In the first case, the micro-resonator is frozen, and an additional element moves in its near field, the additional element can be an injection and / or extraction waveguide.
    The invention is not limited to the examples described above, and many variants can be made without departing from the scope of the invention.
    For example, the elementary waveguides may not be arranged in the form of a ring, but in another form of closed loop.
    The optical device according to the invention can also comprise a plurality of micro-resonators according to the invention, optically coupled together by an evanescent coupling.
    The optical sensor according to the invention makes it possible to detect and measure nanometric displacements (for example less than 20 nm), within the micro-resonator or in its near field.
    These nanometric displacements can be generated by a stress such as an acceleration of the reference frame receiving the optical device according to the invention, a rotation of this reference frame, a displacement of a particle of non-zero mass (for example a particle falling on a nano -beam as described above), a photon displacement, an atom displacement, etc.
    The analysis device can be arranged to convert the measurement of such a displacement, into a value of acceleration, or angular velocity, or mass, or electromagnetic radiation, or atom displacement, etc., for thus forming an accelerometer, or gyrometer, or mass-sensitive sensor such as a mass spectrometer, or radiation pressure sensor, or sensor for a photon source, etc.
    The invention does not relate to the micro-resonator optical device as such.
    FIG. 11 schematically illustrates an example of a method of manufacturing an optical device according to the invention.
    On the left, the device during manufacture is shown in a sectional view. On the right, the device during manufacture is shown in a top view. The manufacturing process uses a so-called SOI stack (for “Silicon On Insulator”), consisting of the following three superposed layers: a substrate 101 (for example made of silicon), an intermediate layer 102 made of silicon dioxide, and an upper layer 103 made of silicon (starting point 11).
    During a first step 12, the upper layer 103 of silicon is etched over its entire thickness, here to form the injection and extraction waveguide 1110 and a notched disc 104 of silicon. Each notch of the notched disc 104 corresponds to an elementary wave guide 1121 of the micro-resonator.
    The method according to the invention then comprises a step 13 of etching the disc 104, over only part of its thickness. During this step 13, the disc 104 is etched in a central region thereof, to form the micro-resonator 1120.
    The etching retains a small thickness of the central region of the disc 104, which makes it possible to ensure the mechanical strength of the micro-resonator 1120, and in particular to keep the elementary waveguides 1121 integral with each other (cf. support plate described with reference to Figures 7A and 7B).
    According to a variant not shown, one engraves, in step 12, a full disc (and not a notched disc). In step 13, the solid disc is etched over part of its thickness, in a central region and in annular regions thereof. The elementary waveguides are then placed on a residual disc of small thickness.
    Finally, in a step 14, the intermediate layer 102 is etched over its entire thickness to form a cavity 105 under the micro-resonator 1120 and the injection and extraction waveguide 5 1110. The etching preserves, under the micro- resonator 1120, a pedestal 1170 for holding the micro-resonator 1120 suspended above the substrate 101. The pedestal 1170 is approximately centered on the center of the micro-resonator 1120.
    The intermediate layer remaining around the cavity 105 is used in particular for the mechanical maintenance of the injection and extraction waveguide 1110, suspended above the substrate 101.
    The engraving here is a wet engraving over time.
    Each of the engravings preferably uses an etching mask.
    An annex mobile element can, like the injection and extraction waveguide, be etched in the upper layer 103 of silicon.
    As a variant, the annex mobile element may be made of a material different from that of the waveguides. It is for example a carbon nanotube.
    权利要求:
    Claims (15)
    [1" id="c-fr-0001]
    1. Optical sensor (1000; 1000 '; 5000) comprising:
    an optical device (100; 100 '; 500) comprising a waveguide micro-resonator (120; 520; 720; 820; 920A; 920B; 920C; 920D; 1020; 1120), arranged to guide a light beam according to a closed loop optical path, and an injection and extraction waveguide (110; 1010A; 1010B; 1110), or an injection waveguide (110A) and an extraction waveguide ( 110B), optically coupled to the micro-resonator for the injection and extraction of said light beam;
    a photo-detector (150; 550), disposed at the outlet of the injection and extraction waveguide, respectively at the outlet of the extraction waveguide; and an analysis device (160; 560), receiving as input a signal supplied by the photodetector, arranged to compare this signal with reference data, and to deduce therefrom information relating to a movement within the optical device (100 ; 100 '; 500);
    characterized in that the micro-resonator consists of a plurality of elementary waveguides (121; 521; 721; 821; 921; 1121) spaced from one another, and arranged one after the other according to a loop-shaped arrangement.
    [2" id="c-fr-0002]
    2. Optical sensor (1000; 1000 ') according to claim 1, characterized in that it further comprises an additional movable element (130), adapted to move relative to the micro-resonator so as to partially or totally pass through a space free (122) between two neighboring elementary waveguides.
    [3" id="c-fr-0003]
    3. Optical sensor (5000) according to claim 1 or 2, characterized in that the elementary waveguides (521; 721; 821; 921; 1121) of the micro-resonator are suspended above a substrate (772 ; 872; 101), and around a pedestal (570; 770; 870; 1170).
    [4" id="c-fr-0004]
    4. Optical sensor (5000) according to claim 3, characterized in that the pedestal (570; 770; 870; 1170) has a cylinder shape, the base of the cylinder having a diameter (Dl) between 0.25 and 0 , 75 times the diameter (D2) of the micro-resonator.
    [5" id="c-fr-0005]
    5. Optical sensor (5000) according to claim 3 or 4, characterized in that the elementary waveguides (521; 721; 921; 1121) of the micro-resonator are mounted integral with a support plate (771; 971A ; 971B; 971C; 971D), itself resting on the pedestal.
    [6" id="c-fr-0006]
    6. Optical sensor according to claim 5, characterized in that the support plate has one or more trenches (925), each of these trenches extending from a peripheral region of the support plate, located between two waveguides neighboring elementaries, to a central region of the support plate.
    [7" id="c-fr-0007]
    7. Optical sensor according to claim 6, characterized in that the support plate has at least one pair of trenches (925), each pair delimiting on the support plate a so-called isolated area (9711A; 9711B; 9711C; 9711D), receiving one or more elementary waveguides.
    [8" id="c-fr-0008]
    8. Optical sensor according to claim 7, characterized in that the support plate (971A; 971B) has a single pair of trenches.
    [9" id="c-fr-0009]
    9. Optical sensor according to claim 7, characterized in that the support plate (971C) has two pairs of trenches, arranged symmetrical to one another.
    [10" id="c-fr-0010]
    10. Optical sensor according to claim 6, characterized in that the support plate (971D) has a plurality of trenches together delimiting a plurality of symmetrical isolated zones (9711D) in pairs.
    [11" id="c-fr-0011]
    11. Optical sensor according to claim 3 or 4, characterized in that the elementary waveguides (821) are suspended around the pedestal (870), by means of arms (875, 876) which extend in a plane parallel to the plane of the micro-resonator.
    5
    [12" id="c-fr-0012]
    12. Optical sensor (1000; 1000 ') according to claim 1 or 2, characterized in that the elementary waveguides (121) are supported on a substrate (172), without lever arm.
    [13" id="c-fr-0013]
    13. Optical sensor (1000; 1000 '; 5000) according to any one of claims 1
    10 to 12, characterized in that the elementary waveguides (121; 521; 721; 821; 921; 1121) of the micro-resonator are distributed periodically one after the other, in a regular step called step distribution.
    [14" id="c-fr-0014]
    14. Optical sensor according to claim 13, characterized in that the pitch of
    [15" id="c-fr-0015]
    15 distribution (P) is less than:
    λ
    2n h with λ a resonance wavelength of the micro-resonator; and n h the average refractive index of the elementary waveguides.
    类似技术:
    公开号 | 公开日 | 专利标题
    FR3068778B1|2019-08-30|DISPLACEMENT SENSOR WITH SEGMENTED RING MICRO RESONATOR.
    EP3276337B1|2020-09-02|Optical device with segmented-ring micro-resonator
    EP0033048B1|1984-12-05|Interferometer with tunable optical cavity comprising a monomodal optical fibre, and its application to filtration and spectrography
    EP3460547B1|2021-12-15|Optical coupling device for a photonic circuit
    EP3147646A1|2017-03-29|Imaging device with no lens and associated observation method
    FR2613826A1|1988-10-14|INTEGRATED OPTICAL DISPLACEMENT SENSOR
    FR3064078A1|2018-09-21|OPTOELECTRONIC DEVICE FOR GENERATING A FREQUENCY COMB
    FR3050526A1|2017-10-27|ELECTROMAGNETIC RADIATION DETECTION DEVICE WITH ENCAPSULATION STRUCTURE HAVING AT LEAST ONE INTERFERENTIAL FILTER
    EP2027450A1|2009-02-25|Optical component operating in near field transmission
    FR3062209A1|2018-07-27|OPTICAL DETECTOR OF PARTICLES
    EP0647311B1|1997-04-23|Sagnac effect optical gyrometer having a fully integrated structure
    WO2005043205A1|2005-05-12|Frequency selective light coupling and decoupling device
    EP3494381B1|2020-05-20|Absorption cavity with input and output waveguides for a biological or chemical sensor
    EP3447549A1|2019-02-27|Semiconductor structure with suspended membrane under stress comprising an optical cavity
    FR3088119A1|2020-05-08|MEASURING DEVICE BASED ON OPTICAL MEASUREMENT IN AN OPTO-MECHANICAL CAVITY.
    EP3647738A1|2020-05-06|Opto-mechanical resonator with a wave sub-length waveguide
    FR2964795A1|2012-03-16|PHOTODETECTEUR AND CORRESPONDING DETECTION MATRIX
    EP3527967B1|2020-08-12|Acousto-optic detector with opto-mechanical coupling
    EP3486603A1|2019-05-22|System for transducing a displacement into an optical phase shift
    EP3968066A1|2022-03-16|Waveguide comprising a multimode optical fibre and adapted to spatially concentrate the guided modes
    EP3043166B1|2018-11-07|Optical focusing device
    FR2739195A1|1997-03-28|Narrow band optical coupler with round dielectric resonator
    EP3936912A1|2022-01-12|Device for wavelength demultiplexing, in particular for out-of-plane demultiplexing
    EP3575774A1|2019-12-04|Device and method for observing particles, in particular submicron particles
    FR3046853A1|2017-07-21|OPTICAL CAVITY COUPLED OPTICALLY TO A WAVEGUIDE.
    同族专利:
    公开号 | 公开日
    US20190011261A1|2019-01-10|
    EP3425344B1|2021-03-24|
    EP3425344A1|2019-01-09|
    FR3068778B1|2019-08-30|
    US10578437B2|2020-03-03|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US20090220184A1|2008-03-03|2009-09-03|Ramot At Tel-Aviv University Ltd.|Electro-Optical Modulator Structure|
    US20150168441A1|2013-12-13|2015-06-18|Intel Corporation|Optomechanical sensor for accelerometry and gyroscopy|
    US20170146738A1|2015-11-24|2017-05-25|Omega Optics, Inc.|Subwavelength Photonic Crystal Waveguide in Optical Systems|US11073412B2|2018-10-26|2021-07-27|Commissariat A L'energie Atomique Et Aux Energies Alternatives|Subwavelength waveguide opto-mechanical resonator|US55202A|1866-05-29|Improvement in sawing-machines |
    US6665476B2|2000-09-29|2003-12-16|Sarnoff Corporation|Wavelength selective optical add/drop multiplexer and method of manufacture|
    GB201209837D0|2012-06-01|2012-08-29|Univ Bristol|Orbital angular momentum|
    US9863771B2|2013-04-02|2018-01-09|Esa European Space Agency|Optical rotation sensor as well as method of manufacturing an optical rotation sensor|
    FR3054664B1|2016-07-27|2018-09-07|Commissariat A L'energie Atomique Et Aux Energies Alternatives|SEGMENTED RING MICRO RESONATOR OPTICAL DEVICE FOR BIOLOGICAL OR CHEMICAL SENSOR|FR3056306B1|2016-09-20|2019-11-22|Commissariat A L'energie Atomique Et Aux Energies Alternatives|OPTICAL GUIDE HAVING A PSEUDO-GRADIENT INDEX RISE|
    FR3069707B1|2017-07-27|2019-08-30|Commissariat A L'energie Atomique Et Aux Energies Alternatives|INFRARED DEVICE|
    FR3074587B1|2017-12-06|2020-01-03|Commissariat A L'energie Atomique Et Aux Energies Alternatives|PHOTONIC CHIP WITH OPTICAL PATH FOLDING AND INTEGRATED COLLIMATION STRUCTURE|
    FR3077652A1|2018-02-05|2019-08-09|Commissariat A L'energie Atomique Et Aux Energies Alternatives|PHOTONIC CHIP WITH INTEGRATED COLLIMATION STRUCTURE|
    FR3078155B1|2018-02-19|2020-08-14|Commissariat Energie Atomique|PHOTO-ACOUSTIC SENSOR WITH OPTO-MECHANICAL COUPLING.|
    法律状态:
    2019-01-11| PLSC| Publication of the preliminary search report|Effective date: 20190111 |
    2019-07-31| PLFP| Fee payment|Year of fee payment: 3 |
    2020-07-31| PLFP| Fee payment|Year of fee payment: 4 |
    2021-07-29| PLFP| Fee payment|Year of fee payment: 5 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1756293|2017-07-04|
    FR1756293A|FR3068778B1|2017-07-04|2017-07-04|DISPLACEMENT SENSOR WITH SEGMENTED RING MICRO RESONATOR.|FR1756293A| FR3068778B1|2017-07-04|2017-07-04|DISPLACEMENT SENSOR WITH SEGMENTED RING MICRO RESONATOR.|
    EP18181241.3A| EP3425344B1|2017-07-04|2018-07-02|Movement sensor with segmented ring micro-resonator|
    US16/026,535| US10578437B2|2017-07-04|2018-07-03|Displacement sensor with segmented ring microresonator|
    [返回顶部]