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    • 专利摘要:
    A crucible has a first resistance heater arranged spaced above the top of the crucible and a second resistance heater having a first resistive section spaced below the bottom of the crucible and having a second resistive section spaced around the outside of the crucible side. The crucible is charged with a seed crystal at the top of an inner crystal. of the crucible and a single source material in the interior of the crucible at intervals between the seed crystal and the bottom of the crucible. Electrical power is sufficiently applied to the first and second resistance heaters to create a temperature gradient in the interior of the crucible of sufficient temperature to cause the source material to sublimate and condense on the seed crystal, thereby forming a growth crystal.
    公开号:SE1150634A1
    申请号:SE1150634
    申请日:2009-12-08
    公开日:2011-07-05
    发明作者:Varatharajan Rengarajan；Ilya Zwieback；Michael C Nolan；Bryan K Brouhard
    申请人:Ii Vi Inc；
    IPC主号:
    专利说明:

    At these temperatures and pressures, the source material 13 evaporates and fills the interior of the crucible 11 with volatile molecular species such as Si, SigC and SiCg. During the growth of the growth crystal 15 on the seed crystal 14, the temperature of the source material 13 is maintained higher than that of the seed crystal 14, typically by 10 to 200 ° C. This temperature difference forces the vapors to migrate the growth of and condense on the seed crystal 14 causing the growth crystal 15.
    The quality of PVT-grown SiC crystals depends on the growth conditions, such as the sign and the value of radial temperature gradients in the upper part of the crucible 11 where the growth of the growth crystal 15 takes place. Strong temperature gradients in the growth crystal 15, in particular radial ones, cause thermoelastic stress and the induction of defects and cracks in the growth crystal 15.
    It is known in the art of SiC growth by sublimation that the interface of crystal growth closely follows the shape of isotopes in the crystal and (where the growth crucible rises in the radial direction from the axis of the crucible to the proximity of the crucible. Positive radial gradients inside the wall) produces a convex the source material 13) growth interface. Negative radial gradients (where the temperature drops in the radial direction from the axis of the crucible towards the wall of the crucible) produce a concave (towards the source material 13) growth interface. A radial zero gradient (where the temperature does not change in the radial direction from the axis of the crucible to the wall of the crucible) produces a flat growth branch surface.
    Curved growth interfaces, convex or concave, can lead to coarse macro steps appearing on the growth interface, causing polytype instability and causing defects. Accordingly, it is generally considered that a flat growth interface is the most conducive to the growth of high quality crystals, such as the growth crystal 15. Usually, the conventional PVT heating geometry shown in Fig. 1 creates an axisymmetric thermal field in crucible ll with strong radial temperature gradients that are difficult to control.
    Another problem with PVT heating with simple RF coil shown in Fig. 1 is that it is difficult to scale up for the growth of larger diameter crystals. As the diameter of the crucible and the diameter of the coil increase, radial gradients become steeper, while electromagnetic coupling between coil and crucible becomes less efficient.
    A growth technique via PVT sublimation called axial gradient transport (AGT) is described in the patent US 6,800,136 (hereinafter the "l36 patent") radial AGT and aims to reduce unwanted temperature gradients. A conceptual diagram of the growth geometry of the 'lssö patent is shown in Fig. 2.
    The AGT technology uses two independent flat heaters, namely a source heater and a rod heater. The heaters can be either inductive or resistive.
    The heaters are placed coaxially with the crucible, with the source heater arranged and the rod heater arranged above below the source material the growth crystal.
    The AGT technology includes means for reducing the heat dissipation in the radial direction, desirably to zero. This means comprises cylindrical thermal insulation and an additional heater arranged around the AGT growth cell. A properly fitted combination of the cylindrical thermal insulation and the heater can reduce radial heat loss to zero. The AGT geometry shown in Fig. 2 is claimed to lead to strict axial heat fl fate with radial gradients substantially equal to zero.
    The AGT apparatus using inductive heating is described in detail in the '136 patent, which is incorporated herein by reference. This inductively heated AGT device is shown in Fig. 3. It uses two flat RF coils, namely the top coil 30a and the bottom coil 30b. The cylindrical crucible 31 comprising the source material 32 and a seed crystal 33, on which a growth crystal 35 grows, is arranged between these coils, the top and bottom of the crucible serving as flat RF susceptors. Arrows 34 denote steam transport in the growth crucible in the direction from the source to the crystal.
    A disadvantage of the design of the AGT cell shown in Fig. 3 is related to the nature of the RF coupling between the flat coils 30a and 30b and the flat top and bottom of the crucible 31. There are two main types of flat RF coils, commonly known as "snail" coil and snake coil. When a “snigeP coil is coupled to a disk-shaped susceptor, it will deposit its RF energy mostly at the edges of the susceptor due to skin effect, as shown in Fig. 3. This type of coupling leads to poorly controllable radial temperature gradients in the crucible. "Snake" coils offer better uniformity in energy deposition, but their overall coupling efficiency is low.
    An AGT apparatus using flat resistive heaters is also described in the '136 patent. At temperatures for sublimation of the source material, radiation is the main mechanism for heat transfer from the heater to the crucible.
    Therefore, flat resistive heaters should be without the disadvantages of flat RF coils.
    A simple resistively heated AGT device is shown in Fig. 4A. The cylindrical crucible 41 sits between two flat resistive heaters 40a and 40b, which are shaped as round discs with diameters larger than those of the crucible. The upper heater 40a is arranged above a seed crystal 43, on which a growth crystal 45 grows, while the lower heater 40b is arranged below the source material 42. The arrows 44 denote the direction of steam transport in the crucible.
    The device in Fig. 4A has the disadvantage that it creates negative radial gradients (concave isotherms) in the vicinity of the growth crystal. This is illustrated in Fig. 4B which shows the results of finite element simulations of the AGT cell shown in Fig. 4A. The strongly concave isotherms 46 are visible 10 15 20 25 30 5 The root cause of these concave isotherms 46 is radially clear. heat losses.
    To some extent, concave isotherms 46 can be reduced by increasing the thickness of cylindrical thermal insulation around the AGT growth cell and / or by using an additional cylindrical heater, as described above in connection with Fig. 2. However, this will make such AGT growth systems deterrent large, complex and expensive.
    For SiC sublimation growth, graphite is a natural choice of heater material. To achieve the required temperature inside the growth crucible (up to 2400 ° C), the temperature of the heater should be 100-200 ° higher. Stability and reliability of graphite heaters at such high temperatures are poorly studied.
    A particular problem with all resistive heaters operating at high temperatures in an atmosphere of inert gas is the phenomenon of thermoionic emission. At high temperatures electron clouds form around the heater. Driven by the electric field created by electric current passing through the heater, these electrons migrate into the gas-filled space and contribute to the total current between the poles of the heater. By increasing the voltage of the heater, the electrons can get enough energy to ionize the gas. The generated gases can cause secondary (cascade) ionization of the gas which leads to glow discharge.
    Glow discharge changes the geometry of the heating and leads to erosion of the graphite crucible, the heater and the thermal insulation. In addition, at the beginning of the glow discharge, the electric current across the heater becomes unstable and thus creates instabilities in the growth, which leads to voltage and defects in the growth crystal.
    Gases accelerated by the electric field bombard the surface of the heater and can cause secondary electron emission. This chain of surface bombardment and ionization events at high temperatures is called thermoionic emission (glow discharge is in fact the first stage of 10 thermonionic emission). With a further increase in the heater's temperature and voltage, and with a sufficient supply of gases, glow discharge develops into an arc. Such a light bend can cause serious damage to the heater, the crucible and the power supply. Therefore, in order to realize the benefits of resistive heating in AGT growth of SiC crystals, it is desirable to avoid glow discharge in the growth system.
    SUMMARY OF THE INVENTION The present invention is an apparatus for crystal growth via axial gradient transport. The apparatus comprises a crucible with a top, a bottom and a side extending between the top of the crucible and a bottom of the crucible.
    The crucible is adapted to support an inoculum crystal at the top of an interior of the crucible and source material in the interior of the crucible with spaces between the inoculum crystal and the bottom of the crucible. The space between the source material and the bottom of the crucible defines a cavity in the interior of the crucible. A first resistance heater is arranged at intervals above the top of the crucible. A second resistance heater has a first section arranged at intervals below the bottom of the crucible and a second section arranged at intervals around the outside of the side of the crucible.
    The first and second resistance heaters may be operative to grow on the seed crystal arranged at the top of an interior of the crucible a growth crystal having a convex growth interface, a ratio between the radius of curvature of the convex growth interface and the diameter of the grown crystal being between about 2 and about 4.
    The top and bottom of the crucible can be round. The first resistance heater can be disc-shaped. The first section of the second resistance heater may be disc-shaped.
    The first heater and the first section of the second resistance heater may have outer diameters which are between 110% and 130%, included, of the outer diameter of the respective top and bottom of the crucible. The first resistance heater and the first section of the second resistance heater may have center holes with a diameter of between 25% and 75% of a diameter of the crucible.
    The side of the crucible and the second section of the second resistance heater may be cylindrical.
    The top of the second section of the second resistance heater may be arranged in a position between 50% and 75% of the height of the crucible.
    The inner diameter of the second section of the second resistance heater may be separated from the outside of the crucible by a radial distance of between 10 mm and 25 mm.
    The cavity inside the crucible between the source material and the bottom of the crucible can have a ratio between height and diameter of between 0.2 and 1.
    The invention is also an axial gradient growth method. The method comprises: (a) providing a crucible with a top, a bottom and a side extending between the top of the crucible and a bottom of the crucible, a first resistance heater arranged at intervals above the top of the crucible and a second resistance heater having a first resistive section arranged spaced below the bottom of the crucible and a second resistive section spaced around the outside or outside of the crucible side, (b) providing a seed crystal at the top of an interior of the crucible and a source material in the interior of the crucible spaced between the seed crystal and the bottom of the crucible, (c) applying electrical power to the first and second resistance heaters of a sufficient extent to create in the interior of the crucible a temperature gradient of sufficient temperature to cause the source material to sublimate and condense on the seed crystal, thereby forming a growth crystal, and (d) to maintain the electrical power of the first and second resistance heaters ti The growth crystal has grown to a desired size. 10 15 20 25 30 8 The first resistance heater can receive between 10% and 30% of the electrical power. The second resistance heater can receive between 70% and 90% of the electrical power.
    The voltage applied to each heater is desirably less than 30 VAC RMS and more desirably less than 25 VAC RMS.
    An inner and an outer side of the crucible and the heaters are in the presence of an inert gas of between 1 Torr and 40 Torr during the growth of the growth crystal.
    The inert gas may be helium.
    Step (c) may comprise controlling the electrical power applied to the first and second resistance heaters in a manner to cause a growth crystal to grow on the seed crystal, the grown growth crystal having a convex growth interface, a ratio between the convex growth interface and the curvature of the growth interface. the diameter of the grown growth crystal is between about 2 and about 4.
    BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic diagram of a growth cell for sublimation via physical vapor transport according to prior art, Fig. 2 is a conceptual diagram of an axial gradient transport apparatus (AGT). prior art, Fig. 3 is a schematic diagram of the prior art AGT growth cell of Fig. 2, Fig. 4A is a schematic diagram of a resistively heated AGT growth cell of the prior art, Fig. 4B is a graph of isotherms to be realized in the interior of the resistively heated AGT growth cell of the prior art according to Fig. 4A in use, Fig. 5 is a schematic diagram of a resistively heated AGT growth apparatus in accordance with the present invention, Fig. 6A is a schematic diagram of the resistively heated AGT growth cell according to Fig. 5, Fig. ÖB is a graph of isotherms that would be realized in the interior of the resistively heated AGT growth cell according to Fig. 6A in use, Fig. 7 is a graph of electrical conductance against gas pressure (helium pressure) for the gray heaters in the resistively heated AGT growth apparatus according to Fig. 5, Fig. 8 is a plan view of the top heater in the resistively heated AGT growth apparatus of Fig. 5, Fig. 9A is a plan view of the bottom heater of the resistively heated AGT growth apparatus of Fig. 5, Fig. 9B is a cross-sectional view taken along line IXB - IXB of Fig. 9A, Figs. 10A, 10B and 1OC are photographs of 100 mm SiC rods of polytypes 6H SI, 6H SI and 4H nt, respectively, which are grown in the AGT growth apparatus of Fig. 5, Figs. 11A and 11B are X-ray diffraction graphs of the rods. in Figs. 10B and 10C, respectively, obtained from scans performed along the axes and <10 -10>, and Figs. 12A and 12B are microtube density maps. micropipe density maps) over the rods of Figs. 10B and 10C, respectively.
    DETAILED DESCRIPTION OF THE INVENTION The present invention is a process and apparatus for AGT growth, including the geometry of the heaters, as well as measures for reducing or eliminating glow discharge in the growth core. The AGT growth process described herein has a growth interface that is slightly convex toward the bottom of the crucible. This slightly convex growth interface can yield large SiC single crystals of polytypes 6H and 4H suitable for making high quality SiC substrates that are 3 inches and 100 mm in diameter.
    Here, when temperature gradients inside the crucible increase in the radial direction from the axis of the crucible to the wall of the crucible, such radial temperature gradients are known as positive radial temperature gradients. Isotherms of positive radial temperature gradients inside the crucible are convex towards the bottom of the crucible (ie towards the source material 13). In contrast, when temperature gradients inside the crucible decrease in the radial direction from the axis of the crucible to the wall of the crucible, such radial temperature gradients are known as negative radial temperature gradients. Isotherms of negative radial temperature gradients inside the crucible are concave towards the bottom of the crucible. Finally, when temperature gradients inside the crucible do not change in the radial direction from the axis of the crucible to the wall of the crucible, such radial temperature gradients are known as radial zero gradients in temperature. Isotherms with radial zero gradients in temperature inside the crucible are flat and perpendicular to the axis of the crucible.
    With reference to Fig. 5, a resistively heated AGT growth apparatus according to the present invention comprises a cylindrical growth crucible 51 having therein a SiC source material 52 and a SiC seed crystal 53. The growth crucible 51 is placed between two resistive heaters arranged coaxially with growth crucible 51. 50a and bottom heater 50b. The growth crucible 51 and the heaters 50a and 50b are surrounded. These heaters comprise top heaters of thermal insulation 57 made of lightweight fibrous graphite. Electrical power is provided to the heaters 50a and 50b via bead extension electrodes 59 which extend through windows 56 of the thermal insulation 57. It is desirable that the growth crucible 51, the heaters 50a and 50b and the thermal insulation 57 be arranged in a larger container (not shown) which can maintain the crucible 51, the heaters 50a and 50b and the thermal insulation 57 at a suitable pressure (which will be discussed hereinafter) during the growth of a growth crystal 64 on the seed crystal 53.
    The top heater 50a is disc-shaped with a center hole 60. The outer diameter of the top heater 50a is larger than the growth crucible 51. It is desirable that 110% 130% of the inner diameter (ie the diameter of the center heel 60) be smaller than the growth crucible 51. It is desirable that the outer diameter 50a is between and the diameter of the growth crucible 51. The inside diameter of the top heater 50a that the inside diameter of the top heater 50a is between 25% and 75% of the diameter of the growth crucible 51. The top heater 50a is arranged above the growth crucible 51 at a distance from the growth crucible 51, desirably between 10% and 30% of the diameter of the crucible 51.
    The bottom heater 50b is cup-shaped. More specifically, the bottom heater 50b comprises two heating sections, namely a first, flat or disc-shaped section 61a and a second, cylindrical section 61b. The bottom heater 50b is arranged below and around the source material 52 in the growth crucible 51. The flat section 6la of the bottom heater 50b has a center hole 62 with a diameter smaller than that of the growth crucible 51. It is desirable that the diameter of the bottom heater 62b center hole 62 be between 25% and 75% of the growth crucible's 51 diameter. The flat section of the bottom heater 50b is desirably arranged at a distance from the growth crucible 51 of between 10% and 30%. The bottom heater 50b surrounds the side of the growth crucible 51. It is desirable that of the diameter of the crucible 51. the cylindrical section 61b of the height of the cylindrical section 61b is between 50% and 75% of the height of the growth crucible 51. It is desirable that the inner diameter of the cylindrical section 61b be separated from the outer diameter of the growth crucible 51 by a radial distance of between 10 mm and 25 mm.
    It is desirable that the source material 52 be arranged on a structure 63 at a distance from the bottom of the crucible 51 to create a void or cavity 54 between the source material 52 and the bottom of the crucible 51. The structure 63 may be made of any suitable and / or desirable material, such as, without being lightweight fibrous Desirably, the cavity 54 has limiting, graphite. the dimensional ratio between height and diameter of between 0.2 and 1.
    Pyrometric windows 58 may be formed in the upper and lower portions of the thermal insulation 57 to measure the temperature of the crucible 51 via a pyrometer.
    A section of the resistively heated AGT growth cell of Fig. 5 is shown separately in Fig. 6A. The result of a thermal simulation on the piece of the resistively heated AGT growth cell shown in Fig. 6A is shown in Fig. 6B.
    Figs. 6A and 6B are as in Fig. 5.
    The reference numerals in the same AGM growth cell heating geometry shown in Fig. 5 create isotherms 55 in the vicinity of the growth crystal 64 which are slightly convex towards the bottom of the crucible.
    The AGT heating geometry shown in Fig. 5 has the following advantages: (i) the radial temperature gradients in the vicinity of the growth crystal 64 are slightly positive (ie slightly convex towards the bottom of the growth crucible 51), which helps to avoid a concave growth interface towards the bottom of the growth crucible 51 or one and (ii) the growth crystal 64 is relatively small, which helps to avoid stress and flat growth interface, radial temperature gradients in cracks in the growth crystal 64.
    An advantage of the AGT heating geometry shown in Fig. 5 is that it creates relatively small and positive radial temperature gradients in the vicinity of the growing SiC crystal 64. Such gradients avoid or eliminate multiple growth centers, coarse macro steps, polytype instability and associated defects in the growth crystal 64. .
    The AGT growth apparatus and growth process of Fig. 5 yields SiC crystals with a convex growth interface. For SiC crystal rods capable of giving 3 ”substrates, the radius of the curvature of the interface is desirable between 15 cm and 30 cm.
    For large diameter SiC rods capable of providing 100 mm substrate, the radius of curvature of the interface is desirable between 20 cm and 40 cm. For each rod of a certain diameter, the ratio between the radius of curvature of the convex growth interface and the diameter is between about 2 and about 4, eg 20 cm / 100 mm = 2, and 40 cm / 100 mm = 4.
    In the AGT growth cell shown in Fig. 5, the bottom heater 50b is the main heater delivering about 80% of the required power, while the top heater 50a supplies about 20% of the power. The purpose of the top heater 50a is to create a desired temperature distribution in the upper part of the growth crucible 51. Fine adjustment of the thermal gradients in the upper part of the growth crucible 51 can be achieved by further adjusting the shape of the upper heater 50a, for example by changing the diameter of the center hole 60a.
    In a prior art PVT device, single-coil RF heating created conditions in which the crucible's cylindrical wall, which serves as an RF susceptor, was hotter than the bottom of the crucible. This led to the deposition of polycrystalline SiC on the bottom of the crucible and poor use of the source material.
    In the growth cell shown in Fig. 5, both the cup-like shape of the bottom heater 50b and the cavity 54 provided below the source material 52 serve to eliminate this deficiency. Due to the radiation nature of heat transport, the high emissivity of graphite (c1 = 0.95 ~ 0.98) and the aforementioned dimensional ratio of height to diameter of the cavity 54 of 0.2 to 1.0, the temperature distribution inside the cavity 54 is spatially uniform. i.e. with low temperature gradients. Accordingly, the distance between the isotherms inside the cavity 54 in Fig. ÖB is large.
    The presence of the cavity 54 below the source material 52 helps to raise the temperature at the bottom of the source material 52 and the crucible 51. As a result, deposition of polycrystalline SiC on the bottom of the crucible is avoided or eliminated and the utilization of the source material 52 is improved.
    The onset of glow charging in a resistive heated system depends on the nature of the gas, its pressure and heater voltage, but does not depend on the material of the heater, provided that a sufficiently high temperature is reached. Fig. 7 shows the dependence between the electrical conductance of a gray heater and the pressure of an inert gas (helium) at a voltage on the resistive heater of 25 VAC RMS and a temperature of 2200 ° C. The sharp increase in heater conductance at pressures between 0.1 and 40 Torr indicates the contribution of glow discharge (thermoionic emission) to the total electrical current that flows between the poles of the heater.
    The explanation for this phenomenon is as follows. At a low gas pressure, the concentration of gations is low, and the additional electron / ion current is small. With increasing gas pressure, the electric current increases due to thermoionic emission, and the measured conductance of the heater increases.
    With a further increase in the gas pressure, scattering and energy dissipation via the gas atoms dampens the emission, which leads to a reduction in the measured heat conductance. emission depends on the nature of the inert gas used. With heavy gases with a low pressure range and the magnitude of thermoionic ionization potential, such as argon, thermoionic emission starts at lower voltages, reaches higher amplitudes and develops rapidly into arcs. With light gases with high ionization potential, such as helium, thermoionic emission starts at higher voltages and its amplitude is lower. Helium is a light gas that has the highest ionization potential among inert gases. Therefore, helium is the best choice for resistively heated growth systems for SiC crystals.
    Another factor to prevent thermoionic emission is the heat geometry.
    Glow discharge starts in areas of a heater where the temperature and electric field strength are highest. Therefore, it is desirable to avoid the design of the AGT heater of the present invention tight-fitting poles (extension electrodes) which are below the highest potential difference.
    Resistantly heated AGT systems in accordance with the present invention, utilized for the growth of industrial size SiC crystals, have shown that growth of SiC crystals can be successfully carried out in helium without glow discharge. Desirably, the He pressure is above 25 Torr and, more desirably, above 30 Torr, and the voltage applied to the heater desirably does not exceed 30 VAC RMS and, more desirably, does not exceed 25 VAC RMS.
    The aforementioned limitation of the heater voltage determines the heater resistance. An example of a practical calculation is given below. Assume that the heat losses in the AGT growth apparatus require 15 kW of power to achieve and maintain the desired temperature for SiC growth. This means that the bottom heater should generate about 12 kW of power, while the top heater should generate about 3 kW. Assume further that to prevent glow discharge, the voltage of the bottom heater is limited to 20 VAC RMS and the voltage of the top heater is limited to 12 VAC RMS. Then the resistance of the lower heater should be about 0.03 Ohm and the resistance of the top heater should be about 0.05 Ohm. The electric current in the heaters will be about 660 A RMS in the bottom heater 50b and about 240 A RMS in the top heater 50a.
    Preferred dimensions of a preferred top heater 50a that meet the above requirements are shown in Fig. 8. Preferred dimensions of a preferred bottom heater 50b that meet the above requirements are shown in Figs. 9A and 9B. The burr material for the heaters 50a and 50b is desirably isostatically pressed, fine-grained burrs of a density of desirably between 1.73 and 1.82 g / cmß and resistivity of desirably between 9 and 14 uOhm-meters at room temperature.
    Preferred top heater 50a shown in Fig. 8 includes a plurality of internal slots (or slots) 66, each of which extends radially outward from the center hole 60 and terminates between the center hole 60 and the perimeter of the top heater 50a. The top heater 50a also includes a plurality of external slots (or slots) 68, each of which extends radially inwardly from the circumference of the top heater 50a and terminates between the center hole 60 and the circumference of the top heater 50a. It is desirable that the internal slots 66 and the external slots 68 be uniformly spaced around the circumference of the top heater 50a in a cam-like pattern, in which a piece of each slot 66 resides between a pair of the slots 68, and a piece of each slot 68 resides. between a pair of slots 66. Preferred top heater 50a includes twelve slots 66 and twelve slots 68. However, this should not be construed as limiting the invention.
    Preferred flat or disc-shaped section 61a of the preferred bottom heater 50b shown in Fig. 9A includes a plurality of internal slots (or slots) 70, each of which extends radially outwardly from the center hole 62 and terminates between the center hole 62 and the circumference of the disc-shaped section 61a. The plate-shaped section 61a also includes a plurality of external slots (or slots) 72, each of which extends radially inwardly from the circumference of the top heater 50a and terminates between the center hole 62 and the circumference of the top heater 50a. It is desirable that the internal slots 70 and the external slots 72 be uniformly distributed around the circumference of the disc-shaped section 61a in a cam-like pattern, in which a piece of each slot 70 resides between a pair of the slots 72, and a piece of each slot 72 resides. between a pair of slots 70. Preferred disc-shaped section 61a comprises ten slots 70 and ten slots 72. However, this should not be construed as limiting the invention.
    Preferred cylindrical section 61b of the preferred bottom heater 50b shown in Fig. 9B includes a plurality of upwardly slotted slots (or springs) 74, each of which extends upwardly from the disc-shaped section 61a and terminates before the upper edge of the cylindrical section 61b.
    The cylindrical section 61b also includes a plurality of slots (or slots) 76, each of which extends downwardly from the upper edge of the cylindrical section 61b and either terminates before the disc-shaped section 61a or extends completely to the disc-shaped section 61a. However, this should not be construed as limiting the invention.
    The foregoing description of the slots on the top heater 50a, disc-shaped section 61a and cylindrical section 61b should not be construed as limiting the invention as it may be understood that each of the top heater 50a, disc-shaped section 61a and cylindrical section 61b may have a suitable and / or desirable arrangement of slits.
    Advantages of the present invention include: A process and apparatus for crystal growth via axial gradient transport (AGT) for the sublimation growth of SiC single crystals comprising a cylindrical growth crucible for supporting the SiC source material and the SiC seed crystal in the crucible at intervals. The AGT growth apparatus comprises two resistive heaters, a top heater and a bottom heater, arranged coaxially with the cylindrical growth crucible. The top heater is arranged above the growth crystal and the bottom heater is arranged around and below the source material. The top heater is disc-shaped with a center hole.
    The bottom heater is cup-shaped with two heating sections - one flat and one cylindrical. The top heater and the bottom heater are made of graphite.
    The disc-shaped top heater has an outer diameter which is desirably between 10% and 30% larger than the diameter of the crucible and an inner diameter (hollow diameter) desirably between 25% and 75% of the diameter of the crucible. The top heater is arranged above the growth crucible at a distance from the crucible of desirably between 10% and 30% of the diameter of the crucible.
    The cup-shaped bottom heater comprises a flat section which is arranged at a distance from the crucible of desirably between 10% and 30% of the diameter of the crucible. The flat section has a center hole with a diameter of desirably between 25% and 75% of the diameter of the crucible. The cylindrical section has a height of desirably between 50% and 75% of the height of the crucible. The cylindrical section has an inner diameter of desirably between 10 mm and 25 mm larger than the outer diameter of the crucible.
    The heaters are desirably made of isostatically pressed, fine-grained burr of a desired desirability between 1.73 and 1.82 g / cm 3 and resistivity of desirably between 9 and 14 uOhm-meters at room temperature. The growth crucible desirably comprises a cavity separating the source material from the crucible. bottom. The cavity has a dimensional ratio between height and diameter of desirably between 0.2 and 1.0.
    The process for AGT crystal growth uses a top heater and a bottom heater. The bottom heater desirably provides between 70% and 90% of the electrical power necessary to heat the growth crucible to the temperature necessary for sublimation growth. The top heater desirably provides between 10% and 30% of the electrical power necessary to heat the growth crucible to the required temperature for sublimation growth. The top heater defines a thermal field in the upper part of the growth crucible characterized by low and positive radial temperature gradients to generate planar or slightly convex isotherms.
    The voltage applied to the heaters desirably does not exceed S0 VAC RMS and, more desirably, does not exceed 25 VAC RMS.
    The process of AGT crystal growth desirably takes place in an atmosphere of inert gas, such as, without limitation, helium, at a pressure of desirably above 25 Torr and, more desirably, above 30 Torr.
    Technical advantages of the invention: Application of the invention to sublimation growth of silicon carbide gives SiC single crystals of high quality and with low thermal stress.
    The gain has been exercised during your runs of SiC growth. These runs yielded large diameter, high quality semi-insulating 6H and nt4H crystals, as described below.
    A schematic diagram of the resistively heated AGT growth apparatus used in these runs is shown in Fig. 5. The heating assembly included two resistive heaters similar to those shown in Figs. 8, 9A and 9B.
    That is, the bottom heater was cup-shaped, while the top heater was disc-shaped. The center holes in the heaters were 50 mm in diameter for the top heater and 75 mm in diameter for the bottom heater. The axial distances between each heater and the crucible were about 25 mm. The radial distance between the outer surface of the crucible and the inner surface of the piece of the bottom heater surrounding the side of the crucible was 12 mm.
    The heaters were made of dense graphite with low porosity and a density of 1.75 g / cm 3. The resistance of the heaters was 0.03 Ohm for the top heater and 0.05 Ohm for the bottom heater (measured at room temperature). During a growth cycle, the bottom heater generated 80% of the required power, while the top heater generated 20% of the required power. The voltage at the poles of each heater did not exceed 20 VAC RMS. 10 15 20 25 30 19 All growth runs took place in the presence of helium at a pressure of 40 Torr.
    Since the crucible is made of porous graphite, the helium pressure inside the crucible as well as outside the crucible and around the heaters was about the same, ie. 40 Torr.
    During growth, the temperatures of the source and the seed crystal were maintained at 2180 ° C and 2130 ° C, respectively.
    Figs. 10A, 10B and 10C are photographs of some SiC rods grown using the resistively heated AGT growth apparatus shown in Fig. 5 which reached 100 mm in diameter. Fig. 10A is a photograph of a 6H SI rod number DCO020, Fig. 10B is a photograph of a beer-I SI rod number DE0001 and Fig. 10C is a photograph of a 4H nt rod number DF0001. All SiC crystal rods grown in the improved process and apparatus for AGT growth, including 3 ”and 100 mm rods, had a slightly convex growth interface with a radius of curvature of between 25 and 35 cm. The 10A, 10B and 10C were successfully machined into plates, including 3 inch diameter plates and the grown crystals shown in Fig. 100 mm diameter plates.
    Fig. 11A shows graphs of rocking curves from X-ray scans performed on the axes <1-210> and <10-10> in the OH crystal rod (DEOOO1) shown in Fig. 10B. The full width at half maximum (FWHM) for the X-ray re-selection serves as a good measure of crystal quality; the narrower the reflection and the lower the FWHM value, the better the crystal quality. For comparison, the 61-1 SiC Lely lamellae of the best quality measured FW1-IM values of between 20 and 40 beak seconds. FWHM in typical PVT-grown SiC bulkheads is usually higher - between 40 and 100 beak seconds. As can be seen in Fig. 10A, the FWHM values of the crystal DE0001 are between 25 and 60 bic seconds. Such low FWHM values testify to the excellent crystal quality.
    Fig. 11B shows graphs of waving curves from X-ray scans performed on the axes <1-210> and <10-10> in the 4H crystal rod (DF0001) shown in Fig. 10C. The measurement conditions were the same as in the above cases. The FWHM values measured on this 4H crystal rod were even lower; between 18 10 15 20 20 and 40 arcseconds. Thus, even for this rod, the X-ray analysis revealed excellent crystal quality.
    Another measure of crystal quality is its micropipe density (MPD). Micropipes are harmful defects that cause component failure, and the majority of component applications require low MPD values in the SiC substrate. While SiC substrates with MPD equal to zero are becoming commercially available, the current state of the art across the industry is in the order of 5 to 40 microtubule-cm-Q.
    Figs. 12A and 12B show MPD maps measured on the AGT-grown crystals DEOOOI and DFOOO1 in Figs. 10B and 10C, respectively. Both crystals show average MPD below 0.5 microtube cm / cm, where rod DEOOO1 (Fig. 11A) is virtually microtube free.
    The invention has been described with reference to the preferred embodiment.
    Obvious modifications and changes will become apparent to those skilled in the art upon reading and understanding the foregoing detailed description. It is intended that the invention be construed as including all such modifications and changes insofar as they fall within the scope of the appended claims or the equivalents thereof.
    权利要求:
    Claims (15)
    [1]
    An axial gradient type growth apparatus comprising: a crucible having a top, a bottom and a side extending between the top of the crucible and a bottom of the crucible, the crucible being adapted to support a seed crystal at the top of an interior of the crucible and a source material. in the interior of the crucible with space between the seed crystal and the bottom of the crucible, where the space between the source material and the bottom of the crucible defines a cavity in the interior of the crucible, a first resistance heater spaced above the top of the crucible, and a second resistance heater with a first section spaced below the bottom of the crucible and a second section arranged at intervals around the outside of the crucible side.
    [2]
    The apparatus of claim 1, wherein the first and second resistance heaters are operable to grow on the seed crystal arranged at the top of an interior of the crucible PVT-grow a growth crystal with a convex growth interface, a ratio between the radius of curvature of the convex growth interface and the diameter of the grown crystal. between about 2 and about 4.
    [3]
    The apparatus of claim 1, wherein: the top and bottom of the crucible are round, the first resistance heater is disc-shaped, and the first section of the second resistance heater is disc-shaped.
    [4]
    The apparatus of claim 3, wherein the first heater and the first section of the second resistance heater have outer diameters that are between 110% and 130%, included, of the outer diameter of the respective top and bottom of the crucible.
    [5]
    The apparatus of claim 3, wherein the first resistance heater and the first section of the second resistance heater have center holes with a diameter of between 25% and 75% of a diameter of the crucible. 10 15 20 25 30 22
    [6]
    The apparatus of claim 1, wherein: the side of the crucible is cylindrical, and the second section of the second resistance heater is cylindrical.
    [7]
    The apparatus of claim 6, wherein the top of the second section of the second resistance heater is arranged in a position of between 50% and 75% of the height of the crucible.
    [8]
    The apparatus of claim 6, wherein the inner diameter of the second section of the second resistance heater is separated from the crucible by a radial distance of between 10 mm and 25 mm.
    [9]
    The apparatus of claim 1, wherein the cavity has a height to diameter ratio of between 0.2 and 1.
    [10]
    An axial gradient type growth method comprising: (a) providing a crucible with a top, a bottom and a side extending between the top of the crucible and a bottom of the crucible, a first resistance heater spaced above the top of the crucible and a second resistance heater with a first resistive section spaced below the bottom of the crucible and a second resistive section spaced around the outside of the crucible side, (b) providing a seed crystal at the top of an interior of the crucible and a source material inside the crucible spaced between the seed crystals and the bottom of the crucible, (c) applying electrical power to the first and second resistance heaters of a sufficient extent to create in the interior of the crucible a temperature gradient of sufficient temperature to cause the source material to sublimate and condense on the seed crystal, thereby forming a growth crystal, and (d) maintaining the electrical power of the first and second the resistance heater until the growth crystal has grown to a desired size. 10 15 20 25 28
    [11]
    11. ll. The method of claim 10, wherein: the first resistance heater receives between 10% and 30% of the electrical power, and the second resistance heater receives between 70% and 90% of the electrical power.
    [12]
    The method of claim 10, wherein a voltage applied to each heater is less than 30 VAC RMS.
    [13]
    The method of claim 12, wherein a voltage applied to each heater is less than 25 VAC RMS.
    [14]
    The method of claim 10, wherein an inner and an outer side of the crucible and the heaters are in the presence of an inert gas of between 1 Torr and 40 Torr during the growth of the growth crystal.
    [15]
    The method of claim 10, wherein step (c) comprises controlling the electrical power applied to the first and second that a growth crystal grows on the resistance heater to cause the seed crystal, the grown growth crystal having a convex growth interface, wherein a ratio between the the radius of curvature of the convex growth interface and the diameter of the grown growth crystal are between about 2 and about 4.
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    同族专利:
    公开号 | 公开日
    CN104120489B|2017-04-26|
    US20160097143A1|2016-04-07|
    JP5406936B2|2014-02-05|
    SE537049C2|2014-12-16|
    CN102245813A|2011-11-16|
    CN102245813B|2014-08-06|
    DE112009003667T5|2012-10-11|
    WO2010077639A2|2010-07-08|
    US20100139552A1|2010-06-10|
    CN104120489A|2014-10-29|
    JP2012510951A|2012-05-17|
    US9228274B2|2016-01-05|
    WO2010077639A3|2010-09-10|
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    法律状态:
    2021-08-03| NUG| Patent has lapsed|
    优先权:
    申请号 | 申请日 | 专利标题
    US12055608P| true| 2008-12-08|2008-12-08|
    PCT/US2009/067112|WO2010077639A2|2008-12-08|2009-12-08|Improved axial gradient transportgrowth process and apparatus utilizing resistive heating|
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