US3124686A - Goorissen - Google Patents

Goorissen Download PDF

Info

Publication number
US3124686A
US3124686A US3124686DA US3124686A US 3124686 A US3124686 A US 3124686A US 3124686D A US3124686D A US 3124686DA US 3124686 A US3124686 A US 3124686A
Authority
US
United States
Prior art keywords
infra
red
enclosure
radiation
semiconductor material
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
Application number
Priority date (The priority date 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 date listed.)
Publication date
Application granted granted Critical
Publication of US3124686A publication Critical patent/US3124686A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/52Means for observation of the coating process
    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22FCHANGING THE PHYSICAL STRUCTURE OF NON-FERROUS METALS AND NON-FERROUS ALLOYS
    • C22F1/00Changing the physical structure of non-ferrous metals or alloys by heat treatment or by hot or cold working
    • C22F1/16Changing the physical structure of non-ferrous metals or alloys by heat treatment or by hot or cold working of other metals or alloys based thereon
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-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
    • C30B13/00Single-crystal growth by zone-melting; Refining by zone-melting
    • C30B13/28Controlling or regulating
    • C30B13/30Stabilisation or shape controlling of the molten zone, e.g. by concentrators, by electromagnetic fields; Controlling the section of the crystal
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-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
    • C30B15/00Single-crystal growth by pulling from a melt, e.g. Czochralski method
    • C30B15/20Controlling or regulating
    • C30B15/22Stabilisation or shape controlling of the molten zone near the pulled crystal; Controlling the section of the crystal
    • C30B15/26Stabilisation or shape controlling of the molten zone near the pulled crystal; Controlling the section of the crystal using television detectors; using photo or X-ray detectors
    • YGENERAL 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
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10TTECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
    • Y10T117/00Single-crystal, oriented-crystal, and epitaxy growth processes; non-coating apparatus therefor
    • Y10T117/10Apparatus
    • Y10T117/1004Apparatus with means for measuring, testing, or sensing
    • Y10T117/1008Apparatus with means for measuring, testing, or sensing with responsive control means
    • YGENERAL 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
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10TTECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
    • Y10T117/00Single-crystal, oriented-crystal, and epitaxy growth processes; non-coating apparatus therefor
    • Y10T117/10Apparatus
    • Y10T117/1024Apparatus for crystallization from liquid or supercritical state
    • Y10T117/1076Apparatus for crystallization from liquid or supercritical state having means for producing a moving solid-liquid-solid zone
    • Y10T117/1088Apparatus for crystallization from liquid or supercritical state having means for producing a moving solid-liquid-solid zone including heating or cooling details

Definitions

  • the enclosure has a wall made at least in part of a transparent material such as vitreous quartz in order to permit observation.
  • the invention utilizes the property of a semi-conductor material that it transmits infra-red radiation over a certain wavelength range in contradistinction to, for example, a metal, so that infra-red radiation of a wavelength within this range is also transmitted by the deposit of the semi-conductor material on the wall.
  • a conventional transparent wall portion of vitreous quartz is also permeable to such radiation.
  • an infra-red image converter is used for observing the material under treatment.
  • the term infra-red image converter as used herein denotes in general a device capable of converting an infra-red radiation image into an ice image of visible light.
  • the image converter may be an infra-red viewer known in the art, as described in Proceedings of the IRE. 47 (1959), No. 5, page 904, or a flat image intensifier sensitive to infrared radiation.
  • a camera tube sensitive to infra-red radiation may be used according to principles known from television, the signal delivered by this tube being converted into a visible image in a display tube.
  • the infra-red image converter must be sensitive to the infra-red radiation transmitted by the semi-conductor material concerned.
  • the wavelength range of the transmitted radiation is bounded at the short wave end by an absorption boundary of the semi-conductor material which is related to the energy spacing, hereinafter referred to as the band spacing, between the valency band and the conduction band of the semi-conductor material and which is situated at a smaller wavelength according as the band spacing is larger.
  • the heated semi-conductor material itself may serve as the source of infra-red radiation, however, this material may alternatively be irradiated by infra-red radiation.
  • an infra-red image converter may have further advantages, for example when mists occur during the treatment which disperseinfra-red radiation in a materially smaller degree and, if they consist of semi-conductor material, absorb this radiation to a lesser extent than visible radiation. Furthermore, when a layer of semi-conductor material is deposited on a support, the thickness of the layer can be determined during the deposition by means of interference of reflected infra-red radiation and this generally is not possible with visible radiation due to the frequently high absorptive power of the semi-conductor material for visible light.
  • infra-red image converter Although observation by means of an infra-red image converter generally will be satisfactory when using a conventional wall portion of vitreous quartz, use may also be made of wall portions made from other material transmitting infra-red radiation, for example portions consisting of infra-red transmitting glasses or a window made of the same material or of another semi-conductor material having a band spacing equal to or greater than that of the material to be treated.
  • reference numeral 1 denotes a vertical tube of vitreous quartz in which a vertical rod 2 of silicon is arranged.
  • This rod comprises two solid portions 3 and 4 secured at their upper and lower ends respectively in holders (not shown) and an intermediate substantially drop-shaped molten zone 5 heated by means of a high-frequency coil 6. Due to the high surface tension of the melt the molten zone 5 is held in place between the two rod portions 3 and 4-.
  • the vitreous quartz tube 1 and the rod 2 are gradually lowered vertically by means (not shown) in the direction indicated by an arrow, whereas the coil 6 does not change position so that the molten zone 5 passes through the silicon rod 2, the rod portion 3 gradually melting on at its lower end and the rod portion 4 gradually growing at its upper end.
  • the shape and the length of the molten zone 5 and the diameter or" the growing rod portion 4 can be controlled by adjusting the strength of the current in the high-frequency coil, which current is provided by a highfrequency generator (not shown). Owing to the high temperature of the melt, part of the silicon will evaporate from the zone 5 and be partly deposited as an opaque coating 7 on the inside of the vitreous quartz tube 1 so that observation of the zone with the naked eye is impeded.
  • the apparatus also includes an infra-red image converter shown diagrammatically in the drawing as an infra-red viewer 3 comprising a concentrating lens or lens system for infra-red radiation 9 and a vacuum tube ltl consisting of a photo-cathode 11 which is sensitive to infra-red radiation of a wavelength exceeding 1.1 the absorption boundary of silicon, a set of electrodes (not shown) and a cathodoluminescent screen 12.
  • the heated molten zone 5 emits infrared radiation of which the part having wavelengths exceeding 1.1 passes substantially unimpeded through the silicon layer 7 deposited on the inner wall of the vitreous-quartz tube l and can be collected by the infrared viewer 8.
  • An infra-red image of the molten zone 5 is projected onto the photo-cathode 11 by means of the lens or lens system 9.
  • the electrons emitted by the photo-cathode 11 are projected with the aid of the electrodes (not shown) provided in the tube onto the screen 12 so that a visible image of the molten zone 5 is produced on this screen.
  • the observer 13 is enabled to follow the zone-melting process without the use of a crucible and, if required, to control this process, for example by varying the high-frequency current supplied to the coil by the generator, without being impeded by the silicon deposit 7 on the vitreous quartz tube 1.
  • rod portions 3 and 4 are irradiated by infrared radiation, they can also be observed by means of the image converter. It has been found that generally normal daylight contains a sufiicient amount of infra-red radiation for this purpose.
  • an infra-red image converter can also be used in heat treatments of other semi-conductor materials and in further heat treatments, for example zone melting in a crucible, drawing crystals from the melt, deposition of semi-conductor material by sublimation or decomposition of volatile compounds, etc. without departing from the scope of the present invention.
  • a method of treating semiconductor material within an enclosure containing a portion substantially transparent to infra-red radiation and controlling the said treatment comprising the steps of heating the semiconductor material as part of the treatment under conditions at which semiconductor vapors are formed that condense on the substantially transparent enclosure portion forming a layer that is substantially opaque to visible radiation but substantially transparent to infra-red radiation, and utilizing an infra-red image converter located outside the enclosure for detecting through the said substantially transparent enclosure portion and layer an infra-red image of the heated semiconductor material and for converting that infra-red image into a visible image of the heated semiconductor material which can be observed for the purpose of controlling the treatment of the material.
  • a method of zone-melting silicon semiconductor material within an enclosure containing a low-pressure protective atmosphere and including a wall portion substantially transparent to infra-red radiation and controlling the said treatment comprising the steps of heating and melting the semiconductor material as part of the treatrnent whereby vapors of the material are formed within the enclosure that deposit on the said wall portion forming a layer that is substantially opaque to visible radiation but substantially transparent to infra-red radiation, and utilizing an infra-red image converter located outside the enclosure for detecting through the said substantially transparent wallportion and layer an infra-red image of the heated semiconductor material and for converting that infra-red image into a visible image of the heated semiconductor material which can be observed for the purpose of controlling the treatment of the material.
  • Apparatus for heat treatment of a semiconductor material and for controlling that treatment comprising an enclosure in which the semiconductor material is located, said enclosure containing a portion substantially transparent to infra-red radiation, means for controlling the atmosphere within the enclosure, means for heating the semiconductor material while in the enclosure under conditions at which an infra-red image of the heated semiconductor material is generated and vapors are formed that condense on the substantially-transparent enclosure portion forming a layer that is substantially opaque to visible radiation but substantially transparent to infra-red radiation, and means located outside the enclosure but adjacent the said substantially transparent portion for detecting the said infra-red image therethrough and for converting the said infra-red image into a visible imagewhich can be observed for the purpose of controlling the treatment of the material.
  • Apparatus for zone-melting of silicon semiconductor material and for controlling it comprising an enclosure in which the semiconductor material is located, said enclosure being of a material substantially transparent to infra-red radiation, means for providing a low pressure protective atmosphere withinv the enclosure, means for heating the semiconductor material while in the enclosure to a temperature at which the material melts and vapors of the material are formed which deposit on the enclosure walls forming a layer opaque to visible radiation but transparent to infra-red radiation and under the conditions at which an infra-red image of the heated semiconductor material is generated, and means located outside the enclosure but adjacent thereto for detecting the said infra-red image therethrough and for converting the said infra-red image into a visible image which can be observed for the purpose of controlling the zonemelting of the material.

Landscapes

  • Chemical & Material Sciences (AREA)
  • Organic Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Mechanical Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Thermal Sciences (AREA)
  • Electromagnetism (AREA)
  • Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)

Description

March 10, 1964 .1. GOORISSEN 3,124,636
METHOD OF AND APPARATUS FOR HEAT TREATMENT OF SEMI-CONDUCTOR MATERIAL Filed Sept. 12, 1960 INVENTOR 7- MM AGENT United States Patent 3,124,686 METHQD OF AND APPARATUS FOR HEAT TREAT- MENT 0F SEMI-CONDUCTOR MATERIAL Jan Goorissen, Eindhoven, Netherlands, assignor to North American Phiiips Company, Inc, New York, N.Y., a
corporation of Delaware Filed Sept. 12, 196i), Ser. No. 55,372 Claims priority, application Netherlands Sept. 24, 1959 4 (Ilaims. (Cl. 25083.3)
In the production of semi-conductor material and the manufacture of bodies from these materials use is frequently made in practice of heat treatments, for example for separating the material from the gas phase, for purifying it or working it up into single-crystal bodies. Examples of these treatments are treatments in which a body of semi-conductor material in the shape of a rod grows by solidification of a melt of the material, such as zonemelting treatments, which may either be performed in an elongated crucible according to Pfann or without the use of a crucible according to Keck, and the drawing of crystals from a melt of semi-conductor material according to the method of Czochralski. A further example is the deposition of semi-conductor material on a support, for example by sublimation or by decomposition of volatile compounds when heated.
In such treatments generally changes occur, for example melt formation, solidification and changes in shape, which are perceptible with the eye so that the course of the treatment can be followed and, if required, controlled. In treatments in which a body of semi-conductor material grows to form a rod by solidification of a melt it is of importance that the thickness of the rod during its growth is supervised and controlled by the observer, for example by controlling the supply of heat to the melt. When semi-conductor material is segregated from the gas phase on to a support it is desirable that the degree of growth of the deposited material should be followed by observation and controlled according to this observation in order to ensure the most eflicient and uniform deposition.
Since with semi-conductor materials it is undesirable that heat-treatments should be performed in air, such a treatment is carried out in an enclosure in which the composition of the atmosphere can be controlled. Generally the enclosure has a wall made at least in part of a transparent material such as vitreous quartz in order to permit observation.
It has, however, been found that frequently a coating of the semi-conductor material is deposited on the wall of the enclosure and prevents direct observation of the material to be treated. Such a deposit is formed in particular when elevated temperatures are used and/ or at a very low gas pressure in the enclosure, for example if the heat treatment is carried out in a vacuum.
It is an object of the invention to permit continuous observation of the phenomena occurring during heat treatment of semi-conductor materials. The invention utilizes the property of a semi-conductor material that it transmits infra-red radiation over a certain wavelength range in contradistinction to, for example, a metal, so that infra-red radiation of a wavelength within this range is also transmitted by the deposit of the semi-conductor material on the wall. In general a conventional transparent wall portion of vitreous quartz is also permeable to such radiation.
According to the invention during the heat treatment an infra-red image converter is used for observing the material under treatment. The term infra-red image converter as used herein denotes in general a device capable of converting an infra-red radiation image into an ice image of visible light. The image converter may be an infra-red viewer known in the art, as described in Proceedings of the IRE. 47 (1959), No. 5, page 904, or a flat image intensifier sensitive to infrared radiation. A camera tube sensitive to infra-red radiation may be used according to principles known from television, the signal delivered by this tube being converted into a visible image in a display tube. The infra-red image converter must be sensitive to the infra-red radiation transmitted by the semi-conductor material concerned. The wavelength range of the transmitted radiation is bounded at the short wave end by an absorption boundary of the semi-conductor material which is related to the energy spacing, hereinafter referred to as the band spacing, between the valency band and the conduction band of the semi-conductor material and which is situated at a smaller wavelength according as the band spacing is larger. In general the heated semi-conductor material itself may serve as the source of infra-red radiation, however, this material may alternatively be irradiated by infra-red radiation.
It has also been found that the use of an infra-red image converter may have further advantages, for example when mists occur during the treatment which disperseinfra-red radiation in a materially smaller degree and, if they consist of semi-conductor material, absorb this radiation to a lesser extent than visible radiation. Furthermore, when a layer of semi-conductor material is deposited on a support, the thickness of the layer can be determined during the deposition by means of interference of reflected infra-red radiation and this generally is not possible with visible radiation due to the frequently high absorptive power of the semi-conductor material for visible light.
Although observation by means of an infra-red image converter generally will be satisfactory when using a conventional wall portion of vitreous quartz, use may also be made of wall portions made from other material transmitting infra-red radiation, for example portions consisting of infra-red transmitting glasses or a window made of the same material or of another semi-conductor material having a band spacing equal to or greater than that of the material to be treated.
The invention will now be described more fully with reference to the accompanying drawing in which the figure is a vertical sectional and partly diagrammatical View of an apparatus for zone melting without the use of a crucible.
In this figure, reference numeral 1 denotes a vertical tube of vitreous quartz in which a vertical rod 2 of silicon is arranged. This rod comprises two solid portions 3 and 4 secured at their upper and lower ends respectively in holders (not shown) and an intermediate substantially drop-shaped molten zone 5 heated by means of a high-frequency coil 6. Due to the high surface tension of the melt the molten zone 5 is held in place between the two rod portions 3 and 4-. The vitreous quartz tube 1 and the rod 2 are gradually lowered vertically by means (not shown) in the direction indicated by an arrow, whereas the coil 6 does not change position so that the molten zone 5 passes through the silicon rod 2, the rod portion 3 gradually melting on at its lower end and the rod portion 4 gradually growing at its upper end.
The shape and the length of the molten zone 5 and the diameter or" the growing rod portion 4 can be controlled by adjusting the strength of the current in the high-frequency coil, which current is provided by a highfrequency generator (not shown). Owing to the high temperature of the melt, part of the silicon will evaporate from the zone 5 and be partly deposited as an opaque coating 7 on the inside of the vitreous quartz tube 1 so that observation of the zone with the naked eye is impeded. The apparatus also includes an infra-red image converter shown diagrammatically in the drawing as an infra-red viewer 3 comprising a concentrating lens or lens system for infra-red radiation 9 and a vacuum tube ltl consisting of a photo-cathode 11 which is sensitive to infra-red radiation of a wavelength exceeding 1.1 the absorption boundary of silicon, a set of electrodes (not shown) and a cathodoluminescent screen 12. During the treatment the heated molten zone 5 emits infrared radiation of which the part having wavelengths exceeding 1.1 passes substantially unimpeded through the silicon layer 7 deposited on the inner wall of the vitreous-quartz tube l and can be collected by the infrared viewer 8. An infra-red image of the molten zone 5 is projected onto the photo-cathode 11 by means of the lens or lens system 9. The electrons emitted by the photo-cathode 11 are projected with the aid of the electrodes (not shown) provided in the tube onto the screen 12 so that a visible image of the molten zone 5 is produced on this screen. By this image the observer 13 is enabled to follow the zone-melting process without the use of a crucible and, if required, to control this process, for example by varying the high-frequency current supplied to the coil by the generator, without being impeded by the silicon deposit 7 on the vitreous quartz tube 1. l
If the rod portions 3 and 4 are irradiated by infrared radiation, they can also be observed by means of the image converter. It has been found that generally normal daylight contains a sufiicient amount of infra-red radiation for this purpose.
Although in this example the process of zone-melting silicon without the use of a crucible has only been described, it goes without saying that an infra-red image converter can also be used in heat treatments of other semi-conductor materials and in further heat treatments, for example zone melting in a crucible, drawing crystals from the melt, deposition of semi-conductor material by sublimation or decomposition of volatile compounds, etc. without departing from the scope of the present invention.
What is claimed is:
1. A method of treating semiconductor material within an enclosure containing a portion substantially transparent to infra-red radiation and controlling the said treatment, comprising the steps of heating the semiconductor material as part of the treatment under conditions at which semiconductor vapors are formed that condense on the substantially transparent enclosure portion forming a layer that is substantially opaque to visible radiation but substantially transparent to infra-red radiation, and utilizing an infra-red image converter located outside the enclosure for detecting through the said substantially transparent enclosure portion and layer an infra-red image of the heated semiconductor material and for converting that infra-red image into a visible image of the heated semiconductor material which can be observed for the purpose of controlling the treatment of the material.
2 A method of zone-melting silicon semiconductor material within an enclosure containing a low-pressure protective atmosphere and including a wall portion substantially transparent to infra-red radiation and controlling the said treatment, comprising the steps of heating and melting the semiconductor material as part of the treatrnent whereby vapors of the material are formed within the enclosure that deposit on the said wall portion forming a layer that is substantially opaque to visible radiation but substantially transparent to infra-red radiation, and utilizing an infra-red image converter located outside the enclosure for detecting through the said substantially transparent wallportion and layer an infra-red image of the heated semiconductor material and for converting that infra-red image into a visible image of the heated semiconductor material which can be observed for the purpose of controlling the treatment of the material.
3. Apparatus for heat treatment of a semiconductor material and for controlling that treatment, comprising an enclosure in which the semiconductor material is located, said enclosure containing a portion substantially transparent to infra-red radiation, means for controlling the atmosphere within the enclosure, means for heating the semiconductor material while in the enclosure under conditions at which an infra-red image of the heated semiconductor material is generated and vapors are formed that condense on the substantially-transparent enclosure portion forming a layer that is substantially opaque to visible radiation but substantially transparent to infra-red radiation, and means located outside the enclosure but adjacent the said substantially transparent portion for detecting the said infra-red image therethrough and for converting the said infra-red image into a visible imagewhich can be observed for the purpose of controlling the treatment of the material.
4. Apparatus for zone-melting of silicon semiconductor material and for controlling it, comprising an enclosure in which the semiconductor material is located, said enclosure being of a material substantially transparent to infra-red radiation, means for providing a low pressure protective atmosphere withinv the enclosure, means for heating the semiconductor material while in the enclosure to a temperature at which the material melts and vapors of the material are formed which deposit on the enclosure walls forming a layer opaque to visible radiation but transparent to infra-red radiation and under the conditions at which an infra-red image of the heated semiconductor material is generated, and means located outside the enclosure but adjacent thereto for detecting the said infra-red image therethrough and for converting the said infra-red image into a visible image which can be observed for the purpose of controlling the zonemelting of the material.
References Cited in the file of this patent UNITED STATES PATENTS Loy Apr. 24, 1962 OTHER REFERENCES Infrared Oil-Film Camera Shows Heat Patterns, Electronics, April'195'6, page 190.

Claims (1)

1. A METHOD OF TREATING SEMICONDUCTOR MATERIAL WITHIN AN ENCLOSURE CONTAINING A PORTION SUBSTANTIALLY TRANSPARENT TO INFRA-RED RADIATION AND CONTROLLING THE SAID TREATMENT, COMPRISING THE STEPS OF HEATING THE SEMICONDUCTOR MATERIAL AS PART OF THE TREATMENT UNDER CONDITIONS AT WHICH SEMICONDUCTOR VAPORS ARE FORMED THAT CONDENSE ON THE SUBSTANTIALLY TRANSPARENT ENCLOSURE PORTION FORMING LAYER THAT IS SUBSTANTIALLY OPAQUE TO VISIBLE RADIATION BUT SUBSTANTIALLY TRANSPARENT TO INFRA-RED RADIATION, AND UTILIZING AN INFRA-RED IMAGE CONVERTER LOCATED OUTSIDE THE ENCLOSURE FOR DETECTING THROUGH THE SAID SUBSTANTIALLY TRANSPARENT ENCLOSURE PORTION AND LAYER AN INFRA-RED IMAGE OF THE HEATED SEMICONDUCTOR MATERIAL AND FOR CONVERTING THAT INFRA-RED IMAGE INTO A VISIBLE IMAGE OF THE HEATED SEMICONDUCTOR MATERIAL WHICH CAN BE OBSERVED FOR THE PURPOSE OF CONTROLLING THE TREATMENT OF THE MATERIAL.
US3124686D 1959-09-24 Goorissen Expired - Lifetime US3124686A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
NL243734A NL108788C (en) 1959-09-24 1959-09-24

Publications (1)

Publication Number Publication Date
US3124686A true US3124686A (en) 1964-03-10

Family

ID=19751951

Family Applications (1)

Application Number Title Priority Date Filing Date
US3124686D Expired - Lifetime US3124686A (en) 1959-09-24 Goorissen

Country Status (5)

Country Link
US (1) US3124686A (en)
DE (1) DE1146722B (en)
FR (1) FR1268179A (en)
GB (1) GB932668A (en)
NL (1) NL108788C (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3384732A (en) * 1964-01-08 1968-05-21 Taylor Winfield Corp Induction annealing of strip joints

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2054382A (en) * 1935-07-16 1936-09-15 United States Steel Corp Radiation pyrometer device
US2166824A (en) * 1936-01-14 1939-07-18 Gen Electric High temperature pyrometer
US2234328A (en) * 1937-09-24 1941-03-11 Rca Corp Radiant energy receiving device
US2591561A (en) * 1943-04-28 1952-04-01 Elgin Nat Watch Co Apparatus for producing refractory rods
US2692950A (en) * 1952-01-04 1954-10-26 Bell Telephone Labor Inc Valve for infrared energy
US2870309A (en) * 1957-06-11 1959-01-20 Emil R Capita Zone purification device
US2916593A (en) * 1958-07-25 1959-12-08 Gen Electric Induction heating apparatus and its use in silicon production
US2982856A (en) * 1955-06-27 1961-05-02 Rca Corp Tunable infrared apparatus and methods
US2997590A (en) * 1959-06-26 1961-08-22 Ibm Infrared radiation entrance window
US3031576A (en) * 1957-11-06 1962-04-24 Philips Corp Device for measuring and detecting radiations

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2054382A (en) * 1935-07-16 1936-09-15 United States Steel Corp Radiation pyrometer device
US2166824A (en) * 1936-01-14 1939-07-18 Gen Electric High temperature pyrometer
US2234328A (en) * 1937-09-24 1941-03-11 Rca Corp Radiant energy receiving device
US2591561A (en) * 1943-04-28 1952-04-01 Elgin Nat Watch Co Apparatus for producing refractory rods
US2692950A (en) * 1952-01-04 1954-10-26 Bell Telephone Labor Inc Valve for infrared energy
US2982856A (en) * 1955-06-27 1961-05-02 Rca Corp Tunable infrared apparatus and methods
US2870309A (en) * 1957-06-11 1959-01-20 Emil R Capita Zone purification device
US3031576A (en) * 1957-11-06 1962-04-24 Philips Corp Device for measuring and detecting radiations
US2916593A (en) * 1958-07-25 1959-12-08 Gen Electric Induction heating apparatus and its use in silicon production
US2997590A (en) * 1959-06-26 1961-08-22 Ibm Infrared radiation entrance window

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3384732A (en) * 1964-01-08 1968-05-21 Taylor Winfield Corp Induction annealing of strip joints

Also Published As

Publication number Publication date
GB932668A (en) 1963-07-31
DE1146722B (en) 1963-04-04
NL108788C (en) 1964-04-15
FR1268179A (en) 1961-07-28

Similar Documents

Publication Publication Date Title
US3615203A (en) Method for the preparation of groups iii{14 v single crystal semiconductors
US3499736A (en) X-ray or gamma ray use in control of crystal diameter
US3681033A (en) Horizontal growth of crystal ribbons
US4791261A (en) Crucible for evaporation of metallic film
US3124686A (en) Goorissen
US3351433A (en) Method of producing monocrystalline semiconductor rods
US3261671A (en) Device for treating semi-conductor materials by melting
JPS63315589A (en) Single crystal production apparatus
US3226203A (en) Apparatus for preparing semiconductor rods
JP2709310B2 (en) Single crystal pulling device
US3756799A (en) Method for beam heating of glass
US3124633A (en) Certificate of correction
JP2943430B2 (en) Method and apparatus for producing single crystal
US3341360A (en) Method of precipitating crystalline layers of highly pure, brittle materials
US3816601A (en) Process for the production of pure metal halides
US3360405A (en) Apparatus and method of producing semiconductor rods by pulling the same from a melt
Laszlo et al. Thoria single crystals grown by vapor deposition in a solar furnace
US3929556A (en) Nucleating growth of lead-tin-telluride single crystal with an oriented barium fluoride substrate
US3053639A (en) Method and apparatus for growing crystals
US3141849A (en) Process for doping materials
US4876114A (en) Process for the self fractionation deposition of a metallic layer on a workpiece
US3649210A (en) Apparatus for crucible-free zone-melting of crystalline materials
US3226193A (en) Method for growing crystals
JPS59172715A (en) Molecular beam generating equipment
JP3079256B2 (en) Crystal growth method