fig1 shows the head ( 10 ) of a scintillation camera including thirty - seven photomultiplier tubes or photomultipliers ( 11 ), a scintillation crystal ( 12 ), a collimator ( 13 ), and a housing structure ( 14 ) by which the components are held together in a unitary manner . the crystal ( 12 ) is a disc - shaped , planar scintillation crystal , such as thallium - activated sodium iodide , mounted in the housing ( 14 ) by means of suitable shoulders ( 15 ). such crystals are available in different sizes ; and a convenient size in wide use at present is 19 inches in diameter . the collimator ( 13 ) is interposed between the crystal ( 12 ) and the radiation field ( 16 ) and has a plurality of holes , the axes of which are perpendicular to the plane of the crystal , for the purpose of passing only those gamma rays which originate in the radiation field in a region directly beneath the hole . the photomultiplier tubes ( 11 ) are conventional in nature and , with a nineteen inch scintillation crystal , it is conventional to use thirty - seven photomultipliers , each of whose diameter is about 3 inches . the photomultipliers are perpendicular to the plane of the crystal , as shown in fig1 and the photocathodes of the photomultipliers are spaced from the upper surface of the crystal ( 12 ) in order to optimize the geometrical sensitivity of the photomultipliers . the spacing is chosen so that the geometric sensitivity is constant and has the largest value . the gamma ray ( 17 ) emanating from a point in the radiation field ( 16 ) and passing through a hole in the collimator ( 13 ) above the point will enter the crystal ( 12 ), and , depending on its energy and the thickness of the crystal , will interact therewith at some depth causing light event ( 18 ) to occur . such light event is seen by all photomultipliers . it is the function of the circuitry associated with the head ( 10 ) to compute the coordinates of the point in the radiation field causing the light event . before referring to this circuitry , it will be helpful to an understanding of the invention to define some general terms in connection with the array of photomultipliers shown in fig2 since the invention is applicable to other arrays . in general , the motif of any repeating pattern of photomultipliers , regardless of their number , must include at least seven photomultipliers . fig1 shows the schematic of the system and its functions . the output signals from the photomultiplier tubes are connected to the preamplifier circuits and a variable gain amplifier controller ( 20 ) that are provided for each photomultiplier and are controlled by the automatic gain control system ( 22 ). the output signals from each preamplifier is connected to the integrating adc ( 24 ) associated with each photomultiplier and the output of the adc ( 24 ) is transferred to the energy selection circuit ( 42 ). undesirable events are rejected by the energy selection circuit ( 42 ) and the desirable events are transferred to the relative position circuit ( 44 ). the event position from the energy selection circuit ( 42 ) is calculated by the relative position circuit ( 44 ) which passes the event relative position information to the energy calculation circuit which loops the information back to the relative position circuit ( 44 ) to improve the precision of the calculation . the output of the energy calculation circuit ( 46 ) is used by the absolute position calculation circuit ( 48 ) with the data from the relative position circuit ( 44 ) to produce the absolute xy location of the event to increment the appropriate memory location of the computer memory ( 50 ) which is subsequently displayed by the display ( 52 ). it is to be understood that the above description is not intended to limit the scope of the invention as defined in the appended claims , as other arrangements are possible . the position of the gamma event is determined by signals coming from multiple photomultiplier tubes . it is known in the art to calculate the location of the event using an algorithm , and then to apply a smoothing technique . in accordance with the present invention , the location of such events are calculated using more than one algorithm . thus , by using more than one method to calculate where the event occurred , i . e . use more than one algorithm to calculate the location of the event , then two positions are obtained from one gamma event . where the gamma event occurs on the crystal is a single point . at that point a light flash or scintillation occurs . since the light travels in many directions , the light is generally detected by more than one photomultiplier tube , and a number of photomultiplier tubes generate signals . the photomultiplier tube closest to the scintillation gets the most light and has the strongest outer signal . these photomultiplier tube output signals can be used by more than one algorithm to calculate the position of the event . note that when , for example , two algorithms are used , the number of events may have to be divided into two groups during certain quantative analyses , depending on their characteristics and relative efficiency of the two algorithms . if two algorithms are used , both generated images or image data can be written into the display matrix . the image statistics are thus improved because each algorithm uses different aspects and content of the data to derive the position of each event . two algorithms are used to calculate the location of each event prior to assigning data to one or more pixels . as long as the signals from the photomultiplier tubes are used by the algorithms in different ways , i . e . as long as the algorithms extract different data from the photomultiplier tube signals , then information is gained . one of the ways that the processing algorithms should differ is in the way that the algorithms deal with the noise content of the signals from the photomultiplier tubes . a given algorithm may perform better with respect to signals received from photomultiplier tubes corresponding to different areas of the scintillation crystal . certain algorithms may perform better within regions of the scintillation crystal or may perform better overall throughout the crystal . if more then one algorithm is used with a relatively low number of counts , image quality and perceived resolution is improved . this is the situation usually encountered when using scintillation cameras . if more than one algorithm is used with relatively high number of counts , image quality and perceived resolution will generally deteriorate compared with using one algorithm because one of the algorithms will be superior . for a certain number of counts image quality and perceived resolution will be the same for both methods . in one embodiment of the invention , two or more algorithms can be used until good statistics are obtained . after a time , for the pixels with good information , just the best algorithm may be used ; the data obtained by the second best algorithm may either be used or discarded . the present invention enables better images to be obtained in the same length of time . similarly , the invention enables similar images to be obtained in less time . while obtaining superior visual quality , less accuracy is lost compared with smoothing techniques . the resolution of the camera system r s is given by the formula : r s = ( w a  r a + w b  r b 2 ) 2 + r c 2 r a is the resolution of the first algorithm ; r b is the resolution of the second algorithm ; r c is the resolution of the collimator ; r s is the resolution of the system , w a and w b are weighting factors depending on event fractions and correlations of the algorithms . a gamma ray passing through collimator plate encounters the scintillation crystal which produces light . the crystal does not always produce exactly the same amount of light . the photomultiplier tubes convert light to an electrical signal , which is not always exactly the same . adjacent photomultiplier tubes may generate the following signals , for example : 90 / 800 / 110 , 100 / 805 / 100 , 110 / 795 / 95 . this sets the limit of the intrinsic resolution , i . e . the resolution of the crystal and photomultiplier tube assembly . the system resolution is the square root of the sum of the squares of the intrinsic resolution and the collimator resolution . the collimator resolution relates to the range of angles at which gamma rays can pass through the collimator , which depends on the apertures in the collimator . by using a second algorithm , for example , the system resolution may change from 7 . 74 mm ( with a single algorithm ) to 7 . 78 mm ( with two algorithms , given an r a = 3 . 3 ; r b = 3 . 5 ; r c = 7 ). for this relatively small reduction in resolution twice the number of counts are generated and the image is improved . examples of algorithms that can be used may be referred to as the centroid algorithms and the circle algorithm . however , this invention is not algorithm specific , and a number of suitable algorithms can be selected by one skilled in the art . it should also be noted that the algorithm are to be weighted . one algorithm might be superior in one area , another in a second area , and yet another in a third area . three algorithms could be differently weighted depending on where the light event occurs relative to the photomultiplier tubes . with the reference to fig1 the scintillation camera system comprises the digital camera 40 , energy rejection circuit 42 , relative position calculation 44 , energy calculation circuit 46 , absolute position calculation circuit 48 . in its preferred embodiment , the energy rejection calculation is digital and independent of the relative position calculation , which means that it can be performed , before , or in parallel with the relative position calculation . if it is performed after relative position calculation then it becomes position dependent . if the energy correction is performed before the relative position calculation , events which are outside the required energy window can be filtered earlier in the process , which improves the efficiency , and hence the speed of the positioning . in the preferred embodiment it is assumed that a tuning device exists , as descried in commonly assigned application entitled “ photodetector calibration in a scintillation camera using a single light source ” ser . no . 08 / 354 , 546 filed dec . 14 , 1994 or as described in u . s . pat . no . 5 , 237 , 173 but not limited to such devices , and that the tuning is done before the acquisition for the energy information and positional information . the assumption is that before acquisition , tuning is performed on the detector head , which will normalize the responses of all the light detectors . the assumption is that the detector head is digital , but not limited to being digital . ( this energy correction method can be used with any detector head on the market , which can improve the characteristics of the detector heads .) after or instead of those tuning devices , a new calibration is also performed based on a hole phantom image acquisition . outputs from the digital detector head as seen in fig1 are the following : 1 . the label or sequential number associated with the light detector in the detector head t , with the highest response , or in the close neighbourhood of the detector with the highest response . the light detector with the highest response or in close neighbourhood will be called the centre light detector . the assumption is that the absolute coordinates of each light detector is known in the detector head . 2 . the response signal of the central light detector of an n - tuple , defining the n - tuple as a group of the light detectors in the neighbourhood of the centre light detector . 3 . the responses of all light detectors in the neighbouring n - tuple of the central light detector , defining the n - tuple as a group of the light detectors in the neighbourhood of the centre light detector . energy rejection circuit 42 , produces a sum signal of said n - tuple of light detector signals including the signal of the central light detector , ( e . relative position calculation circuit 44 , produces x and y values for the particular n - tuple of the light detectors . output from the position calculation is the associated label or sequential number t of the centre light detector in the n - tuple . energy rejection circuit 42 let pass the events with an energy within the peak energy window . for those events , relative position calculation and energy calculation are weakly dependent . energy calculation may give back an energy evaluation to the relative position calculation , which improves the precision of the position . this loop may be done zero , one or more times . the energy calculation method consists of three well defined phases : first , acquisition of the energy information ; second producing the energy calculation tables ; third , applying the energy calculation 46 in real time acquisitions . acquisition of energy information : for each of many n - tuples with corresponding central light detector in the preferred embodiment , n by m histograms are recorded which cover the area of calculation of one n - tuple . each histogram consists of at least 256 bins . histograms are addressed by the highest n bits of the x position and the highest m bits of the y position . for each event with particular position x and y , particular histogram is chosen depending on position , and the counter of that histogram is increased , depending on the energy . the number of counts in each histogram has to be statistically sufficient . acquisition is done with the known energy , and without any structured phantoms or collimators . for producing the energy tables ; in the preferred embodiment , histogram should be filtered with a 3d filter for each n - tuple to smooth the response . it is known in the prior art that the response of the light detectors is higher in the centre , and it decreases towards the periphery of the light detector , and that the response is continuous . responses of the n - tuples are also smooth . for each n - tuple , the maximum response of each of the histograms is computed after filtering . for each histogram the factor should be computed so that the responses of all the light detectors are equal . for each n - tuple , a table of n by m factors is stored in the energy table . when applying the energy calculation 46 in real time , for each event , and depending on the central light detector of the n - tuple , address or label , and also depending on the first m bits of x coordinate and n bits of y coordinate , a particular address in the table is addressed . the computed energy , which is the sum of all the signals in the n - tuple of light detectors including the central light detector , is multiplied by the factor in the table . this produces the energy calculated value for that event . in the preferred embodiment , the relative position calculation method consists of four well defined phases . first , acquisition of the position information ; second , producing the position calculation tables for each light detector in the n - tuple and third applying the relative position calculation 46 in real time acquisitions . the fourth phase consists of adding the relative position of the n - tuple to the known geometric position of that n - tuple in the scintillation detector to create the absolute position 48 . assumption is that the detector head is capable of providing : 1 . associated label of the light detector in the detector head , with the highest response , or in the close neighbourhood . we will call the light detector with the highest response in one event the centre light detector . 2 . assumption is that the absolute coordinate of each light detector is known in the detector head . 3 . responses of all the light detectors in the neighbouring n - tuple , defining the n - tuple as a group of the light detectors , in the vicinity of the centre light detector . 4 . in preferred embodiment n - tuple is consisting of seven or more light detectors . 5 . definition of the event : event is one incidence of the gamma photon producing the scintillation effect in the crystal of the detector head . detector head outputs the label t of the centre light detector , and the values of the centre light detector and the intensity values of the light detectors in the neighbouring n - tuple . 6 . positional calculation is the translation of the events from the light detectors output to x , y and energy values . in the acquisition of position information ; acquisition consists of two parts . first , acquisition with the structured phantom in front of the scintillation camera ( similar to smith phantom ), and second , acquisition without phantom , the so - called flood acquisition . smith phantom is known in the art , and consists of a lead plate with lots of pinholes in a rectangular array . the preferred embodiment uses a hexagonal pattern of holes array , with cycle harmonized to the disposition of the light detectors within the detector head . a mechanism is added to the hexagonal lead plate such that , by manoeuvring one of three levers , the plate may be moved half a distance between two neighbouring holes , so that the resolution along the three axes defining the hexagonal pattern is doubled . acquisition is done with the radioactive isotope having a known energy . for each of many n - tuples with a corresponding central light detector , in the preferred embodiment , image data is acquired . the images are distorted depending on the geometric arrangement or constellation of the light detectors , the light detector and electronic channel properties , and the method of the position calculation . the position of each pinhole from the phantom is determined . the second acquisition of the flood is needed to determine that the uniformity criterion is satisfied . this means that the number of counts in each area in between the position determined by the image of the pinholes and bounded by the splines which connect all the positions of the pinholes in horizontal and vertical direction . the number of counts in each image has to be statistically sufficient to determine the position of the pinholes , or to check if the uniformity criterion is satisfied . to apply the relative position calculation 44 in real time ; for each event , and depending on the central light detector of the n - tuple , address or label , and also depending on each light detector signal of the n - tuple , a particular address in the table is addressed , which gives a distance from the scintillation to the light detector centre . this is done for each light detector , giving a n - tuple of said distances . position calculation is performed by solving the linear system of distances . this produces the position calculated value for that event . circuit 48 calculates the absolute position correction in real time . for each event , after calculation of the relative addresses and depending on the central light detector of the n - tuple , address or label , the position of the n - tuple is added to the relative position inside the n - tuple to form the absolute address . in the preferred embodiment , the position calculation method consist of three well defined phases . first , acquisition of the position information , with one radioactive isotope with lower energy ( approximately 100 kev ) and later with the radioactive isotopes in the medium ( 250 kev ) and high energy ranges ( 511 kev ). second , producing the expansion correction factors in table form or function with interpolation for the energies between the acquired energies . in the preferred embodiment , to improve the energy independent position correction method consist of three well defined phases . first , acquisition of the position information ; with one radioactive isotope with lower energy ( approximately 100 kev ), and later with the radioactive isotopes in the medium ( 250 kev ) and high energy ranges ( 511 kev ). second , producing the expansion correction factors in table form or function with interpolation for the energies between the acquired energies . in circuit 46 , the expansion correction factors are applied to the x , y values calculated in 44 , together with the sum of the light detectors values ( e given by the energy rejection circuit 42 . although the preferred embodiment illustrates a purely digital camera , it is to be understood that the above described methods can be easily adapted to operate when analog position calculation is used . the centroid algorithm is used to calculate the incident location of a gamma ray on the crystal of a gamma ray camera detector head . the primary inputs to the algorithm are the energy response signals of an array of photomultiplier tubes ( pmts ) that lie on the opposite side of the detector head crystal . pmts are small ( 3 ″ diameter ) cylindrical devices that detect light rays and output an electrical signal proportional to the intensity of the detected light . the further an event occurred from a pmt the lower its signal . the first step of the centroid algorithm is to calculate the centroid , or the intensity weighted averaged position of the event . this is calculated by summing the product of the position of each pmt and its energy response to an event , and dividing this sum by the sum of the intensities of each pmt . this can be expressed mathematically as where ( c x , c y ) is the centroid calculated position , ( pmt x , pmt y ) is the position of a pmt , pmt c is the energy response of this pmt , and the sum is over all the pmts . this first calculation is very approximate , and weights all events toward the centre of the pmt under which the event happened . as such , it is not clinically useful without further corrections . the first such correction is that for linearity . a linearity correction table is created by exposing a known configuration of a gamma emitting point sources and calculating the first step centroid for each gamma event . this results in an image of a point sources whose locations have been moved from their actual position due to the known tendency of the centroid method to skew events toward the centre of each pmt . the linearity correction table contains the correlations between the known (“ real ”) position of the gamma emitting source , and the position calculated by the centroid equation . applying the linearity correction table to the centroid image of the point sources will produce an image of the point sources in their “ real ” orientation . uniformity and energy corrections are subsequently applied to the image , but these are not particular to the centroid algorithm . linearity correction is also not exclusive to the centroid method , but is absolutely mandatory . analog cameras use linearity corrections as well , but the pre - linearity corrected images from analog cameras are much closer to the real image than with digital cameras employing the centroid method . another algorithm which may be used to calculate the incident location of a gamma ray on the crystal of the gamma camera detector is the “ circles ” algorithm . as in the centroid algorithm the inputs to the calculation are the measured energy responses of the photomultiplier tubes to the incident gamma ray . the principle of this algorithm is that the energy response of the photomultiplier tube to a fixed energy incident gamma ray is non - linearly , but monotonically related to the distance of the point of incidence from the centre of that tube via the so called “ roll - off ” curve , and consequently the energy may be used to determine a circle of possible incidence around each tube . the radius is given as a function of energy r = r ( e ). taking the radii and centres of the circles for several such tubes responding to a given gamma event , allows the calculation of a common point of intersection of the circles , localising the point of incidence absolutely . the incident point ( x , y ) of the gamma ray may be calculated after , suitable approximations , using the equation : with a similar form for y . the sum is over the photomultipliers responding to the event , z is a normalisation constant , r k is the radius from the centre of the k th pmt , and x k is the x position of the pmt . as for the centroid algorithm , the resulting point is approximate and requires corrections for non - linearities of the system . numerous modifications , variations and adaptations may be made to the particular embodiments of the invention described above without departing from the scope of the invention , which is defined in the claims .