Electrode for plasma processing apparatus, plasma processing apparatus, plasma processing method and storage medium
a plasma processing apparatus and plasma technology, applied in the direction of electrical equipment, basic electric elements, electric discharge tubes, etc., can solve the problems of reducing the intensity of the electric field around the periphery of the wafer, substantially difficult to optionally control the distribution of the electric field, and cannot solve the above problems in nature. uniformity of the electric field of the plasma, enhanced uniformity of the electric field of the plasma
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example 1
[0101]Under the following conditions, the simulation as described above was performed. In this simulation, the magnitude of the sheath electric field was calculated, with the size of the recess 57 being fixed, while the relative permittivity of the dielectric in the recess 57 and the resistivity of the electrode plate 54 were changed, respectively.
(Simulation Conditions)
[0102]Diameter R of the recess 57: 100 mm
[0103]Thickness t2 of the recess 57: 5 mm
[0104]High frequency for the plasma generation: 100 MHz
[0105]Relative permittivity (∈) of the dielectric in the recess 57: 1 / 3.8 / 10 / 50
[0106]Resistivity (Ωm) of the electrode plate 54: no / 0.02 / 0.5 / 1 / 5 / 10
[0107]As the material actually used for setting the dielectric in the recess 57 at the relative permittivity as described above, a vacuum (∈: 1), powder of silicon dioxide (∈: 3.8), powder of ceramics, e.g., Al2O3 (∈: 10 to 50) and the like can be mentioned. In the case of setting the resistivity into the range as described above, each de...
example 2
[0111]Another simulation similar to the simulation in the above Example 1 was carried out, with the recess 57 having a 200 mm diameter R. As shown in FIGS. 12(a) to 12(e), it was found that the intensity of the electric field of the plasma can be reduced, over the region corresponding to the recess 57 (i.e., a region from the center of the wafer W to an approximately 100 mm radial point) can be reduced by gradually decreasing the relative permittivity of the recess 57, in the same manner as in the above simulation. Similarly, it was found that the intensity of the electric field of the plasma can be controlled, over the whole surface of the wafer W, by changing the resistivity of the electrode plate 54 together with the relative permittivity of the recess 57.
[0112]Additionally, as shown in FIG. 12(f), the intensity of the electric field of the plasma can be similarly controlled, by changing the relative permittivity of the dielectric in the recess 57 as well as by changing the thick...
example 3
[0113]Next, as shown in FIG. 13, still another simulation similar to the simulation in the above Example 1 was carried out, with the recess 57 having a 300 mm diameter R. Also in this simulation, it was found that the intensity of the electric field of the plasma can be reduced, over the region corresponding to the recess 57 (i.e., a region from the center of the wafer W to an approximately 150 mm radial point) can be reduced by gradually decreasing the relative permittivity of the recess 57, in the same manner as described above. Again, it was found that the intensity of the electric field of the plasma can be controlled, over the whole surface of the wafer W, by changing the resistivity of the electrode plate 54 together with the relative permittivity of the recess 57. From these results, it was found that the diameter R of the recess 57 is preferably set at a value less than the diameter of the support member 51, for example, 300 mm or less, because the sheath electric field (or ...
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