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Active quenching circuit used for APD detector in Geiger mode

A technology of quenching circuit and Geiger mode, which is applied in the direction of protection equipment, etc., can solve the problems that continuous random detection cannot be realized, and achieve the effect of random continuous detection, simple and compact circuit structure, and low power consumption

Inactive Publication Date: 2016-06-22
TIANJIN UNIV
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Problems solved by technology

The gating mode can well solve the problem of large avalanche current and afterpulse, but the premise is that the arrival time of the photons is known, so this circuit structure is only suitable for the overhead detection of the airborne platform, but for the random arrival of photons Front-illuminated detection cannot be used, and continuous random detection cannot be achieved

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  • Active quenching circuit used for APD detector in Geiger mode
  • Active quenching circuit used for APD detector in Geiger mode
  • Active quenching circuit used for APD detector in Geiger mode

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Embodiment Construction

[0021] The technical solution of the present invention will be further described in detail below in conjunction with the accompanying drawings and specific embodiments, and the described specific embodiments are only for explaining and illustrating the present invention, and are not intended to limit the present invention.

[0022] Compared with passive quenching circuits and gated mode circuits, active quenching circuits are more versatile. In general, the design idea is to convert the avalanche current into an avalanche voltage signal, and make the bias voltage between the two poles of the APD detector lower than the avalanche voltage V through the feedback structure. B , to achieve quenching of the APD detector. At the same time, the avalanche voltage signal will turn on the hold-off circuit behind to delay the APD detector to ensure that the photoelectrons captured by the trap can be released and annihilated by the trap within this delay, thereby reducing the after-pulse e...

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Abstract

The invention discloses an active quenching circuit used for an APD detector in a Geiger mode, and the circuit comprises an nmos tube M1, an nmos tube M2, a pmos tube M3, an nmos tube M4, a pmos tube M5, a pmos tube M6, an nmos tube M7, an nmos tube M8, a capacitor C1, a phase inverter Inv1, a phase inverter Inv2, and an NAND gate NAND. A drain electrode of the nmos tube M1 is connected with the anode of the APD detector, and the cathode of the APD detector is connected with a biasing reversal high-voltage VB+ex. The subnanosecond-level active quenching and quick resetting of the APD detector or an APD array are achieved through a feedback structure, and the quenching time is at a subnanosecond level. The maximum hold-off time is 5ns, and can be adjusted automatically according to the actual condition. The whole circuit structure is simple and compact, is small in area, is low in power consumption, is high in speed, is suitable for the quenching of a single or pixel-level APD detector, and reliably guarantees that the APD detector achieves the random continuous detection and the service life of a device is prolonged.

Description

technical field [0001] The invention belongs to the field of laser detection and readout circuits, in particular to an active quenching circuit applied to a Geiger mode APD detector. Background technique [0002] In 1953, K.G. McKay and K.B. McAfee discovered the multiplication phenomenon of silicon germanium photocurrent. More than ten years later, in 1965, the first avalanche photodiode (Avalanche PhotoDiode, APD) came out. This optoelectronic device has excellent characteristics different from other optoelectronic devices. at avalanche voltages above V B Under the reverse bias voltage bias, it has the ability to respond to a single photon and has extremely high detection sensitivity. APD is a photodetection device based on the internal photoelectric effect and has an internal high gain. The photogenerated carriers form an avalanche effect under the action of a high electric field to obtain a macroscopic photocurrent. It is the most promising photodetection device in re...

Claims

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Application Information

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IPC IPC(8): G01D3/08
CPCG01D3/08
Inventor 赵毅强赵佳姮夏显召赵公元刘银齐王景帅
Owner TIANJIN UNIV
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