Superconducting magnet device for crystal pulling device

Abstract: The present invention provides a superconducting magnet device for a crystal pulling device comprising a pair of ring-like superconducting coils (2a, 2b) facing with each other, with the crystal pulling device disposed therebetween, a radiation shield (42) surrounding the superconducting coils (2a, 2b), and a vessel (51) surrounding the radiation shield (42), wherein the vessel (51) on the side (55) facing to the crystal pulling device is made from a nonmagnetic substance (55), and the vessel (51) on the other side (52, 53, 56, 57, 58) is made from a magnetic substance.

Description: The present invention relates to a superconducting magnet device according to the preamble portion of claim 1 to be used in a crystal pulling device for generating a crystal for a semiconductor device, In pulling a crystal from a molten semiconductor crystal material with a pulling device for crystals for a semiconductor, a superconducting magnet device is used as a static magnetic field generating device for preventing the movement by the heat convection by applying the static magnetic field to the molten semiconductor crystal material. FIG. 1 is a perspective view showing a configuration of a conventional superconducting magnet device for a crystal pulling device. FIG. 2 is a cross-sectional view viewed from the direction shown by the arrows II-II of FIG. 1. As shown in FIG. 1, the superconducting magnet device is provided such that two superconducting coils 2a, 2b are arranged facing with each other in a C-shaped cryostat 1, and the magnetic field direction 3 generated by the superconducting coils 2a, 2b is orthogonal to the crystal pulling direction 4. Furthermore, as shown in FIG. 2, the cryostat 1 has the superconducting coil 2a in a helium container 40 so that the coil 2a is soaked in a coolant 41 such as liquid helium, and the like. Moreover, a radiation shield 42 is provided outside the helium container 40, and the entirety of the helium container 40 and the radiation shield 42 is stored in a vessel 43 so as to comprise the cryostat as a whole. Although the case provided with one radiation shield 42 is shown in the above-mentioned example, double radiation shields can be provided as needed. Furthermore, a system where the superconducting coils 2a, 2b in the helium container 40 are cooled down to the superconducting state with a freezer without using a coolant such as liquid helium, and the like, can also be used. In this case, the helium container and the coolant shown in FIG. 2 are not provided. This is an example of a magnetic device where a crystal pulling device is provided in the bore 5 at the center part of the C-shaped cryostat 1 for applying the horizontal magnetic field to the crystal pulling device. FIG. 3 shows another configuration of a conventional superconducting magnetic device for a crystal pulling device. The superconducting magnet device is provided such that two superconducting coils 2a, 2b are provided facing with each other, and the magnetic field direction 3 generated by the superconducting coils 2a, 2b is orthogonal to the crystal pulling direction 4 as in FIG. 1 in a double-cylindrical cryostat 11 comprising the inner cylinder and the outer cylinder. This is an example of a magnetic device where a crystal pulling device is provided in the bore 12, which is a space of room temperature, inside the inner cylinder of the cryostat 11 for applying the horizontal magnetic field to the crystal pulling device. FIG. 4 shows still another configuration of a conventional superconducting magnet device for a crystal pulling device. The superconducting magnet device is provided such that two superconducting coils 2a, 2b are provided facing with each other with an optional distance therebetween with respect to the axial direction of a cryostat 31 in the double-cylindrical cryostat 31 so that magnetic fields 30a, 30b are generated in the direction the coils 2a, 2b are opposed so as to generate the cusp magnetic field. In this case, the crystal pulling device is disposed in the bore 32, and the crystal pulling direction 4 is as shown in the figure. Since the magnetic field becomes zero on the line 6 in the figure in the cusp magnetic field, it is said that a high quality crystal compared with the cases of FIGS. 1 and 3 can be obtained by pulling the crystal on the line. Since a nonmagnetic material such as stainless steel and aluminum has been used as the vessel of the cryostat in the above-mentioned conventional superconducting magnet devices for a crystal pulling device, the magnetic field generated from the superconducting coils is leaked to the outside of the magnet so as to affect a motor or component members made from a magnetic substance existing in the vicinity of the vessel. In this case, since the magnetic substance and the superconducting coils are attracted with each other and the attraction force is proportional with the volume, the weight and the magnetic field gradient of the magnetic substance, the larger the magnetic component member or the magnet are, the larger the attraction force becomes accordingly. Therefore, it involves a problem in that the component members should be made from a nonmagnetic material, which is expensive, or the cross-section of the support in the cryostat for supporting the coils should be large, and thus the heat penetration amount of the cryostat becomes large. Furthermore, if a motor or a measurement device easily affected by the magnetic field exists in the vicinity of the cryostat, it may lead to the malfunction of the devices. Moreover, since the superconducting magnets adjacent to each other are affected by the leakage magnetic fields of each other if the leakage magnetic field is large so as to disturb the magnetic field strength or the magnetic field distribution necessary in the bore, the installation space of the adjacent magnets and the crystal pulling device should be wide, and thus the installation space cannot be used advantageously. A prior art superconducting magnet device for a crystal pulling device with the features of the preamble portion of claim 1 is described in JP-A-1033093. This device has, for the purpose of shielding a magnetic field, magnetic shielding material containing a superconductive material provided to all surfaces of an outer vessel surrounding the main superconducting coils. Another superconducting magnetic device is disclosed in JP-A-6051691 which teaches for the same purpose to surround the main superconducting coils with a magnetic shield provided on the radial outer circumferential surface of a non-magnetic stainless steel body. An object of the present invention is to provide a superconducting magnetic device for a crystal pulling device which is capable of reducing the leakage magnetic field at comparatively low cost, small size and light weight. In order to achieve this object the present invention provides a superconducting magnet device for a crystal pulling device as set out in claim 1. Preferred embodiments of the present invention are defined in the subclaims. The present invention provides a superconducting magnet device for a crystal pulling device comprising a pair of ring-like superconducting coils facing with each other with respect to the axial direction, with the crystal pulling device disposed therebetween, a radiation shield surrounding the superconducting coils, and a vessel surrounding the radiation shield, wherein auxiliary coils for generating the magnetic field in the opposite direction with respect to that of the main coils are provided within the angle elongating from the intersection point of the symmetrical axis of the main superconducting coils and the central axis of the superconducting coils toward the main superconducting coils. Therefore, since the auxiliary coils generate the magnetic field in the opposite direction with respect to that of the main coils, the leakage magnetic field generated from the main coils can be offset by the auxiliary coils. In the present invention, the vessel interposed between the coils facing with each other is made from a magnetic substance. Moreover, by further adding a magnetic shield to the auxiliary coils, more shield effect can be provided in the present invention. In the present invention, the auxiliary coils are electrically short-circuited. Therefore, since the auxiliary coils induce the magnetic field in the opposite direction with respect to that of the main coils in the present invention, the magnetic shield by the auxiliary coils can be obtained only by exciting the main coils. This can be achieved by a magnet either with the lateral magnetic field, the vertical magnetic field, or the cusp magnetic field. In the present invention, either one of the main coils facing with each other is electrically short-circuited. Therefore, in the present invention, by exciting only one main coil, the magnetic field in the opposite direction (cusp magnetic field) can be induced in the other main coil, and furthermore, the magnetic field can be generated in the auxiliary coils in the direction opposite to that of the main coils, respectively so as to obtain the magnetic shield. This summary of the invention does not necessarily describe all necessary features so that the invention may also be a sub-combination of these described features. The invention can be more fully under stood from the following detailed description when taken in conjunction with the accompanying drawings, in which: FIG. 1 is a perspective view showing a configuration of a conventional superconducting magnet device for a crystal pulling device; FIG. 2 is a cross-sectional view viewed from the arrow direction, taken on the line II-II of FIG. 1; FIG. 3 shows another configuration of a conventional superconducting magnet device for a crystal pulling device; FIG. 4 shows yet another configuration of a conventional superconducting magnet device for a crystal pulling device; FIG. 5 is a longitudinal cross-sectional view showing a part of a first a super-conducting magnet device for a crystal pulling device for explaining certain features of the present invention; FIG. 6 is a cross-sectional view viewed from the arrow direction, taken on the line VI-VI of FIG. 5; FIG. 7 is a longitudinal cross-sectional view showing a part of a second super-conducting magnet device for a crystal pulling device for explaining certain features of the present invention; FIG. 8 is a cross-sectional view viewed from the arrow direction, taken on the line VII-VII of FIG. 7; FIG. 9 is a longitudinal cross-sectional view showing a part of a third super-conducting magnet device for a crystal pulling device for explaining certain features of the present invention; FIG. 10 is a longitudinal cross-sectional view showing a part of a fourth super-conducting magnet device for a crystal pulling device for explaining certain features of the present invention; FIG. 11 is a longitudinal cross-sectional view showing a part of a fifth super-conducting magnet device for a crystal pulling device for explaining certain features of the present invention; FIG. 12 is a longitudinal cross-sectional view showing a part of a sixth super-conducting magnet device for a crystal pulling device for explaining certain features of the present invention; FIG. 13 shows the configuration of a coil provided in the vessel of an embodiment of a superconducting magnet device for a crystal pulling device according to the present invention; FIG. 14 shows the configuration of a coil provided in the vessel of another embodiment of a superconducting magnet device for a crystal pulling device according to the present invention; FIG. 15 shows the configuration of the connection of a coil provided in the vessel of a further embodiment of a superconducting magnet device for a crystal pulling device according to the present invention; FIG. 16 shows the configuration of the connection of a coil provided in the vessel of a still further embodiment of a superconducting magnet device for a crystal pulling device according to the present invention; and FIG. 17 shows the configuration of the connection of a coil provided in the vessel of a still further embodiment of a superconducting magnet device for a crystal pulling device according to the present invention. DETAILED DESCRIPTION OF THE INVENTION Hereinafter preferable embodiments of the present invention will be explained with reference to the accompanied drawings. FIG. 5 is a longitudinal cross-sectional view showing a part of a super-conducting magnet device for a crystal pulling device having certain features of the present invention, and FIG. 6 is a lateral cross-sectional view of the device as a whole. In FIGS. 5 and 6, a vessel (e.g. a cryostat or a vacuum container) 51 comprises a frame 54 formed in a C-shape with a rear plate 52 and a pair of side plates 53, a U-shaped inner plate 55, forming the bore in the frame 54, front plates 56 for closing the spaces between the inner plate 55 and front ends of the frame 54, and an upper plate 57 and a lower plate 58 for closing the upper opening end and the lower opening end of the frame 54 and the inner plate 55. In the vessel 51, a helium container 40 where two ring-like superconducting coils 2a, 2b (one of them, the superconducting coil 2a is shown in FIG. 5) are provided facing with each other in the direction of the central axis of the container and soaked in a coolant 41 such as liquid helium is provided, and a radiation shield 42 is provided outside the helium container 40 for surrounding the same, so as to comprise cryostat as a whole. In the cryostat, among the component members of the vessel 51, the rear plate 52, the side plates 53, the front plates 56, the upper plate 57 and the lower plate 58 are made from a material, which is a magnetic substance, and the inner plate 55 facing to the crystal pulling device (not illustrated) to be inserted in the bore is made from a nonmagnetic material. Therefore, according to the cryostat, since the rear plate 52, the side plates 53, the front plates 56, the upper plate 57 and the lower plate 58 comprised in the vessel 51 are made from a magnetic material, and only the inner plate 55 is made from a nonmagnetic material, the magnetic field generated from the superconducting coils 2a, 2b is absorbed by the magnetic substance without leaking to the outside, and thus a motor or components made from a magnetic substance in the vicinity thereof cannot be affected. Moreover, since the vessel 51, of which components other than the inner plate 55 comprise a magnetic substance, also serves as the magnetic shield, a small size and the light weight can be realized as a whole, and a comparatively low price can be achieved compared with the conventional one with the entirety of the vessel comprising a nonmagnetic substance. Moreover, since a part of the magnetic field is contained by the magnetic shield, the magnetic field strength at the bore center becomes high. That is, compared with a coil without a magnetic shield, the magnetomotive force (ampere turn number) can be smaller so that a low capacity power source with a low current value can be used and a superconducting coil with a smaller number of turns can be used. Although the case with a C-shaped frame 54 and an inner plate 55 comprising a vessel has been explained in the above-mentioned example, the same effect can be obtained also in a cylindrical or cusp magnetic field shape cryostat by having the vessel member facing to the crystal pulling device made from a nonmagnetic member and the other vessel member made from a magnetic material. FIG. 7 is a longitudinal cross-sectional view showing a part of a super-conductin magnet device for a crystal pulling device having cerfain features of the present invention, and FIG. 8 is a cross-sectional view of the entire device. For the parts the same as those of FIGS. 5 and 6, the same numerals are applied and further explanation is not given here. Only the differences will be described. In this example, as shown in FIGS. 7 and 8, the front opening end parts of the U-shaped inner plate 55, which is a part of a component member of the vessel 51, are provided with magnetic substances 60. Therefore, according to the cryostat, since the front opening end parts of the inner plate 55 are made from the magnetic substances 60, the line of magnetic force leaked from the inner plate side end parts of the upper plate 57 and the lower plate 58 can be absorbed to the inside so that the leakage magnetic field on the upper and lower surface of the magnet and on the crystal pulling device axis can be further reduced. Moreover, the leakage magnetic field at the opening parts of the vessel 51 can be absorbed by the magnetic substances 60 so as to be reduced. FIG. 9 is a longitudinal cross-sectional view showing a part of a super-conducting magnet device for a crystal pulling device having certain features of the present invention. For the parts the same as those of FIG. 5, the same numerals are applied and further explanation is not given here. Only the differences will be described. In this example, as shown in FIG. 9, when the distance Y between the upper plate 57 of the vessel 51 and the coil 2a is shorter than the distance X between the side plate 53 and the coil 2a, the plate thickness t2 of the upper plate 57 is made thicker than the plate thickness t1 of the side plate 53. The front plates and the rear plate, which are not illustrated, are the same as the first example. Therefore, according to the cryostat, since the thickness of the plate with a shorter distance with respect to the coil 2a is thicker than the thickness of the plate with a longer distance, the leakage magnetic field at a side closer to the coil where the magnetic field is stronger can further be absorbed. Accordingly, since all the magnetic vessel members need not be made thicker, a lighter weight can be achieved as a whole. FIG. 10 is a longitudinal cross-sectional view showing a part of a fourth example of a super-conducting magnet device for a crystal pulling device having certain features of the present invention. For the parts the same as those of FIG. 5, the same numerals are applied and further explanation is not given here. Only the differences will be described. In the fourth example, as shown in FIG. 10, an upper auxiliary plate 71, a lower auxiliary plate 72 and side auxiliary plates 73 of a predetermined thickness are attached to the upper plate 57, the lower plate 58 and the inner surface of the side plates 53 corresponding to the coil, respectively. In this case, the auxiliary plates 71 to 73 are made from a magnetic material and bonded mechanically or metallurgically. Therefore, according to the cryostat, since the leakage magnetic field in the vicinity of the coil where the magnetic field is strongest can be absorbed, the other members can be thin, and thus the light weight of the vessel can be achieved. Although auxiliary plates are provided on the inner surface of the plates in the above-mentioned embodiment, they can be provided on the outer surface as well. FIG. 11 is a longitudinal cross-sectional view showing a part of a fifth example of a super-conducting magnet device for a crystal pulling device having certain features of the present invention. For the parts the same as those of FIG. 4, the same numerals are applied for the explanation. The superconducting magnet device for a crystal pulling device shown in FIG. 11 forms a cusp magnetic field by providing two superconducting coils 2a, 2b facing with each other in the axial direction of the cryostat 31 with an appropriate distance in the double cylindrical cryostat 31 so as to generate the magnetic fields 30a, 30b in the direction toward each other as shown in FIG. 11. In the fifth example, the outer cylindrical member 31a and an upper plate 31c and a lower plate 31d to be disposed between the outer cylindrical member 31a and an inner cylindrical member 31b are made from a magnetic material (hatched parts in the figure), the inner cylindrical member 31b is made from a nonmagnetic material, and an auxiliary ring 80 made from a magnetic material is attached to the inner surface of the outer cylindrical member 31a corresponding with the part between the two superconducting coils 2a, 2b in the superconducting magnet device with such a configuration. In the figure, the numeral 32 denotes the diameter of a space part (bore), to which the crystal pulling device will be inserted. Therefore, according to the cryostat with the configuration, since a magnetic substance is added to the surface of the outer cylindrical member 31a corresponding with the center part of the pair of the upper and lower superconducting coils 2a, 2b with respect to the axial direction, where the leakage magnetic field is large, the ability of absorbing the leakage magnetic field can further be improved and the magnetomotive force of the coils can further be lowered. FIG. 12 is a longitudinal cross-sectional view showing a part of a sixth example of a super-conducting magnet device for a crystal pulling device having certain features of the present invention. For the parts the same as those of FIG. 5, the same numerals are applied and further explanation is not given here. Only the differences will be described. In the sixth example, as shown in FIG. 12, a rear plate (not illustrated), both side plates 53, an upper plate 57 and a lower plate 58 of a C-shaped frame comprising the vessel are covered by an upper plate 91, a lower plate 92, and an outer plate 93 made from a magnetic material and a U-shaped inner plate 55 made from a nonmagnetic material in multiple layers. Therefore, according to the cryostat, the leakage magnetic field from the inner magnetic substance can further be reduced by the outer magnetic substance. FIG. 13 shows the configuration of a coil provided in the vessel of an embodiment of a super-conducting magnet device for a crystal pulling device according to the present invention. In this embodiment, as shown in FIG. 13, in addition to a superconducting coil 2a, an auxiliary coil 100 having a diameter larger than that of the superconducting coil is provided so as to generate a magnetic field in the opposite direction with respect to that of the superconducting coil 2a. In this case, if the conductor center P of the auxiliary coil exists inside the range of the angle g, formed by the lines 202, 203 linking the intersection point N of the symmetrical axis of the superconducting coil 2a and the opposing coil and the central axis M of the coil and the outer diameter part symmetrical axis side corner part 200 and the opposite side corner part 201 of the superconducting coil 2a, or the lines 206, 207 linking the intersection point N and the inner diameter part symmetrical axis side corner part 204 and the opposite side corner part 205. For example, if the conductor center P of the auxiliary coil 100 exists in the range of the angle h formed by the lines 206, 207 linking the intersection point N and the corner parts 204, 205 at the opposite side with respect to the coil inner diameter part symmetrical axis L of the superconducting coil 2a and the coil winding central axis M. It is effective for reducing the leakage magnetic field on the central axis M, but it is not effective for reducing the leakage magnetic field on the symmetrical axis L. Furthermore, if the conductor center P of the auxiliary coil 100 exists in a range larger than the angle (g+h), it is opposite to the above-mentioned case, that is, it is effective for reducing the leakage magnetic field on the symmetrical axis L, but it is not effective for reducing the magnetic field on the central axis M. In this embodiment, the conductor center P of the auxiliary coil 100 is provided such that it is disposed in the angle g formed by the lines elongating from the intersection point N of the symmetrical axis of the main superconducting coil 2a, to which the cross-section of the auxiliary coil 100 faces, and the coil winding central axis M toward the edges of the cross-section of the superconducting coil 2a. Therefore, according to the cryostat provided with the coil of the above-mentioned configuration, the leakage magnetic field generated by the main coil can be offset efficiently by the auxiliary coil 100 in both outer diameter direction (symmetrical axis L direction) and central axis M direction so that an efficient magnet with a small magnetomotive force can be provided as a whole, and thus a further light weight can be achieved compared with the magnetic shield method using a magnetic substance. FIG. 14 shows the configuration of a coil provided in the vessel of another embodiment of a superconducting magnet device for a crystal pulling device according to the present invention. For the parts the same as those of FIG. 13, the same numerals are applied and further explanation is not given here. Only the differences will be described. In this embodiment, an outer plate 110 made from a magnetic material is provided as a part of the vessel in addition to the configuration of the previous embodiment. Therefore, according to the cryostat with the above-mentioned configuration, the leakage magnetic field can be further reduced, and the magnetomotive force of the main coil and the auxiliary coil can be smaller. Although the outer plate made from a magnetic material is provided as a part of the vessel in the embodiment shown in the figure, the same effect can be achieved by providing it as another member other than the vessel on the inside or the outside of the vessel. FIG. 15 shows the configuration of the connection of a coil provided in the vessel of a further embodiment of a superconducting magnet device for a crystal pulling device according to the present invention. In this embodiment, a pair of main coils 120, 121, provided facing with each other in a cryostat 123 are connected in series as well as the main coil 120 is connected with an exciting power source 124, and both ends of the main coil 121 are short-circuited and connected with one end of the exciting power source 124. In the cryostat with the coil connection configuration, one main coil 120 is excited by the external exciting power source 124 so as to generate the magnetic field. At the time, electric current for generating the magnetic field with the current value the same as the main coil 120 in the opposite direction flows in the main coil 121 electrically short-circuited in the cryostat 123 according to the change by time passage of the magnetic field generated during the excitement of the main coil 120. Therefore, by exciting only the main coil 120, the other main coil 121 is excited as well. Since both main coils in the cryostat are connected common electrically in series in the conventional connection configuration, the inductance of the coil is larger than this embodiment, and thus power source with a large exciting voltage is required. According to this embodiment, a low capacity power source can be used. FIG. 16 shows the configuration of the connection of a coil provided in the vessel of a still further embodiment of a superconducting magnet device for a crystal pulling device according to the present invention. In this embodiment, as shown in FIG. 16, main coils 130a, 130b, provided in a cryostat 123 are connected electrically in series as well as both ends thereof are connected with an exciting power source 124 such that the coils can generate magnetic fields in the same direction or magnetic fields in the opposite directions, and auxiliary coils 131a, 131b, with both ends short-circuited are provided, respectively. Therefore, according to the above-mentioned configuration, since electric current for generating the magnetic field in the direction opposite to that of the main coil can be induced in the auxiliary coils 131a, 131b by exciting the main coils 130a, 130b, a power source is not required for the auxiliary coils. FIG. 17 shows the configuration of the connection of a coil provided in the vessel of a still further embodiment of a superconducting magnet device for a crystal pulling device according to the present invention. In this embodiment, in addition to the coil connection configuration shown in FIG. 15, auxiliary coils 131a, 131b are provided as in FIG. 16. Therefore, according to the above-mentioned configuration, since the main coil 121 is disposed such that the coil opposes the main coil 120, the cusp magnetic field is generated, and further, the auxiliary coils 131a, 131b generate a magnetic field in the direction opposite to the magnetic field generated by each main coil, the same effect as in the previous embodiments can be achieved. As heretofore mentioned, according to the superconducting magnetic device for a crystal pulling device according to the present invention, the following effects can be achieved. (1) Since an auxiliary coil for generating the magnetic field in the opposite direction is provided in a predetermined angle, the leakage magnetic field can be reduced efficiently. Furthermore, by adding a magnetic substance thereto, a further effect can be achieved. (2) Since the magnetic interference of magnets installed adjacent with each other can be prevented by the magnetic field, the magnetic can be installed with a smaller interval, and thus the installation space can be utilized advantageously. (3) Since the leakage magnetic field becomes smaller, the attraction force between the magnet and the magnetic components in the vicinity thereof becomes smaller, and thus the components need not be made from a nonmagnetic substance. (4) Since the influence on the devices provided in the vicinity of the magnet such as a motor and measurement devices, which can easily be affected by the magnetic field becomes smaller, the devices can be mounted in a position closer to the magnet compared with the conventional ones, and thus it contributes to achieving a smaller size of the pulling device as a whole. (5) Since at least either one of the main coil and the auxiliary coil is connected electrically in the cryostat, a large magnet can be excited with a small capacity exciting power source. Moreover, by adopting such a connection, the inductance becomes smaller, and thus the excitement change and the magnetic force change can be faster thereby. (6) Since the members of the vessel facing to the crystal pulling device are a nonmagnetic member and the other members not facing thereto are a magnetic member, the magnetic field leaked to the outside can be reduced with the weight and the size the same as the conventional one. Furthermore, by having the magnetic members thicker, the magnetic shield effect can further be improved. (7) Since the magnetic field is contained inside the vessel by the magnetic shield, and consequently the magnetic field strength of the inside becomes large, the magnetomotive force of the coil can be smaller for that. That is, a coil, can be excited by a small capacity power source can be produced with a small number of turns at a low cost. (8) Since a part of the side facing to the crystal pulling device is made from a magnetic substance as well, the magnetic shield effect can be further improved.

Claims: A superconducting magnet device for a crystal pulling device, comprising: a pair of ring-like main superconducting coils (2a,2b;120,121;130a,130b) facing each other with respect to the axial direction, with the crystal pulling device to be disposed therebetween, for generating a magnetic field; a radiation shield (42) surrounding the main superconducting coils (2a,2b;120;130a,130b); a vessel (51) surrounding the radiation shield (42), said vessel (51) including an outer plate (53;110) made from a magnetic substance; characterized by comprising auxiliary coils (100;131a,131b) configured to generate a magnetic field in an opposite direction with respect to the magnetic field of the main superconducting coils (2a,2b;120,121;130a,130b); wherein a conductor center (P) of the auxiliary coils (100) is located in a range (g) defined by first (202,203) and second lines (206,207), the first lines (202,203) extending from an intersection point (N) of a symmetrical axis (L) with a central axis (M) of said pair of main superconducting coils (2a,2b;120,121;130a,130b) through symmetrical axis side corner parts (200,201) on an outer diameter part of at least one main superconducting coil (2a,2b;120,121;130a,130b), and the second lines (206,207) extending from said intersection point (N) through central axis side corner parts (204,205) on an inner diameter part of said at least one main superconducting coil (2a,2b;120,121;130a,130b). The superconducting magnet device for a crystal pulling device according to claim 1, wherein both ends of the auxiliary coils (100;131a,131b) are electrically short-circuited. The superconducting magnet device for a crystal pulling device according to claim 2, wherein both ends of either one of the main superconducting coils (2a,2b;120) facing each other are electrically short-circuited.

Inventors: MASANORI ARATA, TAKASHI SASAKI, MASANORI, ARATA, TAKASHI, SASAKI, Masanori, Arata, c/o Int. Prop. Div., K.K. Toshiba, Takashi, Sasaki, c/o Int. Prop. Div., K.K. Toshiba
Applicants: TOSHIBA KK, KABUSHIKI KAISHA TOSHIBA
Application year: 1999
Main classification: C30B15
IPC codes: H01L39, C30B15, H01F6