Radiation detector

Abstract: A radiation detector has a film-like pyroelectric element which has a fan shape, and two support plates which are made of an electrical and thermal insulating resin and adhered to the both ends elongating from the pivot of the fan shape to the peripheral portion. After a radiation absorbing layer is attached to one face of the pyroelectric element , the resin plates are adhered to each other so that the layer is positioned inside and the pyroelectric element is formed into a conic shape, thereby forming a conic portion. Radiation entering an opening of the bottom face of the conic portion is absorbed by the layer in the form of heat. The temperature rise is converted by the pyroelectric element into an electric signal, thereby detecting the energy amount of the radiation. A reflected component of radiation entering the layer again enters the layer . Since the input radiation is repeatedly reflected and absorbed by the layer , the radiation is absorbed and detected with about 100 % irrespective of the wavelength.

Description: The invention relates to a radiation detector which measures radiation energy. Recently, industrial application of UV or IR radiation expands beyond the wavelength range of 250 nm to 2.5 µm. Particularly, in evaluation of characteristics of radiation of a discharge lamp or a laser in the UV or IR region, the extension of the wavelength range of the radiometry standard becomes a serious problem. Conventionally, as the irradiance standard, employed is a method in which a blackbody furnace is used, or an absolute radio meter which consists of a thermal detector. In a UV region of a wavelength of 250 nm or shorter, however, a blackbody furnace generates radiation energy of a very low level. Therefore, an absolute radio meter is employed in such a region. A thermal detector comprises a thermal element such as a thermopile or a pyroelectric element which converts thermal energy into electrical energy, and a radiation absorbing layer which functions as a light receiving face and is made of a gold black deposition layer or a black coating composition. The radiation absorbing layer converts radiation energy into thermal energy, and the thermal element converts the thermal energy into electrical energy, thereby detecting the radiation energy. Consequently, the relative spectral responsivity of a thermal detector depends on the spectral absorption factor of the radiation absorbing layer to be used. In order to configure a thermal detector having a relative spectral responsivity which is free from the wavelength dependence, therefore, a radiation absorbing material having a relative spectral responsivity which is free from the wavelength dependency is required. In the prior art, for the sake of satisfying this requirement, gold black is used which is obtained by evaporating gold in an atmosphere of nitrogen. In order to eliminate the wavelength dependence of the spectral absorption factor, the thickness of the gold black layer must be increased. However, the configuration of the prior art has a problem in that, when the gold black layer has a large thickness, the heat loss in the layer is large and hence the sensitivity is largely impaired. It is reported that a thermal detector using gold black has a spectral responsivity which is constant with respect to the wavelength in the visible wavelength region, but exhibits the wavelength dependence in the UV and IR regions so that a deviation of about 3 % is observed at a wavelength of 250 nm (CIF Pub. No. 64: Determination of spectral responsivity of optical radiation detector). In order to eliminate the wavelength dependence of a spectral responsivity, a cryogenic radiometer has been developed. The radiometer comprises a cavity which is formed by a metal such as copper, and the inside of which is blackened by a black coating composition. The metal cavity is cooled to 5 K by liquid helium, radiation is repeatedly reflected by the inner wall of the cavity to be absorbed, and the temperature rise of the cavity due to the absorbed energy is measured by a thermocouple which is disposed outside the cavity. However, the radiometer has large restrictions or problems in that a cryostat, a temperature control apparatus and the like for the cooling process have a large-scaled configuration, that the cavity which functions as a detecting unit is positioned at the innermost portion of the cryostat and hence light to be measured must be formed as a beam having a very small spread, and that the measurement must be conducted through a window for preventing dew condensation and hence the transmittance of the window must accurately be measured. A cryogenic radiometer of the above kind is described in US-A-3660659. US-A-4906849 describes a radiation detector comprising a thermoelectric converting element which has an opening and a conic shape and in which a radiation absorbing layer is attached to an inner face thereof, wherein said radiation absorbing layer absorbs and converts light to be measured which enters said opening of said thermoelectric converting element into heat and where said thermoelectric converting element converts a temperature rise into an electrical signal thereby detecting an energy amount of the radiation. The present invention solves the above-discussed problems. It is an object of the invention to realize an improved radiation detector of a thermal type which can conduct the measurement at ordinary temperature, which has a spectral responsivity not depending on the wavelength, and which can obtain a stable output. This object is achieved with a radiation detector having the features of either of claims 1 or 4. Preferred embodiments are the subject matter of the appended subclaims. With the present invention, it is possible to realize a radiation detector having an S/N ratio which is twice that of the radiation detector. Fig. 1(A) is a longitudinal section view showing the configuration of a radiation detector. Fig. 1(B) is a rear view showing the configuration of the radiation detector of Fig. 1(A). Fig. 1(C) is a perspective view showing the configuration of the radiation detector of Fig. 1(A). Fig. 2(A) is a longitudinal section view showing the configuration of another radiation detector. Fig. 2(B) is a rear view showing the configuration of the radiation detector of Fig. 2(A). Fig. 2(C) is a perspective view showing the configuration of the radiation detector of Fig. 2(A). Fig.3(A) is a longitudinal section view showing the configuration of another radiation detector. Fig.3(B) is a rear view showing the configuration of the radiation detector of Fig. 3(A). Fig.3(C) is a perspective view showing the configuration of the radiation detector of Fig. 3(A). Fig.4(A) is a longitudinal section view showing the configuration of another radiation detector. Fig.4(B) is a rear view showing the configuration of the radiation detector of Fig. 4(A). Fig.4(C) is a perspective view showing the configuration of the radiation detectors of Fig. 4(A). Fig. 5(A) is a longitudinal section view showing the configuration of another radiation detector. Fig. 5(B) is a rear view showing the configuration of the radiation detector of Fig. 5(A). Fig. 6 is a diagram of the electrical connection of the radiation detector of Fig. 5 . Fig.7 is a view showing the internal reflection model having various apex angles. Fig.8 is a graph showing the relation between the wavelength and the reflectance. Fig.9 is a graph showing the relation between the wavelength and the reflectance. Fig.10(A) is a longitudinal section view showing the configuration of another radiation detector. Fig.10(B) is a rear view showing the configuration of the radiation detector of Fig. 10(A). Fig. 11(A) is a section view showing the configuration of another radiation detector. Fig. 11(B) is a rear view showing the configuration of the radiation detector of Fig. 11(A). Fig.12(A) is a longitudinal section view showing the configuration of another radiation detector. Fig.12(B) is a rear view showing the configuration of the radiation detector of Fig. 12(A). Fig. 13(A) is a longitudinal section view showing the configuration of a radiation detector of an embodiment of the invention. Fig. 13(B) is a rear view showing the configuration of the radiation detector of Fig. 13(A). Fig.14(A) is a longitudinal section view showing the configuration of a radiation detector of an embodiment of the invention. Fig.14(B) is a perspective view showing the configuration of the radiation detector of Fig. 14(A). Fig.15(A) is a longitudinal section view showing the configuration of a radiation detector of an embodiment of the invention. Fig.15(B) is a front view showing the configuration of the radiation detector of Fig. 15(A). Fig.15(C) is a perspective view showing the configuration of the radiation detector of Fig. 15(A). Fig.16(A) is a longitudinal section view showing the configuration of a radiation detector of an embodiment of the invention. Fig.16(B) is a front view showing the configuration of the radiation detector of Fig. 16(A). Fig.16(C) is a perspective view showing the configuration of the radiation detector of Fig. 16(A). Fig.17(A) is a longitudinal section view showing the configuration of a radiation detector of an embodiment of the invention. Fig.17(B) is a perspective view showing the configuration of the radiation detector of Fig. 17(A). Fig.18(A) is a longitudinal section view showing the configuration of a radiation detector of an embodiment of the invention. Fig.18(B) is a perspective view showing the configuration of the radiation detector of Fig. 18(A). Hereinafter, an embodiment of the invention will be described with reference to the drawings. Fig. 1(A) is a longitudinal section view, Fig. 1(B) is a rear view from the back side of the Fig. 1(A), and Fig.1(C) is a perspective view. In the figure, radiation 2 which enters through an incident aperture 1 in which an opening has a diameter 1 of about 10 mm enters a radiation absorbing layer 4 made of gold black and deposited on the inner face of a pyroelectric element 3 which has a conic shape and is made of PVF 2 (polyvinylidene fluoride). The apex angle 1 of the conic shape is 30°. A portion of the light is absorbed, and the remaining portion of the light is reflected to again enter the gold black radiation absorbing layer 4. This process is repeated so that the radiation 2 is fully absorbed by the gold black radiation absorbing layer 4. When the spectral reflectance of the radiation absorbing layer is indicated by γ ( λ ) and when the repetition of the number of reflections and absorptions of the radiation in the cone which enters in a direction perpendicular to the opening of the cone is indicated by n, the effective absorption factor α ( λ ) is given by the following expression: equation 1: α ( λ ) = 1 - γ ( λ ) n When the gold black radiation absorbing layer 4 having a spectral reflectance γ ( λ ) < 0.1 is applied to the inside of a cone having a apex angle 1 of 30°, and N = 6, α ( λ ) < 0.9999999 or the effective absorption factor α ( λ ) is 99.99999 %. In other words, the wavelength dependence of the responsivity is eliminated. Fig.7 shows such operation. The pyroelectric element 3 has electrodes which are formed by depositing aluminum on both faces of a film having a thickness of 9 µm, and is flexible. The pyroelectric element 3 is fixed by support plates 5 so as to have a conic shape. The support plates 5 are fixed to the incident aperture 1. Specifically, the pyroelectric element 3 is first cut into a fan shape. The support plates 5, made of an electrical and thermal insulating resin or ceramics which is excellent in electrical and thermal insulating properties, are adhered to both ends of the fan shape from the pivot to the peripheral portion, respectively. The radiation absorbing layer 4 is formed by evaporating gold in an atmosphere of a nitrogen gas pressure of 1,3 to 2,7 mbar (1 to 2 torr) while making the pyroelectric element 3 flat. When a film of gold black is formed so as to have a thickness of about 10 µm, it is possible to obtain a radiation absorbing layer 4 that has an excellent heat conductivity. In the embodiment, gold black was attached as the radiation absorbing layer 4 to the surface of the pyroelectric element 3. Alternatively, metal black formed by evaporating another metal may be attached, or a black coating composition may be attached. After the gold black is formed as described above, the support plates 5 at the both ends of the pyroelectric element 3 were bonded to each other so that a cone is formed with the radiation absorbing layer 4 positioned inside the cone. Ends of the support plates 5 of the pyroelectric element formed into a conic shape are fixed to the incident aperture 1, thereby constituting the radiation detector shown in Fig. 1. The reference numeral 15 designates an auxiliary support plate which cooperates with the support plates 5 and supplementally fixes the pyroelectric element 3 to the incident aperture 1. The electrodes of the pyroelectric element 3 are not shown in the figure. The measurement of radiation is conducted in the following manner. The radiation 2 modulated by an optical chopper or the like enters the radiation detector through the incident aperture 1. An electric output of the pyroelectric element 3 due to the light is detected in synchronization with the modulation frequency by a lock-in amplifier (not shown) having a high input impedance. The lock-in amplifier can attain a sensitivity of 1 µ V/( µ W/cm 2 ) or higher when the input impedance is 10 MΩ and the modulation frequency is 18.5 Hz. The sensitivity of the pyroelectric element is inversely proportional to the modulation frequency. When the modulation frequency is lowered to about 2 Hz, therefore, it is possible to obtain a radiation detector having a high sensitivity which is about 20 times that of a conventional thermal type (thermopile) radiation detector having the same opening area and light receiving area as incident aperture 1. The radiation absorbing layer 4 repeatedly captures reflected radiation components of the radiation 2. Therefore, the wavelength dependence on sensitivity is eliminated. As described above, according to the embodiment, a radiation detector of a thermal type can be realized in which the pyroelectric element to be used has a film-like shape and hence the radiation detector can easily be produced, and which can conduct the measurement at ordinary temperature, has a spectral responsivity not depending on the wavelength, and can obtain a stable output. In the radiation detector of Fig.2 the pyroelectric element 3 has the shape of a triangular prism. Fig. 2(A) is a longitudinal section view. Fig. 2(B) is a rear view illustrating the back side of Fig. 2(A), and Fig. 2(C) is a perspective view. By using such a polyhedral shape, the radiation absorbing layer 4 repeatedly captures reflected radiation components of the radiation 2. Therefore, the wavelength dependence of the sensitivity is eliminated. In the radiation detector of Fig.3 the pyroelectric element 3 has the shape of a four sided pyramidal shape. Fig. 3(A) is a longitudinal section view, Fig. 3(B) is a rear view illustrating the back side of Fig. 3(A), and Fig. 3(C) is a perspective view. By using such a pyramidal shape, the radiation absorbing layer 4 repeatedly captures reflected radiation components of the radiation 2. Therefore, the wavelength dependence of the sensitivity is eliminated. In the radiation detector of Fig.4 the aperture from the detector of Fig.1 is eliminated. Fig.4 is a longitudinal section view, Fig.4(B) is a rear view from the back side of Fig.4(A), and Fig.4(C) is a perspective view. By such a detector having no aperture, the radiation absorbing layer 4 repeatedly captures reflected radiation components of the radiation 2. Therefore, the wavelength dependence of the sensitivity is eliminated. The cone structure of the embodiment of Fig. 1 may be configured by using two pyroelectric elements. The pyroelectric elements are electrically connected in series so that the polarities of pyroelectric polarization are aligned in one direction, thereby reducing the electric time constant. Fig. 5 is a view showing this configuration. Fig. 5(A) is a section view, and Fig. 5(B) is a rear view . Fig. 6 is a diagram of the electrical connection of the two pyroelectric elements 3,3. In Fig. 5, 21 designates a first pyroelectric element which has a film-like shape. Support plates 23 made of a plate-like electrical and thermal insulating resin are adhered to both ends of the pyroelectric fan shaped element from the pivot to the peripheral portion. Furthermore, 22 designates a second pyroelectric element which has a film-like shape. Similarly, support plates 24 are adhered to the both ends of this pyroelectric fan shaped element 22 also. In the same manner as the embodiment of Fig. 1, a black coating composition or gold black is attached as a radiation absorbing layer 4 to one face of each of the first and second pyroelectric elements 21 and 22. The support plates 23 and 24 fixed to the ends of the first and second pyroelectric elements 21 and 22 are adhered to each other so that the radiation absorbing layer 4 is positioned inside, and the first and second pyroelectric elements 21 and 22 are bent and then attached to each other in the form of a conic shape. As shown in Fig. 6, the first and second pyroelectric elements 21 and 22 are connected in series by wires so that the polarities of pyroelectric polarization are aligned in one direction, thereby forming a configuration in which radiation 2 entering through the bottom opening of the cone, formed by the first and second pyroelectric elements 21 and 22, is converted into an electric signal and the energy amount of the radiation is detected. In Fig. 6, the arrangement of the pyroelectric elements 21 and 22 is shown in a deformed manner for easier understanding of the description. The operation of the thus configured embodiment will be described. Because the pyroelectric element responds to a differential amount, namely a variation of the temparature of the element, the pyroelectric element detects light which is modulated by a chopper or the like. When the modulation frequency is indicated by ω , R indicates a combined resistance of the internal resistances of the pyroelectric elements and an input resistance of a preamplifier 6 for connecting the elements, C indicates a combined capacitance of the internal capacitances of the pyroelectric elements and an input capacitance of the preamplifier 6 for connecting the elements, S indicates the area of the opening of the cone, S' indicates the area of the light receiving element or the internal area of the cone, P indicates the pyroelectric coefficient of the pyroelectric elements, G indicates the thermal conductance of the elements with respect to the surrounding, H indicates the thermal capacitance of the pyroelectric elements, the thermal time constant of the elements is indicated by τ T (= H/G), and the electrical time constant of the elements is indicated by τ E (= CR), the responsivity of the pyroelectric elements can be expressed by the following expression: equation 2 : R V = η ω RSS'P/G . (1+ω 2 τ T 2 ) -1/2 (1+ω 2 τ E 2 ) -1/2 When ω > 1/τ E , therefore, the sensitivity R V of the pyroelectric elements is larger as the frequency is higher. When 1/τ E > ω > 1/τ T , the sensitivity of the pyroelectric elements is constant irrespective of the frequency. When 1/ τ T > ω , the sensitivity of the pyroelectric elements is increased in proportion to the reduction of the frequency. When input radiation is modulated at 18.5 Hz and radiation detection is conducted by using an amplifier having an input impedance R = 10 8 Ω, the thermal time constant τ T of the elements is 1 sec. or longer, and the electrical time constant τ E is 15 msec. or longer. In this case, ω > 1/ τ T and 1/ τ E , and therefore the following relationship holds: equation 3: R V = η SP/ ω C V dC where C V is the volume specific heat of the elements and d is the thickness of the elements, and the following holds: equation 4: τ T = C V . S' . d . G From the above, it will be seen that, when the diameter  1 of the opening is set to be constant or 10 mm or in other words the opening area S' is constant, the sensitivity of the detector is inversely proportional to the capacity C of the elements. Actually, the sensitivity of the detector was measured as shown in Table 1 while the element area or the element capacitance was varied by changing the apex angle (opening angle) while keeping the opening area constant, as listed in the table below. In the detector having a apex angle of 90° , the repetition number of reflections and absorptions is 2. Therefore, this apex angle is the limit of attaining the repeated reflection and absorption effect. In the case where the opening area is constant, the detector having a apex angle of 90° shows the smallest element capacitance and attains the highest sensitivity. SHAPE AND SIZE OF A CONIC RADIATION DETECTOR OF A THERMAL TYPE (DESIGNED VALUE) APEX ANGLE OF 30°C APEX ANGLE OF 45°C APEX ANGLE OF 60°C APEX ANGLE OF 90°C FLAT TYPE LENGTH OF OBLIQUE LINE 19mm 13mm 10mm 7mm - DEPOSIT AREA OF GOLD BLACK 299mm 2 204mm 2 157mm 2 109mm 2 79mm 2 (10mm⊘) ELECTRODE AREA OF PYROELECTRIC ELEMENT 320mm 2 236mm 2 190mm 2 143mm 2 113mm 2 (12mm⊘) CAPACITANCE C P OF PYROELECTRIC ELEMENT 3510pF 2590pF 2085pF 1570pF 1240pF REPETITION NUMBER OF REFLECTION 6 4 3 2 1 (INCIDENT OPENING AREA 10 MM⊘) Fig.7 shows the internal reflection model of a conic shape having various apex angles. In order to check the repeated reflection and absorption effect in a cone, detectors in which gold black of a thickness of 4 µm was deposited in an atmosphere of a nitrogen gas pressure of 2 mbar (1.5 torr) were produced and the effective reflectance was measured while changing the apex angle. As shown in Fig.8, even in the detector having a apex angle of 90° in which the repetition number of reflections and absorptions is 2, the reflectance is improved to 0.7 % or less while the reflectance of the detector of flat gold black was 8 % or less. In other words, radiation can be absorbed with 99.4 % or more. Fig.9 shows sensitivities which were measured while the element area or the element capacitance was varied by changing the apex angle (opening angle) while the opening area remained constant. As seen from the above, the radiation detector of the embodiment has a capacitance which is one-half that of the radiation detector of the embodiment of Fig.1 , and therefore the sensitivity is improved to be doubled. In the radiation detector of Fig.10 the pyroelectric element 3 has a shape which is obtained by dividing a conic shape, in a direction perpendicular to an axial direction, into two portions. Fig. 10(A) is a longitudinal section view, and Fig. 10(B) is a rear view from the back side of Fig. 10(A). The shape can be selected from different shapes, such as a truncated conic shape, a pyramidal shape, or a truncated pyramidal shape. And the number of the divisions is not limited to two, that is, it can be three or more . The cone structure of the embodiment of Fig. 1 may be configured by a semiconic pyroelectric element to which a radiation absorbing layer is applied, and a semiconic mirror which has the same shape as the element, so that light entering the semiconic mirror is reflected toward the semiconic pyroelectric element, thereby detecting the radiation. Fig. 11(A) is a longitudinal section view, and Fig. 11(B) is a rear view from the back side of Fig. 11(A). As shown in Fig. 11, 41 designates a semiconic pyroelectric element in which a radiation absorbing layer is attached to the inner face in the same manner as the embodiment of Fig. 2 , and 42 designates a semiconic mirror in which the inner face is a mirror face. The semiconic mirror 42 may have any configuration as long as the inner face can reflect light. The reference numerals 43 and 44 designate support plates respectively fixed to the ends of the semiconic pyroelectric element 41 and the semiconic mirror 42. The support plates 43 and 44 are adhered to each other so that the radiation absorbing layer is positioned inside and the semiconic pyroelectric element 41 and the semiconic mirror 42 form a conic shape. The ends of the support plates are fixed to the incident aperture 1, thereby constituting the radiation detector. The operation of the thus configured embodiment will be described. Among the radiation which enters the opening of the bottom face of the cone formed by the semiconic pyroelectric element 41 and the semiconic mirror 42, light directly entering the radiation absorbing layer is absorbed as it is by the radiation absorbing layer in the form of heat, and light entering the semiconic mirror 42 is reflected therefrom to indirectly enter the radiation absorbing layer. The result is that the radiation absorbing layer absorbs the direct light and the indirect light and the pyroelectric element converts the temperature rise into an electric signal, thereby detecting the energy amount of the radiation. As seen from the above, according to this embodiment, the radiation entering the unit area of the radiation absorbing layer which functions as a light receiving face is doubled, and hence it is possible to realize a radiation detector having an S/N ratio which is twice that of the radiation detector of the embodiment of Fig. 1. In the embodiment, the semiconic pyroelectric element 41 and the semiconic mirror 42 are formed so as to be a semiconic shape which is obtained by dividing a cone in the axial direction into two laterally-separated portions . Alternatively, a cone may be divided in a direction perpendicular to the axial direction into front and rear portions as shown in Figs. 12(A) and 12(B). In this alternative, the portion which is closer to the incident aperture 1 may be formed as the mirror portion, and the remaining portion as the pyroelectric element in which a radiation absorbing layer is attached to the inner face. According to the alternative, radiation is converged by the mirror to the radiation absorbing layer. Hereinafter, an embodiment of the invention will be described with reference to the drawings of Figs. 13(A) and 13(B). In Figs. 13(A) and 13(B) 51 designates an incident aperture, 52 designates radiation, 53 designates a conic pyroelectric element in which a black coating composition or gold black is attached as a radiation absorbing layer 54 on one face, and 55 designates two support plates which are made of an electrical and thermal insulating resin and respectively adhered to the both ends of the film-like pyroelectric fan shaped element from the pivot of the fan shape to the peripheral portion. The support plates 55 are adhered to each other so that the radiation absorbing layer 54 is positioned on the outside, and the pyroelectric element 53 forms a conic shape. The reference numeral 56 designates a mirror barrel which is disposed so as to cover the conic structure of the pyroelectric element, and 57 designates a mirror face which is formed on a face of the incident aperture 51 in the side of the mirror barrel 56. The incident aperture 51 is disposed at a position opposed to the pyroelectric element 53 across the mirror barrel 56. Radiation entering through the incident aperture 51 is incident on the radiation absorbing layer 54, and a radiation component reflected therefrom is reflected from the mirror barrel 56 and the mirror face 57 of the incident aperture 51 to again enter the radiation absorbing layer 54. This process is repeated so that all of the incident radiation 52 is absorbed by the radiation absorbing layer 54 in the form of heat. The temperature rise is converted by the pyroelectric element 53 into an electric signal, thereby detecting the energy amount of the radiation. In other words, the configuration of this embodiment is characterized as follows: the configuration of the embodiment of Fig. 1 is modified so that the radiation absorbing layer 4 is positioned outside the cone formed by the pyroelectric element 3, that the mirror barrel and the incident aperture 51 are disposed so as to cover the radiation absorbing layer 4, and that the face of the incident aperture 51 which opposes the pyroelectric element 53 is formed as the mirror face 57. In the embodiment, therefore, radiation entering through the incident aperture 51 is incident on the radiation absorbing layer 54, and a radiation component reflected therefrom is reflected from the mirror barrel 56 and the mirror face 57 of the incident aperture 51 to again enter the radiation absorbing layer 54. This process is repeated so that the incident radiation 52 is absorbed by the radiation absorbing layer 54 in the form of heat. The temperature rise is converted by the pyroelectric element 53 into an electric signal, thereby detecting the energy amount of the radiation. In the same manner as the embodiment of Fig. 1 , therefore, a high-sensitivity radiation detector in which the wavelength dependence of the sensitivity is eliminated can be obtained. Further the radiation detector of Figs. 14(A) and 14(B) is an embodiment of the present invention and the second pyroelectric element 53' is provided instead of the tubular mirror 56 of the embodiment of Fig. 13. Fig. 14(A) is a longitudinal section view, and Fig. 14(B) is a perspective view. The wavelength dependence of the sensitivity is eliminated. Further the radiation detector of Figs. 15(A), (B) and (C) is an embodiment of the present invention where the aperture present in the embodiment of Fig. 13 is eliminated. Fig. 15(A) is a longitudinal section view, Fig. 15(B) is a front view, and Fig. 15(C) is a perspective view. The wavelength dependence of the sensitivity is eliminated. Further the radiation detector of Figs.16(A), (B) and (C) is an embodiment of the present invention where the pyroelectric element 53 has a shape which is obtained by dividing the pyroelectric element 53 of the embodiment of Fig.15. Fig. 16(A) is a longitudinal section view, Fig. 16(B) is a front view, and Fig. 16(C) is a perspective view. The wavelength dependence of the sensitivity is eliminated. Further the radiation detector of Figs. 17(A) and (B) is an embodiment of the present invention were the tubular mirror 56 has a truncated conic shape instead of the shape of the tubular mirror of Fig.15. Fig. 17(A) is a longitudinal section view, and Fig. 17(B) is a perspective view. The wavelength dependence of the sensitivity is eliminated. Further the radiation detector of Figs. 18(A) and (B) is an embodiment of the present invention where the shape of the pyroelectric element 53 is also the truncated conic shape instead of the pyroelectric element 53 of Fig.17. Fig. 18(A) is a longitudinal section view, and Fig. 18(B) is a perspective view. The wavelength dependence of the sensitivity is eliminated. In the invention, another radiation absorbing material such as NiP may be used in place of gold black. As described above, according to the invention, a high sensitivity which is 10 to 100 times that of a conventional thermal detector using a thermocouple is attained, the radiation detector can easily be produced without increasing the size of the apparatus, and the temperature drift of the sensitivity does not occur because the measurement is conducted while the pyroelectric element detects the modulated incident light . Consequently, it is possible to realize a radiation detector that has no output temperature drift at ordinary temperature, which is compact, and which has a high sensitivity not depending on the wavelength.

Claims: Radiation detector including a thermoelectric converting device, said thermoelectric converting device comprising: an opening, a flexible thermoelectric converting element having a conic shape, a truncated conic shape, a pyramidal shape, or a truncated pyramidal shape and an outer face; a radiation absorbing layer (54) attached to at least part of said outer face of said at least one flexible thermoelectric converting element, said flexible thermoelectric converting element supporting said radiation absorbing layer in a shape consistent with said flexible thermoelectric converting element, wherein said radiation absorbing layer (54) absorbs light (52) to be measured which enters through said opening in a form of heat, and said at least one thermoelectric converting element converts a temperature rise into an electric signal thereby detecting an energy amount of the radiation (52), and a mirror barrel (56) having an inner face which houses said thermoelectric converting element (53), at least a part of said inner face being a mirror face, wherein radiation (52) entering said mirror barrel (56) enters into said radiation absorbing layer (54) or is reflected from said mirror barrel to enter said radiation absorbing layer (54). Radiation detector according to claim 1, comprising an aperture (51) formed in said opening which is in said mirror barrel (56), through which radiation is incident onto said radiation absorbing layer. Radiation detector according to claim 1, wherein said mirror barrel (56) has a truncated conic shape, or a truncated pyramidal shape, and a portion of said mirror barrel at a side where radiation (52) enters has a tapered shape. Radiation detector including a thermoelectric converting device, said thermoelectric converting device comprising: an opening, a first flexible thermoelectric converting element (53) having a conic shape, truncated conic shape, a pyramidal shape, or a truncated pyramidal shape and an outer face; a second thermoelectric converting element (53') having a tubular form housing said first thermoelectric converting element, said second thermoelectric converting element having an inner face and an opening; and a first radiation absorbing layer (54) attached to at least a part of said outer face of said first thermoelectric converting element (53), said first thermoelectric converting element supporting said first radiation absorbing layer in a shape consistent with said first thermoelectric converting element, wherein said first radiation absorbing layer (54) absorbs light (52) to be measured which enters through said opening in a form of heat, and said first thermoelectric converting element converts a temperature rise into an electric signal thereby detecting an energy amount of the radiation (52), a second radiation absorbing layer attached to at least a part of said inner face of said second thermoelectric converting element (53'), said second thermoelectric converting element (53') supporting said second radiation absorbing layer in a shape consistent with said second thermoelectric converting element, respectively, wherein said second radiation absorbing layer absorbs light to be measured which enters through said opening in a form of heat, and said second thermoelectric converting element converts a temperature rise into an electric signal thereby detecting an energy amount of the radiation (52). Radiation detector according to claim 4, comprising an aperture (51) formed in said opening of said second thermoelectric converting element (53'), through which radiation is incident onto said radiation absorbing layers. Radiation detector according to one of the claims 4 and 5, wherein said second thermoelectric converting element (53') has a truncated conic shape, or a truncated pyramidal shape and a portion of said second thermoelectric converting element near said opening has a tapered shape. Radiation detector according to claim one of the preceding claims, comprising an electrically and thermally insulating member (5,43,44,55) supporting said at least one thermoelectric converting element (3,21,22,41,53,53') having said predetermined shape. Radiation detector according to one of the preceding claims, wherein said at least one thermoelectric converting element (3,21,22,41,53,53') comprises a pyroelectric film and said radiation absorbing layer (4,54) comprises metal black, black coating, or gold black.

Inventors: NAKAGAWA YASUO, OKUBO KAZUAKI, NAKAGAWA, YASUO, OKUBO, KAZUAKI
Applicants: MATSUSHITA ELECTRIC IND CO LTD, MATSUSHITA ELECTRIC INDUSTRIAL CO., LTD.
Application year: 1995
Main classification: G01J5
IPC codes: G01J5