Dry-etching method

Abstract: In microwave dry etching, the substrate/resist etching selectivity is controlled by adding a material, such as an additional gas, to the reaction gas plasma that heats the substrate with greater energy transfer efficiency than the resist. For example, a W substrate having a resist is etched with an SF₆ reaction gas to which is added an Xe gas for generating incident ions that impinge the substrate with greater energy transfer than with respect to the resist. This produces a greater hot spot temperature for the substrate than the resist to increase the substrate/resist etching selectivity. The hot spot temperature difference can be further effected by applying a bias potential to the substrate during the etching with an RF power supply.

Description: The present invention relates to a dry-etching method and particularly, to a dry-etching method capable of acheiving highly selective etching. In a conventional dry-etching method, the reaction is triggered by active species from the plasma of a reactive gas. The reaction is promoted by the incident energy of the ions but anisotropy develops since there is anisotropy in the incident direction of the ions. In this case, the energy of the incident ions is transferred to the surface of the material to be etched to locally heat that portion, and the etching reaction proceeds very quickly due to the hot spot which is produced by the local heating (e.g. Journal of Vacuum Science and Technology, B4, 1986, p. 459). The measurement of the hot spot temperature has been reported in the Journal of Applied Physics, 64, 1988, p. 315. In low-temperature etching technology (Japanese Patent Laid-Open No. JP-A-60158627, Japanese Patent Laid-Open No. JP-A-63291423), the sample is maintained at a very low temperature to suppress the etching caused by the spontaneous reaction of incident particles such as radicals, and the etching reaction is established at the hot spot only in order to achieve high anisotropy. In the conventional dry-etching method, however, hot spots are produced on the portions that are desired to be etched as well as on the portions that are not desired to be etched due to ions incident from the plasma. Furthermore, the temperature of the hot spots has not been particularly controlled and the hot spot temperature becomes high. This can cause the etching reaction to proceed even on those portions that are not desired to be etched. Therefore, very highly selective etching is not realized. In the conventional dry-etching method, furthermore, the temperature of a hot spot is not sufficiently raised on the surface of the material that is to be etched depending upon the combination of ions incident from the plasma and the material that is to be etched. Therefore, the etching rate is small and a sufficiently large selectivity is not obtained. This problem becomes conspicuous particularly when the material to be etched is one that contains heavy atoms such as tungsten (W) and the like. Moreover, the conventional dry-etching apparatus is not provided with a mechanism for measuring and controlling the hot spot temperature. Therefore, the rate of the etching reaction is not sufficiently controlled, and the selectivity of the etching is small for the materials. An object of the present invention is to provide a dry-etching method capable of realizing highly selective etching of the materials. This object is achieved by a dry etching method as defined in claim 1. In particular, the application relates to dry-etching methods, wherein: (1) in the dry-etching method using plasma, the energy transfer efficiency from the incident ions to the atoms of the material to be etched is greater than the energy transfer efficiency from the incident ions to the atoms of the mask material or the energy transfer efficiency from the incident ions to the atoms of the mask material and of the underlying layer; (2) the ions having an atomic weight of greater than 60 are made incident at the time of etching the material containing atoms of an atomic weight greater than 60 by the plasma of a gas containing fluorine; (3) the ions having an atomic weight of greater than 60 are made incident on the material to be etched in the method of dry-etching the material that is patterned using a carbon containing photo-resist mask by the plasma of a gas containing fluorine; (4) a helium gas is used as an additive gas in the method of dry-etching the carbon containing photo-resist material by the plasma of a gas; (5) a material containing at least one kind of atoms selected from He, Li, Be and B in an amount of more than 1% is used as a masking material; and further relates to the dry-etching apparatus wherein: (1′) the dry-etching apparatus has an ion source capable of controlling the energy and ion seeds, a radical source and a method of time-of-flight measurement for measuring the temperature of the hot spots on the surface of the sample. The temperatures of the hot spots vary depending upon the incident energy of the ions and the energy transfer efficiency from the ions to the atoms of a solid material. Further, the energy transfer efficiency is determined by a mass ratio of an ion to an atom of a solid material. Here, if the incident energy of an ion is denoted by E, the mass of an ion by M 1 , the mass of an atom of a solid material by M 2 , the energy which the atom of solid material receives from the ion by T, and a mass ratio of the atom of a solid material to the ion by M 2 /M 1 = A, then a rate T/E at which the energy is given to the atom of a solid material when the ion comes into collision with the atom of solid material head-on is expressed by, T/E = 4 A/(1+A) 2 This equation is derived from the conservation of momentum and the conservation of energy principles. In practice, the energy is transferred from the incident ions to the surface of a solid material not only by the ions that come in head-on collision with atoms of a solid material, but also by ions that impact the surface at a scattering angle. In this case, however, merely a coefficient of sin 2  is multiplied when the scattering angle is , and the equation (1) can be used to represent the energy transfer efficiency. Figure 3 shows a relationship between the energy transfer efficiency from the ions to the surface of a solid material and the mass ratio A of the ions to the atoms of a solid material. The energy transfer efficiency becomes the greatest when the ion and the atom of a solid material have an equal mass (A = 1) and decreases as the mass ratio separates away from 1, i.e., as the difference in the mass increases between them. When the energy transfer efficiency is high, the energy of incident ions is quickly transferred to the surface of a solid material and the temperature of the hot spot becomes high. When the energy transfer efficiency is low, the temperature of the hot spot becomes low. Figure 4 is a diagram which specifically illustrates the relationships between atomic weights of atoms of solid materials and the energy transfer efficiency when incident ions are comprised of He + , Ne + , Ar + , Kr + and Xe + . The masses of these noble gas ions are nearly the same as the masses of halogen ions that are widely used in conventional dry etching, therefore, Figure 4 further illustrates the transfer efficiency from various halogen ions over the same range of atomic weights. The feature of the present invention resides in that the hot spot temperature on the surface of a solid material is controlled by controlling the energy transfer efficiency. This feature will now be described with reference to a first embodiment of the invention using the etching of W with an SF 6 gas plasma as an example, with the understanding that this embodiment is similarly suitable for the etching of Ta, Pb and Zr. In the conventional W etching, the energy transfer efficiency from the incident F + ion into W is as low as 0.34 and, hence, the hot spot temperature is low and the etching rate is small. As is obvious from Figure 4, furthermore, the energy transfer efficiency from an F + ion to the C atom of the resist or to Si is close to 1. With Si or resist, therefore, the hot spot temperature is high, and the etching rate is large. Therefore, the selectivity is small between W and Si or the resist. It will be understood from Figures 3 and 4 that if ions having a mass close to W are permitted to be incident, the energy transfer efficiency is improved making it possible to increase the hot spot temperature of W. The same is true if Xe + ions are made incident during the etching of Ta, Pb and Zr, according to Figure 4. If Xe ions are used with W, the energy transfer efficiency becomes close to 1. In this case, the energy transfer efficiency to Si or C having a mass different from that of W becomes as small as 0.6, and the hot spot temperature decreases causing the etching rate to become small and making it possible to obtain a large selectivity. From the above fact, furthermore, it becomes possible to increase the etching selectivity by controlling the hot spot temperature by increasing a difference in the mass between a material that is to be etched and a material that is not to be etched. As for the resist mask, for instance, there may be added He, Li, Be or B having a mass smaller than that of C to lower the etching rate. The hot spot temperature varies depending upon the energy of incident ions and upon the condition specific to the material. Optimum energy of the incident ions can be detected by providing the etching device with a method for measuring the hot spot temperature. It becomes further possible to automatically control the energy of the incident ions by utilizing the measured hot spot temperature to adjust or set the parameters of etching, such as the bias potential applied to the sample, etc. Figure 1 is a diagram illustrating a relationship between the ratio of Xe added to an SF 6 gas and the etching rate of W by a dry-etching method according to a first embodiment of the present invention. Figure 2 is a diagram illustrating a relationship between the ratio of Xe added to an SF 6 gas and the W/resist etching selectivity of W by the dry-etching method of the first embodiment of the present invention. Figure 3 is a diagram illustrating a relationship between the energy transfer efficiency from the ions in a dry-etching method to the surface of a solid material being etched and a mass ratio of the ions to the atoms of a solid material. Figure 4 is a diagram illustrating a relationship between the atomic weight of an atom of a solid material and the energy transfer efficiency thereof when the incident ions are He + , Ne + , Ar + , Kr + and Xe + in a dry-etching method. Figure 5 is a diagram illustrating a relationship between the ratio of Xe added to an SF 6 gas and the etching rate for Si by a dry-etching method which is not part of the present invention. Figure 6 is a diagram illustrating a relationship between the ratio of Xe added to an SF 6 gas and the Si/resist etching selectivity in a dry-etching method of Figure 5. Figure 7 is a diagram illustrating a relationship between the energy of He + ions and the etching rates for SiO 2 and Si when SiO 2 and Si are etched using the etching apparatus that has an F·CF 2 radical source of an He ion source by a method which is also not part of the present invention. Figure 8 is a diagram of a dry-etching apparatus for performing the method of the present invention. Figure 1 shows the relationship between the amount of Xe added to the SF 6 gas in the dry etching of W according to a first embodiment of the present invention. The dry etching of W has heretofore been carried out using the plasma of a gas containing fluorine such as SF 6 gas plasma. The rate of etching W based on the conventional SF 6 gas plasma is small and when the etching is conducted at a temperature as low as -30°C, the etching rate is 100 nm/min (when Xe/(SF 6 + Xe) = 0% in Figure 1). Under this condition, the rate of etching of the resist is 100 nm/min and the W/resist etching selectivity becomes 1. Therefore, SiO 2 has heretofore been used as a masking material to etch W. When SF 6 gas plasma is used, the rate of etching W is small because the ratio of mass between the W atoms and the incident ions is great and, hence, the energy of the incident ions is not efficiently transferred to the surface of the W material causing the hot spot temperature to remain low. That is, the atomic weight of W is 184 and the atomic weight of F + , which is a principal incident ion seed, is 19, and the mass ratio is: W/F = 9.7. Therefore, the energy transfer efficiency from the incident ions to W is as low as 0.34. If the transfer efficiency'is improved, the etching rate can be increased to be comparable to that of the case of Si etching (mass ratio Si/F = 1.5, energy transfer efficiency 0.96). In this embodiment, use is made of Xe having a mass comparable to that of W. Since the atomic mass of Xe is 131, the mass ratio is: W/Xe = 1.4, and the energy transfer efficiency from the incident ions to W is 0.97. Thus, the energy of the incident ions is efficiently transferred to W, and the hot spot temperature can be increased. Here, the Xe gas is a noble gas which can be safely used as an additive gas to SF 6 or as an ion source without seriously affecting the characteristics of the plasma. Furthermore, the first ionization potential of Xe is as low as 12.13 eV as compared with the first ionization potential of 17.4 eV of F, and the ionization efficiency of Xe is high in the plasma. In the experiment of this embodiment, the flow rates of SF 6 gas and Xe gas are adjusted to etch W based on the plasma of an SF 6 + Xe gas. The electric discharge is that of a microwave discharge that offers good ionization efficiency. The gas pressure is 1 Pa and the sample temperature is -30°C in order to suppress an undesired etching reaction such as side etching caused by radicals. As evident from the diagram of Figure 1, the energy transfer efficiency of the incident ions to W increases with an increase in the amount of Xe added to SF 6 during the initial stage, and the etching rate of W increases. As the amount of Xe added further increases, however, the amount of SF 6 which is an etchant decreases and the etching rate of W consequently decreases. Under the conditions of this embodiment, the etching rate of W becomes the greatest when the mixing ratio of Xe is 20%, i.e., about 700 nm/min. On the other hand, the rate of etching of the resist monotonously decreases with an increase in the mixing ratio of Xe. One of the reasons for this is that the amount of etchant decreases due to the decrease in the ratio of SF 6 . When the mixing ratio of Xe is 10%, however, the rate of etching of the resist is 50 nm/min which is a 50% reduction from when the mixing ratio of Xe is 0%. This is due to a reduction in the energy transfer efficiency of the incident ions to the resist since the incident ion seed changes from F + into Xe + in addition to being affected by a decrease in the amount of the etchant. The principal atoms of the resist are H and C. The atomic mass of H is as small as 1, and the mass ratio relative to the incident ion seed H/M 1 is usually smaller than 0.1. Therefore, the energy transfer efficiency from the incident ions to H is as small as 0.33, and the energy is transferred from the incident ions to the resist chiefly via C atoms. In the plasma of 100% of SF 6 gas, the incident ions are chiefly F + . Since the mass ratio is: C/F = 0.63, the energy transfer efficiency from the incident ions to the resist is 0.95. If Xe is added to SF 6 , the incident ions become chiefly Xe. In this case, the mass ratio is C/Xe = 0.092 and the energy transfer efficiency becomes as small as 0.23. Therefore, addition of Xe lowers the hot spot temperature of the resist and lowers the etching rate. Figure 2 is a diagram showing a relationship between the ratio of Xe added to SF 6 and the W/resist etching selectivity in this embodiment. When SF 6 is 100%, ( Xe/(SF 6 + Xe) = 0% , the etching rate of W is small and is comparable with the rate of etching of the resist; i.e., the selectivity is 1. When Xe is added to the SF 6 gas, the W/resist etching selectivity increases due to an increase in the hot spot temperature of W and a decrease in the hot spot temperature of the resist. Under the conditions of this embodiment, the greatest selectivity of 28 is obtained with the rate of Xe added is at an addition ratio of 40%. As the rate of Xe addition is further increased, the feeding amount of the etchant decreases, the rate of etching W becomes small and the W/resist etching selectivity decreases. As an alternative to using Xe + ions, it is also possible to use Kr + ions as the incident ions in the etching of W, according to the first embodiment of the invention. As shown in Figure 4, the energy transfer efficiency for Kr is less than that for Xe to W, but the W resist etching selectivity may still be suitable under certain conditions. Further in the foregoing description the etching of W was discussed, but the above-mentioned method can be effectively adapted to achieve highly selective etching of films that contain heavy elements such as Ta 2 O 5 and PZT . From Figure 4, it can be seen that the mass ratio of the heavy elements contained in such films to Kr and particularly Xe permit a high energy transfer efficiency fo these ions to the atoms of the films while maintaining a correspondingly low energy transfer efficiency to the atoms of typical resist materials for thereby achieving highly selective etching of these types of films. Figure 5 is a diagram showing the results of dry-etching Si using an (SF 6 + Xe) gas mixture by the dry-etching method according to an example which is not part of the present invention. When Xe is added to the SF 6 gas, the energy transfer efficiency of Xe to the resist becomes as small as 0.23 as described in embodiment 1, and the hot spot temperature on the resist surface decreases and the rate of etching of the resist becomes very small. On the other hand, the mass ratio of Si/Xe is 0.21 and the energy transfer efficiency is as small as 0.57 which , however, is about twice as great as the energy transfer efficiency to the resist of 0.23. Therefore, the hot spot temperature of Si affected by the Xe ions becomes higher than the hot spot temperature of the resist. However, since the transfer efficiency is about 60% of the energy transfer efficiency of F + to Si which is 0.96, the addition of the Xe gas causes the amount of the etchant to decrease and the hot spot temperature to decrease even under the same etching conditions, and the rate of etching Si becomes very small like that for the resist. However, the energy transfer efficiency of Xe + to Si is 0.57 which is greatly different from that of the energy transfer efficiency of Xe + to the resist of 0.23, and there exists a large difference in the hot spot temperature between these surfaces. Therefore, a suitable bias potential is applied to the sample why in order to control the hot spot temperature on the surface of Si to be a temperature at which the etching reaction takes place and the hot spot temperature on the surface of the resist to be a temperature at which the etching reaction does not take place. In the case of this example, the microwave plasma etching is carried out while applying a bias of a frequency of 13,56 MHz at a power of 100 W to the sample. The bias may be applied by any other conventional method. In order to suppress the etching reaction by radicals, furthermore, the etching is carried out by maintaining a sample temperature at -130°C under a gas pressure of 1 Pa and changing the mixing ratio of SF 6 and Xe. Under the above bias conditions, the hot spot temperature of Si rises to a temperature high enough to create the etching reaction due to the incidence of Xe + . Therefore, the etching rate is decreased by the addition of Xe by only a rate at which the amount of etchant is decreased. On the surface of the resist, on the other hand, the hot spot temperature is not sufficiently elevated by the addition of Xe + under the above bias conditions, and the etching rate is greatly decreased by the addition of Xe. Figure 6 shows the relationship between the mixing ratio of Xe gas and the Si/resist etching selectivity in this example. It will be understood that a very high selectivity, as high as 30, can be obtained with an Xe mixing ratio of 40%. Furthermore, the Si etching rate is 600 nm/min which is large enough for practical applications. The above etching method can even be applied to systems other than the SF 6 /Xe mixture system in an Si/resist dry-etching method. That is, the incident ion seed is so selected as to develop a difference in the energy transfer efficiency between a material that is to be etched and a material that is not to be etched, and a suitable bias is applied to set the hot spot temperature of the material to be etched to a value high enough for the etching reaction to proceed and to also set the hot spot temperature of the material that is not to be etched to a value at which the etching reaction is adequately decreased. Thus, highly selective etching can be performed. The incident ions may be obtained, not only from a gas that is mixed into the plasma, but from an independent source of ions generated from a separate plasma source, for example, that is added to the etching chamber. Moreover, if a separate source of ions is generated for providing the incident energy, then neutral particles may be made to be incident instead of ions. In the experiment of this embodiment, an organic resist is used as a masking material. Though the energy transfer efficiency of Xe + to C is as small as 0.23, the addition of atoms having an atomic weight smaller than that of C as atoms of resist causes the energy transfer efficiency to further decrease and the selectivity to further increase. Examples of such atoms include He, Li, Be and B. Addition of at least one kind of these elements to the resist material in an amount of greater than 1% enables the energy transfer efficiency from the incident ions to the resist mask to be decreased and the selectivity relative to Si to be increased. The resist mask can be effectively used even in the case of etching a material to be etched containing atoms having atomic weights greater than that of C. Similar effects can further be obtained by using inorganic resists such as that of diamond which consists chiefly of carbon, in addition to using organic resists. Figure 7 is a diagram illustrating a relationship between the energy of He + ions and the etching rates for SiO 2 and Si when SiO 2 and Si are etched by using an etching apparatus having a source of F·CF 2 radicals and a source of He ions. SiO 2 includes oxygen (O) atoms. Therefore, the etching selectivity for Si can be improved if the energy transfer efficiency to O atoms is increased to be higher than that for the Si atoms. The energy transfer efficiency becomes the greatest when the mass of the incident ions is equal to the mass of the atoms of the solid material, and the energy transfer efficiency decreases with an increase in the mass ratio. In order to increase the energy transfer efficiency to O so that it is greater than the energy transfer efficiency to Si, therefore, ions lighter than O sould be used. In this example, He ions are used as such incident ions. The energy transfer efficiency of He + to O is 0.64 which is higher than the energy transfer efficiency to Si of 0.44. Therefore, the hot spot temperature of SiO 2 becomes sufficiently high with the He + incidence of 200 eV, and the etching rate is saturated with the feeding rate of radicals. With Si, on the other hand, the feeding rate is obtained with the He + incidence of 400 eV. It is therefore made possible to obtain a selectivity of greater than 10 at around the He + incident energy of 200 eV. Favorable results are exhibited to some extent even when an He gas is added to the conventional plasma of CF 4 gas. However, the first ionization potential of He is 24.6 eV which is greater than the ionization potential of F of 17.4 eV, and the He gas is not allowed to completely suppress the incidence of the F + ions. Further, the energy transfer efficiency from the F + ions to Si is 0.96 which is a little different from the energy transfer efficiency to  of 0.99. Therefore, the effect decreases with the plasma of (CF 4 + He) gas that is not capable of preventing the incidence of F + ions or CF X + ions. In practice, however, there exists no problem if the discharge conditions are so set that He + becomes much more than F + . In etching a resist, such as a multi-layer resist, furthermore, it is possible to greatly increase the energy transfer efficiency to H in the resist to 0.64 by permitting the He + ions to act thereupon. A simple and efficient method consists of adding an He gas in etching the resist at a low temperature using the plasma of an O 2 + Cl 2 gas. Figure 8 is a diagram of a dry-etching apparatus for performing the method according to the present invention which comprises a magnetron 1, a waveguide 2, a discharge zone 3, a gas inlet 4, an electromagnet 5, a sample stage 6, a refrigerant inlet 8, a heater 9, a heater power supply 10, a vacuum pump 11, a radical source 12, an ion source 13, a flight tube 14, a quadrupole mass separator 15, a time-of-flight measurement system 16, a measurement and control computer 17, and an RF power supply 18. In this apparatus, the microwaves generated by the magnetron 1 are guided through the waveguide 2 and are radiated into the discharge zone 3. Further, a gas of a predetermined pressure is introduced from the gas inlet 4 into the discharge zone 3, and a plasma is efficiently generated by the microwave electric discharge by using the electromagnet 5 in order to etch the sample 7 placed on the sample stage 6. The sample stage 6 is equipped with the refrigerant inlet 8 for cooling the sample to a low temperature. The heater 9 is provided with electric power from the heater power supply 10. A bias power is applied to the sample 7 from the RF power supply 18. Furthermore, the radical source 12, ion source 13, flight tube 14, quadrupole mass separator 15, time-of-flight measurement system 16, and measurement and control computer 17 are provided in order to measure the hot spot temperature, and the measurement and control computer 17 works to control the RF power supply 18, ion source 13 and radical source 12. Described below is a method of measuring the hot spot temperature and a method of utilizing the measured results to adjust the etching parameters. First, radicals of etchant are generated from the radical source 12 and are absorbed by the sample 7. Then, predetermined ions are permitted to be incident upon the sample 7 from the ion source 13 so that the etching reaction takes place at the hot spot and the reaction product is desorbed. In this case, the reaction product is desorbed at a rate in accordance with the Maxwell-Boltzmann distribution that reflects the hot spot temperature. Therefore, the desorption rate of the reaction product is found by the flight tube 14, quadrupole mass separator 15, and time-of-flight measurement system 16 thereby to measure the hot spot temperature. The measured results are analyzed by the measurement and control computer 17. The measurement and control computer 17 automatically controls the radical source 12 and the ion source 13 thereby to automatically find a relationship between the incident energy of ions of various masses and the hot spot temperature. The measurement and control quadrupole mass separator 15 in order to simultaneously measure plural kinds of hot spot temperatures on the surface of the solid material. This measurement makes it possible to determine the ion seed and the incident energy of ions best suited for obtaining a hot spot temperature that helps accomplish the greatest selectivity. A bias power from the RF power supply 18 is set in order to set the energy of the incident ions. In the apparatus as described above, even the RF power supply is controlled by the measurement of the hot spot temperature so that the optimum etching parameters can be achieved. Furthermore, the etching conditions that are found are stored in the measurement and control computer 17 in order to automatically adjust or set the etching parameters. In the case of polycrystalline and amorphous samples, the hot spot temperature is measured at around the etching conditions that are stored, though the hot spot temperatures vary depending upon the film-forming conditions thereby to automatically determine optimum conditions within short periods of time. As described above, the dry-etching method according to the present invention are employed in the process for manufacturing semiconductors in order to solve the problems inherent in the prior art and to realize highly selective etching of the materials.

Claims: A dry etching method, comprising the steps of: supporting a body having on a surface a material to be etched comprising an element of atomic weight greater than 60 and a material which is not to be etched in a dry etching apparatus; supplying a reaction gas for the dry etching and adding to the reaction gas an additional gas for heating of the body during the dry etching, said additional gas comprising atoms of an element of atomic weight greater than 60; forming a plasma of the reaction gas and the additional gas and exposing said surface of the body to the plasma; and etching and heating the body with the plasma; wherein said material which is not to be etched comprises a resist including carbon; and atomic weights of the plasma ions derived from the additional gas, the material to be etched and the material not to be etched are such that the energy transfer efficiency from ions of the additional gas to the material to be etched is greater than that from the ions of the additional gas to the material not to be etched, so that the hot spot temperature of said material to be etched is made greater than that of said material not to be etched during said etching, the energy transfer efficiency T/E being given by: T/E = 4A / (1+A) 2 where T is the energy received by an atom of the solid material with which the ion collides, E is the energy of the ion of the additional gas, A is the ratio M 2 /M 1 of the mass M 1 of the ion and the mass M 2 of the atoms of the solid material. A dry etching method according to claim 1, wherein said reaction gas is a gas containing fluorine. A dry etching method according to claim 1 or 2, wherein said material to be etched is tantalum, tungsten, lead or zirconium. A dry etching method according to claim 1, 2 or 3, wherein said additional gas is selected from Kr and Xe. A dry etching method according to claim 4, wherein the additional gas is Kr or Xe that is added in an amount of 10 to 50% with respect to the reaction gas. A dry etching method according to claim 5, wherein the material to be etched is Ta, W, Pb or Zr, and the reaction gas is SF 6 . A dry etching method according to claim 1, wherein said material not to be etched is a mixture of resist and an additional element selected from He, Li, Be and B. A dry etching method according to any one of claims 1 to 7 comprising controlling the hot spot temperature of the material to be etched by monitoring the hot spot temperatures of the materials and applying a bias potential to the body by means of an RF power supply in accordance with the monitoring. A dry etching method according to any of claims 1 to 8, wherein a bias potential is applied with respect to said body for increasing the incidence of said additional gas ions for increasing the heating of the body.

Inventors: KUMIHASHI TAKAO, TACHI SHINICHI, TSUJIMOTO KAZUNORI, KUMIHASHI, TAKAO, TACHI, SHINICHI, TSUJIMOTO, KAZUNORI, TSUJIMOTO, KAZUNORI, SAKURAGAOKADANCHI 5-305
Applicants: HITACHI LTD, HITACHI, LTD.
Application year: 1992
Main classification: H01L21
IPC codes: C23F4, H01L21, G03F7