Photomultiplier

Abstract: An electron lens electrode (5) for guiding photoelectrons emitted from a photocathode (2) to an electron multiplier section is arranged between the photocathode and the light-incident portion of a sealed container, and an opening (15a) is formed at a portion of the electron lens electrode opposing the light-incident portion. Incident light reaches the photocathode through the opening without being scattered or absorbed at all. The transmittance of light incident on a photomultiplier is improved, and the output waveform is uniformed, resulting in an improved S/N ratio.

Description: The invention relates to a photomultiplier. More specifically the invention relates to a photomultiplier comprising: a sealed container having at least a portion which can transmit radiation, the container containing a photocathode, and an electron multiplier section, wherein in use radiation enters the container through the transmitting portion to be incident on the photocathode. Related Background Art Figs. 1 and 2 show a conventional photomultiplier. This photomultiplier is generally called a side-on type photomultiplier, and light as the measurement target is incident on the photomultiplier from the side surface of its glass bulb 1 which is a transparent sealed container. Upon incidence of the light, transmitted through the glass bulb 1, on the photoelectric surface of a reflection type photocathode 2, photoelectrons are emitted from the photoelectric surface and sent to an electronic multiplier section 3 constituted by a plurality of stages of dynodes 3a to 3d. The photoelectrons are sequentially multiplied by the electronic multiplier section 3, and the multiplied photoelectrons are collected as the output signal by an anode 4. In order to guide the photoelectrons emitted from the photocathode 2 to the first-stage dynode 3a, a grid electrode 6 is arranged between a light-incident portion 5 of the glass bulb 1 and the photocathode 2 and set to the same potential as that of the photocathode 2. Various types of grid electrodes 6 are available. For example, a thin conductor wire is arranged literally in a grid-like manner (not shown) to constitute a grid electrode 6, or as shown in Fig. 1, one thin conductor wire 6c is spirally wound on two support rods 6a and 6b to constitute a grid electrode 6. In the conventional photomultiplier as described above, since the grid electrode 6 is arranged in front of the photocathode 2, light incident on the photocathode 2 through the glass bulb 1 is partly scattered and absorbed by the conductor wire 6c of the grid electrode 6. Even if the incident light is uniform, the light does not partly reach the photocathode 2. In general, the grid electrode 6 has a transmittance of 75%. Hence, 25% of the light does not reach the photocathode 2. Fig. 3 is a graph showing the relationship between the position of a light spot formed and the output (relative value) of the anode 4 serving as the collector electrode when spot light is radiated as it is moved from an upper point a to a lower point b along the plane A - A of Fig. 1. Referring to Fig. 3, the output is not uniform. The position of a recess in the output corresponds to the position of the conductor wire 6c of the grid electrode 6. It is apparent that the transmittance is decreased at this position. As countermeasures against the problem of the decrease in transmittance, means disclosed in Japanese Patent Laid-Open Nos. 53-18864 and 55-29989 are known. As shown in Fig. 4, according to the means disclosed in Japanese Patent Laid-Open No. 53-18864, a glass plate 7 having a transparent conductor film formed on its surface is used in place of the grid electrode 6. When light is transmitted through a glass material, however, a loss occurs due to absorption or scattering. When the glass plate 7 is arranged in a glass bulb 1, light is transmitted through the glass material twice, doubling the loss. Another problem arises in manufacture. More specifically, in the conventional manufacturing process of a photocathode 2, an alkali metal for forming the photoelectric surface flows as indicated by broken lines in Fig. 4 to reach the photoelectric surface. When the glass plate 7 is arranged in the moving path of the alkali metal, the alkali metal cannot be uniformly guided, making it very difficult to form a uniform photoelectric surface. As shown in Fig. 5, according to the means disclosed in Japanese Patent Laid-Open No. 55-29989, although a grid electrode 6 is used, the grid density constituted by a conductor wire 6c of the grid electrode 6 is set high in a portion 6d close to a portion of the grid electrode 6 which is coupled to a photocathode 2 and low in a portion 6e through which most of the incident light is transmitted. When the grid density of the grid electrode 6 is set low only partly, although the transmittance is increased as compared to that obtained in the conventional arrangement shown in Fig. 1. But the conductor wire 6c of the grid electrode 6 still serves as an obstacle to decrease the transmittance, leaving the problem unsolved. Different transmittances in different portions of the grid electrode 6 mean different transmittances of light to be incident in different portions on the photocathode 2. This causes non-uniformity in the sensitivity of the photocathode 2. FR-A-1443279 describes a photomultiplier comprising a sealed container having at least a portion which can transmit radiation, the container containing a photocathode, and an electron multiplier section, wherein in use radiation enters the container through the transmitting portion to be incident on the photocathode. The present invention aims to improve the transmittance of light incident on a photomultiplier, and to make more uniform the output waveform, thereby improving the S/N ratio. According to the present invention, there is provided a photomultiplier comprising a sealed container having at least a portion which can transmit radiation, the container containing a photocathode, and an electron multiplier section, wherein in use radiation enters the container through the transmitting portion to be incident on the photocathode; characterised by: a transparent conductor portion formed on said transmitting portion of said sealed container. In a photomultiplier embodying the invention (to be described in detail hereinafter), there is provided a directing electrode, referred to herein as an electron lens electrode, arranged at a position adjacent to a first-stage dynode and opposing part of a light-incident portion, for guiding photoelectrons emitted from a photocathode to an electronic multiplier section. In the photomultiplier embodying the invention, as the opening is formed in the electron lens electrode arranged between the photocathode and the light-incident portion of the sealed container, light incident from the light-incident portion reaches the photocathode through the opening in the electron lens electrode. Accordingly, uniform incident light directly reaches the photocathode, and an output at an anode becomes uniform. It is apparent from experiments that it suffices if the electron lens electrode for guiding the photoelectrons by deflection is arranged between the photocathode and the light-incident portion of the sealed container and at a position at least adjacent to the first-stage dynode. Accordingly, by forming an opening in part of the electron lens electrode, or by causing the electron lens electrode to oppose only part of the light-incident portion the photoelectrons emitted from the photocathode are effectively guided to the electron multiplier section. When the electron lens electrode is arranged to oppose only part of the light-incident portion, light incident from other portions of the light-incident portion reaches the photocathode without being interfered at all. When an opening is formed in the photoelectron-deflecting electron lens electrode or the size of the electron lens electrode is decreased, some of the photoelectrons emitted from the photocathode may undesirably reach the light-incident portion of the sealed container to electrically charge this portion. Such electrical charging causes hysteresis in the photomultiplier output. When, however, a transparent conductor portion is formed on the inner or outer wall surface of the light-incident portion of the sealed container, the resistance in this portion on which the conductor portion is formed is decreased to prevent electrical charging, thereby preventing a hysteresis phenomenon. The present invention will become more fully understood from the detailed description given hereinbelow and the accompanying drawings which are given by way of illustration only, and thus are not to be considered as limiting the scope of the claims. Further scope of applicability of the present invention will become apparent from the detailed description given hereinafter. However, it should be understood that the detailed description and specific examples, while indicating preferred embodiments of the invention, are given by way of illustration only, since various changes and modifications within the scope of the claims will become apparent to those skilled in the art form this detailed description. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a front view showing a conventional photomultiplier; Fig. 2 is a sectional view taken along the line X - X of Fig. 1; Fig. 3 is a graph showing the relationship between the position of a light spot formed and the output when spot light is radiated on the photomultiplier of Fig. 2; Fig. 4 is a horizontally sectional view showing another arrangement of the conventional photomultiplier; Fig. 5 is a front view showing still another arrangement of the conventional photomultiplier; Fig. 6 is a front view showing a photomultiplier that is the subject of European Patent Application No. 93304015.6 from which this application is divided; Fig. 7 is a sectional view taken along the line II - II of Fig. 6; Figs. 8 to 10 are front views showing modifications of electron lens electrodes applicable to the photomultiplier embodying the present invention; Figs. 11 to 13 are front views showing other modifications of electron lens electrodes applicable to the photomultiplier embodying the present invention; Fig. 14 is a graph showing the relationship between the position of a light spot formed and the output when spot light is radiated on the photomultiplier of Fig. 6; and Fig. 15 is a horizontally sectional view showing a photomultiplier embodying the present invention in which a transparent conductor portion is formed. The preferred embodiments of the present invention will be described in detail with reference to the accompanying drawings. The same or corresponding portions as in the conventional arrangements described above are denoted by the same reference numerals, and upper and lower, and right and left sides referred to in the following description are based on the upper and lower, and right and left sides of the drawings. Figs. 6 and 7 show a so-called side-on type photomultiplier that is the subject of European Patent Application No. EP-A- 93304015.6 from which this application is divided. Referring to Figs. 6 and 7, reference numeral 1 denotes a translucent sealed container, more specifically, a transparent cylindrical glass bulb having closed upper and lower ends. Insulator plates 8a and 8b made of, e.g., a ceramic are provided in the upper and lower portions in the glass bulb 1. Various types of electrodes are supported by the insulator plates 8a and 8b. Terminals 10 extend to the outside from the bottom portion of the glass bulb 1 through a base 9. A photocathode 2, an electronic multiplier section 3, and an anode 4 are supported between the upper and lower insulator plates 8a and 8b. The photocathode 2 is inclined at a predetermined angle with respect to a light-incident portion 5 of the glass bulb 1. The electronic multiplier section 3 is constituted by a plurality of stages of dynodes 3a to 3d for sequentially multiplying the photoelectrons emitted from the photocathode 2. The anode 4 collects an output signal. An electrode (electron lens electrode) 11a, serving as an electron lens to cause the photoelectrons emitted from the photocathode 2 to be effectively incident on the first-stage dynode 3a, is arranged between the light-incident portion 5 of the glass bulb 1 and the photocathode 2. In this embodiment, the electron lens electrode 11a is welded to support rods 12a and 12b supported by the upper and lower insulator plates 8a and 8b. However, the electron lens electrode 11a may be directly supported by the insulator plates 8a and 8b without using the support rods 12a and 12b. The electron lens electrode 11a is a rectangular flat plate electrode. As shown in Fig. 6, a large rectangular opening 15a is formed in the central portion of the electron lens electrode 11a, i.e., in a portion of the electron lens electrode 11a opposing the light-incident portion 5. In Fig. 6, a portion 15b located on the left side of the opening 15a has a cell structure in which a large number of small parabolic holes are aligned in the vertical direction. A large number of small rectangular holes are formed in a portion 15C, located on the right side of the opening 15a, in the vertical direction. The potential of the electron lens electrode 11a is set to be the same as that of the photocathode 2, or is optimized as an electron lens. Hence, most of the photoelectrons emitted from the photocathode 2 are deflected by the electron lens electrode 11a and directed to the first-stage dynode 3a of the electronic multiplier section 3, as indicated by a broken arrow in Fig. 7. In order to cause the photoelectrons emitted from the photocathode 2 to be effectively incident on the first-stage dynode 3a, it suffices if an electrode having a certain width is arranged at a portion of the electron lens electrode 11a contacting the photocathode 2, and at a portion of the electron lens electrode 11a adjacent to the outer periphery of the first-stage dynode 3a. This is apparent from various experiments. Hence, it is preferable that the opening 15a of the electron lens electrode 11a is set as large as possible while leaving electrode portions sufficient for not disturbing the path of the photoelectrons. From this point of view, the electron lens electrode 11a can be of various other shapes, in addition to that shown in Figs. 6 and 7. For example, in an electron lens electrode 11a shown in Fig. 8, a left cell structure portion 15b is constituted by small rectangular holes, in the same manner as a right cell structure portion 15c. As shown in Fig. 9, right and left cell structure portions 15c and 15b may have honeycomb structures. As shown in Fig. 10, right and left cell structure portions 15c and 15b may be flat plates having no holes. Furthermore, as shown in each of Figs. 11 to 13, a left portion 15b may be narrowed to a width sufficient for being welded to a support rod 12a in order to enlarge an opening 15a. In this case, the left,portion 15b does not include a cell structure. Regarding an electron lens electrode 11a shown in each of Figs. 11 to 13, its function of deflecting photoelectrons depends substantially only on its right portion 15c. Hence, it is obvious that an electron lens electrode having an operation substantially the same as those shown in Figs. 11 to 13 can be obtained even if its upper and lower portions 15d and 15e and its left portion 11b are removed. In this manner, with the use of the electron lens electrode 11a having the opening 15a, or the narrow electron lens electrode 11b or 11c arranged only on the side of the first-stage dynode 3a, a portion of the glass bulb 1 opposing the light-incident portion 5 is widely opened. Then, light incident through the light-incident portion 5 directly reaches the photocathode 2 without being scattered or absorbed. For example, when spot light is radiated from the point a to point b along the plane A - A of Fig. 6, the waveform of an output signal derived from the anode 4 is uniform, as shown in Fig. 16. In this manner, as the uniformity of the output signal is maintained and a loss in light is eliminated in the electron lens electrode 11a, 11b, or 11c, the S/N ratio of the photomultiplier is improved. The conventional grid electrode 6 shown in Fig. 1 also has a function of improving the hysteresis characteristics, in addition to the function as the electron lens. Hysteresis is a phenomenon in which when pulse light is incident on a photomultiplier, an output signal does not rise immediately but rises gradually and is stabilized. It is supposed that when the hysteresis occurs, photoelectrons emitted from the photocathode 2 collide against the light-incident portion 5 of the glass bulb 1 to electrically charge this portion, and the potential of this portion becomes unstable to adversely affect the path of the photoelectrons. In the conventional grid electrode 6, the conductor wire 6c is arranged entirely in front of the photocathode 2 to shield the photoelectrons emitted from the photocathode 2 toward the light-incident portion 5. In a photomultiplier embodying the present invention, however, since the large opening 15a is formed in the electron lens electrode 11a, the photoelectrons may partly reach the light-incident portion 5 of the glass bulb 1. In order to the prevent invention, a transparent conductor portion 13 is formed on the inner wall surface of the light-incident portion 5 of the glass bulb 1, as shown in Fig. 15. As the resistance of a portion of the light-incident portion 5 on which the conductor portion 13 is formed is decreased, even if the photoelectrons emitted from photocathode 2 reach the inner wall the surface of the glass bulb 1 through the opening 15a of the electron lens electrode 11a, this portion of the inner wall surface of the glass bulb 1 is not substantially charged. As a result, the potential of the light-incident portion 5 of the glass bulb 1 is stabilized to improve the hysteresis characteristics. The conductor portion 13 can be formed by various methods, and is preferably formed by depositing chromium on the inner wall surface of the glass bulb 1. Since a deposited chromium film has a high transmittance of 98%, a loss in light transmitted through the chromium film is very small. In order to prevent the light-incident portion 5 of the glass bulb 1 from being electrically charged, a transparent conductor portion 5 may be formed on the outer wall surface of the glass bulb 1 to obtain the same effect. From the invention thus described, it will be obvious that the invention may be varied in many ways. Such variations are not to be regarded as a departure from the scope of the following claims.

Claims: A photomultiplier comprising: a sealed container having at least a portion (5) which can transmit radiation, the container containing a photocathode (2), and an electron multiplier section (3), wherein in use radiation enters the container through the transmitting portion (5) to be incident on the photocathode (2); characterised by: a transparent conductor portion (13) formed on said transmitting portion (5) of said sealed container. A photomultiplier as claimed in claim 1, further comprising a directing electrode (11a) for directing electrons emitted from the photocathode to the electron multiplier section. A photomultiplier as claimed in claim 1 or 2, wherein said transparent conductor portion is formed on the inner surface of said transmitting portion of said sealed container. A photomultiplier as claimed in claim 1 or 2, wherein said transparent conductor portion is formed on the outer surface of said transmitting portion of said sealed container. A photomultiplier as claimed in any preceding claim, wherein said directing electrode (11a) is arranged at a position adjacent to a first-stage dynode, of said electron multiplier section (3), and opposing part of said transmitting portion (5).

Inventors: HASHIMOTO TAKEO, KUROYANAGI TOMIHIKO, NAKAMURA KIMITSUGU, WASHIYAMA HIROAKI, HASHIMOTO, TAKEO, KUROYANAGI, TOMIHIKO, NAKAMURA, KIMITSUGU, WASHIYAMA, HIROAKI
Applicants: HAMAMATSU PHOTONICS KK, HAMAMATSU PHOTONICS KABUSHIKI KAISHA
Application year: 1993
Main classification: H01J43
IPC codes: H01J43