The advantages of the secondary
electron emission tube are high repetition frequency, small
trigger delay and shaking, and the
disadvantage is that the pulse output
voltage amplitude is only a few hundred volts, and the life is short, unstable, and noisy; the
discharge gap switch, such as the
spark gap, is prone to thousands of pulses. Larger pulse amplitude above volts and shorter sub-
nanosecond rise time, but low repetition frequency and large shaking; such as the
Chinese patent "Automatic Intelligent Strong Fast Edge
Electromagnetic Pulse Generator" (CN102323501B), using an air gap spark switch , can generate a single-edge pulse with a
rise time of 2.3±0.5ns, but its pulse width is narrow and cannot be adjusted arbitrarily, and there is no technical solution for the adjustability of pulse amplitude and repetition frequency; the working voltage of the trigger tube can reach ten Thousands of volts, the
disadvantage is that the trigger
pulse voltage is high and the vibration is large; the
operating voltage range of the
thyristor can reach hundreds of kilovolts, the switching speed is
nanosecond level, and the repetition frequency is also high. The
disadvantage is that the vibration is large and the volume is large. For example, the
Chinese patent "ultra-compact high-voltage
nanosecond pulse source" with the publication number CN104158430A has a total weight of nearly 100kg. At the same time, the device with this type of device as the core is complex overall and has many
peripheral drives, which reduces reliability and limits its use. The scope of application, especially in the occasions with high precision requirements and small size
Although it has been reported in the literature that the repetition frequency of the avalanche tube
pulse power supply can reach several kHz, it is almost impossible to achieve more than tens of kHz.
At the same time, since the avalanche working voltage of the avalanche tube has an optimal range, especially the output voltage of the
single tube is low, to increase the output voltage, the Marx circuit must be combined with the series connection of multiple tubes, which is affected by the
internal resistance of the avalanche
triode series circuit. When the number of tubes in series increases, the output pulse amplitude does not increase significantly, and the output voltage is difficult to achieve continuous adjustment, so the application of avalanche tubes is greatly limited
Such as the
Chinese patent "A kind of electro-optic Q-switching switch driving power supply", the pulse power supply in (CN101719624A) is to use double MOSFETs in parallel, and switch in turn to increase the
operating frequency, but it does not involve how to reduce the output pulse rise /
fall time and improve the reliability of the circuit. properties, etc., and the patent also cannot realize continuous adjustable pulse width
The Chinese patent "A Method for Realizing a High-
Voltage Square Wave Generator" (CN103684360A) uses an avalanche tube and
MOSFET to form a high-voltage switch to generate a high-voltage
square wave, but its output voltage is only 300-1000V, and the adjustable pulse width is only 10-220μs. The specific repetition frequency,
duty cycle and high-voltage pulse rising / falling edge time are also not given in the embodiment, and its practicability is undoubtedly limited
Chinese patent "A
High Voltage Square Wave Generator with Adjustable Pulse Width and
High Voltage Square Wave Generation Method" (CN105391428A), using MOSFET pair tubes to realize
high voltage switching, the repetition frequency can reach 3.3MHz, and the rising / falling edge time is several ns , but its output voltage is only -200 ~ 50V
The utility model patent "An All-
Solid High-
Voltage Pulse Power Supply Device" (CN202550918U) uses a large number of MOSFETs and IGBTs in series and parallel switches, but the repetition frequency is only 10Hz-1kHz and the maximum
duty cycle is 1%, so no specific details can be given.
High voltage pulse rising / falling edge time, indicating that the power supply can not really get fast edge
high voltage pulse
In 2007, ThomasP.Rutten et al disclosed a MOSFET high-voltage pulse circuit in Review of Scientific Instruments ("REVIEW OF SCIENTIFIC INSTRUMENTS", Vol.78, P073108). Its
operating frequency is only 1kHz, and the pulse width cannot be continuously adjusted.
In 2011, Xian-wang Feng et al published a MOSFET high-voltage pulse circuit in
Scientific Instrument Review ("REVIEW OF SCIENTIFIC INSTRUMENTS" Vol.82, P075102), the rising edge is slow (~49.04ns), and the maximum voltage is only 3000V. Whether the width and working frequency can be continuously adjusted, the literature has not been involved
The special high-current "overdrive" circuit used in the literature is a pulse generated by the avalanche tube avalanche. From the measured
pulse waveform, the voltage actually loaded on the gate of the MOSFET is always accompanied by a large reverse pulse. The driving voltage puts the MOSFET tube in extreme working conditions, which can easily cause damage to the MOSFET tube
Furthermore, when multi-stage MOSFETs are cascaded, each stage is driven by pulses generated by an independent avalanche circuit, and the number of cascaded MOSFETs increases, so it is obviously very difficult to synchronize the avalanche circuit within a few ns
Therefore, this technology cannot achieve continuous adjustable pulse width and frequency, nor can it obtain higher-amplitude high-voltage pulses, nor can it simultaneously realize the flexible output of boost or decompression high-voltage pulses with only one fast edge according to needs.
Since the pulse generation principle is obtained by charging and discharging the load
capacitance, when the load
capacitance value changes greatly, or the load is not a capacitance, how to ensure the normal operation of the pulse source, the literature does not give a good solution