Abstract:
A demodulation pixel architecture allows for demodulating an incoming modulated electromagnetic wave, normally visible or infrared light. It is based on a charge coupled device (CCD) line connected to a drift field structure. The drift field is exposed to the incoming light. It collects the generated charge and forces it to move to the pick-up point. At this pick-up point, the CCD element samples the charge for a given time and then shifts the charge packets further on in the daisy chain. After a certain amount of shifts, the multiple charge packets are stored in so-called integration gates, in a preferred embodiment. The number of integration gates gives the number of simultaneously available taps. When the cycle is repeated several times, the charge is accumulated in the integration gates and thus the signal-to-noise ratio increases. The architecture is flexible in the number of taps. A dump node can be attached to the CCD line for dumping charge with the same speed as the samples are taken. Different implementations are described herein, which allow for smaller design or faster speed. The pixel structure can be exploited for e.g. 3D time-of-flight imaging. Both heterodyne and homodyne measurements are possible. Due to the highly-efficient charge transport enabled by static drift fields in the photo-sensitive region and small-sized gates in the CCD chain, high frequency bandwidth from just a few Hertz (Hz) up to greater GHz is supported. Thus, the pixel allows for highly-accurate optical distance measurements. Another possible application of this pixel architecture is fluorescence lifetime imaging microscopy (FLIM), where short laser pulses for triggering the fluorescence have to be suppressed.

Description:
RELATED APPLICATIONS 
     This application claims the benefit under 35 USC 119(e) of U.S. Provisional Application No. 61/092,548, filed on Aug. 28, 2008, which is incorporated herein by reference in its entirety. 
     BACKGROUND OF THE INVENTION 
     The demodulation of modulated light at the pixel level requires the switching of a photo-generated charge current. While possible to handle both electron as well as hole currents, the common methods today use the photo-generated electron currents. This choice is largely due to the higher mobility of electrons in the semiconductor material. Some pixel architectures do the necessary signal processing based on the photo-current while others work directly in the charge domain. 
     All of the pixel architectures transfer photocharges through the photo-sensitive detection region to a subsequent storage area or to a subsequent processing unit. In the case of charge-domain based pixel architectures, the photocharges are generally transferred to an integration node. In order to demodulate an optical signal, the pixel has to contain at least two integration nodes that are accumulating the photo-generated charges during different time intervals. 
     Different pixel concepts have been realized in the last few decades. The basic principle of an in-pixel demodulation sensor was first described in U.S. Pat. No. 5,856,667 to Thomas Spirig and Peter Seitz. Each pixel of the sensor had photo-sensitive areas and transfer gates or switches associated with each of the integration sites. The sensor enables in-pixel sampling of the impinging light signal with theoretically an arbitrary number of samples. 
     Another similar pixel concept was described in T. Ushinaga et al., “A QVGA-size CMOS time-of-flight range image sensor with background light charge draining structure”, Three-dimensional image capture and applications VII, Proceedings of SPIE, Vol. 6056, pp. 34-41, 2006. Here, a thick field-oxide layer is used to smear the potential distribution below the demodulation gates. 
     A common problem of the afore-mentioned pixel architectures is the slowness of the charge transport through the semiconductor material. This decreases significantly the quality of the in-pixel demodulation process. In all pixel structures, the limiting transport speed is the step-wise potential distribution in the semiconductor substrate that is used to transport the charges through the semiconductor in lateral direction out of the photosensitive region. In those configurations, thermal diffusion dominates the transport speed instead of movement by the lateral electric drift fields resulting from the step-wise potential distribution. 
     More recently, new approaches to speeding the in-pixel transport of the charges have been proposed. One example by Peter Seitz and described in U.S. Pat. No. 7,498,621 B2 generates the lateral electric drift fields by passing a current through very high-resistive poly-silicon gate electrodes with the intent of producing a smoother potential distribution. Similarly, D. van Nieuwenhove et al., “Novel Standard CMOS Detector using Majority Current for guiding Photo-Generated Electrons towards Detecting Junctions”, Proceedings Symposium IEEE/LEOS Benelux Chapter, 2005, introduced another drift field pixel where a drift field in the substrate is generated by the current of majority carriers. To perform demodulation of photo-generated minority carriers, the majority current is dynamically controlled by the modulation signal. 
     The afore-mentioned drift field pixel concepts have drawbacks, however. First, the demodulation requires the switching of large capacitances since the whole sensitive area needs to be dynamically controlled. Secondly, an electronic current is used to generate the drift fields, resulting in significant in-pixel power consumption. 
     An alternative pixel concept uses a static drift field pixel. The architecture described in European Patent Application EP 1 624 490 A1, entitled “Large-area pixel for use in an image sensor”, overcomes these two problems. In contrast to the architectures mentioned before, it separates the detection and the demodulation regions within the pixel. It shows lower power consumption and, at the same time, it supports fast in-pixel lateral charge transport and demodulation. 
     One major application of demodulation pixels is found in real-time 3-D imaging. By demodulating the optical signal and applying the discrete Fourier analysis on the samples, parameters such as amplitude and phase can be extracted for the frequencies of interest. If the optical signal is sinusoidally modulated for example, the extraction based at least three discrete samples will lead to the offset, amplitude and phase information. The phase value corresponds proportionally to the sought distance value. Such a harmonic modulation scheme is often used in real-time 3-D imaging systems having incorporated the demodulation pixels. 
     Another possible application of these pixel architectures is fluorescence lifetime imaging microscopy (FLIM), where short laser pulses are used to trigger the fluorescence. 
     The precision of the pixel-wise distance measurement is directly proportional to the modulation frequency. Therefore, high-speed charge transfer from the photo-sensitive area to the storage site is of highest importance to enable high precision phase measurement. 
     SUMMARY OF THE INVENTION 
     Current demodulation pixels typically need to trade off high sampling frequencies against the number of samples taken. In most commercially available pixels, photocharges are stored in only two storage sites per pixel in order to maximize sampling frequencies. The present invention has the capability to have both a high sampling frequency and a relatively large number of samples. This is achieved by having a photosensitive region, possibly using a static drift field, in combination with a subsequent daisy chain of storage sites. 
     Sensors based on this pixel architecture allow for developing completely new applications, where many samples need to be acquired at very high speed. One example is submillimeter pseudo noise 3D-imaging based on the time-of-flight principle. 
     Embodiments of the invention can have almost an arbitrary number of sample nodes. So far, the implementation of demodulation pixels with more than two sampling storage sites were strongly hindered by the integrated circuit design layout rules restrictions. Since the demodulation region is preferably quite small compared to photo-sensitive area, in most cases the demodulation region does not offer enough space to implement the design of more than two sampling stages. 
     Furthermore, embodiments can reduce the problem of mismatch of the different sampling channels. The behavior mismatch of the different samples is mainly caused by the different directions of the photocharge transfer for different samples. Here, all samplings can be performed in the same direction of the semi-conductor lattice. In other words, the transfer direction does not have to be changed and, hence, the mismatch between samples is strongly reduced. 
     In general, according to one aspect, the invention features a pixel comprising a photosensitive region in which incoming light is converted into photocharges, a lateral drift field in the photosensitive region transporting the photocharges to a pickup point and a chain of charge storage sites that receives the photocharges from the photosensitive region at the pickup point, the photocharges corresponding to different time intervals are conveyed through successive charge storage sites of the chain. 
     In general, according to another aspect, the invention features a photosampling method comprising converting incoming light into photocharges, transporting the photocharges to a start of a chain of storage sites with a lateral drift field, and moving the photocharges as charge packets corresponding to different time intervals through successive charge storage sites of the chain. 
     In general, according to another aspect, the invention features a sensor comprising a one or two dimensional array of pixels, wherein each of the pixels comprises a photosensitive region in which incoming light is converted into photocharges and transported with a lateral drift field, and a chain of charge storage sites that receives the photocharges from the photosensitive region, the photocharges corresponding to different time intervals are conveyed through successive charge storage sites of the chain. 
     In general, according to another aspect, the invention features an imaging system comprising: a light source for illuminating a scene with a modulated optical signal characterized by a modulation period, and a sensor for detecting the modulated optical signal from the scene, the sensor comprising an array of pixels, each of the pixels including: a photosensitive region in which incoming light is converted into photocharges, and a chain of charge storage sites that receive the photocharges from the photosensitive region, the photocharges corresponding to different time intervals within the modulation time period are conveyed through successive charge storage sites of the chain. 
     In general, according to still another aspect, the invention features a pixel comprising: a photosensitive region in which incoming light is converted into photocharges, a chain of charge storage sites that receives the photocharges from the photosensitive region at the pickup point, the photocharges corresponding to different time intervals are conveyed through successive charge storage sites of the chain, and charge integration sites associated with respective charge storage sites, the photocharges being transferred from the charge storage sites to the associated charge integration sites. 
     In general, according to still another aspect, the invention features a photosampling method comprising: converting incoming light into photocharges, transporting the photocharges to a start of a chain of storage sites, moving the photocharges as charge packets corresponding to different time intervals through successive charge storage sites of the chain, and integrating charge packets from the same time intervals within different periods in integration sites associated with respective storage sites. 
     In general, according to another aspect, the invention features a sensor comprising a one or two dimensional array of pixels, wherein each of the pixels comprises: a photosensitive region in which incoming light is converted into photocharges, and a chain of charge storage sites that receives the photocharges from the photosensitive region, the photocharges corresponding to different time intervals are conveyed through successive charge storage sites of the chain, and charge integration sites associated with respective charge storage sites, the photocharges being transferred from the charge storage sites to the associated charge integration sites. 
     The above and other features of the invention including various novel details of construction and combinations of parts, and other advantages, will now be more particularly described with reference to the accompanying drawings and pointed out in the claims. It will be understood that the particular method and device embodying the invention are shown by way of illustration and not as a limitation of the invention. The principles and features of this invention may be employed in various and numerous embodiments without departing from the scope of the invention. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       In the accompanying drawings, reference characters refer to the same parts throughout the different views. The drawings are not necessarily to scale; emphasis has instead been placed upon illustrating the principles of the invention. Of the drawings: 
         FIG. 1  is a schematic drawing of a demodulation pixel according to one embodiment of the present invention; 
         FIG. 2  is a circuit diagram showing processing circuitry for the demodulation pixel; 
         FIG. 3  is a circuit diagram showing a sensor incorporating demodulation pixels; 
         FIG. 4  is a schematic drawing of a demodulation pixel according to another embodiment of the present invention; 
         FIGS. 5   a - 5   d  show the operation of the 4-tap demodulation pixel; 
         FIGS. 6   a  and  b  show the operation of the demodulation on a 3-tap pixel; 
         FIG. 7  is a schematic drawing of a 4-tap demodulation pixel according to another embodiment of the present invention. 
         FIG. 8  is a schematic drawing of a demodulation pixel according to another embodiment of the present invention; 
         FIG. 9  shows a conventional scheme of the three-dimensional-measurement set-up using a sensor comprising demodulation pixels; and 
         FIGS. 10   a  and  10   b  are plots representing the optical intensity and the charge flow as a function of the time for the emitted signal and the received signal, respectively, using the scheme of  FIG. 8 . 
     
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     The following discussion concerns a sensor with a p-doped substrate in which electrons are the useful photo-generated charge carriers. All considerations can also be done for n-doped material, with holes as carriers of information. In this case the voltages applied to gates and/or diffusions would be reversed. 
       FIG. 1  shows a demodulation pixel  100  embodied in a semiconductor substrate that has been constructed according to the principals of the present invention. 
     The pixel  100  comprises a photosensitive region  110 . This is typically characterized by a portion of the semiconductor substrate that receives incoming light or other radiation and is not otherwise shielded by opaque layers, such as metal, layers. The photosensitive region  110  has a photocharge transport area  115  that moves the photocharges to a pickup point  112 , typically at one end of the transport area  115 . 
     The photocharge transport area  115  transports the photocharges to the pickup point  112  typically as fast as possible in order to minimize any low-pass filtering effects on the optoelectronically converted signal. The fast charge carrier transport is realized by a lateral drift field  116 . That drift field  116  can be generated by various methods. The following is an itemization of some possible methods. One realization of static drift fields is made by a photo-transparent gate of high-resistive material above the semiconductor substrate and an intervening insulator layer. The application of a potential difference generates a current flow through the gate, and hence a constant lateral electric field is created. That potential distribution is mirrored to the semiconductor substrate due to the capacitive coupling between the gate and the semiconductor so that photo-generated charges will be directed by the electric drift field. Another method to generate the lateral electric drift field within the photo-sensitive area  110  is to implement built-in drift fields. The built-in drift field can be generated by gradually changing the doping concentration through the photo-sensitive area. Other examples for generating lateral electric drift fields within the photosensitive detection region  110  of the pixel  100  are discrete gate structures, floating gates or floating diffusions, dendritic gate structures, PIN photo diodes, and majority carrier currents through the substrate. The current preferred embodiment uses overlapping gates structures to which different static potentials are applied. Combinations of the above mentioned methods to generate the lateral electric drift fields can also be implemented. The electrons generated in the drift field region are attracted by positive potentials. Therefore the gate potentials increase from the far end to the pick-up point  112 . At this pick-up point all electrons are accumulated until the dedicated sampling process is finished. After that they are transported into the daisy chain  152 . 
     More examples and description on implementations of the photocharge transport area  115 , therein termed the “detection region”, are provided in U.S. patent application Ser. No. 12/090,404, by Bernhard Buettgen, filed on Apr. 16, 2008, entitled Device and Method for the Demodulation of Modulated Electromagnetic Wave Fields, which is incorporated herein in its entirety by this reference. 
     From the pickup point  112  the photo-generated charges are transferred to a daisy chain of charge storage sites  152 . This daisy chain  152  is preferably in a non-photosensitive region  150 . In its implementation, the daisy chain  152  comprises a series of charge-coupled device (CCD) gates. Typically, metal layers are used to cover this region  150  to block the generation of photocharges in the substrate. 
     In more detail, the daisy chain  152  of storage sites, or gates,  154  comprises a first storage site  154   a  that is separated from the pickup point  112  by a first isolation node, or barrier gate structure,  156   a . In operation the potentials applied to the isolation nodes  156  and storage sites  154  are controlled by a pixel controller  102  so that photocharges generated in the photosensitive region  110  and transported to the pickup point  112  by the lateral drift field  116  are allowed to flow through the first isolation node  156   a . The pixel controller  102  raises the potential applied to the isolation node  156   a  so that the first charge storage site  154   a  contains a charge packet of photocharges that were generated in the photosensitive region  110  during a time interval. The pixel controller  102  then isolates the first charge storage site  154   a  from the pickup point  112  by lowering the potential applied to the isolation node  156   a.    
     During a subsequent time interval, the charge packet contained in first storage site  154   a  is transferred to a second storage site  154   b  in the daisy chain  152 . This process is accomplished by the pixel controller  102  lowering the potential applied to the first storage site  154   a  while raising the potential applied to the second storage site  154   b  and an intervening second isolation node, or barrier gate structure,  156   b . The potential applied to the second isolation node  156   b  is thereafter lowered to isolate the second storage site  154   b  from the first storage site  154   a . This transfer process leaves the first storage site  154   a  ready to receive the next charge packet associated with the next sampling time interval. 
     During a third time interval, the charge packet contained in second storage site  154   b  is transferred to a third storage site  154   c  and the charge packet contained in the first storage site  154   a  is transferred to the second storage site  154   b . This process is again accomplished by the pixel controller  102  lowering the potentials applied to the upstream storage sites and isolation nodes while raising the potentials applied to the successive storage sites. The potentials applied to the isolation nodes is thereafter lowered to isolate the storage sites from each other. This transfer process again leaves the first storage site  154   a  ready to receive the next charge packet associated with the next sampling time interval. 
     In the illustrated embodiment, the daisy chain  152  is shown with a series of three storage sites  154   a - 154   c . The illustrated pixel can be implemented with an almost arbitrary number of storage sites in the daisy chain  152 , however. For sinusoid demodulation or phase determination, at least three storage sites in the daisy chain  152  is desirable. More storage sites are desirable when demodulating or determining the phase of other functions. Demodulation of n-bit pseudo noise sequences uses n-length daisy chains, where n=4 to 16, or more, in some implementations. 
     In the preferred embodiment, each storage site  154  has at least one associated integration site  160 . The integration site is typically implemented as integration gate or diffusion. In the illustrated example, the first storage site has two integration sites  160   a   2 ,  160   a   2 . Similarly, the second storage site has two integration sites  160   b   2 ,  160   b   2 , and the third storage site has two integration sites  160   c   2 ,  160   c   2 . 
     Each of the integration sites  160  is separated from the associated storage sites from a transfer node or gate structure  158 . 
     In typical operation, once the daisy chain  152  has been completely filled with charge packets corresponding to a series of sampling time intervals, the charge packets are transferred from the storage sites  154  to the integration sites  160 . This process is controlled by the pixel controller  102  that raises the potentials of the transfer nodes  158  while lowering the potentials of the storage sites  154 . For example, to transfer the charge packet from the second storage site  154   b  to the integration site  160   b   2 , the pixel controller  102  lowers the potential of the second storage site  154   b , while raising the potential of the transfer gate  158   b   2 . In this way, the photocharges from many sampling sequences are integrated together for improved signal to noise operation. That is, the process of filling the daisy chain  152  with charge packets is repeated, such as 10 or 100 or even up to 1 million times or more, with each of the integration sites  160  storing the total number of photocharges from these repeated sampling processes. 
     It is not mandatory that each integration site or gate  160  has its own separately controlled transfer node(s) or gate(s)  158 , but it is also possible that there is one large transfer node or gate  158  for all integration sites  160  that is controlled by the pixel controller  102  with one master signal such that the charge packets are transferred out of the storage sites  154  to the integration sites  160  all together at the same time, in one implementation. 
       FIG. 2  shows additional circuitry associated with the pixel  100 . The integration sites  160  are coupled to processing circuitry  210  implemented in each pixel  100 . This circuitry  210  preferably includes analog to digital converters, subtraction elements and/or comparator circuits for determining the amount of photocharge contained in each of the integration sites  160  or the relative amount of photocharges within the integration sites  160 . In other examples, the circuitry  210  determines the amount of photocharge contained in each of the storage sites  154  directly, without the necessity for the integration sites  160 , especially in low noise environments. In one such example, without separate integration sites  160 , the storage sites  154  are configured in a ring topology and thus the charge packets contained in the storage sites move stepwise around the ring and are successively further filled each time they are opposite the pickup point with the newly generated photocharges. 
       FIG. 3  shows the general implementation of the pixel architecture within the frame of a full sensor  200 . Typically, sensor  200  comprises a one or two dimensional array of pixels  100 . Row selection is accomplished with row decoder  212 . Column selection is realized via shift registers or digital decoders. Readout circuitries include registers  214  and additional processing circuits  216 . 
       FIG. 4  illustrates one implementation of the pixel  100  based on a 4-tap architecture, which is a specific implementation of this pixel concept. 
     If the pixel  100  is used to sample a sinusoidally modulated light signal for time intervals corresponding to four time points, each separated by pi/2, the two upper integration sites  160   d ,  160   b  preferably correspond to the phases 0 and 180 degrees and the bottom integration sites  160   c ,  160   a  correspond to 90 and 270 degrees. 
     A dump node  410  is included at the end of the daisy chain  152 . During an initial calibration or pixel reset operation, photocharges are cleared from the pixel  100  by shifting them into the dump node  410 . Often these photocharges are the result of background illumination and thus constitute a noise source. The dump node does not have to be at the end of the daisy chain, however. For example, in other implementations, the dump node replaces one of the integration sites. 
     The whole 4-tap sampling procedure is depicted in  FIGS. 4 and 5   a - 5   d . During sampling of the optical signal, all photocharges drift to the pick-up point  112 , forced by the lateral electrical drift field  116 . When the sampling time or interval is finished, the photocharges are transferred into the daisy chain  152  by a normal charge-coupled device (CCD) register operation, in one implementation, as shown in  FIG. 4 . Then, the next charge packet can be sampled as shown in  FIG. 5   a . After each sampling step the charge packets in the CCD daisy chain  152  are shifted further as shown in  FIGS. 5   b  and  5   c . The CCD daisy chain might be implemented e.g. as 3-phase CCD structure or as 4-phase CCD structure. This means the isolation nodes  156  each comprise a barrier gate structure of typically more than one CCD gate. 
     After the fourth sampling, four charge packets are within the CCD daisy chain  152 , as shown in  FIG. 5   d . In order to store them, the charge packets in each of the storage sites  154   a ,  154   b ,  154   c ,  154   d  are shifted to the integration sites  160   a ,  160   b ,  160   c ,  160   d  dedicated to the particular signal phases. The whole 4-tap sampling is repeated several times even up to more than 1 million times and the charges are accumulated within the integration sites  160   a ,  160   b ,  160   c ,  160   d  in order to increase the signal-to-noise ratio of the demodulation process. 
     The dump node  410  at the right end of the CCD daisy chain  152  allows for the dumping of photocharges during the readout phase. Basically, the design of a dump node features a flexible operation of this pixel architecture allowing for using different optical modulation techniques such as burst mode of operation or pulse mode of operation. 
       FIGS. 6   a ( 1 )- 6   a ( 5 ) show the demodulation principle based on a 3-tap pixel.  FIG. 6   a  illustrates the timing how the charges are first conveyed from the pick-up point  112  through the different isolation nodes  156   a - c  and storage sites  154   a - c  as shown in  FIGS. 6   a ( 1 )-( 4 ). As soon as all the storage sites  154   a - c  get their charge packet  FIG. 6   a  ( 4 ), the charges are transferred below the transfer gates  158   a - c  to the integration sites  160   a - c    FIG. 6   a  ( 5 ). This process can then be repeated up to more than 1 million times. Again, a dump node can be implemented to remove those electrons generated by the background light while no modulated light is emitted. Here, the daisy chain  152  can be implemented with a 3 phase CCD gate structure or a 4 phase CCD gate structure. 
       FIG. 6   b  shows on the specific case of sine wave modulated system, where the impinging sine wave is sampled at three different time intervals. The photo-charges for each time interval sample are integrated once each period in the corresponding integration sites  160   a - c.    
       FIG. 7  sketches a pixel with four integration sites  160   a - d . The daisy chain is built using a 4-phase CCD gate structure principle by repeating the G 1  to G 4  gate array in each of the storage sites  154   a - 154   d  and isolation nodes  156   a - 156   d . In this case, the isolation nodes  156   a - d  consists of three gates G 2 -G 3 , while the storage sites  154   a - d  represents G 1 . A 3-phase CCD transfer gate structure can be designed similarly by e.g. removing all G 4  gates from the isolation nodes  158   a - d.    
     Embodiments of the present invention can show some significant gains compared to previous drift field pixels. In summary those are:
         Design of N taps possible without decreasing the sampling performance due to the necessity of enlarging the pick-up node.   Speed of the pixels is not limited by the number of taps. It is rather determined by the size of the detection region and on the transfer speed from one to another CCD shift register. Independent on the speed, an arbitrary number of taps could be designed.   No strong impact of inclined optical incident on the sampling process is expected since all four taps experience the charge accumulation under the same gate and the transport is into the same direction.   Dump nodes can easily be integrated without leading to the requirement of switching the constant voltage used for the lateral electric drift fields.       

     Consideration of the Sampling Frequency 
     The sampling frequency is determined by the geometry of the photo-sensitive detection/drift region and by the time needed to transport the accumulated charge from one CCD register gate to the next one within the CCD daisy chain  152 . Here, the sampling frequency is not influenced by the number of taps that one pixel has. More taps just add more CCD registers or storage sites  154  but do not require any change of the detection region or pick-up node. 
     A theoretical analysis of the maximum 3 dB-cut-off sampling frequency limited by the finite charge transport time through the detection region of any kind of demodulation pixel to the sample node can be estimated. Basically, an average transport time can be modeled, which is the sum of any drift and diffusion times of the charges until they reach the sample node. Based on the mean transport time Ttr, a 3 dB-frequency Fmax can be found as
 
 F max=7/(16  Ttr )
 
     In a simplified model we can assume that there is one time component caused by charge drift Tdrift and one component Treg due to the transport through the register so that
 
 Ttr=T drift+ Treg  
 
     The pixel design with regard to the geometry of the detection region and the CCD chain&#39;s gates needs to be accomplished in such a way that
 
( T drift+ Treg )&lt;7/(16  F desired)
 
     is fulfilled. Here Fdesired is the maximum sampling frequency that is desired to be still supported by the pixel. 
     As originally stated, the equation has no dependence on the number of pixel taps. The pixel can be optimized for speed by optimizing the drift time and the transport time through the CCD register. This implies at the same time, that the current system benefits from the ongoing miniaturization of semiconductor processes because smaller process feature sizes allow for shorter charge transport times. 
       FIG. 8  shows an embodiment where the charge samples can be moved to one of two daisy chain segments  152 - 1 .  152 - 2 . Here, the transfer gates  158  and integration gates are located on only one side, resulting in advantages for routing. 
       FIG. 9  illustrates the basic principle of a 3D-measurement camera system based on a sensor  200  comprising the demodulation pixels  100  described above. 
     Modulated illumination light ML 1  from an illumination module or light source IM is sent to the object OB of a scene. A fraction of the total optical power sent out is reflected to the camera  10  and detected by the 3D imaging sensor  200 . The sensor  200  comprises a two dimensional pixel matrix of the demodulation pixels  100 . Each pixel  100  is capable of demodulating the impinging light signal ML 2  as described above. A control board CB regulates the timing of the camera  10 . The phase values of all pixels correspond to the particular distance information of the corresponding point in the scene. The two-dimension gray scale image with the distance information is converted into a three-dimensional image by image processor IP. This can be displayed to a user via display D or used as a machine vision input. 
     The distance R for each pixel is calculated by
 
 R =( c *TOF)/2,
 
with c as light velocity and TOF corresponding to the time-of-flight. Either pulse intensity-modulated or continuously intensity-modulated light is sent out by the illumination module or light source IM, reflected by the object and detected by the sensor. With each pixel  100  of the sensor  200  being capable of demodulating the optical signal at the same time, the sensor is able to deliver 3D images in real-time, i.e., frame rates of up to 30 Hertz (Hz), or even more, are possible. In pulse operation the demodulation would deliver the time-of-flight directly. However, continuous sine modulation delivers the phase delay (P) between the emitted signal and the received signal, also corresponding directly to the distance R:
 
 R =( P*c )/(4*pi* f  mod),
 
where f mod is the modulation frequency of the optical signal. Typical state-of-the-art modulation frequencies range from a few MHz up to a few hundreds of MHz or even GHz.
 
       FIGS. 10   a  and  10   b  show the relationship between signals for the case of continuous sinusoidal modulation and the signal sampling. Although this specific modulation scheme is highlighted in the following, the utilization of the pixel in 3D-imaging is not restricted to this particular scheme. Any other modulation scheme is applicable: e.g. pulse, rectangular, pseudo-noise or chirp modulation. Only the final extraction of the distance information is different. 
       FIG. 10   a  shows both the modulated emitted illumination signal ES and received signal RS. The amplitude A, offset B of the received signal RS and phase P between both signals are unknown, but they can be unambiguously reconstructed with at least three samples of the received signal. BG represents the received signal part due to background light. 
     In  FIG. 10   b , a sampling with four samples per modulation period is depicted. Each sample is an integration of the electrical photo-signal in the integration gates or diffusion regions described above over a duration dt that is a predefined fraction of the modulation period. Typically, in demodulation pixels with 4 integration sites dt corresponds to a quarter of the period. In order to increase the signal to noise ratio of each sample the photo-generated charges may be accumulated over several—up to more than 1 million—modulation periods in the integration sites. 
     The electronic timing circuit, employing for example a field programmable gate array (FPGA), generates the signals for the synchronous channel activation in the demodulation stage. 
     Using these four samples, the three decisive modulation parameters amplitude A, offset B and phase shift P of the modulation signal can be extracted by the equations
 
 A=sqrt [( A 3− A 1)^2+( A 2− A 1)^2]/2
 
 B=[A 0 +A 1 +A 2+ A 3]/4
 
 P =arctan [( A 3 −A 1)/( A 0− A 2)]
 
     While this invention has been particularly shown and described with references to preferred embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the scope of the invention encompassed by the appended claims.