US20040201559A1 - Liquid-crystal luminous quantity adjuster, method for driving liquid crystal luminous quantity adjuster, and camera comprising liquid crystal luminous quantity adjuster - Google Patents

Liquid-crystal luminous quantity adjuster, method for driving liquid crystal luminous quantity adjuster, and camera comprising liquid crystal luminous quantity adjuster Download PDF

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Publication number
US20040201559A1
US20040201559A1 US10/468,274 US46827403A US2004201559A1 US 20040201559 A1 US20040201559 A1 US 20040201559A1 US 46827403 A US46827403 A US 46827403A US 2004201559 A1 US2004201559 A1 US 2004201559A1
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driving pulses
driving
liquid
amount adjusting
optical transmittance
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English (en)
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Toshifumi Takaoka
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Sony Corp
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Sony Corp
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Publication of US20040201559A1 publication Critical patent/US20040201559A1/en
Priority to US11/973,194 priority Critical patent/US7394498B2/en
Abandoned legal-status Critical Current

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    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/13306—Circuit arrangements or driving methods for the control of single liquid crystal cells
    • G—PHYSICS
    • G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B9/00—Exposure-making shutters; Diaphragms
    • G03B9/02—Diaphragms
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N23/00—Cameras or camera modules comprising electronic image sensors; Control thereof
    • H04N23/60—Control of cameras or camera modules
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N23/00—Cameras or camera modules comprising electronic image sensors; Control thereof
    • H04N23/70—Circuitry for compensating brightness variation in the scene
    • H04N23/75—Circuitry for compensating brightness variation in the scene by influencing optical camera components
    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2203/00—Function characteristic
    • G02F2203/60—Temperature independent

Definitions

  • the present invention relates to a liquid-crystal light-amount adjusting device that controls the amount of transmitting light, and to an apparatus for driving the liquid-crystal light-amount adjusting device.
  • the present invention also relates to a camera in which the liquid-crystal light-amount adjusting device is used as a diaphragm.
  • FIG. 8 is a schematic diagram showing an optical system of a conventional camera.
  • the degree of degradation in resolution due to the diffraction is determined by the ratio between the amount of the light 112 that transmits through the diaphragm aperture 107 and the amount of the diffracted light 113 that diffracts at the edges of the diaphragm aperture 107 , and it therefore becomes larger as the size of the camera is reduced and the size of the diaphragm is reduced accordingly.
  • this problem is significant considering the recent miniaturization of cameras.
  • liquid-crystal light-amount adjusting device that employs liquid crystal has been proposed.
  • the liquid-crystal light-amount adjusting device is disposed in place of a blade diaphragm. Since the optical transmittance is substantially uniform over the entire surface on which light is incident, and the optical transmittance can be controlled continuously, the liquid-crystal light-amount adjusting device allows adjustment of the amount of light without causing degradation in resolution due to diffraction. That is, the aperture value can be adjusted.
  • a voltage that is higher (or lower) than a target voltage for achieving a specified optical transmittance (a driving,voltage for acceleration) is applied to a liquid crystal for a short period.
  • a driving,voltage for acceleration By supplying a certain electric power by the driving voltage for acceleration, a large driving force is exerted on the liquid-crystal molecules in the process of changing the orientation of the liquid crystal.
  • the pulses When the driving voltage for acceleration is applied by pulses, the pulses must be applied for an optimal time in order to achieve optimal response characteristics. For that purpose, the resolution increases as the frequency of the pulses becomes higher, allowing delicate control of the time of application.
  • the liquid-crystal light-amount adjusting device is electrically a capacitor having the liquid crystal held between electrodes, a large amount of power is consumed at pulse edges if the frequency is high.
  • it is possible to reduce the current by disposing a resistor in series with the liquid crystal held between the electrodes.
  • a low-pass filter is formed by the liquid crystal and the capacitor, causing degradation in the response characteristics of the liquid crystal.
  • the frequency of the pulses is preferably as low as possible.
  • the frequency of the pulses of the driving voltage for acceleration must satisfy contradicting requirements.
  • the frequency of driving pulses for acceleration and the frequency of driving pulses for dimming are allowed to be different.
  • the effective power of the driving pulses for acceleration can be optimized in accordance with driving status of a liquid-crystal light-amount adjusting device. Accordingly, a liquid-crystal light-amount adjusting device that exhibits favorable response characteristics can be implemented. Furthermore, a liquid-crystal light-amount adjusting device with low power consumption can be implemented. Furthermore, a liquid-crystal light-amount adjusting device with an extended lifetime can be implemented since DC components can be suppressed.
  • FIG. 1 is a diagram showing the construction of a camera according to an embodiment of the present invention.
  • FIG. 2 is a diagram showing the construction of a liquid-crystal light-amount adjusting unit.
  • FIGS. 3A to 3 C are diagrams showing an example of driving pulses and an example of optical transmittance.
  • FIG. 4 is a diagram showing a driving-pulse generating circuit.
  • FIGS. 5A and 5B are (first) diagrams for explaining the operation of the driving-pulse generating circuit.
  • FIG. 6 is a (second) diagram for explaining the operation of the driving-pulse generating circuit.
  • FIG. 7 is a diagram for explaining the operation of the liquid-crystal light-amount adjusting unit.
  • FIG. 8 is a schematic diagram showing an optical system of a conventional camera.
  • FIG. 1 is a diagram showing the construction of a camera according to an embodiment of the present invention.
  • the camera includes lenses 11 and 13 , a liquid-crystal light-amount adjusting unit 12 , an imaging device 14 , a driving circuit 15 , a signal processing circuit 18 , a microcomputer 19 , a storage circuit 20 , and a temperature detecting circuit 21 .
  • the incident light is adjusted by the liquid-crystal light-amount adjusting unit 12 so that an adjusted amount of light will be transmitted, and the resulting light enters the lens 13 . Since the liquid-crystal light-amount adjusting unit 12 alters optical transmittance substantially uniformly over the entire surface on which the light is incident, the light incident on the liquid-crystal light-amount adjusting unit 12 is dimmed substantially uniformly when it comes out. That is, the light that comes out of the lens 11 transmits the liquid-crystal light-amount adjusting unit 12 by a specified optical transmittance with no change between an area of the incident surface and an area of the emitting surface of the liquid-crystal light-amount adjusting unit 12 .
  • FIG. 2 is a diagram showing the construction of the liquid-crystal light-amount adjusting unit.
  • the liquid-crystal light-amount adjusting unit 12 includes substrates 31 a and 31 b , electrodes 32 a and 32 b , oriented films 33 a and 33 b , and a liquid crystal 34 .
  • the electrode 32 a is formed on one surface of the substrate 31 a , and the oriented film 33 a is formed on a surface of the electrode 32 a .
  • the electrode 32 b is formed on one surface of the substrate 31 b , and the oriented film 33 b is formed on a surface of the electrode 32 b .
  • These arrangements are disposed substantially in parallel with each other at a predetermined distance, with the oriented films 33 a and 33 b being opposed to each other, and the gap between the oriented films 33 a and 33 b is filled with the liquid crystal 34 .
  • the substrates 31 a and 31 b are formed of transparent parts, such as glass films or plastic films.
  • the electrodes 32 a and 32 b are transparent electrodes formed of, for example, ITO (indium tin oxide).
  • the oriented films 33 a and 33 b are formed of a material selected in accordance with a material of the liquid crystal 34 .
  • the liquid crystal 34 is a two-color guest-host liquid crystal.
  • the orientation of the liquid-crystal molecules is determined by intermolecular forces between the liquid-crystal molecules and the oriented films 33 a and 33 b and between the liquid-crystal molecules themselves.
  • the liquid-crystal molecules are polarized, causing a Coulomb force with an electric field between the electrodes 32 a and 32 b .
  • the orientation of the liquid-crystal molecules is determined by the balance between the Coulomb force and the intermolecular forces mentioned above.
  • the orientation of the liquid-crystal molecules can be changed by changing the potential difference between the electrodes 32 a and 32 b , and the optical transmittance of the liquid-crystal light-amount adjusting unit 12 can be changed accordingly. Since the electrodes 32 a and 32 b are disposed substantially in parallel to each other, the electric field generated therebetween is substantially uniform in a plane that is parallel to the electrodes 32 a and 32 b . Thus, the optical transmittance of the liquid-crystal light-amount adjusting unit 12 becomes substantially uniform.
  • dye molecules that determine optical characteristics have shapes like thin rods, and move in association with the liquid-crystal molecules. This movement occurs so that the potential energy associated with intermolecular forces with the liquid-crystal molecules becomes smaller. That is, the dye molecules move so as to become parallel with the liquid-crystal molecules.
  • the orientation of the liquid-crystal molecules changes in accordance with the potential difference between the electrodes 32 a and 32 b , and the direction of absorption axis of the dye molecules changes in accordance with the change in the orientation of the liquid-crystal molecules, whereby the optical transmittance of the two-color guest-host liquid-crystal light-amount adjusting unit 12 changes.
  • the liquid-crystal molecules used in this embodiment are not spontaneously polarized and are polarized by an external electric field, the Coulomb potential is minimized when a polarization-facilitating axis of the liquid-crystal molecules coincides with the direction of the external electric field.
  • the orientation of the liquid-crystal molecules is determined by the intensity of the electric field alone.
  • the effective power supplied from the electrodes 31 a and 31 b to the liquid crystal 34 is a function of the optical transmittance of the liquid-crystal light-amount adjusting unit 12 .
  • the frequency characteristics of the orientation of the two-color guest-host liquid crystal is on the order of several tens Hz
  • pulses having a frequency that is sufficiently higher compared therewith a frequency at which the direction of the orientation of the dye molecules does not follow change in the direction of the electric field
  • the effective power is given by a duty ratio of the pulses multiplied by a pulse amplitude voltage.
  • FIGS. 3A to 3 C are diagrams showing an example of driving pulses and an example of optical transmittance.
  • FIGS. 3A and 3B show driving pulses.
  • the effective power is larger in FIG. 3B since the pulse width is larger.
  • FIG. 3C shows an example of relationship between effective power and optical transmittance.
  • the optical transmittance starts changing from a threshold value Pth, and increases as the effective power becomes larger.
  • the optical transmittance has a one-to-one relationship with the effective power in a range of effective power larger than the threshold value Pth.
  • the light incident on the lens 13 is focused on a surface of the imaging device 14 through the lens 13 . More specifically, the lens 13 is moved between the liquid-crystal light-amount adjusting unit 12 and the imaging device 14 along an optical axis by a moving mechanism not shown, thereby focusing the incident light on the imaging device 14 within a range of focal -depth.
  • lens sets each including a plurality of lenses may be used in accordance with required capabilities of viewing-angle adjustment and focusing.
  • the optical system may include a plurality of lens sets, e.g., three lens sets or four lens sets, for viewing-angle adjustment and focusing.
  • the liquid-crystal light-amount adjusting unit 12 serves to change the aperture value similarly to a conventional diaphragm, and is disposed between a pair of lens sets among the plurality of lens sets.
  • the imaging device 14 performs photoelectric conversion for converting an incident light into an amount of electricity in accordance with the brightness of the incident light, signal accumulation for holding and integrating an amount of electricity for a certain period in order to improve sensitivity, and scanning for yielding time-series image signals from a spatial distribution of the amount of electricity obtained in relation to an image corresponding to the incident light.
  • the imaging device 14 can be implemented by a solid-state imaging device such as a charge-coupled device (CCD).
  • An output from the imaging device 14 is processed by the signal processing circuit 18 in accordance with a desired video signal format, and the result is output from the signal processing circuit 18 to the microcomputer 19 or to a display or a recorder not shown.
  • the temperature detecting circuit 21 detects an ambient temperature of the liquid-crystal light-amount adjusting unit 12 , and outputs a result of detection to the microcomputer 19 .
  • the temperature detecting circuit 21 can be implemented, for example, by a thermistor.
  • the microcomputer 19 is also connected to the storage circuit 20 that stores a comparison-value association table and various data, as will be described later.
  • the liquid-crystal light-amount adjusting unit 12 is driven by the driving circuit 15 .
  • the driving circuit 15 includes a driving-pulse generating circuit 16 , and a plurality of-comparison-value supplying circuits 17 for respectively supplying comparison values to the driving-pulse generating circuit 16 .
  • the comparison-value supplying circuits 17 include four comparison-value supplying circuits 17 a to 17 d .
  • the plurality of comparison-value supplying circuits 17 a to 17 d are controlled by the microcomputer 19 , as will be described later, to respectively supply comparison values to the driving-pulse generating circuit 16 .
  • FIG. 4 is a diagram showing the driving-pulse generating circuit.
  • the driving-pulse generating circuit 16 includes a binary counter 51 , comparators 53 , 57 , 58 , and 59 , an AND circuit 60 , inverters 62 and 65 , and field-effect transistors (FETs) 61 , 63 , 64 , and 66 .
  • FETs field-effect transistors
  • the binary counter 51 has a clock input to which a clock signal having a predetermined cycle is input, and a reset input to which an output of the comparator 53 is input. An output of the binary counter 51 is input to the comparator 53 , the comparator 57 , the comparator 58 , and to the comparator 59 .
  • the comparator 53 also receives input of a comparison value 1 supplied from the comparison-value supplying circuit 17 a .
  • the comparator 53 compares the comparison value 1 with the output of the binary counter 51 , and outputs an output signal if these values coincide with each other.
  • the comparator 57 also receives input of a comparison value 2 supplied from the comparison-value supplying circuit 17 b .
  • the comparator 57 compares the comparison value 2 with the output of the binary counter 51 , and outputs an output signal if these values coincide with each other.
  • the comparator 58 also receives input of a comparison value 3 supplied from the comparison-value supplying circuit 17 c .
  • the comparator 58 compares the comparison value 3 with the output of the binary counter 51 , and outputs an output signal if these values coincide with each other.
  • the comparator 59 also receives input of a comparison value 4 supplied from the comparison-value supplying circuit 17 d .
  • the comparator 59 compares the comparison value 4 with the output of the binary counter 51 , and outputs an output signal if these values coincide with each other.
  • the output signal of the comparator 57 is supplied to the gate of the FET 61 , and is also supplied, after being inverted by the inverter 62 , to the gate of the FET 63 .
  • the source of the FET 61 is connected to a power source Vcc, and the drain of the FET 61 is connected to the source of the FET 63 .
  • a node between the drain of the FET 61 and the source of the FET 63 is connected tc a first one of the electrodes 32 a and 32 b of the liquid-crystal light-amount adjusting unit 12 .
  • the drain of the FET 63 is grounded.
  • the FET 61 and the FET 63 are implemented by a pair of FETs of mutually different channel types.
  • the FET 61 is a p-channel FET and the FET 63 is an n-channel FET.
  • the output signals of the comparators 58 and 59 are input to the AND circuit 60 .
  • An output signal of the AND circuit 60 is supplied to the gate of the p-channel FET 64 , and is also supplied, after being inverted by the inverter 65 , to the gate of the n-channel FET 66 .
  • the source of the FET 64 is connected to the power source Vcc, and the drain of the FET 64 is connected to the source of the FET 66 .
  • a node between the drain of the FET 64 and the source of the FET 66 is connected to a second one of the electrodes 32 a and 32 b of the liquid-crystal light-amount adjusting unit 12 .
  • the drain of the FET 66 is grounded.
  • FIGS. 5A and 5B are (first) diagrams for explaining the operation of the driving-pulse generating circuit.
  • FIG. 6 is a (second) diagram for explaining the operation of the driving-pulse generating circuit.
  • FIGS. 5A and 5B the horizontal axis represents time and the vertical axis represents voltage.
  • the horizontal direction represents elapse of time and the vertical direction represents voltage magnitude.
  • an output of the binary counter 51 is used as an input to the comparator 53 , and an output of the comparator 53 is used as a reset input of the binary counter 51 .
  • the output of the binary counter 51 forms a triangular wave that is reset at the comparison value 1, as shown in FIGS. 5A and 5B.
  • the triangular wave is input to each of the comparators 57 , 58 , and 59 .
  • the output of the comparator 57 form pulses that rise at timings when the voltage value of the triangular wave coincides with the comparison value 2 and fall at timings when the voltage value of the triangular wave coincides with the comparison value 1, as shown in FIG. 5A.
  • the output of the AND circuit 60 to which the outputs of the comparators 58 and 59 are input, forms pulses that rise at timings when the voltage value of the triangular wave coincides with the comparison value 3 and fall at timings when the voltage value of the triangular wave coincides with the comparison value 4, as shown in FIG. 5B.
  • the output of the comparator 57 is applied to the gate of the p-channel FET 61 , and is also applied, via the inverter 62 , to the gate of the n-channel FET 63 .
  • the voltage applied to the electrode 32 a are pulses whose pulse widths are controlled in accordance with the magnitude of the comparison value 2, as shown in part (A) of FIG. 6.
  • the output of the AND circuit 60 is applied to the gate of the p-channel FET 61 , and is also applied, via the inverter 62 , to the gate of the n-channel FET 63 .
  • the voltage applied to the electrode 32 b are pulses whose pulse widths are controlled in accordance with the difference between the comparison values 3 and 4 , as shown in part (B) of FIG. 6.
  • the pulses shown in parts (A) and (B) of FIG. 6 are applied to the electrodes 32 a and 32 b of the liquid-crystal light-amount adjusting unit 12 , respectively.
  • the potential difference between the electrodes 32 a and 32 b form pulses that fall to a predetermined pulse amplitude voltage ⁇ Vt when the voltage applied to the electrode 32 b rises, that return to zero voltage when the voltage applied to the electrode 32 a rises, that rise to a predetermined pulse amplitude voltage +Vt when the voltage applied to the electrode 32 b falls, and that return to zero voltage when the voltage applied to the electrode 32 a falls, as shown in part (C) of FIG. 6.
  • the period TO of the pulses applied between the electrodes 32 a and 32 b is controlled in accordance with the comparison value 1, and the duty ratio D thereof is controlled in accordance with the comparison values 2, 3, and 4.
  • FIG. 7 is a diagram for explaining a method of driving the liquid-crystal light-amount adjusting unit.
  • the horizontal direction represents elapse of time and the vertical direction represents voltage magnitude.
  • the microcomputer 19 When an aperture value has been determined, the microcomputer 19 , with consideration of a result of detection by the temperature detecting circuit 21 , supplies driving pulses as shown in FIG. 7 from the driving circuit 15 to the liquid-crystal light-amount adjusting unit 12 so that an optical transmittance in accordance with the aperture value will be achieved.
  • an optimal aperture value is calculated from the amount of light received by the imaging device 14 .
  • an aperture value is determined according to a program stored in the storage circuit 20 in the case of automatic exposure, and an aperture value is determined according to an input value input by a user via an input device not shown in the case of manual exposure.
  • the driving pulses include driving pulses for acceleration and driving pulses for dimming.
  • the driving pulses for dimming are used to drive the liquid-crystal light-amount adjusting unit 12 so that an optical transmittance in accordance with the aperture value will be achieved.
  • the frequency fd, the pulse amplitude Vt, and the duty ratio D of the driving pulses for dimming are determined with consideration of the areas of the electrodes 32 a and 32 b , the distance (gap) between the electrodes 32 a and 32 b , an ambient temperature, the type of material of the liquid crystal 34 , etc. in the liquid-crystal light-amount adjusting unit 12 .
  • the driving pulses for acceleration are used to speed up response in changing the optical transmittance of the liquid-crystal light-amount adjusting unit 12 .
  • the frequency fa, the pulse amplitude Vt, the duty ratio D, and the applying time Ta of the driving pulses for acceleration are determined with consideration of relationship between current driving pulses for dimming and target driving pulses for dimming, in addition to the areas of the electrodes 32 a and 32 b , the distance (gap) between the electrodes 32 a and 32 b , an ambient temperature, the type of material of the liquid crystal 34 , etc. in the liquid-crystal light-amount adjusting unit 12 .
  • the target driving pulses for dimming are adjusted so that the effective power thereof will be smaller than the effective power of the current driving pulses for dimming.
  • the target driving pulses for dimming are adjusted so that the effective power thereof will be larger than the effective power of the current driving pulses for dimming. If the pulse amplitude Vt is constant, the effective power is adjusted by adjusting the pulse width (duty ratio D).
  • the frequencies fd and fa of the driving pulses must be high enough not to cause flicker. If the frequency is low, polarized liquid-crystal molecules is able to follow the driving pulses alternating between +Vt and ⁇ Vt, so that flicker occurs due to the optical transmittance changing in synchronization with the pulse cycle.
  • the frequencies fd and fa of the driving pulses must be low enough so that the impedance of the liquid-crystal light-amount adjusting unit 12 remains. This is because adjustment of light amount is not allowed if the frequencies of the driving pulses are high and if the impedance of the liquid-crystal light-amount adjusting unit 12 is thus eliminated.
  • the driving pulses must avoid generating DC components. More specifically, if pulses having a 1 ⁇ 4 period or pulses having a 1 ⁇ 2 period exist during the applying time Ta or the applying time Td, a DC component is generated. Thus, the number of pulses in the driving pulses must be an integer multiple of one period in each of the applying times Ta and Td. If a DC component is generated, the liquid crystal 34 is electrolyzed, and metallic ions, etc. in the liquid crystal 34 precipitates on the electrodes 32 a and 32 b . This inhibits transmittance of light, degrading performance of the liquid-crystal light-amount adjusting unit 12 .
  • the applying time Td of the driving pulses for dimming is determined when the applying time Ta of the driving pulses for acceleration is determined.
  • the imaging time Tp for one screen is approximately 16.7 ms corresponding to a field (a period of one cycle at 60 Hz) if imaging is performed on a field-by-field basis, or approximately 33.3 ms corresponding to a frame (a period of one cycle at 30 Hz) if imaging is performed on a frame-by-frame basis.
  • the imaging time Tp for one screen is determined according to a shutter speed.
  • the driving pulses for acceleration are needed to be applied when the optical transmittance of the liquid-crystal light-amount adjusting unit 12 is to be changed.
  • the driving pulses for acceleration are not needed, and the driving pulses for dimming are used over the entire imaging time Tp for one screen. That is, the applying time Td of the driving pulses for dimming is equal to the imaging time Tp for one screen.
  • the driving pulses for dimming and the driving pulses for acceleration are determined by actual measurements, and stored in the storage circuit 20 in the form of a comparison-value association table.
  • the comparison-value association table includes a table of association between aperture values and driving pulses for dimming, defining association between a plurality of aperture values and driving pulses for dimming for achieving the respective aperture values, and a table of association between driving pulses for dimming and driving pulses for acceleration, defining association between a plurality of relationships between target driving pulses for dimming and respective driving pulses for acceleration.
  • the comparison-value association table is created on a temperature-by-temperature basis at a predetermined temperature interval.
  • the fields for driving pulses for dimming in the table of association between aperture values and driving pulses for dimming store comparison values 1 to 4 for generating the driving pulses for dimming
  • the fields of driving pulses for acceleration in the table of association between driving pulses for dimming and driving pulses for acceleration store comparison values 1 to 4 and an applying time Ta of driving pulses for acceleration for generating the driving pulses for acceleration.
  • the microcomputer 19 when an aperture value is specified and a need is raised to change the aperture value, obtains the comparison values 1 to 4 for the driving pulses for acceleration and the applying time Ta of the driving pulses for acceleration, and the comparison values 1 to 4 for the driving pulses for dimming, from the comparison-value association table at a relevant temperature.
  • the microcomputer 19 first outputs the comparison values 1 to 4 for the driving pulses for acceleration to the comparison-value supplying circuits 17 a to 17 d of the driving circuit 15 , and exercises control so that the comparison-value supplying circuits 17 a to 17 d will generate the associated comparison values 1 to 4.
  • the comparison-value supplying circuits 17 a to 17 d generate specified comparison values, and supplies the comparison values generated to the comparators 53 , 57 , 58 , and 59 , respectively.
  • the driving-pulse generating circuit 16 generates driving pulses for acceleration according to the comparison values, thereby driving the liquid-crystal light-amount adjusting unit 12 .
  • the microcomputer 19 When the applying time Ta of the driving pulses for acceleration elapses, the microcomputer 19 outputs the comparison values 1 to 4 for the driving pulses for dimming to the comparison-value supplying circuits 17 a to 17 d of the driving circuit 15 , and exercises control so that the comparison-value supplying circuits 17 a to 17 d will generate the associated comparison values 1 to 4, respectively.
  • the comparison-value supplying circuits 17 a to 17 d generate the specified comparison values, and output the comparison values generated to the comparators 53 , 57 , 58 , and 59 , respectively.
  • the driving-pulse generating circuit 16 generates driving pulses for dimming in accordance with the comparison values, thereby driving the liquid-crystal light-amount adjusting unit 12 .
  • the microcomputer 19 controls the comparison-value supplying circuits 17 a to 17 d so that the liquid-crystal light-amount adjusting unit 12 will be driven by the driving pulses for dimming until the imaging time Tp for one screen is reached.
  • the microcomputer 19 controls the driving circuit 15 to supply driving pulses to the liquid-crystal light-amount adjusting unit 12 , thereby adjusting the amount of light to achieve a specified aperture value.
  • the frequency fa of the driving pulses for acceleration and the frequency fd of the driving pulses for dimming are allowed to be different from each other.
  • the driving pulses for acceleration can be controlled independently of the driving pulses for dimming.
  • the effective power of the driving pulses for acceleration can be optimized in accordance with the difference between the current optical transmittance and the target optical transmittance, the ambient temperature, the gap between the electrodes 32 a and 32 b , dye concentration, etc. in the liquid-crystal light-amount adjusting unit 12 .
  • predetermined driving pulses for acceleration are supplied, speeding up change in optical transmittance. Furthermore, the pulse shape of the predetermined driving pulses for acceleration and the pulse shape of the driving pulses for dimming can be controlled independently. Thus, the pulse shape of the driving pulses for acceleration can be controlled without being constrained by the pulse shape of the driving pulses for dimming. Accordingly, the predetermined driving pulses for acceleration are reliably obtained, serving to further enhance speed. Furthermore, in a liquid-crystal light-amount adjusting device, power consumption is reduced and lifetime is extended.

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  • Optics & Photonics (AREA)
  • Chemical & Material Sciences (AREA)
  • Mathematical Physics (AREA)
  • Liquid Crystal (AREA)
  • Diaphragms For Cameras (AREA)
  • Transforming Light Signals Into Electric Signals (AREA)
  • Studio Devices (AREA)
  • Lens Barrels (AREA)
US10/468,274 2001-12-18 2002-11-15 Liquid-crystal luminous quantity adjuster, method for driving liquid crystal luminous quantity adjuster, and camera comprising liquid crystal luminous quantity adjuster Abandoned US20040201559A1 (en)

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US11/973,194 US7394498B2 (en) 2001-12-18 2007-10-05 Liquid-crystal light-amount adjusting device, method of driving liquid-crystal light-amount adjusting device, and camera including the liquid-crystal light-amount adjusting device

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JP2001-384385 2001-12-18
JP2001384385A JP3873739B2 (ja) 2001-12-18 2001-12-18 液晶光量調整装置および液晶光量調整装置の駆動方法、ならびに該液晶光量調整装置を用いたカメラ。
PCT/JP2002/011965 WO2003052499A1 (fr) 2001-12-18 2002-11-15 Dispositif de reglage de la quantite lumineuse a cristaux liquides, procede de commande de ce dispositif et appareil photo comprenant ce dispositif

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US11/973,194 Expired - Lifetime US7394498B2 (en) 2001-12-18 2007-10-05 Liquid-crystal light-amount adjusting device, method of driving liquid-crystal light-amount adjusting device, and camera including the liquid-crystal light-amount adjusting device

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US (2) US20040201559A1 (zh)
EP (1) EP1457810B1 (zh)
JP (1) JP3873739B2 (zh)
KR (1) KR101016551B1 (zh)
CN (1) CN1228668C (zh)
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US20080151095A1 (en) * 2006-12-21 2008-06-26 Altek Corporation Image-capturing system and method
US11082663B2 (en) * 2016-04-04 2021-08-03 SMR Patents S.à.r.l. Imaging system

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KR100599652B1 (ko) * 2004-08-17 2006-07-12 삼성에스디아이 주식회사 액정표시장치 및 그의 구동방법
US8072574B2 (en) * 2008-02-25 2011-12-06 LensVector Tunable liquid lens with reduced aberration
US8908081B2 (en) 2010-09-09 2014-12-09 Red.Com, Inc. Optical filter opacity control for reducing temporal aliasing in motion picture capture
CN103033942B (zh) 2011-09-29 2015-07-15 通用电气公司 光学成像系统和方法以及孔径光阑组合和孔径元件
JP5948788B2 (ja) * 2011-10-18 2016-07-06 ソニー株式会社 動作制御装置および動作制御方法、撮像装置、並びにプログラム
WO2013088630A1 (ja) * 2011-12-16 2013-06-20 パナソニック株式会社 可変焦点レンズの制御装置、可変焦点レンズの制御方法、および電子メガネ
CN105264880B (zh) 2013-04-05 2018-08-28 Red.Com 有限责任公司 用于相机的滤光
US9497363B2 (en) * 2014-01-09 2016-11-15 Taiwan Semiconductor Manufacturing Co., Ltd. Photographic apparatus and manufacturing method thereof
JP2015198292A (ja) * 2014-03-31 2015-11-09 ソニー株式会社 撮像装置、フリッカの補正方法及びプログラム
JP6957944B2 (ja) * 2017-04-05 2021-11-02 凸版印刷株式会社 液晶調光装置及び液晶調光方法
TW202006451A (zh) * 2018-07-17 2020-02-01 先進光電科技股份有限公司 可調變進光量光學成像系統
CN113189805B (zh) * 2021-04-28 2023-04-07 维沃移动通信（杭州）有限公司 显示模组、电子设备、拍摄控制方法和拍摄控制装置

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US20080151095A1 (en) * 2006-12-21 2008-06-26 Altek Corporation Image-capturing system and method
US11082663B2 (en) * 2016-04-04 2021-08-03 SMR Patents S.à.r.l. Imaging system

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CN1491369A (zh) 2004-04-21
JP3873739B2 (ja) 2007-01-24
TWI227344B (en) 2005-02-01
WO2003052499A1 (fr) 2003-06-26
US7394498B2 (en) 2008-07-01
EP1457810A1 (en) 2004-09-15
CN1228668C (zh) 2005-11-23
TW200301388A (en) 2003-07-01
KR20040073961A (ko) 2004-08-21
JP2003186078A (ja) 2003-07-03
EP1457810A4 (en) 2007-10-03
US20080074532A1 (en) 2008-03-27
EP1457810B1 (en) 2012-01-04
KR101016551B1 (ko) 2011-02-24

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