Ohmic contact electrodes for n-type semiconductor cubic boron nitride

Abstract: An ohmic contact electrode formed on an n-type semiconductor cubic boron nitride by using a IVa metal; an alloy with a IVa metal; a metal with Si or S; an alloy with Si or S; a metal with B, Al, Ga, or In; an alloy with B, Al, Ga, or In; a Va metal; or an alloy with a Va metal.

Description: BACKGROUND OF THE INVENTION Field of Invention The present invention relates to an ohmic contact electrode for an n-type semiconductor cubic boron nitride and a method for forming such an electrode. Description of Related Art Attention has been given to a semiconductor cubic boron nitride as a new material for semiconductor devices such as diodes, transistors, sensors, and so on. Although an insulating cubic boron nitride is known broadly, that which is discussed here is a semiconductor cubic boron nitride having low resistivity. A cubic boron nitride has a wide forbidden band width (7.0 eV) and a high heat-proof temperature (1300°C), and is chemically stable. Consequently, a semiconductor cubic boron nitride has been strongly expected to be an excellent material for environment-proof power devices, and blue light emission elements. A cubic boron nitride does not naturally exist but can be formed through high-pressure synthesis. Further, recently, the formation of thin film through vapor phase synthesis has been reported. A p-type cubic boron nitride can be obtained by doping beryllium (Be). An n-type cubic boron nitride, on the other hand, can be obtained by doping sulfur (S) or silicon (Si). At resent, a pn-junction diode is produced for trial by using a high-pressure synthetic method in such a manner that an n-type cubic boron nitride is continuously grown with a p-type cubic boron nitride as a seed crystal. The pn-junction diode which is produced has a diode characteristic under 650°C. Further, it has been reported that a pn-junction diode emits, by injection of minority carries, light from ultraviolet to blue centering around 340 nm. A contact between a metal and a semiconductor is either a Schottky contact or an ohmic contact. The Schottky contact has a rectification property so that a current does not flow in a reverse direction. In the case of producing semiconductor devices, it is very important to form electrodes which can be formed by ohmic contact. The term "ohmic contact electrode" means an electrode in which the characteristic of a current flowing through the electrode and the characteristic of a voltage across the electrode are symmetrical forward and backward in accordance with the Ohm's law. Further, it is preferable that the contact resistance is reduced as much as possible. The term "contact resistance" is defined as a voltage to be applied so as to make a unit current flow through a unit contact surface. The unit of the contact resistance is Ω·cm 2 . There has not yet been found a superior electrode for an n-type cubic boron nitride. Although silver (Ag), silver paste, or the like is used as an electrode for an n-type cubic boron nitride ((1) R.H.Wentorf, Jr.: J. of Chem. Phys. Vol. 36 (1962) 199O; (2) 0. Mishima, etc.: Science Vol. 238 (1987) 181), there has been no report that an ohmic contact could be obtained. The technique for forming ohmic contact is necessary and indispensable to produce semiconductor devices. Further, if an ohmic contact is obtained, it is desirable that the contact resistance in the ohmic contact portion be reduced as much as possible. The contact resistance of general electron devices is 10 -2 Ω·cm 2 or less, and a smaller contact resistance of 10 -4 Ω·cm 2 or less is required in high-speed and high-frequency devices. If a formed contact is not an ohmic one but a Schottky one, carriers cannot be effectively Injected into a produced device because of the existence of a Schottky barrier in the contact electrode portion even when the current is to be made to flow in one device. This results in low efficiency of carrier injection. Further, the voltage drop across the contact electrode portion is remarkably large because the resistance is larger at the contact electrode portion. Therefore, the effective voltage applied to the device ends up being small. As a result, the particularly desireable characteristics discussed above for the device cannot be obtained. Further, the generation of heat in the contact electrode portion is a large problem. Accordingly, the formation of an ohmic contact electrode is necessary and indispensable in crder to make it possible to utilize a semiconductor cubic boron nitride as a material for semiconductor devices. An object of the present invention is therefore to form an ohmic contact electrode on an n-type semiconductor cubic boron nitride. From semiconductors and semimetals, Vol. 15, "Contacts, junctions, Emitters", Academic Press, New York 1981, pages 1 and 9 to 18, different ohmic contacts for n-type III - V semiconductors such as GaAs are known. For obtaining the ohmic contact metals or a mixture of metals are deposited on the surface of the semiconductor to produce a degenerate surface layer. Possible materials are Si, Ge, Se or Te. About n-type cBN nothing is disclosed in this document. It is notified that in this document group IVb and VIb correspond to group IVa and VIa elements of this application. SUMMARY OF THE INVENTION The ohmic contact electrode for an n-type semiconductor cubic boron nitride according to the present invention is an electrode formed on an n-type semiconductor cubic boron nitride so that an ohmic contact electrode can be obtained by using: (1) a IVa-family metal which includes titanium (Ti), zirconium (Zr), and hafnium (Hf) or an alloy containing a IVa-family metal; or (2) a Va-family metal which includes vanadium (V), niobium (Nb), and tantalum (Ta) or an alloy containing a Va-family metal. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a band diagram in the case where a high concentration doped layer is formed in the vicinity of a metal/semiconductor interface when one of the following materials is applied to an n-type semiconductor cubic boron nitride: (1) IVa-family metal or an alloy containing a IVa-family metal; or (2) a Va-family metal or an alloy containing a Va-family metal. Fig. 2 is a band diagram in the case where high-density localized states are formed in the vicinity of a metal/semiconductor interface when one of the following materials is applied to an n-type semiconductor cubic boron nitride: (1) a IVa-family metal or an alloy containing a IVa-family metal; or (2) a Va-family metal or an alloy containing a Va-family metal. Fig. 3 is a plan showing an electrode pattern which was used in measuring the contact resistance between the semiconductor cubic boron nitride and the electrodes. In the drawing, hatched portions represent the electrodes: 1... Fermi-level of electrode; 2... Fermi-level of semiconductor; 3...lower end of conduction band of semiconductor; 4...upper end of valence band of semiconductor; 5...electrode/semiconductor interface. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS According to the present invention, an ohmic contact electrode can be obtained by coating an n-type cubic boron nitride with the following: (1) A IVa-family metal (Ti, Zr, or Hf) or an alloy containing a IVa-family metal; or (2) A Va-family metal (V, Nb, or Ta) or an alloy containing a Va-family metal. This technique has been found through repeated experiments. Although the reason is unclear why an ohmic contact is obtained by using the above mentioned metals or alloys, some possibilities can be considered. IVa-family elements When a IVa-family metal such as Ti, Zr, Hf, TiC, ZrNi, or the like, or an alloy containing a IVa-family metal is formed as an electrode on an n-type cubic boron nitride, the electrode constituent element/elements as well as boron and nitrogen are activated by the heating of a substrate at the time of electrode formation, radiation heat at the time of electrode evaporation, annealing after the electrode formation, etc., so that mutual diffusion is generated in an interface between the electrode and the semiconductor. The IVa-family elements (Ti, Zr, and Hf), on the other hand, are also apt to react with boron and nitrogen so as to easily form a boride such as TiB 2 , ZrB 2 , HfB 2 , etc. and a nitride such as TiN, ZrN, HfN, etc. This phenomenon is well known. Therefore, the mutual diffusion in the electrode constituent elements as well as boron and nitrogen is further accelerated. Moreover, a metal compound layer is formed in the electrode/semiconductor interface in which the mutual diffusion is generated, and the substantial electrode/semiconductor interface is shifted into a semiconductor layer so as to form a clean interface. Further, there is a possibility that the IVa-family elements (Ti, Zr, and Hf) diffused into the cubic boron nitride become donors for the cubic boron nitride. There is a further possibility that holes or defects formed at places where boron and nitrogen have been removed by the diffusion become donors. As a result, an n-layer (n + layer) doped with high concentration is formed in the region where the mutual diffusion has been generated. Although the cubic boron nitride is of the n-type originally, it becomes of the n-type having a doping concentration considerably higher than the original mean doping concentration. The thickness of the barrier layer is reduced by the high-concentration doping so that the contact becomes ohmic by a tunneling current. Si or S Similarly, when a metal or alloy containing Si or S is formed as an electrode on an n-type cubic boron nitride, the Si or S contained in the electrode is activated by heating of a substrate at the time of electrode formation, radiation heat at the time of electrode evaporation, annealing after the electrode formation, etc., so that the Si or S gradually diffuses into the adjacent cubic boron nitride. The Si or S acts as an effective donor in the cubic boron nitride. This phenomenon is well known. Therefore, in the region where Si or S has been diffused, an n-layer (n + -layer) doped with high concentration is formed. B, Al, Ga, or In Similarly when a metal or alloy consisting of at least one of B, Al, Ga and In is formed as an electrode on an n-type cubic boron nitride, an electrode constituent element/elements as well as boron and nitrogen are activated by heating of a substrate at the time of electrode formation, radiation heat at the time of electrode evaporation, annealing after the electrode formation, etc., so that mutual diffusion is generated in an interface between the electrode and the semiconductor. Such elements as Al, Ga, In, etc. easily react with nitrogen so as to easily form nitride such as AlN, GaN, InN, etc. This phenomenon is well known. Also in the case where an electrode includes B, of course, nitrogen diffuses into B. Further, Al easily forms boride such as AlB 2 , etc. This is well known. Therefore, the mutual diffusion in the electrode constituent elements as well as boron and nitrogen is further accelerated. Moreover, a metal compound layer is formed in the electrode/semiconductor interface in which the mutual diffusion is generated, and the substantial electrode/semiconductor interface is shifted into a semiconductor layer so as to form a clean interface. Va-family metal Similarly, when a Va-family metal such as V, Nb, Ta, VC, Nb 3 Al, or the like, or an alloy containing a Va-family metal is formed as an electrode on an n-type cubic boron nitride, an electrode constituent element/elements as well as boron and nitrogen are activated by heating of a substrate at the time of electrode formation, radiation heat at the time of electrode evaporation, annealing after the electrode formation, etc., so that mutual diffusion is generated in an interface between the electrode and the semiconductor. The Va-family elements (V, Nb, and Ta) are also apt to react with boron and nitrogen so as to easily form a boride such as VB 2 , NbB 2 , TaB 2 , etc. and a nitride such as VN, NbN, TaN, etc. This phenomenon is well known. Therefore, the mutual diffusion in the electrode constituent elements as well as B and N is further accelerated. Moreover, a metal compound layer is formed in the electrode/semiconductor interface in which the mutual diffusion is generated, and the substantial electrode/semiconductor interface is shifted into a semiconductor layer so as to form a clean interface. Presently for all four types of coatings, there is the possibility that holes or defects formed at places where boron or nitrogen have been removed by the diffusion thereof into the electrode act as donors. In fact, in the case of GaN which is a III-V family compound and which is of the same kind as boron nitride, extreme n-type semiconductor characteristics are shown without any doping. This is, perhaps, because holes at which nitrogen has been removed act as donors. As a result of mutual diffusion, an n-layer (n + -layer) in which high concentration donor is formed in the region in the vicinity of the interface between the electrode and the cubic boron nitride. Although the cubic boron nitride is of the n-type originally, it becomes of the n-type having a donor concentration considerably higher than the original mean donor concentration. The thickness of the barrier layer is reduced by the high-concentration donor so that the contact becomes ohmic by a tunneling current. In an ideal case, whether a metal/semiconductor contact becomes an ohmic one or a Schottky one is determined depending on the work function ( m ) of the metal and the electron affinity (X s ) of the semiconductor. Here, the work function of a metal is energy required for drawing out electrons in Fermi-level to an infinite distance. The electron affinity of a semiconductor is energy required for drawing out electrons existing in the bottom of a conduction band to an infinite distance. In the case of an n-type semiconductor, the height ( B ) of a barrier in a metal/semiconductor contact is expressed by the following equation.  B =  m - X s The contact becomes therefore: an ohmic one when  B < 0; and a Schottky one when  B > 0. Since  B represents the height of the barrier, electrons are checked by the barrier if the value of  B is positive so that the contact becomes a Schottky one, while if the value of  B is negative, there is no barrier so that the contact becomes an ohmic one. It seems, from the above equation, that an ohmic contact can be obtained if a metal having a low work function is selected to be an electrode. In an actual metal/semiconductor contact, however, defects exist in a metal/semiconductor contact interface so as to form localized states (also called interface states,  0 : interface level) in the vicinity of the center in a band gap. If a large number of defects exist, the Fermi-level of the semiconductor is pinned up to the level of  0 . As a result, if the band gap of the semiconductor is represented by E g ,  B is expressed by the following equation, and hardly depends on the kind of metal at all.  B = E g -  0 The  is measured from the upper end of the valence band. This is because electrons from the metal can freely flow into the localized states to occupy the states so that the upper end of the localized states coincides with the Fermi plane of the metal and the Fermi level of the semiconductor coincides with the Fermi plane of the metal. Since it is the case, of course, that  B > 0, the metal/semiconductor contact becomes a Schottky one. This phenomenon is known as the pinning effect, and is remarkable particularly in the case of III-V family compound semiconductors. Further,  0 is about 1/3 - 1/2 times as large as E g . Also in the case of a cubic boron nitride, various kinds of interface defects may exist because it is not a single element material. Further, it is thought that a large number of interface defects exist which thereby cause the pinning effect because a cubic boron nitride crystal in the present circumstances is imperfect and has a large number of defects. Fig. 1 is a band diagram of a Schottky contact between a metal and an n-type semiconductor. A Fermi-level 2 of the semiconductor is continued from a Fermi-level 1 of the outside metal. A conduction band and a valence band exist in the semiconductor. The reference numerals 3 and 4 designate the lower end of the conduction band and the upper end of the balance band respectively. Since the semiconductor is of the n-type, the lower end 3 of the conduction band is approximate to the Fermi-level 2. The Fermi-level is pinned up to the interface level  0 at a boundary 5, so that a barrier having a height of  B is formed. The band is extremely bent upward in the vicinity of the boundary 5 because the donor density is high at the boundary. Although electrons accumulate in a downward curved portion 6 in the conduction band, the electrons may fly into the metal because of the tunneling effect. Since all the donors at the metal/semiconductor boundary are donated electrons and have positive charges of e . The positive charges are substantially uniformly distributed in the vicinity of the boundary and therefore this portion becomes a depletion layer in which no electron exists. The thickness of this portion can be calculated as follows. The following equation is established by integrating the Gaussian expression relating to an electric field and electric charges. d = [2 · ε S · ε 0 · (  B - V)/(e · N d )] 1/2 d:depletion layer width ε S :specific inductive capacity of the semiconductor ε 0 :dielectric constant in the vacuum V:applied voltage e:elementary electric charge N d : donor density in the semiconductor Although  B is a potential having an energy dimension as before,  B is treated below as a value of voltage obtained by dividing the potential by the elementary electric charge e . As seen from the equation (3), the depletion layer width d becomes smaller as the donor density in the semiconductor becomes higher. Since electrons easily pass through the thin depletion layer, the contact comes to have low resistance. This phenomenon will be described in more detail. Being a tunneling current, a current I per unit area can be expressed as follows. in which U represents the potential of a conduction electron measured from the bottom of the conduction band. U is expressed as follows as a function of x by integrating the Gaussian expression. U = e( B - V){1-(x/d)} 2 A = 4 π em e ·k 2 /h 3 in which, m e represents the effective mass of electrons in the semiconductor, h represents the Planck's constant, k represents the Boltzmann constant, and T represents the absolute temperature. In the case of free electrons, A is 120 A/cm 2 K 2 . If integration is made with respect to x,the following expression is obtained. I = AT 2 exp { - ( B - V)/V 00 } in which V 00 = hNd 1/2 / 4π (ε 0 ε S m e ) 1/2 Assuming that Nd=10 21 cm -3 , m e represents the free electron mass, and ε s =1, ε 0 =1, and T= 300°K, then V 00 is 0.56 V. Although the definition of  B has been described above, it is considered that if an n-type impurity is doped with high concentration, the  B itself decreases. This is because, as the localized states increase,  0 increases. E g is 7 eV, while  B decreases to about 6-3 v. It is assumed that the concentration of doping is extremely large in the vicinity of the boundary. If V 00 =0.5 V, this contact can be regarded substantially as an ohmic one from the equation (6). This is the case provided that the direction of the voltage from the semiconductor side toward the metal electrode is defined to be positive. Resistance (R c ) is obtained by partially differentiating the current with respect to the voltage on the assumption that V=0. The R c at this time is expressed by the following equation. R C = (V 00 /AT 2 )exp( B /V 00 ) Assuming that Nd=10 21 cm -3 , the mass of free electrons is represented by m e , εo=1, and T=300°K, then V 00 =0.56 V. If the coefficient before exp. is included in exp., the following equation is obtained. R C = exp {( B /0.56) - 16.77) If  B =6 V, R c becomes 10 -3 Ω·cm 2 , while if  B =7 V, R c becomes 10 -2 Ω·cm 2 . Assuming that Nd=10 20 cm -3 , then V00 becomes 0.18 V and the following equation is obtained. R C = exp {( B /0.18) - 17.91} If  B =3V, R c is about 10 -1 Ω·cm 2 , while if  B =2.5V, R c is about 10 -2 Ω·cm 2 . Thus, if an n-type impurity is doped with high concentration, the depletion layer thickness d decreases. Further, there is such an effect that the localized state of the surface is increased by high concentration doping so that  0 increases and  B decreases. Although description has been made as to the case where  B is about 1/2 - 2/3 times as large as the band gap (7eV), it is considered that the  B may be further reduced. Thus, the higher the donor density is made by high concentration doping, the more the thickness of the depletion layer decreases and the more  B decreases so as to make a tunneling current flow easily. Thus, it can be expected that the contact becomes ohmic. But the fact is not yet clearly understood. It may be that the localized state is transmitted by the tunnelling of electrons. Although such an effect can be expected by doping an impurity with high concentration, if the density of the impurity becomes so high, the result is rather undesirable because the resistance of the electrode increases. It is therefore believed that there exists a suitable range of the concentration. Further, the following possibility is considered. That is, a boride layer and a nitride layer have been formed in a metal/semiconductor interface so that a large number of defects have been brought into the interface and the vicinity of the interface. If the localized states 7 of high density exist in the vicinity of the boundary 5 as shown in Fig. 2, electrons may move between the metal and the semiconductor through the states so that a current may flow between them. Since the higher the localized state density is, the more easily electrons move, which makes the contact resistance become low. Moreover, since the movement is performed bi-directionally, the contact becomes ohmic. Other than those mechanisms described above, various mechanisms for obtaining an ohmic contact can be considered. They cannot be specified at the present time. An ohmic contact, however, can be obtained on an n-type cubic boron by forming an electrode according to the present invention. Examples Ohmic contact electrodes will be described more in detail with reference to examples. In order to inspect the kind of electrode material to which the electrode structure of the present invention was suitable, electrodes were produced from various materials and the ohmic property and contact resistance were evaluated. Example 1 Ti, TiAl, TiB 2 , TiC, TiCr, TiFe, TiN, TiNb, TiNi, TiSi, Zr, ZrAl, ZrB 2 , ZrC, ZrN, ZrNb, ZrNi, ZrS 2 , ZrSi 2 , Hf, HfB 2 , HfC, HfN, HfS 2 , and HfSi 2 were formed, as the electrodes, according to the present invention, on a high-pressure synthesized Si-doped n-type cubic boron nitride, and the ohmic property and contact resistance of the thus formed electrodes were evaluated. The electrodes were formed at a substrate temperature of 400°C by vacuum evaporation or sputtering depending on the material. At that time, an electrode pattern shown in Fig. 3 was formed on the cubic boron nitride by using a metal mask. The thickness of each of four electrodes was about 0.2 - 0.3 µm. The length was 0.8 mm and the width was 0.1 mm. They were arranged in parallel to each other at intervals of 0.1 mm, 0.2 mm, and 0.3 mm. The current-voltage characteristic between arbitrary electrcdes was measured in a voltage range of from -10V to +10V to thereby judge the ohmic property of the electrodes. With respect to the electrodes of which the ohmic characteristic has been measured, the contact resistance was measured by using a transmission line model on the basis of the resistance and electrode distance between two electrodes of the electrode pattern of Fig. 3. Table 1 shows the summary of the results of applying one of the above metals to form an ohmic contact electrode. Electrodes Containing IVa-Family Metal, Current-Voltage Characteristic, and Contact Resistance Electrode (atom ratio) Method of Formation Current-voltage Characteristics Contact Resistance (Ω·cm 2 ) Ti Vacuum evap. Ohmic 2 x 10 -1 TiAl Sputtering Ohmic 3 x 10 -1 TiB 2 Sputtering Ohmic 8 x 10 -2 TiC Sputtering Ohmic 1 x 10 -1 TiCr(80:20) Sputtering Ohmic 5 x 10 -1 TiFe Sputtering Ohmic 4 x 10 -1 TiN Sputtering Ohmic 7 x 10 -2 TiNb(66:34) Sputtering Ohmic 3 x 10 -1 TiNi(55:45) Sputtering Ohmic 7 x 10 -1 TiSi 2 Sputtering Ohmic 4 x 10 -2 Zr Vacuum evap. Ohmic 1 x 10 -1 ZrAl(75:25) Sputtering Ohmic 3 x 10 -1 ZrB 2 Sputtering Ohmic 7 x 10 -2 ZrC Sputtering Ohmic 9 x 10 -2 ZrN Sputtering Ohmic 6 x 10 -2 ZrNb(95:5) Sputtering Ohmic 5 x 10 -1 ZrNi Sputtering Ohmic 6 x 10 -1 ZrS 2 Sputtering Ohmic 4 x 10 -2 ZrSi 2 Sputtering Ohmic 5 x 10 -2 Hf Vacuum evap. Ohmic 8 x 10 -2 HfB 2 Sputtering Ohmic 6 x 10 -2 HfC Sputtering Ohmic 2 x 10 -1 HfN Sputtering Ohmic 9 x 10 -2 HfS 2 Sputtering Ohmic 6 x 10 -2 HfSi 2 Sputtering Ohmic 4 x 10 -2 As seen in Table 1, IVa-family metals such as Ti, Zr, Hf, TiC, ZrNi, etc. and alloys containing a IVa-family metal were formed, as the electrodes, on an n-type cubic boron nitride, so that the ohmic characteristic could be obtained although the contact resistance was a value within a range from 10 -2 to 10-1 Ω·cm 2 . Example 2 Si or S was added to Cr, W, Mn, Co, Ni, Pt, Ag, Zn, WC, MnZn, Ni 2 B, PtPd, or AgAl. As the cubic boron nitride, a high-pressure composition was used. The electrodes were formed at a substrate temperature of 400°C, and by the use of vacuum evaporation or sputtering depending on the material. As the electrode materials, used were those in which each of the Si-concentration and S-concentration was 0.1%-0.5%. At that time, an electrode pattern shown in Fig. 3 was formed on the cubic boron nitride by using a metal mask. The thickness of each of four electrodes was about 0.5-0.3 µm. The length was 0.8 mm and the width was 0.1 mm. They were arranged in parallel to each other at intervals of 0.1 mm, 0.2 mm, and 0.3 mm. The current-voltage characteristic between arbitrary electrodes was measured in a voltage range of from -10V to +10V to thereby judge the ohmic property of the electrodes. With respect to the electrodes the ohmic characteristic of which has been measured, the contact resistance was measured by using a transmission line model on the basis of the resistance and electrode distance between two electrodes of the electrode pattern of Fig. 3. The results of the above examples in which either Si or S were added with the above metals to form electrodes are summarized in Tables 2 and 3. Electrodes Containing Si, Current-Voltage Characteristic, and Contact Resistance Electrode Method of Formation Current-Voltage Characteristic Contact Resistance (Ω·cm 2 ) CrSi Vacuum evap. Ohmic 1 x 10 -1 WSi Vacuum evap. Ohmic 4 x 10 -2 MnSi Vacuum evap. Ohmic 2 x 10 -1 CoSi Vacuum evap. Ohmic 6 x 10 -2 NiSi Vacuum evap. Ohmic 6 x 10 -2 PtSi Vacuum evap. Ohmic 7 x 10 -2 AgSi Vacuum evap. Ohmic 8 x 10 -2 ZnSi Vacuum evap. Ohmic 5 x 10 -2 WCSi Sputtering Ohmic 2 x 10 -2 MnZnSi Sputtering Ohmic 9 x 10 -2 Ni 2 BSi Sputtering Ohmic 8 x 10 -2 PtPdSi Sputtering Ohmic 2 x 10 -1 AgAℓSi Sputtering Ohmic 9 x 10 -2 (Here, MSi does not mean that the element ratio of a metal or an alloy M to Si is 1:1 but means that a certain quantity of Si is contained in the metal or alloy M. That is, MSi does not mean a molecular formula with respect to Si.) Electrodes Containing S, Current-Voltage Characteristic, and Contact Resistance Electrode Method of Formation Current-Voltage Characteristic Contact Resistance (Ω·cm 2 ) CrS Vacuum evap. Ohmic 2 x 10 -1 WS Vacuum evap. Ohmic 2 x 10 -2 MnS Vacuum evap. Ohmic 9 x 10 -2 CoS Vacuum evap. Ohmic 7 x 10 -2 NiS Vacuum evap. Ohmic 1 x 10 -1 PtS Vacuum evap. Ohmic 8 x 10 -2 AgS Vacuum evap. Ohmic 6 x 10 -2 ZnS Vacuum evap. Ohmic 8 x 10 -2 WCS Sputtering Ohmic 2 x 10 -2 MnZnS Sputtering Ohmic 7 x 10 -2 Ni 2 BS Sputtering Ohmic 6 x 10 -2 PtPdS Sputtering Ohmic 1 x 10 -1 AgAℓS Sputtering Ohmic 8 x 10 -1 (Here, MS does not mean that the atom ratio of a metal or an alloy M to S is 1:1 but means that a certain quantity of S is contained in the metal or alloy M. That is, MS does not mean a molecular formula with respect to S.) Inspection was made on various metal materials and metal compounds, and as seen in Tables 2 and 3, the ohmic characteristic could be obtained with respect to all the material, although the contact resistance was a value within a range from 10 -2 to 10 -1 Ω·cm 2 . This fact makes reasonable the aforementioned estimation of the electron tunnel effect due to high concentration donor generation at the boundary between a metal and a semiconductor. Example 3 When a metal or a metal compound containing Si or S is used as a material for the electrode, inspection was made to obtain a proper concentration of Si or S. The electrodes were made from PtSi or PtS (this does not mean that the atomic ratio is 1:1 but means that a certain quantity of Si or S is contained in Pt) under the condition that the respective concentrations of Si and S were changed variously. The results of evaluation of the ohmic characteristic and contact resistance are shown in Tables 4 and 5. As the cubic boron nitride, a high-pressure composition was used. The electrodes were formed through a vacuum evaporation method without heating the substrates and subjected to annealing in an atmosphere of N 2 + H 2 (H 2 :10%) at 800°C for 10 minutes. Si Concentration, Current-Voltage Characteristic, and Contact Resistance Si Concentration (PtSi) Current-Voltage Characteristic Contact Resistance (Ω·cm 2 ) 0.01% Ohmic 2 x 10 0 0.1% Ohmic 1 x 10 -1 1.5% Ohmic 6 x 10 -2 1.0% Ohmic 5 x 10 -2 5.0% Ohmic 2 x 10 -1 10.0% Ohmic 3 x 10 -1 S Concentration, Current-Voltage Characteristic, and Contact Resistance S Concentration (PtS) Current-Voltage Characteristic Contact Resistance (Ω·cm 2 ) 0.01% Ohmic 1 x 10 0 0.1% Ohmic 9 x 10 -2 0.5% Ohmic 4 x 10 -2 1.0% Ohmic 4 x 10 -2 5.0% Ohmic 1 x 10 -1 10.0% Ohmic 2 x 10 -1 From the Tables 4 and 5, it can be seen that the ohmic contact could be obtained over all the range of Si- or S-concentration, and that although the contact resistance decreased as the Si- or S-concentration increases, it reached the minimum at several % and then increased thereafter. Further, it is not desirable to make the Si- or S-concentration excessively high, because the resistance of the electrode per se becomes high. In practice, it suffices to select the Si- or S-concentration to be about 1 % by weight. Example 4 B, AlB 2 , CrB 2 , SiB 4 , WB, Al, AlCu, AlSi, Ga, GaIn, GaSn, GaZn, In, InMg, and InSn were formed, as the electrodes on a high-pressure synthesized Si-doped n-type cubic boron nitride, and the ohmic property of the thus formed electrodes was evaluated. In the case of low melting point metals and alloys such as Ga, In, GaIn, etc., after electrode materials were set at two positions on a cubic boron nitride, electrodes were formed through alloying treatment in an N 2 atmosphere at 400°C for five minutes. The current-voltage characteristic between those electrodes was measured in a voltage range of from -10V to +10V to thereby judge the ohmic property of the electrodes. The other electrodes were formed by using a vacuum evaporation method or a sputtering method depending on the materials under the condition that the substrate temperature was kept at room temperature. After formation of the electrodes, annealing was made in an N 2 atmosphere at 400°C for 20 minutes. Further, in formation of the electrodes, an electrode pattern shown in Fig. 3 was formed on the cubic boron nitride by using a metal mask. The thickness of each of four electrodes was about 0.2-0.3 µm. The Length was 0.8 mm and the width was 0.1 mm. They were arranged in parallel to each other at intervals of 0.1 mm, 0.2 mm, and 0.3 mm. With respect to the electrodes the ohmic characteristic of which has been measured, the contact resistance was measured by using a transmission line model on the basis of the resistance and electrode distance between two electrodes of the electrode pattern of Fig. 3. Table 6 shows the summary of the results of the above examples. Electrodes Containing B, Al, Ga, or In; Current-Voltage Characteristic and Contact Resistance Electrode (atom ratio) Method of Formation Current-Voltage Characteristic Contact Resistance (Ω·cm 2 ) B Vacuum evap. Ohmic 4 x 10 -1 AℓB 2 Sputtering Ohmic 9 x 10 -2 CrB 2 Sputtering Ohmic 4 x 10 -1 SiB 4 Sputtering Ohmic 5 x 10 -2 WB Sputtering Ohmic 3 x 10 -1 Aℓ Vacuum evap. Ohmic 2 x 10 -1 AℓCu Sputtering Ohmic 5 x 10 -1 AℓSi Sputtering Ohmic 8 x 10 -2 Ga Alloying Ohmic - GaIn Alloying Ohmic - GaSn Alloying Ohmic - GaZn Sputtering Ohmic 6 x 10 -1 In Alloying Ohmic - InMg Sputtering Ohmic 7 x 10 -1 InSn Alloying Ohmic - As seen in Table 6, a metal or alloy consisting of at least one of the elements B, Al, Ga and In was formed, as an electrode, on an n-type cubic boron nitride, so that the ohmic characteristic could be obtained. The contact resistance of the electrode formed through vacuum evaporation or sputtering was within an order of 10 -2 -10 -1 Ω·Cm 2 . Example 5 V, VB 2 , VC, V 3 CO, VaG 3 , VN, VS, V 3 Si, V 2 Zr, Nb, Nb 3 Al, NbB 2 , NbC, Nb 3 Ga, Nb 3 Ge, NbN, NbS 2 , NbSi 2 , Ta, TaB 2 , TaC, TaN, TaS 2 , and TaSi 2 were formed, as the electrodes according to the present invention, on a high-pressure synthesized Si-doped n-type cubic boron nitride, and the ohmic property and contact resistance of the thus formed electrodes were evaluated. The electrodes were formed at a substrate temperature of 400°C by vacuum evaporation or sputtering depending on the material. At that time, an electrode pattern shown in Fig. 3 was formed on the cubic boron nitride by using a metal mask. The thickness of each of four electrodes was about 0.2-0.3 µm. The length was 0.8 mm and the width was 0.1 mm. They were arranged in parallel to each other at intervals of 0.1 mm, 0.2 mm, and 0.3 mm. The current-voltage characteristic between arbitrary electrodes was measured in a voltage range of from -10V to +10V to thereby judge the ohmic property of the electrodes. With respect to the electrodes the ohmic characteristic of which has been measured, the contact resistance was measured by using a transmission line model on the basis of the resistance and electrode distance between two electrodes of the electrode pattern of Fig. 3. Table 7 shows the summary of the results of the above example. Electrodes Containing IVa-Family Metal, Current-Voltage Characteristic, and Contact Resistance Electrode (atom ratio) Method of Formation Current-Voltage Characteristic Contact Resistance (Ω·cm 2 ) V Vacuum evap. Ohmic 3 x 10 -1 VB 2 Sputtering Ohmic 9 x 10 -2 VC Sputtering Ohmic 1 x 10 -1 V 3 Co Sputtering Ohmic 7 x 10 -1 V 3 Ga Sputtering Ohmic 5 x 10 -1 VN Sputtering Ohmic 8 x 10 -2 VS Sputtering Ohmic 5 x 10 -2 V 3 Si Sputtering Ohmic 6 x 10 -2 V 2 Zr Sputtering Ohmic 2 x 10 -1 Nb Vacuum evap. Ohmic 3 x 10 -1 Nb 3 Aℓ Sputtering Ohmic 5 x 10 -1 NbB 2 Sputtering Ohmic 8 x 10 -2 NbC Sputtering Ohmic 1 x 10 -1 Nb 3 Ga Sputtering Ohmic 5 x 10 -1 Nb 3 Ge Sputtering Ohmic 6 x 10 -1 NbN Sputtering Ohmic 9 x 10 -2 NbS 2 Sputtering Ohmic 5 x 10 -2 NbSi 2 Sputtering Ohmic 4 x 10 -2 Ta Vacuum evap. Ohmic 1 x 10 -1 TaB 2 Sputtering Ohmic 8 x 10 -2 TaC Sputtering Ohmic 1 x 10 -1 TaN Sputtering Ohmic 9 x 10 -2 TaS 2 Sputtering Ohmic 3 x 10 -2 TaSi 2 Sputtering Ohmic 4 x 10 -2 As seen in Table 7, Va-family metals such as V, Nb, Ta, VC, Nb 3 Al, etc. and alloys containing a Va-family metal were formed, as the electrodes, on an n-type cubic boron nitride, so that the ohmic characteristic could be obtained although the contact resistance was a value within a range from 10 -2 to 10 -1 Ω·cm 2 . It is effective to perform suitable annealing after formation of electrodes with the metals used in the above examples 1-5. Although the optimum values of the annealing temperature and time vary depending on the electrode material to be used, it is preferable to select the annealing temperature to be about 300°C - 1800°C. Since oxidation of the electrode may progress at the time of annealing depending on the electrode material, it is desirable to perform the annealing in an inert gas, N 2 or H 2, or in a vacuum. Further, in the case where the temperature is as high as 1000°C or more, it is preferable to perform annealing in an inert gas, N 2 or H 2, or in a vacuum, similarly to the above case, because of the oxidization or hexagonal boron-nitriding of the cubic boron nitride progresses when O 2 is present. Moreover, it is more effective to use a high temperature at the time of formation of the electrodes in place of annealing. It is desirable to select this temperature to be 300°C - 1800°C, although it depends on the electrode material. It is also more effective that a metal alloy of known dopant (Si, S, or the like) and a IVa-family element (Ti, Zr, or Hf) is formed, as the electrodes, on the n-type semiconductor cubic boron nitride. Moreover, if the electrodes according to the present invention and metal electrodes coated with Au, Ag, or the like having low resistance, are laminated to be a multilayer structure, the effect becomes more remarkable. As described above, a IVa-family metal (Ti, Zr, or Hf) or an alloy containing a IVa-family metal; or a Va-family metal or an alloy containing a Va-family metal is formed, as an electrode, on an n-type semiconductor cubic boron nitride, so that an ohmic contact can be obtained with respect to the n-type semiconductor boron nitride. Since this technique is indispensable to produce semiconductor cubic boron nitride devices, it is effective in formation of all kinds of devices.

Claims: An ohmic contact electrode contacting an n-type cubic boron nitride semiconductor, the electrode comprising at least one layer of a material selected from the group consisting of: a IVa metal; an alloy with a IVa metal; a Va metal; an alloy with a Va metal. An ohmic contact electrode according to claim 1 wherein said at least one layer comprises Ti, TiAl, TiB 2 , TiC, TiCr, TiFe, TiN, TiNb, TiNi, TiSi, Zr, ZrAl, ZrB 2 , ZrC, ZrN, ZrNb, ZrNi, ZrS 2 , ZrSi 2 , Hf, HfB 2 , HfC, HfN, HfS 2 , or HfSi 2 . An ohmic contact electrode according to claim 1 wherein said at least one layer comprises V, VB 2 , VC, V 3 Co, V 3 Ga, VN, VS, V 3 Si, V 2 Zr, Nb, NbB 2 , NbC, Nb 3 Ga, Nb 3 Ge, NbN, NbS 2 , NbSi 2 , Ta, TaB 2 , TaC, TaN, TaS 2 , TaSi 2 , or HfSi 2 . An ohmic contact electrode according to claim 1 wherein said electrode is a multilayer structure comprising at least one layer of a metal selected from the group consisting of Au and Ag. A method of forming the ohmic contact electrode according to claim 1, characterised by coating an Si-doped n-type cubic boron nitride with at least one layer of the material according to claim 1 at a substrate temperature from 300°C to 1800°C by vacuum evaporation, sputtering or alloying. A method according to claim 5, characterised in that the coating step is at a substrate temperature of substantially 400°C and the coating step is followed by an annealing step wherein the electrode is heated from 300°C to 1800°C in an atmosphere comprising an inert gas, N 2 , H 2 or a vacuum. A method according to claim 5, characterised in that after the coating step the Si-doped n-type cubic boron nitride is coated with at least one layer of a metal selected from the group consisting of Au and Ag.

Inventors: FUJITA NOBUHIKO, KIMOTO TUNENOBU, TOMIKAWA TADASHI, FUJITA, NOBUHIKO,, KIMOTO, TUNENOBU,, TOMIKAWA, TADASHI,, FUJITA, NOBUHIKO, C/O ITAMI WORKS OF SUMITOMO, KIMOTO, TUNENOBU, C/O ITAMI WORKS OF SUMITOMO, TOMIKAWA, TADASHI, C/O ITAMI WORKS OF SUMITOMO
Applicants: SUMITOMO ELECTRIC INDUSTRIES, SUMITOMO ELECTRIC INDUSTRIES, LTD.
Application year: 1991
Main classification: H01L29
IPC codes: H01L29