Phase difference control device
阅读说明:本技术 相位差控制装置 (Phase difference control device ) 是由 三好有一 于 2019-01-30 设计创作,主要内容包括:本发明涉及一种能够在CD光谱仪中利用的相位差控制装置的响应性改善技术。相位差控制装置具备:分割偏振器(14),其将来自光源(12)的光分割成直线偏振的测定光和直线偏振的参照光;PEM(16),其以与分光测定相对应的方式对测定光和参照光赋予相位差;PEM驱动器(18),其向PEM(16)供给调制电压;PEM控制电路(24),其输入参照光作为反馈信号,并且向PEM驱动器(18)输出调制控制量信号,相位差控制装置还具备CPU电路(26),该CPU电路监视分割偏振器(14)的光的波长,并输入波长变化作为波长信号,CPU电路(26)将波长信号变换成前馈信号,前馈信号被输出到PEM控制电路(24),PEM控制电路(24)进行基于反馈信号和前馈信号的运算处理,来向PEM驱动器(18)输出调制控制量信号。(The present invention relates to a technique for improving the responsiveness of a phase difference control device that can be used in a CD spectrometer. The phase difference control device is provided with: a splitting polarizer (14) that splits light from the light source (12) into linearly polarized measurement light and linearly polarized reference light; a PEM (16) for giving a phase difference to the measurement light and the reference light so as to correspond to the spectroscopic measurement; a PEM driver (18) that supplies a modulated voltage to the PEM (16); and a PEM control circuit (24) that receives the reference light as a feedback signal and outputs a modulation control amount signal to the PEM driver (18), wherein the phase difference control device further comprises a CPU circuit (26) that monitors the wavelength of the light split into the polarizers (14) and receives a wavelength change as a wavelength signal, wherein the CPU circuit (26) converts the wavelength signal into a feedforward signal, and the feedforward signal is output to the PEM control circuit (24), and wherein the PEM control circuit (24) performs an arithmetic process based on the feedback signal and the feedforward signal and outputs the modulation control amount signal to the PEM driver (18).)
1. A phase difference control device used in a spectrometer for performing a spectroscopic measurement of a sample, the phase difference control device being characterized in that,
the phase difference control device includes: splitting the polarizer: which splits incident light from a light source into linearly polarized measurement light and linearly polarized reference light; a photoelastic modulator, that is, a PEM, that performs a phase modulation operation for imparting a phase difference to the measurement light and the reference light so as to correspond to the spectroscopic measurement; a PEM driver which supplies a modulation voltage for performing a phase modulation operation to the PEM; and a PEM control circuit which inputs the reference light as a feedback signal and outputs a modulation control amount signal to the PEM driver,
the phase difference control device further includes a CPU circuit for monitoring the wavelength of the light in the divided polarizer, inputting a change in the wavelength as a wavelength signal,
the CPU circuitry converts the wavelength signal into a feed forward signal, which is output to the PEM control circuitry,
the PEM control circuit performs an arithmetic process based on the feedback signal and the feedforward signal to output a modulation control amount signal to the PEM driver.
2. The phase difference control device according to claim 1,
the CPU circuit calculates a feedforward signal from an output instruction table previously created in the CPU circuit.
3. The phase difference control device according to claim 1 or 2,
the phase difference control device further comprises a temperature compensation circuit for supplying a modulation voltage for making a phase difference given to the measurement light and the reference light constant even if the temperature of the PEM changes from the PEM driver to the PEM,
the temperature compensation circuit receives a detection value detected by a temperature detector for detecting the temperature of the PEM and performs a temperature compensation operation.
4. The phase difference control device according to claim 3,
the PEM driver is configured to include the temperature compensation circuit in at least a portion thereof, the temperature compensation circuit configured to include a temperature compensated crystal oscillator.
5. A phase difference control method for controlling a phase difference of a PEM in a spectrometer including at least a light source, a splitting polarizer, a photoelastic modulator (PEM), a PEM driver, and a PEM control circuit, the phase difference control method comprising the steps of:
supplying a modulation voltage for performing a phase modulation operation from the PEM driver to a PEM, splitting incident light from a light source into linearly polarized measurement light and linearly polarized reference light by the splitting polarizer, imparting a phase difference to the obtained measurement light and reference light by the PEM in a manner corresponding to spectroscopic measurement, inputting the reference light to which the phase difference is imparted to the PEM control circuit as a feedback signal, and outputting a modulation control amount signal to the PEM driver to constitute a feedback control loop; and
the spectrometer is provided with a CPU circuit for monitoring the wavelength of light in the split polarizer and inputting the change in the wavelength as a wavelength signal, the CPU circuit converts the wavelength signal into a feedforward signal and outputs the feedforward signal to the PEM control circuit,
wherein the PEM control circuit outputs a modulation control quantity signal to the PEM driver using the feedback signal and the feedforward signal.
Technical Field
The present invention relates to a technique for improving the responsiveness of a phase difference control device used in various spectrometers and the like including a photoelastic modulator (PEM), and particularly a phase difference control device that can be used in a circular dichroism spectrometer (CD) and a linear dichroism spectrometer (LD).
Background
In the past, Photoelastic modulators (PEM) were used in various spectrometric measurements. Generally, a PEM is known as an element for phase modulating incident polarized light using birefringence. Moreover, the sensitivity of the polarized light measurement using the PEM is very high, and for example, when the wavelength of incident light to the PEM is changed, the phase modulation action of the PEM is also greatly influenced. That is, there is a possibility that the measurement result of the spectroscopic measurement is greatly affected by a change in the wavelength of incident light to the PEM or the like.
Therefore, patent document 1 discloses one of the following techniques: the phase difference control device is provided with a photoelastic modulator control circuit, and controls the ratio of the amplitude of the alternating current component having an angular frequency of 2 ω to the magnitude of the direct current component in the detected reference beam to be constant, so that the phase difference given by the photoelastic modulator can be kept constant even if the wavelength of light incident on the photoelastic modulator or the temperature of the photoelastic modulator changes.
Disclosure of Invention
Problems to be solved by the invention
However, by using the configuration of patent document 1 in the phase difference control device, it is possible to cope with an environmental change of the photoelastic modulator (a change in wavelength of incident light, etc.), but since this configuration has a limit in responsiveness of control (since it is control of acquiring whether or not a change is made in the photoelastic modulator as a signal, it is inevitably affected by the change), it is possible to cope with only step scanning when actually acquiring the spectrum data. That is, there are the following problems: such a technique cannot be applied to a spectrometer or the like that requires continuous scanning, such as a circular dichroism spectrometer.
Means for solving the problems
The present invention has been made in view of the above-described problems of the prior art, and an object of the present invention is to provide a phase difference control device and method that can achieve stable phase difference control even when a wavelength change of incident light or the like occurs in a photoelastic modulator, improve the responsiveness of phase difference control, and can also cope with continuous scanning.
In order to solve the above-mentioned problems, a phase difference control device according to the present invention is used in a spectroscopic measuring apparatus for performing spectroscopic measurement on a sample, the phase difference control device being characterized in that,
the phase difference control device includes: splitting the polarizer: which splits incident light from a light source into linearly polarized measurement light and linearly polarized reference light; a PEM that performs a phase modulation operation for applying a phase difference to the measurement light and the reference light so as to correspond to the spectroscopic measurement; a PEM driver which supplies a modulation voltage for performing a phase modulation operation to the PEM; and a PEM control circuit which inputs the reference light as a feedback signal and outputs a modulation control amount signal to the PEM driver,
the phase difference control device further includes a CPU circuit for monitoring the wavelength of the light in the divided polarizer, inputting a change in the wavelength as a wavelength signal,
the CPU circuitry converts the wavelength signal into a feed forward signal, which is output to the PEM control circuitry,
the PEM control circuit performs an arithmetic process based on the feedback signal and the feedforward signal to output a modulation control amount signal to the PEM driver.
In addition, the phase difference control device according to the present invention is characterized in that,
the CPU circuit calculates a feedforward signal from an output instruction table previously created in the CPU circuit.
In addition, the phase difference control device according to the present invention is characterized in that,
the phase difference control device further comprises a temperature compensation circuit for supplying a modulation voltage for making a phase difference given to the measurement light and the reference light constant even if the temperature of the PEM changes from the PEM driver to the PEM,
the temperature compensation circuit receives a detection value detected by a temperature detector for detecting the temperature of the PEM and performs a temperature compensation operation.
In addition, the phase difference control device according to the present invention is characterized in that,
the PEM driver is configured to include the temperature compensation circuit in at least a portion thereof, the temperature compensation circuit configured to include a temperature compensated crystal oscillator.
A phase difference control method according to the present invention is a phase difference control method for controlling a phase difference of a PEM in a spectrometer including at least a light source, a split polarizer, the PEM, a PEM driver, and a PEM control circuit, the phase difference control method including the steps of:
supplying a modulation voltage for performing a phase modulation operation from the PEM driver to a PEM, splitting incident light from a light source into linearly polarized measurement light and linearly polarized reference light by the splitting polarizer, imparting a phase difference to the obtained measurement light and reference light by the PEM in a manner corresponding to spectroscopic measurement, inputting the reference light to which the phase difference is imparted to the PEM control circuit as a feedback signal, and outputting a modulation control amount signal to the PEM driver to constitute a feedback control loop; and
the spectrometer is provided with a CPU circuit for monitoring the wavelength of light in the split polarizer and inputting the change in the wavelength as a wavelength signal, the CPU circuit converts the wavelength signal into a feedforward signal and outputs the feedforward signal to the PEM control circuit,
wherein the PEM control circuit outputs a modulation control quantity signal to the PEM driver using the feedback signal and the feedforward signal.
ADVANTAGEOUS EFFECTS OF INVENTION
According to the present invention, the phase difference control device includes a PEM control circuit to form a feedback control loop, and further includes a CPU circuit to monitor a wavelength change of incident light to the PEM (a wavelength change of light in the split polarizer), to calculate a feed forward signal under a constant condition, and to calculate a modulation control amount signal by performing arithmetic processing on the feed forward signal and the feedback signal in the PEM control circuit. By controlling the PEM driver with the modulation control amount signal, the response is improved compared to the conventional one, and stable phase difference control can be achieved even when a wavelength change of incident light occurs. As a result, since the responsiveness of the phase difference control is improved, it is possible to realize, for example, a phase difference control device and method that can cope with not only step scanning but also continuous scanning.
Drawings
Fig. 1 is a schematic configuration diagram showing a CD spectrometer to which a phase difference control device according to an embodiment of the present invention is applied.
Fig. 2 is a schematic configuration diagram showing a modification of the CD spectrometer to which the phase difference control device of the present invention is applied.
Fig. 3 (a) shows a series TCXO circuit that can be used for a temperature compensation circuit in the present embodiment, and fig. 3 (b) shows an indirect TCXO circuit that can be used for a temperature compensation circuit in the present embodiment.
Description of the reference numerals
10: CD spectrometer (phase difference control device); 12: a light source; 14: dividing the polarizer; 16: a PEM; 18: a PEM driver; 20: a sample; 22: a detection circuit; 24: a PEM control circuit; 26: a CPU circuit; 28: a PMT detector; 30: a preamplifier; 32: a DC amplifier; 34: an operational amplifier; 36: adjusting the sensitivity HT; 38: a sense amplifier; 40: a lock-in amplifier; 42: a temperature compensation circuit; 44: a temperature detector.
Detailed Description
The phase difference control device of the present invention will be described below with reference to the drawings, but the present invention is not limited to the following examples as long as the gist of the present invention is not exceeded.
Fig. 1 is a schematic configuration diagram of a circular dichroism spectrometer (CD spectrometer) as a spectroscopic measuring instrument according to an embodiment of the present invention. The
Light from the
The
Here, a description will be given of a detection process of the CD value in the
The CD voltage includes a direct current component and an alternating current component, and the direct current component in the amplified CD voltage is selectively amplified by the
Also, the CD voltage stabilized by these processes is input to the lock-in
AboutPhase difference control
Next, the phase difference control of the PEM16 in the
Although not shown in fig. 1, the reference light input to the
In this way, by performing the phase difference control of the PEM16 using the feedback control loop constituted by the
The
That is, the
A feedback signal as reference light in the PEM16 and a feed forward signal calculated from a change in the wavelength of incident light incident to the PEM16 are input to the
Calculation of feed forward signal
As described above, the feedforward signal is calculated by using a table prepared in advance or performing arithmetic processing based on an algorithm with respect to the wavelength signal (the wavelength change of the incident light to the PEM 16). For example, the feedforward signal can be calculated inside the
Then, an output command table necessary for the spectroscopic measurement (phase difference control) can be obtained by calculating in advance a voltage value that becomes the maximum value of the CD. As a method of calculating the voltage value that becomes the CD maximum value, for example, the PEM voltage is increased at every designated step, CD value data corresponding to each PEM voltage is acquired, the peak position of the data is set to the CD maximum value, and the voltage value at that time is set to the vmax value.
The feedforward signal can also be calculated by a predetermined algorithm prepared in advance in the
As still another method, the feedforward signal can be calculated by executing a program including an optimization algorithm such as a steepest descent method or peak detection. Here, the steepest descent method is an algorithm of a gradient method in which the minimum value of a certain function is searched only from the slope (first order differential) of the function, or an algorithm based on a similar consideration method. In the present embodiment, the output command table can be created by the steepest descent method or peak detection. Further, although the output command table for each PEM can be obtained by calculating the vmax value obtained by the above-described method over the entire wavelength range and all wavelength points of the measurement device, the operation of calculating the output command table can be made efficient by limiting the wavelength at which the vmax value is calculated and performing interpolation using the following numerical expression showing the relationship between V and wavelength.
[ numerical formula 1]
λ: wavelength of light
Vm: maximum value of voltage
A: phase difference
Q: coefficient of photoelasticity
In addition, as the calculation of the feedforward signal, in a CD spectrometer or the like, a in the above numerical expression is 1.841 radians, but in an ellipsometer, for example, a in the above numerical expression is 2.405 radians, and the maximum value of the CD value can be calculated. Similarly, for example, in an optical rotation spectrometer (ORD) or a linear dichroism spectrometer (LD), the maximum value of the CD value can be calculated by setting a in the above numerical expression to 3.05 radians. The calculation algorithm of the feedforward signal in the
Specifically, the algorithm for calculating the CD maximum value in the output command table can be, for example, a gauss-newton method, a Pattern Search (Pattern Search) method, a Nelder-Mead method, a genetic algorithm, a particle swarm optimization, a differential evolution method, a cuckoo Search, a firefly algorithm, or the like.
As described above, by providing the
< modification example >
In the PEM characteristics, the Q value is very high, and therefore, even if a slight temperature change occurs, the transmission frequency greatly fluctuates, and the measurement result may be greatly affected. Therefore, the phase difference control device in the present modification is configured by adding a circuit configuration capable of coping with the influence of such temperature change.
Fig. 2 is a schematic configuration diagram showing a modification example of the CD spectrometer according to the embodiment of the present invention. In fig. 2, as in fig. 1, the
The
As the
In the phase difference control, the ambient temperature of the PEM16 (or the temperature of the PEM16 itself) detected by the
That is, in the present modification, the
Further, according to the present invention, the following steps are performed as described above: a step of inputting a feedback signal from the PEM16 by the
In the above-described embodiment and modification, the phase difference control device and the phase difference control method according to the present invention are applied to a CD spectrometer, but the same effects can be obtained when the phase difference control device and the phase difference control method are applied to other spectrometers such as an ellipsometer, an optical rotation spectrometer (ORD), and a linear dichroism spectrometer (LD).
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