an embodiment of the present invention will be described hereinafter with reference to the accompanying drawings . fig1 is a schematic diagram of an examination apparatus according to one embodiment of the present invention . fig2 is a plan view of a cap in helmet form . as shown in fig1 and 2 , a helmet - like cap 10 has a plurality of light launching fibers 11 - l to 11 - n and a plurality of light pickup fibers 12 - l to 12 - m that are attached to the cap in such a way that they surround uniformly an object to be measured , say a head 13 . these fibers are attached in such a way that their tips are located either in contact with the head 13 or in its vicinity when the cap 10 is put on the head 13 . the launching fibers 11 - l to 11 - n are connected at the other ends to associated pulse light sources , such as laser diodes , pl to pn . the pickup fibers 12 - l to 12 - m are held together in a bundle which is connected to a single photodetector 14 . light sources pl - pn are sequentially driven with a drive circuit 16 under the control of a computer 15 in such a periodic way that the operational timing of one light source is out of phase with that of another . the outputs of the photodetector 14 are read in synchronism with the drive timing of pulse light sources pl - pn and supplied to an integrator 18 through an amplifier 17 . the integrated outputs are subjected to analog - to - digital conversion in an a / d converter 19 and stored in the computer 15 as detection data to which assigned are addresses corresponding to the respective numbers of the pulse light sources pl - pn . with the constitution described above , the light sources pl - pn are sequentially driven as shown in fig3 to launch light beams into the head 13 through launching fibers 11 - l to 11 - n . for instance , a light source pi is driven to have light launched into the head 13 through a launching fiber 11 - i . as shown in fig4 the incident light is scattered and its direction becomes random as it goes deeper into the head and travels away from the incident site i . therefore , the absorption information to be obtained from the head 13 is chiefly determined by the absorption information in the vicinity of the incident site i and that in the vicinity of the output site , and the absorption information in the remaining whole part of the head 13 merely contributes as an averaged manner . in other words , optical outputs m ij and m im from respective output sites j and m are expressed as follows : p o : the intensity of light launched into the incident site i ; s i : the light transmittance in the vicinity of the incident site i ; i k : the light transmittance in the internal part of the head 13 ( e . g ., site k ); s j : the light transmittance in the vicinity of the output site j ; and s m : the light transmittance in the vicinity of the output site m . it is assumed in obtaining equation ( 1 ) that in the process of light travel to the output sites j and m the light transmittance in the internal part of the head 13 is averaged as expressed by σi k and the same value of light transmittance is picked up from any output site . the optical outputs m il to m im from all output sites are supplied to the single photodetector 14 through associated pickup fibers 12 - l to 12 - m and added together to produce : ## equ1 ## as one can see from equation ( 2 ), the light transmittance values of individual output sites are averaged by summing up outputs m il to m im and as a consequence , a parameter that is proportional to the transmittance s i at incident site i can be detected by the photodetector 14 . light from pulse light source p i is cyclically launched into the head 13 at the incident site i , and the transmittance s i at the incident site i that is detected with the photodetector 14 at each time of light launching is sent to the integrator 18 via the amplifier 17 to be integrated at prescribed times . the integrated transmittance s i is subjected to analog - to - digital conversion in the a / d converter 19 and stored in the computer 15 as detection data corresponding to the pulse light source p i . pulse light sources other than p i are sequentially driven and similar operations are performed to determine the light transmittance values of incident sites other than i as detection data that correspond to the respective driven pulse light sources . the detection data thus obtained are processed by predetermined procedures to determine the time - dependent change in the transmittance , that is , the light absorption at a plurality of local sites , that is , the incidence sites in the brain . in the prior art examination apparatus shown in fig5 a light launching fiber is located in one - to - one correspondence to a light pickup fiber and the light absorption on the straight line in the brain that connects these fibers is detected as the necessary information . this is not the case in the embodiment of the present invention described above , in which scattered light beams resulting from the launching of light at a selected incident site i is picked up simultaneously from all of the output sites and the outputs thus picked up are added together as mathematical processing . this offers the advantage that even if the intensity of incident light p o launched at the site i is not very high , the absorption of light at the local incident site i can be detected with high sensitivity . as a further advantage , any variation that might occur in the result of detection as a consequence of slight changes in the position or direction in which the light launching fibers 11 - l to 11 - n and the pickup fibers 12 - l to 12 - m are attached can be prevented effectively in the apparatus of the present invention . in the embodiment described above , scattered light beams from a plurality of output sites are sent to the single photodetector 14 where the individual outputs are added together . alternatively , a plurality of photodetectors that correspond to the respective pickup fibers 12 - l to 12 - m may be provided in such a way that the outputs of the photodetectors are added together in the computer 15 . the examination apparatus shown in fig1 may be modified in such a way that a plurality of light sources that emit light beams of different wavelengths are employed and that comparison is made between the intensities of outputs that correspond to the respective wavelengths . in this way , the differences in absorption spectra inherent in such substances as oxygen and glucose in the brain are utilized to achieve high - speed measurements of the spatial distribution and temporal change of a particular substance in the brain ( cerebral cortex ). the foregoing embodiment concerns examination of a certain abnormality in the brain . it should be noted that the apparatus of the present invention may be applied for diagnostic purposes to other organs of a human or animal body , as well as ordinary objects to be measured such as a piece of flesh . as described on the foregoing pages , the apparatus of the present invention is adapted to detect light absorption at a local site in an object of interest by performing mathematical processing on the intensities of scattered light beams picked up from a plurality of sites in the object . therefore , this apparatus enables light absorption at a local site in the object to be detected with high sensitivity even if the intensity of incident light is not very strong . as a further advantage , the apparatus provides highly precise results of detection without being greatly influenced by a deviation in the position or direction in which a fixture such as an optical fiber is attached to the object to be measured .
an examination apparatus for examining with transmission photometry an object of interest . the apparatus comprises : light launching means for successively launching an incidence light beam to the object at an incidence site ; and light pickup means for picking up , in synchronism with launching of the incidence light beam , light beams scattered in the object from a plurality of output sites as light intensity data , and performing mathematical processing on the light intensity data for every launching of said incidence light beam to obtain absorption data representing a light absorption quantity at the incidence site .