YANG De-qiang, PAN Jin, ZHAO Zhi-qin, and NIE Zai-ping

(School of Electronic Engineering, University of Electronic Science and Technology of China Chengdu 610054)

Design of Balanced Output High-Voltage Nanosecond Pulse Source for Symmetrical Antenna

YANG De-qiang, PAN Jin, ZHAO Zhi-qin, and NIE Zai-ping

(School of Electronic Engineering, University of Electronic Science and Technology of China Chengdu 610054)

Time-domain impulse generator is a very important unit in time-domain ultra-band radar systems.Most time-domain impulse antennas are symmetrically designed which require balanced output pulse generators in order to realize wideband matching. Aiming to solve the compatible problem of high voltage and balanced output,which commonly exists in high-voltage pulse generators, this paper designs a new pulse generator circuit, the cascade Marx circuit with balanced output. With this generator and a loaded bow-tie antenna, a 300 V nanosecond pulse was generated. The measured result validates the effectiveness of the proposed pulse generator.

balanced output; Marx circuit; nanosecond pulse; symmetrical antenna

The time-domain impulse has been widely used in ground penetrating radar (GPR) for concealed targets detection[1]. The antennas used for transmission are usually symmetrically designed in order to realize wideband matching[2-4]. Therefore, pulse generator with balanced output is adopted. In radar system, the detection range is a very important parameter. Usually high amplitude output of the pulse generator is demanded for long distance detection. However, it is impossible for a single avalanche transistor to produce such high amplitude output (e.g. hundreds of volts).Cascade Marx circuit can significantly promote the output voltage. But this kind of circuit usually provides unbalanced output[5-8]. Therefore, an unbalancedto-balanced conversion should be taken on the symmetrical antenna which is extremely difficult for ultra-band time-domain pulse. In order to solve the compatible problem of high voltage and balanced output, this paper designs a new pulse generator circuit,which uses the cascade Marx circuit with balanced output. Experimental result shows that the new pulse generator can meet the requirements of balanced output and high amplitude of a bipolar pulse.

1 Design of the Symmetrical Marx Circuit

In recent years, due to the emergence of high performance avalanche transistors, it is possible to miniaturize the size of solid high-voltage pulse generator, which has been widely used in the pulse circuits. When the transistor's collector voltage is high enough, its amplitude of electric field in the chargeregion of the junction is many times higher than that at the normal low-pressure condition. The carriers in the collector are accelerated by the strong electric field,leading to huge energies. Their collisions with the lattice give rise to new electron-hole pairs. Then the newly generated electron-hole pairs will be accelerated again in the electric field. Repeating the above process,the currents flow through the collector will rapidly grow and bring avalanche multiplication phenomenon.This is the transistor's avalanche multiplication phenomenon. The obvious multiplication phenomenon of the transistor is called as the avalanche transistors.

Fig. 1 gives the circuit diagram of a pulse generator. The base of the avalanche transistor is reverse biased. The working voltage reaches the requirements of avalanche zone. Before the arrival of the trigger pulse, the avalanche transistor is cut off.The VCC voltage source charges the capacitor C2through the R4resistor and the R3resistor, as illustrated by the line ① in the Fig. 1. When the trigger pulse arrives, the transistor turns on rapidly. The capacitor C2rapidly discharges through its own small resistance to the ground. Since the voltage across the capacitor can not abruptly jump, a negative pulse in the output terminal will be generated. Confined by the voltage characteristics of the transistor, usually this transistor can only produce tens of volts pulse. If one wants to generate larger pulse, cascade circuit is always adopted.

Fig. 1 The circuit diagram of a pulse generator

Fig. 2 is a principle sketch map of the Marx circuit. When the switchers S turn off, all the capacitances C are on charge. When the switchers turn on, all the capacitances discharge which produce a high-voltage pulse. The theoretical output voltage of the pulse is Uout=N× VCC , where N is the total number of the capacitances, and VCC is the voltage of the electric power. The avalanche transistor is a very suitable switcher. Using avalanche transistor can miniaturize the size of the pulse generator.

The same capacitances can be set for each capacitor at all levels, i.e. C1= C2== CN, hence the actual capacitance in the discharge process equals to C=CNN. The smaller the capacitance is, the lower the pulse amplitude will be. Nevertheless, the pulse will be narrower. Whereas, the bigger the capacitance is, the higher the pulse amplitude is, but the wider the pulse width will be. Vice versa.

Fig. 2 The principle sketch map of the Marx circuit

As shown in Fig.3, when the avalanche transistors are biased at the critical avalanche state, the power charges for capacitors C2and C3through the resistors R1, R2and R4. When a trigger pulse arrives, the transistor will be avalanche breakdown. Because the voltages across the capacitors can not abruptly jump, a positive pulse and a negative pulse at the output port will be generated.

Then they can be used as a balanced symmetrical output pulse source directly connected to a symmetrical antenna. Different from the non-symmetrical pulse, it does not need the unbalanced-to-balanced conversion. It can directly match the time-domain wideband antenna.Therefore, the symmetrical pulse is very important. It can improve the antenna radiation efficiency and reduce the pulse tail.

Fig. 3 The trigger port of symmetrical Marx circuit with balanced output

Because of the breakdown voltage characteristics of the transistor in Fig. 3, usually it is very difficulty to generate a pulse which is higher than 100 V using single level Max circuit. Some references also proposed how to generate pulses with hundreds or even thousands volts using cascade circuit. But they are all non-symmetrical pulses. It has never reported how to generate a symmetrical nanosecond pulse with hundreds volts with cascade circuit. In this paper, a cascade Marx circuit with balanced output is proposed.

Fig. 4 The sketch map of the 5 cascade stages balanced output Marx circuit

The new cascade Marx circuit with balanced output proposed in this paper is shown in Fig. 4. The amplitude of the input trigger is larger than 1 V and the pulse wide is less than 10 ns. The trigger signal is transformed into one positive and one negative trigger pulses by T1. The positive trigger pulse makes the cascade Marx circuits which consist of the avalanche transistors T2～T6avalanche continuously to produce a positive high amplitude pulse. At the same time, the negative trigger pulse makes the serial Marx circuits which consist of the avalanche transistors T7～T11avalanche continuously to produce a negative high amplitude pulse. The amplitude of the output pulse generated by this circuit can be up to ±10 kV.

2 Experimental Results

A balanced output pulse generator with 0.5 ns wide and ±300 V amplitude has been realized. Fig. 5 and Fig. 6 show the photographs of the circuit board and the antenna.

Fig. 5 The photographs of the circuit board

Fig. 6 The photographs of the circuit board and the antenna

The experiment of transmitting/receiving a nanosecond pulse is performed by combining the new designed circuit with a bow-tie. The corresponding wave form was recorded by the LeCroy wavepro 7Zi oscillograph as shown in Fig. 7. The tailing of the waveform is very small. The waveform in Fig. 7 is better than that in Ref. [2]. The amplitude and the width of the pulse in Fig. 7 are 3.375 V and 0.5 ns,respectively.

Fig. 7 The wave form in the transmitting/receiving experiment

3 Conclusions

The high-voltage nanosecond pulse generator with balanced output designed in this paper possesses prominent advantages when performing with the symmetrical antenna. Due to the feature of the balanced output, complicated unbalanced-to-balanced conversion can be avoided. The design provides an effective way for producing high amplitude pulse with balanced output. Experimental result has proved the effectiveness of the idea in the paper.

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[2] CHEN Ye, JOINES W T, XIE Zhen-tian, et al. Double-sided exponentially tapered GPR antenna and its transmission line feed structure[J]. IEEE Trans. on Antennas and Propagation,2006，54(9): 2615-2623.

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適合對稱天線的平衡輸出高壓納秒級脈沖源研究

楊德強，潘 錦，趙志欽，聶在平

(電子科技大學(xué)電子工程學(xué)院 成都 610054)

時域脈沖源是時域超寬帶雷達系統(tǒng)中的重要部件，時域脈沖天線大多采用對稱形式，如果用非平衡高壓脈沖源激勵，難以實現(xiàn)很好的寬帶匹配。為此設(shè)計了一種新的電路形式，采用平衡輸出的Marx電路級聯(lián)，解決了脈沖源高幅度和平衡輸出不能兼顧的問題。利用與對稱天線進行的納秒級脈沖收發(fā)實驗驗證了該電路的良好性能。

平衡輸出; Marx電路; 納秒級脈沖; 對稱天線

TN784.1

A

10.3969/j.issn.1001-0548.2011.03.007

2010 ? 11 ? 29;

2011 ? 02 ? 25

國家自然科學(xué)基金(60771042)；高等學(xué)校學(xué)科創(chuàng)新引智計劃(B07046)；國家自然科學(xué)基金委與中國工程物理研究院資助(10776003)

楊德強(1971 ? )，男，博士生，主要從事微波技術(shù)和天線以及瞬變電磁場方面的研究.

date: 2010 ? 11 ? 29; Revised date: 2011 ? 02 ? 25

Supported by the NSFC (60771042 ), 111 project (B07046)，Supported by NSAF(10776003)

Biography: Yang De-qiang, Research interstests include microwave engineering and antenna, transient electromagnetic.

編 輯 稅 紅