Patent Application
20180364100
This invention relates to an arithmetic expression calculation method for correcting an output of a photo detector and an output correction method of the photo detector that is used for an optical analyzer such as a Fourier-transform infrared spectroscopy (FTIR).
A spectroscopic analyzer such as an FTIR analyzes a specimen component based on a wave number intensity distribution (optical spectrum) of the light passing a specimen. A photo detector such as an MCT photo detector is used in order to detect the intensity of the light passing the specimen, however, as a matter of course it is necessary to obtain a relationship (calibration curve) between the output value and the intensity of the incident light prior to the analysis.
Conventionally, the calibration curve is created by obtaining an output value of a photo detector into which a predetermined reference light enters.
Taking the MCT photo detector as an example, in case that the intensity of the incident light is the predetermined value or less, as shown in
However, in case that the intensity of the incident light is more than the predetermined value, as shown in
Patent Document
In order to solve these problems, as shown in the patent document 1, this inventor conceives a method wherein the light emitted from the light source enters the photo detector in both cases that the optical filter is arranged on the optical path and that no optical filter is arranged on the optical path, the first output value and the second output value as being the output value of the photo detector for each light of the multiple wave numbers contained in the incident light and an arithmetic expression (a calibration curve) is obtained to calculate the intensity of the incident light based on the output value of the photo detector using a ratio of the first output value to the second output for each of the predetermined wave numbers and the optical property of the optical filter as parameters.
However, this output correction method is one-point correction using one optical filter. Then, in case that the intensity of the light that enters the photo detector changes, the intensity of the incident light is calculated based on the light intensity that is different from the actual light intensity, resulting in measurement error. It can be conceived that the arithmetic expression is obtained for each of the different light intensity by using multiple optical filters whose optical property differs each other, thereby complicating the device configuration.
The present claimed invention intends to solve all of the problems and a main object of this invention is to make it possible to correct an output (make a calibration curve) of a photo detector used for an optical analyzer without using a plurality of optical filters in a short period of time with a simple arrangement.
More specifically, an arithmetic expression calculation method to linearly correct a photo detector in accordance with this invention is a method that is used for an optical analyzer comprising the photo detector wherein a relationship between intensity of incident light and an output value of the photo detector becomes linear within a predetermined range, and that is characterized by obtaining a linear output value that is obtained by linearly correcting the output value of the photo detector that detects the light of the first intensity wherein the output of the photo detector becomes non-linear in such a way that the relationship between the output value and the light of the first intensity becomes linear, and obtaining a non-linear output value as being an output value of the photo detector that detects the light of the second intensity whose output of the photo detector becomes non-linear, and by obtaining an arithmetic expression to linearly correct the non-linear output value in such a way that a relationship between the non-linear output value and the light of the second intensity becomes linear using the linear output value and the non-linear output value as parameters.
The arithmetic expression includes not only a numerical expression to linearly correct the non-linear output value but also a map or a look-up table, and may be also called a calibration curve.
In accordance with the above-mentioned arrangement, it is possible to obtain the arithmetic expression for calculating the output value in case that the output value of the photo detector that detects the light whose intensity is non-linear is corrected and the photo detector outputs the corrected linear output value just by obtaining the linear output value that is obtained by linear correction and the non-linear output value. For example, if the light from a light source is considered to be the light of the first intensity, and a total of the light other than the light from the light source and the light from the light source is considered to be the light of the second intensity, it is possible to obtain the above-mentioned arithmetic expression. With this arrangement, it is possible to correct the output of the photo detector without using a plurality of optical filters in a short period of time with a simple arrangement.
In order to make it possible to calculate the intensity of the light even though the intensity of the light that enters the photo detector changes, it is preferable that the arithmetic expression is obtained for each intensity wherein the output of the photo detector becomes non-linear.
In addition, if case that the optical analyzer further comprises a measurement cell on which the light from the light source is irradiated, the infrared radiation of the measurement cell changes in accordance with the temperature change. Accordingly, the intensity of the light that enters the photo detector changes.
As mentioned, in case that the light intensity of the photo detector changes due to the infrared radiation of the measurement cell, it is preferable that the light that enters the photo detector is set to be the light of the intensity wherein the output of the photo detector is non-linear by changing the infrared light emitted from the measurement cell by changing the temperature of the measurement cell, and the non-linear output value is obtained in this state. In accordance with this arrangement, it is possible to obtain the arithmetic expression for each temperature (each light intensity) during changing the measurement condition by changing the temperature of the measurement cell.
As an optical detecting device conceived is the optical analyzer that further comprises an analyzing part that calculates a light intensity signal for each light of multiple predetermined wave numbers contained in the incident light based on the output value obtained by the photo detector. In case of this arrangement, it can be conceived that both the linear output value and the non-linear output value are the output value of the photo detector for each light of the multiple predetermined wave numbers contained in the incident light. The wave number also contains a wave length of its inverse number.
Concretely, it can be represented by the arithmetic expression that satisfies the following expression in a predetermined range.
Y
linear(k)=C(y)·Ynon-linear(k)
where, k is the wave number, Ylinear(k) is the above-mentioned linear output value, Ynon-linear(k) is the non-linear output value, y is the output value of the photo detector and C(y) is the above-mentioned arithmetic expression.
It is preferable that the linear output value is obtained by the use of an initial arithmetic expression obtained by the following (a)˜(c) steps.
(a) The first output value as being an output value of the above-mentioned photo detector for each light of multiple predetermined wave numbers contained in the incident light is obtained by entering the light of the light source into the photo detector through an optical element whose wave number transmission property or wave number reflectance property is known in such a way that the intensity of the light falls within the above-mentioned range.
(b) The second output value as being an output value of the above-mentioned photo detector for each light of the multiple predetermined wave numbers contained in the incident light is obtained by entering the light emitted from the light source into the above-mentioned photo detector without any optical element.
(c) An initial arithmetic expression is obtained to linearly correct the output value of the above-mentioned photo detector that detects the light of the intensity that falls out of the above-mentioned range in such a way that the relationship between the output value and the light of the intensity that falls out of the above-mentioned range becomes linear using a ratio of the first output value to the second output value and the wave number transmission property or the wave number reflectance property of the optical element as the parameters.
Concretely, it can be represented that the arithmetic expression calculation method wherein the initial arithmetic expression satisfies the following expression in a predetermined range.
Y
1(k)/{C(y)·Y2(k)}=F(k)
where, k is the wave number, Y1 (k) is the above-mentioned first output value, Y2 (k) is the above-mentioned second output value, F (k) is the wave number transmission property or the wave number reflectance property of the above-mentioned optical element, y is the output value of the photo detector and C (y) is the above-mentioned arithmetic expression.
In addition, the output correction method of a photo detector in accordance with this invention is characterized by comprising an arithmetic expression calculation step to calculate the arithmetic expression by the above-mentioned arithmetic expression calculation method and a correction step to linearly correct the output of the photo detector.
Furthermore, the optical analyzer in accordance with this invention is an optical analyzer that comprises a photo detector wherein a relationship between intensity of incident light and an output value of the photo detector becomes linear in a predetermined range, and is characterized by further comprising an output value obtaining part that obtains a linear output value obtained by linearly correcting the output value of the photo detector that detects the light of the first intensity wherein the output of the photo detector is non-linear in such a way that the relationship between the output value and the light ofthe first intensity becomes linear and that obtains a non-linear output value as being the output value of the photo detector that detects the light of the second intensity wherein the output of the photo detector becomes non-linear, and an arithmetic expression calculation part that calculates an arithmetic expression to calculate an output value in case that the photo detector linearly outputs the light of the intensity to be the non-linear output by correcting the non-linear output value using the linear output value and the non-linear output value as parameters.
In addition, the optical analyzer in accordance with this invention is preferably to further comprise a light source, a measurement cell on which the light from the light source is irradiated, and a temperature adjusting mechanism to adjust temperature of the measurement cell, and the light that enters the photo detector is set to be the light of the intensity wherein the output of the photo detector is non-linear by changing the infrared light emitted from the measurement cell by changing the temperature of the measurement cell by the use of the temperature adjusting mechanism, and the output value obtaining part obtains the non-linear output value in this state.
Furthermore, the output correction device in accordance with this invention is an output correction device that corrects an output of a photo detector wherein a relationship between incident light intensity and an output value of the photo detector becomes linear within a predetermined range, and is characterized by comprising an output value obtaining part that obtains a linear output value obtained by linearly correcting the output value of the photo detector that detects the light of the first intensity wherein the output of the photo detector is non-linear in such a way that the relationship between the output value and the light of the first intensity becomes linear and that obtains a non-linear output value as being the output value of the photo detector that detects the light of the second intensity wherein the output of the photo detector is non-linear, an arithmetic expression calculation part that calculates an arithmetic expression to calculate an output value in case that the photo detector linearly outputs the light of the intensity to be the non-linear output by correcting the non-linear output value using the linear output value and the non-linear output value as parameters, and a correcting part that linearly corrects the output of the photo detector by the use of the arithmetic expression obtained in the arithmetic expression calculation part.
In accordance with this invention having the above-mentioned arrangement, it is possible to obtain the arithmetic expression for calculating the output value in case that the output value of the photo detector that detects the light whose intensity is non-linear is corrected and the photo detector outputs the corrected linear output value just by obtaining the linear output value that is obtained by linear correction and the non-linear output value.
One embodiment of an optical analyzer in accordance with this invention will be explained with reference to drawings.
The optical analyzer 100 of this embodiment is a Fourier-transform infrared spectroscopy, so-called FTIR 100, and as shown in
The light source 1 emits light (continuous light containing light having multiple wave numbers) having a broad spectrum, and for example, a tungsten.iodine lamp or a high-brightness ceramic light source is used.
The interferometer 2 makes use of, a so-called Michelson interferometer comprising a half mirror (a beam splitter) 21, a fixed mirror 22 and a moving mirror 23. The light that is from the light source 1 and that enters the interferometer 2 is divided into reflected light and transmitted light by the half mirror 21. One light is reflected by the fixed mirror 22 and the other light is reflected by the moving mirror 23 and both of them return to the half mirror 21 again and are combined and emitted from the interferometer 2.
The measurement cell 3 is a cell to which a gas (hereinafter also called as a sample gas) as being an object to be measured is introduced and the light from the interferometer 2 is transmitted in the sample in the measurement cell 3 and is introduced into the photo detector 4. The measurement cell 3 comprises a cell body having a cylindrical shape made of a metal such as aluminum and a window member that is arranged on both walls of the cell body and that is made of a translucent material such as quartz glass.
The photo detector 4 in this embodiment is a so-called MCT photo detector 4.
The arithmetic processing unit 5 comprises an analog electric circuit having a buffer and an amplifier, a digital electric circuit having a CPU, a memory and a DSP and an A/D convertor arranged therebetween. The arithmetic processing unit 5 calculates a spectrum of the light that is transmitted in the sample gas based on an output value of the photo detector 4 and produces a function as an analysis part 51 that analyzes the sample by obtaining light absorbance of each wave number based on the optical spectrum by cooperatively working the CPU and its peripheral devices according to predetermined programs stored in the memory.
The analysis part 51 calculates the optical spectrum as follows.
If the moving mirror 23 is moved back and the intensity of the light that is transmitted in the sample gas is monitored with a position of the moving mirror 23 placed on the x axis, in case that the light is a single wave number, the light intensity draws a sine curve due to interference. Meanwhile, since the actual light that is transmitted in the specimen is the continuous light, the sine curve differs from each wave number and the actual light intensity becomes superimposition of the sine curves drawn by each wave number so that the interference pattern (interferogram) becomes a shape of a wave packet.
The analysis part 51 obtains the position of the moving mirror 23 by a speed distance meter such as a He Ne laser (not shown in drawings), and the light intensity at each position of the moving mirror 23 by the photo detector 4. The analysis part 51 conducts the fast Fourier transform (FFT) on the obtained interference pattern and transforms the obtained interference pattern into the optical spectrum with each wave number component placed on the x axis and the light intensity signal placed on the y axis.
At this time the intensity of the light that is transmitted in the specimen, namely, the light that enters the photo detector 4 is calculated based on the output value of the photo detector 4. In order to calculate the light intensity it is necessary to previously obtain a relationship (a calibration curve) between the output value of the photo detector 4 and the intensity of the incident light and to store the relationship in the memory. The calibration curve in this embodiment is an arithmetic expression to transform the output value of the photo detector 4 into the intensity of the incident light, however, it may be a table or a map.
In this embodiment, the measurement cell 3 is so configured to be able to be adjusted in multistage, and the optical analyzer 100 comprises a temperature adjusting mechanism 7 to adjust the temperature of the measurement cell 3 and a temperature adjusting mechanism control part 55 to control the temperature adjusting mechanism 7.
The temperature adjusting mechanism 7 is a heater such as a heating wire arranged to surround the measurement cell 3. In addition, the temperature adjusting mechanism control part 55 controls the heating temperature of the measurement cell 3 due to the heater 7 by controlling a power source circuit that supplies the electric power to the heater 7. For example, the temperature adjusting mechanism control part 55 controls the temperature of the measurement cell 3 to be 25.9° C. (low temperature) and 164.1° C. (high temperature).
In this embodiment, the calibration curve (the arithmetic expression) is obtained for each temperature of the measurement cell 3. Concretely, both the calibration curve (the arithmetic expression) at 25.9° C. (low temperature) and the calibration curve at 164.1° C. (high temperature) are obtained. A method for obtaining the arithmetic expression at 25.9° C. (low temperature) obtained by the use of the optical filter 6 as being an optical element and the arithmetic expression at 164.1° C. (high temperature) obtained without using the optical filter 6 will be explained.
In this embodiment, in order to previously obtain the arithmetic expression at the low temperature, a following mechanism is provided for the optical analyzer 100.
First, as shown in
In addition, as shown in
The output value obtaining part 52 obtains the first output value as being an output value for each wave number of the photo detector 4 at a time when the light from the measurement cell 3 passes the optical filter 6 and enters the photo detector 4, and obtains the second output value as being an output value for each wave number of the photo detector 4 at a time when the light from the measurement cell 3 enters the photo detector 4 without passing the optical filter 6. The output value obtaining part 52 stores the obtained first output value and the second output value in a data storing part 54 arranged in a predetermined area of the memory. The output value obtaining part 52 also obtains a third output value as being an output value of the photo detector 4 when the light from the measurement cell 3 is shut off.
The arithmetic expression calculation part 53 obtains an arithmetic expression to calculate an output value in case that the photo detector 4 linearly outputs the light (the light without passing the above-mentioned optical filter 6) having the intensity that falls out of the linearly range by correcting the first output value of the photo detector 4 using the wave number transmission property of the optical filter 6 that is previously stored in the data storing part 54 as a parameter in addition to the first output value and the second output value, and stores the obtained arithmetic expression in the data storing part 54.
One example of the operation to obtain the arithmetic expression at the low temperature using this mechanism will be explained in detail with reference to
First, the measurement cell 3 is filled with the sample whose state such as temperature, component concentration and pressure is constant. In addition, the temperature of the measurement cell 3 is controlled at 25.9° C. by the temperature adjusting mechanism (Step S1). The reason why these states are made constant is not to change the spectrum of the light that is transmitted in the sample. The sample is preferably a material whose absorbency of the infrared light is small, and for example, nitrogen gas. The measurement cell 3 may not be filled with any sample, and may be evacuated.
Next, an operator places the optical filter 6 on the optical axis. Then, in a state that the light source 1 is lighted and the moving mirror 23 is moving, when the operator conducts a predetermined first arithmetic operation initiation operation by the use of a mouse or a keyboard, the output value obtaining part 52 detects this operation and receives●obtains the output value (interferogram) of the photo detector 4 at each position of the moving mirror 23. At this time, the output value obtaining part 52 corrects the offset of the interferogram by subtracting the output value of the photo detector 4 at a time when the incident light to the photo detector 4 is shut down.
Next, the output value obtaining part 52 calculates the first output value Y1 (k) as being the output value of the photo detector 4 for each wave number by conducting the Fast Fourier Transform on the offset corrected interferogram, and stores the first output value Y1 (k) in the data storing part 54 (Step S2). “k” indicates the wave number.
Next, the operator moves off the optical filter 6 from the optical axis. Then, when the operator conducts a predetermined second arithmetic operation initiation operation, the output value obtaining part 52 detects this operation and obtains the output value (interferogram) of the photo detector 4 at each position of the moving mirror 23. At this time, similar to the above-mentioned, the output value obtaining part 52 corrects the offset of the interferogram by subtracting the output value of the photo detector 4 at a time when the incident light to the photo detector 4 is shut down.
Later, the output value obtaining part 52 calculates the second output value Y2 (k) as being the output value of the photo detector 4 for each wave number by conducting the Fast Fourier Transform on the offset corrected interferogram, and stores the calculated second output value Y2 (k) in the data storing part 54 (Step S2).
Next, the arithmetic expression calculation part 53 obtains the first output value Y1(k) and the second output value Y2 (k) at the predetermined multiple wave numbers (for example, 15 points, P1˜P15 in
The evaluation function is expressed by the expression (1).
Y
1(k)/{C25.9° C. (y)·Y2(k)}=F(k) (1)
where F(k) is the transmittance (filter characteristic) of the optical filter 6 for each wave number, and y is the output value of the photo detector 4. C25.9° C. (y) is the expression expressed by, for example, the follow expression (2) wherein y is a variable and the form other than the coefficient is a previously determined numerical expression.
C
25.9° C. (y)=C1·y+C2·y2+C3·y3 (2)
For the above-mentioned arithmetic expression calculation part 53, coefficients C1˜C3 are obtained by the use of the known optimization method. Thus obtained arithmetic expression C25.9° C. (y) at the low temperature is stored in the data storing part 54.
In this embodiment, the temperature adjusting mechanism control part 55 raises the temperature of the measurement cell 3 from 25.9° C. to 164.1° C. by controlling the temperature adjusting mechanism 7 in order to previously obtain the arithmetic expression at the high temperature. In this process of raising the temperature, the optical filter 6 is evacuated.
In addition, the output value obtaining part 52 obtains the following two kinds of the output. Then the output value obtaining part 52 stores the two kinds of the output in the data storing part 54 provided in the predetermined area of the memory.
(1) A linear output value obtained by linearly correcting the output value of the photo detector 4 that detects the light of the first intensity wherein the output of the photo detector 4 becomes non-linear in such a way that a relationship between the output value and the light of the first intensity becomes linear. In this embodiment, this value is a value obtained by making the light of the first intensity as being the light of the light source 1 and wherein the output value of the photo detector 4 becomes non-linear enter the photo detector 4 and by linearly correcting the output value of the photo detector 4 that detects the incident light for each wave number. Concretely, the linear output value is a value that is obtained by linearly correcting the output value of the photo detector 4 by the use of the above-mentioned arithmetic expression C25.9° C. (y) in case that the measurement cell 3 is adjusted at 25.9° C.
(2) A non-linear output value as being the output value of the photo detector 4 that detects the light of the second intensity (different from the above-mentioned first intensity) wherein the output of the photo detector 4 becomes non-linear. In this embodiment, this value is an output value of the photo detector 4 for each wave number when the photo detector 4 detects an incident light that enters the photo detector 4 by making the light of the second intensity that is a total of the light from the light source 1 and the light from other than the light source 1 and wherein the output value obtained by the photo detector 4 becomes non-linear enter the photo detector 4. Concretely, in addition to the light from the light source 1, the light of the second intensity wherein the output of the photo detector 4 becomes non-linear due to the infrared radiation (infrared light) that increases by raising the temperature of the measurement cell 3 from 25.9° C. to 164.1° C. is formed and the light of the intensity as being the non-linear output enters the photo detector 4.
The arithmetic expression calculation part 53 corrects the above-mentioned non-linear output value using the linear output value and the non-linear output value as parameters, obtains the arithmetic expression to calculate the output value in case that the photo detector 4 linearly outputs the light of the above-mentioned second intensity and stores the obtained arithmetic expression in the data storing part 54.
One example of the operation to obtain the arithmetic expression at the high temperature by the use of this mechanism will be explained in detail with reference to
In this embodiment, the above-mentioned linear output value Ylinear(k) uses a value corrected by the use of the above-mentioned arithmetic expression C25.9° C. (y) at the low temperature (Step S4).
After completing the process of obtaining the above-mentioned arithmetic expression C25.9° C. (y) at the low temperature, the temperature of the measurement cell 3 is controlled to adjust from 25.9° C. to 164.1° C. by the temperature adjusting mechanism 7 (Step S5).
Then, in a state that the light source 1 is lighted and the moving mirror 23 is moving when the operator conducts a predetermined third calculation initiation operation by the use of a mouse or a keyboard, the output value obtaining part 52 detects this operation and receives●obtains the output value (interferogram) of the photo detector 4 at each position of the moving mirror 23.
Later, the output value obtaining part 52 calculates the non-linear output value Ynon-linear (k) as being the output value of the photo detector 4 for each wave number by conducting the Fast Fourier Transform on the interferogram, and stores the calculated non-linear output value Ynon-linear (k) in the data storing part 54 and terminates the operation (Step S6).
Next, the arithmetic expression calculation part 53 obtains the linear output value Ylinear (k) and the non-linear output value Ynon-linear (k) at the predetermined multiple wave numbers (for example, 15 points) from the data storing part 54, and obtains the arithmetic expression C164.1° C. (y) that satisfies the following evaluation function by, for example, an optimization method (Step S7).
The evaluation function is expressed by the expression (3).
Y
linear(k)=C164.1° C.(y)·Ynon-linear(k) (3)
where y is the output value of the photo detector. C164.1° C. (y) is the expression expressed by the follow expression (4) wherein y is a variable and the form other than the coefficient is a previously determined numerical expression.
C
164.1° C. (y)=C1′·y+C2′y2+C3′·y3 (4)
For the above-mentioned arithmetic expression calculation part 53, the coefficients C1′˜C3′ are obtained by the use of the known optimization method. Thus obtained arithmetic expression C164.1° C. (y) at the high temperature is stored in the data storing part 54. In the above-mentioned expression (3), (Ylinear′(k)) that is amplified by a predetermined ratio (for example, a factor of 0.9 or a factor of 1.1) may be used as Ylinear (k).
In case of analyzing the sample gas by the use of the measurement cell 3 at the low temperature (25.9° C.) the analyzing part 51 corrects the output value y (interferogram) of the photo detector 4 at each position of the moving mirror 23 by the use of the arithmetic expression C25.9° C. (y) stored in the data storing part 54. Concretely, a correction detector output value x, namely the light intensity x is calculated by multiplying the C25.9° C. (y) by the output value y of the photo detector 4. Then the optical spectrum is calculated by conducting the fast Fourier transform (FFT) on the correction detector output value x, and the sample is analyzed by obtaining the absorbance of the light of each wave number based on the optical spectrum.
In addition, in case of analyzing the sample gas by the use of the measurement cell 3 at the high temperature (164.1° C., the analyzing part 51 corrects the output value y (interferom) of the photo detector 4 at each position of the moving mirror 23 by the use of the arithmetic expression C164.1° C. (y) stored in the data storing part 54. Concretely, a correction detector output value x, namely the light intensity x is calculated by multiplying the C164.1° C. (y) by the output value y of the photo detector 4. Then the optical spectrum is calculated by conducting the fast Fourier transform (FFT) on the correction detector output value x, and the sample is analyzed by obtaining the absorbance of the light of each wave number based on the optical spectrum.
The output value for each wave number of the photo detector 4 obtained without conducting the linear correction is shown in
According to this, in the output value that is linearly corrected by the use of the arithmetic expression obtained by the above-mentioned (A) and (B), if a signal appears in the wavelength region (100˜600 cm−1) where there is no detector sensitivity, or the signal value is more than or equal to the predetermined threshold value, it is judged that the arithmetic expression is not reasonable. This judgment may be conducted by a man or may be automatically judged by a judging part arranged for the arithmetic processing device 5. In addition, in case that the arithmetic expression is judged not to be reasonable, the above-mentioned (A) and (B) processes may be conducted and the arithmetic expression may be obtained again.
In accordance with this embodiment having this arrangement, it is possible to obtain the arithmetic expression to calculate the output value in case that the photo detector 4 linearly outputs the output value by correcting the output value of the photo detector 4 that detects the non-linear light of the second intensity just by obtaining the linear output value that is obtained by the linear correction and the non-linear output value. In this embodiment, the above-mentioned arithmetic expression can be obtained by setting the light from the light source 1 as the light of the first intensity and the total of the light from the light source 1 and the light from other than the light source 1 as the light of the second intensity. Accordingly, it is possible to correct the output of the photo detector 4 in a short period of time with a simple arrangement without using a plurality of optical filters.
Especially in this embodiment, in accordance with the arrangement wherein the temperature of the measurement cell 3 is adjusted in multiple stages, since it is possible to obtain the light of the second intensity whose output value of the photo detector 4 becomes non-linear by making use of the infrared radiation of the measurement cell 3, there is no need of using a plurality of optical filters whose optical property differs each other and it is possible to make the output correction expression of the photo detector 4, namely to make the above-mentioned arithmetic expression in a short period of time with a simple arrangement.
In addition, as a result of this, there will be a merit that it is possible to inspect or reconstruct a calibration curve with ease at a time of adjusting the temperature of the measurement cell 3.
The present claimed invention is not limited to the above-mentioned embodiment.
For example, in the above-mentioned embodiment, the arithmetic expressions are obtained in two stages at the low temperature and at the high temperature respectively, however, in case of adjusting the temperature in more than or equal to three stages or steplessly, the arithmetic expression may be obtained at each temperature. Concretely, the temperature of the measurement cell 3 is changed to raise from the low temperature to the high temperature at multiple stages, the process that is the same as that of the above-mentioned embodiment (2) is conducted at each temperature, and then the arithmetic expression is obtained for each temperature. In short, the arithmetic expression may be obtained in the temperature (light intensity) wherein the relationship between the output value and the light intensity is non-linear by comparing the temperature (light intensity) wherein the relationship between the output value and the light intensity is linear (linear output) and the arithmetic expression is already obtained with the temperature (light intensity) wherein the relationship between the output value and the light intensity is non-linear (non-linear output) and the arithmetic expression is not obtained. Even if the temperature is adjusted in multiple stages from the high temperature to the low temperature or steplessly, it is possible to obtain the arithmetic expression in the same way. It can be conceived that an initial arithmetic expression prior to the temperature change is obtained by the use of the optical filter similar to the above-mentioned embodiment (1). In addition, the arithmetic expression may be previously obtained for each range of the output value of the photo detector and may switch the arithmetic expression in accordance with the output value of the photo detector.
In the above-mentioned embodiment, the arithmetic expression is obtained by the use of the output value for each wave number of the photo detector 4, however, the arithmetic expression may be obtained by the use of the interferogram obtained by the photo detector 4.
The interferogram has a direct current offset component (DC component) and a vibrational component (non DC component). The waveform of the vibrational component (non DC component) should be the same for both cases that the temperature of the measurement cell is 25.9° C. and 164.1° C. if the measured sample gas is the same. However, since the sensitivity of the detector differs, the shape of the vibrational component (non DC component) differs.
Then, the arithmetic processing unit 5 extracts the vibrational component from the interferogram both at 25.9° C. and 164.1° C. and obtains the arithmetic expression at 164.1° C. by comparing the extracted vibrational component. In this case, the relationship between the output value and the light intensity of the photo detector is regarded to be linear based on the arithmetic expression.
In the abovementioned embodiment, the light of non-linear intensity is produced by the use of the infrared radiation from the measurement cell as the light from other than the light source in order to linearly correct the photo detector, however, the light of non-linear intensity may be produced by the use of an auxiliary light source other than the light source or natural light.
In the abovementioned embodiment, the output value of the photo detector may be linearly corrected without using the optical filter 6. For example, it can be conceived that the linear output value is obtained by making the light in the linear range enter the photo detector 4 by adjusting the light intensity of the light source 1, and then the non-linear output value is obtained by making the light in the non-linear range enter the photo detector 4 by increasing the light intensity of the light source 1. Then, the arithmetic expression for linearly correction is obtained with the linear output and the non-linear output and the increased light intensity as parameters.
The arithmetic expression may be automatically obtained at each temperature. In this case, the optical analyzer 100 automatically moves the optical filter 6 and raises the temperature of the measurement cell 3.
In addition, the optical filter 6 is made detachable and the arithmetic expression at a predetermined temperature may be obtained by mounting the optical filter 6 only at a time of shipment or maintenance. With regard to other temperature, the arithmetic expression at each temperature may be obtained with a value corrected by the arithmetic expression at the predetermined temperature as the criteria.
The optical element is not limited to the transmission type, and may be a reflection type, and in short, it may be acceptable as far as the wave number property is well-known and the incident light intensity falls within a linear maintaining area of the photo detector.
The photo detector is not limited to the MCT photo detector. This invention can be applied to a photo detector wherein the relationship between the incident light intensity and the output value of the photo detector becomes linear within a predetermined range and non-linear within the other range.
In addition, this invention is not limited to the Fourier-transform type infrared spectroscopy, and the same effect can be obtained if this invention is applied to the spectroscopic analyzer of other type or a spectroscopy (an arrangement to obtain an optical spectrum in the above-mentioned embodiment).
A part of the function of the above-mentioned embodiment may be conducted by a machine learning part wherein an arithmetic processing is conducted by the use of machine learning algorithm.
The present claimed invention is not limited to the above-mentioned embodiment and may be variously modified without departing from a spirit of the invention.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2017-117462 | Jun 2017 | JP | national |
