Synchrotron radiation generation apparatus

Abstract: Synchrotron radiation is generated when a base of charged particles is bent by a bending magnet. The synchrotron radiation passes down a lead-out duct (3) as the total number of pumps is limited by the size of the apparatus and many pumps are needed in order to achieve a good vacuum. An ion pump (4) has a main magnetic field (13), normally generated by a magnet (12) of the ion pump (4) which controls the behaviour of the electrons in the ion pump (4). However, the leakage magnetic field (14) of the bending magnet effects the ion pump (4), and therefore the ion pump (4) is arranged so that its main magnetic field (13) is aligned with the leakage magnetic field (14) at the ion pump (4), or at least with a main component thereof. In this way, the effect of the leakage magnetic field (14) on the ion pump (4) is reduced. Indeed, it is possible to use the leakage magnetic field (14) as the main magnetic field of the ion pump (4).

Description: The present invention relates to an apparatus for generating synchrotron radiation, and also to a method of generating synchrotron radiation thereby, and a system involving such an apparatus. A storage ring is one example of a conventional synchrotron radiation generation apparatus (hereinafter SOR apparatus) for generating synchrotron radiation (hereinafter SOR radiation). In such a storage ring, a beam of charged particles such as electrons is caused to follow a looped path, under the influence of a series of bending magnets. Each bending magnet generates a bending magnetic field, which causes the beam to bend at that magnet. The path followed by the beam must be at very low pressure, and different types of vacuum pumps are used to achieve this. In the SOR apparatus described on pages 56 and 57 of the article "UVSOR Storage Ring" published by Science Research Institute (December 1982) the deflection region where the beam of charged particles is bent does not have any vacuum pumps other than an ion pump. Other types of pumps which may be necessary, such as titanium pumps, are positioned between the bending magents. This is because the conventional storage ring described in the above article is large, and there is plenty of space between the magnets for the pumps that are needed. A further type of SOR apparatus is disclosed in EP-A-0278504 (corresponding to US-A-4853640). The SOR apparatus disclosed is generally similar to Fig. 1 of the accompanying drawings, in which the path of the electron beam comprises two straight regions 10 ,11 extending generally parallel, with the ends of those straight regions 10,11 being joined by a semi-circular curved region 12,13. A single bending magnet (as shown in Fig. 1) is provided adjacent to the semi-circular regions 12,13 respectively, to cause the beam to be bent through the corresponding semi-circle. Two inflectors 14,15 are provided along one of the straight regions 11, and one of them (14) is connected via gate valves 16 to a turbo molecular pump 17. Further gate valves 18 and 19 are respectively connected to the two inflectors 14, 15. An RF cavity 20 is provided in the other of the straight regions 10 of the beam path, for accelerating the beam. Futhermore, at each point 21 along the path, there is provided a titanium getter pump and a turbo-molecular pump and at the points 22 are provided two titanium getter pumps. In the SOR apparatus shown in Fig. 1, each semi-circular region 12,13 has four synchrotron radiation ducts 23 extending therefrom. When a beam of charged particles, such as electrons, is caused to move in a curved path, such as round the semi-circular regions 12,13, synchrotron radiation is generated and this is caused to pass down the ducts 23. This will now be described in more detail with reference to Fig. 2 of the accompanying drawings. In Fig. 2, there is a beam duct 1 shaped to correspond to the semi-circular parts of the beam path 12,13 in Fig. 1. The core of a C-shaped bending magnet 2 surrounds the beam duct 1 so that the central axis of the beam duct 1 substantially corresponds to the centre of the magnetic field generated by the bending magnet 2. An SOR radiation lead-out duct 3 corresponds to the ducts 23 in Fig. 1, and SOR radiation is emitted from windows 3a on the outer peripheral side of the duct 1, in the plane of the beam duct 1 and in a tangential direction. The outer edge of the lead-out duct 3 is sealed by a gate valve 5 and a seal flange 6 and is connected to a radiation beam line 7 which carries the synchrotron radiation beam to a user thereof. An ion pump 4 is provided at the wall of the lead-out duct 3 between the outer frame of the core of the magnet 2 and the gate valve 5. A standard ion pump has field generation means for generating a magnetic field therein, and in the standard SOR apparatus, this field is aligned with the direction of elongation of the duct 3. Fig. 2 also shows that the electromagnet 2 generates a leakage field 14. The type of SOR apparatus shown in Figs. 1 and 2 was developed for industrial use. Standard SOR apparatuses have been for scientific study, and the size and cost thereof is not critical. However, in an SOR apparatus for industrial use, the size and cost becomes extremely important. Therefore, the arc of the beam duct, and the corresponding arc of the bending magnet for bending the beam, must be small, and therefore the field intensity of the magnetic field produced by the bending magnet must be large. Therefore, a superconductive electromagnet may be used. As the size of the storage ring increases, the space permitted for pumps, etc., decreases and therefore it is increasingly important that an ion pump is connected to the duct for the synchrotron radiation. This is because a decrease in the size of the path for the beam reduces the number of pumps that may be included within that path, and in order to provide a satisfactory degree of vacuum, pumps become necessary in the ducts. However, it has been appreciated by the inventors of the present application that the leakage magnetic field generated by the electromagnet may have an effect on the ion pump. In a standard ion pump, electrons are contained within a predetermined region by a main magnetic field, which is normally generated by suitable field generation means of the ion pump. The inventors of the present application have appreciated that the presence of the leakage magnetic field from the bending magnet will change the net direction of magnetic field within the ion pump, and this change in direction will reduce efficiency of the ion pump. Therefore, according to a first aspect of the present invention there is provided a synchrotron radiation generation apparatus comprising: a bending magnet for generating a bending field for a charged particle beam so as to bend said beam, the bending magnet also causing a leakage magnetic field to be generated; at least one duct for defining a path for synchrotron radiation generated by the bending of the beam; and an ion pump connected to the at least one duct; wherein: the ion pump is located and oriented in the leakage magnetic field so as to control the effect of said leakage magnetic field thereon such that the leakage magnetic field will not change substantially the net direction of the magnetic field in the ion pump, or will form the main magnetic field for the ion pump. Also, according to a second aspect of the invention there is provided a method of generating synchrotron radiation comprising: generating a bending magnetic field and a leakage magnetic field; causing a charged particle beam to bend due to the bending magnetic field, thereby to generate synchrotron radiation; and causing the synchrotron radiation to pass in a duct; wherein: an ion pump connected to the duct is located and oriented in the leakage magnetic field so as to control the effect of said leakage magnetic field thereon such that the leakage magnetic field will not change substantially the net direction of the magnetic field in the ion pump, or will form the main magnetic field for the ion pump. There are several ways that this can be done. The simplest is to align the magnetic field of the ion pump with the main (i.e. largest) component of the leakage magnetic field. In this way, only the smaller components of the leakage magnetic field influence the ion pump and normally these are sufficiently small to be neglected. Thus, for example, if the ion pump is located in a direction spaced perpendicularly from the plane of the arc of the bending magnet, the main component will be a radial one. On the other hand, if the ion pump is spaced from the duct in the plane of the arc of the bending magnet, then the main component will be perpendicular to that plane. Thus, the orientation of the magnetic field of the ion pump will depend on its location relative to the duct and bending magnet. In a further development, however, the vector composite direction of the leakage magnetic field is determined. If the main magnetic field of the ion pump is then aligned with that vector composite direction, the vector composite field will simply add to the magnetic field of the ion pump, and thus the performance of the ion pump will not be affected by the leakage magnetic field. This alignment of the magnetic field of the ion pump will thus cause that field to be angled relative to the direction of elongation of the duct for the synchrotron radiation. One known form of ion pump has one or more hollow cylindrical anodes which define a region for electrons. In this case, it is the direction of that anode axis relative to the leakage magnetic field that will be important. Another type of ion pump has one or more anode plates, with holes therein, and in this case the through axis of those holes will be aligned with the leakage magnetic field as discussed above. In a further development of the present invention, the ion pump may have shielding for shielding it from components of the leakage magnetic field other than the main component, or may be surrounded by shielding material. The appreciation that the leakage magnetic field will have an effect on the ion pump leads to a further feature of the present invention. As was mentioned above, standard ion pumps have some means for generating a main magnetic field therein. However, since an ion pump used in a synchrotron radiation generation apparatus will be located in a magnetic field (i.e. the leakage magnetic field), and it is therefore possible to use the leakage magnetic field itself as the magnetic field of the ion pump. Embodiments of the present invention will now be described in detail, by way of example, with reference to the accompanying drawings in which: Fig. 1 is a general schematic view of a known synchrotron radiation generation system, and has already been described; Fig. 2 shows in more detail a part of the known synchrotron radiation generation system of Fig. 1, and again has already been described; Fig. 3 shows one type of ion pump which may be used in the present invention; Fig. 4 is a plan view of a first embodiment of a synchrotron radiation apparatus according to the present invention; Fig. 5 is a side view of the embodiment of the present invention as shown in Fig. 1; Fig. 6 is a diagram for explaining the relationship between the leakage magnetic field and the orientation of an ion pump; Fig. 7 is a diagram for explaining the relationship between an anode of the ion pump and the vector composite magnetic field; Fig. 8 is a plan view of a second embodiment of the present invention; Fig. 9 is a side view of the second embodiment of the present invention shown in Fig. 7; and Fig. 9 shows one type of ion pump which may be used in the present invention; Fig. 10 shows another type of ion pump which may be used in the present invention. Before describing embodiments of the present invention in detail, it should be appreciated that the electron synchrotron frequency in a magnetic field is expressed by the following formula: f = Be 2πm where B is flux density; e is the charge on the electron; and m is the mass of the electron. Since the frequency f of the synchrotron radiation increases in proportion to the flux density B, an increase in that flux density B increases the number of times electrons interact with gas molecules to be removed from the synchrotron radiation duct, so that performance is improved if the flux density B is increased. Before describing a first embodiment of the present invention, a first ion pump which may be used in the present invention will be described with reference to Fig. 3. In Fig. 3 there is shown an ion pump having an ion pump case 8, which contains therein a large number of hollow anodes 9, and cathodes 10 are located on respective sides of the anodes 9. These anodes 9 and cathodes 10 are connected to a power source 11. A magnet 12 is fitted to the outside of the pump case 8 so that the axial direction of the hollow anode 9 corresponds to the direction of field 13 of the magnet 12 (the main magnetic field of the ion pump). The reason for this arrangement is as follows. Electrons move inside the hollow of the anodes 9 in the direction of the main magnetic field 13 of the ion pump. They interact with the main magnetic field 13 of the ion pump and move with electron synchrotron motion. However, they are retained within the anodes 9 by the electric field of the cathodes 10 at both ends. Thus, the electrons are entrapped within the hollow anodes 9 and form an electron cloud. When gas molecules to be exhausted by the ion pump pass into this electron cloud, they interact with the electrons and are ionized so that the ions are attracted by the electric field of the cathode 10 at the outlet of the anodes 9, thereby causing the pumping operation of the ion pump. So that the pumping operation operates in a satisfactory manner, therefore, it is important to entrap the electron cloud inside the anodes 9, and this is normally done by bringing the axial direction of the hollow anode 9 into conformity with the direction of the main magnetic field 13 of the ion pump. It can be appreciated that if an ion pump having the construction described above is located at an intermediate part of the lead-out duct 3 on the outer peripheral side of the bending magnet 1 in Fig.2., a leakage field exists due to the bending magnet. Therefore the leakage field of the bending magnet affects the ion pump and the electron cloud cannot be confined in the anodes 9 even through the axial direction of the hollow anodes 9 and the direction of the main magnetic field 13 of the ion pump are brought into conformity with each other. Thus, the pumping performance of the ion pump is reduced drastically and this tendency is particularly significant when the bending magnet is a superconductor electromagnet. Now, an embodiment of the present invention will now be described with reference to Figs. 4 and 5. The general arrangement of the synchrotron radiation generation apparatus of this embodiment is similar to that of the known arrangement shown in Fig. 2, and the same reference numerals are used to indicate corresponding components. Futhermore, it can be appreciated that the synchrotron radiation generation apparatus according to the present invention may be used in a synchrotron radiation generation system such as that shown in Fig. 1. Referring to Fig. 4, a deflection duct 1 for storing electrons is located in a superconductive bending magnet 2 and SOR radiation lead-out ducts 3 extend from the outer periphery of this deflection duct 1. Each duct 3 is connected to a corresponding SOR radiation beam line 7. An ion pump 4 is connected to each duct 3 on the outer peripheral side of the superconductive bending magnet 2 so as to branch from an intermediate part of the SOR radiation lead-out duct 3. In this embodiment each ion pump 4 is located in such a manner that the direction of the main magnetic field of the ion pump 4 substantially conforms with the main (i.e. largest) component of the leakage magnetic field 14 of the superconductive bending magnet 2. Moreover, the ion pump 4 is fitted so that it is positioned below the SOR radiation lead-out duct 3, as shown by Fig. 5. Substantial conformity of the direction of the main magnetic field of the ion pump 4 with the direction of the leakage magnetic field 14 of the superconductive bending magnet 2 means conformity of the axial direction of the hollow anodes (see Fig. 3) with the direction of the leakage magnetic field of the superconductive bending magnet 2 because the direction 13 of the magnetic field of the ion pump 4 is in comformity with the axial direction of the hollow anodes 9. Thus, the ion pump 4 is located so that the axial direction of the hollow anodes 9 is the same as the direction of the main component of the leakage magnetic field 14 of the superconductive bending magnet 2. If the ion pump 4 is of the type shown in Fig. 3, having a pump case 8 with cathodes 10 on both sides of the anodes 9 and a magnet 12 outside the ion pump case 8, the axial direction of the hollow anodes 9 or the direction of the magnetic field 13 of the magnet 12 is substantially in conformity with the direction of the main component of the leakage magnetic field 14. Fig. 5 shows a side view of the first embodiment. The leakage magnetic field 14 from the superconductive bending magnet 2 occurs from below to above as shown in the drawing and penetrates through the interior of the ion pump 4 with an inclination depending on the distance between the duct 3 and the ion pump 4 perpendicular to the plane of the arc of the bending magnet 1. The leakage magnetic field 14 has an inclination, because perpendicular components and tangential components exist in addition to the component of the magnetic field in the radial direction. The influence of these components will be discussed below using specific numerical values. Fig. 6 illustrates the relationship between the main field and leakage field components and of the ion pump 4. The component of the leakage flux density of the superconductor of the superconductor deflection electromagnet in the radial direction will be represented by B R , its component in the tangential direction by B T and its component in the prependicular direction, by B Z . Here, the ion pump is located on the outer periphery of the superconductor deflection electromagnet so that the main magnetic field 13 of the ion pump is in alignment with the direction of B R . According to an example investigated by the present inventors, the leakage field flux density acting on the center of an unshielded ion pump is given below: B R = 0.13T B T = 0.025T B Z = 0.04 T The main magnetic field B IP inherent to the ion pump is B IP = 0.12T The angle of inclination ϑ between the composite magnetic field 16 and the axis of the anode 9 shown in Fig. 6 can be calculated as follows by using the numerical values described above. ϑ = tan⁻¹ B T ²+B Z ² (B IP +B R )²+B T ²+B Z ² = tan⁻¹ 0.025²+0.04² (0.12+0.13)²+0.025²+0.04² = tan ⁻¹ 0.047 0.254 =10.5° According to the embodiment described above, the magnetic field inside the anodes 9 of the ion pump 4 can be increased from 0.12T to 0.254T by bringing the direction of the main magnetic field 13 of the ion pump 4 into conformity with the direction of the leakage magnetic field 14 of the superconductive bending magnet 2. Consequently, the electron synchrotron frequency f is increased to approximately double, so that there is a corresponding increase in ionization events in the gas to be exhausted and the pumping performance of the ion pump can be improved. On the other hand, the vector composite magnetic field 16 is inclined by ϑ = 10.5° with respect to the axis of the anodes 9 of the ion pump 4 due to the B T and BZ components. Accordingly, though the performance of the ion pump 4 is reduced by these components, a higher exhaust performance can still be obtained in comparison with the case where the pump is not aligned with the main component of the leakage magnetic field. Incidentally, reference numeral 17 in Fig. 7 represents electrons. Fig. 6 shows a structure wherein the ion pump 4 is further shielded by a magnetic material 15. The effect on the magnetic field due to this magnetic material 15 will now be examined. If a 12mm-thick steel sheet is put on the ion pump 4 on which the leakage magnetic field 14 from the bending magnet 2 acts, the magnitude of the leakage magnetic field acting on the center of the ion pump 4 is reduced as discussed below: B R = 0.035T B T = 0.0T B Z = 0.005T Similarly, the angle of inclination ϑ is given as follows: ϑ = tan⁻¹ 0.005 (0.12+0.035)²+0.005² = tan⁻¹ 0.005 0.155 = 1.8° As described above, according to the embodiment wherein the leakage magnetic field is added to the main magnetic field of the ion pump 4, the magnitude of the magnetic field inside the ion pump can be increased from 0.12T to 0.155T and the exhaust performance of the ion pump 4 can thus be improved. The inclination of the vector composite magnetic field in this case is as small as 1.8° and can be neglected. As a further alternative, the shielding 15 may be provided only so as to reduce the B T and B Z components of the leakage field. Figs. 8 and 9 show another embodiment of the present invention, wherein the ion pump 4 is located at the central horizontal position of the bending magnet 2 and to the side of the lead-out duct 3. In this case, too, the direction of the main magnetic field of the ion pump 4 and the direction of the main component of the leakage magnetic field 14 of the bending magnet 2 are substantially in conformity with each other. In the embodiment shown in Figs. 8 and 9, the position of the ion pump 4 is such that the main components of the magnetic field is vertical in Fig. 9, and then the radial component is small. The relative magnitudes of B R and B Z are thus changed, as compared with the numerical examples discussed above, but the resultant effect is similar if the main magnetic field 13 of ion pump 4 is aligned with B Z . In the above description, for both the first and second embodiments of the present invention, it has been stated that the main magnetic field 13 of the anodes 9, are aligned with the main component of the leakage field. However, also as described above, that leakage field at any point also may include other components in addition to the main (largest) one. If the main magnetic field 13 of the ion pump 4 is aligned with the main component, those other components reduce the performance of the ion pump 4, but this reduction in performance may be acceptable. However, in order further to improve the performance of the ion pump 4, it is possible for it to be orientated so that the main magnetic field 13 is aligned with the vector composite of the leakage magnetic field 14 at the location of the ion pump 4. Of course, this means that the vector composite direction must be determined, and although this is possible using standard techniques, it adds a further alignment step. In the first and second embodiment as described above, the main component of the leakage field corresponds to either the radial or vertical components of the field, so that it is easier to align the ion pump 4 relative to those radial or vertical directions. On the other hand, if the main magnetic field 13 of the ion 4 is aligned with the vector composite direction of the leakage magnetic field, the problem of the efect of components other than the main component is eliminated. Since the change in angle between the vector composite direction and the direction of the main component is small, the arrangement will be very close to that of Fig. 4 or 8. Fig. 10 shows another ion pump arrangement which may be used with the present invention as an alternative to the ion pump arrangement shown in Fig. 3. Apart from the anode structure, the ion pump 4 shown in Fig. 10 is generally similar to that shown in Fig. 3, and the same numerals are used to indicate corresponding parts. However, in the ion pump 4 shown in Fig. 10, the anodes are formed by anode plates 9a arranged between the cathode plates 10. Although only two anode plates 9a are shown in Fig. 10, there are normally more than this. The anode plates 9a have holes 9b therein, and these holes control the movement of electrons within the anodic region. As can be seen from Fig. 10, the axes of these holes 9b are aligned with the main magnetic field 13 of the ion pump 4, as generated by magnet 12. It was mentioned above that it is possible for the present invention to operate with the leakage magnetic field forming the main magnetic field for the ion pump. In this case, the magnet 12 in Figs. 3 and 10 is omitted, and the ion pump 4 is unshielded. Then, if the ion pump arrangement shown in Fig. 3 is used, the longitudinal axis of the cylindrical anodes 9 are aligned with the vector composite direction (or possibly the main components) of the leakage magnetic field. That leakage magnetic field then acts in exactly the same way as the main magnetic field 13. In a similar way, the ion pump arrangement shown in Fig. 10 is positioned so that the axes of the holes 9b of the anode plates 9a are aligned with the vector composite direction (or the direction of the main component) of the leakage magnetic field. Thus, the present invention proposes that the main magnetic field of an ion pump 4 is aligned with the leakage magnetic field (or a main component thereof). Alternatively, the leakage magnetic field may itself form the main magnetic field of the ion pump 4. Therefore, the effect of the leakage magnetic field on the performance of the ion pump is improved, as compared with known system in which the main magnetic field of the ion pump 4 was aligned with the direction of elongation of the corresponding lead-out duct 3. Thus, the ion pump 4 may operate in an efficient way, and this the present invention is particularly suitable for a small-sized radiation generation system.

Claims: A synchrotron radiation generation apparatus comprising: a bending magnet (2) for generating a bending field for a charged particle beam so as to bend said beam, the bending magnet also causing a leakage magnetic field (4) to be generated; at least one duct (3) for defining a path for synchrotron radiation generated by the bending of the beam; and an ion pump (4) connected to the at least one duct (3); characterised in that: the ion pump (4) is located and oriented in the leakage magnetic field so as to control the effect of said leakage magnetic field thereon such that the leakage magnetic field will not change substantially the net direction of the magnetic field in the ion pump (4), or will form the main magnetic field for the ion pump (4). An apparatus according to claim 1, wherein the ion pump has field generation means (12) for generating a main magnetic field (13) for the ion pump (4). An apparatus according to claim 2, wherein the ion pump (4) is arranged so that the main magnetic field (13) thereof is substantially aligned with a main component of the leakage magnetic field (4) at the location of the ion pump (4). An apparatus according to claim 2 or claim 3, wherein the bending magnet (2) is in the form of an arc, and the main component of the leakage magnetic field (14) is radial of the arc. An apparatus according to claim 4, wherein said ion pump is spaced from said duct (3) in a direction perpendicular to the plane of said arc. An apparatus according to claim 2 or claim 3, wherein the bending magnet (2) is in the form of an arc and the main component of the leakage magnetic field (14) is perpendicular to the arc. An apparatus according to claim 6, wherein said ion pump is spaced from said duct in a direction parallel to the plane of said arc. An apparatus according to any one of claims 1 to 6, wherein the main magnetic field of the pump (4) is aligned in a direction corresponding to the vector composite direction of the leakage magnetic field (14) at the ion pump (4). An apparatus according to any one of the preceding claims, wherein the main magnetic field of the ion pump (4) is aligned in a direction different from the direction of extension of the duct (3). An apparatus according to any one of the preceding claims, wherein the ion pump has at least one hollow cylindrical anode (9) for containing electrons therein. An apparatus according to claim 10, wherein the longitudinal axis of the at least one cylindrical anode (9) is substantially aligned with a main component of the leakage magnetic field (14) at the ion pump (4). An apparatus according to claim 10, wherein the longitudinal axis of the at least one cylindrical anode (9) is substantially aligned with the vector composite direction of the leakage magnetic field (14) at the ion pump (4). An apparatus according to claim 10, wherein the bending magnet (2) is in the form of an arc and the longitudinal axis of the at least one cylindrical anode (9) is substantially aligned with the radial direction of that arc. An apparatus according to claim 10, wherein the bending magnet (2) is in the form of an arc and the longitudinal axis of the at least one cylindrical anode (9) is substantially perpendicular to the plane of that arc. An apparatus according to claim 11, wherein the longitudinal axis of the at least one cylindrical anode (9) is aligned in a direction different from the direction of extension of the duct (3). An apparatus according to any one of claims 1 to 9, wherein the ion pump (4) has at least one anode plate (9a) having at least one hole (9b) therein. An apparatus according to claim 16, wherein the through axis of the at least one hole (9b) is substantially aligned with a main component of the leakage magnetic field (14) at the ion pump (4). An appratus according to claim 17, wherein the through axis of the at least one hole (9b) is substantially aligned with the vector composite direction of the leakage magnetic field (14) at the ion pump (4). An apparatus according to claim 18, wherein the bending magnet (2) is in the form of an arc, and the through axis of the at least one hole (9b) is substantially aligned with the radial direction of that arc. An apparatus according to claim 18, wherein the bending magnet is in the form of an arc and the through axis of the at least one hole is substantially perpendicular to the plane of that arc. An apparatus according to claim 18, wherein thethrough axis of the at least one hole is aligned in a direction different from the direction of elongation of the duct (3). An apparatus according to any one of the preceding claims wherein the ion pump (4) has shielding (15) for reducing at least other components than a main component of the leakage magnetic field. (14) An apparatus according to any one of the preceding claims wherein the ion pump (4) has a casing (15) of magnetic shielding material. An synchrotron radiation generation system having an apparatus according to any one of the preceding claims and at least one further bending magnet, the bending magnet and the at least one further bending magnet defining a looped path for the beam. A method of generating synchrotron radiation comprising: generating a bending magnetic field and a leakage magnetic field; causing a charged particle beam to bend due to the bending magnetic field, thereby to generate synchrotron radiation; and causing the synchrotron radiation to pass in a duct; characterised in that: an ion pump (4) connected to the duct is located and oriented in the leakage magnetic field so as to control the effect of said leakage magnetic field thereon such that the leakage magnetic field will not change substantially the net direction of the magnetic field in the ion pump, or will form the main magnetic field for the ion pump.

Inventors: HAYASAKA TOA, IKEGUCHI TAKASHI, KATANE MAMORU, KITAYAMA TOYOKI, KOBARI TOSHIAKI, MATSUMOTO MANABU, SONOBE TADASI, TAKAHASHI TAKAO, UEDA SHINJIRO, HAYASAKA, TOA, IKEGUCHI, TAKASHI, KATANE, MAMORU, KITAYAMA, TOYOKI, KOBARI, TOSHIAKI, MATSUMOTO, MANABU, SONOBE, TADASI, TAKAHASHI, TAKAO, UEDA, SHINJIRO
Applicants: HITACHI LTD, NIPPON TELEGRAPH & TELEPHONE, HITACHI, LTD., NIPPON TELEGRAPH AND TELEPHONE CORPORATION
Application year: 1990
Main classification: H05H7
IPC codes: H05H7, H01J41, H05H13