• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
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    • 专利摘要:
    Photonic sensor device, method of analysis of samples that makes use of it and uses of said device. Described herein is a sensor device and a method of analyzing samples that makes use of said device, both based on the use of a sub-grouping of guides that is used as a reference together with another sub-grouping of guides that presents a series of windows defined in the waveguides in such a way that there are variations in the evanescence field of each portion of the waveguides of the window, or of the windows in the case of window formations, which is in optical contact through the window with a portion of the sample to analyze. Measurements of such variations with respect to a reference measurement taken from the reference sub-cluster allow the analyte of the sample to be determined and quantified. (Machine-translation by Google Translate, not legally binding)
    公开号:ES2636713A1
    申请号:ES201631544
    申请日:2016-12-02
    公开日:2017-10-06
    发明作者:Pascual Muñoz Muñoz；Bernardo GARGALLO JAQUOTOT；Gloria MICO CABANES；Daniel PASTOR ABELLÁN
    申请人:Universidad Politecnica de Valencia；
    IPC主号:
    专利说明:

    OBJECT OF THE INVENTION
    The present invention is framed in the field of research and analysis of substances by optical means.
    More specifically, the invention relates to a photonic device for spectrometry techniques by means of the use of optical means and an analytical method that makes use of said device.
    BACKGROUND OF THE INVENTION
    In the field of optical devices and photonics devices known as AWG are known by its acronym in English (Arrayed Waveguide Grating). These devices are commonly used as multiplexers or optical demultiplexers in WDM (Wavelength Division Multiplexed) systems. These devices are capable of multiplexing / demultiplexing a large number of wavelengths into a single optical fiber, thereby increasing the transmission capacity of optical networks.
    Conventional AWGs consist of a pair of free propagation zones that act as couplers. Both couplers are connected to each other by a discrete set of waveguides commonly called waveguide clusters (in English, Uarrayed waveguides "or AWs). One or more waveguides are connected to the input of the first coupler and the second. wave that will act as the AWG input and output ports respectively.
    When light is injected through at least one of the input guides, the beam propagates through said waveguide (s) and reaches the first coupler. This acts as a region of free propagation where the light is no longer confined laterally, but diffracts to the opposite side of the coupler. Said diffracted light is collected
    then by the grouping of waveguides (AWs) that have an incremental length between them. Said incremental length is an integer number of times (m) (also known as diffraction order) the wavelength of the light propagated in said guides I1L = m {Ao / nWG {Ao)), AO being the wavelength AWG's central vacuum design and nWG {Ao) is the effective refractive index of the waveguide. This difference in length between adjacent waveguides determines a phase change that therefore depends on the wavelength of the applied light A (which in general may be different from that of design), said change being 11 <jJ = 2 ; nWG (A) (mAo / nwdAo)).
    All these guides are connected to the second coupler where the light coming from each of the guides of the grouping is freely propagated thus obtaining at the exit of the coupler an interference of the fields coming from said guides. In this way, in the output plane we will obtain positions in which the interference occurs constructively and positions in which the interference is destructive. This interference is dependent on the wavelength, due to the relative lag between the light of the clustering guides, 11 <jJ, described above. Those positions where one or more of the wavelengths interfere constructively are known as AWG focal points, and that is where the output waveguides are positioned to pick up the light of one or more wavelengths. In this way, the operation of the complete device consists in separating the different wavelengths introduced by an input guide in different spatial positions and, therefore, in different waveguides, or ports, of output (demultiplexing). Being a passive and reciprocal component, if light signals whose wavelengths have a certain relationship with each other and with the particular design of the AWG are introduced by the different output guides, these wavelengths will be combined in a single port input (multiplexing).
    The use of AWG devices with different functionalities is known in the state of the art, in this sense it is that the document PCT I ES2014 I 070782 describes an AWG reflective assembly provided with Sagnac reflectors in order to minimize the size of the device. In addition, the use of Sagnac reflectors allows the modification of the spectral response of the device, which is typically of the Gaussian type.
    In the doctoral thesis of Dr. ZhixiongHu (Zhixiong "Development of an integrated microspectrometer using Arrayed Waveguide Grating (AWG)" PhD thesis, University of Glasgow) a spectroscopic fluorescence sensor is described. It consists of an AWG and a sample cuvette linked to a micro-fluid chip; This device can only work in fluorescence analysis, not being useful in analyzes based on refractive index or absorption.
    In the case of B. Gargallo, P. Muñoz "Full field model for interleave-chirped arrayed waveguide gratings" Optics Express 2013; 21 (6); 6928-6942 theoretically describes an AWG Interleave-Chirped AWG type device whose grouping of waveguides between couplers is divided into intercalated subgroups, each subgrouping with different physical base length (which depends on the wavelength) and certain incremental length for each sub-grouping. Each sub-group acts independently of the source that each input wavelength to the device can be focused on as many points of the output plane as there are sub-groupings. It is also possible to modify the relative phase between said wavelengths by setting different 1l <fJ for each sub-grouping.
    In K. Kodate, Y. Komai "Compact spectroscopic sensor using an affay waveguide grating" J. Opt. A: Pure Appl. Opt. 2008; 10 (044011) a spectrometric sensor for measuring the spectrum of liquid transmittance is described. The device consists of a common AWG device like the one described above provided with several sample injection slots inside the input coupler acting as detection zones. While in Z. Hu, A. Glidle, C. lronside, J. M. Cooper and H. Yin ': 4n integrated microspectrometer for localized multiplexing measurements "Lab Chip 2015;
    15: 283-289 an AWG spectrometer with lenses for fluorescence measurements is presented. However, although in both cases spectrometric sensors are described, one for the measurement of the transmittance spectrum and the other for fluorescence measurements being both based on AWG devices, in said documents it is detailed that the detection zones of these spectrometers are located, respectively, in one of the couplers of the AWG or in the entrance guide of this one.
    Similarly, document US2006 / 0045412 describes a compact device for the
    Simultaneous interrogation of multiple wavelength modulated fiber optic sensors, which contains a materialized demultiplexer as an AWG element that leads to multiple output waveguides and photo detectors corresponding to the different detection wavelengths. In US2006 / 0045412 the AWG device does not constitute or form part of a sensor device, but is an element associated with the treatment of the signals obtained in the sensors, of a nature not relevant in that invention.
    EP2620753 details an arrangement for the optical determination and analysis of a plurality of optical output signals, each of them of a different wavelength, which is based on an AWG device, which acts as a multiplexer to multiplex in A common signal is the output signals to a receiving unit.
    The optical sensor of US 20120298849 uses parts or surfaces of a waveguide element (a resonator ring) as an evanescent field measuring element when in contact with a substance or affected by some other measurement quantity.
    And finally, document EP1927839 describes an interrogator device of several sensors materialized in optical fiber, in this case for the detection of impacts that, by means of an AWG device, collects and demultiplexes the output signals of the sensors separating them according to their wavelength, towards the respective photodetectors. The AWG device acts as a signal processing device obtained in sensors, and not as a sensor itself, neither as a whole or in parts thereof.
    DESCRIPTION OF THE INVENTION
    In one aspect of the invention there is a photonic sensor device that acts as a spectrometer. This device is based on an AWG (Arrayed Waveguide Grating) which has been modified using interleaving techniques, that is, the waveguide cluster, is divided into interleaved subgroups. , is de-tuned, that is, with different phase relationships within each sub-grouping, giving rise to a DI-AWG (from English "Detuned Interleaved" -AWG), in which at least one of the sub-clusters


    interspersed acts as a sensor.
    The aforementioned interleaved and DI-AWG tuning configuration of two or more mutually outdated waveguide subgroups allows the signal to be replicated at various focal points for the same wavelength. In this way one of the sub-groups is used as a reference and the sub-group (s) attracts (s), which includes (n) detection windows within a surrounding medium such that the light of said sub -grouping may come into contact with a substance present in said medium, (n) is used for the detection I measurement of said substance based on the reference signal. Since the device offers a number of focal points at its output for each wavelength, at least as many as sub-clusters, and that the input light to the device can have multiple wavelengths, the device acts as a spectrometric sensor with multiple configurations
    The substance deposited in the detection windows interacts with the evanescent field of the waveguides, whose particular implementation is detailed below, this interaction being the basis of the detection or analysis that allows the device of the invention to be carried out. Electromagnetic modes guided by dielectric waveguides are not fully confined, but a portion of the propagation mode, whose magnitude depends on the particular implementation of the waveguide, propagates through the region outside the nucleus; This effect gives rise to the known evanescence field, which is in direct contact with the environment surrounding the waveguide. In the case of waveguides that include detection windows, the evanescent field is in direct contact (at least optically) with the medium through the window.
    Therefore, when a substance is in the space included in said window, the sample interacts with the corresponding evanescence field generating alterations in it. Such alterations affect the real, imaginary part, or both, of the effective refractive index of the waveguide (s) for which the window (s) is defined; Variations in the effective refractive index of a waveguide can be measured by quantifying the changes in intensity, phase or polarization of the light observed at the focal points
    previously described, light that is collected in the waveguides or output ports .; the study of said interaction between the light formed by a set of wavelengths, and intensity, phase and polarization determined, and matter, is commonly belonging to the field of spectroscopy, that is why the device object of the invention can be denominate spectrometer. The device of the invention allows to obtain information of the sample in real time when carrying out its inspection when they are in contact, at least optical, through the detection windows so that the phase changes or absorption of the light that Circulating through the guides allow obtaining information on the composition and concentration of the sample at a certain moment, and its evolution over a certain period of time of obselVation
    In another aspect of the invention there is a method of sample analysis that makes use of the photonic sensor device of the invention, while an additional aspect of the invention relates to the use of the device of the invention for spectroscopy, more specifically for spectroscopy. absorption, refraction or fluorescence.
    DESCRIPTION OF THE DRAWINGS
    To complement the description that is being made and in order to help a better understanding of the characteristics of the invention, according to a preferred example of practical realization thereof, a set of drawings is accompanied as an integral part of said description. where, for illustrative and non-limiting purposes, the following has been represented:
    Figure 1.-Shows a diagram of a device of the state of the art.
    Figure 2.- Shows a diagram of the device of the invention.
    Figures 3a, 3b.-It shows in figure 3b a diagram of the device of the invention in operation as a sensor, while in figure 3a the windows of the waveguides of the sub-grouping of detection guides are appreciated, these being and the waveguides of the sub-grouping of reference guides respectively

    referenced
    Figure 4.- It shows in figure 4 a diagram of the device of the invention in operation as a sensor operating in reflective mode.
    Figures 5a, 5b.-It shows in figure 5b a diagram of the device of the invention in operation for absorption spectroscopy, while in figure 5a the waveguides of the sub-grouping of detection guides marked as
    absorbent material from which they are made.
    Figures 6a, 6b.-Shows in figure 6b a diagram of the device of the invention in
    operation for refractive spectroscopy, while in figure 6a the waveguides of the sub-grouping of detection guides marked as refractive material from which they are made are appreciated.
    Figures 7a, 7b - It shows in figure 7b a diagram of the device of the invention in operation for fluorescence spectroscopy, while in figure 7a the waveguides of the sub-grouping of detection guides marked as fluorescent material are appreciated.
    PREFERRED EMBODIMENT OF THE INVENTION
    In a preferred embodiment of the device (1) object of the first aspect of the invention shown in Figure 2, there is an AWG (Array Waveguide Grating) photonic sensor device (1) which comprises a plurality of waveguides
    (2) where at least one sub-grouping of reference guides (24) is defined, and at least one sub-grouping of detection guides (23) whose wave guides (2) comprise at least one optical window (21) defined in a section of waveguides (22). Said device (1) is complemented by an optical input coupler (3) and an optical output coupler (4) connected to each other by means of waveguides (2), and they are also respectively connected to input waveguides. (31) And some output waveguides (41). The couplers (3,4) can be of various types, preferably Dragone type free space couplers, star couplers, multimode type couplers ("multimode type"
    interference, MMI ") Or couplers based on gradual index guides. Preferably, the waveguides (2) are flat guides, cylindrical guides, groove guides, bimodal guides, or sub-wavelength guides, comprising sections that may be straight, curved and / or spiral, of a transparent material at the working wavelengths 5, comprising Indian, Silicon or Germanium Phosphide, preferably Silicon or Silicon Nitride, and it is preferred that the waveguides (2) have incremental lengths, so that even waveguides (.ó.Le) and
    Odd waveguides (lJ. Lo) follow the following equations:
    • .ó.Le = m Ao / nWG; where m is an integer, AO is the center wavelength and nWG is the refractive index of the waveguide (2), and
    • .ó.Lo = .ó.Le + lJ .; such that the even waveguides (.ó.Le) and the odd waveguides (l! .Lo) define the respective sub-groupings (23, 24), where or. it is determined such that each sub-grouping (23, 24) produces a lag
    different for the same wavelength.
    The device of the invention is completed with a light radiation source (5)
    associated to the optical input coupler (3) to generate a signal, and a network of
    detectors connected to the optical output coupler (4).
    The configuration defined in the previous section can be implemented in a possible
    preferred embodiment of the invention that can be seen in Figure 3, where the
    subgroups (23,24) are optically out of date with each other, so that
    when a light of one or more wavelengths one or more wavelengths,
    25 At. A2. A3 • ..., AN where At> A2> A3> ...> AN, is fed into one of the input waveguides (31), said light is separated in the output waveguides (41), in virtue of the wavelength.
    The input guides (31) are fed by the light source (5) of
    30 such that the light is divided by the optical input coupler (3) and distributed to the plurality of waveguides (2) that interconnect the couplers (3,4). The light passing through the waveguides (2) of the subgroup of reference guides
    (24) undergoes the alteration due exclusively to those waveguides (2) of said subgroup of reference guides (24), while the light passing through those
    35 waveguides (2) of the sub-grouping of detection guides (23) are altered by the properties of an analyte in contact with the windows (21) defined in the waveguide sections (22) of the waveguides. wave (2) of the sub-grouping of guides
    detection (23).
    The plurality of waveguides (2) feeds the optical output coupler (4) so that the combination of said optical output coupler (4) and the alterations experienced by light in the subgroups (23,24) allows that the light passing through those waveguides (2) of the sub-grouping of reference guides (24) focuses on a subset of reference output guides (41 1), while the light of the sub-grouping of detection guides (23) focuses on a subset of detection output guides (412), these subsets of output guides (411, 412) being disjoint or overlapping.
    The device (1) can operate in transmission mode or in reflection mode, in the latter mode the waveguides (2) are truncated, preferably at a midpoint of their optical length, and are equipped with reflectors located at the ends generated when cutting the waveguides (2), said reflectors are preferably Sagnac type, (in English "Sagnac Loop Ref1ector '~ SLR).
    In an alternative embodiment of the device (1) of the first aspect of the invention corresponding to the reflection mode, the device (1) has to be operated in reflective mode (R-AWG) using Sagnac reflectors and using a single coupler (3, 4). The subgroups (23,24) are connected on one side to the coupler (3,4), and on the other it is terminated with SLR reflectors, one for each waveguide (2) of the grouping.
    In a second aspect of the invention there is a method for carrying out biological material analysis, or sample analysis, method in which the output waveguides (41) are connected to detectors, thus when an optical field, composed of one
    or more wavelengths, A_1, A_2,), _ 3, .. LA] _N, such that A_1> A_2> A_3> ···> A_N, enters one of the input waveguides (31), said field optical is separated in the output waveguides (41), by virtue of the wavelength, a part thereof in the waveguides (2) of the sub-grouping of reference guides (24) (A_i i = 1 .. N) And another part in the waveguides (2) of the sub-grouping of detection guides (23) (Aj "i = 1..N), so that the signal of the same wavelength it is present in at least one waveguide (2) of the subgroup of reference guides (24) and
    also in at least one waveguide (2) of the subgroup of detection guides (23). Since the field of guides of the sub-group of detection guides (23) comes from those wave guides (2) of the sub-group of detection guides
    (2. 3) that is exposed to the analyte can be obtained at the same time, and spatially separated, the reference and the sensing signal for all wavelengths of the optical input field.
    In an alternative embodiment of the second aspect of the invention, a device (1), with a plurality of waveguides (2) interconnecting a single coupler (3,4), with a set of reflectors (7), of way that the device works in reflection. The radiation source (5) connected to the input waveguides (31) feeds the coupler (3,4) that divides the light into the plurality of waveguides (2). The operation of the sub-groupings (23,24) is analogous to that of the main embodiment, except that the light travels one way from the single coupler (3,4) to the mirrors (7) and back, from them back to the same single coupler (3,4). The combination of said single coupler (3,4) and the alterations experienced by the light in the subgroups (23,24) has the effect analogous to the main embodiment. The configuration of the detectors in this particular embodiment is similar, being located in this particular embodiment, but not necessarily, in two subsets of guides (411, 412): the subset of reference output guides
    (411) and the subset of detection output guides (412) around an inner waveguide (413) to which the radiation source (5) is connected.
    In a possible more preferred embodiment of the second aspect of the invention in which an application of the invention is carried out in tasks of absorption spectroscopy and which is shown in Figure 5a with a configuration like that shown in Figure 5b, when a field optical, consisting of one or more wavelengths, A_1), _ 2) _ 3, .. LA] _N such that A_1> A_2> A_3> ···> A_N, is fed into at least one of the waveguides of input (31), said optical field is separated in the output waveguides (41), by virtue of the wavelength, a part thereof in the reference output guides (41 1) (A_i i = 1. .N) And another part in the detection output guides (412) (A_i ..... i = 1 .. N), so that the signal of the same wavelength is present in at least one of the reference output guides
    (411) and also in at least one detection output guide (412). In this particular embodiment, the light passing through the waveguides (2) of the subgroup of detection guides (23) is altered by the absorbent properties of the analyte in the windows (21), preferably of equal length each, defined in the waveguide sections (22). The relative absorption of the analyte for each wavelength is determined by comparing the amount of light between the reference output guides (411), whose amount of light is not altered by the analyte, with the light in the guides detection output (412), which comes from the sub-grouping of detection guides (23) if it is in interaction with the anal ita, and therefore, may present a change in its intensity. Said comparison is preferably made, but not in a restricted way, in pairs, that is, ,, _ i with ,, _ i '"for i = l ... N.
    In an even more preferred embodiment, the application of the invention is applied in refractive spectroscopy techniques, as seen in Figure 6a with a configuration like that shown in Figure 6b. In this embodiment when an optical field, consisting of one or more wavelengths, "_1," _ 2, "_ 3, ... K,"] _ N such that A_1> "_ 2>" _ 3> ···> "_ N , is fed into at least one of the input waveguides (31), said optical field is separated in the output waveguides (41), by virtue of the wavelength, a part thereof in the guides reference output (4 11) (,, _ i i = l .. N) And another part in the detection output guides (412) (,, _ i '"i = l .. N), so that the signal of the same wavelength is present in at least one reference output guide (411) and also in at least one detection output waveguide (412). In this particular embodiment, the light passing through the waveguides
    (2) of the sub-grouping of detection guides (23) is altered by the refractive properties of the analyte in the windows (21), being able to be in this embodiment of different length, defined in the waveguide sections (22) .
    The length of the consecutive waveguide windows (21) (2) in the subgrouping of detection guides (23), in a particular embodiment, may be the same or differ by a constant amount. This enables the interaction of light with the analyte in the waveguides (2) of the sub-grouping of detection guides (23) undergoes a linear offset between waveguides (2) due to the refractive properties of the analyte. Therefore, the wavelengths (,, _ i '"i = l .. N) are shifted from their initial positions, and the amount of light detected in the detection output guides (412) changes. By comparing preferably, but not in a restricted way, in pairs, that is ,, _ i with ,, _ il 'for i = 1 .. N, you can determine the amount of wavelength shift (,, _ V "i = 1 .. N), and therefore the change in refractive index due to analyte.
    In an even more preferred embodiment, the invention is applied in fluorescence spectroscopy techniques such as the one shown in Figure 7a with a configuration like that shown in Figure 7b, in which when an optical field, consisting of a or more wavelengths, _ 3,), _ 4 such that, _ 3>, _ 4, is fed into at least one of the input waveguides (2) (31), said optical field travels through the guides wave (2) of the reference sub-grouping (24), and by the waveguides (2) of the sub-grouping of detection guides (23), in which windows (21) are defined, preferably of equal length for each waveguide (2) and defined in the waveguide sections (22). When an analyte with fluorescent properties is presented in said windows (21), the wavelengths of the input fed optical field are absorbed by the analyte, and the energy thereof is emitted at longer wavelengths, by the phenomenon of fluorescence, 1._ ', 1, _2 in the simplified example of Figure 7b, where A_'> A_2> A_3> K> AL 4. The short wavelengths of the input, coming from the waveguides (2) of the sub-grouping of reference guides (24) are projected and separated in the reference output guides (41 1), while the long wavelengths emitted by fluorescence in the analyte and collected by the waveguides ( 2) of the subgrouping of detection guides (23) are projected and separated in the detection output guides (412). The measurement and comparison of the light intensities of the reference output guides (411) and the detection output guides (412) makes it possible to compose the spectrum of the radiation source (5) and the fluorescence produced in the analyte.
    As can be seen from reading the details of the second aspect of the invention, the device of the first aspect of the invention can be used for absorption spectroscopy, for refraction spectroscopy or for fluorescence spectroscopy. These uses being a third aspect of the invention.
    In that second aspect of the invention referred to the method of analysis of samples that makes use of the photonic sensor device of the first aspect the invention, it is necessary
    The method is based on contacting the sample with the waveguide sections (22) exposed through the window (s) (21), to subsequently circulate the signal from the radiation source (5) through the input coupler (3) to the waveguides (2), then being able to measure in the output coupler (4) data of the light radiation corresponding to the signal that has passed through the waveguides (22) of the reference subgrouping (24) - these data can be power, phase and polarization of the light radiation - and the waveguides (22) of the detection subgroup (23) whose sections of waveguides (22) comprise the minus an optical window (21). With this, at least one of the presence, concentration and distribution of analyte in the sample can be determined from the measurements carried out.
    In the second aspect of the invention, the sample analysis may comprise absorption spectroscopy techniques, refractive spectroscopy techniques or fluorescence spectroscopy techniques.
    When the analysis is carried out by fluorescence spectroscopy techniques, such as those shown in Figures 7a and 7b, it is necessary to feed at least one of the input waveguides (2) (31) an optical field composed of a
    or more wavelengths, "_3) _ 4 such that" _3> "_ 4, causing said optical field to travel through the waveguides (2) of the reference sub-grouping (24), and by the waveguides (2) of the sub-grouping of detection guides (23), in which windows (21) are defined, to subsequently contact in said windows (21) an analyte with fluorescent properties, such that those wavelengths of the optical field are absorbed by the analyte, and their energy is emitted at longer wavelengths, by the phenomenon of fluorescence, so that the short wavelengths of the input, coming from the waveguides (2 ) of the subgrouping of reference guides (24) are projected and separated in the reference output guides (41 1), while the long wavelengths emitted by fluorescence in the analyte and collected by the waveguides (2) of the sub-grouping of detection guides (23) are projected and separated in the detection output guides (412). This done, it is necessary to measure and compare the light intensities of the reference output guides (411) and the detection output guides (412), to later compose the spectrum of the radiation source (5) and the fluorescence produced In the analyte.

    权利要求:
    Claims (14)
    [1]
    1. Device (1) photonic sensor based on AWG (Arfay Waveguide Grating) characterized by comprising:
    • a plurality of waveguides (2) that define:
    • at least one reference sub-grouping (24), and
    • at least one detection subgroup (23) whose waveguides (2) comprise at least one optical window (21) defined in a section of waveguides (22),
    the subgroups (23,24) being optically out of date with each other,
    • an optical input coupler (3) and an optical output coupler (4) connected to each other by the waveguides (2),
    • a light radiation source (5) associated with the optical input coupler (3) to generate a signal, and
    • a network of detectors connected to the optical output coupler (4).
    [2]
    2. Sensor photonic device (1) according to claim 1 characterized in that the couplers (3,4) are selected from: Dragone type free space couplers, star couplers, multimode type couplers ("MMn multimode interference and index guide based couplers" gradual.
    [3]
    3. Sensor photonic device (1) according to claim 1 characterized in that the waveguides (2) are selected from: flat guides, cylindrical guides, groove guides, bimodal guides and sub-wavelength guides, comprising sections that can be straight , curved or spiral.
    [4]
    Four. Sensor photonic device (1) according to claim 1 characterized in that the waveguides (2) have incremental lengths, such that the even waveguides (l! .Le) and the odd waveguides (l! .Lo) follow The following equations:
    • l! .Le = m Ao / nWG, where m is an integer, AO is the center wavelength and nWG is the refractive index of the waveguide (2), and

    • l1Lo = l1Le + .ó; in such a way that even waveguides
    (l1Le) and odd waveguides (l1Lo) define the
    respective sub-groupings (23, 24), where 6 are
    determines such that each sub-grouping (23, 24) produces a
    different lag for the same wavelength.
    [5]
    5. Photonic sensor device (1) according to claim 1 characterized in that the waveguides (2) of the subgroups (23,24) have different focal points for the same wavelength, so that the signal generated by the radiation source
    (5) when passing through the respective waveguides (2) it replicates at different points of
    exit.
    [6]
    6. Sensor photonic device (1) according to any one of the preceding claims characterized in that the waveguides (2) are made of a material transparent to the working wavelengths and comprising Indian, Silicon or Germanium Phosphide, preferably Silicon or Silicon Nitride
    [7]
    7. Method of analysis of samples using the device (1) described in any one of claims 1 to 6, a method characterized in that it comprises the following steps:
    • contact the sample with the waveguide sections (22) exposed through at least one of the windows (21),
    • circulating a signal from the radiation source (5) through the input coupler (3) to the waveguides (2), and
    • measure in the output coupler (4) a light radiation corresponding to the signal that has passed through:
    • the waveguides (22) of the reference sub-grouping (24), and
    • the waveguides (22) of the detection subgroup (23) whose sections of waveguides (22) comprise optical window (21), and
    • determine at least one of: presence, concentration and distribution of analyte in the sample from the measurements carried out in the previous step.
    [8]
    8. Sample analysis method according to claim 7 characterized in that the measurement is carried out in the optical output coupler (4) and comprises measuring at least one of: power, phase and polarization of the light radiation.
    [9]
    9. Sample analysis method using the device (1) described in any one of claims 1 to 6 wherein the sample analysis comprises absorption spectroscopy techniques.
    [10]
    10. Method of sample analysis using the device (1) described in any one of claims 1 to 6 wherein the sample analysis comprises refractive spectroscopy techniques.
    [11]
    eleven. Method of sample analysis using the device (1) described in any one of claims 1 to 6 wherein the sample analysis comprises fluorescence spectroscopy techniques, the method being characterized in that it comprises:
    • feed into at least one of the input waveguides (31), an optical field, consisting of one or more wavelengths, "_3 ,,, _ 4 such that ,, _ 3> ,, _ 4, causing said optical field travel by the waveguides (2) of the reference sub-grouping (24), and by the waveguides (2) of the sub-grouping of detection guides (23), in which the windows are defined (twenty-one),
    • contacting in said windows (21) an analyte with fluorescent properties, such that those wavelengths of the optical field are absorbed by the analyte, and their energy is emitted at longer wavelengths due to the fluorescence phenomenon , so that the short wavelengths of the input, coming from the waveguides (2) of the subgroup of reference guides (24) are projected and separated into the reference output guides (411), while that the long wavelengths emitted by fluorescence in the analyte and collected by the waveguides (2) of the subgroup of detection guides (23) are projected and separated in the detection output guides (412),
    • measure and compare the light intensities of the exit guides of
    reference (41 1) And the detection output guides (412), and
    • compose the spectrum of the radiation source (5) and the fluorescence produced in the analyte.
    [12]
    12. Use of the device described in any one of claims 1 to 6 for absorption spectroscopy.
    [13]
    13. Use of the device described in any one of claims 1 to 6 for 10 refractive spectroscopy.
    [14]
    14. Use of the device described in any one of claims 1 to 6 for fluorescence spectroscopy.
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    同族专利:
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    WO2018100223A1|2018-06-07|
    ES2636713B2|2018-05-18|
    引用文献:
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    JP2000028526A|1998-07-13|2000-01-28|Nippon Telegr & Teleph Corp <Ntt>|Refractive index measuring method and refractive index measuring device|
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    US20060132764A1|2004-12-16|2006-06-22|Andevices, Inc.|Integrated optics based high-resolution spectrophotometer|
    EP2450693A1|2010-11-08|2012-05-09|Nederlandse Organisatie voor toegepast -natuurwetenschappelijk onderzoek TNO|An arrayed waveguide grating |
    CN109632657A|2019-02-26|2019-04-16|京东方科技集团股份有限公司|Spectrum detection device|
    CN110031466A|2019-04-25|2019-07-19|山东大学|A kind of contact-type linear concentration sensor and its fluid detection method based on array wave-guide grating structure|
    CN112305668A|2020-10-21|2021-02-02|浙江大学|Array waveguide grating with double-layer structure|
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