(1) Field of the Invention
This invention is related to MEMS devices, and more particularly, to methods of forming a MEMS scanning mirror with tunable resonance frequency.
(2) Description of the Related Art
Micro-electro-mechanical systems (MEMS), the smallest functional machines that can be manufactured currently, are made up of components ranging from a few micrometers to several millimeters in size. MEMS, a rapidly growing semiconductor field, have many important practical and potential commercial applications. MEMS scanning mirrors have been found in many applications such as barcodes, laser printers, projection displays, and rear projection TV's, for example. A MEMS scanning mirror is formed by the mirror itself, anchors, and a spring coupling the mirror and the anchors. Such a MEMS scanning mirror could be driven by either magnetic or electrostatic force. The MEMS scanning mirror device of the present invention is based on an electrostatic comb actuator.
A MEMS scanning mirror is usually driven at its resonance frequency under alternating current (AC) to achieve a high scanning angle. For different applications and products, the required resonance frequency might be different. The resonance frequency of a MEMS scanning mirror depends on the mirror's mass, its dimension, and materials properties such as the elastic modulus. The resonance frequency can be pre-determined through mask design and it can be adjusted by mirror mass change during mirror fabrication.
Adjusting resonance frequency through mirror mass change has been proven efficient. U.S. Patent Application 2009/0080051 to Yoon et al discloses removing a portion of the backside of a moving plate to a predetermined depth to reduce the weight of the moving plate and increase resonance frequency. However, the etching is performed without patterning.
U.S. Pat. No. 7,187,488 and U.S. Patent Application 2007/0117051, both to Fu, disclose trimming a sacrificial portion of a mirror by laser beam or ion beam. Since there is no etch selectivity with those methods, etch uniformity and frequency control can be very poor.
U.S. Pat. No. 7,217,587 (Fu) notes removing a mass by laser trimming, but using different steps from the invention.
It is the primary objective of the present invention to set a particular resonance frequency for a MEMS scanning mirror.
It is another objective of the invention to set a particular resonance frequency for a MEMS scanning mirror through mirror backside mass removal.
In accordance with the objectives of the invention, a method of fabricating a MEMS scanning mirror having a tunable resonance frequency is achieved. A silicon-on-insulator wafer is provided comprising a top silicon layer, a bottom silicon layer, and a silicon dioxide layer between the top and bottom silicon layers. A silicon dioxide hard mask is formed on the bottom silicon layer and patterned. Portions of the bottom silicon layer and the silicon dioxide layer are etched away from a backside of the silicon-on-insulator wafer and portions of the top silicon layer are etched away from the backside directly underlying the MEMOS scanning mirror wherein choosing a depth of the portions of the top silicon layer achieves the tunable resonance frequency for the MEMS scanning mirror. The bottom and top silicon layers are etched using the silicon dioxide hard mask and the silicon dioxide layer as hard masks and the silicon dioxide layer is etched using the silicon layer as a hard mask.
Also in accordance with the objectives of the invention, a method of setting a particular resonance frequency for a MEMS scanning mirror through mirror backside mass removal is achieved. A silicon-on-insulator wafer is provided comprising a top silicon layer, a bottom silicon layer, and a silicon dioxide layer between the top and bottom silicon layers. A top hard mask is formed on the top silicon layer. A bottom hard mask is formed on the bottom silicon layer having an opening for a mass removal area. The bottom hard mask and bottom silicon layer are coated with a photoresist layer. The photoresist layer is patterned to provide openings in the mass removal area and in other areas. The bottom silicon layer is first partially etched away where it is not covered by the photoresist layer and bottom hard mask in the mass removal area. Next, the bottom hard mask is removed where it is not covered by the photoresist layer. A second etching away of the bottom silicon layer where it is not covered by the photoresist layer stops at the silicon dioxide layer in the mass removal area wherein a portion of the bottom silicon layer remains covering the silicon dioxide layer in all other areas. Then, the silicon dioxide layer exposed in the mass removal area is removed and the photoresist layer is stripped. A third etching away of the bottom silicon layer etches into the top silicon layer to a predetermined depth in the mass removal area and stops at the silicon dioxide layer in the other areas. The bottom hard mask is removed. A glass wafer is anodically bonded to the bottom silicon layer. A silicon wafer is temporarily bonded to the glass wafer. Finally, the top silicon layer is etched through, the top hard mask is removed, and metal is deposited to form a MEMS scanning mirror.
Also in accordance with the objectives of the invention, another method of setting a particular resonance frequency for a MEMS scanning mirror through mirror backside mass removal is achieved. A silicon-on-insulator wafer is provided comprising a top silicon layer, a bottom silicon layer, and a silicon dioxide layer between the top and bottom silicon layers. A top hard mask on the top silicon layer and a bottom hard mask are formed on the bottom silicon layer. The bottom hard mask and bottom silicon layer are coated with a photoresist layer which is patterned to provide an opening for a mass removal area. The bottom silicon layer is first etched away where it is not covered by the photoresist layer in the mass removal area, stopping at the silicon dioxide layer. Next, the silicon dioxide layer exposed in the mass removal area is removed and the photoresist layer is stripped. A second etching away of the bottom silicon layer where it is not covered by the bottom hard mask etches into the top silicon layer in the mass removal area and stops at the silicon dioxide layer in all other areas. The silicon dioxide layer and bottom hard mask are removed. A glass wafer is anodically bonded to the bottom silicon layer. A silicon wafer is temporarily bonded to the glass wafer. Finally, the top silicon layer is etched through, the top hard mask is removed, and metal is deposited to form a MEMS scanning mirror.
In the accompanying drawings forming a material part of this description, there is shown:
In the prior art, creating a sacrificial portion on the mirror has been provided as a way to change mirror mass and, in turn, to adjust resonance frequency of the MEMS scanning mirror. But this sacrificial portion is on the same layer as the spring and comb teeth. If reactive ion etching (RIE) were used here to etch the sacrificial portion, the spring and the comb teeth might also be affected. In the prior art, if the mirror mass is removed from the backside, the mass removal process is decoupled from the spring and comb teeth process. The backside mass removal can be realized by RIE, ion beam etching (IBE), or laser beam etching.
The mass removal process of the present invention can be realized mainly by deep silicon etching. The etch profile can be controlled very well in the handle silicon and also in the active silicon layer. Both silicon and silicon dioxide etching is performed from the backside, using either Si or SiO2 as a hard mask when the other material is etched. The structure release step is partially performed during the backside SiO2 etch. With the help of advanced metrology, rework could achieve an accuracy of frequency control within 1 Hz.
Two preferred process flow embodiments are presented here, as shown in
Referring now to
Next, the bottom silicon dioxide layer 16 is patterned using photoresist and RIE to form the bottom hard mask defining the backside pattern, including the mass remove area, isolation line, and pad. This is shown in
Referring now to
As shown in
A second deep silicon etch is performed from the backside of the wafer, as shown in
Next, in a first structure release step, the bottom silicon dioxide layer 16 is removed by an oxide etch, as shown in
Now, as shown in
As illustrated in
A second preferred embodiment of the present invention will be described with reference to
Referring now to
Next, the bottom silicon dioxide layer 16 is patterned using photoresist and RIE to form the bottom hard mask defining the mass remove area. This is shown in
Referring now to
Next, an oxide etch from the backside opens the hard mask 16 for the cavity, anchor, and pad area, as shown in
A second deep silicon etch is performed from the backside of the wafer, as shown in
As shown in
Next, the bottom silicon dioxide layer 16 and exposed BOX 11 are removed by an oxide etch, as shown in
As illustrated in
The present invention provides two methods for forming a MEMS scanning mirror having a particular resonance frequency. The resonance frequency can be tuned to the particular application desired. The particular resonance frequency is set by the mass removal steps of the present invention, using special patterns on the bottom of mirror. This means that the backside etch not only provides a way to control frequency, but also provides a way to make the mirror very stable during high frequency scanning. The mass is removed from the backside of the mirror so as to avoid interfering with the topside mirror structures.
Although the preferred embodiment of the present invention has been illustrated, and that form has been described in detail, it will be readily understood by those skilled in the art that various modifications may be made therein without departing from the spirit of the invention or from the scope of the appended claims.
Number | Name | Date | Kind |
---|---|---|---|
5914801 | Dhuler et al. | Jun 1999 | A |
6087747 | Dhuler et al. | Jul 2000 | A |
6201629 | McClelland et al. | Mar 2001 | B1 |
6628041 | Lee et al. | Sep 2003 | B2 |
6827866 | Novotny | Dec 2004 | B1 |
6905614 | Novotny | Jun 2005 | B1 |
6914710 | Novotny et al. | Jul 2005 | B1 |
6963679 | Novotny et al. | Nov 2005 | B1 |
7014115 | Fu | Mar 2006 | B2 |
7187488 | Fu | Mar 2007 | B2 |
7190854 | Novotny et al. | Mar 2007 | B1 |
7217587 | Fu | May 2007 | B2 |
7224097 | Obi et al. | May 2007 | B2 |
7542188 | Zhou et al. | Jun 2009 | B2 |
7605966 | Tani et al. | Oct 2009 | B2 |
7616371 | Fu | Nov 2009 | B2 |
7710627 | Yoon et al. | May 2010 | B2 |
7824945 | Chang et al. | Nov 2010 | B2 |
7872394 | Gritters et al. | Jan 2011 | B1 |
8035874 | Fu | Oct 2011 | B1 |
8107157 | Tsuboi et al. | Jan 2012 | B2 |
8353600 | Fu | Jan 2013 | B1 |
8378434 | Krylov et al. | Feb 2013 | B2 |
20010021058 | McClelland et al. | Sep 2001 | A1 |
20010022682 | McClelland et al. | Sep 2001 | A1 |
20010034938 | Behin et al. | Nov 2001 | A1 |
20020005976 | Behin et al. | Jan 2002 | A1 |
20020050744 | Bernstein et al. | May 2002 | A1 |
20020118850 | Yeh et al. | Aug 2002 | A1 |
20030007262 | Tsuboi et al. | Jan 2003 | A1 |
20040032634 | Hah et al. | Feb 2004 | A1 |
20050139678 | Helsel et al. | Jun 2005 | A1 |
20050156481 | Zhou et al. | Jul 2005 | A1 |
20050269655 | Fu | Dec 2005 | A1 |
20060166444 | Fu | Jul 2006 | A1 |
20070216986 | Huber et al. | Sep 2007 | A1 |
20080279498 | Sampsell et al. | Nov 2008 | A1 |
20090185253 | Tani et al. | Jul 2009 | A1 |
20100006958 | Krylov et al. | Jan 2010 | A1 |
20110136283 | Gritters et al. | Jun 2011 | A1 |
20110268384 | Akkaya et al. | Nov 2011 | A1 |
20120080612 | Grego et al. | Apr 2012 | A1 |
Entry |
---|
PCT Search Report—PCT/US 11/01704, Mail date—Feb. 14, 2012, Magic Technologies, Inc. |
Number | Date | Country | |
---|---|---|---|
20120085728 A1 | Apr 2012 | US |