Crystal-pulling apparatus for pulling and growing a...

Single-crystal – oriented-crystal – and epitaxy growth processes; – Apparatus – For crystallization from liquid or supercritical state

Reexamination Certificate

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C117S208000, C117S217000, C117S900000

Reexamination Certificate

active

06648967

ABSTRACT:

This application claims Paris Convention priority of Japanese Application No. 2001-342002 filed Nov. 7, 2001, the complete disclosure of which is hereby incorporated by reference.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a crystal-pulling apparatus for pulling and growing a monocrystalline silicon ingot according to the Czochralski method (CZ method hereinafter), and a method therefor.
2. Description of the Related Art
The CZ method has been employed as one of the methods for growing silicon single crystals. The CZ method proceeds as follows. Firstly, a polycrystalline silicon material is heated in a quartz crucible to a temperature higher than the melting point of that silicon material, to give a silicon melt. Then, a seed crystal is dipped into the silicon melt kept in the quartz crucible. After the seed crystal has been dipped and itself partially melted, pulling of the seed is started. During pulling, first a thin crystal section, called a neck, is grown to eliminate dislocation growth into the ingot. Then a crystalline ingot is developed from the neck as the crystal is allowed to increase its diameter gradually, so that first a cone-shaped portion, next a shoulder portion, and then a cylindrical portion with a uniform diameter may be formed. The crystalline seed, after having undergone the above steps, grows into a monocrystalline silicon ingot in the form of a solid cylinder.
While a silicon crystal grows according to the CZ method, the internal wall of a quartz crucible is in contact with the silicon melt and will gradually dissolve as a result of the reaction as represented by the following formula (1).
SiO
2
+Si→2SiO  (1)
As shown (FIG.
12
), the majority of SiO dissolving into the silicon melt (
1
) will evaporate, as SiO gas, from the free surface
1
a
of the silicon melt (
1
), whereas a small amount thereof will be incorporated through the solid-liquid interface (
1
b
) into the monocrystalline silicon ingot (
3
), to supply the ingot with oxygen which is an impurity. During the early phase of pulling, the contact area between the silicon melt (
1
) and the internal wall of the quartz crucible (
2
) is comparatively large, and thus the concentration of oxygen dissolving into the silicon melt (
1
) becomes very high. However, when the crystal growth process advances and a monocrystalline silicon ingot (
3
) starts to form as shown (FIG.
13
), the surface (
1
a
) of the silicon melt (
1
) gradually drops, and the contact area between the silicon melt (
1
) and the internal wall of the quartz crucible (
2
) becomes smaller compared with what is observed during the early phase of pulling. The reduction of the contact area between the crucible and the melt will cause the concentration of the oxygen transferring from the crucible (
2
) into the silicon melt (
1
) to decrease. Accordingly, a fully grown monocrystalline silicon ingot (
3
) will show an uneven oxygen distribution along its longitudinal axis: more specifically, the oxygen concentration will vary depending on whether the oxygen measurement is made at the seed end of the crystal, in the mid portion of the crystal, or at the tail end of the crystal.
N-type monocrystalline silicon ingot which is heavily doped with an element such as As, P or Sb is favored as a starting material for epitaxial wafers (epi-wafers hereinafter) used in the power discrete market, and its production tends to increase. Two of the essential requirements for a good epi-wafer substrate are its bulk resistivity and its intrinsic gettering capability. The intrinsic gettering capability of a wafer is closely related to the intrinsic oxygen concentration that has been grown into the crystalline structure. It was found in the past that there is a direct correlation between the bulk resistivity of a N-type silicon crystal and the oxygen concentration of such a heavily doped N-type monocrystalline silicon crystal. The lower the resistivity of a specific crystal is, the lower is the oxygen concentration that a crystal incorporates naturally into the crystal structure. The reason for this behavior is partially that elements such as As and Sb evaporate easily from the free surface of the melt while forming oxygen compounds, therefor reducing the oxygen amount in the melt. Take antimony (Sb) as an illustration. If Sb is in a silicon melt, it will bind with oxygen transferred to the melt, to encourage the further dissolution of oxygen, and then it will evaporate alone or as a compound in the form of Sb
2
O. As a result, if a silicon melt contains a high concentration of Sb, the concentration of coexistent oxygen will decrease, and thus it is difficult to achieve high oxygen incorporation into the a heavily doped Sb-type crystal. As seen above, it has been difficult to obtain an N-type monocrystalline silicon ingot that presents a low resistivity and a high oxygen concentration simultaneously.
SUMMARY OF THE INVENTION
An object of this invention is to provide a crystal-pulling apparatus for pulling and growing a monocrystalline silicon ingot whereby it is possible to produce a heavily doped N-type monocrystalline silicon while adjusting the oxygen concentration of the ingot to a desired level, and a method therefor.
A further object of this invention is to provide a crystal-pulling apparatus for pulling and growing a heavily doped N-type monocrystalline silicon ingot whereby it is possible to produce a monocrystalline silicon ingot whose oxygen concentration at the seed end is kept at a level determined by natural equilibrium conditions, while the reduction in oxygen concentration at the cylindrical portion and at the tail end which would be otherwise introduced, is effectively restrained, and a method therefor.
A first aspect of this invention relates to an improved crystal-pulling apparatus for pulling and growing a monocrystalline silicon ingot comprising, within a chamber, of a quartz crucible containing a silicon melt from which a monocrystalline silicon ingot will be pulled; a graphite crucible container which surrounds the outer wall of the crucible at the external base surface of the quartz crucible to support it; and a heater which surrounds the outer wall of the crucible container and is intended to heat the silicon melt. Its constitution has a further notable feature: a spacer which has a top area smaller than the area of the external base surface of the quartz crucible and consists of a material having a higher melting point than that of silicon, is inserted between the external base surface of the quartz crucible and the internal base surface of the crucible container while a seed crystal is pulled to produce a monocrystalline silicon ingot.
According to the first aspect of this invention, a specific property characteristic of the quartz crucible, that is, softening of a quartz during the pulling of a monocrystalline silicon ingot is utilized. When a quartz crucible softens, being heated by a heater to the softening temperature, the base of the quartz crucible will gradually undergo deformation, so that because of its own weight and the weight of the silicon melt kept in the crucible, the a gap formed between the crucible and the crucible container, will be abolished. If the quartz crucible starts to deform, its base will gradually become convex upwards, and thus the internal base area of the crucible will increase. The increased internal base area of the crucible will cause the area of the internal base of the quartz crucible in contact with the silicon melt to increase. Further, because then the silicon melt is raised upwards relative to a given level on the internal wall of crucible, provided that other things remain invariable, the surface of the silicon melt relative to the internal side-wall of crucible would be also raised. This implicit elevation of the surface of the silicon melt will retard the downfall of the same surface which will be brought about in association with the pulling of a monocrystalline silicon ingot. Thus, the downfall of the surface of the s

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