WO2002097874A1 - Method for deep and vertical dry etching of dielectrics - Google Patents

Method for deep and vertical dry etching of dielectrics Download PDF

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Publication number
WO2002097874A1
WO2002097874A1 PCT/CA2002/000784 CA0200784W WO02097874A1 WO 2002097874 A1 WO2002097874 A1 WO 2002097874A1 CA 0200784 W CA0200784 W CA 0200784W WO 02097874 A1 WO02097874 A1 WO 02097874A1
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WO
WIPO (PCT)
Prior art keywords
etching
sample
plasma source
deep
dielectric
Prior art date
Application number
PCT/CA2002/000784
Other languages
French (fr)
Inventor
Boris Lamontagne
Lynden Erickson
Dan-Xia Xu
Andre Delage
Siegfried Janz
Pavel Cheben
Sylvain Charbonneau
Original Assignee
Lnl Technologies Canada Inc.
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Lnl Technologies Canada Inc. filed Critical Lnl Technologies Canada Inc.
Publication of WO2002097874A1 publication Critical patent/WO2002097874A1/en

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic System or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/30Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
    • H01L21/31Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26 to form insulating layers thereon, e.g. for masking or by using photolithographic techniques; After treatment of these layers; Selection of materials for these layers
    • H01L21/3105After-treatment
    • H01L21/311Etching the insulating layers by chemical or physical means
    • H01L21/31105Etching inorganic layers
    • H01L21/31111Etching inorganic layers by chemical means
    • H01L21/31116Etching inorganic layers by chemical means by dry-etching

Definitions

  • the invention relates to a method of etching of dielectrics, especially transparent dielectrics, such as S1O 2 , for example, for use in the manufacture of planar waveguides and gratings.
  • dielectrics especially transparent dielectrics, such as S1O 2
  • 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 ⁇ m) etching of an SiO 2 layer.
  • 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.
  • 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 F 8 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.
  • Figure 1 is an SEM image of a Si0 2 ridge etched using the inventive process
  • Figure 2 shows the effect of DC bias on selectivity and etch rate
  • Figure 3 is a table showing the results obtained for various samples under different conditions.
  • SiO 2 sample in this example, silicon rich silicon glass (SRSG) was placed in a vacuum chamber.
  • An aluminum hard mask was formed on the Si0 2 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 F 8 as the etchant in Argon.
  • the C 4 F 8 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.
  • Figure 1 shows an example of a SiO 2 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 etch rate slightly increases.
  • 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 F 8 flow rate of 25 seem, an argon flow rate of 25 seem, and a temperature of about 70°C.
  • the temperature can be varied to control the verticality of the sidewalls.
  • 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.

Abstract

A method of etching a dielectric, such as SiO2, to produce vertical sidewalls is disclosed wherein the process is carried out at a high etch rate, using low energy ion bombardment, using C4F8 as a main etchant gas. The SiO2 sidewall profiles are controlled by varying the temperature of the temperature of the sample.

Description

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.

Claims

Claims
1. A method of etching a dielectric sample to produce vertical sidewalls, comprising: performing a high rate plasma etch on said dielectric 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.
2. A method as claimed claim 1 , wherein said dielectric is SiO2.
3. A method as claimed in claim 1 or 2, wherein said main etchant gas is C4F8.
4. A method as claimed in any of claims 1 to 3, wherein said plasma is provided by a high density plasma source.
5. A method as claimed in claim 4, wherein said high density plasma source is operated at a power of about 235 watts.
6. A method as claimed in claim 4, wherein said high density plasma source is an inductively coupled plasma source to permit said low energy bombardment.
7. A method as claimed in claim 6, wherein said inductively coupled plasma source operates at a power of about 1500 watts.
8. A method as claimed in any of claims 1 to 7, wherein said plasma etch is performed through a hard mask.
9. A method as claimed in claim 8, wherein said hard mask is aluminum.
PCT/CA2002/000784 2001-05-28 2002-05-28 Method for deep and vertical dry etching of dielectrics WO2002097874A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
CA2,349,032 2001-05-28
CA 2349032 CA2349032A1 (en) 2001-05-28 2001-05-28 Method for deep and vertical dry etching of sio2

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WO2002097874A1 true WO2002097874A1 (en) 2002-12-05

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20150034592A1 (en) * 2013-07-30 2015-02-05 Corporation For National Research Initiatives Method for etching deep, high-aspect ratio features into glass, fused silica, and quartz materials

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5468342A (en) * 1994-04-28 1995-11-21 Cypress Semiconductor Corp. Method of etching an oxide layer
US5711851A (en) * 1996-07-12 1998-01-27 Micron Technology, Inc. Process for improving the performance of a temperature-sensitive etch process
US5814563A (en) * 1996-04-29 1998-09-29 Applied Materials, Inc. Method for etching dielectric using fluorohydrocarbon gas, NH3 -generating gas, and carbon-oxygen gas

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5468342A (en) * 1994-04-28 1995-11-21 Cypress Semiconductor Corp. Method of etching an oxide layer
US5814563A (en) * 1996-04-29 1998-09-29 Applied Materials, Inc. Method for etching dielectric using fluorohydrocarbon gas, NH3 -generating gas, and carbon-oxygen gas
US5711851A (en) * 1996-07-12 1998-01-27 Micron Technology, Inc. Process for improving the performance of a temperature-sensitive etch process

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20150034592A1 (en) * 2013-07-30 2015-02-05 Corporation For National Research Initiatives Method for etching deep, high-aspect ratio features into glass, fused silica, and quartz materials
US9576773B2 (en) * 2013-07-30 2017-02-21 Corporation For National Research Initiatives Method for etching deep, high-aspect ratio features into glass, fused silica, and quartz materials

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