Patent Document

CROSS REFERENCE TO RELATED APPLICATIONS 
       [0001]    This application is a continuation of United States Application for U.S. Pat. No. 14/050,620 filed Oct. 10, 2013, which claims the priority benefit of French patent application serial number 1260168, filed on Oct. 25, 2012, which are hereby incorporated by reference to the maximum extent allowable by law. 
     
    
     TECHNICAL FIELD 
       [0002]    The present disclosure generally relates to electronic methods and circuits, and more specifically aims at a method and a circuit for detecting the luminosity level. 
       BACKGROUND 
       [0003]    Detectors of a luminosity or illumination level are known, which comprise a photodiode used in reverse mode, having its junction capacitance discharged by a photocurrent according to a received light intensity. 
       SUMMARY 
       [0004]    An embodiment provides a method wherein the updating of a counter is triggered when a photodiode reaches a discharge threshold. 
         [0005]    According to an embodiment, the photodiode is reset when it reaches said discharge threshold. 
         [0006]    According to an embodiment, a light intensity received by the photodiode is deduced from the state of the counter at the end of a time interval. 
         [0007]    According to an embodiment, a discharge time of the photodiode is measured after its resetting. 
         [0008]    According to an embodiment, the time interval is such that the sum of the discharge times measured during the interval is equal to a reference period. 
         [0009]    According to an embodiment, the reference period is selected according to the frequency of A.C. signal provided by an electric power supply network. 
         [0010]    According to an embodiment, the reference period is a multiple of 50 ms. 
         [0011]    According to an embodiment, a charge level of the photodiode at the end of said time interval is measured. 
         [0012]    Another embodiment provides the use of the above-mentioned method to detect the ambient luminosity level close to the photodiode. 
         [0013]    Another embodiment provides a circuit comprising a photodiode, a counter, and a control circuit configured to trigger an update of the counter when the photodiode reaches a discharge threshold. 
         [0014]    According to an embodiment, the control circuit is further configured to reset the photodiode when it reaches the discharge threshold. 
         [0015]    According to an embodiment, the control circuit is further configured to deduce a light intensity received by the photodiode from the state of the counter at the end of a time interval. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0016]    The foregoing and other features and advantages will be discussed in detail in the following non-limiting description of specific embodiments in connection with the accompanying drawings, wherein: 
           [0017]      FIG. 1  is a simplified electric diagram of an embodiment of a luminosity level detector; 
           [0018]      FIG. 2  is a timing diagram illustrating the operation of the detector of  FIG. 1 ; and 
           [0019]      FIG. 3  is a simplified electric diagram of an alternative embodiment of a luminosity level detector. 
       
    
    
       [0020]    For clarity, the same elements have been designated with the same reference numerals in the different drawings and, further, the timing diagram of  FIG. 2  is not to scale. 
       DETAILED DESCRIPTION 
       [0021]    Luminosity level detectors may be used in combination with illuminated display screens in devices such as telephones, tablets, computers, photographic cameras, etc. to automatically adjust the screen backlighting power according to the ambient luminosity, and thus achieve power savings and/or improve the user-friendliness. 
         [0022]    A luminosity level can be deduced from the measurement of the voltage across the photodiode, at the end of an integration period before and after the detector is reset by recharging of its photodiode. The voltage decrease across the photodiode during the integration depends on the amount of light received by the photodiode. 
         [0023]    A problem is that, if the integration period is too long, in case of a strong luminosity, the photocurrent may be such that the photodiode reaches, before the end of the integration period, a so-called saturation discharge threshold, beyond which luminosity differences can no longer be discriminated. However, if the integration period is too short, in case of a low luminosity, the photodiode discharge during the integration period may not be sufficient to enable to discriminate luminosity differences. In practice, it is thus provided to adjust the integration period according to the order of magnitude of the luminosity level to be measured. To achieve this, it is generally provided to repeat several times the measurement by starting from a short integration period, and by progressively increasing this period until a useable measurement is obtained. The time necessary to obtain a useable measurement may be relatively long. Further, this time is dependent from the luminosity level to be measured, which may pose certain problems. 
         [0024]    Another problem is that possible linearity defects in the photodiode response may cause inaccuracies in the measurement provided by the detector. 
         [0025]    Another problem is that a luminosity level detector is often sensitive to the flickering of artificial light sources, supplied in A.C. mode, for example, by the mains voltage. Such a flickering may significantly disturb the measurements performed by the detector. To solve this problem, it may be provided to select an integration sub-period of the photodiode which is a multiple of the half-period of the A.C. power supply voltage, for example, a multiple of 10 ms for a 50-Hz power supply source, or a multiple of 8.33 ms for a 60-Hz power supply source. This indeed enables to ascertain that the duration when the light source is off during the integration period of the photodiode is independent from the phase-shift between the integration period of the photodiode and the A.C. power supply of the light source. However, this necessitates that the photodiode integration period may not be shorter than the half-period of the A.C. power supply source. Now, in case of a strong luminosity, the detector may saturate before the end of a half-period of the A.C. power supply voltage. The discrimination of the higher luminosity levels is then impossible. 
         [0026]    An embodiment solves all or part of these problems. 
         [0027]      FIG. 1  is a simplified schematic diagram of an embodiment of a luminosity level detector  100 . Detector  100  comprises a photodiode  101  having its anode connected to a low power supply rail GND, for example, the ground, and having its cathode K connected, via a reset switch  103 , for example, a MOS transistor, to a high power supply rail V RT . In this example, cathode K of diode  101  is further connected to an input El of a comparator  105 . Comparator  105  further comprises an input E 2 , and an output S. In this example, the operation of comparator  105  is such that voltage V CMP  on its output S is at a first level when the voltage between inputs E 1  and E 2  is positive, and at a second level, for example, higher than the first level, when the voltage between inputs E 1  and E 2  is negative. In this example, detector  100  further comprises a control circuit  107 , receiving output signal V CMP  of comparator  105 , and providing a signal RST for controlling reset switch  103 . Circuit  107  further comprises an output OUT configured to provide a value representative of a luminosity level measured by the detector. 
         [0028]      FIG. 2  is a timing diagram illustrating the operation of detector  100  of  FIG. 1 .  FIG. 2  shows the variation of signal RST for controlling reset switch  103 , of voltage V PX  on cathode K of photodiode  101 , of voltage V REF  on input E 2  of comparator  105 , and of voltage V CMP  on output S of comparator  105 . In this example, when signal RST is in a high state, the switch is turned on, which causes the charging of photodiode  101 . Voltage V PX  on cathode K of photodiode  101  is then substantially equal to high power supply voltage V RT  (to within the voltage drop of switch  103 ). However, when signal RST is in a low state, switch  103  is off and photodiode  101  is disconnected from rail V RT . The photodiode is then sensitive to light, and voltage V PX  of its cathode decreases at a rate which depends on the light intensity received by the photodiode. 
         [0029]    According to an aspect, detector  100  is configured so that, within a luminosity level measurement time interval T M , each time photodiode  101  reaches a discharge threshold, a counter  109  (CP), for example, comprised within control circuit  107 , is updated, that is, incremented or decremented. Detector  100  is further configured so that, in measurement interval T M , each time photodiode  101  reaches the discharge threshold triggering the update of counter  109 , the photodiode is reset. 
         [0030]    In the illustrated example, measurement interval T M  starts with a resetting of photodiode  101 . To achieve this, control circuit  107  applies to signal RST a pulse  201   1  for controlling the turning-on of transistor  103 . During pulse  201   1 , cathode voltage V PX  of diode  101  is substantially equal to high power supply voltage V RT . 
         [0031]    Falling edge  202   1  of pulse  201   1  marks the beginning of an integration period of the photodiode, during which voltage V PX  decreases at a rate depending on the light intensity received by the photodiode. During this integration period, a constant voltage V REF , lower than voltage V RT , is applied to input node E 2  of comparator  105 . Voltage V REF  is for example slightly greater than the saturation threshold of photodiode  101 . 
         [0032]    During the reset phase (pulse  201   1 ) and at the beginning of the integration period, voltage V PX  being higher than voltage V REF , output voltage V CMP  of comparator  105  is in the low state. 
         [0033]    After a discharge time T d1  which depends on the light intensity received by the photodiode, and which is thus not known before the beginning of the integration period, voltage V PX  reaches voltage V REF , and comparator  105  switches state. Control circuit  107  is configured to detect such a state switching (that is, a rising edge of signal V CMP  in this example) and, as a response, to update counter  109  and reset the photodiode by applying to signal RST a pulse  201   2  for controlling the turning-on of switch  103 . 
         [0034]    A new integration period of the photodiode then starts, and the above-mentioned sequence (discharge of the photodiode down to threshold V REF , detection of a state switching of the comparator, counter update, and resetting of the photodiode) is repeated, and so on until the end of measurement interval T M . 
         [0035]    Thus, during measurement interval TM, detector  100  carries out n (n being an integer greater than or equal to 1) discharge cycles of photodiode  101 , each cycle comprising a photodiode reset step, followed by an integration period. Each cycle ends after the photodiode has reached the discharge threshold set by voltage V REF , except for the last cycle which may end before voltage V PX  reaches threshold V REF . Counter  109  is updated at the end of each full discharge cycle. The number of cycles carried out within an interval T M  depends on the light intensity received by the photodiode, and is thus not known before the beginning of interval T M . The higher the light intensity received by the photodiode, the greater the photodiode discharge speed, and the higher the number of cycles performed within interval T M . Conversely, the lower the light intensity received by the photodiode, the lower the photodiode discharge speed, and the smaller the number of cycles performed within interval T M . Below a given luminosity threshold, the photodiode never reaches the discharge threshold set by voltage V REF  during interval T M . In this case, interval T M  only contains a partial discharge cycle. 
         [0036]    Thus, the number of updates of counter  109  during interval T M  is representative of the luminosity level received by the photodiode during interval T M . At the end of measurement interval T M , a luminosity level received by the photodiode during interval T M  may be deduced from the state of counter  109 . 
         [0037]    As an example, counter  109  may be reset at the beginning of interval T M , and the state of counter  109  at the end of interval T M  may be directly used as a measurement of the luminosity level, and transferred onto output OUT of the detector. In this case, an advantage is that detector  100  does not require providing an analog-to-digital converter to sample a discharge level of its photodiode. This enables to decrease the bulk, the cost, and the power consumption of the detector. 
         [0038]    As a variation, to make the measurement more accurate still, detector  100  may comprise an analog-to-digital converter (not shown) and may be configured so as to, at the end of the last discharge cycle of photodiode  101 , which may be a partial discharge cycle, sample the discharge level of photodiode  101 . An output value OUT representative of the luminosity level received by the photodiode can then be determined by taking into account not only the number of updates of counter  109  during interval T M , but also the level reached by the photodiode at the end of the last discharge cycle. 
         [0039]    The duration of interval T M  may be set before the beginning of the measurement. In this case, the total effective discharge time of the photodiode during interval T M  depends on the luminosity received by the photodiode. Indeed, the higher the luminosity, the larger the number of discharges cycles during interval T M , and the larger the portion of interval T M  used to reset the photodiode and update counter  109 . Conversely, the lower the luminosity, the lower the number of discharges cycles during interval T M , and the smaller the portion of interval T M  used to reset the photodiode and update counter  109 . It should indeed be noted that the duration of the photodiode reset and counter update phases between discharge cycles is independent from the luminosity level received by the detector. Thus, for a given measurement interval T M , the higher the luminosity, the shorter the total effective photodiode discharge time during interval T M , and conversely. 
         [0040]    In an embodiment, only total effective photodiode discharge time T D  during interval T M  is set before the beginning of the measurement, and interval T M  varies according to the luminosity received by the photodiode. For this purpose, in each photodiode discharge time during measurement interval T M , effective discharge time T di  (i being an integer ranging from  1  to n) of the photodiode, between falling edge  202   i  of reset pulse  201   i  and the time of the cycle when the photodiode reaches the discharge threshold set by voltage V REF , is measured, for example, by means of a time measurement circuit  111  which may be part of control circuit  107 . Circuit  111  for example comprises a clock (not shown) and a counter (not shown) capable of being triggered by the rising and/or falling edges of the clock. The end of interval T M  coincides with the time when the addition of discharge times T di  measured from the beginning of interval T M  reaches a reference threshold duration T D  set before the beginning of the measurement. For a given effective discharge time T D , measurement interval T M  will be all the longer as the luminosity is high, and conversely. 
         [0041]    Total discharge time T D  of the photodiode preferably is a multiple of the half-period of the mains A.C. power supply voltage. This enables to make the detector insensitive to the flickering of artificial light sources powered by the mains. Preferably, time T D  is a multiple of 50 ms. Indeed, most A.C. electric power supply distribution networks operate either at 50 Hz or at 60 Hz, and 50 ms is a multiple both of the half-period of a 50-Hz A.C. signal (10 ms) and of the half-period of a 60-Hz A.C. signal (8.33 ms). The selection of a time T D  which is a multiple of 50 ms thus enables to make the detector insensitive to flickering, whatever the location where the detector is used. 
         [0042]    An advantage of the embodiment described in relation with  FIGS. 1 and 2  is that it is not necessary to repeat the measurement several times to adjust an integration period of the photodiode according to the ambient luminosity level to obtain a useable measurement. Indeed, in the embodiment of  FIGS. 1 and 2 , measurement interval T M , or the effective total discharge time T D  of the photodiode, may be selected to be sufficiently long to be compatible both with the lowest luminosity levels and with the highest luminosity levels. It should indeed be noted that, in the embodiment of  FIGS. 1 and 2 , the selection of a long measurement time T M  or total discharge time T D  is not incompatible with the discrimination of high luminosity levels. Generally, it should be noted that in the embodiments of  FIGS. 1 and 2 , whatever the luminosity level to be measured, the longer the measurement time T M  or total discharge time T D  of the photodiode, the higher the accuracy of the measurement provided by the detector. 
         [0043]    Another advantage of the embodiment of  FIGS. 1 and 2  is that total effective discharge time T D  of the photodiode may be selected to be sufficiently long to provide a measurement independent from the flickering of artificial light sources power in A.C. mode, without for the discrimination of the highest luminosity levels to be adversely affected by this. 
         [0044]    Another advantage of the embodiment of  FIGS. 1 and 2  is that the measurement of the luminosity level provided by the detector is not, or is only slightly, affected by possible linearity defects of photodiode  101 . This especially results from the fact that diode  101  operates in full discharge cycles always ending at a same level, set by voltage V REF , and that the indication of the luminosity level does not depend, for the most part, on a measurement of a discharge level of the photodiode at the end of an integration period. 
         [0045]    Another advantage is that the signal-to-noise ratio of the measurements provided by detector  100  is higher than that of the measurements provided by a detector where the indication of the luminosity level essentially results from a measurement of the discharge level of the photodiode after an integration period. 
         [0046]      FIG. 3  is a simplified electric diagram of an alternative embodiment of the luminosity level detector of  FIG. 1 . Detector  300  of  FIG. 3  comprises a photodiode  101  having its anode connected to a low power supply rail GND, for example, the ground, and having its cathode K connected, via a reset switch  103 , for example, a MOS transistor, to a high power supply node or rail V RT . In this example, cathode K of diode  101  is further connected to the gate of a MOS transistor  301  assembled as a voltage follower, having its conduction nodes N and M respectively connected to a high power supply rail V DD , via a current source  302 , and to low power supply rail GND. It should be noted that high voltage node V RT  may be directly connected to high power supply rail V DD  or may be connected to the output of a regulator providing a high-level voltage different from voltage V DD . In this example, node N is connected to a first electrode of a capacitor C having its second electrode connected to an input El of a comparator  105 . Comparator  105  further comprises an input E 2  and an output S. As in the example of  FIG. 1 , in operation, voltage V CMP  on output S of comparator  105  is at a first level when the voltage between inputs E 1  and E 2  is positive, and at a second level when the voltage between inputs E 1  and E 2  is negative. Detector  300  further comprises a switch  303  connecting input E 1  to output S of the comparator. Switch  303 , when it is in the on state, forms a negative feedback loop resetting the detector by forcing input E 1  of comparator  105  to the voltage of input E 2 . In operation, the turning-on of switch  303  causes the resetting of capacitor C to a charge level set by a voltage V REF  applied to terminal E 2  of the comparator. In this example, detector  300  further comprises a control circuit  307 , receiving output signal V CMP  of comparator  105 , and providing a signal RST for controlling reset switch  103  of photodiode  101 , and a signal AZ for controlling switch  303  for resetting capacitor C. Circuit  107  further comprises an output OUT configured to provide a value representative of a luminosity level measured by the detector. 
         [0047]    In operation, in a detector reset step, switches  103  and  303  are turned on, which causes the charge of photodiode  101  to a level set by voltage V RT , and the resetting of capacitor C to a level set by voltage V REF . In a photodiode integration or discharge phase, following a reset step, switches  103  and  303  are off. The cathode voltage of photodiode  101 , substantially equal to voltage V RT  at the beginning of the integration, is transferred onto input E 1  of comparator  105  via transistor  301  and capacitor C. The voltage at node E 1  then decreases at a rate depending on the luminosity level received by the photodiode, to reach level V REF , which causes a state switching of the comparator and the updating of counter  109 . 
         [0048]    The embodiment of  FIG. 3  has all the advantages of the embodiment of  FIGS. 1 and 2  and is compatible with the operation described in relation with  FIGS. 1 and 2 . 
         [0049]    Another advantage of the embodiment of  FIG. 3  is that transistor  301  and capacitor C enable to achieve an impedance matching between photodiode  101  and comparator  105 . 
         [0050]    As a variation, a complementary circuit, not shown, may be provided to apply a first reference voltage on input El of the comparator during detector reset steps, and a second reference voltage lower than the first voltage during photodiode discharge phases. 
         [0051]    Specific embodiments have been described. Various alterations, modifications, and improvements will occur to those skilled in the art. In particular, the described embodiments are not limited to the detection circuit examples of  FIGS. 1 and 3 . Based on the teachings of the present application, it will be within the abilities of those skilled in the art to form other circuits for detecting the luminosity level, capable of implementing the desired operation, that is, counting, during a measurement time interval, the number of discharge cycles of a photodiode, and deducing therefrom a luminosity level received by the photodiode. 
         [0052]    Such alterations, modifications, and improvements are intended to be part of this disclosure, and are intended to be within the spirit and the scope of the present invention. Accordingly, the foregoing description is by way of example only and is not intended to be limiting. The present invention is limited only as defined in the following claims and the equivalents thereto.

Technology Category: 3