US3121619A - Zone-melting method and apparatus - Google Patents
Zone-melting method and apparatus Download PDFInfo
- Publication number
- US3121619A US3121619A US63345A US6334560A US3121619A US 3121619 A US3121619 A US 3121619A US 63345 A US63345 A US 63345A US 6334560 A US6334560 A US 6334560A US 3121619 A US3121619 A US 3121619A
- Authority
- US
- United States
- Prior art keywords
- coil
- coils
- given
- frequency
- zone
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000004857 zone melting Methods 0.000 title claims description 16
- 238000000034 method Methods 0.000 title description 18
- 239000007787 solid Substances 0.000 claims description 8
- 238000012986 modification Methods 0.000 claims description 5
- 230000004048 modification Effects 0.000 claims description 5
- 238000009826 distribution Methods 0.000 description 5
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- 239000003795 chemical substances by application Substances 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000005265 energy consumption Methods 0.000 description 2
- 229910052732 germanium Inorganic materials 0.000 description 2
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000001627 detrimental effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
Images
Classifications
-
- C—CHEMISTRY; METALLURGY
- C25—ELECTROLYTIC OR ELECTROPHORETIC PROCESSES; APPARATUS THEREFOR
- C25D—PROCESSES FOR THE ELECTROLYTIC OR ELECTROPHORETIC PRODUCTION OF COATINGS; ELECTROFORMING; APPARATUS THEREFOR
- C25D11/00—Electrolytic coating by surface reaction, i.e. forming conversion layers
- C25D11/02—Anodisation
- C25D11/04—Anodisation of aluminium or alloys based thereon
- C25D11/18—After-treatment, e.g. pore-sealing
- C25D11/24—Chemical after-treatment
- C25D11/246—Chemical after-treatment for sealing layers
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B13/00—Single-crystal growth by zone-melting; Refining by zone-melting
- C30B13/28—Controlling or regulating
- C30B13/30—Stabilisation or shape controlling of the molten zone, e.g. by concentrators, by electromagnetic fields; Controlling the section of the crystal
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T117/00—Single-crystal, oriented-crystal, and epitaxy growth processes; non-coating apparatus therefor
- Y10T117/10—Apparatus
- Y10T117/1024—Apparatus for crystallization from liquid or supercritical state
- Y10T117/1076—Apparatus for crystallization from liquid or supercritical state having means for producing a moving solid-liquid-solid zone
- Y10T117/1084—Apparatus for crystallization from liquid or supercritical state having means for producing a moving solid-liquid-solid zone having details of a stabilizing feature
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T117/00—Single-crystal, oriented-crystal, and epitaxy growth processes; non-coating apparatus therefor
- Y10T117/10—Apparatus
- Y10T117/1024—Apparatus for crystallization from liquid or supercritical state
- Y10T117/1076—Apparatus for crystallization from liquid or supercritical state having means for producing a moving solid-liquid-solid zone
- Y10T117/1088—Apparatus for crystallization from liquid or supercritical state having means for producing a moving solid-liquid-solid zone including heating or cooling details
Definitions
- FIG.6 is a diagrammatic representation of FIG.6.
- This invention relates to methods of manufacturing rod-like bodies by zone melting with the use of a magnetic high-frequency field produced by a coil and extending in the axial direction of the rod, a molten zone being formed inside the coil. It also relates to apparatus for zone-melting rod-like bodies by means of inductive high-frequency heating.
- An object of the invention is inter alia to provide a method which permits of influencing the shape of the boundary surfaces, more particularly of obtaining flatter boundary surfaces. 7
- At least one other field viewed in the axial direction adjacent and of opposite sense to the first field is produced by the addition of at least one additional coil without a molten zone being formed inside the last-mentioned coil.
- the two fields must naturally have the same frequency.
- a high frequency current should pass through the additional coil 'in a sense opposite to that of the current through the first coil.
- the induction current produced in the additional coil by the first field is in itself too small to be able to produce a resultant field of opposite sense.
- the method according to the invention must not be confused with the conventional method of purifying by zone-melting a rod-like body in an elongated crucible, wherein a few molten zones are produced inside a corresponding number of high-frequency coils and wherein juxtaposed coils are traversed by a high-ire quency current in opposite directions for the purpose of preventing the zones from melting together.
- the fields of the coils associated with these zones usually have the same intensity in contradistinction to the fields of the coilsin the method according to the invention wherein the intensity of the field of the additional coil is less than the intensity of. the field of the first coil.
- the first-mentioned intensity is at most two thirds and at least one third of the last-mentioned intensity.
- the intensity of a field produced by one coil is to be understood to mean herein the average field strength within this coil, when no other partial fields, produced by other coils, are present.
- Two oppositely directed fields are preferably produced on each side of the first-mentioned field.
- a device is characterized in that it comprises at least two such juxtaposed coils which coaxially surround a body and are coupled so as to be traversed by high-frequency currents of different intensities in opposite directions.
- Each coil prefer-ably comprises only one turn.
- Use is preferably made of three coils which are connected together so that the central coil is connected in series with the two outer coils, which are interconnected in parallel.
- the distance between adjacent coils is preferably at least equal to the distance of the central coil to the surface of the rod-like body and at most twice the diameter of the central coil.
- FIG. 1 shows, partly in vertical section and partly in elevation, a portion of a device for fioating-zone-melting, wherein one molten zone is produced in a rod-like body.
- FIGURE 2 shows a similar rod-like body having a molten zone formed in a different way
- FIGURE 3 shows, for comparison, a similar molten zone such as produced in conventional methods.
- FIGURE 4 shows schematically a circuit for feeding the coils of the apparatus of FIG. 1.
- FIGURE 5 shows schematically the field distribution caused by the action of the three coils of FIG. 1.
- FIGURE 6 shows schematically in vertical cross-section the heat-transport in a silicon rod, disposed within the high-frequency coils of FIGURE 1.
- a rod-like body for example of silicon or germanium, is secured at each end (not shown) to the device by means of holders (not shown).
- a molten zone 3 is produced in the rod 1 by the field of a high-frequency coil 2 surrounding the rod, which coil consists of a single turn and is fed from a high-frequency current generator (not shown).
- the device also comprises two high-frequency coils 4' and 5 which are arranged coaxially with the coil 2 on each side thereof.
- Each of the coils 4 and 5 consist of a single turn and can be fed by the same high-frequency current generator.
- the currents traversing the coils 4 and 5 have opposite directions to that of the current through the coil 2, as indicated by arrows.
- the current strength in the coil 4 and in the coil 5 is smaller than that in the coil 2.
- the currents in the coils 4 and 5 may be for example, half the current in the coil 2, which may be realised in a simple manner by connecting the central coil in series with the two outer coils and connecting the last-mentioned coils in parallel.
- FIGURE 4 shows schematically a circuit for zone-melting with the aid of the coils 2, 4i and 5 of FIGURE 1.
- the linevoltage is supplied via an ammeter A to atransformer with adjustable primary to adjust the output of the transformer which is supplied. to a rectifier arrangement.
- the output of the rectifier constitutes the DC. supply for a. high frequency generator the high frequency output of which is supplied to the high frequency coils 2, 4 and 5 in a way as shown by the arrows.
- the high frequency current from the generator will. pass coil 2. after which it is divided into two parts which pass the coils 4 and 5 respectively in a sense opposite to the sense in which the current passes the coil 2.
- Leads for combining the currents passed through the coils 4 and 5 and for conducting the resulting combined current back to the generator are present.
- the intensity of the current in each of the coils 4 and 5 will thus be about half the intensity of the current in coil 2. 7
- the current intensity by the ammeter is also a measure of the energy consumption of nearly all the energy being consumed by the fields of the high frequency coils.
- adjusting the transformer the output of the generator and the energy consumption of the fields of the coils may be controlled. In this way it is possible to control the length of the molten zone 3 of FIGURE 1 by observation and adjustment of the transformer.
- the boundaries or interfaces 6 and 7 of the molten zone and the two solid parts 8 and 9 of the rod are comparatively flat, as shown in FIGURE 1.
- the molten zone may be moved along the rod in the usual known manner.
- the coils could be fixed in position and the rod ll moved vertically, or the rod 1 fixed and the coils 2, 4 and 5 fixedly interconnected in the relationship illustrated in FIG. 1 and moved as a whole along the length of the rod, a typical rate being about 1 mm. per minute.
- the coil 2 may comprise a 4 mm. wire forming a single turn 25 rnms. in diameter.
- the coils 4 and 5 may be of the same size wire and have the same diameter, and are each spaced between 15 and 25 mms, for example about 20 mms, vertically from the center turn 2.
- a 6 kilowatt generator at a frequency of 5 megacycles per second may be employed.
- FIGURE 3 shows, for comparison, the shape of the convex boundary surfaces such as usually formed by known methods.
- This figure also shows that in the known method, when a comparatively long molten zone is produced, the distance between the non-melted parts of the rod is small, so that more particularly in the case of thick rods the risk is involved that the Zone cannot penetrate to the core of the rod for the maximum permissible length of the zone as limited by the surface tension. This risk is less for boundary surfaces such as obtained by the method accordin to the invention and, in addition, the growing part of the rod contains fewer disturbances in the crystal lattice because of the fiat shape of these boundary surfaces.
- FIG. 5 shows schematically in a diagram the magnetic field strength distribution in the axial direction of the coils.
- the axis" of abscissa indicates the field strength and the axis of ordinates the distance from the center coil 2.
- the points 11 and 12 indicate points within the coils 4 and 5 respectively.
- the dot-dash curve 13 indicates the partial field strength of the field produced by the coil 2 alone.
- heat will be generated at a large part of the surface of the rod 1 of FIGURE 6.
- the heat currents 14 will run from quite large surface parts within and near the coil 2 to the interior of the rod ll.
- the dashed curve 15 perpendicular to the curves 14 indicates an isotherm which is at the axis of the rod measured in the axial direction for nearer to the coil 2 than at the surface of the rod.
- FIG. 5 may be represented in FIG. 5 by the interrupted curves 16 and 17 respectively.
- the action of the three coils together will give rise to a resultant field distribution as indicated by the full curve 18.
- the resultant field strength is zero.
- a field is mainly set up by the action of the center coil 2.
- On both sides of this field a resultant field of opposite sense exists caused by the action of the outer coils 4 and 5.
- the isotherms 26 and 27 will be approximately flat, the distance between the isotherm 2'7 and the coils, measured in the axial direction, being at the center of the rod even somewhat larger than at the surface of the rod.
- These isotherms may explain that the boundary of the molten zone may have a substantially flat form as shown in FIGURE 1 or even a concave form as shown in FIGURE 2.
- the present invention also permits the length of the zone to be kept small, more particularly at the free surface of the rod, thus limiting the risk that this zone may flow out forrnaterials having a comparatively low surface tension, such as germanium.
- High-frequency zone-melting apparatus comprising means for supporting an elongated body, at least two juxtaposed coils surrounding the body, means for applying to one of the two coils high-frequency current of given frequency in a given sense and of a magnitude establishing a magnetic field in a given direction in the body portion within the said one coil producing therein a molten zone with a given liquid-solid interface adjacent the other of the two coils, and means for applying to the other of the two coils high-frequency current of said given frequency but in a sense opposite to said given sense and of a lower magnitude establishing in the body portion
- Within the said other coil a magnetic field intensity between about one-third and two-thirds that in the body portion within the said one coil and a resultant field within the other coil in a direction opposite to said given direction, said resultant field being insufiicient to establish a molten zone in the body portion within the said other coil but causing a modification of the shape of the liquid-solid interface of the molten zone produced by the said one
- High-frequency zone-melting apparatus comprising means for supporting an elongated body, at least three juxtaposed coils surrounding the body, means for applying to the center coil of the three coils high-frequency current of given frequency, in a given sense and of a magnitude establishing a magnetic field in a given direction in the body portion within the said center coil producing therein a molten zone with a given liquidsolid interface adjacent the outer two coils, and means for applying to the outer two coils high-frequency currents of said given frequency but in a sense opposite to said given sense and of a lower magnitude establishing in the body portions within the said outer coils a field intensity between about one-third and two-thirds that in the body portion within the said center coil and a resultant field within the outer coils in a direction opposite to said given direction, said resultant field being insufiicient to establish a molten zone in the body portions within the said outer coils but causing a modification of the shape of the liquidsolid interface of the molten zone produced by the said center coil
- a method of zone-melting an elongated body comprising providing two juxtaposed coils surrounding the body, passing through one of the two coils high-frequency current in a given sense and of a magnitude sufficient to establish a magnetic field in a given direction and a molten zone within the body portion within the said one coil forming an interface of given shape with the contiguous solid portions, and passing through the other of the two coils high-frequency current of the same frequency but of opposite sense and of a magnitude insulficient to establish a molten zone within the body portion within the said other coil, said latter current being controlled to establish in the body portion Within the said other coil a magnetic field having an intensity between about one-third and two-thirds that established within the body portion within the said one coil and producing within the body portion within the said other coil a resultant magnetic field in a direction opposite to said given direction resulting in a modification of the shape of the interface of the molten zone within the said one coil.
- a method of zone-melting an elongated body comprising providing three juxtaposed coils surrounding the body, passing through the center coil high-frequency current at a given frequency, in a given sense and of a magnitude sufficient to establish a magnetic field in a given direction and a molten zone within the body portion within the center coil forming an interface of a given shape with the contiguous solid portions, and passing through the outer two coils high-frequency currents of the same given frequency but of opposite sense to said given sense and of a magnitude insufiicient to establish a molten zone within the body portions within the outer two coils, said latter currents being controlled to establish in the body portions within the outer two coils a magnetic field having an intensity between one-third and two-thirds that established within the body portion within the center coil and producing within the body portions within the outer coils a resultant magnetic field in a direction opposite to said given direction resulting in a modification of the shape of the interface of the molten zone within the center coil.
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- Chemical & Material Sciences (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Metallurgy (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Electrochemistry (AREA)
- General Chemical & Material Sciences (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Crystallography & Structural Chemistry (AREA)
- General Induction Heating (AREA)
- Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Furnace Details (AREA)
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NL244489 | 1959-10-19 |
Publications (1)
Publication Number | Publication Date |
---|---|
US3121619A true US3121619A (en) | 1964-02-18 |
Family
ID=19751988
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US63345A Expired - Lifetime US3121619A (en) | 1959-10-19 | 1960-10-18 | Zone-melting method and apparatus |
Country Status (5)
Country | Link |
---|---|
US (1) | US3121619A (de) |
CH (1) | CH425735A (de) |
DE (1) | DE1257740B (de) |
GB (1) | GB954991A (de) |
NL (2) | NL112520C (de) |
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3242015A (en) * | 1963-09-24 | 1966-03-22 | Monsanto Co | Apparatus and method for producing single crystal structures |
US3250842A (en) * | 1963-01-15 | 1966-05-10 | Atomic Energy Commission | Electron beam zone refining |
US3258314A (en) * | 1963-04-12 | 1966-06-28 | Westinghouse Electric Corp | Method for interior zone melting of a crystalline rod |
US3275417A (en) * | 1963-10-15 | 1966-09-27 | Texas Instruments Inc | Production of dislocation-free silicon single crystals |
DE1262978B (de) * | 1965-01-05 | 1968-03-14 | Siemens Ag | Verfahren zum Herstellen eines Halbleitereinkristalls |
US3649210A (en) * | 1965-07-10 | 1972-03-14 | Siemens Ag | Apparatus for crucible-free zone-melting of crystalline materials |
US3915660A (en) * | 1972-07-13 | 1975-10-28 | Siemens Ag | Preparing oriented semiconductor monocrystalline rods |
US5069742A (en) * | 1990-02-05 | 1991-12-03 | Bleil Carl E | Method and apparatus for crystal ribbon growth |
WO2004113596A1 (de) * | 2003-06-20 | 2004-12-29 | Leibniz-Institut Für Festkörper- Und Werkstoffforschung Dresden E.V. | Verfahren und vorrichtung zum ziehen von einkristallen durch zonenziehen |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109139639B (zh) * | 2018-08-24 | 2020-10-16 | 上海宇航***工程研究所 | 一种快速锁定的轻量化位姿可调连接机构 |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2743199A (en) * | 1955-03-30 | 1956-04-24 | Westinghouse Electric Corp | Process of zone refining an elongated body of metal |
US2897329A (en) * | 1957-09-23 | 1959-07-28 | Sylvania Electric Prod | Zone melting apparatus |
US2905798A (en) * | 1958-09-15 | 1959-09-22 | Lindberg Eng Co | Induction heating apparatus |
US3323091A (en) * | 1964-11-05 | 1967-05-30 | Honeywell Inc | Multicore transformer including integral mounting assembly |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
AT194444B (de) * | 1953-02-26 | 1958-01-10 | Siemens Ag | Verfahren und Einrichtung zur Behandlung einer längserstreckten Halbleiterkristallanordnung |
-
0
- NL NL244489D patent/NL244489A/xx unknown
- NL NL112520D patent/NL112520C/xx active
-
1960
- 1960-10-14 GB GB35302/60A patent/GB954991A/en not_active Expired
- 1960-10-15 CH CH1154560A patent/CH425735A/de unknown
- 1960-10-17 DE DEN19044A patent/DE1257740B/de active Pending
- 1960-10-18 US US63345A patent/US3121619A/en not_active Expired - Lifetime
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2743199A (en) * | 1955-03-30 | 1956-04-24 | Westinghouse Electric Corp | Process of zone refining an elongated body of metal |
US2897329A (en) * | 1957-09-23 | 1959-07-28 | Sylvania Electric Prod | Zone melting apparatus |
US2905798A (en) * | 1958-09-15 | 1959-09-22 | Lindberg Eng Co | Induction heating apparatus |
US3323091A (en) * | 1964-11-05 | 1967-05-30 | Honeywell Inc | Multicore transformer including integral mounting assembly |
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3250842A (en) * | 1963-01-15 | 1966-05-10 | Atomic Energy Commission | Electron beam zone refining |
US3258314A (en) * | 1963-04-12 | 1966-06-28 | Westinghouse Electric Corp | Method for interior zone melting of a crystalline rod |
US3242015A (en) * | 1963-09-24 | 1966-03-22 | Monsanto Co | Apparatus and method for producing single crystal structures |
US3275417A (en) * | 1963-10-15 | 1966-09-27 | Texas Instruments Inc | Production of dislocation-free silicon single crystals |
DE1262978B (de) * | 1965-01-05 | 1968-03-14 | Siemens Ag | Verfahren zum Herstellen eines Halbleitereinkristalls |
US3649210A (en) * | 1965-07-10 | 1972-03-14 | Siemens Ag | Apparatus for crucible-free zone-melting of crystalline materials |
US3915660A (en) * | 1972-07-13 | 1975-10-28 | Siemens Ag | Preparing oriented semiconductor monocrystalline rods |
US5069742A (en) * | 1990-02-05 | 1991-12-03 | Bleil Carl E | Method and apparatus for crystal ribbon growth |
WO2004113596A1 (de) * | 2003-06-20 | 2004-12-29 | Leibniz-Institut Für Festkörper- Und Werkstoffforschung Dresden E.V. | Verfahren und vorrichtung zum ziehen von einkristallen durch zonenziehen |
Also Published As
Publication number | Publication date |
---|---|
NL244489A (de) | |
GB954991A (en) | 1964-04-08 |
CH425735A (de) | 1966-12-15 |
DE1257740B (de) | 1968-01-04 |
NL112520C (de) |
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