Distribution type detector using scintillation fibers

A distribution type detector comprises scintillation fibers identical in length to each other, an optical delay fiber having a refractive index substantially identical to those of cores and claddings of the scintillation fibers, photosensitive elements, preamplifiers, constant fraction discriminators, a time-to-pulse height converter, an analog-to-digital converter, and a multichannel pulse-height analyzer. A position where a radiation falls on its corresponding scintillation fiber, is detected based on a difference between time intervals necessary for propagation of optical pulses produced in the corresponding scintillation fiber by the radiation. Thus, even if the length of each scintillation fiber is increased, position resolution can be kept high and a measuring circuit system can be simplified.

BACKGROUND OF THE INVENTION 
1. Field of the Invention 
The present invention relates to a distribution type detector using at 
least one scintillation fiber, which detects an incident position of 
radiation on the scintillation fiber or its intensity (a dose rate 
relative to the radiation). This distribution type detector can be used 
for detecting an optical pulse in a specific wavelength region. 
2. Description of the Related Art 
FIG. 38 is a view showing the configuration of a conventional distribution 
type detector using a scintillation fiber described in, for example, a 
collection of summarized articles issued by a next-generation radiation 
measuring system research institute, p.p. 44. In the drawing, reference 
numeral 101 indicates collimated radiation. Reference symbols 110a and 
110b respectively indicate optical pulses produced by fluorescence. 
Reference numeral 3201 indicates a scintillation fiber. Reference symbols 
104a and 104b respectively indicate photosensitive elements connected to 
the scintillation fiber 3201. Reference symbols 105a and 105b indicate 
preamplifiers respectively. Reference symbols 106a and 106b indicate 
constant fraction discriminators respectively. Reference numeral 3202 
indicates a signal delay circuit. Reference numeral 107 indicates a 
time-to-pulse height converter. Reference numeral 108 indicates an 
analog-to-digital converter. Reference numeral 109 indicates a 
multichannel pulse-height analyzer. 
The conventional distribution type detector using the scintillation fiber 
is constructed as described above. When one radiation 101 falls on the 
scintillation fiber 3201, fluorescence is produced within the 
scintillation fiber 3201 so that the optical pulses 110a and 110b are 
propagated toward both ends of the scintillation fiber 3201. Thereafter, 
the optical pulses 110a and 110b respectively enter into the 
photosensitive elements 104a and 104b where they are converted into 
electric pulse signals respectively. Next, the signals are respectively 
amplified by the preamplifiers 105a and 105b. The amplified signals are 
respectively waveform-shaped by the constant fraction discriminators 106a 
and 106b which are timing pulse generating circuits, followed by 
conversion into signals each indicative of the pulse time. The signal 
outputted from the constant fraction discriminator 106a passes through the 
signal delay circuit 3202 from which a signal is outputted so that the 
time to output the signal becomes later than that of the signal outputted 
from the constant fraction discriminator 106b. Thereafter, the two signals 
are inputted to the time-to-pulse height converter 107 with a given time 
difference between the two signals. The time-to-pulse height converter 107 
needs to determine the sequence of the pulses inputted to two input 
terminals thereof. Further, the required minimum value is included in the 
time difference between the firstly-input pulse and the subsequently-input 
pulse. When the time difference is less than or equal to the required 
minimum value, an accurate time difference cannot be measured. The signal 
delay circuit 3202 is provided to meet the above condition even if the 
radiation 101 falls on any position of the scintillation fiber 3201. Thus, 
a delay time of the signal delay circuit 3202 must be greater than the sum 
of a time interval necessary for the optical pulse to propagate over the 
entire length of the scintillation fiber and the above minimum time. If a 
difference between the length of a cable connected between circuits and 
the length of a cable connected between other circuits exists on the 
firstly-input pulse side and the subsequently-input pulse side, then the 
difference must be considered as a factor that leads up to the time 
difference. The time-to-pulse height converter 107 outputs an electric 
pulse having a pulse height proportional to the above time difference. The 
electric pulse is inputted to the multichannel pulse-height analyzer 109 
through the analog-to-digital converter 108. The scintillation fiber 3201 
is supplied not only with one radiation 101 alone but with several 
radiations 101. However, the incident positions of the radiations 101 on 
the scintillation fiber 3201 can be determined by discriminating between 
the pulse heights by the multichannel pulse-height analyzer 109. Further, 
a dose rate can be detected from the number of counts. 
The signal delay circuit is used under the above-described construction in 
the conventional distribution type detector using the scintillation fiber. 
Therefore, when the length of the scintillation fiber is increased, the 
delay time of the signal delay circuit must be made longer and hence the 
maximum time difference between the two signals inputted to the 
time-to-pulse height converter is affected by the length of the 
scintillation fiber and the delay time of the signal delay circuit. When 
the time difference becomes greater than a predetermined value, an input 
time-difference range of the time-to-pulse height converter must be 
raised. As a result, position resolution at the measurement of the 
incident position of the radiation on the scintillation fiber becomes 
poor. Since the measuring circuits are connected to both ends of the 
scintillation fiber on a two-system basis, an error is produced due to the 
difference in characteristics between the circuits, thereby causing a 
reduction in the accuracy of the detector. Further, the distribution type 
detector has problems in that, for example, the energy of an incident 
radiation cannot be identified, an energy characteristic relative to the 
radiation is poor due to a thin detecting unit, a measuring range is 
small, a dependence on the position of irradiation of the radiation 
exists, an increase in position resolution falls into difficulties due to 
a circuit characteristic, and a size reduction in the detector falls into 
difficulties due to the existence of two-systematic measuring circuits. 
SUMMARY OF THE INVENTION 
With the foregoing problems of prior art in view, it is therefore a first 
object of the present invention to eliminate, by using an optical delay 
fiber, the need for a signal delay circuit whose delay time is long and to 
improve position resolution. 
It is a second object of the present invention to reduce an error in 
measurement, which is produced due to the difference in characteristic 
depending on the systems, by uniting measuring circuits that needed two 
systems in the prior art into one system so as to simplify the united 
measuring circuit. 
It is a third object of the present invention to measure an energy spectrum 
of a radiation or a light pulse simultaneously with the incident position 
of the radiation or the light pulse and its intensity. 
Other objects of the present invention are to obtain a high sensitivity 
upon radiation detection, to increase a range of energy to be measured 
while a dependence of sensitivity on the energy remains low, reduce a 
dependence on the irradiated position of the radiation and to make it 
easier to calibrate the irradiated position of radiation or its intensity. 
In a distribution type detector using scintillation fibers, according to a 
first aspect of the present invention, a scintillation fiber is connected 
to an optical delay fiber. Ends of the fibers are respectively connected 
to photosensitive elements, followed by connection to preamplifiers, 
constant fraction discriminators, a time-to-pulse height converter, an 
analog-to-digital converter and a multichannel pulse-height analyzer. 
In a distribution type detector using scintillation fibers, according to a 
second aspect of the present invention, an optical delay fiber is inserted 
into and connected to a central portion of the scintillation fiber. 
Further, a time-to-pulse height converter does not draw a distinction 
between a terminal supplied with a firstly propagated signal and a 
terminal supplied with a subsequently propagated signal. 
In a distribution type detector using a scintillation fiber, according to a 
third aspect of the present invention, one end face of the scintillation 
fiber and an end face of an optical delay fiber connected to the other end 
of the scintillation fiber are connected to the same photosensitive 
element. The photosensitive element, a preamplifier and a constant 
fraction discriminator are respectively provided as single. Two optical 
signals propagated to both ends of the scintillation fiber are received by 
the single photosensitive element. Further, a measuring circuit is used 
which is capable of measuring the difference between time intervals 
necessary for the two optical signals to reach the photosensitive element. 
In a distribution type detector using a scintillation fiber, according to a 
fourth aspect of the present invention, a photosensitive element is 
connected to one end of the scintillation fiber. A reflector is attached 
to an end face of an optical delay fiber connected to the other end of the 
scintillation fiber. The photosensitive element, a preamplifier and a 
constant fraction discriminator are respectively provided as single. Two 
optical signals corresponding to an optical signal directly incident on 
the single photosensitive element and an optical signal reflected from the 
reflector enter into the single photosensitive element with a time 
difference made between the two optical signals. However, the distribution 
type detector utilizes a measuring circuit capable of measuring the time 
difference. 
In a distribution type detector using a scintillation fiber, according to a 
fifth aspect of the present invention, an analog-to-digital converter and 
a multichannel pulse-height analyzer are provided for measuring an energy 
spectrum of an optical pulse incident on the scintillation fiber based on 
branched output signals. The branched output signals are obtained from an 
output produced from at least one amplifier. 
In a distribution type detector using a scintillation fiber, according to a 
sixth aspect of the present invention, a loss of an optical signal, which 
is produced by its propagation distance, is compensated by software or 
hardware. 
In a distribution type detector using scintillation fibers, according to a 
seventh aspect of the present invention, a plurality of the scintillation 
fibers are shaped in the form of a bundle and the scintillation fiber 
bundle is constructed as a detecting unit. 
In a distribution type detector using scintillation fibers, according to an 
eighth aspect of the present invention, a fiber plate obtained by shaping 
a plurality of scintillation fibers in the form of a plate is constructed 
as a detecting unit. 
In a distribution type detector using scintillation fibers, according to a 
ninth aspect of the present invention, a plurality of fiber plates each 
obtained by shaping a plurality of the scintillation fibers in the form of 
a plate are disposed in parallel. 
In a distribution type detector using scintillation fibers, according to a 
tenth aspect of the present invention, each of fiber plates is produced by 
shaping a plurality of the scintillation fibers in the form of a plate. A 
combination obtained by stacking two fiber plates on one another so that 
fiber extending directions intersect at right angles, is provided as at 
least one pair of fiber plates. 
In a distribution type detector using a scintillation fiber, according to 
an eleventh aspect of the present invention, material capable of absorbing 
a low-energy radiation is disposed forward of the scintillation fiber used 
as a detecting unit. 
In a distribution type detector using a scintillation fiber, according to a 
twelfth aspect of the present invention, material capable of 
backscattering a high-energy radiation is disposed behind the 
scintillation fiber used as a detecting unit. 
In a distribution type detector using a scintillation fiber, according to a 
thirteenth aspect of the present invention, inorganic scintillator 
material which includes an element having a higher atomic number and is 
large in specific gravity, is used as a material for the scintillation 
fiber. 
In a distribution type detector using a scintillation fiber, according to a 
fourteenth aspect of the present invention, a light amplifier is provided 
on a path of the scintillation fiber or an optical delay fiber. 
In a distribution type detector using a scintillation fiber, according to a 
fifteenth aspect of the present invention, a fiber doped with a wavelength 
shifter material is provided on the input side of a light amplifier. 
In a distribution type detector using scintillation fibers, according to a 
sixteenth aspect of the present invention, radiation sources are 
respectively attached to the scintillation fibers. 
A distribution type detector using a scintillation fiber, according to a 
seventeenth aspect of the present invention includes a drive mechanism for 
driving the scintillation fiber used as a detecting unit in the direction 
orthogonal to that of the scintillation fiber. 
In a distribution type detector using a scintillation fiber, according to 
an eighteenth aspect of the present invention, a photosensitive element is 
embedded in an at least one end of the fiber by micromachining technology. 
According to the distribution type detector using the scintillation fibers, 
of the first aspect of the present invention, the scintillation fiber is 
connected to the optical delay fiber. The ends of the fibers are 
respectively connected with the photosensitive elements, followed by 
connection with the preamplifiers, the constant fraction discriminators, 
the time-to-pulse height converter, the analog-to-digital converter and 
the multichannel pulse-height analyzer. Thus, the use of the optical delay 
fiber enables an improvement in position resolution, simplification of a 
measuring circuit system, integration of measuring circuits into one 
system, etc. 
According to the distribution type detector using the scintillation fibers, 
of the second aspect of the present invention, the optical delay fiber is 
inserted into and connected to the central portion of the scintillation 
fiber so that the difference between the time intervals necessary for the 
two signals inputted to the time-to-pulse height converter to reach the 
time-to-pulse height converter becomes greater than a predetermined value. 
The distribution type detector is provided with the time-to-pulse height 
converter which does not draw a distinction between the terminal supplied 
with the firstly propagated signal and the terminal supplied with the 
subsequently propagated signal. This construction eliminates the need for 
the change of the length of the optical delay fiber to another even if 
each scintillation fiber increases in length. Thus, the maximum time 
difference inputted to the time-to-pulse height converter is affected by 
the length of each scintillation fiber alone. The value of its length 
becomes (n+t)/(2n+t) times the value employed in the prior art, where n 
represents a time necessary for each optical pulse to propagate over the 
entire length of each scintillation fiber and t indicates a required 
minimum time difference between the firstly input pulse and the 
subsequently input pulse, into the time-to-pulse height converter. 
Hereinafter, the required minimum time difference is referred to as an 
unmeasurable time. The length of the optical delay fiber may be set so 
that the propagation time of light becomes longer than the dead time 
produced in the time-to-pulse height converter. The value of the length 
thereof is equal to t/(n+t) times the value employed in the prior art. In 
doing so, the rising edge of the signal pulse can be restrained from 
expanding, thereby making it possible to improve position resolution as 
compared with the prior art. 
According to the distribution type detector using the scintillation fiber, 
of the third aspect of the present invention, the one end face of the 
scintillation fiber and the end face of the optical delay fiber connected 
to the other end of the scintillation fiber are connected to the same 
photosensitive element. The photosensitive element, the preamplifier and 
the constant fraction discriminator are respectively provided as single. 
The two optical signals propagated to both ends of the scintillation fiber 
are received by the single photosensitive element. Further, the measuring 
circuit is used which is capable of measuring the difference between the 
time intervals necessary for the two optical signals incident on the 
single photosensitive element to reach the photosensitive element. Due to 
this construction, measuring circuits are integrated into one system. An 
error produced due to the difference in characteristic between measuring 
instruments can be eliminated and the detector can be reduced in size. 
According to the distribution type detector using the scintillation fiber, 
of the fourth aspect of the present invention, the photosensitive element 
is connected to the one end face of the scintillation fiber. The reflector 
is attached to the end face of the optical delay fiber connected to the 
other end of the scintillation fiber. The photosensitive element, the 
preamplifier and the constant fraction discriminator are respectively 
provided as single. The two optical signals corresponding to the optical 
signal directly incident on the single photosensitive element and the 
optical signal reflected from the reflector enter into the single 
photosensitive element with the time difference made between the two 
optical signals. However, the distribution type detector utilizes the 
measuring circuit capable of measuring the time difference. Due to this 
construction, one-systematic measuring circuit can be set up and an error 
produced due to the difference in characteristic between measuring 
instruments can be eliminated. 
According to the distribution type detector using the scintillation fiber, 
of the fifth aspect of the present invention, a preamplifier is provided 
which is capable of outputting two signals therefrom in response to a 
single signal inputted thereto. One of the two outputs is used for 
measurement of a position of an incident radiation or an incident optical 
pulse in a given wavelength region, whereas the other of the two outputs 
is used for measurement of the distribution of energy. Due to this 
construction, the distribution of energy can be also measured as well as 
the incident position of the radiation or the optical pulse. 
According to the distribution type detector using the scintillation fiber, 
of the sixth aspect of the present invention, the loss of the optical 
signal, which is produced by its propagation distance, is compensated by 
software or hardware. Thus, the difference between distribution results on 
energy at respective incident positions of a radiation to be measured or a 
light pulse to be measured, in a given wavelength region can be reduced. 
According to the distribution type detector using the scintillation fibers, 
of the seventh aspect of the present invention, a plurality of the 
scintillation fibers are shaped in the form of the bundle and the 
scintillation fiber bundle is constructed as the detecting unit. Due to 
this construction, the probability that an incident radiation or optical 
pulse in a given wavelength region will react within each scintillation 
fiber by fluorescence, can be raised and the quantity of light incident on 
each photosensitive element can be also increased. 
According to the distribution type detector using the scintillation fibers, 
of the eighth aspect of the present invention, the fiber plate obtained by 
shaping the plurality of the scintillation fibers in the form of the plate 
is constructed as the detecting unit. Thus, a position of an incident 
radiation or an incident position of an optical pulse in a given 
wavelength region can be measured on a two-dimensional basis. 
According to the distribution type detector using the scintillation fiber, 
of the ninth aspect of the present invention, since the plurality of fiber 
plates are disposed in parallel, the distribution type detector can 
measure a track of a radiation or a light pulse in a wavelength region. 
According to the distribution type detector using the scintillation fiber, 
of the tenth aspect of the present invention, since the fiber plates are 
stacked on one another so that the fiber extending directions intersect at 
right angles, a reduced number of photosensitive elements can measure each 
incident position of a radiation or an optical pulse on a two-dimensional 
basis. 
According to the distribution type detector using the scintillation fiber, 
of the eleventh aspect of the present invention, the material capable of 
absorbing the low-energy radiation is disposed forward of the 
scintillation fiber used as the detecting unit. Due to this construction, 
the difference between the probability that the low-energy radiation will 
react within the scintillation fiber and the probability that a 
high-energy radiation will react within the scintillation fiber, can be 
reduced and the sensitivity of a dose rate with respect to the energy of 
the radiation can be flattened. 
According to the distribution type detector using the scintillation fiber, 
of the twelfth aspect of the present invention, the material capable of 
backscattering the high-energy radiation is disposed behind the 
scintillation fiber used as the detecting unit. Due to this construction, 
the difference between the probability that a low-energy radiation will 
react within the scintillation fiber and the probability that the 
high-energy radiation will react within the scintillation fiber, can be 
reduced and the sensitivity of a dose rate with respect to the energy of 
the radiation can be flattened. 
According to the distribution type detector using the scintillation fiber, 
of the thirteenth aspect of the present invention, the inorganic 
scintillator material is used as the material for the scintillation fiber. 
Due to this construction, the probability that a high-energy radiation 
will react within the scintillation fiber, can be raised. 
According to the distribution type detector using the scintillation fiber, 
of the fourteenth aspect of the present invention, the light amplifier is 
provided on the path of the scintillation fiber or the optical delay 
fiber. Owing to this construction, a transmission loss of light propagated 
within the fiber can be supplemented and hence a measuring range can be 
expanded. 
According to the distribution type detector using the scintillation fiber, 
of the fifteenth aspect of the present invention, the fiber doped with the 
wavelength shifter material is provided between the scintillation fiber 
and the light amplifier. Due to this construction, the wavelength of each 
optical pulse produced by fluorescence within the scintillation fiber can 
be shifted to an amplifierable wavelength band of the light amplifier by 
the wavelength shifter even if the wavelength of each optical pulse is 
shorter than the amplifierable wavelength band thereof. As a result, a 
transmission loss of light propagated within the fiber can be supplemented 
and hence a measuring range can be expanded. 
According to the distribution type detector using the scintillation fibers, 
of the sixteenth aspect of the present invention, the radiation sources 
are respectively attached to the scintillation fibers. By providing the 
radiation sources used as standards for position measurement in this way, 
position accuracy with respect to the measurement of a position where a 
radiation or an optical pulse in a given wavelength region enters into its 
corresponding scintillation fiber, can be improved. 
According to the distribution type detector using the scintillation fiber, 
of the seventeenth aspect of the present invention, the scintillation 
fiber, which serves as the detecting unit, is set to a movable type. By 
doing so, a measuring range can be expanded and a spatial distribution of 
a radiation to be measured or an optical pulse in a given wavelength 
region can be measured. 
According to the distribution type detector using the scintillation fiber, 
of the eighteenth aspect of the present invention, the photosensitive 
element is embedded in the end of the fiber by micromachining technology. 
Due to this construction, the detector can be reduced in size. Further, a 
loss of light transmitted within the fiber, which is produced at the end 
face of the fiber, can be reduced, thereby making it possible to expand a 
measuring range. 
The above and further objects and novel features of the present invention 
will more fully appear from the following detailed description when the 
same is read in connection with the accompanying drawings. It is to be 
expressly understood, however, that the drawings are for purpose of 
illustration only and are not intended as a definition of the limits of 
the invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
Preferred embodiments of the present invention will hereinafter be 
described in detail with reference to the accompanying drawings. 
First Embodiment! 
FIG. 1 is a configurational view showing a distribution type detector 
according to a first embodiment of the present invention. In FIG. 1, 
reference numeral 101 indicates radiation to be measured, i.e., an optical 
pulse in a specific wavelength region. Reference numerals 102a and 102b 
respectively indicate scintillation fibers identical in length to one 
another. Reference numeral 103 indicates an optical delay fiber having a 
refractive index substantially identical to that of each core of the 
scintillation fibers 102a and 102b. The scintillation fibers 102a and 102b 
emit or give fluorescence in response to a radiation or light in a 
specific wavelength region, such as ultraviolet radiation or rays. 
However, as the optical delay fiber, one that does not produce 
fluorescence is employed. Reference numerals 104a and 104b indicate 
photosensitive elements respectively and reference numerals 105a and 105b 
indicate preamplifiers respectively. Reference numerals 105a and 106b 
indicate constant fraction discriminators respectively. Reference numeral 
107 indicates a time-to-pulse height converter. In response to one 
radiation or an optical pulse in a given wavelength region, two timing 
pulses are respectively inputted to two input terminals of the 
time-to-pulse height converter 107. However, different from the 
conventional one, the time-to-pulse height converter 107 is capable of 
measuring a time difference regardless of which one of the pulses is 
firstly inputted. Reference numeral 108 indicates an analog-to-digital 
converter. Reference numeral 109 indicates a multichannel pulse-height 
analyzer. Designated at numerals 110a and 110b are respectively optical 
pulses generated by fluorescence. 
The operation of the distribution type detector shown in FIG. 1 will now be 
described. 
When the radiation or light pulse 101 in the specific wavelength region 
falls on or strikes the scintillation fiber 102a or 102b, fluorescence is 
produced therein so that the generated optical pulses 110a and 110b are 
propagated toward both ends of the scintillation fiber 102a or 102b. At 
this time, no fluorescence is produced even if the radiation or light 
pulse 101 in the given wavelength region is launched into the optical 
delay fiber 103. After the optical pulses 110a and 110b have been 
propagated through the scintillation fibers 102a and 102b respectively, 
they enter into their corresponding photosensitive elements 104a and 104b. 
The photosensitive elements 104a and 104b respectively convert the optical 
pulses 110a and 110b into electric signals. Thereafter, the converted 
electric signals are successively amplified by the preamplifiers 105a and 
105b. Further, the constant fraction discriminators 106a and 106b shape 
the waveforms of the amplified electric signals into waveforms suitable 
for timing pulses respectively. The time-to-pulse height converter 107 
outputs an electric pulse having a wave or pulse height proportional to 
the time difference between the two signals inputted to the time-to-pulse 
height converter 107. Thereafter, the analog-to-digital converter 108 
converts a crest value of the analog signal into digital form, followed by 
inputting to the multichannel pulse-height analyzer 109 where the signal 
is counted at each value thereof. 
To the time-to-pulse height converter 107, the two timing pulses are 
inputted in response to the radiation or optical pulse in the given 
wavelength region. These two timing pulses are inputted thereto with a 
given time difference produced between them at all times by the optical 
delay fiber 103. By adjusting the length of the optical delay fiber 103, 
the minimum value of the time difference between the two timing pulses 
inputted to the time-to-pulse height converter 107 can be adjusted. When 
the time difference between the firstly input signal and the subsequently 
input signal is less than or equal to a predetermined value, the 
time-to-pulse height converter 107 produces an error in measurement. 
However, this error can be eliminated by setting the length of the optical 
delay fiber 103 to a predetermined value or more. When the length of each 
scintillation fiber is made longer, the maximum time difference between 
the two timing pulses inputted to the time-to-pulse height converter 107 
becomes greater. It is however unnecessary to increase the length of the 
optical delay fiber 103 by using the aforementioned optical delay fiber 
103 as an alternative to a conventional signal delay circuit and using the 
aforementioned time-to-pulse height converter 107. Namely, the optical 
delay fiber 103 may be provided by a length equivalent to the 
aforementioned unmeasurable time period at a position of the time-to-pulse 
height converter 107, which corresponds to the aforementioned unmeasurable 
time period. It is unnecessary to set the length of the optical delay 
fiber 103 to a delay time longer than a time during which an optical pulse 
is propagated over the entire length of a scintillation fiber as in the 
case of the conventional signal delay circuit 3202. Namely, the length of 
the optical delay fiber 103 may be set in such a way that the propagation 
time of light becomes longer than the aforementioned unmeasurable time, in 
the time-to-pulse height converter. The value of the length thereof is 
equal to t/(n+t) (where n: time during which an optical pulse is 
propagated over the entire length of each scintillation fiber and t: 
aforementioned unmeasurable time in the time-to-pulse height converter) 
times the value employed in the prior art. In doing so, the rising edge of 
the signal pulse can be restrained from expanding, thereby making it 
possible to improve position resolution as compared with the prior art. 
At this time, the maximum time difference between the two timing pulses 
becomes (n+t)/(2n+t) times the conventional one. Thus, a time difference 
range of the time-to-pulse height converter can be kept low so that the 
position resolution for position detection can be raised as compared with 
the prior art. 
Since the signal delay circuit can be omitted, a measurement system can be 
simplified. Further, since the optical delay fiber is superior in 
high-frequency characteristic to an electrical signal delay circuit, the 
distortion of a waveform to be transmitted is lowered and a change of the 
delay time due to a change in temperature is reduced. It is therefore 
possible to improve a position detecting precision. 
FIG. 2 shows the way of laying out the optical delay fiber and the 
scintillation fibers both employed in the first embodiment. 
Since the optical delay fiber 103 is provided at the position corresponding 
to the unmeasurable time period of the time-to-pulse height converter 107 
as described above, the region of the optical delay fiber 103 is an 
unmeasurable region if the optical delay fiber 103 is linearly disposed as 
shown in FIG. 1. To avoid this, the optical delay fiber 103 may be 
disposed in such a way that a space is not provided between the 
scintillation fibers 102a and 102b as shown in FIG. 2. As the fibers, 
scintillation fibers shielded against the radiation or light may be used. 
Second Embodiment! 
FIG. 3 is a configurational view showing a distribution type detector 
according to a second embodiment. There are shown in FIG. 3, a 
scintillation fiber 301, an optical delay fiber 302, a photosensitive 
element 303 for receiving therein two optical pulses generated based on 
one radiation or an optical pulse in a given wavelength region, a 
preamplifier 304, a constant fraction discriminator 305, a signal 
discriminating circuit 306 for causing two timing pulses outputted from 
the constant fraction discriminator 305 to branch to two and for 
outputting the firstly input pulse and the subsequently input pulse from 
terminals different from one another, and a time-to-pulse height converter 
307. 
The operation of the distribution type detector shown in FIG. 3 will now be 
described. 
When one radiation or an optical pulse 101 in a given wavelength region 
falls upon the scintillation fiber 301, fluorescence is produced within 
the scintillation fiber 301 to generate optical pulses 110a and 110b. The 
optical pulse 110a of the two pulses is propagated through the optical 
delay fiber 302 so as to launch into the photosensitive element 303. On 
the other hand, the remaining optical pulse 110b is directly launched into 
the photosensitive element 303. When a time interval, during which the 
optical pulses are propagated over the entire length of the optical delay 
fiber 302, is longer than a time interval during which the optical pulses 
are propagated over the entire length of the scintillation fiber 301, the 
optical pulse 110b is firstly introduced into the photosensitive element 
303. An error in measurement, which is produced due to the fact that the 
time difference between the input two timing pulses is extremely small, 
exists in the time-to-pulse height converter 307 provided at the 
subsequent stage. If, however, the difference between the propagation time 
intervals is longer than the minimum time difference during which this 
error is not produced, then this error is prevented from being produced. 
Thereafter, the two optical pulses 110a and 110b are converted into 
electric pulses by the photosensitive element 303, which are in turn 
transmitted through the preamplifier 304 and the constant fraction 
discriminator 305, followed by inputting to the signal discriminating 
circuit 306. The signal discriminating circuit 306 causes the firstly 
input signal and the subsequently input signal to branch to the two and 
outputs them from the terminals different from each other. Thereafter, the 
time-to-pulse height converter 307 outputs an electric pulse having a wave 
or pulse height proportional to the time difference between the two 
signals inputted to the time-to-pulse height converter 307. Further, an 
analog-to-digital converter 108 converts a crest value of the analog 
signal into digital form, followed by inputting to a multichannel 
pulse-height analyzer 109 where the signal is counted at each value 
thereof. 
In the present embodiment as described above, since the measuring circuit 
system can be set as a single system unlike the prior art, an error 
produced due to the difference in characteristic between measuring 
instruments can be eliminated. Furthermore, a detector can be reduced in 
size. 
Incidentally, a scintillation fiber shielded against radiations or light 
may be used as the optical delay fiber. 
Third Embodiment! 
In this embodiment, a circuit of such a type that after the first signal 
has been inputted thereto, the second signal is allowed to pass through a 
path different from that used for the first signal by a switching device 
and after the second signal has been inputted thereto, the corresponding 
circuit is reset to its original condition, is constructed, as an 
alternative to the signal discriminating circuit 306 employed in the 
second embodiment. At this time, the difference in input time between the 
two input signals is set so as to remain unchanged. 
Thus, the signal discriminating circuit 306 causes the two signals inputted 
from the single terminal to branch to two and is able to output them to 
terminals different from each other. 
One example of a signal discriminating circuit used for this purpose will 
be shown in FIG. 4A. FIG. 4B illustrates signal waveforms obtained at 
respective parts of the signal discriminating circuit shown in FIG. 4A. 
Referring to FIGS. 4A and 4B, since an output C produced from a monostable 
circuit 3062 and a bar C represented by placing a bar over the output C 
are respectively LOW and HIGH in its initial state, a gate circuit 3063 is 
opened and a gate circuit 3064 is closed. Thus, a firstly input signal P1 
of two input signals P1 and P2 is outputted from the gate circuit 3063. In 
response to the input signal P1, a monostable circuit 3061 generates an 
output pulse B longer in time than the input signal P1 therefrom and 
inverts the monostable circuit 3062 at the trailing end of the output 
pulse B. Thereafter, the gate circuit 3063 is closed and the gate circuit 
3064 is opened during a period in which the output C and the bar C 
produced from the monostable circuit 3062 are being inverted. Accordingly, 
the input signal P2 is outputted from the gate circuit 3064. Incidentally, 
AND circuits may be used as an alternative to the gate circuits 3063 and 
3064. 
Fourth Embodiment! 
In the signal discriminating circuit 306 employed in the second embodiment, 
a first pulse signal and a second pulse signal are allowed to pass through 
paths different from each other by pulse-height discriminating circuits, 
using a difference in crest value between the first and second pulse 
signals. At this time, the difference in input time between the two input 
signals is set so as to remain unchanged. 
Thus, the signal discriminating circuit 306 causes the two signals inputted 
from the single terminal to branch to two and is able to output them to 
terminals different from each other. 
One example of a signal discriminating circuit used for this purpose will 
be shown in FIG. 5A. FIG. 5B shows signal waveforms obtained at respective 
parts of the signal discriminating circuit. Referring to FIGS. 5A and 5B, 
a single channel pulse-height analyzer (SCA-H) 3065 generates an output B 
based on P1 of input pulses P1 and P2 in response to a pulse having a 
crest-value range V.sub.H. A single channel pulse-height analyzer (SCA-L) 
3066 generates an output C based on the input signal P2 in response to a 
pulse of a crest-value range V.sub.L. Since the pulses B and C are used 
for pulse discrimination but the signals outputted from the single channel 
pulse-height analyzers are generated with being delayed with respect to 
the input signal, an output D produced from a constant fraction 
discriminator 305 is delayed by a delay circuit 3067 so as to be timed to 
the above delays, thereby producing an output E. An AND circuit 3068 
selects the P1 (delay) timed with the SCA-H 3065 and generates an output 
signal F therefrom based on the P1. An AND circuit 3069 selects the P2 
(delay) and generates an output signal G therefrom based on the P2. Thus, 
the AND circuit 3068 outputs the timing signal corresponding to the input 
signal having the crest-value range V.sub.H, whereas the AND circuit 3069 
outputs the timing signal corresponding to the input signal having the 
crest-value range V.sub.L. 
Fifth Embodiment! 
FIG. 6A shows another example of the signal discriminating circuit 306 
employed in the second embodiment. FIG. 6B illustrates signal waveforms 
obtained at individual parts of the signal discriminating circuit 306. A 
signal discriminating circuit 356 employed in the present embodiment 
doubles the functions of the constant fraction discriminator 305 and the 
signal discriminating circuit 306 employed in the second embodiment. Since 
two pulses for measuring a time difference must be separated from one 
another in terms of time when the two pulses pass through the same path, 
the time difference between$.sup.- the pulses, which is close to within a 
respective pulse width, cannot be measured. The signal discriminating 
circuit employed in the present embodiment can overcome such inconvenience 
and generates output pulses corresponding to individual times of 
overlapping two pulses at separate output terminals. A delay line shaping 
circuit 3561 shapes a signal having a stepped waveform, which is outputted 
from a preamplifier, into a rectangular wave. When the two input signals 
P1 and P2 are close to each other, the delay line shaping circuit 3561 
outputs a rectangular wave B obtained by overlaying the signals on one 
another. Signals outputted from a delay circuit 3562 and a 1/4 attenuator 
3563 are supplied to a subtracter 3565 wher$Na timing signal corresponding 
to the first pulse P1 is generated. On the other hand, a 3/4 attenuator 
3564 supplies an output signal to a subtracter 3566 from which a timing 
signal corresponding to the second pulse P2 is generated. Thus, even when 
the time difference between the two input signals is smaller than each 
pulse width, the signal discriminating circuit 356 can output the timing 
signals from the two different output terminals. If a delay time of the 
delay circuit 3562 is selected to half the width of the pulse outputted 
from the delay line shaping circuit 3561, then a measurable 
time-difference range can be maximized. 
Six Embodiment! 
FIG. 7 is a configurational view showing a main part of a distribution type 
detector according to a sixth embodiment of the present invention. In FIG. 
7, reference numerals 401, 402, 403 and 404 indicate a scintillation 
fiber, an optical delay fiber, a reflector and a photosensitive element 
respectively. 
The operation of the present embodiment will now be described. 
When one radiation or an optical pulse 101 in a given wavelength region 
falls on the scintillation fiber 401, fluorescence is produced within the 
scintillation fiber 401 to generate optical pulses 110a and 110b. The 
optical pulse 110a of the two is propagated through the optical delay 
fiber 402 and is reflected from the reflector 403 provided at the end of 
the optical delay fiber 402 so as to enter into the photosensitive element 
404. On the other hand, the remaining optical pulse 110b directly enters 
the photosensitive element 404. An error in measurement, which is produced 
due to the fact that the time difference between the input two timing 
pulses is extremely small, exists in a time-to-pulse height converter 
provided at the subsequent stage. If, however, the time difference between 
the two optical pulses inputted to the photosensitive element 404 is 
greater than the minimum time difference during which this error is not 
produced, then this error is prevented from being produced. To prevent the 
occurrence of the error, the length of the optical delay fiber 402 is set 
to such a length that a time interval required to move the optical pulse 
forward and backward alternately becomes longer than the minimum time 
during which no error is produced. Measuring circuits provided subsequent 
to the photosensitive element 404 may be similar to those employed in the 
second embodiment. 
When the length of the scintillation fiber 401 is made long under the above 
construction, the maximum time difference between the two optical pulses 
110a and 110b inputted to the photosensitive element 404 becomes large. 
However, the use of the above-described optical delay fiber as an 
alternative to the conventional signal delay circuit makes it unnecessary 
to increase the length of the optical delay fiber 402. Namely, it is 
unnecessary to increase a delay time. Thus, a time-difference range of the 
time-to-pulse height converter can be kept low in a manner similar to the 
first embodiment, thereby making it possible to improve position 
resolution for position detection as compared with the prior art. 
In the present embodiment, since a measuring circuit system can be set as a 
single system unlike the prior art, an error produced due to the 
difference in characteristic between measuring instruments can be 
eliminated. Furthermore, a detector can be reduced in size. 
The reflector 403 employed in the six embodiment may be constructed such 
that an end face of the optical delay fiber 402 is flatly ground and a 
flat reflective material is stuck to the end face thereof with silicon 
adhesive or the like. 
Thus, the loss of light incurred at reflecting surface of the reflector 403 
can be reduced. 
A hole may be defined in the leading end of a core of the optical delay 
fiber 402 by etching so that the reflector 403 employed in the sixth 
embodiment is embedded therein. 
Thus, the loss of light incurred at the reflecting surface of the reflector 
403 can be reduced in the same manner as described above. 
Seventh Embodiment! 
FIG. 8 is a configurational view illustrating a distribution type detector 
according to seventh embodiment of the present invention and is also a 
view showing the structure of a device for measuring an energy spectrum of 
a radiation or an optical pulse in a given wavelength region as well as a 
position where the radiation or the optical pulse in the given wavelength 
region employed in the first embodiment is entered. In FIG. 8, reference 
numeral 501 indicates a preamplifier for outputting two signals in 
response to a single input signal. Reference numeral 502 indicates an 
amplifier. Reference numeral 503 indicates an analog-to-digital converter. 
Reference numeral 504 indicates a multichannel pulse-height analyzer. 
The operation of the distribution type detector shown in FIG. 8 will now be 
described. 
An electric pulse outputted from a photosensitive element 104b is inputted 
to the preamplifier 501 from which the two signals are outputted. One of 
the two signals is supplied to a constant fraction discriminator 106b. The 
subsequent operation is performed in a manner similar to the first 
embodiment. The other of the two signals is inputted to the amplifier 502 
where the signal is further amplified. The amplified signal is inputted to 
the analog-to-digital converter 503, followed by inputting to the 
multichannel pulse-height analyzer 504. 
A crest value of a pulse counted by the multichannel pulse-height analyzer 
504 is substantially proportional to the energy of a radiation or an 
optical pulse 101 in a given wavelength region, which enters into each 
scintillation fiber. Thus, the energy spectrum of the radiation or the 
optical pulse 101 in the given wavelength region, which has entered each 
scintillation fiber, can be measured by discriminating between the input 
signals according to the crest value by the multichannel pulse-height 
analyzer 504. In the present embodiment, the energy signal is taken out 
from the one side of the preamplifier alone. Alternatively, the energy 
signal may be taken out from the preamplifier 105a side so as to measure 
an energy spectrum based on the sum of both signals. In doing so, an 
advantage can be brought about which is capable of reducing a dependence 
on the incident position of a radiation or an optical pulse in a given 
wavelength region. 
As an alternative to an analog-to-digital converter 108 and the 
analog-to-digital converter 503 both employed in the seventh embodiment, a 
multiparameter type analog-to-digital converter may be used so as to 
supplement the functions of these two analog-to-digital converters in the 
form of one function. Such a construction enables the provision of a 
single multichannel pulse-height analyzer so that the same effects as 
those obtained in the seventh embodiment can be achieved and the measuring 
circuit can be made compact in size. 
Eighth Embodiment! 
FIG. 9 is a configurational view showing a distribution type detector 
according to an eighth embodiment of the present invention and is also a 
view showing the structure of a device for measuring an energy spectrum of 
a radiation or an optical pulse in a given wavelength region as well as a 
position where the radiation or the optical pulse in the given wavelength 
region employed in the first embodiment is entered. Upon measurement of 
the distribution of energy, this device can also compensate for dependence 
on the position where the radiation or the optical pulse in the given 
wavelength region is entered, on a hardware basis. In FIG. 9, reference 
numeral 601 indicates an arithmetic circuit for compensating for the 
dependence on the above incident position. This arithmetic circuit 
includes a coincidence circuit. Reference numeral 602 indicates an 
analog-to-digital converter and reference numeral 603 indicates a 
multichannel pulse-height analyzer. 
The operation of the distribution type detector shown in FIG. 9 will now be 
described. 
An electric pulse outputted from a photosensitive element 104b is inputted 
to a preamplifier 501 from which two signals are outputted. One of the two 
signals is inputted to a constant fraction discriminator 106b. The 
subsequent operation is performed in a manner similar to the first 
embodiment. The other of the two signals is inputted to an amplifier 502 
where the signal is further amplified. When, however, scintillation fibers 
102a and 102b or an optical delay fiber 103 is so long in length, the 
crest value of the signal greatly varies depending on at which position of 
the scintillation fiber 102a or 102b the radiation or the optical pulse in 
the given wavelength region enters, even if the energy of the radiation or 
the optical pulse is kept constant. This is because the optical pulses 
generated by fluorescence suffer losses when propagated through the 
scintillation fibers and the optical delay fiber. To compensate for the 
losses, the degree or level of a loss relative to a distance over which 
each optical pulse produced by fluorescence is propagated within its 
corresponding fiber, is measured in advance and a distance to be 
propagated through the corresponding fiber is measured according to the 
incident position of the radiation or the optical pulse in the given 
wavelength region upon actual measurement. Thereafter, the crest value of 
each propagated optical pulse may be compensated based on the value of the 
propagated distance. The arithmetic circuit 601 is provided to compensate 
for the crest value thereof. The arithmetic circuit 601 is supplied with a 
signal outputted from an amplifier 502 and a signal outputted from a 
time-to-pulse height converter 107. The coincidence circuit included in 
the arithmetic circuit 601 starts arithmetic computations after the two 
signals have been inputted thereto. Namely, the arithmetic circuit 601 
calculates the propagated distance of the optical pulse based on the 
signal outputted from the time-to-pulse height converter 107 and 
compensates for the crest value of the signal outputted from the amplifier 
502. Further, the arithmetic circuit 601 outputs the compensated signal to 
the analog-to-digital converter 602. After the signal has been supplied to 
the analog-to-digital converter 602, it is inputted to the multichannel 
pulse-height analyzer 603. 
The crest value of the pulse, which is counted by the multichannel 
pulse-height analyzer 603, is substantially proportional to the energy of 
a radiation or an optical pulse 101 in a given wavelength region, which 
falls on each scintillation fiber. Thus, an energy spectrum of the 
radiation or the optical pulse 101 in the given wavelength region, which 
has entered into its corresponding scintillation fiber, can be measured by 
discriminating between the input signals according to the crest value with 
the multichannel pulse-height analyzer 603. 
Ninth Embodiment! 
FIG. 10 is a configurational view illustrating a distribution type detector 
according to a ninth embodiment of the present invention and is also a 
view showing the structure of a device for measuring an energy spectrum of 
a radiation or an optical pulse in a given wavelength region as well as a 
position where the radiation or the optical pulse in the given wavelength 
region employed in the first embodiment is entered. Upon measurement of 
the distribution of energy, this device can also compensate for dependence 
on the position where the radiation or the optical pulse in the given 
wavelength region is entered, on a software basis. In FIG. 10, reference 
numeral 701 indicates a coincidence circuit. Reference numeral 702 
indicates a multichannel type analog-to-digital converter which starts to 
operate after having been supplied with an external trigger. Reference 
numeral 703 indicates a computer such as a personal computer and reference 
numeral 704 indicates a multichannel pulse-height analyzer. 
The operation of the detector shown in FIG. 10 will now be described. 
An electric pulse outputted from a photosensitive element 104b is inputted 
to a preamplifier 501 from which two signals are outputted. One of the two 
signals is inputted to a constant fraction discriminator 106b. The 
subsequent operation is performed in a manner similar to the first 
embodiment. The other of the two signals is inputted to an amplifier 502 
where the signal is further amplified. Each optical pulse can be more 
accurately measured by compensating for the crest value of each of the 
optical pulses produced by fluorescence within the scintillation fiber 
102a and 102b as described in the eighth embodiment. To compensate for it, 
the degree or level of a loss relative to a distance over which each 
optical pulse produced by fluorescence is propagated within its 
corresponding fiber, is measured in advance and a distance to be 
propagated through the corresponding fiber is measured according to the 
incident position of the radiation or the optical pulse in the given 
wavelength region upon actual measurement. Thereafter, the crest value of 
each propagated optical pulse may be compensated based on the value of the 
propagated distance. When two signals corresponding to a signal outputted 
from the amplifier 502 and a signal outputted from a time-to-pulse height 
converter 107 are inputted to the coincidence circuit 701 during a 
predetermined time, the coincidence circuit 701 outputs a signal to a gate 
input terminal of the analog-to-digital converter 702. Further, a signal 
outputted from the amplifier 502 and a signal outputted from the 
time-to-pulse height converter 107 are converted into digital form by the 
analog-to-digital converter 702. Next, the computer 703 receives the two 
signals. The signal obtained by converting the signal outputted from the 
time-to-pulse height converter 107 into digital form is also inputted to a 
multichannel pulse-height analyzer 109. The computer 703 compensates for 
the crest value of the signal outputted from the amplifier 502 based on 
the two signals inputted thereto in the same manner as described in the 
eighth embodiment. The computer 703 outputs the compensated value to the 
multichannel pulse-height analyzer 704 as a signal. 
The crest value of the pulse, which is counted by the multichannel 
pulse-height analyzer 704, is substantially proportional to the energy of 
a radiation or an optical pulse 101 in a given wavelength region, which 
falls on each scintillation fiber. Thus, an energy spectrum of the 
radiation or the optical pulse 101 in the given wavelength region, which 
has entered into its corresponding scintillation fiber, can be measured by 
discriminating between the input signals according to the crest value with 
the multichannel pulse-height analyzer 704. 
Tenth Embodiment! 
FIG. 11 is a configurational view showing a scintillation fiber according 
to a tenth embodiment of the present invention. In FIG. 11, reference 
numeral 801 indicates a scintillation fiber bundle obtained by forming a 
plurality of scintillation fibers into one with fusing bonding, adhesion 
or the like. A drawing on the right side of FIG. 11 is a cross-sectional 
view of the bundle. A cross-section of the single scintillation fiber at 
this time shows a circle. Optical pulses generated by the scintillation 
fiber bundle 801 are received by one photosensitive element attached to an 
end face of the scintillation fiber bundle 801 or an optical delay fiber 
or by two photosensitive elements attached to end faces thereof. 
The operation will now be described. 
The formation of the plurality of scintillation fibers into one 
scintillation fiber bundle as shown in FIG. 11 enables the expansion of a 
range in which a radiation or an optical pulse in a given wavelength 
region, which enters into the scintillation fiber bundle, interacts with 
the scintillation fiber bundle. Namely, the probability of the interaction 
of the radiation or the optical pulse with the scintillation fiber bundle 
increases and the number of optical pulses produced when one radiation or 
an optical pulse in a given wavelength region enters, becomes greater, 
with the result that the quantity of light received by the photosensitive 
element can be increased. It is therefore possible to raise the 
sensitivity of a detector. Further, the optical pulses generated by the 
scintillation fiber bundle 801 are received by the one or two 
photosensitive elements attached to the end faces of the scintillation 
fiber bundle 801 or the optical delay fiber. 
Eleventh Embodiment! 
FIG. 12 is a configurational view showing a scintillation fiber according 
to an eleventh embodiment of the present invention. In FIG. 12, reference 
numeral 901 indicates a scintillation fiber bundle obtained by forming a 
plurality of scintillation fibers each quadrangular in section into one by 
fusion bonding or the like. A drawing on the right side of FIG. 12 
corresponds to a cross-sectional view of the scintillation fiber bundle. 
Further, optical pulses generated by the scintillation fiber bundle 901 
are received by one photosensitive element attached to an end face of the 
scintillation fiber bundle 901 or an optical delay fiber or by two 
photosensitive elements attached to end faces of the scintillation fiber 
bundle 901 or the optical delay fiber. According to this invention, the 
same operations and effects as those obtained in the tenth embodiment can 
be brought about. 
Twelfth Embodiment! 
FIG. 13 is a configurational view showing fiber plates according to a 
twelfth embodiment of the present invention. In FIG. 13, reference numeral 
1001 indicates a radiation or an optical pulse in a given wavelength 
region. Reference numerals 1002 and 1003 respectively indicate fiber 
plates each formed by joining scintillation fibers to one another in the 
form of a plate. Reference numerals 1004 and 1005 indicate fluorescent 
points respectively. Reference numerals 1006a, 1006b, 1007a and 1007b 
respectively indicate optical pulses generated by fluorescence. Further, 
optical delay fibers or photosensitive elements are attached to end faces 
of each of the fiber plates 1002 and 1003 so that information can be 
obtained from individual scintillation fibers. 
The operation will now be described. 
In the aforementioned tenth and eleventh embodiments, the scintillation 
fibers are shaped in the form of the bundle. In the present invention, 
however, the scintillation fibers are shaped in plate form by fusion 
bonding, adhesion or the like without forming them into the single bundle 
and the two fiber plates 1002 and 1003 are arranged in parallel with each 
other as shown in FIG. 13. When several radiations or optical pulses in a 
given wavelength region enters in the form of a locus as shown in FIG. 13, 
fluorescence is produced at the fluorescent point 1004 or 1005 in the 
fiber plate 1002 or 1003. Thus, the optical pulses 1006a, 1006b, 1007a and 
1007b are generated and propagated so as to reach both ends of the 
respective scintillation fibers. By receiving the optical pulses 1006a, 
1006b, 1007a and 1007b with the photosensitive elements disposed on their 
corresponding extensions of the scintillation fibers that give rise to 
fluorescence, each position where the radiations or the optical pulses in 
the given wavelength region on the fiber plates 1002 and 1003 enters, can 
be two-dimensionally determined. Further, tracks of the radiations or the 
optical pulses in the given wavelength region can be understood from the 
information obtained from the two fiber plates. 
Thirteenth Embodiment! 
FIG. 14 is a configurational view showing fiber plates according to a 
thirteenth embodiment of the present invention. Elements of structure 
shown in FIG. 14 are identical to those employed in the twelfth 
embodiment. However, a fiber plate 1003 is provided so as to be rotated 
through 90 degrees with respect to FIG. 13. Further, optical delay fibers 
or photosensitive elements are attached to both ends of the respective 
fiber plates 1002 and 1003 so that information can be brought about from 
individual scintillation fibers. Even if they are disposed in the 
above-described manner, effects are identical to those obtained in the 
twelfth embodiment. In the present embodiment, the photosensitive elements 
may be connected to individual scintillation fibers of each fiber plate. 
However, even if the fiber plates 1002 and 1003 are closely disposed and 
the respective photosensitive elements are connected to both ends of each 
fiber plate so as to take out only position information in the 
longitudinal direction of the fibers of each fiber plate, two-dimensional 
position information can be obtained by the fiber plates 1002 and 1003 
orthogonal to each other. Further, track information can be also obtained 
by providing the two intersecting fiber plates in the form of two sets. 
Fourteenth Embodiment! 
FIG. 15 illustrates an embodiment in which photosensitive elements are 
attached to the scintillation fibers or the optical delay fibers employed 
in the twelfth and thirteenth embodiments. In FIG. 15, reference numeral 
1201 indicates a fiber plate obtained by shaping scintillation fibers in 
the form of a plate or an optical delay fiber group (optical delay fibers 
may not be shaped in the form of a plate). Reference symbols 1202a through 
1202f indicate photosensitive elements respectively. The fibers of the 
fiber plate 1201 are in one-to-one correspondence with the photosensitive 
elements. The mating faces between the fibers and the photosensitive 
elements are joined to one another with silicon adhesives or connectors or 
the like. It is thus possible to obtain information from the individual 
scintillation fibers. 
Fifteenth Embodiment! 
FIG. 16 shows an embodiment in which a photosensitive element is attached 
to the scintillation fibers or the optical delay fibers employed in the 
twelfth and thirteenth embodiments. In FIG. 16, reference numeral 1301 
indicates a fiber plate obtained by shaping scintillation fibers in the 
form of a plate or an optical delay fiber group (optical delay fibers may 
not be shaped in the form of a plate). Reference numeral 1302 indicates a 
photosensitive element. Reference symbols 1303a through 1303f respectively 
indicate electric signals outputted from the photosensitive element 1302. 
The photosensitive element 1302 is of the multianode type. The fibers are 
in one-to-one correspondence with anodes of the photosensitive element 
1302. Thus, the outputs 1303a through 1303f produced from the 
photosensitive element 1302 match with their corresponding fibers. The 
mating faces between the fibers and the photosensitive element are joined 
to one another with silicon adhesive or connectors or the like. 
Thus, information can be obtained from the individual scintillation fibers. 
Sixteenth Embodiment! 
FIG. 17 illustrates an embodiment in which photosensitive elements are 
mounted to the scintillation fibers or the optical delay fibers employed 
in the twelfth and thirteenth embodiments. In FIG. 17, reference numeral 
1401 indicates a fiber plate obtained by shaping scintillation fibers in 
the form of a plate or an optical delay fiber group (optical delay fibers 
may not be shaped in the form of a plate). Reference symbols 1402a and 
1402b indicate photosensitive elements respectively. Reference symbols 
1403a through 1403f respectively indicate electric signals outputted from 
the photosensitive elements 1402a and 1402b. 
Each of the photosensitive elements 1402a and 1402b is of the multianode 
type. The fibers are in one-to-one correspondence with anodes of the 
photosensitive elements. Thus, the outputs 1403a through 1403f produced 
from the photosensitive elements 1402a and 1402b match with their 
corresponding fibers. The mating faces between the fibers and the 
photosensitive elements are joined to each other with silicon adhesives or 
connectors or the like. 
Thus, information can be obtained from the individual scintillation fibers. 
The configuration shown in FIG. 17 is substantially similar to that shown 
in FIG. 16. If, however, the number of the fibers is greater than the 
number of the anodes of the photosensitive elements, then the 
configuration shown in FIG. 17 may be adopted. 
Seventeenth Embodiment! 
FIG. 18 is a configurational view showing a seventeenth embodiment of the 
present invention. The present embodiment shows, as an illustrative 
example, a case where the optical delay fibers employed in the tenth 
through sixteenth embodiments are attached to the scintillation fibers. In 
FIG. 18, reference numeral 1501 indicates a combination obtained by 
joining optical delay fibers identical in diameter and number to 
scintillation fibers to one another in the form of a bundle or a plate 
with fusion bonding or the like. Reference numeral 1502 indicates a 
combination obtained by joining scintillation fibers to one another in the 
form of a bundle or a plate. At the mating face between the two 
combinations, the scintillation fibers are in one-to-one correspondence 
with the optical delay fibers and the two combinations are joined to one 
another with a silicon adhesive or the like. Thus, the loss of light at 
the mating face therebetween can be reduced. 
Eighteenth Embodiment! 
FIG. 19 is a configurational view showing an eighteenth embodiment of the 
present invention. The present embodiment shows, as an illustrative 
example, a case where the optical delay fiber employed in each of the 
tenth and eleventh embodiments is attached to scintillation fibers. In 
FIG. 19, reference numeral 1601 indicates a single optical delay fiber. 
Reference numeral 1602 indicates a light guide of acrylic, for example. 
Reference numeral 1603 indicates a scintillation fiber bundle obtained by 
joining scintillation fibers to one another in the form of a bundle. At 
the mating face between the optical delay fiber and the optical guide, and 
between the scintillation fiber bundle and the optical guide, they are 
bonded to one another with fusion or silicon adhesives or the like. 
Thus, the light can be efficiently propagated through the scintillation 
fiber bundle and the optical delay fiber. 
In the case where the optical delay fiber is used in plural form in the 
eighteenth embodiment, the same effects as described above can also be 
obtained. 
Nineteenth Embodiment! 
FIG. 20 is a configurational view showing a nineteenth embodiment of the 
present invention. In FIG. 20, reference symbols 1701a, 1701b and 1701c 
indicate radiations to be measured respectively. Reference symbols 1702a, 
1702b, 1702c and 1702d indicate points at which the radiations interact 
with their corresponding substances. Reference numeral 1703 indicates a 
cross-section of a scintillation fiber. Reference numeral 1704 indicates a 
cross-section of a material such as an aluminum foil applied to the 
scintillation fiber 1703, which is capable of absorbing a low-energy 
radiation. Reference numeral 1705 indicates a cross-section of a 
backscattering material such as lead bonded onto the scintillation fiber 
1703, which is capable of backscattering a high-energy radiation. 
Reference symbol 1701d indicates a secondary radiation scattered by the 
backscattering material 1705. 
The operation will now be described. 
When the radiation 1701a is of a low-energy radiation (e.g., several keV 
through several ten keV), the radiation 1701a interacts with the aluminum 
foil 1704 at the point 1702a in the aluminum foil 1704 and the probability 
that the radiation 1701a will be absorbed, becomes high. On the other 
hand, when the radiation 1701c is of a high-energy radiation (e.g., 1 MeV 
or higher), the probability that the radiation 1701c will interact with 
the aluminum foil 1704, becomes low. Further, there is also a possibility 
of transmission of the radiation 1701c through the scintillation fiber 
1703. A part of the low-energy radiation or a part of the high-energy 
radiation interacts with the scintillation fiber 1703 at the point 1702b 
in the scintillation fiber 1703 as in the case of the radiation 1701b. The 
above depends on the thickness of each of the aluminum foil 1704, the 
scintillation fiber 1703, and the lead 1705. However, the above can take 
place if the thickness thereof is adjusted. The backscattering material 
1705 is provided to allow the radiation 1701c to interact with the 
scintillation fiber 1703. There is a possibility that the radiation 1701c 
will interact with the backscattering material 1705 at the point 1702c in 
the backscattering material 1705 after having passed through the 
scintillation fiber 1703. If the interaction produced therebetween at this 
time is of Compton scattering, then there is a possibility that a 
radiation, which is backscattered and produced on a secondary basis, will 
enter into the scintillation fiber 1703 again. Since this secondary 
radiation 1701d is lower in energy than the primary radiation, there is a 
strong likelihood that the radiation 1701d will interact with the 
scintillation fiber 1703 at the point 1702d in the scintillation fiber 
1703. 
The probability that the low-energy radiation will interact with its 
corresponding substance within the scintillation fiber, is forcibly 
lowered by providing the aluminum foil and the lead around the 
scintillation fiber as described above, thereby making it possible to 
increase the probability that the high-energy radiation will interact with 
its corresponding substance within the scintillation fiber. 
When high-energy radiations normally become identical in dose rate to 
low-energy radiations, the number of the low-energy radiations increases. 
Namely, when the low-energy radiations enter into a detector even if they 
are identical in dose rate to each other, the counting rate of the 
detector increases. It is thus necessary to cut the low-energy radiations 
to some level as compared with the high-energy radiations in order to hold 
the sensitivity of the detector relative to the dose rate at a 
substantially constant level regardless of the energy. This results in the 
adoption of the above construction. 
Thus, the sensitivity of the radiation detector with respect to the dose 
rate can be kept substantially constant regardless of the energy of a 
radiation. 
In the nineteenth embodiment, the material for absorbing the low-energy 
radiation and the material for backscattering the high-energy radiation 
are made circular in cross section. Alternatively, they may be rectangular 
in cross section as shown in FIG. 21. In FIG. 21, reference numeral 1801 
indicates an absorbing material for absorbing a low-energy radiation. 
Reference numeral 1802 indicates a material for backscattering a 
high-energy radiation. 
Even if such a construction is adopted, the same effects as those obtained 
in the nineteenth embodiment can be obtained. 
FIG. 22 shows a case where the scintillation fiber employed in the 
nineteenth embodiment is rectangular in cross section. In FIG. 22, 
reference numeral 1901 indicates a scintillation fiber rectangular in 
cross section. 
The same effects as those obtained in the nineteenth embodiment can also be 
brought about in the case of such a construction. 
Twentieth Embodiment! 
FIG. 23 is a configurational view illustrating a twentieth embodiment of 
the present invention. In FIG. 23, reference numeral 2001 indicates a 
cross-section of a scintillation fiber. Reference numeral 2002 indicates a 
backscattering material for backscattering radiations. 
The operation of the present embodiment will now be described. 
In order to keep the sensitivity of a detector substantially constant 
without recourse to the energy of an incident radiation as described in 
the nineteenth embodiment, it is necessary to cut a low-energy radiation 
as compared with a high-energy radiation. However, when the construction 
used in the nineteenth embodiment cannot be adopted, the backscattering 
material 2002 is disposed as shown in FIG. 23 so as to increase the 
probability of interaction of the high-energy radiation with the 
scintillation fiber and prevent a reduction in the probability of 
interaction with the low-energy radiation. 
Owing to such a construction, the sensitivity of the radiation detector 
with respect to the dose rate can be kept substantially constant without 
depending on the radiation energy. 
FIG. 24 further shows a case where the backscattering material employed in 
the twentieth embodiment is wound around its corresponding portion of a 
scintillation fiber along the scintillation fiber. In FIG. 24, reference 
numeral 2101 indicates a backscattering material for backscattering a 
high-energy radiation. 
Such a construction can bring about the same effects as those obtained in 
the twentieth embodiment. 
Twenty-First Embodiment! 
FIG. 25 is a configurational view showing a twenty-first embodiment of the 
present invention. In FIG. 25, reference numeral 2201 indicates a 
scintillation fiber. Reference numeral 2202 indicates a cross-section of a 
material such as an aluminum foil stuck onto the scintillation fiber 2201, 
which is capable of absorbing a low-energy radiation. 
The operation will now be described. 
In order to keep the sensitivity of a detector substantially constant 
without recourse to the energy of an incident radiation as described in 
the nineteenth embodiment, it is necessary to cut a low-energy radiation 
with respect to a high-energy radiation and make the probability of 
interaction with the high-energy radiation as high as possible. However, 
when the construction used in the nineteenth embodiment cannot be adopted, 
the absorbing material 2202 is disposed forward of the scintillation fiber 
2201 as shown in FIG. 25 so as to cut a part of the low-energy radiation 
before it enters the scintillation fiber 2201. 
Owing to this construction, the sensitivity of the radiation detector 
relative to the dose rate can be held substantially constant without 
recourse to the energy of a radiation. 
FIG. 26 further shows a case where the absorbing material employed in the 
twenty-first embodiment is wound on its corresponding portion of a 
scintillation fiber along the scintillation fiber. In FIG. 26, reference 
numeral 301 indicates an absorbing material for absorbing a low-energy 
radiation. 
In the case of such a construction, the same effects as those obtained in 
the twenty-first embodiment can also be brought about. 
Twenty-Second Embodiment! 
In the present embodiment, a scintillation fiber is different from a 
conventional one. An inorganic monocrystal scintillation material such as 
bismuth-germanate or the like is used as a material used for the 
scintillation fiber. 
Since the bismuth-germanate is relatively low in scintillation efficiency 
light absorption rate but includes a higher atomic number element and has 
a large specific gravity, the probability that the bismuth-germanate will 
interact with a radiation, becomes high. It is therefore possible to 
increase the probability that a high-energy radiation will react with the 
scintillation fiber and to flatten or smooth the sensitivity of a dose 
rate with respect to the energy of the radiation. 
Twenty-Third Embodiment! 
FIG. 27 is a configurational view showing a twenty-third embodiment of the 
present invention. In FIG. 27, reference numeral 2401 indicates a 
radiation or an optical pulse in a given wavelength region. Reference 
numeral 2402 indicates a scintillation fiber. Reference numeral 2403 
indicates an optical pulse generated by fluorescence. Reference numeral 
2404 indicates a semiconductor light-amplifier module using a GaAIAs 
semiconductor, for example. Reference numeral 2405 indicates an optical 
delay fiber. Reference numeral 2406 indicates a photosensitive element. 
Further, a semiconductor light amplifier amplifies the height of an 
optical pulse propagated through the scintillation fiber in the direction 
opposite to that of the optical pulse 2403. 
The operation will now be described. 
When the radiation or optical pulse 2401 in the given wavelength region 
falls on the scintillation fiber 2402, fluorescence is produced so as to 
generate the optical pulse 2403. When the optical pulse 2403 is 
transmitted through the scintillation fiber 2402, an optical loss is 
produced and hence the value of the pulse height is lowered. To supplement 
the loss, the semiconductor light-amplifier module 2404 is connected to 
the scintillation fiber 2402 so as to amplify the height of the optical 
pulse 2403. Thereafter, the amplified optical pulse is transmitted through 
the optical delay fiber 2405, followed by inputting to the photosensitive 
element 2406 where the optical pulse is converted into an electric pulse. 
The transmission loss of light transmitted within the scintillation fiber 
can be supplemented owing to such a construction, thereby making it 
possible to increase a measuring range. 
In the twenty-third embodiment, the semiconductor light-amplifier module 
2404 and the photosensitive element 2406 shown in FIG. 27 may be directly 
connected to each other without the optical delay fiber 2405. 
In the case of such a construction, the transmission loss of light 
transmitted within the fiber can also be supplemented, thereby making it 
possible to increase a measuring range. 
Twenty-Fourth Embodiment! 
FIG. 28 is a configurational view showing a twenty-fourth embodiment of the 
present invention. In FIG. 28, reference numeral 2501 indicates a 
wavelength shifting fiber doped with a wavelength shifter material. 
When the wavelength of an optical pulse 2403 generated within a 
scintillation fiber 2402 is shorter than a wavelength band that can be 
amplified by a semiconductor light-amplifier module 2404, the wavelength 
shifting fiber 2501 is inserted between the scintillation fiber 2402 and 
the semiconductor light-amplifier module 2404 so that the wavelength of 
the propagated optical pulse is shifted to the wavelength band that can be 
amplified by the semiconductor light-amplifier module 2404. 
According to this construction, even if the wavelength of the optical pulse 
2403 generated in the scintillation fiber 2402 is shorter than the 
amplifierable wavelength band of the semiconductor light-amplifier module 
2404, the wavelength thereof can be amplified by shifting it to the 
amplifierable wavelength band. Therefore, the transmission loss of light 
transmitted within the fiber can be supplemented so that a measuring range 
can be expanded 
Twenty-Fifth Embodiment! 
FIG. 29 is a configurational view showing a twenty-fifth embodiment of the 
present invention. In FIG. 29, reference symbols 2601a and 2601b 
respectively indicate transmission optical fibers connected to their 
corresponding scintillation fibers 102a and 102b and identical in length 
to each other. Reference symbols 2602a and 2602b respectively indicate 
support members for supporting the transmission optical fibers. Reference 
symbols 2603a and 2603b indicate drive motors with rails respectively. 
Incidentally, photosensitive elements are respectively connected to the 
leading ends of the transmission optical fibers and are activated in the 
same manner as the first embodiment. 
The operation will now be described. 
The support members 2602a and 2602b for supporting the transmission optical 
fibers 2601a and 2601b respectively are fixed to their corresponding drive 
motors 2603a and 2603b. When the drive motors 2603a and 2603b are driven, 
the support members 2602a and 2602b are raised or lowered over the rails. 
Thus, a range of the scintillation fiber, for detecting a radiation or an 
optical pulse in a given wavelength region is expanded. In practice, the 
drive motors 2603a and 2603b with the rails cause the scintillation fibers 
102a and 102b to move to predetermined positions. Further, the radiation 
or the optical pulse is measured at the predetermined positions as in the 
first embodiment. After completion of its measurement, the drive motors 
2603a and 2603b cause the scintillation fibers 102a and 102b to move to 
the following positions again, followed by measurement of the radiation or 
the optical pulse. By repeating this processing several times, a 
wide-range measurement is made possible. 
Since the transmission optical fibers 2601a and 2601b simply transmit the 
optical pulses propagated through the scintillation fibers 102a and 102b 
to their corresponding photosensitive elements, they do not exert 
influences on the principle of measurement. 
Twenty-Sixth Embodiment! 
FIG. 30 is a configurational view showing a twenty-sixth embodiment of the 
present invention. In FIG. 30, reference symbols 2701a and 2701b 
respectively indicate O/E conversion modules including photosensitive 
elements and preamplifiers connected to their corresponding scintillation 
fibers 102a and 102b. Reference symbols 2702a and 2702b respectively 
indicate cables for transmitting signals outputted from the O/E conversion 
modules 2701a and 2701b. Incidentally, constant fraction discriminators 
are connected to their corresponding leading ends of the transmission 
cables 2702a and 2702b and are activated in a manner similar to the first 
embodiment. 
In the case of this construction, the same effects as those obtained in the 
twenty-fifth embodiment can also be brought about. 
Twenty-Seventh Embodiment! 
FIG. 31 is a configurational view showing a twenty-seventh embodiment of 
the present invention. In FIG. 31, reference symbols 2801a and 2801b 
respectively indicate standard radiation sources embedded in their 
corresponding scintillation fibers 102a and 102b and used as standards for 
position measurements. Each standard radiation source is constructed by 
selectively etching only a cladding using the difference in composition 
between the cladding and each core and embedding, for example, cesium 137 
into a recess (whose diameter is 1 mm or so, for example) defined by 
etching. However, the etching of the cladding is effected not so as to 
reach each core and exert an influence on the propagation of light within 
each core. Reference symbols 2802a and 2802b respectively indicate 
photosensitive elements connected to their corresponding scintillation 
fibers 102a and 102b. Reference symbols 2803a and 2803b respectively 
indicate cables for transmitting electric signals outputted from their 
corresponding photosensitive elements 2802a and 2802b. 
The operation will now be described. 
In the prior art, the position where the radiation or the optical pulse in 
the given wavelength region enters into the scintillation fiber 102a or 
102b, is calculated from the output (corresponding to the difference 
between the time intervals during which the optical pulses propagated to 
both ends of the fiber reach their corresponding photosensitive elements) 
and the speed of light transmitted through the fiber. However, the speed 
of light propagated through the fiber slightly varies depending on the 
refractive index and shape of the fiber and the way of laying out the 
fiber. Thus, an error is developed in the position measurement. To 
compensate for the error, the standard radiation sources 2801a and 2801b 
are embedded into predetermined positions respectively. As a result, 
fluorescence is produced in the cores provided at the positions where the 
standard radiation sources 2801a and 2801b are embedded, to thereby 
generate optical pulses. The resultant pulses are propagated through the 
fibers so as to reach the photosensitive elements 2802a and 2802b provided 
at both ends. As the result of measurement (corresponding to one obtained 
by representing values outputted from a multichannel pulse-height analyzer 
in the form of a graph), peaks are respectively outputted to the locations 
where the standard radiation sources 2801a and 2801b are embedded. The 
position where the measuring radiation or optical pulse in the given 
wavelength region enters into the corresponding fiber, can be determined 
with sufficient accuracy based on the difference in position between the 
two peaks and the difference between the positions where the standard 
radiation sources are embedded. Incidentally, the principle of measurement 
is identical to that employed in the first embodiment. 
FIG. 32 is a configurational view showing a modification of the 
twenty-seventh embodiment. In FIG. 32, reference symbols 2901a and 2901b 
respectively indicate standard radiation sources of such types that, for 
example, radiation nuclides are allowed to uniformly diffuse into glass 
beads each having a diameter of 1 mm or so and the glass beads are 
embedded in plastic plates. The standard radiation sources 2901a and 2901b 
are bonded onto their corresponding scintillation fibers 102a and 102b. 
Owing to this construction, the same effects as those obtained in the 
twenty-seventh embodiment can be brought about. 
Incidentally, the twenty-seventh embodiment shows the case where the two 
standard radiation sources are respectively embedded in or bonded onto the 
scintillation fibers. However, two or more standard radiation sources may 
be respectively embedded in or bonded onto scintillation fibers or an 
optical delay fiber according to the lengths of the scintillation fibers 
or the length of the optical delay fiber. 
In the case of this construction, the same effects as those obtained in the 
twenty-seventh embodiment can also be brought about. 
Twenty-Eighth Embodiment! 
FIG. 33 is a configurational view showing a twenty-eighth embodiment of the 
present invention. In FIG. 33, reference numeral 3001 indicates a core in 
a scintillation fiber or an optical delay fiber. Reference numeral 3002 
indicates a cladding in the scintillation fiber or optical delay fiber. 
Reference numeral 3003 indicates a photosensitive element wherein a 
cathode, an anode and the like are three-dimensionally shaped in the form 
of an array by micromachining technology. Reference numeral 3004 indicates 
a cable for transmitting an electric signal outputted from the 
photosensitive element 3003 to a preamplifier. No coating is applied to 
the outside of the cladding in FIG. 33. However, whether or not the 
coating is applied thereto, is determined depending on measuring 
conditions and measuring environments. 
Incidentally, the photosensitive element 3003 is embedded in the 
scintillation fiber or the optical delay fiber in accordance with the 
following technique or method. Firstly, only the core is selectively 
etched using the difference in composition between the cladding and core 
of the scintillation fiber or the optical delay fiber to thereby form a 
recess or concave portion. The photosensitive element 3003 is then 
embedded in the recess. 
A detector can be reduced in size owing to such a construction. Further, an 
optical pulse propagated through the fiber can be efficiently detected by 
the photosensitive element 3003. 
Twenty-Ninth Embodiment! 
FIG. 34 is a configurational view illustrating a twenty-ninth embodiment of 
the present invention. In FIG. 34, reference numeral 3101 indicates such a 
photosensitive element as described in the twenty-eighth embodiment. 
Reference numeral 3102 indicates, for example, a silicon adhesive poured 
into a spacing defined between the photosensitive element 3101 and a 
recess or concave portion defined by processing in a core of a 
scintillation fiber or an optical delay fiber. Reference numeral 3103 
indicates a cable for transmitting an electric signal outputted from the 
photosensitive element 3101 to a preamplifier. No coating is applied to 
the outside of a cladding in FIG. 34. However, whether or not the coating 
is applied thereto, is decided depending on measuring conditions and 
measuring environments. 
There is a possibility that a space will be defined between the 
photosensitive element 3101 and the recess defined in the core of the 
fiber as shown in FIG. 34. In order to detect an optical pulse which has 
been efficiently propagated through the fiber even if the space exists, 
the adhesive 3102 is poured into the spacing to fix the photosensitive 
element 3101. 
In the case of this construction, a detector can also be reduced in size in 
a manner similar to the twenty-eighth embodiment. Further, the optical 
pulse transmitted through the fiber can be efficiently detected by the 
photosensitive element 3101. 
Since the invention is constructed as described above, the following 
advantageous effects can be brought about. 
According to a first aspect of the present invention, since a configuration 
wherein an optical delay fiber is connected as well as scintillation 
fibers, is adopted, the simplification of a measuring circuit system 
capable of raising position resolution, the integration of measuring 
circuits into a single system, etc. can be achieved. 
According to a second aspect of the present invention, since an optical 
delay fiber is centrally inserted between scintillation fibers and a 
time-to-pulse height converter is provided wherein a terminal supplied 
with a firstly-propagated signal is not distinguished from a terminal 
supplied with a subsequently-propagated signal, a measuring range of the 
time-to-pulse height converter can be reduced and hence position 
resolution can be improved as compared with the prior art. 
According to a third aspect of the present invention, since one end face of 
a scintillation fiber and an end face of an optical delay fiber connected 
to the other end of the scintillation fiber are connected to the same 
photosensitive element, the photosensitive element, a preamplifier and a 
constant fraction discriminator are provided as single and measuring 
circuits are integrated into one system by using a measuring circuit 
capable of measuring the difference between time intervals necessary for 
two optical signals introduced into the single photosensitive element, an 
error produced due to the difference in characteristic between measuring 
instruments can be eliminated and a detector can be reduced in size. 
According to a fourth aspect of the present invention, since a 
photosensitive element is connected to one end face of a scintillation 
fiber, a reflector is attached to an end face of an optical delay fiber 
connected to the other end of the scintillation fiber and measuring 
circuits are brought into one system by using a measuring circuit capable 
of measuring the difference between time intervals necessary for two 
optical signals launched into the single photosensitive element, an error 
developed due to the difference in characteristic between measuring 
instruments can be eliminated and a detector can be reduced in size. 
According to a fifth aspect of the present invention, since a preamplifier 
capable of outputting two signals therefrom in response to a single signal 
inputted thereto is provided, the distribution of energy can be measured 
as well as the incident position of the radiation or the optical pulse in 
the specific wavelength. 
According to a sixth aspect of the present invention, since a loss of an 
optical signal produced by its propagation distance is compensated by 
software or hardware, the difference between distribution results on 
energy at respective incident positions of a radiation to be measured or a 
light pulse to be measured, in a given wavelength region can be reduced. 
According to a seventh aspect of the present invention, since a plurality 
of scintillation fibers are shaped in the form of a bundle and the bundle 
is constructed as a detecting unit, the probability that an incident 
radiation or optical pulse in a given wavelength region will react with 
each scintillation fiber within the scintillation fiber bundle, can be 
raised and the quantity of light incident on a photosensitive element can 
be also increased. 
According to an eighth aspect of the present invention, since a fiber plate 
obtained by shaping a plurality of scintillation fibers in the form of a 
plate is constructed as a detecting unit, a position where a radiation or 
an optical pulse in a given wavelength region enters into the fiber plate, 
can be measured on a two-dimensional basis. 
According to a ninth aspect of the present invention, since a plurality of 
fiber plates are disposed in parallel, a distribution type detector using 
scintillation fibers can measure a track of a radiation or a light pulse 
in a given wavelength region. 
According to a tenth aspect of the present invention, since fiber plates 
are stacked on one another so that fiber extending directions intersect at 
right angles, a distribution type detector using scintillation fibers can 
two-dimensionally measure each incident position of a radiation or an 
optical pulse in a given wavelength region using a reduced number of 
photosensitive elements. 
According to an eleventh aspect of the present invention, a distribution 
type detector using a scintillation fiber is constructed such that a 
material capable of absorbing a low-energy radiation is disposed forward 
of the scintillation fiber used as a detecting unit. Owing to this 
construction, the difference between the probability that the low-energy 
radiation will react within the scintillation fiber and the probability 
that a high-energy radiation will react within the scintillation fiber, 
can be reduced and the sensitivity of a dose rate with respect to the 
energy of the radiation can be flattened. 
According to a twelfth aspect of the present invention, a distribution type 
detector using a scintillation fiber is constructed such that a material 
capable of backscattering a high-energy radiation is disposed behind the 
scintillation fiber used as a detecting unit. Owing to this construction, 
the difference between the probability that a low-energy radiation will 
react within the scintillation fiber and the probability that the 
high-energy radiation will react within the scintillation fiber, can be 
reduced and the sensitivity of a dose rate with respect to the energy of 
the radiation can be flattened. 
According to a thirteenth aspect of the present invention, a distribution 
type detector using a scintillation fiber is constructed such that an 
inorganic scintillation material is used as a material for the 
scintillation fiber. Owing to this construction, the probability that a 
high-energy radiation will react within the scintillation fiber, can be 
raised. 
According to a fourteenth aspect of the present invention, a distribution 
type detector using a scintillation fiber is provided with a light 
amplifier on a path of the scintillation fiber or an optical delay fiber. 
Owing to this construction, a transmission loss of light propagated within 
the fiber can be supplemented and a measuring range can be increased. 
According to a fifteenth aspect of the present invention, a distribution 
type detector using a scintillation fiber is constructed such that a fiber 
doped with a wavelength shifter material is provided between the 
scintillation fiber and a light amplifier. Owing to this construction, the 
wavelength of each optical pulse produced by fluorescence within the 
scintillation fiber can be shifted to an amplifierable wavelength band of 
the light amplifier by the wavelength shifter even if the wavelength of 
each optical pulse produced within the scintillation fiber is shorter than 
the amplifierable wavelength band thereof, with the result that a 
transmission loss of light propagated within the fiber can be supplemented 
and a measuring range can be expanded. 
According to a sixteenth aspect of the present invention, a distribution 
type detector using scintillation fibers is provided with radiation 
sources respectively attached to the scintillation fibers. By providing 
the radiation sources used as standards for position measurement in this 
way, position accuracy with respect to the measurement of a position where 
a radiation or an optical pulse in a given wavelength region enters, can 
be improved. 
According to a seventeenth aspect of the present invention, a distribution 
type detector using a scintillation fiber is one of a type wherein the 
scintillation fiber which serves as a detecting portion, can be moved. By 
doing so, a measuring range can be expanded and a spatial distribution of 
a radiation to be measured or an optical pulse in a given wavelength 
region can be measured. 
According to an eighteenth aspect of the present invention, since a 
photosensitive element is embedded in an end of a fiber by micromachining 
technology, a detector can be reduced in size and a loss of light 
transmitted within the fiber, which is produced at the end face of the 
fiber, can be reduced, thereby making it possible to expand a measuring 
range. 
While the present invention has been described with reference to the 
illustrative embodiments, this description is not intended to be construed 
in a limiting sense. Various modifications of the illustrative 
embodiments, as well as other embodiments of the invention, will be 
apparent to those skilled in the art on reference to this description. It 
is therefore contemplated that the appended claims will cover any such 
modifications or embodiments as fall within the true scope of the 
invention.