Patent Application
20180074197
This application is based upon and claims the benefit of priority from Japanese Patent Application No. 2016-179309 filed Sep. 14, 2016, the entire contents of which are incorporated herein by reference.
The present invention relates to a distance measuring device using pulses of light.
Distance measuring devices using pulses of light are publicly known (for example, refer to Japanese Patent No. 4832720).
These techniques using pulses of light can perform distance measurement with greater accuracy by using a pulse waveform with a narrower pulse width. Directly sampling a pulse waveform by an A/D converter to obtain a digital signal is an ideal method. When a pulse width is narrow, an A/D converter having a high sampling frequency is required. However, the A/D converter having a high sampling frequency tends to (1) be extremely expensive, (2) consume a great amount of power, and (3) generate a great amount of heat.
In response to this problem, as disclosed in Japanese Patent No. 4832720, a method of converting a pulse signal into a damped oscillation waveform by a damping circuit, such as an LC filter, to increase the number of sampling points, was developed.
Distance measuring devices using pulses of light may use a highly sensitive avalanche photodiode (APD) as a photodetector. The APD outputs electric current proportional to the intensity of a beam of detected light when operated under application of a bias voltage. This characteristic is evaluated as an avalanche gain. The characteristic of the avalanche gain varies among products, and thus, a bias voltage to be applied should be finely adjusted in each product in production of distance measuring devices. This adjustment is complicated and is a factor increasing production cost.
In view of these circumstances, an object of the present invention is to provide a highly accurate distance measuring device at low cost.
A first aspect of the present invention provides a distance measuring device using pulses of light, and the device includes a photoelectric transducer, an amplifier circuit, a differential amplifier, damping circuits, and an A/D converter. The photoelectric transducer detects pulsed light that is reflected from an object to be measured. The amplifier circuit converts electric current output from the photoelectric transducer into a voltage pulse signal. The differential amplifier is arranged in a rear stage of the amplifier circuit and differentially amplifies the voltage pulse signal. The damping circuits are arranged in a rear stage of the differential amplifier and convert the pulse signals from the differential amplifier into signals with a damped oscillation waveform. The A/D converter converts the signals with the damped oscillation waveform by A/D conversion. The signal path from the photoelectric transducer to the A/D converter allows a direct current signal to pass therethrough.
According to a second aspect of the present invention, in the first aspect of the present invention, the photoelectric transducer may be a photodiode. According to a third aspect of the present invention, in the second aspect of the present invention, the photodiode may be an avalanche photodiode.
The present invention provides a highly accurate distance measuring device at low cost.
The APD 101 is configured to be applied with the bias voltage through a current limiting circuit 102. The current limiting circuit 102 prevents excessive current from flowing in the APD 101, thereby avoiding the APD 101 from being damaged and deteriorated. The output of the APD 101 is amplified by a transimpedance amplifier (TIA) 103. The TIA 103 is an amplifier that converts an electric current output from the APD 101 into a voltage signal by an IN conversion, and it can be made using a commercially available operational amplifier.
The APD 101 and the TIA 103 do not have a coupling capacitor therebetween. Thus, the output of the APD 101 is directly amplified by the TIA 103. The output of the TIA 103 is input to a differential amplifier 104 and is differentially amplified thereat. The differential output of the differential amplifier 104 is input to damping circuits 105 and 106, which are respectively formed of an LC circuit.
The APD 101 detects a distance measuring light, which is a pulsed light. The outputs of the APD 101, the TIA 103, and the differential amplifier 104 are also pulse signals. The differential amplifier 104 outputs a positive (hot) differential pulse signal and a negative (cold) differential pulse signal, and these differential pulse signals are converted into signals with a damped oscillation waveform by the damping circuits 105 and 106. The detected signals with the damped oscillation waveform are balanced and input to an A/D converter 107 in a rear stage.
The A/D converter 107 converts the detection signals with the damped oscillation waveform into a digital signal. The output of the A/D converter 107 is input to a distance measuring arithmetic circuit 108, and a measured distance is calculated. The calculation method of the measured distance is the same as, or similar to, the method used in an ordinary distance measuring device using pulses of light. The distance measuring arithmetic circuit 108 may be constructed of a dedicated circuit such as an application specific integrated circuit (ASIC) or a programmable logic device (PLD), such as a field programmable gate array (FPGA).
The distance measuring device may further include a pulsed light emitting circuit, a pulsed light emitting optical system, and a pulsed light receiving optical system, a reference light optical path, an entire operation controlling system, and other components, but these are the same as, or similar to, those in an ordinary distance measuring device using pulses of light, and therefore, details thereof are not described.
When a voltage applied to the APD 101 exceeds a predetermined value, avalanche breakdown is generated, and electric current is suddenly made to flow. The voltage at this time is a breakdown voltage. The photodetection is performed in a condition in which the APD 101 is applied with a voltage that is lowered by a predetermined value from the breakdown voltage. For example, when the breakdown voltage is 90 V, the photodetection is performed by applying a voltage that is lower than the breakdown voltage, such as 85 V. Under this condition, light irradiating the APD 101 allows electric current to flow in the APD 101 in accordance with the intensity of the light.
The value of the breakdown voltage varies among APDs. The range of the variation is as great as 80 to 150 V, for example. However, even though the breakdown voltage varies among APDs, applying a voltage lower than the breakdown voltage by a predetermined value enables the APD 101 to provide a desired avalanche gain. That is, different APDs can output electric current having the same value when detecting light having the same intensity.
The circuit of this embodiment is made by DC connection from the APD 101 to the A/D converter 107, and a breakdown current of direct electric current can be detected. Thus, the breakdown voltage is easily determined. The voltage to be applied is made lower than the determined breakdown voltage by a predetermined value to adjust the APD 101.
The structure shown in
The damped oscillation waveform, which is obtained by passing the pulse waveform through each of the damping circuits 105 and 106, is a waveform with damping and repeating oscillation. Even though the same A/D converter having the same sampling frequency is used, a greater number of sampling points that are effective as distance measuring signals is reliably obtained from the damped oscillation waveform compared with the case of using the original pulse waveform. Thus, a sufficient number of sampling points is reliably obtained from a signal even though the signal has a narrow pulse width. This structure enables inexpensive production of a distance measuring device with a high distance measurement accuracy.
The avalanche gain characteristic of the APD 101 varies among products and should be adjusted in each product. The structure shown in
If damping circuits are arranged immediately after the APD 101, and an amplifier is arranged after the damping circuits, an AC coupling capacitor is required before the amplifier. In this circuit structure, an AC signal is required in adjusting the APD, or a separate circuit to detect the breakdown voltage of the APD is necessary. Naturally, the cost of the part is increased. In contrast, in the present embodiment, the adjustment is performed by using a DC signal and is thus performed simply, as described above. Moreover, there is no need for a circuit for the AC signal and for a circuit to be used only for detecting the breakdown of the APD.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2016-179309 | Sep 2016 | JP | national |
