WO1994028206A1 - Appareil et procede de production d'une matiere monocristalline - Google Patents
Appareil et procede de production d'une matiere monocristalline Download PDFInfo
- Publication number
- WO1994028206A1 WO1994028206A1 PCT/JP1994/000821 JP9400821W WO9428206A1 WO 1994028206 A1 WO1994028206 A1 WO 1994028206A1 JP 9400821 W JP9400821 W JP 9400821W WO 9428206 A1 WO9428206 A1 WO 9428206A1
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- WO
- WIPO (PCT)
- Prior art keywords
- heat
- single crystal
- metal chamber
- melt
- insulating member
- Prior art date
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Classifications
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- 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
- C30B15/00—Single-crystal growth by pulling from a melt, e.g. Czochralski method
- C30B15/14—Heating of the melt or the crystallised materials
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- 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
- C30B15/00—Single-crystal growth by pulling from a melt, e.g. Czochralski method
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- 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
- Y10T117/1032—Seed pulling
-
- 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
- Y10T117/1032—Seed pulling
- Y10T117/1052—Seed pulling including a sectioned crucible [e.g., double crucible, baffle]
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- 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
- Y10T117/1032—Seed pulling
- Y10T117/1056—Seed pulling including details of precursor replenishment
-
- 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
- Y10T117/1032—Seed pulling
- Y10T117/1068—Seed pulling including heating or cooling details [e.g., shield configuration]
-
- 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
- Y10T117/1032—Seed pulling
- Y10T117/1072—Seed pulling including details of means providing product movement [e.g., shaft guides, servo means]
Definitions
- the present invention relates to an apparatus for manufacturing a single crystal such as silicon and a method for manufacturing a single crystal using the apparatus, and relates to a method for manufacturing a single crystal which is free from contamination of the single crystal and thermal oxidation-induced stacking faults and has excellent oxide film breakdown voltage characteristics.
- the present invention relates to a manufacturing apparatus and a manufacturing method suitable for precise control of oxygen concentration and oxygen concentration.
- FIG. 6 is a schematic cross-sectional view showing the implementation status of the Chiyo-Kralski method.
- Crucible 1 has a double structure, consisting of a quartz container la on the inside and a graphite container lb on the outside.
- a heater 2 is provided outside the crucible 1, and a melt 5 of a crystal raw material melted by the heater is accommodated in the crucible 1.
- a single crystal 4 is grown at the lower end.
- These parts and members are housed in a water-cooled metal chamber 6, and constitute a single crystal manufacturing apparatus as a whole.
- a high-purity argon gas is always supplied as an inert gas from the central portion above the metal chamber 16 to form a gas flow 30.
- Gas stream 30 evaporates from the surface of silicon melt 5
- a gas flow 31 is formed with silicon oxide (Sio) and carbon monoxide (CO) generated by the reaction of the silicon monoxide with a high-temperature member such as a heater 2 or a graphite container lb.
- the water flows down the inner and outer peripheral surfaces of the container and is discharged from the discharge port 8.
- FIG. 4 shows a device (first device) proposed by U.S. Pat. No. 4,330,362 and Japanese Patent Publication No. 57-40119.
- This device has an upper flat annular rim 7a projecting from the edge of the crucible, and a connecting portion 7b attached to the annular rim 7a and tapering downward from the inner edge in a circular shape. Further, it is characterized in that the inner height of the connecting portion 7b is 0.2 to 1.2 times the depth of the crucible 1.
- FIG. 5 shows an apparatus (second apparatus) disclosed in Japanese Patent Application Laid-Open No. 64-72984.
- This device includes a heat-resistant heat-insulating cylinder 10 extending downward from the junction between the metal chamber 16 and the sub-chamber 6c, and air-tightly joined to the sub-chamber 6c to coaxially surround the growing single crystal 4;
- a doughnut-shaped heat-resistant heat-insulating plate 11 1 having an outer periphery closely contacting the upper end of the heat-insulating member 12 and substantially matching the outer periphery of the heat-insulating member 12, and having a through hole at the center of the heat-insulating cylinder 10. It is characterized by having.
- the first and second devices described above are used to pull up crystals due to the radiation heat shielding effect. This is effective in improving the polishing rate, preventing the silicon monoxide fine powder from dropping into the silicon melt, and suppressing thermal oxidation-induced stacking faults (hereinafter referred to as OSF) of the crystal substrate.
- OSF thermal oxidation-induced stacking faults
- these devices have a problem in improving the oxide film breakdown voltage characteristics required for highly integrated fine semiconductors.
- the formation mechanism of the defects that deteriorate the oxide breakdown voltage characteristics has not yet been sufficiently elucidated.
- a defect nucleus is generated in the crystal, which is a cause of poor oxide film breakdown voltage characteristics.
- the defect nucleus shrinks in a high temperature region (1250 ° C or higher) and grows in a low temperature region (1100 ° C or lower).
- the oxide pressure resistance is due to the thermal history immediately after crystal growth. .
- the internal height of the frustoconical cylindrical connecting portion 7b disposed around the pulled crystal is as short as 0.2 to 1.2 times the crucible height. Therefore, the crystal immediately after the crystal growth is directly exposed to the atmosphere in the metal chamber kept at a low temperature, so that the crystal is rapidly cooled, the defect nuclei do not shrink, and the oxide film breakdown voltage characteristics are reduced.
- the heat-resistant heat-insulating cylinder 10 is air-tightly joined to the junction between the water-cooled metal chamber 16 and the sub-chamber 16c by heat conduction.
- the inner surface of 10 becomes low temperature and is rapidly cooled in the high temperature region immediately after crystal growth. For this reason, in the crystal immediately after crystal growth, the defect nucleus does not shrink, and the withstand voltage characteristics of the oxide film deteriorate.
- the oxygen concentration in the single crystal in order to effectively perform the above-mentioned intrinsic gettering, should be 0.75 xi 0 17 atoms / cra 3 relative to the target value. Although it is required to control the oxygen concentration with high accuracy, the oxygen concentration is strongly affected by the flow state of the argon gas.
- Argon gas flow rate V g is gas supply pressure P g, gas flow rate Q g, It depends on the gas passage space sectional area A g and the furnace pressure P f, and is expressed by the following equation (A).
- This gas flow rate V g is not only the concentration of oxygen in the single crystal, but also the contamination of the single crystal from carbon monoxide generated by the reaction of graphite members such as silicon monoxide evaporated from the melt surface and heaters. Has also had a significant impact.
- V g (Q g / A g) x (P g / P f) (A)
- the argon gas flowing from above the pulling chamber is a complicated turbulent flow, and the upward flow of silicon monoxide evaporating from the surface of the melt 5 affects the flow of the argon gas in the circumferential direction of the connection portion 7b. Is not uniform. Therefore, the argon gas flowing out from the lower end of the connecting portion 7b does not uniformly flow in the circumferential direction, and the argon gas flow rate Vg flowing through the gap between the lower end of the connecting portion 7b and the surface of the melt 5 causes a partial speed difference.
- the flow in the gap between the tip of the connection portion 7b and the surface of the melt 5 is When the velocity V g increases, the surface of the melt 5 vibrates, and a situation may occur in which dislocation-free single crystals cannot be pulled.
- the present invention provides an oxide film withstand voltage characteristic that appropriately forms a temperature distribution in the pulling direction of a single crystal, avoids contamination of the single crystal with impurities, and does not impair precise control of oxygen concentration in the crystal.
- An object of the present invention is to provide a manufacturing apparatus and a manufacturing method capable of pulling and growing a single crystal excellent in quality, and an object of the present invention is to provide a silicon single crystal manufacturing apparatus of the following (1) and use of the apparatus. This is achieved by providing a method for producing a single crystal according to the following (2).
- a single crystal manufacturing apparatus comprising pulling means 9 for bringing a single crystal 4 into contact with a seed crystal 3 to grow and a metal chamber 6 accommodating each of the above members, a cylinder surrounding a single crystal pulling region is provided.
- a cylindrical heat-resistant and heat-insulating member 7 reduced in diameter from above to below is provided between the upper end of this member 7 and the ceiling 6a of the metal chamber 6 above the metal chamber 6. From the inert gas 33 flowing downward inside the member 7 and the inert gas 32 flowing downward outside the member 7, An apparatus for producing a single crystal, which is supported from above a ceiling 6a or a side wall 6b of a metal chamber 1.
- a method for manufacturing a single crystal using a single crystal manufacturing apparatus including a pulling means 9 for growing a single crystal 4 and a metal chamber 6 for accommodating the above components a cylinder surrounding a pulling area of the single crystal 4 is provided.
- a cylindrical heat-insulating member 7 having a diameter reduced from the top to the bottom is disposed above the melt 5 in the crucible 1, and the upper end of the heat-insulating member 7 and the ceiling 6 a of the metal chamber 6.
- a space h which allows the flow of an inert gas, is provided between the inert gas 33 and the inert gas 33 flowing downward from the inside of the member 7 to the inert gas 30 supplied from above the metal chamber 16. After diverging into the inert gas 32 flowing downward on the outside of the Method for producing a single crystal according to Toku ⁇ that is merged inert gas obtained by Toki.
- the heat-resistant and heat-insulating member 7 of (1) and (2) is made of graphite, and its surface is desirably coded with silicon carbide.
- the distance between the upper end of the member 7 and the ceiling 6a of the metal chamber 6 (h can be adjusted within the range of 5 mn! -100mm), and the flow rate of the inert gas flowing through this distance, that is, the flow velocity is adjusted It is desirable to do.
- FIG. 1 is a diagram showing the device of the present invention, (a) is a longitudinal sectional view of the device, (b) shows an enlarged view of the main part.
- FIG. 2 is a view showing an example of a holding state of the heat- and heat-insulating member.
- (A) is a longitudinal sectional view
- (b) is a horizontal sectional view
- (c) is a perspective view of the held heat-insulating member. is there.
- FIG. 3 is a view showing another example of the holding state of the heat-resistant and heat-insulating member, where (a) is a longitudinal sectional view, (b) is a perspective view of the supporting leg material, and (c) is the heat-insulating property to be held. It is a perspective view of a member.
- FIG. 4 is a longitudinal sectional view showing an example of a conventional single crystal manufacturing apparatus
- FIG. 5 is a longitudinal sectional view showing another example of a conventional single crystal manufacturing apparatus. Further figure
- FIG. 6 is a schematic cross-sectional view showing an implementation state of the Chiyoklarski method.
- FIG. 1 is a view showing the configuration of the apparatus of the present invention, in which (a) is a longitudinal sectional view of the apparatus, and (b) is an enlarged view of a main part of (a) for easy understanding.
- reference numeral 1 denotes a crucible, which has a double structure with a quartz container la on the inside and a graphite container lb on the outside, and is set on a crucible support shaft lc.
- the crucible support shaft l c can not only rotate the crucible but also raise and lower the crucible.
- the water-cooled metal chamber 6 in the figure is a cylindrical vacuum vessel composed of a ceiling 6a and a side wall 6b centered on the single crystal pulling axis, and the crucible 1 is located at the center of the vacuum chamber.
- a heating heater 2 is arranged around the periphery of the heating heater.
- a pulling means 9 is vertically suspended from the center of the ceiling 6a of the metal chamber 6 so as to be rotatable and vertically movable, and a seed crystal 3 is mounted at a lower end thereof. Seed crystal 3 rises while being rotated by pulling means 9, and single crystal 4 grows at the lower end, which is the contact surface with melt 5.
- a heat-resistant cut conical with the pulling means 9 The heat-resistant member 7 does not contact the ceiling 6a of the metal chamber 6, and an interval (h!) Is provided between the upper end of the heat-insulating member 7 and the ceiling 6a so that an inert gas, that is, an argon gas can flow. ) And is placed around the single crystal pulling area with a distance (h 2 ) from the surface of the melt 5.
- FIG. 2 is a diagram showing an example in which the heat- and heat-insulating member 7 is held by the support member 21.
- FIG. 7A is a vertical cross-sectional view of the holding state by the support member 21, and
- FIG. 7B is a horizontal cross-sectional view taken along the line AA.
- FIG. 3C is a perspective view of the heat- and heat-insulating member 7.
- four square rod-shaped support members 21 are disposed at 90 ° intervals on the ceiling 6a of the metal chamber 6, and the support members 21 and the fastening ports 21a allow the heat-insulating and heat-insulating members 7 to be formed. Hold the upper end.
- the upper end of the heat-resistant and heat-insulating member 7 does not come into contact with the ceiling 6a, and an interval is provided so that the argon gas branches and flows downward inside and outside the heat-resistant and heat-insulating member 7. Hold member 7.
- the number of the support members 21 is not limited to the above-mentioned four, and the shape thereof is not limited to a square rod shape.
- the heat-resistant and heat-insulating member 7 is provided at its upper end with a holding through hole 7c through which the plurality of bolts 21a pass.
- a holding through hole 7c through which the plurality of bolts 21a pass.
- this adjusting means is a means shown in the drawing).
- Fig. 3 is a diagram showing another example in which the heat-resistant and heat-insulating member 7 is held by the support leg members 22.
- the heat-resistant and heat-insulating member 7 is located above the side wall 6b of the metal chamber 6.
- FIG. 9 is a perspective view of the heat-resistant and heat-insulating member 7 held by the support leg member 22, and has protrusions 7d provided at four locations on a circumference of an upper end surface thereof.
- the support leg member 22 is held by fitting the upper end ring 22a of the support leg member 22 to the fastening ring 23 provided on the upper part of the side wall 6b of the metal chamber 16.
- the claw portion 22c of the support leg member 22 is engaged with the projection 7d of the heat-resistant and heat-insulating member 7, and is separated from the ceiling portion 6a to hold the heat-resistant and heat-insulating member 7.
- adjustment of the distance (In) between the upper end of the heat-resistant and heat-insulating member 7 and the ceiling 6a is performed by adjusting the length and angle of the support leg 22b of the support leg member 22.
- the shape of the support leg member 22 and the number of the support legs 22b are not limited to those illustrated.
- the structure of the support member only needs to be configured so as not to close the space between the upper end of the heat-insulating and heat-insulating member 7 and the ceiling 6a.
- the distance between the upper end of the member 7 and the ceiling 6a is such that the argon gas supplied from above the metal chamber 6 is branched and flows downward through the area inside the heat-insulating member 7 and the area outside it. It is provided in As long as such a supporting member is used to support the heat-resistant and heat-insulating member 7 from the ceiling 6a or the side wall 6b of the metal chamber 6, the object of the present invention is achieved.
- the heat-resistant and heat-insulating member 7 is made of graphite, and its shape is a cylinder or a tube whose diameter is reduced from top to bottom, and its surface is coated with silicon carbide. It is desirable.
- the reason why the heat-resistant and heat-insulating member 7 is made of graphite is that it can be manufactured with high purity and there is little risk of contamination of the pulled crystal by heavy metals or the like. If the surface is coated with silicon carbide, gas emission from the pores of the graphite member is prevented, and the reaction between silicon monoxide vaporized from the surface of the melt 5 and the graphite member is also prevented. Can be.
- the temperature gradient of the pulled crystal It is necessary to appropriately adjust the arrangement, and in particular, it is necessary to provide a temperature gradient for gradually cooling the high temperature region immediately after crystal growth.
- the heat-insulating member 7 is provided in a wide range from the surface of the melt 5 in the crucible to the ceiling 6 a of the metal chamber 6 around the pulling area of the single crystal. And it is mounted with an appropriate gap between the ceiling part 6a of the water-cooled metal chamber 16 and is not air-tightly joined to the ceiling part.
- the crystal immediately after crystal growth may be directly exposed to the low-temperature atmosphere in the metal chamber due to the low internal height of the connecting portion 7b as in the device shown in FIG. Absent.
- the temperature of the heat-insulating member 7 is prevented from lowering due to heat conduction as compared with a case where the device is airtightly bonded to the ceiling of the metal chamber as in the apparatus shown in FIG. Can be kept at a high temperature. Therefore, in the apparatus and method of the present invention, the temperature gradient immediately after crystal growth can be reduced, and the single crystal is gradually cooled in a high temperature region of 1 100 ° C. or more, and the oxide withstand voltage characteristics are improved. It becomes possible.
- the flow 30 of the argon gas supplied from above the metal chamber 6 flows through the inside of the heat-insulating member 7 from the distance between the upper end of the heat-insulating member 7 and the ceiling 6a. It is once branched into a gas flow 33 flowing downward and a gas flow 32 flowing downward outside the heat- and heat-insulating member 7.
- the branched gas flows 32 and 33 merge at the outer peripheral region of the crucible 1 to form a gas flow 34, which flows between the crucible 1 and the heater 1 and the outside of the heater 2, and contains silicon monoxide and carbon monoxide. With this, it is discharged out of the chamber through the exhaust port 8.
- the gas flow rate is reduced by reducing the flow rate of the gas flow 33 so that the partial velocity difference generated in the flow of the argon gas between the lower end of the heat-insulating member 7 and the surface of the melt 5 is reduced. Even if it is late, the gas flows toward the exhaust port 8 as long as the gas flow 32 flowing downward outside the heat-insulating member 7 is sufficiently secured.
- the flow velocity of the flowing gas flow 34 can be maintained at a certain value or more. Therefore, the oxygen concentration in the single crystal can be accurately controlled, and silicon monoxide and carbon monoxide can be appropriately discharged.
- the distance (h,) between the upper end of the heat-resistant and heat-insulating member 7 and the ceiling 6a is preferably set in the range of 5 to 100 mm. That is, when h, is less than 5, the gas flow 33 becomes dominant, and the flow of argon gas between the lower end of the heat-insulating member 7 and the surface of the melt 5 has a large partial velocity difference. However, a change occurs in the surface temperature of the melt 5 and the convection of the melt 5, and it becomes difficult to precisely control the oxygen concentration in the crystal to a desired range. On the other hand, if h i exceeds 100, the cooling rate of the pulled crystal 4 increases due to the influence of the water-cooled metal chamber 6, and the withstand voltage characteristics of the oxide film decrease.
- the distance (h 2 ) between the lower end of the heat-insulating member 7 and the surface of the melt 5 is 10 nrn!
- a range of ⁇ 50 is preferred. If h 2 exceeds 50 mm, the size effect of the radiant heat from the heating heater or the melt into pulling crystal no longer must be reduced crystal pull-up speed.
- h 2 a to lever the range of 10-50 negation, that the gas flow of argon gas between the lower end and the melt 5 surface of the heat resistant and heat insulating member 7 homogenized, to ensure even heat shielding effect of the pulling crystal it can.
- the flow rate of argon gas on the surface of the melt 5 must be controlled. It is necessary to make it as small as possible and to minimize the partial speed difference. Controlling this gas flow rate with good reproducibility requires the distance h! Between the upper end of the heat-insulating member 7 and the ceiling 6a. And heat resistant This is achieved by adjusting the distance h 2 between the lower end of the heat insulating member 7 and the surface of the melt 5 within the above range.
- the flow rate and the flow rate of the argon gas are adjusted so as to be appropriate in accordance with the single crystal pulling conditions such as the single crystal size, the pulling rate, and the required oxygen concentration. , The interval h in advance! And after setting the distance h 2, to manufacture a single crystal.
- the heat-insulating member 7 has a height of 380 mm, an upper end inner diameter of 400 mra, and a lower end inner diameter of 200. And The distance between the upper end of the heat-resistant and heat-insulating member 7 and the ceiling 6a of the metal chamber 6 through the holding of the support member 21 in FIG. the distance h 2 between the surface as a 30 wicked person, is disposed substantially coaxially with the pulling shaft 9 of the single crystal.
- the material of the heat-resistant and heat-insulating member 7 was graphite, and the surface was coated with silicon carbide.
- the pulled single crystal 4 is a silicon single crystal with a diameter of 6 inches, the quartz crucible la used has an inner diameter of 04O6rara (16 inches), and the flow rate of argon gas flowing into the metal chamber 6 is 60 liters. Under the conditions of torr / rain, the pulling speed was 1. lmm / min and the pulling length was 1200 ram. Further, as a comparative example, pulling was performed with the device having the configuration shown in FIG. 4 (first device) under the same pulling conditions.
- the pulled single crystal was evaluated by test items of a dislocation-free single crystal yield, an OSF conformity rate, an oxide film withstand voltage conformity rate, and an oxygen concentration pass rate.
- the dislocation-free single crystal yield is represented by the ratio of the weight of the dislocation-free single crystal obtained by cutting and removing the dislocation portion to the weight of the raw material polycrystal used.
- the OSF non-defective rate is calculated by cutting out silicon wafers, 780 ° C x 3 hours, And heat treatment at 1000 ° C x 16Hr, and then selective etching. If the SF defect is less than the standard value (10 pieces / cm 2 ), it is considered to be non-defective, and the ratio of OSF non-defective wafer to total wafer number Represent.
- the oxide film breakdown voltage non-defective rate was evaluated by a voltage ramping method.
- the gate electrode was composed of polycrystalline silicon of phosphorus (P) doping, and was a dry oxide film with a film pressure of 250 A. As for 8 MI 2 , pass / fail was evaluated as a non-defective product, which did not cause dielectric breakdown even at a reference value (average electric field of 8 MvZcm) or more.
- the oxygen concentration pass rate is as follows:-Of the single crystals pulled up without dislocations, those with an accuracy within ⁇ 0.75x i0 17 atoms / cra 3 with respect to the standard value are judged to be acceptable, and the oxygen concentration is passed. Ratio is expressed by the ratio of the weight of the dislocation single crystal to the weight of the dislocation-free single crystal.
- Table 1 shows the test results.
- the temperature gradient in the pulling direction of the single crystal can be adjusted, and the branching and merging of the gas flow in the chamber can be appropriately controlled.
- contamination of the single crystal with contaminants can be avoided, the oxide film breakdown voltage characteristics of the single crystal substrate can be improved, and the oxygen concentration in the crystal can be precisely controlled.
- it can be used in the metal processing industry and the semiconductor industry.
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- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Crystallography & Structural Chemistry (AREA)
- Materials Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
Description
Claims
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
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US08/545,777 US5730799A (en) | 1993-05-31 | 1994-05-23 | Device for producing single crystals |
EP94915281A EP0702100A4 (en) | 1993-05-31 | 1994-05-23 | METHOD AND DEVICE FOR PRODUCING SINGLE CRYSTAL MATERIALS |
Applications Claiming Priority (6)
Application Number | Priority Date | Filing Date | Title |
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JP5/128795 | 1993-05-31 | ||
JP12879593 | 1993-05-31 | ||
JP6/20073 | 1994-02-17 | ||
JP2007394 | 1994-02-17 | ||
JP6/100190 | 1994-05-13 | ||
JP6100190A JP2619611B2 (ja) | 1993-05-31 | 1994-05-13 | 単結晶の製造装置および製造方法 |
Publications (1)
Publication Number | Publication Date |
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WO1994028206A1 true WO1994028206A1 (fr) | 1994-12-08 |
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/JP1994/000821 WO1994028206A1 (fr) | 1993-05-31 | 1994-05-23 | Appareil et procede de production d'une matiere monocristalline |
Country Status (4)
Country | Link |
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US (2) | US5730799A (ja) |
EP (1) | EP0702100A4 (ja) |
JP (1) | JP2619611B2 (ja) |
WO (1) | WO1994028206A1 (ja) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6214109B1 (en) * | 1996-10-15 | 2001-04-10 | Memc Electronic Materials, Inc. | Apparatus for controlling the oxygen content in silicon wafers heavily doped with antimony or arsenic |
Families Citing this family (8)
Publication number | Priority date | Publication date | Assignee | Title |
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JP3267225B2 (ja) * | 1997-12-26 | 2002-03-18 | 住友金属工業株式会社 | 単結晶引き上げ方法、及び単結晶引き上げ装置 |
JP3885452B2 (ja) * | 1999-04-30 | 2007-02-21 | 三菱マテリアル株式会社 | 結晶シリコンの製造方法 |
JP3838013B2 (ja) * | 2000-09-26 | 2006-10-25 | 信越半導体株式会社 | シリコン単結晶の製造方法 |
US6764548B2 (en) * | 2000-10-31 | 2004-07-20 | Shin-Etsu Handotai Co., Ltd. | Apparatus and method for producing silicon semiconductor single crystal |
JP3698080B2 (ja) * | 2001-09-11 | 2005-09-21 | 三菱住友シリコン株式会社 | 単結晶引上げ方法 |
JP4193503B2 (ja) * | 2003-01-31 | 2008-12-10 | 株式会社Sumco | シリコン単結晶の製造方法 |
US8152921B2 (en) * | 2006-09-01 | 2012-04-10 | Okmetic Oyj | Crystal manufacturing |
JP6268936B2 (ja) * | 2013-11-05 | 2018-01-31 | 株式会社Sumco | シリコン単結晶製造方法 |
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JPH01100086A (ja) * | 1987-10-12 | 1989-04-18 | Mitsubishi Metal Corp | 単結晶引上装置 |
JPH04219386A (ja) * | 1990-04-18 | 1992-08-10 | Nkk Corp | シリコン単結晶の製造装置 |
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GB2139918B (en) * | 1983-05-21 | 1986-09-10 | Cambridge Instr Ltd | Crystal growing apparatus |
JPS62138386A (ja) * | 1985-12-11 | 1987-06-22 | Shin Etsu Handotai Co Ltd | 単結晶の引上装置 |
US5004519A (en) * | 1986-12-12 | 1991-04-02 | Texas Instruments Incorporated | Radiation heat shield for silicon melt-in manufacturing of single crystal silicon |
JPH0639352B2 (ja) * | 1987-09-11 | 1994-05-25 | 信越半導体株式会社 | 単結晶の製造装置 |
US5264189A (en) * | 1988-02-23 | 1993-11-23 | Mitsubishi Materials Corporation | Apparatus for growing silicon crystals |
JP2507888B2 (ja) * | 1988-11-19 | 1996-06-19 | 工業技術院長 | ヘテロ構造体の製造方法 |
JP2710433B2 (ja) * | 1990-01-24 | 1998-02-10 | 三菱マテリアル株式会社 | 単結晶引上装置 |
JP3019949B2 (ja) * | 1990-11-30 | 2000-03-15 | 東芝セラミックス株式会社 | 単結晶引上装置 |
DE4204777A1 (de) * | 1991-02-20 | 1992-10-08 | Sumitomo Metal Ind | Vorrichtung und verfahren zum zuechten von einkristallen |
EP0591525B1 (en) * | 1991-06-24 | 1997-09-03 | Komatsu Electronic Metals Co., Ltd | Device for pulling up single crystal |
JPH05254988A (ja) * | 1992-03-13 | 1993-10-05 | Ishikawajima Harima Heavy Ind Co Ltd | 単結晶の製造方法および装置 |
JPH05294784A (ja) * | 1992-04-17 | 1993-11-09 | Sumitomo Metal Ind Ltd | 単結晶成長装置 |
JP2720262B2 (ja) * | 1992-10-26 | 1998-03-04 | 科学技術振興事業団 | 単結晶引上げ装置 |
JP2807609B2 (ja) * | 1993-01-28 | 1998-10-08 | 三菱マテリアルシリコン株式会社 | 単結晶の引上装置 |
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1994
- 1994-05-13 JP JP6100190A patent/JP2619611B2/ja not_active Expired - Fee Related
- 1994-05-23 US US08/545,777 patent/US5730799A/en not_active Expired - Lifetime
- 1994-05-23 WO PCT/JP1994/000821 patent/WO1994028206A1/ja not_active Application Discontinuation
- 1994-05-23 EP EP94915281A patent/EP0702100A4/en not_active Ceased
-
1996
- 1996-12-19 US US08/769,528 patent/US5925147A/en not_active Expired - Lifetime
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JPH0535119B2 (ja) * | 1986-03-18 | 1993-05-25 | Sakaguchi Electric Heaters | |
JPH01100086A (ja) * | 1987-10-12 | 1989-04-18 | Mitsubishi Metal Corp | 単結晶引上装置 |
JPH04219386A (ja) * | 1990-04-18 | 1992-08-10 | Nkk Corp | シリコン単結晶の製造装置 |
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US6214109B1 (en) * | 1996-10-15 | 2001-04-10 | Memc Electronic Materials, Inc. | Apparatus for controlling the oxygen content in silicon wafers heavily doped with antimony or arsenic |
Also Published As
Publication number | Publication date |
---|---|
US5730799A (en) | 1998-03-24 |
EP0702100A1 (en) | 1996-03-20 |
US5925147A (en) | 1999-07-20 |
JP2619611B2 (ja) | 1997-06-11 |
EP0702100A4 (en) | 1997-11-26 |
JPH07277887A (ja) | 1995-10-24 |
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