CN118315152A - Method for adjusting superconducting magnet device - Google Patents
Method for adjusting superconducting magnet device Download PDFInfo
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- CN118315152A CN118315152A CN202410573308.9A CN202410573308A CN118315152A CN 118315152 A CN118315152 A CN 118315152A CN 202410573308 A CN202410573308 A CN 202410573308A CN 118315152 A CN118315152 A CN 118315152A
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- 238000000034 method Methods 0.000 title claims abstract description 43
- 238000005259 measurement Methods 0.000 claims abstract description 125
- 239000013078 crystal Substances 0.000 claims abstract description 30
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims abstract description 27
- 229910052710 silicon Inorganic materials 0.000 claims abstract description 27
- 239000010703 silicon Substances 0.000 claims abstract description 27
- 239000007788 liquid Substances 0.000 claims abstract description 16
- 230000000712 assembly Effects 0.000 claims description 31
- 238000000429 assembly Methods 0.000 claims description 31
- 238000004458 analytical method Methods 0.000 claims description 20
- 239000000306 component Substances 0.000 claims description 12
- 230000001105 regulatory effect Effects 0.000 claims description 4
- 239000008358 core component Substances 0.000 claims description 3
- 230000005284 excitation Effects 0.000 claims description 3
- 239000000155 melt Substances 0.000 abstract description 2
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- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 5
- 229910052802 copper Inorganic materials 0.000 description 5
- 239000010949 copper Substances 0.000 description 5
- 229910021421 monocrystalline silicon Inorganic materials 0.000 description 4
- 230000008569 process Effects 0.000 description 4
- 230000009471 action Effects 0.000 description 3
- 238000004364 calculation method Methods 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 229920000049 Carbon (fiber) Polymers 0.000 description 2
- 239000004917 carbon fiber Substances 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000009434 installation Methods 0.000 description 2
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 2
- 230000008439 repair process Effects 0.000 description 2
- 239000004593 Epoxy Substances 0.000 description 1
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- 238000010276 construction Methods 0.000 description 1
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- 238000005457 optimization Methods 0.000 description 1
- 238000005086 pumping Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/02—Measuring direction or magnitude of magnetic fields or magnetic flux
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
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- Physics & Mathematics (AREA)
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- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
Abstract
The embodiment of the application relates to a method for adjusting a superconducting magnet device. The adjusting method comprises the steps of obtaining a radial magnetic field measured value and an axial magnetic field measured value at each measuring point in a plurality of measuring points on a first measuring circle through measurement; adjusting the relative position of the center of the crucible and the center of the magnetic field zero magnetic surface generated by the superconducting magnet based on the radial magnetic field measurement value so that the center of the crucible coincides with the center of the magnetic field zero magnetic surface; and adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on the axial magnetic field measured value so that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible. The adjusting method provided by the embodiment of the application can enable the center of the crucible to coincide with the center of the magnetic field zero magnetic surface and enable the magnetic field zero magnetic surface to be parallel to the liquid level of the melt in the crucible so as to ensure the subsequent crystal pulling quality.
Description
The application is a divisional application of an application patent application with a parent application date of 2024, 03, 05 and an application number of CN202410245068. X.
Technical Field
The application relates to the technical field of semiconductors, in particular to a method for adjusting a superconducting magnet device.
Background
The magnetic control Czochralski single crystal superconducting magnet is a superconducting magnet system for growing Czochralski single crystal silicon. In the process of pulling the monocrystalline silicon, the uniformity of the monocrystalline silicon rod can be effectively improved by adding a magnetic field with a certain strength, and the quality of the monocrystalline silicon rod is further improved.
After the magnetron czochralski single crystal superconducting magnet is arranged around the single crystal furnace, the center of the zero magnetic surface of the magnetic field generated by the magnetron czochralski single crystal superconducting magnet and the center of the crucible may deviate, and the levelness of the zero magnetic surface of the magnetic field generated by the magnetron czochralski single crystal superconducting magnet may also deviate, and the deviation directly influences the crystal pulling quality.
Disclosure of Invention
In view of the above, an embodiment of the present application provides a method for adjusting a superconducting magnet device to solve at least one of the problems in the prior art.
The embodiment of the application provides an adjusting method of a superconducting magnet device, which comprises a first container and a coil assembly, wherein the first container comprises a first shell, a closed first cavity is formed in an inner cavity of the first shell, a first through hole is formed in the first shell in a surrounding mode, the first through hole is used for accommodating a single crystal furnace, and the single crystal furnace is used for placing a crucible for bearing silicon solution; the coil assembly is positioned in the first cavity, and comprises a superconducting coil, wherein the superconducting coil is used for generating a magnetic field and acting on silicon melt in the crucible, and is a core component of a superconducting magnet; the adjusting method comprises the following steps:
Obtaining a radial magnetic field measured value and an axial magnetic field measured value at each of a plurality of measuring points on a first measuring circle through measurement, wherein the center of the first measuring circle is the center of a crucible in a single crystal furnace, the plane of the first measuring circle is parallel to the mechanical center plane of the upper end face and the lower end face of the first container, the distances between the adjacent measuring points are equal, and the superconducting magnet is a superconducting magnet after excitation;
Adjusting the relative position of the center of the crucible and the center of the magnetic field zero magnetic surface generated by the superconducting magnet based on the radial magnetic field measurement value so that the center of the crucible coincides with the center of the magnetic field zero magnetic surface;
and adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on the axial magnetic field measured value so that the magnetic field zero magnetic surface is parallel to the liquid level of the silicon melt in the crucible.
In combination with the first aspect of the application, in an alternative embodiment, adjusting the relative position of the center of the crucible and the center of the zero magnetic surface of the magnetic field generated by the superconducting magnet based on the radial magnetic field measurement comprises:
obtaining a standard value of a radial magnetic field of the measuring point;
Determining a minimum standard deviation of a plurality of measurement points on the first measurement circle based on the radial magnetic field measurement values of the plurality of measurement points and the standard value;
judging whether the minimum standard deviation value is smaller than or equal to a first set value;
if yes, judging that the center of the crucible is coincident with the center of the magnetic field zero magnetic surface;
If not, adjusting the relative positions of the center of the crucible and the center of the zero magnetic surface of the magnetic field based on analysis of a plurality of measurement points.
With reference to the first aspect of the application, in an alternative embodiment, adjusting the relative position of the center of the crucible and the center of the zero magnetic surface of the magnetic field based on analysis of a plurality of the measurement points comprises:
Calculating an average value of the radial magnetic field measured values of a plurality of measuring points;
Calculating a difference between the average value and each of the radial magnetic field measurements;
Obtaining at least a maximum value of the differences;
and adjusting the relative position of the center of the crucible and the center of the superconducting magnet based on at least the maximum value in the difference value so that the center of the crucible coincides with the zero magnetic surface center of the magnetic field.
In combination with the first aspect of the present application, in an alternative embodiment, adjusting the position of the measurement point in the axial direction of the superconducting magnet based on the axial magnetic field measurement value so that the magnetic field zero magnetic surface is parallel to the silicon melt level in the crucible includes:
Adjusting the position of the superconducting magnet in the axial direction of the superconducting magnet at least at one measurement point corresponding to the position based on analysis of the axial magnetic field measurement value;
Obtaining a current axial magnetic field measured value of each measuring point through measurement;
calculating a difference between the current axial magnetic field measurement value and the axial magnetic field measurement value;
calculating the adjustment distance of the superconducting magnet at the corresponding position of each measuring point in the axial direction of the superconducting magnet;
calculating root mean square values of the axial magnetic fields of the plurality of measurement points after adjustment based on the adjustment distance and the difference value between the current axial magnetic field measurement value and the axial magnetic field measurement value;
Judging whether the root mean square value is smaller than or equal to a second set value;
If yes, judging that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible;
if not, adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on analysis of the current axial magnetic field measured value.
With reference to the first aspect of the present application, in an alternative embodiment, adjusting the position of at least one of the measurement points in the axial direction of the superconducting magnet based on an analysis of the axial magnetic field measurement values includes:
Calculating an average value of the axial magnetic field measured values of a plurality of measuring points;
calculating a difference value between the average value and each axial magnetic field measured value;
Obtaining at least a maximum value of the differences;
the position of the superconducting magnet in the axial direction thereof at the position corresponding to the measurement point corresponding thereto is adjusted based on at least the maximum value of the difference values.
With reference to the first aspect of the present application, in an alternative embodiment, adjusting the position of at least one of the measurement points in the axial direction of the superconducting magnet based on an analysis of the axial magnetic field measurement values includes:
Calculating an average value of the axial magnetic field measured values of a plurality of measuring points;
calculating a difference value between the average value and each axial magnetic field measured value;
Sequentially arranging a plurality of differences from large to small;
The positions of the superconducting magnets at the positions corresponding to the measurement points corresponding thereto are adjusted in the axial direction thereof based on the plurality of difference values arranged forward.
In combination with the first aspect of the application, in an alternative embodiment, the plurality of measurement points are measured on a second measurement circle having a radius larger than the radius of the crucible.
With reference to the first aspect of the present application, in an alternative embodiment, the superconducting magnet device further includes a plurality of adjustment assemblies and a plurality of pull rod assemblies, one end of each pull rod assembly is located in the first chamber and connected to the coil assembly, and the other end of each pull rod assembly is connected to the adjustment assembly;
adjusting the relative position of the center of the crucible and the center of the zero magnetic surface of the magnetic field generated by the superconducting magnet based on the radial magnetic field measurement value, comprising:
And regulating the magnetic field zero magnetic surface generated by the superconducting magnet by utilizing a plurality of regulating components, and enabling the center of the magnetic field zero magnetic surface to coincide with the center of the crucible.
With reference to the first aspect of the present application, in an alternative embodiment, a plurality of said measurement points on said first measurement circle correspond to positions of a plurality of said adjustment assemblies;
Adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on the axial magnetic field measured value so that the magnetic field zero magnetic surface is parallel to the silicon melt liquid level in the crucible, wherein the method comprises the following steps:
and adjusting the positions of the superconducting magnets at the positions corresponding to the measuring points in the axial direction by utilizing a plurality of adjusting assemblies so that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible.
In combination with the first aspect of the application, in an alternative embodiment, the radius of the first measuring circle is smaller than or equal to the radius of the crucible.
According to the adjustment method of the superconducting magnet device, provided by the embodiment of the application, the relative positions of the center of the zero magnetic surface of the magnetic field generated by the superconducting magnet and the center of the crucible are adjusted based on the radial magnetic field measured value by selecting the first measuring circle and measuring the radial magnetic field measured value and the axial magnetic field measured value of each measuring point, so that the center of the crucible is overlapped with the center of the zero magnetic surface of the magnetic field; and adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on the axial magnetic field measured value so that the zero magnetic surface of the magnetic field is parallel to the liquid level of the melt in the crucible, thereby ensuring the subsequent crystal pulling quality.
Additional aspects and advantages of the application will be set forth in part in the description which follows and, in part, will be obvious from the description, or may be learned by practice of the application.
Drawings
The accompanying drawings, which are included to provide a further understanding of the application and are incorporated in and constitute a part of this specification, illustrate embodiments of the application and together with the description serve to explain the application and do not constitute a limitation on the application. In the drawings:
Fig. 1 is a schematic view of the overall structure of a superconducting magnet device according to an embodiment of the present application;
fig. 2 is a schematic view showing a partial internal structure of a superconducting magnet device according to an embodiment of the present application;
Fig. 3 is a top view of a superconducting magnet device provided by an embodiment of the present application;
FIG. 4 is a cross-sectional view of A-A of FIG. 3;
fig. 5 is a schematic view showing a partial structure of a superconducting magnet device according to another embodiment of the present application;
Fig. 6 is a schematic structural view of a pull rod member in a superconducting magnet device according to an embodiment of the present application;
FIG. 7 is an enlarged view at B in FIG. 4;
Fig. 8 is a schematic overall flow chart of an adjustment method of a superconducting magnet device according to an embodiment of the present application;
fig. 9 is a schematic diagram of a structure of a superconducting magnet divided into four measurement points in an adjustment method of a superconducting magnet device according to an embodiment of the present application;
FIG. 10 is a flow chart illustrating the relative position between the center of the crucible and the center of the zero magnetic surface of the magnetic field in the adjustment method of the superconducting magnet device according to the embodiment of the present application;
FIG. 11 is a flow chart illustrating analysis of a plurality of measurement points in a method for adjusting a superconducting magnet device according to an embodiment of the present application;
FIG. 12 is a flow chart of a method for adjusting an axial magnetic field generated by a superconducting magnet in a method for adjusting a superconducting magnet device according to an embodiment of the present application;
FIG. 13 is a flow chart illustrating analysis of axial magnetic field measurements in a method of tuning a superconducting magnet device according to an embodiment of the present application;
FIG. 14 is a graph showing the variation of axial magnetic field measured values after one of the measurement points is adjusted by applying the adjustment method of the superconducting magnet device according to the embodiment of the present application;
FIG. 15 is a graph of axial magnetic field measurements versus angle prior to adjustment using the method for adjusting a superconducting magnet device provided by embodiments of the present application;
fig. 16 is a graph of axial magnetic field measurement value versus angle after adjustment by applying the adjustment method of the superconducting magnet device according to the embodiment of the present application.
Reference numerals:
10. A first container; 101. a first through hole; 110. a first housing; 120. a first chamber; 131. a second housing; 132. a second chamber; 140. a support cylinder; 20. a coil assembly; 210. a superconducting coil; 220. a coil bobbin; 30. a pull rod assembly; 300. a base; 310. a first pin; 320. a second pin; 330. a third pin; 340. a fourth pin; 356. an annular pull rod; 350. a first pull rod; 360. a second pull rod; 370. a connecting plate; 380. copper is soft; 40. an adjustment assembly; 410. an adjusting nut; 420. a pull rod stud; 510. a control tower; 520. a refrigerating machine; 530. a signal line connector; 540. and a vacuum valve.
Detailed Description
Exemplary embodiments of the present disclosure will be described in more detail below with reference to the accompanying drawings. While exemplary embodiments of the application are shown in the drawings, it should be understood that the application may be embodied in various forms and should not be limited to the specific embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the disclosure to those skilled in the art.
In the following description, numerous specific details are set forth in order to provide a more thorough understanding of the present application. It will be apparent, however, to one skilled in the art that the application may be practiced without one or more of these details. In other instances, well-known features have not been described in detail so as not to obscure the application; that is, not all features of an actual implementation are described in detail herein, and well-known functions and constructions are not described in detail.
In the drawings, the size of layers, regions, elements and their relative sizes may be exaggerated for clarity. Like numbers refer to like elements throughout.
It will be understood that when an element or layer is referred to as being "on" … …, "" adjacent to "… …," "connected to" or "coupled to" another element or layer, it can be directly on, adjacent to, connected to or coupled to the other element or layer, or intervening elements or layers may be present. In contrast, when an element is referred to as being "directly on" … …, "" directly adjacent to "… …," "directly connected to" or "directly coupled to" another element or layer, there are no intervening elements or layers present. It will be understood that, although the terms first, second, third, etc. may be used herein to describe various elements, components, regions, layers and/or sections, these elements, components, regions, layers and/or sections should not be limited by these terms. These terms are only used to distinguish one element, component, region, layer or section from another element, component, region, layer or section. Thus, a first element, component, region, layer or section discussed below could be termed a second element, component, region, layer or section without departing from the teachings of the present application. When a second element, component, region, layer or section is discussed, it does not necessarily mean that the first element, component, region, layer or section is present.
Spatially relative terms, such as "under … …," "under … …," "below," "under … …," "over … …," "above," and the like, may be used herein for ease of description to describe one element or feature's relationship to another element or feature as illustrated in the figures. It will be understood that the spatially relative terms are intended to encompass different orientations of the device in use and operation in addition to the orientation depicted in the figures. For example, if the device in the figures is turned over, elements or features described as "under" or "beneath" other elements would then be oriented "on" the other elements or features. Thus, the exemplary terms "below … …" and "under … …" may include both an upper and a lower orientation. The device may be otherwise oriented (rotated 90 degrees or other orientations) and the spatially relative descriptors used herein interpreted accordingly.
The terminology used herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the application. As used herein, the singular forms "a", "an" and "the" are intended to include the plural forms as well, unless the context clearly indicates otherwise. It will be further understood that the terms "comprises" and/or "comprising," when used in this specification, specify the presence of stated features, integers, steps, operations, elements, and/or components, but do not preclude the presence or addition of one or more other features, integers, steps, operations, elements, components, and/or groups thereof. As used herein, the term "and/or" includes any and all combinations of the associated listed items.
In order to provide a thorough understanding of the present application, detailed steps and detailed structures will be presented in the following description in order to explain the technical solution of the present application. Preferred embodiments of the present application are described in detail below, however, the present application may have other embodiments in addition to these detailed descriptions.
In the prior art, during the process of installing the magnetron czochralski superconducting magnet device around the corresponding single crystal furnace, various problems may exist to cause the finally measured magnetic field to be not up to standard, such as: overlay tolerance during assembly. After the installation of the magnetic control straight-pull superconducting magnet device is completed, if the magnetic field measurement does not reach the standard, the magnetic control straight-pull superconducting magnet device is required to be disassembled and repaired, and a large amount of disassembly and assembly cost is required.
Based on the technical problems described above, the embodiments of the present application provide a superconducting magnet device, in which an adjusting assembly 40 is connected to a plurality of pull rod assemblies 30, and if the magnetic field measurement does not reach the standard after the installation of the magnetic control czochralski superconducting magnet device is completed, the levelness of the zero magnetic surface of the superconducting magnet is adjusted by using the adjusting assembly 40, so that the superconducting magnet device already assembled on the single crystal furnace does not need to be disassembled and repaired, thereby greatly improving the adjustment efficiency of the superconducting magnet and reducing the adjustment cost of the superconducting magnet.
Referring now to the drawings, a superconducting magnet device according to an embodiment of the present application is shown in fig. 1 and 2, and includes a first container 10, a coil assembly 20, a plurality of pull rod assemblies 30, and a plurality of adjustment assemblies 40.
The first container 10 includes a first housing 110, a closed first chamber 120 is formed in an inner cavity of the first housing 110, and a first through hole 101 is formed around the first housing 110, where the first through hole 101 is used for accommodating a single crystal furnace.
The coil assembly 20 is disposed in the first chamber 120, the coil assembly 20 includes a bobbin 220 and a superconducting coil 210, the superconducting coil 210 is wound around the bobbin 220, and the superconducting coil 210 is used to generate a magnetic field and acts on a silicon melt contained in a crucible in a single crystal furnace.
The plurality of pull rod assemblies 30 are circumferentially distributed around the axis of the first container 10, one end of the pull rod assemblies 30 is located in the first chamber 120 and connected with the coil assembly 20, and the other end of the pull rod assemblies 30 is located outside the first chamber 120 and can be connected to the first housing 110, so that the coil assembly 20 is suspended in the first chamber 120.
The plurality of adjusting assemblies 40 are connected to the other end of the pull rod assembly 30, and the superconducting coils 210 move along the axial direction of the first container 10 under the action of the adjusting assemblies 40 to adjust the levelness of the zero magnetic surface of the magnetic field.
The embodiment of the application provides a magnetic pulling single crystal superconducting magnet device with an adjustable pull rod structure, which is convenient for adjusting the zero magnetic surface of a superconducting magnet by utilizing a pull rod assembly 30, can effectively avoid the repair adjustment of the superconducting magnet and saves the manufacturing time and repair cost.
The single crystal furnace is located in the first through hole 101, when the center of the crucible in the single crystal furnace is coincident with the center of the superconducting magnet, the silicon melt in the crucible can be in a symmetrical magnetic field configuration, and the crystal pulling effect can be improved when the magnetic field generated by the superconducting magnet acts on the silicon melt in the crucible.
In an alternative embodiment, the superconducting coil 210 is wound by a specially made superconducting wire, the superconducting coil 210 is wound on the bobbin 220, and the strength of the superconducting coil 210 is reinforced by epoxy impregnation to ensure resistance to high stress generated thereby under a high magnetic field, and prevent the superconducting coil 210 from losing superconducting performance.
In the embodiment of the application, two superconducting coils 210 are provided, the two superconducting coils 210 are arranged in parallel, the running current is opposite, and the two superconducting coils are used for generating a special magnetic field suitable for magnetically controlling the czochralski silicon. The superconducting coil 210 is a core component of a superconducting magnet, and the superconducting magnet generates a strong magnetic field, so that the magnetic field acts on silicon melt in a crucible of the single crystal furnace to improve the crystal pulling quality.
In an alternative embodiment, as shown in fig. 3 and 4, the adjusting assembly 40 includes a first adjusting member and a second adjusting member, the first adjusting member is matched with the second adjusting member, the first adjusting member is connected with the other end of the pull rod assembly 30, and the first adjusting member can be connected with the first housing 110 under the action of the second adjusting member, so that the coil assembly 20 is suspended in the first chamber 120.
The first adjusting member can also drive the superconducting coil 210 to move along the axial direction of the first container 10 under the action of the second adjusting member, so as to adjust the levelness of the zero magnetic surface of the magnetic field.
In the embodiment of the present application, the first adjusting member can be caused to move the superconducting coil 210 along the axial direction of the first container 10 by adjusting the second adjusting member, or the first adjusting member is connected to the first housing 110.
It will be appreciated that the levelness of the zero magnetic surface of the magnetic field generated by the superconducting magnet is further adjusted by adjusting the position and orientation of the superconducting coil 210 by adjusting one or more second adjusting members. When the adjustment of the zero magnetic surface of the magnetic field generated by the superconducting magnet is completed, the first adjusting member is connected to the first housing 110 by adjusting the second adjusting member, so as to define the relative position of the superconducting coil 210 and the first housing 110.
In an alternative embodiment, as shown in fig. 2 and 4, the first container 10 further includes a support cylinder 140, the bottom of the support cylinder 140 is connected to the surface of the first housing 110, the support cylinder 140 has a second through hole along the axial direction thereof, the second through hole is communicated with the first chamber 120, one end of the first adjusting member is located in the second through hole, and the other end of the first adjusting member is located outside the support cylinder 140.
In the embodiment of the present application, the number of the pull rod assemblies 30, the adjusting assemblies 40 and the supporting cylinders 140 corresponds, and based on the limited space in the first chamber 120, the adjusting convenience and the adjusting accuracy of the adjusting assemblies 40 can be improved by connecting the supporting cylinders 140 to the surface of the first housing 110 and connecting the adjusting assemblies 40 to the supporting cylinders 140.
In an alternative embodiment, as shown in fig. 4, the first adjusting member includes a pull rod stud 420, the second adjusting member includes an adjusting nut 410, the adjusting nut 410 is matched with the pull rod stud 420, and the adjusting nut 410 rotates relative to the pull rod stud 420, so that the pull rod stud 420 drives the coil bobbin 220 to move.
That is, one end of the draw rod stud 420 is connected to the draw rod assembly 30, the other end of the draw rod stud 420 is located outside the support cylinder 140 and is connected to the adjusting nut 410 in a matching manner, and the relative position of the superconducting coil 210 and the first housing 110 is adjusted by rotating the adjusting nut 410, so as to further adjust the levelness of the zero magnetic surface of the magnetic field generated by the superconducting magnet.
It will be appreciated that the position and orientation of the superconducting coil 210 is adjusted by rotating one or more adjustment nuts 410, and eventually the zero magnetic field plane generated by the superconducting magnet is parallel to the silicon melt level in the crucible, thereby ensuring crystal pulling quality.
In an alternative embodiment, as shown in fig. 5, the superconducting magnet device further includes a second container, the second container is located in the first chamber 120, the second container includes a second housing 131, a second chamber 132 is formed in an inner cavity of the second housing 131, the coil assembly 20 is located in the second chamber 132, a third through hole is formed around the second housing 131, the third through hole and the first through hole 101 are concentric circles, the pull rod assembly 30 penetrates through a surface of the second housing 131 and is connected with the second housing 131, and a temperature in the second chamber 132 is lower than an external temperature of the second chamber 132.
The superconducting coil 210 is located in the second chamber 132, and a low temperature environment is formed in the second chamber 132, and the superconducting coil 210 is partitioned by the second housing 131, i.e., a cold shield, to ensure that the superconducting coil 210 has sufficiently low leakage heat.
It should be noted that, in fig. 1, the first housing 110 has a notch, in fig. 5, the first housing 110 and the second housing 131 have a notch, and the notches in fig. 1 and fig. 5 are only for facilitating the clarity of the internal structures of the first housing 110 and the second housing 131, and in fact, the notch does not exist.
In an alternative embodiment, the superconducting magnet device further includes a refrigerator 520, the refrigerator 520 is connected to the first housing 110 and located outside the first chamber 120, the refrigerator 520 is used for providing cooling capacity for the superconducting coil 210, when the cooling capacity of the refrigerator 520 is greater than that of the heat leakage, the superconducting coil 210 is cooled to a superconducting low temperature environment by the refrigerator 520, the temperature of the superconducting low temperature environment is 4.2K, and when the superconducting coil 210 is in the superconducting low temperature environment, the superconducting coil has negligible resistance, thereby achieving a superconducting state, and can bear higher current than a conventional coil, and further achieve higher magnetic field strength.
In an alternative embodiment, the superconducting magnet device further comprises a control tower 510, the control tower 510 is in a semicircular arc shape, and the control tower 510 with the semicircular arc structure can save occupied space and improve the compactness of the superconducting magnet device.
In an alternative embodiment, the superconducting magnet device further includes a signal line connector 530, a thermometer and a voltage drop line, wherein the thermometer and the voltage drop line are both connected to the superconducting coil 210 and are used for detecting the temperature of the superconducting coil 210 in real time, the signal line connector 530 is connected to the thermometer and the voltage drop line, and the signal line connector 530 is connected to a display device so as to monitor the temperature of the superconducting magnet and the voltage condition of the superconducting coil 210 in real time, thereby ensuring the normal operation of the superconducting magnet.
In an alternative embodiment, the superconducting magnet device further comprises a vacuum valve 540, wherein the vacuum valve 540 can provide a vacuum pumping channel for the magnetron czochralski single crystal superconducting magnet, and when the vacuum valve 540 is opened, the first chamber 120 obtains vacuum by connecting a vacuum pump, and the vacuum environment temperature is 300K. When the vacuum valve 540 is closed, a high vacuum level is maintained continuously in the first chamber 120. The high vacuum in the first chamber 120 can reduce the transfer of cold energy through the air in the second chamber 132, and can ensure a sufficiently low heat leak in the second chamber 132.
In an alternative embodiment, as shown in fig. 4 and 6, the pull rod assembly 30 includes a base 300 and a pull rod member, the base 300 being coupled to the bobbin 220. One end of the pull rod member is connected with the base 300, the other end of the pull rod member is connected with the first adjusting member, and the pull rod member passes through the first housing 110 and the second housing 131.
In the embodiment of the application, one end of the pull rod member is connected with the base 300, and the other end of the pull rod member is connected with the first adjusting member to the supporting cylinder 140, so that the coil frame 220 and the coil are suspended in the second chamber 132 by taking the supporting cylinder 140 as a supporting connection point.
In an alternative embodiment, as shown in FIG. 6, the pull rod member includes a first pin 310, a second pin 320, and an annular pull rod 356. The first pin 310 is connected to the base 300, and an axis of the first pin 310 is perpendicular to an axis of the first container 10. The second pin 320 is connected to the first housing 110, and an axis of the second pin 320 is parallel to an axis of the first pin 310. One end of the annular pull rod 356 is sleeved on the first pin shaft 310, the other end of the annular pull rod 356 is sleeved on the second pin shaft 320, and the annular pull rod 356 penetrates through the surfaces of the first shell 110 and the second shell 131. The second pin 320 is connected to the first adjusting member through a connection block.
The annular pull rod 356 is sleeved on the first pin shaft 310 and the second pin shaft 320, so that the posture of the superconducting magnet can be changed in a self-adaptive manner when the superconducting magnet is impacted in the transportation process, and the adaptability of the superconducting magnet is improved.
In an alternative embodiment, the annular tie 356 is made of a high strength carbon fiber material, which has the characteristics of light weight and high strength, and also has a low thermal conductivity, so that heat conduction can be reduced, and heat leakage can be reduced. The annular pull rod 356 of carbon fiber material bears the weight of the superconducting coils 210 and the coil bobbin 220 and the impact force during transportation, ensuring the structural stability of the superconducting magnet device.
The annular pull rod 356 passes through the first housing 110 and the second housing 131, so that a gap is formed between the annular pull rod 356 and the first housing 110 and the second housing 131, and the gap is easy to leak heat.
In an alternative embodiment, the annular pull rod 356 is divided into two independent first pull rod 350 and second pull rod 360 in the embodiment of the present application, for the gap between the annular pull rod 356 and the first and second housings 110 and 131 is prone to heat leakage.
Specifically, as shown in fig. 7, the pull rod member further includes a third pin 330, a fourth pin 340, a pair of connection plates 370, and a copper strap 380. The axis of the fourth pin 340 and the axis of the third pin 330 are both parallel to the axis of the first pin 310 or the second pin 320, the fourth pin 340 is located within the second chamber 132, and the third pin 330 is located outside the second chamber 132.
The two ends of the fourth pin 340 and the two ends of the third pin 330 are respectively connected to a pair of connecting plates 370, one end of the connecting plate 370 is located in the second chamber 132, and the other end of the connecting plate 370 is located in the first chamber 120. The copper pads 380 are connected to the second housing 131 by a pair of connection plates 370 at both ends of the copper pads 380.
The annular pull rod 356 includes a first pull rod 350 and a second pull rod 360, two ends of the first pull rod 350 are respectively sleeved on the second pin 320 and the third pin 330, and two ends of the second pull rod 360 are respectively sleeved on the fourth pin 340 and the first pin 310.
That is, the present embodiment divides the ring-shaped tie rod 356 into two independent first and second tie rods 350 and 360, and connects the first and second tie rods 350 and 360 by means of a pair of connection plates 370, while adding the third and fourth pins 330 and 340. In addition, the copper soft parts 380 are connected between the pair of connecting plates 370 and the second shell 131, so that the gap between the second shell 131 and the pull rod piece is greatly reduced, and the heat leakage is reduced. The pair of connection plates 370 is made of heat sink material, and can reduce heat leakage.
In an alternative embodiment, as shown in fig. 1, a plurality of the tie bar assemblies 30 are distributed on the upper end surface and the lower end surface of the first housing 110, and the tie bar assemblies 30 located on the upper end surface correspond to the tie bar assemblies 30 located on the lower end surface in the axial direction of the first container 10.
When one or more pull rod assemblies 30 need to be adjusted, the pull rod assemblies 30 on the upper end face of the first housing 110 are matched with the pull rod assemblies 30 on the corresponding lower end face thereof to adjust, so that the adjustment effect and the adjustment precision of the superconducting magnet are improved. As an example, when one of the tie rod assemblies 30 needs to be adjusted upward by 1mm to achieve adjustment of the superconducting magnet, the adjustment nut 410 of the tie rod assembly 30 on the upper end surface of the first housing 110 needs to be loosened, and at the same time, the adjustment nut 410 of the tie rod assembly 30 on the lower end surface of the first housing 110 corresponding thereto needs to be loosened.
The number of the tie rod assemblies 30 on the superconducting magnet device is not limited in the embodiment of the present application, and may be set according to the volume of the superconducting magnet.
The embodiment of the application also provides a method for adjusting the superconducting magnet device provided by any of the embodiments, as shown in fig. 8, the adjusting method includes the following steps:
S01, after excitation of the superconducting magnet is completed, selecting a first measuring circle by taking the center of a crucible in the single crystal furnace as a circle center.
On the mechanical center surfaces of the upper end surface and the lower end surface of the first container, a radius R is selected as a first measuring circle by taking the center of the crucible of the single crystal furnace as the center of a circle. And selecting a plurality of points on the first measuring circle as measuring points.
In an alternative embodiment, the radius R is less than or equal to the radius of the crucible. The magnetic field generated by the superconducting magnet acts on the silicon melt in the crucible, and in the adjustment process, the radius R of the first measuring circle is selected to be smaller than the radius of the crucible, so that the method is closer to actual operation, and the adjustment accuracy of the superconducting magnet is improved.
In an alternative embodiment, as shown in fig. 9, the position angle and number of the tie rod assembly, i.e., the adjustment assembly, on the superconducting magnet device is defined. As an example, the superconducting magnet device includes eight tie-rod assemblies, and four tie-rod assemblies located at the upper end surface of the first container are numbered No. 1, no. 2, no. 3 and No. 4 in order, and angles corresponding to No. 1, no. 2, no. 3 and No. 4 are 0 degrees, 90 degrees, 180 degrees and 270 degrees, respectively. The four pull rod assemblies positioned on the lower end face of the first container are numbered No. 5, no. 6, no. 7 and No. 8 in sequence, and the angles corresponding to the No. 5, no. 6, no. 7 and No. 8 are 0 degree, 90 degrees, 180 degrees and 270 degrees.
The number of the pull rod assemblies on the superconducting magnet device is not limited in the embodiment of the application, and can be set according to the volume of the superconducting magnet.
S02, selecting a plurality of measuring points on the first measuring circle, wherein the distances between adjacent measuring points are equal.
As an example, the radius of the first measuring circle is 300mm, 24 measuring points are selected on the first measuring circle, and the angles of travel between adjacent measuring points are equal and are all 15 degrees.
S03, obtaining a radial magnetic field measured value and an axial magnetic field measured value of each measuring point through measurement.
The radial magnetic field measured value and the axial magnetic field measured value of each measuring point are obtained through measurement of the magnetic field measuring instrument.
S04, adjusting the relative position of the center of the crucible and the center of the zero magnetic surface of the magnetic field generated by the superconducting magnet based on the radial magnetic field measured value so as to enable the center of the crucible to coincide with the center of the zero magnetic surface of the magnetic field.
In theory, after the superconducting magnet device is assembled around the single crystal furnace, the mechanical center surfaces of the upper end surface and the lower end surface of the superconducting magnet, namely the center of the magnetic field zero magnetic surface, coincide with the center of the crucible, and the measured values of all the measured points of the first measuring circle are equal, but in practice, errors exist after the assembly is completed, the relative positions of the two are adjusted through measuring the radial magnetic field, and the center of the crucible coincides with the magnetic field zero magnetic surface center, so that the subsequent crystal pulling quality is ensured.
S05, adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on the axial magnetic field measured value so that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible.
The step and the step S04 are respectively adjusted from the axial direction and the radial direction of the magnetic field, and when the center of the crucible in the step S04 is overlapped with the center of the magnetic field zero magnetic surface, the step adjusts the levelness of the magnetic field zero magnetic surface based on the axial magnetic field measured value and enables the magnetic field zero magnetic surface to be parallel to the liquid level of the silicon melt in the crucible.
It will be appreciated that, in theory, the axial magnetic field measurement value of each measurement point on the first measurement circle is zero, but in practice, the axial magnetic field measurement value of each measurement point on the first measurement circle may or may not be zero, the position of the superconducting magnet in the axial direction thereof is adjusted based on the axial magnetic field measurement value of each measurement point, and the adjustment of the magnetic field zero magnetic surface is realized by adjusting the pull rod assembly at the corresponding position of each measurement point.
In an alternative embodiment, as shown in fig. 10, step S04 further includes the steps of:
S041, obtaining a standard value of a radial magnetic field of the measuring point. The standard value of the radial magnetic field of the measuring point can be obtained through calculation.
S042, determining the minimum standard deviation value of the plurality of measuring points on the first measuring circle based on the radial magnetic field measured values and the standard values of the plurality of measuring points.
S043, judging whether the minimum standard deviation value is smaller than or equal to a first set value.
S044, if yes, judging that the liquid level of the silicon melt in the crucible and the zero magnetic surface of the superconducting magnet are concentric circles.
And S045, if not, adjusting the relative positions of the center of the crucible and the center of the zero magnetic surface of the magnetic field based on analysis of a plurality of measuring points.
In the embodiment of the application, the uniformity of the radial magnetic field measured values of the plurality of measuring points is determined by using the minimum standard deviation, and when the minimum standard deviation is larger than the first set value, the uniformity of the radial magnetic field measured values of the plurality of measuring points can be judged to be poor, and the relative positions of the crucible and the superconducting magnet are required to be adjusted. When the minimum standard deviation value is smaller than or equal to the first set value, the coincidence of the center of the crucible and the center of the zero magnetic surface of the magnetic field can be judged.
In an alternative embodiment, as shown in fig. 11, when the minimum standard deviation is greater than the first set value in step S045, the relative position of the crucible center and the magnetic zero surface center of the magnetic field is adjusted based on analysis of a plurality of measurement points, where the analysis of the plurality of measurement points specifically includes the following steps:
s0451, calculating to obtain an average value of radial magnetic field measured values of a plurality of measuring points.
S0452, calculating to obtain the difference value between the average value and each radial magnetic field measured value.
S0453, at least obtaining the maximum value in the difference values.
And S0454, adjusting the relative position of the center of the crucible and the center of the superconducting magnet at least based on the maximum value in the difference value so that the center of the crucible coincides with the zero magnetic surface center of the magnetic field.
In the embodiment of the application, it is understood that the average value of the current radial magnetic field measurement value is calculated, the difference value between the average value and the current radial magnetic field measurement value is calculated, the largest value in the difference values is obtained, and the relative position of the center of the crucible and the zero magnetic surface of the magnetic field is adjusted based on the largest value. And after the adjustment is finished, measuring each measuring point, calculating a minimum standard deviation value, and judging whether the center of the crucible is coincident with the center of the zero magnetic surface of the magnetic field or not based on the minimum standard deviation value. The adjustment can be performed circularly for a plurality of times until the minimum standard deviation value is smaller than or equal to the first set value.
In an alternative embodiment, the adjustment can be made not only based on the one of the differences with the largest value, but also based on the larger value of the first few of the differences, such as: the first three differences are arranged from high to low.
In an alternative embodiment, as shown in fig. 12, the step S05 further includes the steps of:
S051 adjusts the position of the superconducting magnet at the position corresponding to the at least one measurement point in the axial direction thereof based on the analysis of the axial magnetic field measurement value.
The second measuring circle is selected by taking the center of the crucible as the center of the circle, the radius of the second measuring circle is larger than the radius of the crucible, namely the area of the second measuring circle is larger than that of the crucible, a plurality of measuring points on the second measuring circle with larger area are measured, the position and the posture of the superconducting magnet are adjusted by the measuring points, and the adjustment precision can be improved.
The axial magnetic field measurement value, i.e. the initial magnetic field before the adjustment of the superconducting magnet, adjusts the position of the superconducting magnet in its axial direction at the corresponding position of the one or more measurement points by analysis of the axial magnetic field measurement value.
In an alternative embodiment, as shown in fig. 13, step S051 further includes:
s0511, calculating to obtain an average value of axial magnetic field measured values of a plurality of measuring points.
And S0512, calculating to obtain the difference value between the average value and each axial magnetic field measured value.
And S0513, obtaining at least the maximum value of the difference values.
S0514, adjusting the position of the superconducting magnet at the position corresponding to the measurement point corresponding thereto in the axial direction thereof based on at least the maximum value of the difference values.
In the embodiment of the application, the axial magnetic field measured value is obtained by measuring each measuring point, namely, the initial magnetic field calculation average value is obtained, the difference value between the average value and each axial magnetic field measured value is calculated, the maximum value in a plurality of difference values or the first few larger numerical values in a large-to-small array in the plurality of difference values are obtained, and the position of the superconducting magnet corresponding to the numerical value in the axial direction is adjusted based on the maximum value in the difference values or the numerical values close to the maximum value.
It is understood that the superconducting magnet at one or more corresponding positions of the plurality of axial magnetic field measurement values, which are greatly different from the average, is adjusted to improve the uniformity of the plurality of axial magnetic field measurement values and further improve the levelness of the magnetic field zero magnetic surface.
S052, obtaining the current axial magnetic field measurement value of each measurement point through measurement.
After the position and the posture of the superconducting magnet are adjusted in step S0514, the current axial magnetic field measurement value is obtained by measuring each measurement point.
It should be noted that, when the position and the posture of the superconducting magnet are adjusted each time, even if only the position of one pull rod assembly on the superconducting magnet is adjusted, the position and the posture of other measuring points are affected. Therefore, each measurement point needs to be measured again after each adjustment of the superconducting magnet position and orientation.
As shown in fig. 14, the graph shown in fig. 14 is a graph of the amount of change in the magnetic field generated at the second measuring circle after the tie rod assembly at 90 degrees in fig. 9 is adjusted upward by 1 mm. As is clear from fig. 14, the magnetic field variation amount is largest at 90 degrees, and changes at positions close to 90 degrees.
S053, calculating a difference value between the current axial magnetic field measured value and the axial magnetic field measured value.
S054, calculating the adjustment distance of the superconducting magnet at the corresponding position of each measuring point in the axial direction.
S055, calculating root mean square values of the axial magnetic fields of the plurality of measurement points after adjustment based on the adjustment distance and the difference value between the current axial magnetic field measurement value and the axial magnetic field measurement value.
Calculating an optimization equation by a linear programming method: min BZm (BZ (θ) =bz 0 (θ) +d1×f1 (θ) + … +d8×f8 (θ)). Wherein, F1 (θ) to F8 (θ) are the magnetic field variation of each measuring point after adjustment, D1 to D8 are the adjustment distance of the pull rod assembly at the corresponding position of each measuring point, BZ0 (θ) is the axial magnetic field measurement value, namely the initial magnetic field, and BZm is the minimum, namely the minimum root mean square value of the axial magnetic fields of a plurality of measuring points, and the levelness of the magnetic field zero magnetic surface is the best.
S056, judging whether the root mean square value is smaller than or equal to a second set value.
S057, if so, judging that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible.
The minimum root mean square value is zero in step S056, which is the most ideal state, but cannot be practically achieved. And when the root mean square value is smaller than or equal to a second set value, judging that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible.
S058, if not, adjusting the position of the superconducting magnet at the corresponding position of the measuring point in the axial direction based on analysis of the current axial magnetic field measured value.
If the rms value is greater than the second set value, further adjustment is required to be performed on the magnetic field zero magnetic plane, and the adjustment method is similar to steps S0511 to S0514, namely, the average value of the current axial magnetic field measurement values is calculated, the differences between the current axial magnetic field measurement values and the average value are calculated, at least the maximum value in the differences is obtained, and the positions of the superconducting magnet at the positions corresponding to the measurement points in the axial direction are adjusted based on the maximum value or the values close to the maximum value in the differences.
After finishing the adjustment, measuring each measuring point again, calculating a minimum root mean square value again on the currently obtained axial magnetic field measuring value, judging whether the minimum root mean square value is smaller than or equal to a second set value, and stopping the adjustment when the minimum root mean square value is smaller than the second set value; otherwise, the measurement, calculation and judgment are circularly carried out.
As shown in fig. 15 and 16, the axial magnetic field measurement values of the plurality of measurement points before the magnetic field zero magnetic surface adjustment are shown in fig. 15, the maximum axial magnetic field measurement value is 23GS at 300 degrees, the minimum axial magnetic field measurement value is-5 GS at 148 degrees, and the difference between the maximum value and the minimum value of the axial magnetic field measurement values of the plurality of measurement points shown in fig. 15 is 28GS. Fig. 16 shows axial magnetic field measurement values of a plurality of measurement points of the magnetic field zero magnetic surface after adjustment, the uniformity is better from the axial magnetic field measurement values of the plurality of measurement points shown in fig. 16, the maximum axial magnetic field measurement value is 1.4GS at 45 degrees, the minimum axial magnetic field measurement value is-1.7 GS at a position around 310 degrees, and the difference between the maximum value and the minimum value of the axial magnetic field measurement values of the plurality of measurement points shown in fig. 16 is 3.1GS. After the adjustment method of the superconducting magnet device provided by the embodiment of the application is applied to the adjustment of the magnetic field zero magnetic surface, the uniformity of the axial magnetic field measured value and the radial magnetic field measured value of the measuring point is greatly improved, and the levelness of the magnetic field zero magnetic surface is further improved.
It should be understood that the above examples are illustrative and are not intended to encompass all possible implementations encompassed by the claims. Various modifications and changes may be made in the above embodiments without departing from the scope of the disclosure. Likewise, the individual features of the above embodiments can also be combined arbitrarily to form further embodiments of the application which may not be explicitly described. Therefore, the above examples merely represent several embodiments of the present application and do not limit the scope of protection of the patent of the present application.
Claims (10)
1. The method for adjusting the superconducting magnet device is characterized by comprising a first container and a coil assembly, wherein the first container comprises a first shell, a closed first cavity is formed in the inner cavity of the first shell, a first through hole is formed in the first shell in a surrounding mode, the first through hole is used for accommodating a single crystal furnace, and the single crystal furnace is used for placing a crucible for bearing silicon solution; the coil assembly is positioned in the first cavity, and comprises a superconducting coil, wherein the superconducting coil is used for generating a magnetic field and acting on silicon melt in the crucible, and is a core component of a superconducting magnet; the adjusting method comprises the following steps:
Obtaining a radial magnetic field measured value and an axial magnetic field measured value at each of a plurality of measuring points on a first measuring circle through measurement, wherein the center of the first measuring circle is the center of a crucible in a single crystal furnace, the plane of the first measuring circle is parallel to the mechanical center plane of the upper end face and the lower end face of the first container, the distances between the adjacent measuring points are equal, and the superconducting magnet is a superconducting magnet after excitation;
Adjusting the relative position of the center of the crucible and the center of the magnetic field zero magnetic surface generated by the superconducting magnet based on the radial magnetic field measurement value so that the center of the crucible coincides with the center of the magnetic field zero magnetic surface;
and adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on the axial magnetic field measured value so that the magnetic field zero magnetic surface is parallel to the liquid level of the silicon melt in the crucible.
2. The method of adjusting a superconducting magnet apparatus according to claim 1, wherein adjusting the relative position of the center of the crucible and the center of the zero magnetic surface of the magnetic field generated by the superconducting magnet based on the radial magnetic field measurement value comprises:
obtaining a standard value of a radial magnetic field of the measuring point;
Determining a minimum standard deviation of a plurality of measurement points on the first measurement circle based on the radial magnetic field measurement values of the plurality of measurement points and the standard value;
judging whether the minimum standard deviation value is smaller than or equal to a first set value;
if yes, judging that the center of the crucible is coincident with the center of the magnetic field zero magnetic surface;
If not, adjusting the relative positions of the center of the crucible and the center of the zero magnetic surface of the magnetic field based on analysis of a plurality of measurement points.
3. The adjustment method of the superconducting magnet device according to claim 2, characterized in that adjusting the relative position of the center of the crucible and the center of the magnetic field zero-magnetic surface based on analysis of a plurality of the measurement points, comprises:
Calculating an average value of the radial magnetic field measured values of a plurality of measuring points;
Calculating a difference between the average value and each of the radial magnetic field measurements;
Obtaining at least a maximum value of the differences;
and adjusting the relative position of the center of the crucible and the center of the superconducting magnet based on at least the maximum value in the difference value so that the center of the crucible coincides with the zero magnetic surface center of the magnetic field.
4. The adjustment method of the superconducting magnet apparatus according to claim 1, characterized in that adjusting the position of the measurement point in the axis direction of the superconducting magnet based on the axial magnetic field measurement value so that the magnetic field zero magnetic surface is parallel to the silicon melt level in the crucible, comprises:
Adjusting the position of the superconducting magnet in the axial direction of the superconducting magnet at least at one measurement point corresponding to the position based on analysis of the axial magnetic field measurement value;
Obtaining a current axial magnetic field measured value of each measuring point through measurement;
calculating a difference between the current axial magnetic field measurement value and the axial magnetic field measurement value;
calculating the adjustment distance of the superconducting magnet at the corresponding position of each measuring point in the axial direction of the superconducting magnet;
calculating root mean square values of the axial magnetic fields of the plurality of measurement points after adjustment based on the adjustment distance and the difference value between the current axial magnetic field measurement value and the axial magnetic field measurement value;
Judging whether the root mean square value is smaller than or equal to a second set value;
If yes, judging that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible;
if not, adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on analysis of the current axial magnetic field measured value.
5. The adjustment method of a superconducting magnet apparatus according to claim 4, wherein adjusting the position of at least one of the measurement points in the superconducting magnet axis direction based on the analysis of the axial magnetic field measurement values includes:
Calculating an average value of the axial magnetic field measured values of a plurality of measuring points;
calculating a difference value between the average value and each axial magnetic field measured value;
Obtaining at least a maximum value of the differences;
the position of the superconducting magnet in the axial direction thereof at the position corresponding to the measurement point corresponding thereto is adjusted based on at least the maximum value of the difference values.
6. The adjustment method of a superconducting magnet apparatus according to claim 4, wherein adjusting the position of at least one of the measurement points in the superconducting magnet axis direction based on the analysis of the axial magnetic field measurement values includes:
Calculating an average value of the axial magnetic field measured values of a plurality of measuring points;
calculating a difference value between the average value and each axial magnetic field measured value;
Sequentially arranging a plurality of differences from large to small;
The positions of the superconducting magnets at the positions corresponding to the measurement points corresponding thereto are adjusted in the axial direction thereof based on the plurality of difference values arranged forward.
7. The method of adjusting a superconducting magnet device according to any one of claims 4 to 6, wherein a plurality of measurement points on a second measurement circle having a radius larger than the crucible radius are obtained by measurement.
8. The method of adjusting a superconducting magnet device according to claim 1, further comprising a plurality of adjustment assemblies and a plurality of pull rod assemblies, wherein one end of each pull rod assembly is located in the first chamber and connected to the coil assembly, and the other end of each pull rod assembly is connected to the adjustment assembly;
adjusting the relative position of the center of the crucible and the center of the zero magnetic surface of the magnetic field generated by the superconducting magnet based on the radial magnetic field measurement value, comprising:
And regulating the magnetic field zero magnetic surface generated by the superconducting magnet by utilizing a plurality of regulating components, and enabling the center of the magnetic field zero magnetic surface to coincide with the center of the crucible.
9. The method of adjusting a superconducting magnet device according to claim 8, wherein a plurality of the measurement points on the first measurement circle correspond to positions of a plurality of the adjustment members;
Adjusting the position of the superconducting magnet at the position corresponding to the measuring point in the axial direction based on the axial magnetic field measured value so that the magnetic field zero magnetic surface is parallel to the silicon melt liquid level in the crucible, wherein the method comprises the following steps:
and adjusting the positions of the superconducting magnets at the positions corresponding to the measuring points in the axial direction by utilizing a plurality of adjusting assemblies so that the zero magnetic surface of the magnetic field is parallel to the liquid level of the silicon melt in the crucible.
10. The method of adjusting a superconducting magnet device according to claim 1, wherein a radius of the first measurement circle is equal to or smaller than a radius of the crucible.
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