Patent Document

FIELD OF THE INVENTION 
       [0001]    The invention relates to a determination circuit for measuring a current, the determination circuit comprising:
   an integration unit for integrating a current over an integration time resulting in an integration value;   a time counter unit for counting the integration time from the start of integrating the current to a predefined maximum integration time.   
 
         [0004]    The invention also relates to a method for measuring a current using such a determination circuit. 
         [0005]    The invention also relates to a computer program product adapted, when being executed by a processor, to integrate a current using such a determination circuit. 
       BACKGROUND OF THE INVENTION 
       [0006]    An embodiment of a determination circuit of this kind is known from the international patent application WO2007/029191 A2. In this document a determination circuit is described for measuring a low current with a large dynamic range, the determination circuit comprising an integration unit and a counter unit. The integration unit is adapted for integrating the current over an integration time, resulting in an integration value. The counter unit is adapted for counting the integration time, resulting in a counting value. The determination circuit is adapted for outputting a first measurement result on the basis of accounting value, if the integration value exceeds a first threshold value before expiration of a maximum integration time. The first threshold may be the saturation voltage of the integration unit comprising an operational amplifier with a capacitor connected to it in parallel. The first measurement result is the integration time needed for the integration value to exceed the first threshold. According to another embodiment, the determination circuit is adapted for outputting a second measurement result on the basis of the integration value, if the integration value is below the first threshold value at the expiration of the maximum integration time. According to yet another embodiment, the determination circuit is adapted for outputting a third measurement result on the basis of the counting value and the integration value, if the integration value exceeds in the first threshold value before the expiration of the maximum integration time and if the counting value is below a second threshold value. A determination circuit for integrating a current with a large dynamic range is useful in, for instance, a device for imaging an interior of an optically turbid medium using diffuse optical tomography. In such a device currents easily span 10 orders of magnitude. 
       SUMMARY OF THE INVENTION 
       [0007]    It is an object of the invention to provide a determination circuit that is more precise than the determination circuit according to the prior art. According to the invention this object is realised in that the determination circuit further comprises:
   a reset counter for counting the number of resets of the integration unit,   wherein the determination unit is adapted for:   (a) outputting a first measurement result if the absolute value of the integration value is below a reset threshold at the expiration of the predefined maximum integration time;   (b) resetting the integration unit if the absolute value of the integration value exceeds the reset threshold before the expiration of the predefined maximum integration time;   (c) repeating the steps of outputting and resetting each time the absolute value of the integration value exceeds the reset threshold until expiration of the predefined maximum integration time, counting the number of resets;   (d) outputting a second measurement result based on at least one of the integration value and the number of resets if the number of resets is nonzero.   
 
         [0014]    The invention is based on the recognition that the invention allows a current that would saturate a determination circuit according to the prior art before expiration of the predefined maximum integration time to be integrated over a longer period of time. In fact, the current is integrated over a series of time intervals, each interval being separated from the previous interval by a reset of the integration unit. The fact that, with the invention, a current that would saturate a determination circuit according to the prior art can be integrated over a longer period of time means that a determination circuit according to the invention is more precise than a determination circuit according to the prior art. After all, it is generally known that the accuracy of a measurement increases as the time interval of all which a signal, in this case a current, is measured increases. Moreover, the integration values obtained for each time interval can be averaged, which also makes the determination circuit according to the invention more precise than a determination circuit according to the prior art, which bases its output on an integration over only a single interval as it cuts off the integration once the integration value exceeds the predetermined threshold. 
         [0015]    It is an additional advantage of the invention that it has higher dynamic range of currents that can be integrated as compared to a determination circuit according to the prior art. If an integration unit comprised in a determination circuit according to the prior art saturates before expiration of the maximum integration time when integrating a certain current, a determination circuit according to the invention can continue integration by resetting the integration unit as many times as needed. 
         [0016]    It is an additional advantage of the invention that it allows a capacitor to be chosen such that the determination circuit is optimised for a specific measuring range. One can, for instance, measure currents in the range 1 fA-1 μA (nine orders of magnitude) or in the range 1 pA-1 mA (also nine orders of magnitude). Whereas the first range is optimised for accurate measurements near the noise floor, the second range is optimised for larger currents. 
         [0017]    Other documents that deal with measuring a current with a large dynamic range are U.S. Pat. No. 6,429,718 B1 and U.S. Pat. No. 6,150,649. However, neither of these documents describe resetting an integration unit (multiple times if needed) if the absolute value of the integration value generated by the integration unit exceeds a reset threshold and continuing integration of the current after the (or each) reset until expiration of a maximum integration time. In particular U.S. Pat. No. 6,429,718 B1 describes switching from one gain factor to another gain factor to enable integration of currents spanning a large dynamic range. U.S. Pat. No. 6,150,649 describes integrating currents spanning a large dynamic range over time intervals of different lengths to obtain different gains for currents of different magnitude. 
         [0018]    An embodiment of the determination circuit according to the invention, wherein the integration unit comprises:
   a higher gain integration circuit for integrating the current if the absolute value of the integration value lies below a switching threshold before expiration of the predefined maximum integration time;   a lower gain integration circuit for integrating the current until expiration of the predefined maximum integration time if the absolute value of the integration value generated by the higher gain integration circuit exceeds the switching threshold before expiration of the predefined maximum integration time. This embodiment has the advantage that it allows measurement of a current having a magnitude such that it causes the integration value generated by the higher gain integration circuit to exceed the switching threshold before expiration of the maximum integration time. As such this embodiment is suitable for measuring a current that would otherwise be too large to be measured without exceeding the switching threshold.   
 
         [0021]    The object of the invention is also realised with a method for measuring a current with a large dynamic range, the method comprising the following steps:
   integrating the current over a predefined maximum integration time using an integration unit, resulting in an integration value;   counting the integration time from the start of integrating the current to the expiration of the predefined maximum integration time;   outputting a first measurement result if the absolute value of the integration value is below a reset threshold at the expiration of the predefined maximum integration time;   resetting the integration unit if the absolute value of the integration value exceeds the reset threshold before the expiration of the predefined maximum integration time;   repeating the steps of outputting and resetting each time the absolute value of the integration value exceeds the reset threshold until expiration of the predefined maximum integration time, counting the number of resets;   outputting a second measurement result based on at least one of the integration value and the number of resets if the number of resets is nonzero.   
 
         [0028]    An embodiment of the method according to the invention, wherein the method further comprises the following additional step:
   switching the integration unit from a higher gain setting to a lower gain setting if the absolute value of the integration value generated in the higher gain setting exceeds a switching threshold before expiration of the predefined maximum integration time. Just as with the embodiment of the method discussed earlier, this embodiment has the advantage that it allows measurement of a current having a magnitude such that it causes the integration value generated by the higher gain integration circuit to exceed the switching threshold before expiration of the maximum integration time.   
 
         [0030]    The object of the invention is also a realised with a computer program product adapted, when being executed by a processor, to carry out the following steps:
   integrating a current over an integration time using an integration unit;   counting the integration time;   outputting a first measurement result if the absolute value of the integration value is below a reset threshold at the expiration of the predefined maximum integration time;   resetting the integration unit if the absolute value of the integration value exceeds the reset threshold before the expiration of the predefined maximum integration time;   repeating the steps of outputting and resetting each time the absolute value of the integration value exceeds the reset threshold until expiration of the predefined maximum integration time, counting the number of resets;   outputting a second measurement result based on at least one of the integration value and the number of resets if the number of resets is nonzero.   
 
         [0037]    An embodiment of the computer program product according to the invention, wherein the computer program product is adapted, when being executed by a processor, to further carry out the following additional step:
   switching the integration unit from a higher gain setting to a lower gain setting if the absolute value of the integration value generated in the higher gain setting exceeds a switching threshold before expiration of the predefined maximum integration time. Just as with the embodiment of the method discussed earlier, this embodiment has the advantage that it allows measurement of a current having a magnitude such that it causes the integration value generated by the higher gain integration circuit to exceed the switching threshold before expiration of the maximum integration time.   
 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0039]      FIG. 1  schematically shows an embodiment of a determination circuit according to the invention comprising a higher gain circuit and a lower gain circuit; 
           [0040]      FIG. 2  schematically shows a lower current measurement using only the higher gain circuit; 
           [0041]      FIG. 3  schematically shows a higher current measurement using both a high against circuit and a lower gain circuit; 
           [0042]      FIG. 4  schematically shows the timing of the multiple integration principle on a higher current; 
           [0043]      FIG. 5  schematically shows an embodiment of the method according to the invention; 
           [0044]      FIG. 6  schematically shows an embodiment of a device for imaging an interior of a turbid medium comprising a determination circuit according to the invention; 
           [0045]      FIG. 7  schematically shows an embodiment of a medical image acquisition device comprising a determination circuit according to the invention; 
       
    
    
       [0046]    Table 1 lists current measurements using only the higher gain circuit, only the lower gain circuit, or both circuits. 
       DETAILED DESCRIPTION OF EMBODIMENTS 
       [0047]      FIG. 1  schematically shows an embodiment of a determination circuit according to the invention comprising a higher gain circuit and a lower gain circuit. The determination circuit  100  comprises an integration unit  105 , a counter unit  110 , an analog-to-digital converter  115 , and a clock  120 , such as a 100 MHz clock. However, different frequencies may be used for clocking. The counter unit  110  may be adapted as a counter/timing FPGA. FPGA is a Field Programmable Gate Array, a device with configurable digital logic, like counters, registers etc. The determination circuit  100  is adapted for measuring a current (or a plurality of currents) with a large dynamic range (for example a range spanning 10 decades or more). The current to be measured may be generated by a photodiode  125 , which detects light from a light guide  130 , such as an optical fibre. The light guide  130  may be comprised in a device for imaging an interior of an optically turbid medium using diffuse optical tomography. The integration unit  105  comprises a higher gain circuit  135  and a lower gain circuit  140 . Both the higher gain circuit  135  and the lower gain circuit  140  may be adapted, for instance, as a 1/2ACF2101 or an IVC102. The higher gain circuit  135  is connected to switch  145  at its minus input. The plus input is connected to the ground  150 . Furthermore, the minus input is connected to capacitor  155  (which may for example have a capacity of 100 pF) and (parallel to capacitor  155 ) switch  160  for performing a reset. The switch  160  is triggered by the R 2  signal from the counter unit  110 . The higher gain circuit  135  is connected to comparator  165 . The comparator  165  compares the integration value generated by the higher gain circuit  135  to a reference voltage (the absolute value of the reference voltage forming the reset threshold). Switch  170  connects the higher gain circuit  135  to the analog-to-digital converter  115 . The switch  170  is triggered by the S 2  signal from the counter unit  110 . Similarly, the lower gain circuit  140  is connected to switch  175  at its minus input. The plus input is connected to the ground  150 . Furthermore, the minus input is connected to capacitor  180  (which may for example have a capacity of 10 nF) and (parallel to capacitor  180 ) switch  185  for performing a reset. The switch  185  is triggered by the R 1  signal from the counter unit  110 . The lower gain circuit  140  is connected to comparator  190 . The comparator  190  compares the integration value generated by the lower gain circuit  140  to a reference voltage (the absolute value of the reference voltage forming the switching threshold). Switch  195  connects the lower gain circuit  140  to the analog-to-digital converter  115 . The switch  195  is triggered by the  51  signal from the counter unit  110 . 
         [0048]    The current to be measured is input into the higher gain circuit  135  over switch  145 , which is connected to the counter unit  110  and triggered by the H 2  signal from the counter unit  110 . The counter unit  110  counts the integration time with 10 ns increments (100 MHz clock). If the maximum integration time expires (for instance 100 ms) without the integration value exceeding the switching threshold, the value generated by the analog-to-digital converter  115  is used (see also  FIG. 2 ). If the integration value exceeds the switching threshold before expiration of the maximum integration time, the current to be measured is input into the lower gain circuit  140  over switch  175 , which is connected to the counter unit  110  and triggered by the H 1  signal from the counter unit  110 . The value of the counter unit  110  is latched and this value can be used as a result of the measurement (see also  FIG. 3 ). If the lower gain circuit  140  is switched on and the integration value generated by the lower gain circuit  140  exceeds the reset threshold (as defined by the comparator  190 ) before expiration of the maximum integration time, the lower gain circuit  140  is reset by closing the switch  185 , which is triggered by the R 1  signal from the counter unit  110 . After resetting the lower gain circuit  140 , the lower gain circuit  140  continues to integrate the current to be measured and is reset each time the integration value exceeds the reset threshold as long as the maximum integration time has not expired. The total number of resets is counted by the counter unit  110 . Counting the number of resets gives information about the measured current (see  FIG. 4 ). 
         [0049]    Clearly, it is possible to introduce at least one further integration circuit into the determination circuit  100  parallel to the higher gain circuit  135  and the lower gain circuit  140 , each further integration circuit having a gain that is lower than the previously lowest gain. In this way, a cascade of circuits would be formed. A further integration circuit would allow a current being measured and the previously lowest gain circuit to be switched to the further integration circuit once integration value generated by the previously lowest gain circuit exceeds the switching threshold of that circuit. The switch from one circuit to the next would be similar to the switch from the higher gain circuit  135  to the lower gain circuit  140  once the integration value generated by the higher gain circuit  135  exceeds the switching threshold of the higher gain circuit  135 . However, to obtain increasingly low gains, capacitors having increasingly large capacitances will be required. In practice, resetting increasingly large capacitances can become problematic. Consequently, a determination circuit  100  as shown in  FIG. 1 , with the lower gain circuit  140  being able to be reset multiple times, is a suitable alternative to a determination circuit comprising a cascade of increasingly lower gain circuits. 
         [0050]    Moreover, it is clear that a determination circuit similar to the determination circuit  100  but comprising only a single gain circuit capable of being reset multiple times is also a possibility. 
         [0051]    The determination circuit  100  enables to measure currents over an extremely wide dynamic range. Limitations are caused by the photodiode  125  rather than the integrator electronics. 
         [0052]      FIG. 2  schematically shows a lower current measurement using only the higher gain circuit shown in  FIG. 1 . Plotted along the horizontal axis is a time interval representing the maximum integration time. In the example of  FIG. 2  the maximum integration time is 100 ms. However, other values may be chosen depending on need. Along the vertical axis electronic potential is plotted, with 0 V representing the potential of the ground  150  (for the reference numbers the reader is referred to  FIG. 1 ) and with Vref representing the reference potential used with the comparator  165  to define the reset threshold. During measurement of a low current, for instance a current of 800 pA, the integration value generated by the higher gain circuit  135  will not reach the reset threshold. The integration value as a function of time is indicated in  FIG. 2  by the line  200 . After expiration of the maximum integration time, V 1  can be used as the measurement result. 
         [0053]      FIG. 3  schematically shows a higher current measurement using both the higher gain circuit and the lower gain circuit circuit shown in  FIG. 1 . Just as in  FIG. 2 , a time interval representing the maximum integration time is plotted along the horizontal axis. In the example of  FIG. 3  the maximum integration time is 100 ms. However, other values may be chosen depending on need. Along the vertical axis electronic potential is plotted, with 0 V representing the potential of the ground  150  (for the reference numbers the reader is referred to  FIG. 1 ), with Vref 1  representing the reference potential used with the comparator  165  to define the switching threshold, and with Vref 2  representing the reference potential used with the comparator  190  to define the reset threshold. At t 1  the integration value generated by the higher gain circuit  135  and indicated by the line  300  exceeds the switching threshold. At that moment the lower gain circuit  140  is switched on. When the maximum integration time expires, the voltage output V 2 , based on the integration value generated by the lower gain circuit  140 , is used as the measurement value. The integration value generated by the lower gain circuit  140  is a function of time is indicated by the line  305 . The current measured in the example shown in  FIG. 3  may, for instance, be 8 μA. This is 10,000 times the current that, by way of example, was measured in  FIG. 2 . 
         [0054]      FIG. 4  schematically shows the timing of the multiple integration principle on a higher current. Just as in the previous two figures, a time interval representing the maximum integration time is plotted along the horizontal axis. In the example of  FIG. 4  the maximum integration time is 100 ms. However, other values may be chosen depending on need. Along the vertical axis electronic potential is plotted, with 0 V representing the potential of the ground  150  (for the reference numbers the reader is referred to  FIG. 1 ), Vref 1  representing the reference potential used with the comparator  165  to to define the switching threshold, and with Vref 2  representing the reference potential used with the comparator  190  to define the reset threshold. At t 1  the integration value generated by the higher gain circuit  135  and indicated by the line  400  reaches the switching threshold. At that moment, the lower gain circuit  140  is switched on. At t 2  the integration value generated by the lower gain circuit  140  and indicated by the line  405  exceeds the reset threshold and the lower gain circuit  140  is reset. Following the reset, the lower gain circuit  140  continues to integrate the current until the maximum integration time expires. Again, the integration value generated by the lower gain circuit  140  as a function of time is indicated by the line  405 . However, in  FIG. 4  the lower gain circuit  140  reaches the reset threshold multiple times after the first reset and before expiration of the maximum integration time. Each time the lower gain circuit  140  reaches the reset threshold, it is reset until the maximum integration time expires. In the example of  FIG. 4 , the current measured by the lower gain circuit  140  equals six reset cycles minus V 2 . 
         [0055]    Inventor: are the results of the higher gain circuit and the lower gain circuit added or is the result of the lower gain circuit compensated for the less than maximal integration time, 100−t 1  ms? 
         [0056]      FIG. 5  schematically shows an embodiment of the method according to the invention. In step  500  a current is integrated over a predefined maximum integration time using an integration unit. An embodiment of such an integration unit is comprised in the determination circuit  100  shown in  FIG. 1 . The integration results in integration value. In step  505  the time during which the current is integrated is counted from the start of the integration to the expiration of the maximum integration time. If the absolute value of the integration value is below a predetermined threshold at the expiration of the maximum integration time a first measurement result is output. This is done in step  510 . If the absolute value of the integration value exceeds the predetermined threshold before the expiration of the maximum integration time, the integration unit is reset in step  515 . Following the reset, the integration unit continues integrating the current. In step  520 , step  515  is repeated until the maximum integration time expires, while counting the number of resets. Finally, in step  525 , a second measurement result is output based on at least one of the integration value and the number of resets. 
         [0057]      FIG. 6  schematically shows an embodiment of a device for imaging an interior of a turbid medium comprising a determination circuit according to the invention. The device  600  comprises a light source  605  for generating light to be coupled into the turbid medium  610 . The turbid medium  610  is accommodated in a receiving volume  615 , which is bounded by a receptacle  620 . The receptacle  620  comprises a plurality of entrance positions for light  625  for coupling light from the light source  605  into the receiving volume  615 . The receptacle  620  further comprises a plurality of collection positions for light  630  for collecting light emanating from the turbid medium  610  and, hence, from the receiving volume  615 . The light source  605  is successively coupled to an entrance position for light chosen from the plurality of entrance positions for light  625  using an optical switch  630 . The light source  605  is optically coupled to the optical switch  635  using light guide  640 . The optical switch  635  is optically coupled to the receptacle  620  using light guides  645 . In medical diagnostics a device such as the device  600  may be used for imaging an interior of a female breast. In that case, light generated by the light source  605  typically has a wavelength within the range of 400 nanometres to 1400 nanometres. Light emanating from the receptacle  620  at the plurality of collection positions for light  630  is coupled to a photodetector unit  650 . The photodetector unit  650  is optically coupled to the receptacle  620  using light guides  655 . The photodetector unit  650  comprises the determination circuit  100  shown in  FIG. 1 . Using the photodetector unit  650  light collected at the plurality of collection positions for light  630  is used to generate electronic signals representing the intensity of light emanating from the receptacle  620  at the plurality of collection positions for light  630 . The based on the obtained electronic signals, an image of an interior of the turbid medium  610  is reconstructed using image reconstruction unit  660 . The space inside the receptacle  620  not occupied by the turbid medium  610  may be filled with a matching medium  665  having optical properties, such as absorption and scattering coefficients, that substantially match the corresponding characteristics of the turbid medium  610 . In this way, boundary of facts stemming from coupling light into and out of the turbid medium  610  reduced. Moreover, use of a matching medium  665  prevents the occurrence of an optical short-circuit. An optical short-circuit occurs if light emanating at a collection position for light comprises both light that has passed through the turbid medium  610  and light that has passed through the receiving volume  615 , but not through the turbid medium  610 . As the turbid medium  610  strongly attenuates light that passes through it, light reaching a collection positions for light without having passed through the turbid medium  610  may dwarf the intensity of light that has passed through the turbid medium  610 . This would hamper a proper measurement. When using a matching medium  665 , the turbid medium  610  and the matching medium  665  effectively form a single turbid medium filling the receiving volume  615 . 
         [0058]      FIG. 7  schematically shows an embodiment of a medical image acquisition device comprising a determination circuit according to the invention. The medical image acquisition device  700  comprises the element is comprised in the device  600  shown in  FIG. 6 . This is indicated by the dashed rectangle  705 . The medical image acquisition device  700  further comprises a screen  710  for displaying a reconstructed image of an interior of the turbid medium  610  and an operator interface  715 , for instance a keyboard, allowing an operator to interact with the medical image acquisition device  700 . 
         [0059]    Table 1 lists current measurements using only the higher gain circuit, only the lower gain circuit, or both circuits. 
         [0060]    It should be noted that the above-mentioned embodiments illustrate rather than limit the invention, and that those skilled in the art will be able to design many alternative embodiments without departing from the scope of the appended claims. In the claims, any reference signs placed between parentheses shall not be construed as limiting the claim. The word “comprising” does not exclude the presence of elements or steps other than those listed in a claim. The word “a” or “an” preceding an element does not exclude the presence of a plurality of such elements. The invention can be implemented by means of hardware comprising several distinct elements, and by means of a suitably programmed computer. In the system claims enumerating several means, several of these means can be embodied by one and the same item of computer readable software or hardware. The mere fact that certain measures are recited in mutually different dependent claims does not indicate that a combination of these measures cannot be used to advantage.

Technology Category: g