JP2017215344A - Specimen sensor and specimen sensing method - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a specimen sensor capable of measuring characteristics of a specimen or a target included in the specimen and achieving both of measurement of a wide phase range and low current consumption with small size, and a specimen sensing method.SOLUTION: A specimen sensor acquires a phase shift value by a heterodyne method from a detection signal and a reference signal obtained from: a detection element 110 for outputting the detection signal according to mass change in a detection unit 111; and a reference element 120 for outputting the reference signal according to mass of a reference unit 121. Thereby, the specimen sensor calculates a target detection amount.SELECTED DRAWING: Figure 1

Description

  The present invention relates to a sample sensor and a sample sensing method capable of measuring a property of a sample or a target contained in the sample.

  2. Description of the Related Art A surface acoustic wave sensor that uses a surface acoustic wave element to measure a property of a liquid as a specimen or a liquid component is known.

  A surface acoustic wave sensor has a detection unit that reacts with a component contained in a specimen sample on a piezoelectric substrate, and measures an electrical signal based on a change in a surface acoustic wave (SAW) propagated through the detection unit. Thus, the property or component of the liquid as the specimen is detected (for example, Patent Document 1).

  The SAW sensor disclosed in Patent Document 1 measures the analyte concentration by detecting the SAW phase difference. In order to measure the phase difference, a quadrature modulation method is generally employed because of the wide range of measurable phase ranges (for example, Non-Patent Document 1).

JP 2008-122105 A

"Development of SAW oscillator integrated SAW sensor system", IEICE Technical Report, IEICE, February 2003

  However, the quadrature modulation method has a problem that it is difficult to reduce the size because of the large number of parts for realizing it. Furthermore, there is a problem in that current consumption increases due to an increase in digital processing.

  Therefore, there is a need for a specimen sensor and a specimen sensing method that can be miniaturized and consume low current.

  An analyte sensor according to an embodiment of the present invention includes a detection unit that changes in mass according to adsorption of a target contained in a sample or reaction with the target, and is an AC signal according to a change in mass of the detection unit. A detection element that outputs a detection signal, a reference unit that does not adsorb the target or does not react with the target, a reference element that outputs a reference signal that is an AC signal for the detection signal, the detection signal, and the reference signal Of the first signal and the second signal, the other signal is branched to the third signal and the fourth signal, and the first signal and the third signal are heterodyne. The phase difference from the first measurement signal is different from the first calculation signal for obtaining the first measurement signal by the method and the heterodyne method from the second signal and the fourth signal (± 180 °). A second calculation unit that obtains a second measurement signal, two first phase change candidate values are calculated from the first measurement signal, and two second phase change candidate values are calculated from the second measurement signal. A measuring unit that sets a combination of the two first phase change candidate values and the two second phase change candidate values that are closest to each other as a first phase change value and a second phase change value; A selection unit that selects, as a phase change value, a signal output value closer to a reference value among the first phase change value and the second phase change value;

  In the analyte sensing method according to an embodiment of the present invention, the detection unit of the detection element, in which the mass of an analyte solution containing an analyte with a target changes according to the adsorption of the target or the reaction with the target, and the target A sample solution supply step for supplying to a reference portion of a reference element that does not adsorb or react with the target, a detection signal that is an AC signal according to a change in mass of the detection portion that is output from the sample detection element, and One of the reference signals, which is an AC signal corresponding to the mass of the reference section output from the reference element, is branched into a first signal and a second signal, and the other signal is divided into a third signal and a fourth signal. A branching process for branching to the first signal, a first calculation process for obtaining a first measurement signal from the first signal and the third signal by a heterodyne method, the second signal and the previous signal A second calculation step of obtaining a second measurement signal having a phase difference different from the first measurement signal (excluding ± 180 °) from the fourth signal by a heterodyne method; and two first phase changes from the first measurement signal Candidate values are calculated, two second phase change candidate values are calculated from the second measurement signal, and the two first phase change candidate values and the two second phase change candidate values are closest to each other. A measurement step in which a combination is formed as a first phase change value and a second phase change value, and the phase change value of the first measurement signal and the second measurement signal whose signal output value is closer to a reference value And a selection step of selecting as.

  According to the analyte sensor and the analyte sensing method according to the embodiment of the present invention, it is possible to combine measurement in a wide phase range with small size and low current consumption.

1 is a principle configuration diagram of an analyte sensor according to a first embodiment of the present invention. It is a schematic diagram explaining the signal processing of a heterodyne system. FIG. 3A is a diagram showing a schematic trajectory of the first measurement signal and the second measurement signal, and FIG. 3B is a diagram showing a trajectory of the selected measurement signal. It is a perspective view of the sample sensor concerning a 1st embodiment of the present invention. FIG. 5 is a perspective view of a state in which a part of the specimen sensor shown in FIG. 4 is broken. 6A is a cross-sectional view taken along the line VIa-VIa in FIG. 4, and FIG. 6B is a cross-sectional view taken along the line VIb-VIb in FIG. FIG. 5 is a top view excluding a part of the specimen sensor shown in FIG. 4. It is a fundamental block diagram of the sample sensor which concerns on 2nd Embodiment of this invention. It is a fundamental lineblock diagram of the sample sensor concerning other embodiments of the present invention. FIG. 9A is a diagram showing a sample sensor according to another embodiment of the present invention, and FIG. 9A is a diagram showing trajectories of the first measurement signal, the second measurement signal, and the third measurement signal, and FIG. ) Is a diagram showing a trajectory of a selected measurement signal. It is a fundamental lineblock diagram of the sample sensor concerning other embodiments of the present invention.

  Hereinafter, an embodiment of an analyte sensor according to an embodiment of the present invention will be described in detail with reference to the drawings. In addition, in each drawing demonstrated below, the same code shall be attached | subjected to the same structural member. Further, the size of each member, the distance between members, and the like are schematically illustrated, and may differ from actual ones.

  In addition, the analyte sensor may be set in any direction upward or downward, but in the following, for convenience, the orthogonal coordinate system xyz is defined and the positive side in the z direction is defined as the upper side and the lower side. The following terms shall be used.

<Sample sensor>
(First embodiment)
(Sample sensor 100)
FIG. 1 is a schematic diagram for explaining the principle of the analyte sensor 100.

  As shown in FIG. 1, the analyte sensor 100 includes a detection element 110, a reference element 120, a branching unit 130, a calculation unit 140, a measurement unit 150, a selection unit 160, and a detection amount calculation unit 170. Have.

(Detecting element 110)
The detection element 110 has a detection unit 111 that adsorbs a target present in the specimen or changes its mass in accordance with the reaction with the target. For example, the detection unit 111 immobilizes a reactive group having a reactivity that specifically adsorbs a target on a gold (Au) film that is not affected by electrical properties such as the conductivity of the specimen. Can be realized. Note that the target itself may not be adsorbed. For example, a reactive group having a property that reacts with a target and does not react with a substance other than the target present in the specimen may be immobilized on the Au film. The Au film is desirably electrically grounded. With such a configuration, the mass of the detection unit 111 changes according to the amount of the target.

(Reference element 120)
The reference element 120 includes a reference unit 121 that does not adsorb a target or does not react with the target. For example, the reference unit 121 does not have such a reactivity as to be specifically adsorbed to a target present in the specimen or cause a substitution reaction with a substance in the specimen by causing a structural change. is there. Specifically, the Au film not having the above reactive group immobilized thereon, or the DNA, RNA, etc. having the same amount of substance as the above reactive group and having a random base sequence are immobilized on the Au film. Can be used. With such a configuration, it is possible to suppress the reference unit 121 from causing a mass change depending on the amount of the target.

  An input signal is applied to the detection element 110 and the reference element 120 from the outside. An input signal given to the detection element 110 passes through the detection unit 111 and is output as a detection signal through a change corresponding to a mass change of the detection unit 111. Similarly, an input signal given to the reference element 120 passes through the reference unit 121 and is output as a reference signal through a change corresponding to the mass of the reference unit 121.

  Here, the detection signal and the reference signal are AC signals, and the reference signal serves as a reference signal for the detection signal.

(Branch 130)
The branching unit 130 includes a first branching unit 131 and a second branching unit 132. The first branch unit 131 is connected to the detection element 110 and branches a detection signal corresponding to a mass change of the detection unit 111 of the detection element 110 into a first signal and a second signal. Here, the first signal and the second signal are signals having the same phase. That is, the detection signal is branched into two identical signals A.

  The second branching unit 132 branches the reference signal from the reference element 120 into a third signal and a fourth signal. The third signal has the same phase as the first signal. The fourth signal is shifted in phase from the first signal by a value excluding 180 °. In this example, the phase is shifted by 90 °. In FIG. 1, the third signal is represented by B and the fourth signal is represented by B ′.

  Such a 1st branch part 131 and the 2nd branch part 132 are comprised with a splitter, for example. The second branching unit 132 may be realized by branching a signal into two by a normal method and then making one line length different from the other line length.

(Calculation unit 140)
The calculation unit 140 includes a first calculation unit 141 and a second calculation unit 142.

  The first calculator 141 obtains a first measurement signal from the first signal A and the third signal B by a heterodyne method. In this example, the first calculator 141 obtains a first measurement signal that is a value obtained by subtracting the third signal B from the first signal A by the heterodyne method.

  The second calculator 142 obtains a second measurement signal from the second signal A and the fourth signal B ′ by a heterodyne method. In this example, the second calculation unit 142 obtains a second measurement signal that is a value obtained by subtracting the fourth signal B ′ from the second signal A by the heterodyne method.

  The first calculation unit 141 and the second calculation unit 142 are configured by, for example, a mixer and a low-pass filter.

(Measurement unit 150)
The measurement unit 150 calculates two first phase change candidate values from the first measurement signal, and determines one of them as the first phase change value. Similarly, two second phase change candidate values are calculated from the second measurement signal, and one of them is determined as the second phase change value.

  Here, since the first measurement signal and the second measurement signal are processed by the heterodyne method, as shown in FIG. 2, the first measurement signal and the second measurement signal are sinusoidal, and the voltage intensity (output value). There are two values x1 and x2 in the phase change value candidate corresponding to y1. This candidate value for phase change indicates the phase difference between the detection signal and the reference signal.

  Considering the first measurement signal and the second measurement signal, there are two first phase change candidate values x11 and x21 for the first measurement signal. Similarly, there are two second phase change candidate values x12 and x22 for the second measurement signal. Here, the combination of x11 and x12, the combination of x11 and x22, the combination of x21 and x12, and the combination of x21 and x22 has the closest value (phase difference value). The phase change candidate values that are combined with each other are set as the first phase change value of the first measurement signal and the second phase change value of the second measurement signal, respectively. Specifically, a difference is obtained for four combinations, and a combination having the smallest value is selected. Then, the phase change candidate values forming the selected combination are set as the first phase change value of the first measurement signal and the second phase change value of the second measurement signal, respectively. This is due to the following mechanism.

  That is, theoretically, one of the two first phase change candidate values of the first measurement signal is the same as one of the two second phase change candidate values of the second measurement signal. This same value is the correct phase change value (first phase change value, second phase change value). However, in the first and second measurement signals of actual measurement, there is a possibility that the same value cannot be taken due to an error. Therefore, the combination that minimizes the difference (that is, the one that takes the closest value) is discriminated as the first phase change value and the second phase change value.

  Conventionally, when signal processing is performed by the heterodyne method, there are two phase change candidate values, which makes it difficult to discriminate, and as a result, the measurable phase range has become very small. However, in the present embodiment, the phase change value can be determined from the phase change candidate value by using the two detection signals (first and second detection signals) as described above.

(Selection unit 160)
The selection unit 160 selects one of the first measurement signal and the second measurement signal as a measurement signal used in the subsequent detection amount calculation unit 170. Similarly, if the measurement signal selected is the first measurement signal, the first phase change value is selected as the phase change value. If the second measurement signal is selected, the second phase change value is selected as the phase change value.

  Specifically, the following steps are performed. First, the trajectory between the first measurement signal and the second measurement signal is obtained in advance, and two positive and negative intensities at the intersection of the first measurement signal and the second measurement signal are obtained. Then, the first measurement signal and the second measurement signal that are located between two positive and negative intensities at the intersection are selected as measurement signals.

  FIG. 3A is a diagram illustrating the locus of theoretical values of the first measurement signal and the second measurement signal. For convenience, the intensity of the first measurement signal is set to V1, the intensity of the second measurement signal is set to V2, and the intensity of the intersection of the locus of the first measurement signal and the locus of the second measurement signal is set to Vmax and Vmin in descending order. . The locus of the first measurement signal is indicated by a broken line, and the locus of the second measurement signal is indicated by a solid line. Theoretically, the intersection strengths Vmax and Vmin are 0.5 times and -0.5 times the maximum strength of V1 and V2.

  A phase value section is divided for each phase value at which the first measurement signal and the second measurement signal have an intensity at any intersection. In FIG. 3A, sections 1 to 5 are shown. Note that the sections 1 to 4 are repeated, and the sections 1 and 5 are the same. Then, the second measurement signal is used as the measurement signal in section 1, the first measurement signal in section 2, the second measurement signal in section 3, the first measurement signal in section 4, and the second measurement signal in section 5. select.

  When the first measurement signal is a measurement signal, the first phase change value is a phase change value, and when the second measurement signal is a measurement signal, the second phase change value is a phase change value.

  In other words, it is as follows.

V1> V2, and V1> Vmax ... V2 is used as the measurement signal V1 <V2, and V2> Vmax ... V1 is used as the measurement signal V1 <V2, and V1 <Vmin ... V2 is used as the measurement signal Adoption V1> V2, and V2 <Vmin... V1 is adopted as the measurement signal. If V1 = V2, either may be adopted as the measurement signal. The trajectory of the measurement signal selected in this way is shown in FIG.

  A phase change value can also be selected according to the measurement signal selected according to the above-described conditions.

(Detection amount calculation unit 170)
Next, the detection amount calculation unit 170 calculates the detection amount of the specimen using the phase change value selected through the above-described process. The detection amount calculation unit 170 is connected to the selection unit 160.

  By configuring as described above, it is possible to provide the sample sensor 100 capable of calculating the detection amount of the target included in the sample.

  Since the sample sensor according to the present embodiment processes the signal by the heterodyne method, the sample detection amount can be calculated only by adding a mixer that takes the difference between the detection signal and the reference signal. For this reason, complicated signal processing is not required as compared with the orthogonal modulation method used conventionally, the number of necessary components is small, miniaturization is possible, and current consumption can be suppressed.

  Further, since the normal heterodyne method cannot determine whether the phase value is positive or negative, the measurable phase range is only from 0 ° to 180 °. However, according to the sample sensor 100 of the present embodiment, the first measurement signal and the second measurement signal are compared with the first and second phase change candidate values, so that the sign of the phase from the phase change candidate value is determined. Judgment can be made and the phase change value can be estimated. Thereby, the measurable phase range can be expanded from −180 ° to 180 °.

  Then, by continuously following the change in voltage intensity between the first measurement signal and the second measurement signal, measurement is possible even in a phase range exceeding 180 °.

  Further, in the normal heterodyne system, since a sinusoidal curve is drawn, the inclination becomes small when the phase difference is 0 ° and ± 180 °, and there is a possibility that the sensitivity is lowered and the error is increased. On the other hand, by adopting the above-described configuration, a region where the inclination is small is omitted, and a measurement signal having a large inclination in all phase ranges is used. Thereby, the voltage change rate can be high with respect to the phase change, and the analyte sensor 100 with high sensitivity can be obtained. In the specimen sensor, the vicinity of 0 ° is particularly effective because it often corresponds to a rising portion of a signal change due to target detection and it is desired to measure with high sensitivity.

  In particular, in the above-described example, the second measurement signal has the highest sensitivity when the first measurement signal has the lowest sensitivity because the fourth signal is shifted by 90 ° with respect to the first to third signals. Since it becomes an area | region, it can be set as the highly sensitive analyte sensor 100. FIG.

  In the above example, the reference signal is branched into the third signal and the fourth signal with the phase shifted, but the detection signal may be branched into the third signal and the fourth signal. Moreover, although the example which shifted the phase of the 4th signal 90 degrees with respect to the 1st signal was demonstrated as the most effective example, as long as it is a value except 180 degrees, other than 90 degrees may be sufficient.

  Furthermore, noise determination can be performed by using two measurement signals (first measurement signal and second measurement signal) as described above. This is due to the following mechanism. Noise may be mixed in the detection signal and the reference signal. Usually, it is difficult to distinguish such noise from noise. On the other hand, according to the sample sensor 100 of the present embodiment, when the measurement is correctly performed, one voltage strength of the first measurement signal and the second measurement signal is in a range between the intersection strengths Vmax and Vmin. Enter a value that falls within the range of the other. In other words, if both the first measurement signal and the second measurement signal take a value within this range or take a value outside this range, it can be determined to be noise. Since noise can be discriminated in this way, the analyte sensor 100 capable of accurate measurement without being affected by noise can be obtained.

  As described above, it is possible to provide the analyte sensor 100 that can detect the phase range having the same width as that of the quadrature modulation method with high accuracy with a small number of parts and a small signal processing.

(Configuration of specimen sensor 100A)
Next, the configuration of the sample sensor 100A according to the first embodiment of the present invention, which embodies the principle of the sample sensor 100, will be described with reference to FIG.

  As shown in the perspective view of FIG. 4, the specimen sensor 100 </ b> A mainly includes a piezoelectric substrate 1 and a cover 3 in appearance. The cover 3 is provided with a first through hole 18 that is an inlet of the sample solution and an air hole or a second through hole 19 that is an outlet of the sample solution.

  FIG. 5 shows a perspective view of the sample sensor 100A when one half of the cover 3 is removed. As shown in the figure, a space 20 serving as a sample flow path for a sample (solution) is formed inside the cover 3. The first through hole 18 is connected to the space 20. That is, the specimen entering from the first through hole 18 flows into the space 20.

  The sample liquid that has flowed into the space 20 includes a target, and the target reacts with a detection unit made of the metal film 7 or the like formed on the piezoelectric substrate 1.

The piezoelectric substrate 1 is made of, for example, a single crystal substrate having piezoelectricity such as lithium tantalate (LiTaO ₃ ) single crystal, lithium niobate (LiNbO ₃ ) single crystal, or quartz. The planar shape and various dimensions of the piezoelectric substrate 1 may be set as appropriate. As an example, the thickness of the piezoelectric substrate 1 is 0.3 mm to 1 mm.

  FIG. 6 shows a cross-sectional view of the specimen sensor 100A. 6A is a cross-sectional view taken along line VIa-VIa in FIG. 4, and FIG. 6B is a cross-sectional view taken along line VIb-VIb in FIG. FIG. 7 shows a top view of the piezoelectric substrate 1.

  As shown in FIGS. 6 and 7, a detection first IDT electrode 5a, a detection second IDT electrode 6a, a reference first IDT electrode 5b, and a reference second IDT electrode 6b are formed on the upper surface of the piezoelectric substrate 1. The detection first IDT electrode 5a and the reference first IDT electrode 5b are for generating a predetermined SAW, and the detection second IDT electrode 6a and the reference second IDT electrode 6b are the detection first IDT electrode 5a and the reference first IDT electrode 5b, respectively. This is for receiving the generated SAW. The detection second IDT electrode 6a is disposed on the propagation path of the SAW generated by the detection first IDT electrode 5a so that the detection second IDT electrode 6a can receive the SAW generated by the detection first IDT electrode 5a. The reference first IDT electrode 5b and the reference second IDT electrode 6b are similarly arranged.

  Since the reference first IDT electrode 5b and the reference second IDT electrode 6b are the same as the detection first IDT electrode 5a and the detection second IDT electrode 6a, the detection first IDT electrode 5a and the detection second IDT electrode 6a will be described below as an example. .

  The detection first IDT electrode 5a and the detection second IDT electrode 6a have a pair of comb electrodes (see FIG. 7). Each comb electrode has two bus bars facing each other and a plurality of electrode fingers extending from each bus bar to the other bus bar side. The pair of comb electrodes are arranged so that a plurality of electrode fingers mesh with each other. The detection first IDT electrode 5a and the detection second IDT electrode 6a constitute a transversal IDT electrode.

  The detection first IDT electrode 5 a and the detection second IDT electrode 6 a are each connected to the pad 9 via the wiring 8. A signal is input from the outside to the detection first IDT electrode 5a through the pad 9 and the wiring 8, and a signal is output to the outside from the detection second IDT electrode 6a.

  The detection first IDT electrode 5a, the detection second IDT electrode 6a, the reference first IDT electrode 5b, the reference second IDT electrode 6b, the wiring 8 and the pad 9 are made of, for example, aluminum (Al), an alloy of aluminum and copper (Cu), or the like. . These electrodes may have a multilayer structure. In the case of a multilayer structure, for example, the first layer is made of titanium (Ti) or chromium (Cr), and the second layer is made of aluminum or an aluminum alloy.

The detection first IDT electrode 5a, the detection second IDT electrode 6a, the reference first IDT electrode 5b, and the reference second IDT electrode 6b are covered with a protective film 4. The protective film 4 contributes to preventing oxidation of each electrode and wiring. The protective film 4 is made of silicon oxide, aluminum oxide, zinc oxide, titanium oxide, silicon nitride, silicon (Si), or the like. In the analyte sensor 100A, silicon dioxide (SiO ₂ ) is used as the protective film 4.

  The protective film 4 is formed over the entire upper surface of the piezoelectric substrate 1 so as to expose the pads 9. The detection first IDT electrode 5a and the detection second IDT electrode 6a are covered with the protective film 4. Thereby, it can suppress that an IDT electrode corrodes.

  The thickness of the protective film 4 is, for example, 100 nm to 10 μm.

  As shown in FIG. 6B, the detection first IDT electrode 5a is accommodated in the first vibration space 11a, and the detection second IDT electrode 6a is accommodated in the second vibration space 12a. Accordingly, the detection first IDT electrode 5a and the detection second IDT electrode 6a are isolated from the outside air and the sample liquid, and the detection first IDT electrode 5a and the detection second IDT electrode 6a can be protected from corrosive substances such as moisture. Further, by securing the first vibration space 11a and the second vibration space 12a, the detection first IDT electrode 5a and the detection second IDT electrode 6a can be brought into a state in which the excitation of the SAW is not significantly hindered.

  The first vibration space 11 a and the second vibration space 12 a can be formed by joining the plate-like body 2 having a recess for forming these vibration spaces to the piezoelectric substrate 1.

  The reference first IDT electrode 5b and the reference second IDT electrode 6b are similarly provided with a first vibration space 11b and a second vibration space 12b.

  Between the concave portions for forming the first vibration space 11a and the second vibration space 12a of the plate-like body 2, a through portion that is a portion penetrating the plate-like body 2 in the thickness direction is formed. . This penetrating portion is provided to form the metal film 7a on the SAW propagation path. That is, when the plate-like body 2 is bonded to the piezoelectric substrate 1, at least a part of the SAW propagation path propagating from the detection first IDT electrode 5 a to the detection second IDT electrode 6 a is exposed from the through portion in plan view. A metal film 7a is formed on the exposed portion.

  Similarly, between the recesses for forming the first vibration space 11b and the second vibration space 12b of the plate-like body 2, other through-holes that are portions that penetrate the plate-like body 2 in the thickness direction Is formed. This penetrating portion is provided to form the metal film 7b on the SAW propagation path.

  The plate-like body 2 having such a shape can be formed using, for example, a photosensitive resist.

  The metal film 7a exposed from the penetrating part of the plate-like body 2 constitutes a specimen liquid detection part. The metal film 7a has a two-layer structure of, for example, chromium and gold formed on the chromium. For example, an aptamer made of nucleic acid or peptide is immobilized on the surface of the metal film 7a. When the sample liquid comes into contact with the metal film 7a on which the aptamer is immobilized in this way, a specific target substance in the sample liquid is bound to an aptamer corresponding to the target substance. With such a configuration, the mass of the metal film 7a monotonously increases as the specimen binds and adsorbs to the aptamer. That is, the mass increases monotonously according to the detection of the specimen. Here, the mass of the metal film 7a monotonously increases only while the specimen is continuously supplied onto the metal film 7a. For example, when the buffer solution is supplied continuously with the sample supply before and after the sample solution is supplied, the sample passes over the metal film 7a, and the mass is reduced due to the separation of the sample and the aptamer. There is no problem.

  Further, the metal film 7b exposed from the other penetrating portion of the plate-like body 2 constitutes a reference portion. The metal film 7b has, for example, a two-layer structure of chromium and gold formed on the chromium. It is assumed that an aptamer immobilized on the metal film 7a is not attached to the surface of the metal film 7a so as not to be reactive with the specimen. Furthermore, a surface treatment may be performed so as to stabilize the sample solution by reducing its reactivity.

  In order to measure the property of the sample solution using SAW, first, a predetermined voltage (signal) is applied to the detection first IDT electrode 5a from the external measuring device via the pad 9 and the wiring 8. Then, the surface of the piezoelectric substrate 1 is excited in the formation region of the detection first IDT electrode 5a, and SAW having a predetermined frequency is generated. Part of the generated SAW passes through the region between the detection first IDT electrode 5a and the detection second IDT electrode, and reaches the detection second IDT electrode 6a. At this time, in the metal film 7a, the aptamer immobilized on the metal film 7a binds to a specific target substance in the sample, and the weight of the metal film 7a changes by the amount of the binding, so it passes under the metal film 7a. The phase characteristics of the SAW to be changed. When the SAW whose characteristics have changed in this manner reaches the detection second IDT electrode 6a, a voltage corresponding to the SAW is generated in the detection second IDT electrode 6a. This voltage is output to the outside as a detection signal of an AC signal through the wiring 8 and the pad 9, and is processed through the branching unit 130 and the calculating unit 140 shown in FIG. be able to.

  That is, the detection element 110 </ b> A is configured by the piezoelectric substrate 1, the metal film 7 a as a detection unit formed on the piezoelectric substrate 1, and the detection first IDT electrode 5 a and the detection second IDT electrode 6 a.

  Similarly, another metal film 7b in which no aptamer is fixed is provided in the same space 20, a signal from the reference first IDT electrode 5b is input, and an AC signal output from the reference second IDT electrode 6b is converted to a temperature characteristic or the like. Reference signal used for calibration of signal fluctuation due to environmental changes such as humidity and humidity.

  That is, the reference element 120A is configured by the piezoelectric substrate 1, the metal film 7b as a reference portion formed on the piezoelectric substrate 1, and the reference first IDT electrode 5b and the reference second IDT electrode 6b.

  In this example, the detection element 110A and the reference element 120A share the same piezoelectric substrate 1, but the detection element substrate (first substrate) and the reference element substrate (second substrate) may be separated. Good.

  The cover 3 is made of, for example, polydimethylsiloxane. By using polydimethylsiloxane as the material of the cover 3, the cover 3 can be formed into an arbitrary shape. Moreover, if polydimethylsiloxane is used, the ceiling part and side wall of the cover 3 can be formed comparatively easily. The thickness of the ceiling part and the side wall of the cover 3 is, for example, 1 mm to 5 mm.

  As shown in FIG. 7, one of the pair of comb-like electrodes constituting each of the detection first IDT electrode 5a, the detection second IDT electrode 6a, the reference first IDT electrode 5b, and the reference second IDT electrode 6b is a reference potential line. 31 is connected. The reference potential line 31 is connected to the pad 9G and becomes a reference potential. Then, of the pair of comb-like electrodes constituting each of the detection first IDT electrode 5a, the detection second IDT electrode 6a, the reference first IDT electrode 5b, and the reference second IDT electrode 6b, an electrode on the side connected to the reference potential is selected. It is arranged on the side where the reference potential line 31 is arranged. In other words, the electrode on the inner side of the pair of comb-like electrodes is connected to the reference potential. With this configuration, it is possible to suppress crosstalk between signals between the detection element 110A and the reference element 120A.

  With this configuration, the wiring 8 can be easily routed between the detection element 110A and the reference element 120A, and the lengths of the wirings 8 can be made uniform. As a result, the reference signal from the reference element 120A becomes more accurate as a reference signal.

(Second Embodiment)
Next, an analyte sensor 100B according to a second embodiment of the present invention will be described with reference to FIG.

  In the sample sensor 100A according to the first embodiment described above, the example in which signals from the detection element 110 and the reference element 120 are directly used has been described. On the other hand, as in the sample sensor 100B according to the second embodiment shown in FIG. 8, between the detection element 110 and the first branch part 131 and between the reference element 120 and the second branch part 132, respectively. The low noise amplifier 133 (first low noise amplifier 133a, second low noise amplifier 133b) may be arranged.

  According to this, high detection accuracy can be obtained even in the following cases.

  In general, in the SAW sensor, when the sensitivity is high, the change in the amplitude characteristic becomes large. Therefore, if the thickness of the protective film 4 is adjusted to increase the sensitivity, the loss may increase and accurate measurement may not be possible. However, high detection accuracy is obtained by interposing the low noise amplifier 133. be able to. On the other hand, if the signal input to the calculation unit 140 is small, noise may increase and the detection accuracy may be lowered. However, by providing a low noise amplifier 133 in the input path to the calculation unit 140, high detection accuracy may be achieved. Can be obtained. The low noise amplifier 133 is preferably provided on the side close to the elements 110 and 120 in the input path to the calculation unit 140.

  In addition, when the signals input to the detection element 110 and the reference element 120 are increased, there is a possibility that the input signals of each other or these input signals and other signals may have an adverse effect such as crosstalk. Further, by interposing the low noise amplifier 133 in the output path from the reference element 120, it is possible to suppress the above-described crosstalk and obtain high detection accuracy. Furthermore, when the signals input to the detection element 110 and the reference element 120 are increased, there is a possibility that the input signals of each other, or these input signals and other signals may leak to the outside as electromagnetic waves. By interposing the low noise amplifier 133 in the output path from the reference element 120, leakage of electromagnetic waves as described above can be suppressed and high detection accuracy can be obtained.

<Sample sensing method>
An analyte sensing method according to an embodiment of the present invention will be described.

(Sample solution supply process)
First, a sample solution supplying step for supplying a sample containing a target to the detection unit of the detection element whose mass changes in accordance with the target adsorption or the reaction with the target and the reference unit of the reference element that does not adsorb or react with the target. Do.

(Branching process)
Next, from the detection signal that is an AC signal according to the mass change of the detection unit and the reference unit, one of the above-described reference signals that is an AC signal is converted into two signals, a first signal and a second signal having the same phase. The other signal is branched into a third signal having the same phase as the first signal and a fourth signal having a phase shifted by a value other than 180 °.

  Here, the phase of the fourth signal can be appropriately selected as long as it is a value excluding ± 180 ° with respect to the phase of the first signal, but is preferably ± 90 °.

  Prior to the branching step described above, it is preferable to amplify each of the detection signal and the reference signal.

(First calculation process)
Next, a first measurement signal is obtained from the first signal and the third signal by a heterodyne method.

  Here, when executing the heterodyne method, the third signal may be subtracted from the first signal, or the first signal may be subtracted from the third signal.

(Second calculation step)
Similarly, a second measurement signal is obtained from the second signal and the fourth signal by a heterodyne method.

  Here, when the heterodyne method is executed, the fourth signal may be subtracted from the second signal, or the second signal may be subtracted from the fourth signal, as in the first calculation step described above.

(Measurement process)
Next, two first phase change candidate values are calculated from the first measurement signal, two second phase change candidate values are calculated from the second measurement signal, and two first phase change candidate values and two second phase change values are calculated. Among the phase change candidate values, the one that forms the smallest combination is defined as a first phase change value and a second phase change value.

(Selection process)
Further, the intensity of two intersection points of the trajectory of the first measurement signal and the second measurement signal is obtained in advance, and the first measurement signal and the second measurement signal that are located between the above two intersection intensity values are obtained. Select as measurement signal. Similarly, the first phase change value and the second phase change value corresponding to this measurement signal are selected as the phase change value.

(Detection amount calculation process)
The detection amount of the specimen is calculated from the phase change value selected in the selection step.

  The detected amount of the sample can be measured through the above steps.

  This invention is not limited to the above embodiment, It can implement in a various aspect.

  For example, in the detection sensor according to the above-described embodiment, as shown in FIG. 3 and the like, the intensity of two intersections of the trajectory of the first measurement signal and the second measurement signal is obtained in advance, and the first measurement signal and the second measurement are obtained. A signal and a signal positioned between two intersection strengths are selected as measurement signals. Instead of this, a configuration in which the signal output value (for example, V1, V2) closer to a predetermined reference value among the first phase change value and the second phase change value may be selected as the phase change value. According to this, while having the same effect as the above-mentioned embodiment, it is possible to specify a phase change value to be selected with a predetermined reference value as a reference. Here, as the reference value, for example, the midpoint of the two intersection strengths described above, or 0 (zero) can be set. When a theoretical trajectory as shown in FIG. 3 is used, the midpoint of the two intersection strengths that are reference values is zero. Note that the reference value is not limited to the midpoint between the two intersection strengths, and is set to an appropriate value so that a highly sensitive measurement signal can be obtained in consideration of the first measurement signal and the second measurement signal. Good.

  In the detection sensor according to the above-described embodiment, as shown in FIGS. 1 to 3 and the like, in the second branching unit 132, the third signal has the same phase as the first signal, and the fourth signal is derived from the first signal. The phase is shifted by 90 °. The setting of the phases of the first to fourth signals is not limited to this, and the first measurement signal and the second measurement signal may be set to have a phase difference excluding ± 180 °. Like the sample sensor 100C shown in FIG. 9, for example, the first signal and the second signal are set to the same phase, the third signal is shifted by -45 ° from the first signal, and the fourth signal is changed to the first signal. The phase may be shifted by + 45 ° with respect to the angle. Even in this case, the same effects as those of the sample sensor according to the above-described embodiment can be obtained.

  In the detection sensor according to the above-described embodiment, as shown in FIG. 1 and the like, the first branching unit 131 and the second branching unit 132 are branched into two signals, respectively. The unit 131 and the second branch unit 132 may be set to branch into three or more signals, respectively. For example, when the first branching unit 131 and the second branching unit 132 branch into three signals, respectively, as in the specimen sensor 100D shown in FIG. 10, two of the obtained signals are used to each other by a heterodyne method. By obtaining three measurement signals having different phase differences, the same effect as that of the detection sensor can be obtained. In addition, in this case, the sensitivity of the three measurement signals is higher than that of the three measurement signals even if the region with a small inclination is wide, in other words, the region where each measurement signal can be measured with high sensitivity. Since it can set so that the measurement signal which has an area | region can be selected, it becomes possible to suppress the fall of a sensitivity more effectively.

  In the detection sensor according to the above-described embodiment, as shown in FIG. 1 and the like, one detection element 110 and one reference element 120 are provided, and one detection element 110 and the first branch portion 131 are connected. In addition, one reference element 120 and the second branch part 132 are connected. Instead, as in the sample sensor 100E shown in FIG. 11, two or more detection elements and reference elements are used, and the two or more detection elements 110a and 110b and the first branch portion 131 are connected, and 2 Two or more reference elements 120a, 120b and the second branch part 132 may be connected. In this case, the first branch unit 131 can be selectively connected to one of the two or more detection elements 110a and 110b by the switch 136a, and the second branch unit can be two or more reference elements by the switch 136b. What is necessary is just to enable it to selectively connect with either of 120a, b. According to this, two or more detection targets can be detected at once, that is, by using one specimen, without changing the configuration after the branching unit 130. Further, as shown in the configuration of the switches 135 and 136 in FIG. 11, for example, each of the first branch unit and the second branch unit can be connected to both the detection element and the reference element. be able to. Furthermore, instead of these configurations, three detection elements and one reference element may be used. In this case, as long as one of the first branch part and the second branch part is connected to the reference element, there is no particular limitation on which of the three detection elements is connected to the other. It can be set as appropriate according to the type and number.

  In the detection sensor according to the above-described embodiment, the detection element 110A and the reference element 120A have been described using an example in which a substrate having piezoelectricity is shared, but the element substrate for the detection element 110A and the reference element The second substrate for the element 120A may be separated. In this case, crosstalk between the detection element 110A and the reference element 120A can be suppressed. In such a case, a separate substrate for holding the element substrate and the second substrate may be provided.

DESCRIPTION OF SYMBOLS 1 ... Piezoelectric substrate 2 ... Plate-shaped body 3 ... Cover 4 ... Protective film 5a ... Detection 1st IDT electrode 5b ... Reference 1st IDT electrode 6a ... Detection 2nd IDT electrode 6b. ..Reference second IDT electrode 7a, 7b ... Metal film 8 ... Wiring 9 ... Pad 11a, 11b ... First vibration space 12a, 12b ... Second vibration space 20 ... Space 31・ ・ ・ Reference potential line 100, 100A, B, C, D, E ... Specimen sensor 110 ... Detection element 111 ... Detection unit 120 ... Reference element 121 ... Reference unit 130 ... Branch part 131 ... 1st branch part 132 ... 2nd branch part 133 ... Low noise amplifier 135a, b, c, d ... Element side switch 136a, b ... Branch part side switch 140 ...・Calculation unit 141 ... first calculating part 142 ... second calculator 150 ... measurement section 160 ... selection unit 170 ... detection amount calculation unit

Claims (9)

A detection element that has a detection unit that changes in mass according to adsorption of a target contained in a specimen or a reaction with the target, and that outputs a detection signal that is an AC signal in accordance with a change in mass of the detection unit;
A reference element that does not adsorb the target or does not react with the target, and outputs a reference signal that is an AC signal for the detection signal;
A branching unit that branches one of the detection signal and the reference signal into a first signal and a second signal, and branches the other signal into a third signal and a fourth signal;
A first calculation unit that obtains a first measurement signal from the first signal and the third signal by a heterodyne method;
A second calculation unit for obtaining a second measurement signal having a phase difference different from the first measurement signal (excluding ± 180 °) from the second signal and the fourth signal by a heterodyne method;
Two first phase change candidate values are calculated from the first measurement signal, two second phase change candidate values are calculated from the second measurement signal, and the two first phase change candidate values and the two first phase change candidate values are calculated. A measurement unit that sets a first phase change value and a second phase change value as a combination of two phase change candidate values that are closest to each other;
A specimen sensor comprising: a selection unit that selects a phase output value that is closer to a reference value of the first phase change value and the second phase change value as a phase change value. A detection element that has a detection unit that changes in mass according to adsorption of a target contained in a specimen or a reaction with the target, and that outputs a detection signal that is an AC signal in accordance with a change in mass of the detection unit;
A reference element that does not adsorb the target or does not react with the target, and outputs a reference signal that is an AC signal for the detection signal;
One of the detection signal and the reference signal is branched into two first and second signals having the same phase, and the other signal is divided into a third signal having the same phase as the first signal, A branching portion that branches into a fourth signal having a phase different from that of the first signal (excluding ± 180 °);
A first calculation unit that obtains a first measurement signal from the first signal and the third signal by a heterodyne method;
A second calculation unit for obtaining a second measurement signal from the second signal and the fourth signal by a heterodyne method;
Two first phase change candidate values are calculated from the first measurement signal, two second phase change candidate values are calculated from the second measurement signal, and the two first phase change candidate values and the two first phase change candidate values are calculated. A measurement unit that sets a first phase change value and a second phase change value as a combination of two phase change candidate values that are closest to each other;
The intensity of two intersection points of the trajectory of the first measurement signal and the second measurement signal is obtained in advance, and is located between the intensity of the two intersection points of the first measurement signal and the second measurement signal. A sample sensor comprising: a selection unit that selects a measurement signal as a measurement signal and selects a phase change value corresponding to the measurement signal from the first phase change value and the second phase change value.   The analyte sensor according to claim 2, wherein the fourth signal is 90 degrees out of phase with the third signal. The detection element includes a first substrate having piezoelectricity, the detection unit disposed on the first substrate, a detection first IDT electrode that generates an elastic wave toward the detection unit, and the detection unit. A detection second IDT electrode that receives the elastic wave that has passed through
The reference element includes: a second substrate having piezoelectricity; the reference unit disposed on the second substrate; a reference first IDT electrode that generates an elastic wave toward the reference unit; and the reference unit A reference second IDT electrode that receives the elastic wave that has passed through
The detection signal is an AC signal obtained by receiving the elastic wave that has passed through the detection unit by the detection second IDT electrode,
The analyte sensor according to claim 1, wherein the reference signal is an AC signal obtained by receiving the elastic wave that has passed through the reference unit with the reference second IDT electrode. A first low-noise amplifier that is located between the detection element and the branch part and amplifies the detection signal from the detection element;
The sample sensor according to claim 1, further comprising: a second low-noise amplifier that is positioned between the reference element and the branch unit and amplifies the reference signal from the reference element. A sample solution containing a sample with a target, the mass of which changes according to the adsorption of the target or the reaction with the target, the detection part of the detection element, and the reference element that does not adsorb the target or does not react with the target A sample solution supply step to be supplied to the reference unit of
One of a detection signal that is an AC signal corresponding to a change in mass of the detection unit output from the analyte detection element and a reference signal that is an AC signal corresponding to the mass of the reference unit output from the reference element A branching step of branching the signal into a first signal and a second signal and branching the other signal into a third signal and a fourth signal;
A first calculation step of obtaining a first measurement signal from the first signal and the third signal by a heterodyne method;
A second calculation step of obtaining a second measurement signal having a phase difference different from the first measurement signal (excluding ± 180 °) from the second signal and the fourth signal by a heterodyne method;
Two first phase change candidate values are calculated from the first measurement signal, two second phase change candidate values are calculated from the second measurement signal, and the two first phase change candidate values and the two first phase change candidate values are calculated. A measurement step in which the closest combination of the two phase change candidate values is the first phase change value and the second phase change value;
A specimen sensing method comprising: a selection step of selecting, as a phase change value, an output value of the first measurement signal and the second measurement signal that is close to a reference value. A sample solution containing a sample with a target, the mass of which changes according to the adsorption of the target or the reaction with the target, the detection part of the detection element, and the reference element that does not adsorb the target or does not react with the target A sample solution supply step to be supplied to the reference unit of
One of a detection signal that is an AC signal corresponding to a change in mass of the detection unit output from the analyte detection element and a reference signal that is an AC signal corresponding to the mass of the reference unit output from the reference element The signal is branched into two first and second signals having the same phase, and the other signal is different in phase from the third signal having the same phase as the first signal and the first signal (± 180 °). Branching step to branch to the fourth signal;
A first calculation step of obtaining a first measurement signal from the first signal and the third signal by a heterodyne method;
A second calculation step of obtaining a second measurement signal from the second signal and the fourth signal by a heterodyne method;
Two first phase change candidate values are calculated from the first measurement signal, two second phase change candidate values are calculated from the second measurement signal, and the two first phase change candidate values and the two first phase change candidate values are calculated. A measurement step in which the closest combination of the two phase change candidate values is the first phase change value and the second phase change value;
The intensity of two intersection points of the trajectory of the first measurement signal and the second measurement signal is obtained in advance, and is located between the intensity of the two intersection points of the first measurement signal and the second measurement signal. A specimen sensing method comprising: selecting a measurement signal as the measurement signal, and selecting a phase change value corresponding to the measurement signal from the first phase change value and the second phase change value.   The analyte sensing method according to claim 7, wherein in the branching step, each of the detection signal and the reference signal is amplified, and the first to fourth signals are obtained based on the amplified detection signal and the reference signal.   The analyte sensing method according to claim 7 or 8, wherein, in the branching step, the phase of the fourth signal is different from the phase of the third signal by 90 °.