Method for deep and vertical dry etching of Dielectrics
The invention relates to a method of etching of dielectrics, especially transparent dielectrics, such as S1O2, for example, for use in the manufacture of planar waveguides and gratings. The manufacture of photonic devices, such as echelle gratings, requires the fabrication of structures having vertical sidewalls. The structures are typically made by deep (5 to 10 μm) etching of an SiO2 layer. In such devices, especially echelle gratings, smooth and vertical etching is critical. Non-verticality of only 2°, e.g. 88° instead of 90°, can introduce additional optical losses of 3 dB in some cases.
Present technology used to etch SiO2 does not provide the right set of etch rate, verticality and control of sidewall profile. Deep (5-10 μm), vertical and smooth etching is critical for the fabrication of Si02 planar waveguides, especially for reflective gratings. Various etching techniques have been disclosed. See, for example, US patent numbers 5,013,398; 5,013,400; 5,021 ,121; 5,022,958; 5,296,879; 5,595,627; 5,611 ,888; 6,117,786; and 6,299,724. Traditionally, deep etching has been accomplished by reactive ion etching (RIE) using various gases (CHF3/CF /H2). In RIE, a plasma is created, and the surface to be etched is bombarded with ions through a hard mask formed on the surface of the sample. Typically, the ions have to be of relatively high energy in order to achieve deep etching suitable for making gratings and the like. A further discussion of such processes can be found, for example, in B. Kim et al., J. Vac. Sci. Technol. A17, 2593, 1999; A. K. Dutta, Proceedings of International Symposium on Surfaces and Thin Films of Electronic Materials, 30, 169, 1995; M .V. Bazylenko and M. Gross, J. Vac. Sci Technol. A14, 2994, 1996; and Ph Nussbaum et a., Proceedings of the SPIE Conference on Micromachine Technology for Diffractive and Holographic Optics, Santa Clara, California, vol. 3879, 63 (1999).
Unfortunately, high energy ions also tend to penetrate the mask and thereby result in low mask selectivity. This has the effect of making it more difficult to
obtain vertical sidewalls. The high ion energy also reduces the capability to control efficiently the sample temperature. If the ion energy is reduce, there is insufficient energy to create the necessary deep etch.
Summary of the Invention According to the present invention there is provided a method of etching a dielectric sample to produce vertical sidewalls, comprising: performing a high rate plasma etch on said sample in the presence of a low energy ion bombardment using a main etchant gas giving a high amount of etching radicals; and controlling the sidewall profiles by varying the temperature of the sample.
The dielectric is typically Si02, especially silicon rich silicon glass (SRSG)
The etchant gas is preferably C F8 since this gives a high etch rate by creating a high amount of etching radicals, although other suitable gases creating a high amount of etching radicals could be employed.
The plasma is preferably provided by a high density plasma source having an RF energy in the region of 200 watts or more. An inductively coupled plasma (ICP) source enables the use of low energy ion bombardment. This gives high etching selectivity with a hard mask, typically a metal mask, such as aluminum. The energy of the ions should be sufficiently low that they do not significantly pass through the hard mask. Also, because the energy of the ions is low, they do not have the same impact on the temperature of the sample as high energy ions.
Other types of mask, such as photoresist and SiChrome have been tried. The best selectivity is obtained with a hard mask, and the preferred hard mask is aluminum, which under the right conditions gives a selectivity of about 80.
A careful choice of parameters (pressure, gas, ion energy, etc.) can allow the precise control of the etching verticality using the sample temperature as the control parameter.
The invention will now be described in more detail, by way of example, only with reference to the accompanying drawings, in which:-
Figure 1 is an SEM image of a Si02 ridge etched using the inventive process;
Figure 2 shows the effect of DC bias on selectivity and etch rate; and Figure 3 is a table showing the results obtained for various samples under different conditions.
An SiO2 sample, in this example, silicon rich silicon glass (SRSG) was placed in a vacuum chamber. An aluminum hard mask was formed on the Si02 sample in a manner known per se. Other materials, such as SiChrome or even photoresist can be employed. The preferred material is aluminum since this has been found to give the best selectivity.
The sample was subjected to a high rate deep plasma etch using C F8 as the etchant in Argon. The C4F8 generates a large amount of etching radicals, which contribute to the high etch rate. An inductively coupled plasma (ICP) source was used to generate the plasma. This permitted a low energy ion bombardment to be employed to perform the vertical etching.
By carefully setting the process parameters, such as pressure, gas, ion energy, etc., the inventors have found that they are able to control the verticality of the sidewalls using temperature as a control parameter.
Figure 1 shows an example of a SiO2 sample that has been etched in accordance with described process. It will be noted how straight and smooth the sidewalls appear at 4,500 magnification.
The precise parameters depend on the actual experimental conditions and can be determined by routine experiment. The inventors have found that as the ICP power increases from 1500 watts to 2000 watts, the etch rate increases by about 30%. However, the selectivity drops by more than 50%.
As the pressure increases from 5 mtorr 10 mtorr, the etch rate decreases by 40% and the selectivity increases by 70%. The selectivity is defined as the ratio of the etch rate into the SiO2/ etch rate into the mask.
The effect DC bias is shown in Figure 2. The optimized conditions are shown in the central box.
As the gas flow increases, the etch rate slightly increases. At an optimal gas flow of 33 to 66% of C F8 in Argon/ F8, mixture, the etching results are not significantly modified. Preferred conditions are an ICP power of 1500 watts, an RF power of 235 watts, a DC bias of 200 volts, a pressure of 8 mTorr, a C F8 flow rate of 25 seem, an argon flow rate of 25 seem, and a temperature of about 70°C. In accordance with the principles of the invention, the temperature can be varied to control the verticality of the sidewalls. These conditions give a selectivity of about 80 with an etch rate of 0.36 μm/min as shown in the Table in Figure 3.
By combining a high etch rate with a low energy bombardment, the inventors are able to achieve good selectivity because the low energy ions do not significantly penetrate the mask, especially if a hard mask is employed.
It will be appreciated by one skilled in the art that many variations of the invention are possible within the scope of the appended claims. All references are incorporate herein by reference.