introduction
The nuclear energy spectrum amplifier is an important part of the energy spectrum measurement system, and its performance directly affects the resolution of the entire energy spectrum measurement system. This paper improves the shortcomings of the traditional nuclear energy spectrum signal amplifier. A universal nuclear energy spectrum signal amplifier with programmable amplification factor is designed and developed, so that it can be used in nuclear energy spectrum measurement instruments such as X-ray fluorescence instrument and gamma spectrometer at the same time, and has universality. If the amplifier further integrates signal acquisition (A/D conversion) technology and digital signal processing (DSP) technology, it can constitute a fully functional nuclear energy spectrum signal processing system.
1 Basic circuit components
The circuit mainly includes three parts: filter shaping, program-controlled amplification, and baseline elimination. The filter shaping circuit includes pole-zero phase cancellation, four-stage Butterworth filter circuit, and polarity selection circuit; the program-controlled amplification circuit includes a first-stage 20-fold amplification and a 12-bit DAC program-controlled amplification circuit; the baseline elimination circuit includes a DC removal circuit, an inverting circuit, and a voltage follower circuit. The structural block diagram is shown in Figure 1.
2 Unit Circuit Principle Analysis
2.1 Pole-zero cancellation
Connecting the pole-zero phase cancellation circuit to the signal input terminal can eliminate the downstroke caused by differentiating the probe signal, making the pulse return to the baseline monotonically. It improves the effects of count rate overload and pulse amplitude superposition, and is suitable for high-resolution and high-count rate spectrometer systems. Figure 2 shows the designed circuit and experimental test signal diagram.
2.2 Filter shaping
The circuit uses two second-order Butterworth filter circuits cascaded into a fourth-order Butterworth filter circuit. The second-order low-pass Butterworth filter circuit designed with an operational amplifier is directly obtained by using the frequency domain analysis method:
In the formula: k is equivalent to the voltage gain of the common-mode amplifier, which is called the passband gain of the filter; Q is the quality factor; ω0 is the characteristic angular frequency. Figure 3 is the design principle diagram of the filter shaping circuit, and Figure 4 is the experimental test results.
This circuit uses two parts: a first-stage 100-fold fixed amplification and a DAC programmable multiple amplification. The first-stage amplification uses operational amplifier positive feedback. The DAC programmable multiple amplification part controls the 12-bit high-speed DAC chip through a single-chip microcomputer, and uses the DAC's internal precision resistor network as the operational amplifier's feedback resistor to improve the amplification accuracy and achieve 1 to 1,000 times programmable amplification. Output voltage:
Wherein, the value range of D is 0 to 4 095.
The DAC programmable amplifier circuit is shown in Figure 5.
2.4 Baseline elimination
The baseline elimination circuit first inputs the shaped nuclear pulse signal into a first-order low-pass filter circuit to extract the DC component, and then subtracts it from the original signal to remove the DC component. The circuit implementation is shown in Figure 6.
3 Main performance indicators
After the programmable nuclear energy spectrum signal amplifier circuit designed in this paper has been made into a board, welded, and debugged, the power supply adopts a 7-20 V regulated power supply, and the circuit converts it to the required +5 V, -5 V. The signal input end passes through the pole-zero cancellation circuit. After debugging, the R and C values are changed according to the frequency requirements of different inputs (X fluorescence and gamma rays) to achieve pole-zero cancellation. The subsequent first-stage amplification and shaping filtering of the nuclear signal are connected. The output signal is a quasi-Gaussian waveform with a flat top of the pulse. The DAC is controlled by a single-chip microcomputer. After testing, the programmable signal is amplified by 0 to 100 times, which fully realizes the design requirements. Figure 7 is the final test output waveform.
4 Conclusion
The programmable nuclear energy spectrum signal amplifier designed in this paper has been analyzed and designed, and the circuit board, welding and debugging have been proved by experiments to meet the design requirements of filtering and shaping the energy spectrum signal and 0-100 times programmable amplification. This design can be used in X-ray fluorescence and gamma spectrum measurement systems, achieving the versatility and flexibility of the design requirements. Compared with traditional nuclear signal amplification and shaping, the programmable signal amplifier designed in this paper also has the advantages of low power consumption and easy hardware miniaturization, meeting the design requirements of modern nuclear signal processing.
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