JP2016166804A - Component concentration measuring apparatus and component concentration measuring method - Google Patents

Abstract

PROBLEM TO BE SOLVED: To acquire a continuous spectrum in a component concentration measuring apparatus utilizing dielectric spectroscopy.SOLUTION: The component concentration measuring apparatus includes an optical notch filter 12 that controls frequencies F1 and F2 of two continuous light waves output from a dual mode light source 11 so that frequency shift is equivalently performed for an intermediate frequency F3 between the frequencies F1 and F2 and filters the intermediate frequency F3 after the dual mode light source 11. Thus, the frequency F3 of a third oscillation peak can be fixed to a predetermined frequency in a filtering band width of the optical notch filter 12. Therefore, the third oscillation peak can be efficiently filtered, and a continuous spectrum in a frequency band can be acquired.SELECTED DRAWING: Figure 1

Description

  The present invention relates to a technique for measuring a component concentration using dielectric spectroscopy.

  As aging progresses, the response to adult diseases has become a major issue. Tests such as blood glucose levels are a heavy burden on patients because they need to collect blood. Therefore, a non-invasive component concentration measuring apparatus that does not collect blood has attracted attention.

  An apparatus using dielectric spectroscopy has been proposed as a noninvasive component concentration measuring apparatus. Dielectric spectroscopy irradiates the skin with electromagnetic waves, absorbs the electromagnetic waves according to the interaction of blood components to be measured, for example, glucose molecules and water, and observes the amplitude and phase with respect to the frequency of the electromagnetic waves. The dielectric relaxation spectrum is calculated from the amplitude and phase with respect to the frequency of the observed electromagnetic wave. In general, the complex dielectric constant is calculated by expressing as a linear combination of relaxation curves based on the Cole-Cole equation. In the measurement of biological components, for example, the complex dielectric constant has a correlation with the amount of blood components such as glucose and cholesterol contained in blood, and is measured as an electrical signal (amplitude, phase) corresponding to the change. A calibration model is constructed by measuring the correlation between the complex dielectric constant change and the component concentration in advance, and the component concentration is calibrated from the measured change in the dielectric relaxation spectrum.

  As a conventional measurement method, there is a dielectric spectroscopic device using photoelectric conversion in a frequency band from microwave to millimeter wave or more (see Patent Document 1 and Non-Patent Document 1). The dielectric spectroscopic device of Patent Document 1 photoelectrically converts an optical signal in which two continuous light waves having different frequencies are combined to generate an electromagnetic wave, for example, a terahertz wave, irradiates the object to be measured with the generated terahertz wave, The configuration is such that the terahertz wave transmitted through the measurement object is received and the reference light synthesized by modulating the phase of one of the two continuous light waves is input to perform homodyne mixing. For example, a detector that performs homodyne mixing uses a photoconductive antenna, and the conductance between the antennas is modulated by the difference frequency between two continuous light waves included in the reference light by irradiation with the reference light. In the conventional dielectric spectroscopic device, when homodyne detection of electromagnetic waves, it is necessary that the two optical path length differences when the optical signal transmitted through the object to be measured and the reference light are mixed by the detector match. It is. Therefore, the propagation length of the terahertz wave propagating in space, the length of the file through which light propagates, and the like are adjusted.

  There is also known a dielectric spectroscopic device in which two continuous light wave light sources are realized by one dual-mode light source using a continuously oscillating acousto-optic element (see Non-Patent Document 2).

JP 2013-32933 A

Jae-Young Kim, Ho-Jin Song, Katsuhiro Ajito, Makoto Yaita, and Naoya Kukutsu, “Continuous-Wave THz Homodyne Spectroscopy and Imaging System With Electro-Optical Phase Modulation for High Dynamic Range”, IEEE Transactions on terahertz science and technology, March 2013, Vol. 3, No. 2, pp.158-164 Steven Jones, JaeYoung Kim, Yoshiyuki Doi, Takashi Yamada, Nobutatsu Koshobu, and Hiroyoshi Togo, “Ultra-Wideband Tunable Dual-Mode Laser for Continuous Wave Teraherts Generation”, Journal of Lightwave Technology, 2014, Vol. 32, Issue 20, pp .3461-3467 Andrew P. Gregory, and Robert N. Clarke, “A Review of RF and Microwave Techniques for Dielectric Measurements on Polar Liquids”, IEEE Transactions on Dielectrics and Electrical Insulation, August 2006, Vol. 13, No. 4, pp.727- 743

  However, in a dual mode light source using an acoustooptic device, when two frequency components are close to 1 THz or less, a third oscillation peak occurs at a frequency intermediate between the two frequencies. For this reason, a difference frequency beat signal is generated in addition to the difference frequency beat signal by a combination of two desired frequencies, and there is a problem that a continuous spectrum cannot be obtained in the frequency band. As a result, it becomes difficult to identify the peak of the substance to be measured using continuously acquired spectra, and it is difficult to determine the concentration using the peak intensity.

  The present invention has been made in view of the above, and an object of the present invention is to obtain a continuous spectrum in a component concentration measurement apparatus using dielectric spectroscopy.

  The component concentration measuring apparatus according to the first aspect of the present invention filters a dual mode light source that outputs an optical signal in which two continuous light waves having different frequencies are combined, and an intermediate frequency between the two continuous light waves of the optical signal. A filter, a measuring means for photoelectrically converting the optical signal to generate an electromagnetic wave, receiving the electromagnetic wave transmitted or reflected by the object to be measured, and measuring an amplitude of the electromagnetic wave, and an intermediate between the two continuous light waves Control means for controlling the dual mode light source so as to change the frequency of the two continuous light waves so that the frequency is fixed in a band to be filtered by the filter.

  In the component concentration measuring apparatus, the filter is an optical notch filter that filters an intermediate frequency between the two continuous light waves.

  In the component concentration measuring apparatus, the filter is disposed at one branch destination and a demultiplexer that demultiplexes the optical signal so that the frequency components of the two continuous light waves are included, and the intermediate frequency is determined. And an optical filter for filtering.

  In the component concentration measuring apparatus, the measuring means measures the phase of the electromagnetic wave by homodyne detection.

  In the component concentration measuring method according to the second aspect of the present invention, the dual mode light source outputs an optical signal in which two continuous light waves having different frequencies are combined, and an intermediate frequency between the two continuous light waves of the optical signal. Filtering, generating an electromagnetic wave by photoelectrically converting the optical signal, receiving the electromagnetic wave transmitted or reflected by the object to be measured and measuring an amplitude of the electromagnetic wave, and an intermediate between the two continuous light waves And controlling the dual-mode light source so that the frequency of the two continuous light waves is changed in such a manner that the frequency is fixed in a band to be filtered in the filtering step.

  In the above component concentration measuring method, the measuring step measures the phase of the electromagnetic wave by homodyne detection.

  According to the present invention, a continuous spectrum can be obtained in a component concentration measuring device using dielectric spectroscopy.

It is a functional block diagram which shows the structure of the component density | concentration measuring apparatus in 1st Embodiment. It is a figure for demonstrating control of a dual mode light source. It is a functional block diagram which shows the structure of another component density | concentration measuring apparatus in 1st Embodiment. It is a functional block diagram which shows the structure of the component density | concentration measuring apparatus in 2nd Embodiment. It is a functional block diagram which shows the structure of another component density | concentration measuring apparatus in 2nd Embodiment. It is a functional block diagram which shows the structure of the component density | concentration measuring apparatus in 3rd Embodiment. It is a functional block diagram which shows the structure of another component density | concentration measuring apparatus in 3rd Embodiment. It is a functional block diagram which shows the structure of another component concentration measuring apparatus in 3rd Embodiment. It is a figure which shows the measurement system of a dielectric spectroscopy sensor. It is a figure which shows the measurement system of another dielectric spectroscopy sensor.

[First Embodiment]
FIG. 1 is a functional block diagram showing the configuration of the component concentration measuring apparatus according to the first embodiment.

  The component concentration measuring apparatus shown in FIG. 1 includes a dual mode light source 11, an optical notch filter 12, an amplitude modulator 13, an oscillator 14, a radiator 15, a detector 16, a lock-in amplifier 17, a monitor 18, and a controller 19. .

  The dual-mode light source 11 is controlled by the controller 19 with a control voltage, and outputs an optical signal in which two continuous light waves having different frequencies are combined. FIG. 2 is a diagram for explaining the control of the dual mode light source 11. As shown in FIG. 2, the controller 19 is configured such that the frequencies F1 and F2 of the two continuous light waves output from the dual mode light source 11 are F1 = 193.125 THz or less and F2 = The control voltage is linearly changed so as to be 193.175 THz or more, and the F2-F1 difference frequency beat signal input to the radiator 15 is linearly swept. For example, in order to generate an electromagnetic wave of 0.6 THz, F1 = 192.85 THz and F2 = 193.45 THz.

  The optical notch filter 12 has a function of filtering an intermediate frequency F3 between optical signal frequencies F1 and F2. For example, the bandwidth to be filtered is 50 GHz, and the center frequency is 193.15 THz. The optical notch filter 12 can be formed of a dielectric multilayer film on a quartz or polymer substrate. A filter having steep filter characteristics can be configured by increasing the number of layers of the dielectric multilayer film. The controller 19 shifts the frequencies F1 and F2 of the optical signal equally with respect to the intermediate frequency F3, so that the frequency F3 of the third oscillation peak can be fixed to the center frequency of the optical notch filter 12. The third oscillation peak can be efficiently filtered by the optical notch filter 12 to obtain a continuous spectrum in the frequency band.

  The optical signal filtered by the optical notch filter 12 is amplitude-modulated to a frequency w = 100 kHz from the oscillator 14 by a Mach-Zehnder type amplitude modulator 13 using an electro-optic effect in order to detect an electromagnetic wave by diode detection.

  The radiator 15 generates an electromagnetic wave (millimeter wave or terahertz wave) having a frequency difference between optical signals obtained by combining two continuous light waves having different frequencies. As the radiator 15, for example, a single traveling carrier photodiode (UTC-PD) can be used.

  An electromagnetic wave transmitted through the sample 100 is received by an SBD (Schottky barrier diode) with an antenna which is the detector 16. In SBD, an electric signal having a frequency w is output by envelope detection. The electric signal is synchronously detected, the amplitude is detected by the lock-in amplifier 17 and processed by the monitor 18.

  FIG. 3 is a functional block diagram showing the configuration of another component concentration measuring apparatus according to the first embodiment.

  In the example shown in FIG. 3, a duplexer 21 that demultiplexes an optical signal into frequencies F1 and F2 after the dual mode light source 11 is provided, and an intermediate frequency between the frequencies F1 and F2 is excluded at one of the outputs of the duplexer 21. The optical filter 22 including the frequency F1 is provided, and the coupler 23 that combines the other optical signal including the frequency F2 demultiplexed by the demultiplexer 21 is provided. Alternatively, a high-pass filter including the frequency F2 may be provided except for an intermediate frequency between the frequencies F1 and F2.

  Compared with the optical notch filter 12, the high-pass or low-pass optical filter 22 can easily realize steep filter characteristics by the dielectric multilayer film, and can reduce the number of layers of the multilayer film and reduce the cost.

  As described above, according to the present embodiment, the frequencies F1 and F2 of the optical signal obtained by combining two continuous light waves output from the dual mode light source 11 are set to the intermediate frequency F3 between the frequencies F1 and F2. The optical oscillation notch filter 12 for filtering the intermediate frequency F3 after the dual mode light source 11 is controlled to shift the frequency F3 of the third oscillation peak to the filtering band of the optical notch filter 12. Therefore, it is possible to efficiently filter the third oscillation peak and obtain a continuous spectrum in the frequency band. As a result, it is possible to identify the peak of the substance to be measured using the continuously acquired spectrum, and it is possible to determine the concentration using the peak intensity.

[Second Embodiment]
FIG. 4 is a functional block diagram showing the configuration of the component concentration measuring apparatus according to the second embodiment.

  The component concentration measuring apparatus shown in FIG. 4 is a component concentration measuring apparatus that performs homodyne detection, and includes a dual mode light source 11, an optical notch filter 12, a splitter 31, an amplitude modulator 32, an oscillator 14, a radiator 15, a detector 16, and a lock. An in-amplifier 17, a monitor 18, and a controller 19 are provided.

  Similar to the first embodiment, the controller 19 sets the dual mode light source so that the frequency F3 of the third oscillation peak is intermediate between the frequencies F1 and F2 of the optical signal obtained by combining two continuous light waves. 11 and the optical notch filter 12 filters an intermediate frequency F3 between the frequencies F1 and F2 of the optical signal.

  The splitter 31 branches the optical signal filtered by the optical notch filter 12. One optical signal is input to the radiator 15 and subjected to photoelectric conversion, and an electromagnetic wave (millimeter wave or terahertz wave) having a frequency matching the frequency difference is generated. The other optical signal is obtained by applying a signal having a single frequency w (for example, 100 kHz) from the oscillator 14 to a Mach-Zehnder type amplitude modulator 32 using an electro-optic crystal that can be electrically amplitude-modulated by a control signal. Amplitude modulation is performed and input to the detector 16. The length of the fiber through which the light propagates is adjusted in advance so that the optical path length difference between the two optical signals matches at the time of mixing by the detector 16. Note that the amplitude modulation may be performed by modulating the bias of the UTC-PD that is the radiator 15, and the terahertz wave may be amplitude-modulated by a chopper or the like.

  The detector 16 receives a transmission signal output from the radiator 15 and transmitted through the sample 100, and outputs an electric signal having a frequency w by homodyne detection. This electric signal is synchronously detected by the lock-in amplifier 17 to detect the amplitude and phase and processed by the monitor 18 (see Non-Patent Document 2). The detector 16 can be realized by mounting a THz mixer composed of an SBD with an antenna and a photomixer composed of an UTC-PD with an antenna in the same package as the optical fiber. Further, as the detector 16, a photoconductive antenna (PCA: Photo-Conductive Antenna) may be used.

  In the terahertz wave band, a sample dielectric 100 is irradiated with a terahertz wave by a free space method using a pseudo optical system using parabolic mirrors 33 and 34, and a complex dielectric constant is measured from a transmission signal.

  In the second embodiment, by performing homodyne detection, the phase can be detected and the dielectric constant derivation accuracy can be improved as compared with the first embodiment.

  FIG. 5 is a functional block diagram showing the configuration of another component concentration measuring apparatus according to the second embodiment.

  The component concentration measuring apparatus shown in FIG. 5 includes a duplexer 35, a phase modulator 36 using an electro-optic crystal that can be electrically phase-modulated by a control signal, and a coupler 37 instead of the amplitude modulator 32 shown in FIG. It is equipped with.

  A signal of a single frequency w (for example, 20 kHz) from the oscillator 14 is applied to the phase modulator 36 to perform serodyne phase modulation, and a frequency shift equivalent to the modulation frequency w is generated in the optical signal. The control voltage of the phase modulator 36 can be expressed as Vm (t) = N2Vπft by the product of the integer N and 2Vπ (control voltage whose phase changes by π: Vπ). When there is one phase modulator 36, a frequency transition 2N times the frequency of the control voltage occurs, and the frequency of the detected signal is 2N times the frequency of the control voltage (see Non-Patent Document 1).

  The detector 16 outputs an electric signal having a frequency w by homodyne detection. This electric signal is synchronously detected by the lock-in amplifier 17 to detect the amplitude and phase and processed by the monitor 18.

  The configuration of FIG. 5 performs frequency transition by phase modulation of local light and performs homodyne detection, thereby enabling homodyne detection without reducing the light intensity of local light compared to FIG. The / N ratio can be increased and the dielectric constant derivation accuracy can be improved.

[Third Embodiment]
FIG. 6 is a functional block diagram showing the configuration of the component concentration measuring apparatus according to the third embodiment.

  The component concentration measuring apparatus shown in FIG. 6 is a concentration measuring apparatus that performs homodyne detection, and includes a dual mode light source 11, a demultiplexer 41, splitters 42 and 43, couplers 44 and 45, a phase modulator 46, an oscillator 14, and a radiator 15. , Detector 16, lock-in amplifier 17, monitor 18, and controller 19.

  Similar to the first embodiment, the controller 19 sets the dual mode light source so that the frequency F3 of the third oscillation peak is intermediate between the frequencies F1 and F2 of the optical signal obtained by combining two continuous light waves. 11 is controlled.

  The demultiplexer 41 uses the intermediate frequency F3 between the frequencies F1 and F2 as a cut-off frequency, one branch as a low pass, and the other as a high pass, and suppresses the intermediate frequency F3 component by the filter characteristics of the demultiplexer 41. To do.

  The splitter 42 splits the optical signal including the frequency F1 into two, and the splitter 43 splits the optical signal including the frequency F2 into two.

  The coupler 44 multiplexes the optical signal including the frequency F1 demultiplexed by the splitter 42 and the optical signal including the frequency F2 demultiplexed by the splitter 43. The optical signal combined by the coupler 44 is input to the radiator 15.

  The phase modulator 46 is a phase modulator using an electro-optic crystal that can be electrically phase-modulated by a control signal, and is disposed between the splitter 43 and the coupler 45. A control signal having a single frequency w from the oscillator 14 is applied to the phase modulator 46 to perform serodyne phase modulation, and a frequency shift equivalent to the modulation frequency w is converted into an optical signal including the frequency F2 demultiplexed by the splitter 43. Cause it to occur.

  The coupler 45 multiplexes the optical signal including the frequency F1 separated by the splitter 42 and the optical signal including the frequency F2 + w phase-modulated by the phase modulator 46. The optical signal combined by the coupler 45 is input to the detector 16.

  The radiator 15 photoelectrically converts the optical signal combined by the coupler 44 and generates an electromagnetic wave (millimeter wave or terahertz wave) having a frequency that matches the frequency difference between the frequencies F1 and F2.

  The detector 16 photoelectrically converts the optical signal combined by the coupler 45 to generate an electromagnetic wave, and receives the electromagnetic wave radiated from the radiator 15 and transmitted through the sample 100 to perform homodyne mixing.

  The lock-in amplifier 17 detects the amplitude and phase by synchronously detecting the electrical signal output from the detector 16, and the monitor 18 processes the amplitude and phase detected by the lock-in amplifier 17.

  FIG. 7 shows a configuration in which an optical notch filter 12 is added after the dual mode light source 11 of FIG.

  FIG. 8 shows a configuration in which the optical filter 22 is added after the duplexer 41 of FIG.

  Next, a measurement system of a dielectric spectroscopic sensor using a lens will be described.

  FIG. 9 is a diagram showing a measurement system of the dielectric spectroscopic sensor of the present embodiment. In the example of FIG. 9, the amplitude and phase of a transmission signal transmitted through a liquid such as an aqueous solution or oil are measured by arranging a transmission type in the measurement system of the dielectric spectroscopic sensor. The terahertz wave radiated from the radiator 15 passes through the lens 51 and enters the sample cell of the dielectric constant measurement cell 53 held by the fixing jig 54. The size of the sample cell is, for example, several millimeters × several millimeters or more as the beam size or more. The material of the window plate 52 for fixing the sample may be a high resistance Si, Z cut crystal, HDPE, TPX, Tsurupica, etc., and a material having a high transmittance is selected according to the measurement frequency. The terahertz wave that has passed through the sample cell passes through the lens 51 and is received by the detector 16. Note that the sample cell may have a flow cell configuration including an inlet and an outlet. Moreover, you may measure solid.

  FIG. 10 is a diagram showing a measurement system of another dielectric spectroscopic sensor of the present embodiment. In the example of FIG. 10, a sample cell is arranged on the ATR prism 55 made of silicon, and the amplitude and phase of the reflected signal reflected by the sample cell are measured. The terahertz wave radiated from the radiator 15 passes through the lens 51 and the ATR prism 55 and is reflected by the sample cell of the dielectric constant measurement cell 53 held by the fixing jig 54. The sample cell is sealed in the dielectric constant measurement cell 53 by the window plate 52. The terahertz wave reflected by the sample cell passes through the ATR prism 55 and the lens 51 and is received by the detector 16.

DESCRIPTION OF SYMBOLS 11 ... Dual mode light source 12 ... Optical notch filter 13 ... Amplitude modulator 14 ... Oscillator 15 ... Radiator 16 ... Detector 17 ... Lock-in amplifier 18 ... Monitor 19 ... Controller 21 ... Demultiplexer 22 ... Optical filter 23 ... Coupler DESCRIPTION OF SYMBOLS 31 ... Splitter 32 ... Amplitude modulator 33, 34 ... Parabolic mirror 35 ... Demultiplexer 36 ... Phase modulator 37 ... Coupler 41 ... Demultiplexer 42, 43 ... Splitter 44, 45 ... Coupler 46 ... Phase modulator 51 ... Lens 52 ... Window plate 53 ... Cell for measuring dielectric constant 54 ... Fixing jig 55 ... ATR prism 100 ... Sample

Claims (6)

A dual-mode light source that outputs an optical signal in which two continuous light waves having different frequencies are combined;
A filter for filtering an intermediate frequency between the two continuous light waves of the optical signal;
Measuring means for photoelectrically converting the optical signal to generate an electromagnetic wave, receiving the electromagnetic wave transmitted or reflected by the object to be measured, and measuring the amplitude of the electromagnetic wave;
Control means for controlling the dual mode light source to change the frequency of the two continuous light waves so that an intermediate frequency between the two continuous light waves is fixed in a band to be filtered by the filter;
A component concentration measuring apparatus comprising:   2. The component concentration measuring apparatus according to claim 1, wherein the filter is an optical notch filter that filters an intermediate frequency between the two continuous light waves.   The filter includes: a demultiplexer that demultiplexes the optical signal so that frequency components of the two continuous light waves are included; and an optical filter that is disposed at one branch destination and filters the intermediate frequency. The component concentration measuring apparatus according to claim 1, which is configured.   4. The component concentration measuring apparatus according to claim 1, wherein the measuring unit measures the phase of the electromagnetic wave by homodyne detection. A dual mode light source outputting an optical signal in which two continuous light waves having different frequencies are combined;
Filtering an intermediate frequency between the two continuous light waves of the optical signal;
Photoelectrically converting the optical signal to generate an electromagnetic wave, receiving the electromagnetic wave transmitted or reflected through the object to be measured, and measuring the amplitude of the electromagnetic wave;
Changing the frequency of the two continuous light waves by controlling the dual-mode light source so that an intermediate frequency between the two continuous light waves is fixed in a band that is filtered in the filtering step;
A component concentration measurement method comprising:   6. The component concentration measuring method according to claim 5, wherein the measuring step measures the phase of the electromagnetic wave by homodyne detection.

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