阅读说明：本技术 一种对称类弹头脉冲成形装置及方法 (Symmetrical warhead pulse forming device and method ) 是由 周建斌 范新洋 杨体波 洪旭 王敏 刘易 周伟 马英杰 代光明 胡彪 于 2021-07-01 设计创作，主要内容包括：本发明公开了一种对称类弹头脉冲成形装置及方法,首先通过核辐射信号采集模块采集核辐射信号,并将其处理为离散的负指数核脉冲x(n)；然后通过数字核信号处理模块对离散的负指数核脉冲x(n)进行处理,得到对称类弹头脉冲S(n),并传输至终端进行显示。本发明提出的对称类弹头脉冲成形装置结构简单,运算量小,便于在FPGA中实现；同时本发明提出的对称类弹头脉冲成形方法兼顾了能量分辨率和脉冲通过率等技术需求,成形脉冲参数可调,自适应性强。(The invention discloses a symmetrical warhead pulse forming device and a method, firstly, a nuclear radiation signal acquisition module acquires a nuclear radiation signal and processes the nuclear radiation signal into discrete negative index nuclear pulses x (n); and then processing the discrete negative exponential nuclear pulse x (n) by a digital nuclear signal processing module to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to a terminal for displaying. The symmetrical warhead pulse forming device provided by the invention has the advantages of simple structure and small operand, and is convenient to realize in an FPGA (field programmable gate array); meanwhile, the symmetrical warhead pulse forming method provided by the invention gives consideration to technical requirements such as energy resolution, pulse passing rate and the like, and has adjustable forming pulse parameters and strong adaptability.)

1. A symmetrical warhead pulse forming device is characterized by comprising a nuclear radiation signal acquisition module and a digital nuclear signal processing module, wherein the output end of the nuclear radiation signal acquisition module is connected with the input end of the digital nuclear signal processing module, and the output end of the digital nuclear signal processing module is connected with a terminal;

the nuclear radiation signal acquisition module is used for acquiring a nuclear radiation signal and processing the nuclear radiation signal into discrete negative-index nuclear pulses x (n);

the digital nuclear signal processing module is used for processing the discrete negative index nuclear pulse x (n) to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to a terminal for displaying.

2. The symmetrical warhead pulse shaping device according to claim 1, wherein the nuclear radiation signal acquisition module comprises a nuclear radiation detector, a preamplifier, a conditioning circuit unit and a high-speed analog-to-digital converter which are connected in sequence;

the nuclear radiation detector is used for detecting nuclear radiation signals;

the preamplifier is used for amplifying the nuclear radiation signal to obtain an amplified signal;

the conditioning circuit unit is used for adjusting the amplified signal to obtain an adjusting signal;

the high-speed analog-to-digital converter is used for carrying out digital processing on the adjustment signal to obtain a discrete negative exponential kernel pulse x (n).

3. The symmetrical warhead-like pulse shaping device of claim 1, wherein said digital kernel signal processing module comprises an inverse RC unit, a delay-subtractor unit, a delay-adder unit, a first integrator, a second integrator, and an adder, wherein an input of said inverse RC unit is used as an input of said digital kernel signal processing module, the output terminals of which are connected to the input terminals of the delay-subtractor unit and the delay-adder unit respectively, the output of the delay-subtractor unit is connected to the input of a first integrator, the output of which is connected to the first input of the adder, the output end of the delay-adder unit is connected with the second input end of the adder, the output end of the adder is connected with the input end of a second integrator, and the output end of the second integrator is connected with a terminal;

the inverse RC unit is used for processing the discrete negative exponential nuclear pulse x (n) to obtain a step pulse v (n);

the delay-subtractor unit is used for processing the step pulse v (n) to obtain an inverse double rectangular pulse D1 (n);

the delay-adder unit is used for processing the step pulse v (n) to obtain a forward double-step pulse D2 (n);

the first integrator is used for processing the reverse double rectangular pulse D1(n) to obtain a reverse double-slope pulse P (n);

the adder is used for summing the forward double-step pulse D2(n) and the reverse double-slope pulse P (n) to obtain a symmetrical double-sawtooth pulse R (n);

the second integrator is used for processing the symmetrical double-sawtooth pulse R (n) to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

4. The symmetrical warhead pulse shaping device of claim 3, wherein the expressions of the step pulse v (n), the reverse double rectangular pulse D1(n), the forward double step pulse D2(n), the reverse double ramp pulse P (n), the symmetrical double sawtooth pulse R (n) and the symmetrical warhead pulse S (n) are respectively:

v(n)＝v(n-1)+x(n)-d*x(n-1)

D1(n)＝v(n-K-1)-v(n-1)+v(n-K-L)-v(n-L)

D2(n)＝(v(n)+v(n-K-L))*K

P(n)＝P(n-1)+D1(n)

R(n)＝P(n)+D2(n)

S(n)＝S(n-1)+R(n)

wherein x (·) represents a negative-index nuclear pulse function, v (·) represents a step pulse function, D1(·) represents a reverse double rectangular pulse function, D2(·) represents a forward double step pulse function, P (·) represents a reverse double-slope pulse function, R (·) represents a symmetric double-sawtooth pulse function, S (·) represents a symmetric warhead-like pulse function, n represents a sampling point, D is a first index and D ═ exp (-Ts/τ), Ts represents a sampling period of a high-speed analog-to-digital converter, τ represents a decay time constant, K represents a rise time of a symmetric warhead-like pulse, and L represents a sum of the rise time and a flat-top time of the symmetric warhead-like pulse.

5. A symmetrical warhead pulse forming method is characterized by comprising the following steps:

s1, acquiring a nuclear radiation signal through a nuclear radiation signal acquisition module, and processing the nuclear radiation signal into discrete negative index nuclear pulses x (n);

s2, processing the discrete negative index nuclear pulse x (n) through the digital nuclear signal processing module to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

6. The symmetrical warhead pulse forming method of claim 5, wherein said step S1 comprises the sub-steps of:

s11, detecting a nuclear radiation signal through a nuclear radiation detector;

s12, amplifying the nuclear radiation signal through a preamplifier to obtain an amplified signal;

s13, adjusting the amplified signal through a conditioning circuit unit to obtain an adjusted signal;

s14, the adjustment signal is digitized through a high-speed analog-to-digital converter to obtain discrete negative exponential kernel pulses x (n).

7. The symmetrical warhead pulse forming method of claim 5, wherein said step S2 comprises the sub-steps of:

s21, processing the discrete negative index nuclear pulse x (n) through an inverse RC unit to obtain a step pulse v (n);

s22, processing the step pulse v (n) through a delay-subtractor unit to obtain a reverse double rectangular pulse D1 (n);

s23, processing the step pulse v (n) through the delay-adder unit to obtain a positive direction double step pulse D2 (n);

s24, processing the reverse double rectangular pulse D1(n) through a first integrator to obtain a reverse double-slope pulse P (n);

s25, summing the forward double-step pulse D2(n) and the reverse double-slope pulse P (n) through an adder to obtain a symmetrical double-sawtooth pulse R (n);

and S26, processing the symmetrical double-sawtooth pulse R (n) through a second integrator to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to a terminal for displaying.

8. The method of claim 7, wherein the expressions of the step pulse v (n), the reverse double rectangular pulse D1(n), the forward double step pulse D2(n), the reverse double ramp pulse P (n), the symmetric double sawtooth pulse R (n), and the symmetric warhead pulse S (n) are respectively:

v(n)＝v(n-1)+x(n)-d*x(n-1)

D1(n)＝v(n-K-1)-v(n-1)+v(n-K-L)-v(n-L)

D2(n)＝(v(n)+v(n-K-L))*K

P(n)＝P(n-1)+D1(n)

R(n)＝P(n)+D2(n)

S(n)＝S(n-1)+R(n)

wherein x (·) represents a negative-index nuclear pulse function, v (·) represents a step pulse function, D1(·) represents a reverse double rectangular pulse function, D2(·) represents a forward double step pulse function, P (·) represents a reverse double-slope pulse function, R (·) represents a symmetric double-sawtooth pulse function, S (·) represents a symmetric warhead-like pulse function, n represents a sampling point, D is a first index and D ═ exp (-Ts/τ), Ts represents a sampling period of a high-speed analog-to-digital converter, τ represents a decay time constant, K represents a rise time of a symmetric warhead-like pulse, and L represents a sum of the rise time and a flat-top time of the symmetric warhead-like pulse.

Technical Field

The invention belongs to the technical field of signal processing, and particularly relates to a design of a symmetrical warhead pulse forming device and a method.

Background

With the rapid development of scientific technology, the conventional analog multichannel technology cannot meet the current nuclear radiation measurement requirement due to the defects of complex circuit structure, high design cost, large power consumption, large influence of environmental factors on analog devices and the like, and the high-performance digital multichannel technology gradually becomes the mainstream. The digital nuclear pulse shaping technology is the key of a digital multichannel technology, and a simple and high-performance digital nuclear pulse shaping algorithm not only can reduce the influence of electronic noise, ballistic deficit, pulse accumulation and the like on energy and time resolution, but also can give consideration to the energy resolution and the pulse passing rate, and improve the flexibility and the self-adaptability of the system.

Disclosure of Invention

The invention aims to overcome the defects of the existing analog multichannel technology, and provides a symmetrical bullet pulse forming device and a method, which adopt a digital symmetrical bullet pulse forming mode to improve the energy resolution, the accumulation resistance and the ballistic loss of energy spectrum measurement.

The technical scheme of the invention is as follows: a symmetrical warhead pulse forming device comprises a nuclear radiation signal acquisition module and a digital nuclear signal processing module, wherein the output end of the nuclear radiation signal acquisition module is connected with the input end of the digital nuclear signal processing module, and the output end of the digital nuclear signal processing module is connected with a terminal; the nuclear radiation signal acquisition module is used for acquiring a nuclear radiation signal and processing the nuclear radiation signal into discrete negative-index nuclear pulses x (n); the digital nuclear signal processing module is used for processing the discrete negative index nuclear pulse x (n) to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

Furthermore, the nuclear radiation signal acquisition module comprises a nuclear radiation detector, a preamplifier, a conditioning circuit unit and a high-speed analog-to-digital converter which are connected in sequence; the nuclear radiation detector is used for detecting a nuclear radiation signal; the preamplifier is used for amplifying the nuclear radiation signal to obtain an amplified signal; the conditioning circuit unit is used for adjusting the amplified signal to obtain an adjusting signal; the high-speed analog-to-digital converter is used for carrying out digital processing on the adjustment signal to obtain a discrete negative exponential kernel pulse x (n).

Furthermore, the digital core signal processing module comprises an inverse RC unit, a delay-subtractor unit, a delay-adder unit, a first integrator, a second integrator and an adder, wherein the input end of the inverse RC unit is used as the input end of the digital core signal processing module, the output end of the inverse RC unit is respectively connected with the input end of the delay-subtractor unit and the input end of the delay-adder unit, the output end of the delay-subtractor unit is connected with the input end of the first integrator, the output end of the first integrator is connected with the first input end of the adder, the output end of the delay-adder unit is connected with the second input end of the adder, the output end of the adder is connected with the input end of the second integrator, and the output end of the second integrator is connected with the terminal.

The inverse RC unit is used for processing the discrete negative exponential nuclear pulse x (n) to obtain a step pulse v (n); the delay-subtractor unit is used for processing the step pulse v (n) to obtain an inverse double rectangular pulse D1 (n); the delay-adder unit is used for processing the step pulse v (n) to obtain a forward double-step pulse D2 (n); the first integrator is used for processing the reverse double rectangular pulse D1(n) to obtain a reverse double-slope pulse P (n); the adder is used for summing the forward double-step pulse D2(n) and the reverse double-slope pulse P (n) to obtain a symmetrical double-sawtooth pulse R (n); the second integrator is used for processing the symmetrical double-sawtooth pulse R (n) to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

Further, the expressions of the step pulse v (n), the reverse double rectangular pulse D1(n), the forward double step pulse D2(n), the reverse double ramp pulse p (n), the symmetrical double sawtooth pulse r (n) and the symmetrical warhead pulse s (n) are respectively:

v(n)＝v(n-1)+x(n)-d*x(n-1)

D1(n)＝v(n-K-1)-v(n-1)+v(n-K-L)-v(n-L)

D2(n)＝(v(n)+v(n-K-L))*K

P(n)＝P(n-1)+D1(n)

R(n)＝P(n)+D2(n)

S(n)＝S(n-1)+R(n)

wherein x (·) represents a negative-index nuclear pulse function, v (·) represents a step pulse function, D1(·) represents a reverse double rectangular pulse function, D2(·) represents a forward double step pulse function, P (·) represents a reverse double-slope pulse function, R (·) represents a symmetric double-sawtooth pulse function, S (·) represents a symmetric warhead-like pulse function, n represents a sampling point, D is a first index and D ═ exp (-Ts/τ), Ts represents a sampling period of a high-speed analog-to-digital converter, τ represents a decay time constant, K represents a rise time of a symmetric warhead-like pulse, and L represents a sum of the rise time and a flat-top time of the symmetric warhead-like pulse.

The invention also provides a symmetrical warhead pulse forming method, which comprises the following steps:

and S1, acquiring the nuclear radiation signal through the nuclear radiation signal acquisition module, and processing the nuclear radiation signal into discrete negative-exponential nuclear pulses x (n).

S2, processing the discrete negative index nuclear pulse x (n) through the digital nuclear signal processing module to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

Further, step S1 includes the following substeps:

and S11, detecting a nuclear radiation signal through a nuclear radiation detector.

And S12, amplifying the nuclear radiation signal through a preamplifier to obtain an amplified signal.

And S13, adjusting the amplified signal through the conditioning circuit unit to obtain an adjusted signal.

S14, the adjustment signal is digitized through a high-speed analog-to-digital converter to obtain discrete negative exponential kernel pulses x (n).

Further, step S2 includes the following substeps:

s21, processing the discrete negative exponential kernel pulse x (n) through an inverse RC unit to obtain a step pulse v (n).

And S22, processing the step pulse v (n) through the delay-subtractor unit to obtain an inverse double rectangular pulse D1 (n).

And S23, processing the step pulse v (n) through the delay-adder unit to obtain the forward double-step pulse D2 (n).

And S24, processing the reverse double rectangular pulse D1(n) through a first integrator to obtain a reverse double-slope pulse P (n).

S25, the forward double-step pulse D2(n) and the reverse double-slope pulse P (n) are summed through an adder to obtain a symmetrical double-sawtooth pulse R (n).

And S26, processing the symmetrical double-sawtooth pulse R (n) through a second integrator to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to a terminal for displaying.

Further, the expressions of the step pulse v (n), the reverse double rectangular pulse D1(n), the forward double step pulse D2(n), the reverse double ramp pulse p (n), the symmetrical double sawtooth pulse r (n) and the symmetrical warhead pulse s (n) are respectively:

v(n)＝v(n-1)+x(n)-d*x(n-1)

D1(n)＝v(n-K-1)-v(n-1)+v(n-K-L)-v(n-L)

D2(n)＝(v(n)+v(n-K-L))*K

P(n)＝P(n-1)+D1(n)

R(n)＝P(n)+D2(n)

S(n)＝S(n-1)+R(n)

wherein x (·) represents a negative-index nuclear pulse function, v (·) represents a step pulse function, D1(·) represents a reverse double rectangular pulse function, D2(·) represents a forward double step pulse function, P (·) represents a reverse double-slope pulse function, R (·) represents a symmetric double-sawtooth pulse function, S (·) represents a symmetric warhead-like pulse function, n represents a sampling point, D is a first index and D ═ exp (-Ts/τ), Ts represents a sampling period of a high-speed analog-to-digital converter, τ represents a decay time constant, K represents a rise time of a symmetric warhead-like pulse, and L represents a sum of the rise time and a flat-top time of the symmetric warhead-like pulse.

The invention has the beneficial effects that:

(1) the invention has simple structure and small operand, and is convenient to realize in FPGA.

(2) The invention gives consideration to the technical requirements of energy resolution, pulse passing rate and the like, and has adjustable forming pulse parameters and strong adaptability.

(3) The invention introduces the flat-top time parameter, so that the flat-top parameter is adjustable, and when the flat-top duration is longer than the maximum charge collection time, the amplitude loss caused by ballistic loss can be effectively overcome, thereby accurately extracting the real amplitude of the original pulse.

(4) The invention provides a brand-new digital nuclear pulse forming technology, which is pioneering.

Drawings

Fig. 1 is a block diagram of a symmetrical warhead pulse forming apparatus according to an embodiment of the present invention.

Fig. 2 is a diagram illustrating an effect of pulse shaping of a symmetrical warhead according to an embodiment of the present invention.

Fig. 3 is a flowchart of a symmetrical warhead pulse forming method according to a second embodiment of the present invention.

Fig. 4 is a schematic diagram of pulse signals at each stage of a symmetric warhead pulse forming method according to a second embodiment of the present invention.

Detailed Description

Exemplary embodiments of the present invention will now be described in detail with reference to the accompanying drawings. It is to be understood that the embodiments shown and described in the drawings are merely exemplary and are intended to illustrate the principles and spirit of the invention, not to limit the scope of the invention.

The first embodiment is as follows:

the embodiment of the invention provides a symmetrical warhead pulse forming device, which comprises a nuclear radiation signal acquisition module and a digital nuclear signal processing module, wherein the output end of the nuclear radiation signal acquisition module is connected with the input end of the digital nuclear signal processing module, and the output end of the digital nuclear signal processing module is connected with a terminal, as shown in figure 1.

The nuclear radiation signal acquisition module is used for acquiring a nuclear radiation signal and processing the nuclear radiation signal into discrete negative-index nuclear pulses x (n); the digital nuclear signal processing module is used for processing the discrete negative index nuclear pulse x (n) to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

As shown in fig. 1, the nuclear radiation signal acquisition module includes a nuclear radiation detector, a preamplifier, a conditioning circuit unit and a high-speed analog-to-digital converter, which are connected in sequence; the nuclear radiation detector is used for detecting a nuclear radiation signal; the preamplifier is used for amplifying the nuclear radiation signal to obtain an amplified signal; the conditioning circuit unit is used for adjusting the amplified signal to obtain an adjusting signal; the high-speed analog-to-digital converter is used for carrying out digital processing on the adjustment signal to obtain a discrete negative exponential kernel pulse x (n).

As shown in fig. 1, the digital core signal processing module includes an inverse RC unit, a delay-subtractor unit, a delay-adder unit, a first integrator, a second integrator, and an adder, wherein an input end of the inverse RC unit is used as an input end of the digital core signal processing module, and an output end of the inverse RC unit is connected to an input end of the delay-subtractor unit and an input end of the delay-adder unit, respectively, an output end of the delay-subtractor unit is connected to an input end of the first integrator, an output end of the first integrator is connected to a first input end of the adder, an output end of the delay-adder unit is connected to a second input end of the adder, an output end of the adder is connected to an input end of the second integrator, and an output end of the second integrator is connected to a terminal.

The inverse RC unit is used for processing discrete negative exponential nuclear pulses x (n) to obtain step pulses v (n); the delay-subtractor unit is used for processing the step pulse v (n) to obtain an inverse double rectangular pulse D1 (n); the delay-adder unit is used for processing the step pulse v (n) to obtain a forward double-step pulse D2 (n); the first integrator is used for processing the reverse double rectangular pulse D1(n) to obtain a reverse double-slope pulse P (n); the adder is used for summing the forward double-step pulse D2(n) and the reverse double-slope pulse P (n) to obtain a symmetrical double-sawtooth pulse R (n); the second integrator is used for processing the symmetrical double-sawtooth pulse R (n) to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

In an embodiment of the present invention, expressions of the step pulse v (n), the reverse double rectangular pulse D1(n), the forward double step pulse D2(n), the reverse double slope pulse p (n), the symmetric double sawtooth pulse r (n), and the symmetric warhead pulse s (n) are respectively:

v(n)＝v(n-1)+x(n)-d*x(n-1)

D1(n)＝v(n-K-1)-v(n-1)+v(n-K-L)-v(n-L)

D2(n)＝(v(n)+v(n-K-L))*K

P(n)＝P(n-1)+D1(n)

R(n)＝P(n)+D2(n)

S(n)＝S(n-1)+R(n)

wherein x (·) represents a negative-index nuclear pulse function, v (·) represents a step pulse function, D1(·) represents a reverse double rectangular pulse function, D2(·) represents a forward double step pulse function, P (·) represents a reverse double-slope pulse function, R (·) represents a symmetric double-sawtooth pulse function, S (·) represents a symmetric warhead-like pulse function, n represents a sampling point, D is a first index and D ═ exp (-Ts/τ), Ts represents a sampling period of a high-speed analog-to-digital converter, τ represents a decay time constant, K represents a rise time of a symmetric warhead-like pulse, and L represents a sum of the rise time and a flat-top time of the symmetric warhead-like pulse.

In the embodiment of the present invention, the finally obtained symmetric warhead pulse s (n) is shown in fig. 2, and it can be known from fig. 2 that:

(1) the invention has adjustable forming parameters and strong adaptability.

(2) The method can separate the accumulated pulses, accurately extract pulse amplitude information, and give consideration to technical indexes such as energy resolution, pulse passing rate and the like.

(3) The invention introduces the flat-top time parameter, so that the flat-top parameter is adjustable, and when the flat-top duration is longer than the maximum charge collection time, the amplitude loss caused by ballistic loss can be effectively overcome, thereby accurately extracting the real amplitude of the original pulse.

Example two:

the embodiment of the invention provides a symmetrical warhead pulse forming method, which comprises the following steps of S1-S2 as shown in FIG. 3:

and S1, acquiring the nuclear radiation signal through the nuclear radiation signal acquisition module, and processing the nuclear radiation signal into discrete negative-exponential nuclear pulses x (n).

The step S1 includes the following substeps S11-S14:

and S11, detecting a nuclear radiation signal through a nuclear radiation detector.

And S12, amplifying the nuclear radiation signal through a preamplifier to obtain an amplified signal.

And S13, adjusting the amplified signal through the conditioning circuit unit to obtain an adjusted signal.

S14, the adjustment signal is digitized through a high-speed analog-to-digital converter to obtain discrete negative exponential kernel pulses x (n).

S2, processing the discrete negative index nuclear pulse x (n) through the digital nuclear signal processing module to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to the terminal for displaying.

As shown in fig. 4, step S2 includes the following substeps S21-S26:

s21, processing the discrete negative exponential kernel pulse x (n) through an inverse RC unit to obtain a step pulse v (n).

And S22, processing the step pulse v (n) through the delay-subtractor unit to obtain an inverse double rectangular pulse D1 (n).

And S23, processing the step pulse v (n) through the delay-adder unit to obtain the forward double-step pulse D2 (n).

And S24, processing the reverse double rectangular pulse D1(n) through a first integrator to obtain a reverse double-slope pulse P (n).

S25, the forward double-step pulse D2(n) and the reverse double-slope pulse P (n) are summed through an adder to obtain a symmetrical double-sawtooth pulse R (n).

And S26, processing the symmetrical double-sawtooth pulse R (n) through a second integrator to obtain a symmetrical warhead pulse S (n), and transmitting the symmetrical warhead pulse S (n) to a terminal for displaying.

In an embodiment of the present invention, expressions of the step pulse v (n), the reverse double rectangular pulse D1(n), the forward double step pulse D2(n), the reverse double slope pulse p (n), the symmetric double sawtooth pulse r (n), and the symmetric warhead pulse s (n) are respectively:

v(n)＝v(n-1)+x(n)-d*x(n-1)

D1(n)＝v(n-K-1)-v(n-1)+v(n-K-L)-v(n-L)

D2(n)＝(v(n)+v(n-K-L))*K

P(n)＝P(n-1)+D1(n)

R(n)＝P(n)+D2(n)

S(n)＝S(n-1)+R(n)

wherein x (·) represents a negative-index nuclear pulse function, v (·) represents a step pulse function, D1(·) represents a reverse double rectangular pulse function, D2(·) represents a forward double step pulse function, P (·) represents a reverse double-slope pulse function, R (·) represents a symmetric double-sawtooth pulse function, S (·) represents a symmetric warhead-like pulse function, n represents a sampling point, D is a first index and D ═ exp (-Ts/τ), Ts represents a sampling period of a high-speed analog-to-digital converter, τ represents a decay time constant, K represents a rise time of a symmetric warhead-like pulse, and L represents a sum of the rise time and a flat-top time of the symmetric warhead-like pulse.

The embodiment of the invention introduces the flat-top time parameter, so that the flat-top parameter is adjustable, and when the flat-top duration is longer than the maximum charge collection time, the amplitude loss caused by ballistic loss can be effectively overcome, thereby accurately extracting the real amplitude of the original pulse.

It will be appreciated by those of ordinary skill in the art that the embodiments described herein are intended to assist the reader in understanding the principles of the invention and are to be construed as being without limitation to such specifically recited embodiments and examples. Those skilled in the art can make various other specific changes and combinations based on the teachings of the present invention without departing from the spirit of the invention, and these changes and combinations are within the scope of the invention.