1. Field of the Invention
The present invention relates to an electron multiplier unit enabling cascade multiplication of electrons through successive emission of secondary electrons in multiple steps in response to incidence of primary electrons, and to a photomultiplier including the same.
2. Related Background Art
The following conventional technologies are known as techniques prior to the electron multiplier unit and the photomultiplier including it according to the present invention.
Japanese Patent Application Laid-Open No. 7-245078
Japanese Patent Application Laid-Open No. 4-315758
WO98/33202
U.S. Pat. No. 5,914,561
The Inventor studied the above-cited conventional technologies and found the following problem.
Namely, the photomultipliers have been applied heretofore as photosensors in a variety of technical fields. Particularly, in application to detection of X-rays and radiated rays, it is necessary to shield the detector part including the photomultipliers, by a heavy metal such as Pb, and the total weight of apparatus depends on the weight of the heavy metal shield.
For example, a γ-camera device used as a medical inspection system is provided with at least a pair of upper and lower camera heads, and each camera head has a structure in which a plurality of photomultipliers are entirely covered by the Pb shield except for a detection window for exposing face plates of the photomultipliers arrayed in a two-dimensional pattern. The number of photomultipliers used has to increase for improvement in detection resolution, and, naturally, the increase of weight of the detector part including the heavy metal shield will pose an impediment to reduction of weight and size of apparatus.
Then the aforementioned Documents introduce the structure for decreasing the axial length (cylinder length) of the photomultipliers used, in order to reduce the gross weight of the heavy metal shield without degradation of detection resolution.
However, a new structure for further reduction of the cylinder length has been needed in order to satisfy the demand for improvement in detection resolution and the demand for reduction of total weight and size of apparatus together.
The present invention has been accomplished in order to solve the problem as discussed above, and an object of the invention is to provide an electron multiplier unit in a structure for enabling further reduction of the cylinder length, while achieving a high gain and maintaining or further improving the excellent fast response, and a photomultiplier including it.
An electron multiplier unit according to the present invention is an electronic component for effecting cascade multiplication of secondary electrons emitted in response to incidence of primary electrons, and is applicable to cascade multiplication structure of electron tubes, cascade multiplication structure of photomultipliers with a cathode for emitting photoelectrons as primary electrons upon acceptance of weak light of a predetermined wavelength, as well as X-rays and radiated rays, and so on.
An electron multiplier unit according to the present invention comprises a first support member provided with an inlet aperture for letting primary electrons in; a second support member located so as to face the first support member; and a first dynode, a second dynode, and an anode disposed in a space between the first and second support members. The first dynode is a dynode for receiving the primary electrons having passed through the inlet aperture of the first support member and for emitting secondary electrons, and has a reflection type secondary electron emission surface located so as to emit the secondary electrons into the space between these first and second support members, in a state in which it covers the inlet aperture of the first support member. The anode for capturing secondary electrons emitted into the space is located in the space between the first and second support members. However, this anode is disposed at a position where the secondary electrons emitted from the first dynode do not directly arrive. This is for the purpose of securing a sufficient installation area for the cascade multiplication structure of the secondary electrons on a secondary-electron travel path from the first dynode to the anode.
In particular, in the electron multiplier unit according to the present invention, the second dynode is a dynode provided for cascade multiplication of secondary electrons in the space between the first and second support members, and also functions as an electrode for changing the travel path of the secondary electrons. Namely, the second dynode has a reflection type secondary electron emission surface located so as to face the first dynode and arranged to emit new secondary electrons to the side where the first dynode is located, in response to the secondary electrons coming from the first dynode. This second dynode alters the travel path of the secondary electrons traveling from the first dynode toward the second dynode (secondary electrons traveling from the center of the unit to the outer periphery) so that it becomes parallel to the first and second support members. In other words, in the electron multiplier unit, the travel path of secondary electrons from the cathode toward the anode is corrected from the path along the radial direction from the center axis, into a path rotating around the center axis.
In the electron multiplier unit according to the present invention, a total length TL of the travel path of secondary electrons, i.e., an electron travel distance from the first dynode to the anode can be kept not less than two times, preferably four times, a distance D between the first support member and the second support member (a width of the space where the dynodes and others are located). By setting the cascade multiplication structure for obtaining an adequate gain, in the width D in this manner, it becomes feasible to further decrease the cylinder length of a photomultiplier tube to which the electron multiplier unit is applied.
The first support member preferably comprises a focusing electrode which surrounds at least a portion of the inlet aperture. This focusing electrode functions to alter trajectories of the photoelectrons, in order to guide the primary electrons (photoelectrons from the cathode in the case of a photomultiplier) to the inlet aperture provided in the first support member. The focusing electrode is a metal plate of trapezoidal shape cut in a tapered form at both ends, and is fixed to the first support member so that the lower base thereof extends along the outer periphery of the first support member.
The first support member may comprise an electrode piece one end of which is fixed to an edge part of the inlet aperture. This electrode piece extends so that the other end is located in a secondary-electron travel space between the first dynode and the second dynode (in the space between the first and second support members), in an assembled state of the electron multiplier unit, and the electrode piece functions as a control electrode (decelerating electrode) for directing the trajectories of the secondary electrons emitted from the first dynode, toward the second dynode.
In the electron multiplier unit according to the present invention, the inlet aperture provided in the first support member is preferably located so that a center of the inlet aperture deviates from a center of the first support member. In a photomultiplier to which the electron multiplier unit is applied, the center of the inlet aperture is located so as to deviate from a tube axis AX. This is for the purpose of efficiently housing the cascade multiplication structure, without increase in the diameter of the first support member or the tube cylinder.
Furthermore, the structure for cascade multiplication in the electron multiplier unit can be constructed of only box type dynodes, or of a combination of various types of dynodes. For example, the cascade multiplication structure from the second dynode to the anode, or the cascade multiplication structure from a third dynode to the anode may be replaced by grid type or mesh type dynodes. Normally, in the case of the mesh type dynodes, electrons pass through the mesh (η=40%), and it is thus necessary to use ten or more stages of dynodes in order to achieve an adequate gain. In contrast, the electron multiplier unit of the present invention involves preliminary multiplication of the secondary electrons emitted from the first dynode, by means of the second dynode or by means of the second and third dynodes, and thus it can achieve an adequate gain even by a dynode unit having a smaller number of stages.
A photomultiplier to which the electron multiplier unit having the structure as described above is applied (a photomultiplier according to the present invention) comprises a sealed envelope an interior of which is maintained in vacuum; a cathode provided in the sealed envelope; and the electron multiplier unit housed in the sealed envelope. The cathode releases photoelectrons as primary electrons into the sealed envelope, in response to incidence of light of a predetermined wavelength. The electron multiplier unit has the structure as described above and effects cascade multiplication of electrons by successively emitting secondary electrons in multiple steps in response to incidence of the photoelectrons released from the cathode.
In the photomultiplier having the structure as described above, the electron multiplier unit is one wherein an electron travel distance from the first dynode to the anode is kept not less than 1.5 times an electron travel distance from the cathode to the first dynode. An electron travel distance from the cathode to the anode is kept not less than 2 times the electron travel distance from the cathode to the first dynode.
Each of embodiments of the present invention will become further fully understandable in view of the detailed description given below and the accompanying drawings. It should be noted that these embodiments will be presented merely for illustrative purposes, and are not to be considered as limiting the present invention.
Further scope of application of the present invention will become apparent from the detailed description given below. It is, however, noted that the detailed description and specific examples, while indicating preferred embodiments of the present invention, are presented for illustrative purposes only, and it is apparent that various modifications and improvements within the spirit and scope of the invention will be obvious to those skilled in the art in view of the detailed description.
Each of embodiments of the electron multiplier unit and the photomultiplier including it according to the present invention will be described below in detail with reference to
The photomultiplier 100A of the first embodiment has a sealed envelope or vessel the bottom part of which is provided with a pipe 132 (unhollowed after evacuation) for evacuating the interior, and has a cathode 110 and an electron multiplier unit 200A (a first embodiment of the electron multiplier unit according to the present invention) enclosed in the sealed envelope.
The sealed envelope is composed of a tube cylinder 100 of cylindrical shape having a face plate with the cathode 110 formed inside, and a stem 130 supporting a plurality of lead pins 131 in a penetrating state. The electron multiplier unit 200A is held at a predetermined position in the sealed envelope by the lead pins 131 extending from the stem 130 inside the sealed envelope.
The electron multiplier unit 200A, as shown in
As shown in
The first support member 210 has a three-layer structure composed of a metal disk 211 set at a predetermined potential, and ceramic disks 212, 213 each made of an insulating material.
The metal disk 211 has holes 211a, spring pieces 211b, and a focusing electrode 211c, in addition to the inlet aperture 300. The lead pins 131 are connected to the metal disk 211 in a state in which the tip thereof penetrates through the holes 211a. The spring pieces 211b are brought into contact with the inner wall of the tube cylinder 100 in order to stabilize the position of the whole of the electron multiplier unit 200A relative to the tube cylinder 100, particularly, the vertical position relative to the tube axis AX. The focusing electrode 211c functions to alter the trajectories of the photoelectrons, in order to guide the photoelectrons from the cathode 110 to the inlet aperture 300 provided in the first support member 210.
Each of ceramic disks 212, 213 is also provided with holes 212a or 213a for letting the lead pins 131 pass, in addition to the inlet aperture 300, and the ceramic disk 213 is further provided with engaging holes 213b for keeping the upper fixing pieces DY1a-DY7a, 410a, and DY8a of the respective members placed between the first and second support members 210, 220, between the ceramic disks 212, 213.
The second support member 220 is a ceramic disk made of an insulating material, and is provided with holes 220a for letting the lead pins 131 pass, and engaging holes 220b for accepting the lower fixing pieces DY1b-DY7b, 410b, and DY8b of the respective members placed between the first and second support members 210, 220. These lower fixing pieces DY1b-DY7b, 410b, and DY8b are electrically connected to the lead pins 131 each extending from the stem 130, whereby each of the members DY1-DY7, 410, and DY8 located between the first and second support members 210, 220 is set at a predetermined potential.
Some of the lead pins 131 extending from the stem 130 are electrically connected to the metal disk 211 via the holes 211a of the metal disk 211 in a state in which each passes through the hole 220a of the second support member 220, the ceramic pipe 230a-230c, and the holes 212a, 213a of the ceramic disks 212, 213.
As described above, the metal disk 211 has the holes 211a for electrically connecting the lead pins 131 extending from the stem 130, to the metal disk 211 in the state in which the pins penetrate the holes; the spring pieces 211b for stabilizing the installation position of the metal disk 211 itself; and the focusing electrode 211c for altering the trajectories of photoelectrons released from the cathode 110. Particularly, the focusing electrode 211c is a metal plate of trapezoidal shape cut in a tapered form at both ends, as shown in
The metal disk 211 further has an electrode piece 310 extending toward the interior of the inlet aperture 300. This electrode piece 310, in an assembled state of the electron multiplier unit 200A, has a part located in the secondary-electron travel space between the first dynode DY1 and the second dynode DY2, and functions as a control electrode (decelerating electrode) for directing the trajectories of secondary electrons emitted from the first dynode DY1, toward the second dynode DY2.
As also seen from this
As shown in this
On the other hand, the lower fixing pieces DY1b-DY7b, 410b, and DY8b of the first to seventh dynodes DY1-DY7, anode 410, and reflection type dynode DY8 each are electrically connected to the lead pins 131 extending from the stem 130, in a penetrating state through the holes 210b provided in the second support member 220. In this manner the electron multiplier unit 200A is supported by the lead pins 131 connected to the lower fixing pieces DY1b-DY7b, 410b, and DY8b of the members DY1-DY7, 410, and DY8 sandwiched between the first and second support members 210, 220.
Next, a specific positional relation of the dynodes in the electron multiplier unit 200A will be described.
Namely, the first to seventh dynodes DY1-DY7, anode 410, and reflection type dynode DY8 are placed in the space with the width D between the first and second support members 210, 220. The first dynode DY1 is held by the first and second support members 210, 220 in a state in which it covers the inlet aperture 300 of the first support member 210. The secondary electron emission surface of the first dynode DY1 is set to receive photoelectrons having passed through the inlet aperture 300 and to emit secondary electrons into the space between the first and second support members 210, 220. The anode 410 is located at a position where the secondary electrons emitted from this first dynode DY1 do not directly arrive. This is for the purpose of securing a sufficient installation area for the structure enabling the cascade multiplication of secondary electrons in the path from the first dynode DY1 to the anode 410. In the electron multiplier unit 200A, the second dynode DY2 performs correction for the main travel path of the secondary electrons, in order to achieve the cascade multiplication of secondary electrons in the space between the first and second support members 210, 220. Specifically, the second dynode DY2 is an electrode having a reflection type secondary electron emission surface arranged to face the first dynode DY1, and functions as a path changing electrode for receiving the secondary electrons from the first dynode DY1 and for changing the travel path of the secondary electrons into a direction different from the axial direction of the sealed envelope so as to emit the secondary electrons toward the third dynode DY3 arranged adjacent to the first dynode DY1. This second dynode DY2 alters the main travel path of secondary electrons from the first dynode DY1 to the second dynode DY2 (secondary electrons traveling in the radial direction from the tube axis AX), into the direction rotating around the tube axis AX (cf
The main travel path of secondary electrons means the shortest trajectory of secondary electrons from the first dynode DY1 to the anode 410, and is defined by connecting the center of the secondary electron emission surface in the first dynode DY1 to the center of the anode 410 via the centers of the secondary electron emission surfaces in the respective dynodes DY2-DY7 by a plurality of line segments.
Namely, since the dynodes applied to the electron multiplier unit 200A are box type dynodes DY, their secondary electron emission surface has the rectangular shape with the height DH and the width Dw, as shown in
The total length TL of the main travel path of secondary electrons defined as described above is thus a total of a travel distance L1 from the first dynode DY1 to the second dynode DY2, a travel distance L2 from the second dynode DY2 to the third dynode DY3, a travel distance L3 from the third dynode DY3 to the fourth dynode DY4, a travel distance L4 from the fourth dynode DY4 to the fifth dynode DY5, a travel distance L5 from the fifth dynode DY5 to the sixth dynode DY6, a travel distance L6 from the sixth dynode DY6 to the seventh dynode DY7, a travel distance L7 from the seventh dynode DY7 to the eighth dynode (inversion type dynode) DY8, and a travel distance L8 from the inversion type dynode DY8 to the anode 410, as shown in
Next, specific outer size ratios of the photomultiplier according to the present invention will be described.
The sample prepared as the photomultiplier according to the present invention is a photomultiplier with the sealed envelope 100 having the diameter of 51.6 mm and the cylinder length of 64.0 mm, as shown in
The Inventors calculated the electron travel distances as to several types of trajectories in the photomultiplier of this sample. Specifically, A in
As shown in the table of
As seen from the above calculation result, in the photomultiplier of the present invention the electron travel distance from the first dynode DY1 to the anode 410 is kept not less than 6 times the distance D (=13.5 mm) between the first support member 210 and the second support member 220. In addition, the electron travel distance from the first dynode DY1 to the anode 410 is kept not less than 1.5 times the electron travel distance from the cathode 110 to the first dynode DY1. Furthermore, the electron travel distance from the cathode 110 to the anode 410 is kept not less than 2 times the electron travel distance from the cathode 110 to the first dynode DY1.
As constructed in the above configuration, the photomultiplier 100A to which the electron multiplier unit 200A is applied has the structure capable of further reducing the tube length H, in comparison with those of the conventional photomultipliers (cf.
The photomultiplier 100A of the first embodiment described above has the structure in which the electron multiplier unit 200A (the first embodiment of the electron multiplier unit according to the present invention) is housed in the tube cylinder 100, but there are no particular restrictions on the shape of the vessel in which the electron multiplier unit 200A is housed. For example,
As shown in
Furthermore, the structure for cascade multiplication in the electron multiplier unit can also be realized without use of only the box type dynodes as described above. Namely, the cascade multiplication structure from the second dynode DY2 to the anode 410, or the cascade multiplication structure from the third dynode DY3 subsequent to the second dynode DY2, to the anode 410 may be replaced by grid type dynodes or mesh type dynodes. Normally, in the case of the mesh type dynodes, electrons pass through the mesh (η=40%), and it is thus necessary to use ten or more stages of dynodes in order to achieve an adequate gain. However, since the present invention involves the preliminary multiplication of secondary electrons emitted from the first dynode DY1, by the second dynode DY2 or by the second and third dynodes DY2, DY3, it can achieve an adequate gain even by the dynode unit having a smaller number of stages.
As shown in
Each of the focusing electrode plate 430 and the anode plate 410 is provided with an upper fixing piece 500a. Each of the focusing electrode plate 430, dynode plates 510, and anode plate is provided with a lower fixing piece 500b to be electrically connected to a lead pin 131 extending from the stem. Each dynode plate 510 is set at a predetermined potential through the lower fixing piece 500b.
As shown in
The first support member 210 has a three-layer structure composed of a metal disk 211 set at a predetermined potential; and ceramic disks 212, 213 each made of an insulating material.
The metal disk 211 has holes 211a, spring pieces 211b, and a focusing electrode 211c, in addition to the inlet aperture 300. The lead pins 131 are connected to the metal disk 211 in a state in which the tip thereof penetrates through the holes 211a. The spring pieces 211b are brought into contact with the inner wall of the tube cylinder 100 in order to stabilize the position of the whole of the electron multiplier unit 200B relative to the tube cylinder 100, particularly, the vertical position relative to the tube axis AX. The focusing electrode 211c functions to alter the trajectories of the photoelectrons, in order to guide the photoelectrons from the cathode 110 to the inlet aperture 300 provided in the first support member 210.
Each of the ceramic disks 212, 213 is also provided with holes 212a or 213a for letting the lead pins 131 pass, in addition to the inlet aperture 300, and the ceramic disk 213 is further provided with engaging holes 213b for keeping the upper fixing pieces DY1a, DY2a, and 500a placed between the first and second support members 210, 220, between the ceramic disks 212, 213.
The second support member 220 is a ceramic disk made of an insulating material, and is provided with holes 220a for letting the lead pins 131 pass, and engaging holes 220b for accepting the lower fixing pieces DY1, DY2b, and 500b of the respective members placed between the first and second support members 210, 220. These lower fixing pieces DY1, DY2b, and 500b are electrically connected to the lead pins 131 each extending from the stem 130, whereby each of the members DY1, DY2, and 500 located between the first and second support members 210, 220 is set at a predetermined potential.
Some of the lead pins 131 extending from the stem 130 are electrically connected to the metal disk 211 via the holes 211a of the metal disk 211 in a state in which each pin passes through the hole 220a of the second support member 220, the ceramic pipe 230a-230c, and the holes 212a, 213a of the ceramic disks 212, 213.
Namely, the aforementioned electron multiplier unit 200B (the electron multiplier unit of the second embodiment) is applied to the photomultiplier 100C of the third embodiment, as shown in
The photomultiplier 100D of the fourth embodiment has a structure in which the dynode unit 500 including the anode plate 410, together with the first dynode DY1, second dynode DY2, and third dynode DY3, is located in the space between the first and second support members 210, 220, as shown in
Normally, where the photomultipliers are applied to detection of X-rays or radiated rays, the photomultipliers are entirely covered except for a detection window by a heavy metal shield, e.g., Pb. For example, a γ-camera device used as a medical inspection system is provided with at least a pair of upper and lower camera heads, and each camera head is entirely covered except for a detection window for exposing face plates of photomultipliers 100A to 100D two-dimensionally arranged, by a Pb shield 600, as shown in
The face plates of the photomultipliers 100A-100D according to each of the aforementioned embodiments all are circular, but the face plates can be, for example, hexagonal as shown in
It is apparent that the present invention can be modified in various ways in view of the above description of the present invention. Such modifications are not to be regarded as departure from the spirit and scope of the present invention, but all improvements as would be obvious to those skilled in the art are intended for inclusion within the scope of the claims which follow.
This application claims the benefit of the provisional application No. 60/646,506 filed on Jan. 25, 2005 by the same Applicant, the entire disclosure of which is herein incorporated by reference.
Number | Date | Country | |
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60646506 | Jan 2005 | US |