Photoelectric conversion device
Abstract
[Purpose] The process of multiplying each signal by a coefficient is performed. [Constitution] Multiple photoelectric conversion elements (B)1 B4), The photoelectric conversion device is provided, wherein an amplifier (A1 ... A4) capable of controlling a gain from the outside is provided at an output terminal of each photoelectric conversion element.
Term
Term ended
Projected expiry passed 28 May 2013, 13.3 years ago.
- Priority and filed
- Published
- Projected expiry
- Today
1 claim: 1 independent, 0 dependent
- 1【特許請求の範囲】 【請求項1】 複数の光電変換要素よりなる光電変換装置において、各光電変換要素の出力端子に、利得を外部より制御できる増幅器を設けたことを特徴とする光電変換装置。
94 paragraphs, as filed
Description: TECHNICAL FIELD [Detailed description of the invention]
【0001】
[Industrial application field]
The present invention relates to a photoelectric conversion device used as a copier, a facsimile, a video camera recorder, an AE sensor of a camera, and an AF sensor.
【0002】
[Explanation of background technology]
In recent years, electronic technology has advanced to a high degree, and even in the field of solid-state image sensors as photoelectric conversion devices, high definition and high image quality have been rapidly realized. By the way, it is very rare that the output signal from the solid-state image sensor is used as it is, and after several stages of signal processing, for example, a TV signal or the like is created.
【0003】
PROBLEM TO BE SOLVED: To solve a technical problem
Therefore, when the number of pixels is increased for high definition, a huge amount of calculation and processing are required in signal processing, and high image quality may be rate-determined by signal processing.
【0004】
[Means for solving problems]
An object of the present invention is to provide a solid-state image sensor that outputs a signal obtained by multiplying each signal by a coefficient in order to incorporate a signal processing function into the solid-state image sensor.
【0005】
The above-mentioned object is achieved by a photoelectric conversion device including a plurality of photoelectric conversion elements, wherein an amplifier capable of controlling a gain from the outside is provided at an output terminal of each photoelectric conversion element.
【0006】
[Example]
(Example 1) FIG. 1 shows a first embodiment according to the present invention. In this embodiment, bipolar photoelectric conversion elements are arranged one-dimensionally as photoelectric conversion elements, and each base region is a MIMO transistor M.<sub>11</sub>~ M<sub>14</sub>It is connected via.
【0007】
Further, amplifiers A1 to A4 are independently connected to the emitter output line of each photoelectric conversion element.
【0008】
The operation of this embodiment will be briefly described with reference to the timing chart of FIG.
【0009】
First, time t<sub>1</sub> In φ<sub>R</sub> When a low level pulse is applied to, the MIMO transistor M<sub>11</sub>~ M<sub>14</sub>Turns on, and bipolar transistor B<sub>1</sub> ~ B<sub>4</sub> Is connected in common and V<sub>BR</sub>It is reset to voltage. Then φ<sub>R</sub> By rising to the Middle level, the MIMO transistor M<sub>11</sub>~ M<sub>14</sub>Turns off and the reset operation ends (clamp reset).
【0010】
Then time t<sub>2</sub> In φ<sub>VC1</sub> When the pulse rises, the NMOS transistor M<sub>21</sub>~ M<sub>24</sub>Turns on, and bipolar transistor B<sub>1</sub> ~ B<sub>4</sub> All emitter terminals are V<sub>VC</sub>Reset to voltage and then time t<sub>3</sub> In φ<sub>R</sub> When the pulse rises to the High level, the bipolar transistor B<sub>1</sub> ~ B<sub>4</sub> Base potential is capacitance C<sub>1</sub> ~ C<sub>4</sub> It is lifted through, and the base and emitter are in a forward bias state, the bipolar transistors perform emitter follower operation all at once, the holes on the base are recombined, and the base potential is V.<sub>VC</sub>+ V<sub>BE</sub>Settle in the vicinity (transient reset operation). Time t when the transient reset operation ends<sub>4</sub> In φ<sub>R</sub> The pulse drops to the Middle level, so the capacitance C<sub>1</sub> ~ C<sub>4</sub> The base potential of each bipolar transistor also drops, and the base-emitter is in a reverse bias state. From this state, the accumulation operation of the optical carrier is started.
【0011】
After the predetermined accumulation time has elapsed, the time t<sub>3</sub> In φ<sub>T</sub> And φ<sub>R</sub> When the pulse of is raised to the High level, the NMOS transistor M<sub>31</sub>~ M<sub>34</sub>Bipolar transistor B as soon as<sub>1</sub> ~ B<sub>4</sub> The base potential of is raised, the bias between the base and the emitter becomes a forward bias state, and the optical carriers accumulated on the base are output from the emitter terminal. At this time, if a predetermined voltage is applied from the power supply 2 to the control terminals of the amplifiers A1 to A4, each amplifier can have a desired gain.
【0012】
The output of amplifiers A1 to A4 is C<sub>T1</sub>~ C<sub>T4</sub>Read out at time t<sub>6</sub> In φ<sub>T</sub> When the pulse drops to the low level, the NMOS transistor M<sub>31</sub>~ M<sub>34</sub>Turns off and each capacity C<sub>T1</sub>~ C<sub>T4</sub>Voltage is retained.
【0013】
Then time t<sub>7</sub> In φ<sub>RES</sub> Apply a high level pulse to the NMOS transistor M<sub>RS</sub>Is turned on, the output line 4 is reset, and then the scanning circuit 1 is operated, and C<sub>T1</sub>Output terminal V via output buffer 3 in order from the above signal<sub>out out</sub> By transferring to, the series of operations is completed.
【0014】
By the way, suitable circuit examples of amplifiers A1 to A4 and their DC characteristic diagrams are shown in FIGS. 3 and 4.
【0015】
FIG. 3 shows an inverting amplifier using an NPN transistor, and the gain is controlled by the gate voltage of the NMOS transistor provided at the emitter terminal.
【0016】
Figure 4 shows the DC characteristic calculation results of this inverting amplifier.
【0017】
Input voltage V on the horizontal axis<sub>IN</sub>, Output voltage V on the vertical axis<sub>out out</sub> And gain control voltage V<sub>C</sub> Is a graph of the parameters. As you can see from the figure, V<sub>C</sub> The larger the value, the larger the gain and the smaller the circuit scale, which is suitable for this embodiment. Needless to say, other types of amplifiers may be used.
【0018】
(Example 2) FIG. 5 shows a second embodiment according to the present invention. This embodiment is an improvement of the first embodiment, the power supply device 2 is omitted, and the gain control voltage of the amplifiers A1 to A4 is input serially from the V-GAIN terminal. ..
【0019】
For example, during the storage period, the scanning circuit 1 is operated, the NMOS transistor M51 is turned on, the gain control voltage of the amplifier A1 is written from the V-GAIN terminal, then the pulse of L1 is set to the low level, and M51 is set. Turn it off and hold the written voltage. This operation is performed sequentially from amplifiers A1 to A4, and after the operation is completed, φ<sub>R</sub> When the pulse is set to High level, each photoelectric conversion element performs a read operation, and the voltage obtained by multiplying each output value by the gain is C.<sub>T1</sub>~ C<sub>T4</sub>Is read out.
【0020】
Operations other than the above can be performed in exactly the same manner as in the first embodiment.
【0021】
Therefore, a significant space saving can be realized as compared with providing a power supply for each amplifier.
【0022】
In the above operation description, the gain control voltage of the amplifiers A1 to A4 is written during the accumulation period, but other periods may be used, for example, C.<sub>T1</sub>~ C<sub>T4</sub>This may be done during the sequential transfer of the charges. In this case, the gain control voltage written to the amplifiers A1 to A4 will be used in the next photoelectric conversion operation.
【0023】
(Example 3) FIG. 6 shows a third embodiment according to the present invention. This embodiment is developed in a two-dimensional photoelectric conversion device of the second embodiment, and a vertical scanning circuit 5 is provided in order to sequentially perform the resetting of the photoelectric conversion element and the signal reading operation in line units. , The basic operation is exactly the same as in the second embodiment.
【0024】
(Example 4) FIG. 7 shows a fourth embodiment of the present invention. In the first to third embodiments, the photoelectric conversion unit is an example in which a bipolar amplification element having a base and collector junction as a photodiode is used, but in this embodiment, MOS is used. The parts similar to the conventional ones are given the same number and the description thereof will be omitted. In No. 11, a photodiode is connected to the gate of the MOS, while the resistance of the MOS amplifier is a variable resistance as shown in 10. The variable resistor of 10 has a double structure of the MOS gate, and as shown in 12, one 13 of the lower gate is connected to the power supply and the other 14 of the upper gate is applied with a voltage pulse. It has become like.
【0025】
The potential of the floating gate changes according to the amplitude of the voltage pulse, so that the MOS shown in 10 acts as a variable resistor. Also in the case of this experiment, the optical signal generated by the photodiode is converted into a value obtained by multiplying the amplifier gain determined by the above 10 variable resistors, and this modulated signal is sequentially read by the shift register via the read capacitance.
【0026】
Although FIG. 7 shows an example of a one-dimensional sensor, it goes without saying that the present invention is not limited to one-dimensional and can be used as a two-dimensional sensor.
【0027】
(Example 5) FIG. 8 shows a fifth embodiment of the present invention. In Sij (ij = 1 to 4), as shown in 11, the base separation PBSO12 and the base potential control capacitance 13 are composed of bipolar 15.
【0028】
Cell S<sub>11</sub>S<sub>21</sub>Is output to vertical line 16, while cell S<sub>12</sub>S<sub>22</sub>Is output to vertical line 17. The selection of each line is pulse φ<sub>PR1</sub> , Φ<sub>PR2</sub> Is done by.
【0029】
First, φ<sub>PR1</sub> High pulse is applied to S<sub>11</sub>And S<sub>12</sub>A cell is selected and each output goes up and down at the same time.<sub>ij</sub>It is read to the gate of (i, j = 1, 2).
【0030】
Each amplifier gain is adjusted from the voltage sources wired above and below through the wiring of 18, 19, 20, and 21, and the amplifier outlet is φ.<sub>PT1</sub> Set the pulse to a high level and S<sub>11</sub>To the light output of a<sub>11</sub>Output to capacity 22 with the amplifier gain of<sub>12</sub>To the light output of a<sub>12</sub>Output with amplifier gain applied to capacity 23, S<sub>11</sub>To the light output of a<sub>21</sub>Output with amp gain applied to capacity 24, while S<sub>21</sub>To the light output of a<sub>22</sub>The output to which the amplifier gain of is applied is read out to the capacity 25.
【0031】
Next φ<sub>PR1</sub> To D-level, φ<sub>PR2</sub> At high level, cell S<sub>21</sub>, S<sub>22</sub>Is selected and a as before<sub>ij</sub>It is read to the gate of the amplifier (ij = 1 ~ 2').
【0032】
φ<sub>PT2</sub> To high level S<sub>11</sub>A to the optical output of the cell<sub>11</sub>Output with amp gain applied to capacity 26, S<sub>12</sub>A to the optical output of the cell<sub>12</sub>Output with amp gain applied to capacity 27, S<sub>21</sub>A to the optical output of the cell<sub>21</sub>Output with amp gain applied to capacity 28, S<sub>22</sub>A to the optical output of the cell<sub>22</sub>The output to which the amplifier gain is applied is read out to the capacity 29.
【0033】
The signals read to the capacities 22, 23, 26 and 27 are added via the capacities 30, 31, 32 and 33 and are added from the amplifier 38, while the signals read to the capacities 24, 25, 28 and 29 are the capacities 34 and 35. It is output from the amplifier 39 added via 36 and 37.
【0034】
The outputs of 38 and 39 are subtracted by the differential amplifier 40. Therefore, the gain may be a mixture of plus and minus, and has the advantage that the Fourier transform output of the image is read out at high speed.
【0035】
[Effect of the invention]
According to the present invention, signal processing in which an arbitrary coefficient is applied to each signal can be satisfactorily performed.
[Simple explanation of drawings]
[Figure 1]
It is a circuit block diagram of the photoelectric conversion apparatus according to Example 1 of this invention.
[Figure 2]
It is a timing chart for demonstrating the operation of the photoelectric conversion apparatus according to Example 1.
[Fig. 3]
It is a circuit diagram of the amplifier used in this invention.
[Fig. 4]
It is a graph which shows the characteristic of the amplifier shown in FIG.
[Fig. 5]
It is a circuit block diagram of the photoelectric conversion apparatus according to Example 2 of this invention.
[Fig. 6]
It is a circuit block diagram of the photoelectric conversion apparatus according to Example 3 of this invention.
[Fig. 7]
It is a circuit block diagram of the photoelectric conversion apparatus according to Example 4 of this invention.
[Fig. 8]
It is a circuit block diagram of the photoelectric conversion apparatus according to Example 5 of this invention.
Every citation, both ways
| Document | Relation | Office | Cited during |
|---|---|---|---|
| JP2008048405A | Cited by | Japan | Examiner |
| US7595819B2 | Cited by | United States of America | Applicant |
| US7440017B2 | Cited by | United States of America | Applicant |
| JP2010263661A | Cited by | Japan | Examiner |
| US8179469B2 | Cited by | United States of America | Applicant |
| US7643077B2 | Cited by | United States of America | Applicant |
| US8488037B2 | Cited by | United States of America | Applicant |
| US7812876B2 | Cited by | United States of America | Applicant |
| US8823849B2 | Cited by | United States of America | Applicant |
6 members in 4 offices
Priority claims3
| Document | Office | Kind | Date |
|---|---|---|---|
| 12708693 | Japan | A | |
| 5127086 | – | – | – |
| JP19930127086 | – | – | – |
Members6
| Document | Office | Kind | |
|---|---|---|---|
| EP0626784A1 | European Patent Office (EPO) | A1 | |
| JPH06339082AThis record | Japan | A | |
| US5539196A | United States of America | A | |
| EP0626784B1 | European Patent Office (EPO) | B1 | |
| DE69431639D1 | Germany | D1 | |
| DE69431639T2 | Germany | T2 |
1 legal event, as the office reported them to INPADOC
Events
| Event | Code | |
|---|---|---|
| Application deemed to be withdrawn because no request for examination was validly filedWithdrawnJAPANESE INTERMEDIATE CODE: A300A300 | A300 |
Numbers
- Publication
- 6-339082
- Publication, DOCDB
- H06339082
- Publication, EPODOC
- JPH06339082
- Application
- 5127086
- Application, DOCDB
- 12708693
- Application, EPODOC
- JP19930127086
Titles2
- Japanese
- 【発明の名称】光電変換装置
- English
- [Title of Invention] Photoelectric conversion device
Classification
- CPC, 7
- H04N25/701
- H04N25/766
- H04N25/778
- H04N25/77
- H04N25/771
- H04N25/78
- H04N25/00
- IPC, 3
- H04N1 028
- H04N1 401
- H04N25 00