Method and apparatus for an improved micromechanical modulator

• US 5,751,469 A
• Filed: 02/01/1996
• Issued: 05/12/1998
• Est. Priority Date: 02/01/1996
• Status: Expired due to Term

• Current Assignee: Avago Technologies General IP PTE Limited (Broadcom, Inc.)
• Original Assignee: Lucent Technologies, Inc. (Nokia Corporation)
• Inventors: Yurke, Bernard, Walker, James A., Greywall, Dennis Stanley, Arney, Susanne C.
• Primary Examiner(s): Epps, Georgia Y.
• Assistant Examiner(s): Bey, Dawn-Marie
• Application Number:
  US08/565,453
• Time in Patent Office: 831 Days
• Field of Search: 359/290, 359/291, 359/247, 359/248
• US Class Current: 359/291
• CPC Class Codes: G02B 26/001 based on interference in an adjustable optical cavity interference filters G02B5/28; devices or arrangements using multiple reflections in spectrometry or monochromators G01J3/26
• CPC Class Codes: G02B 26/02 for controlling the intensity of light G02B26/004 takes precedence

Abstract

An improved modulator and methods for making the modulator are disclosed. A membrane, preferably circular in shape, is formed over a region of a substrate in such a way that a gap results between the membrane and substrate forming a modulator cavity. The membrane forms a continuous surface over the cavity. In particular, the membrane is not supported by discrete support arms, but rather extends beyond the modulator cavity. Preferably, holes are formed in the membrane to aid in damping its motion and to allow access to underlying layers during modulator formation. According to the method, the modulator is formed by forming a means for creating a gap between the substrate and the membrane, forming a membrane, forming a lateral conduit to aid in removing the means for creating the gap and, finally, by removing the means for creating the gap.

Claims

1. A monolithic micromechanical modulator for modulating an optical signal comprising:

a substrate characterized by a first refractive index; and

a membrane for receiving an optical signal, wherein, the membrane has at least a first layer of material having a second refractive index that is approximately equal to the square root of the first refractive index of the substrate;

wherein,

the membrane is supported over a first region of the substrate, the first region having a perimeter defining a modulator cavity, wherein the membrane overlaps a substantial portion of the perimeter of the modulator cavity, and further wherein the substrate and membrane are monolithically integrated.

2. The modulator of claim 1 wherein the membrane is circular in shape.

3. The modulator of claim 1 wherein the membrane further comprises a plurality of holes physically adapted to damp vibration.

10. The modulator of claim 1 further comprising a conductive layer disposed on the membrane.

11. The modulator of claim 10 wherein the conductive layer is formed of a material selected from the group consisting of aluminum, gold, indium tin oxide, chromium/gold, titanium/gold, amorphous silicon, polycrystalline silicon and silicides.

4. A monolithic micromechanical modulator for modulating an optical signal comprising:

a substrate; and

a membrane for receiving an optical signal, the membrane having a plurality of holes physically adapted to damp vibration;

wherein,

the membrane is supported over a first region of the substrate, the first region having a perimeter defining a modulator cavity, wherein the membrane overlaps a substantial portion of the perimeter of the modulator cavity, and wherein the substrate and membrane are monolithically integrated, and further wherein the holes are spaced from each other and have a diameter such that the quality factor of the modulator ranges from about 0.7 to about 0.8.

5. The modulator of claim 4 wherein the modulator cavity is filled with gas and the holes are spaced from each other according to the expression d=2 (Ph²)/(12π

μ

_eff f)!⁰.5, where P is the pressure of the gas, h is the size of the gap between the membrane and the substrate, f is the natural resonant frequency of the micromechanical modulator and μ

_eff is effective gas viscosity, wherein, the effective gas viscosity is given by μ

_eff =μ

/{1+ 6(2-σ

)λ

/σ

h!}, where ν

is the accommodation coefficient and λ

is the mean-free-path of the gas.

6. The modulator of claim 4 wherein the holes have a diameter that is in the range of about two to about four times the size of the gap between the membrane and the substrate, and further wherein the diameter of the holes is a maximum of about one-third of the spacing between holes.

7. The modulator of claim 4 wherein the holes have a diameter in the range of about 2 microns to about 5 microns and are spaced from the nearest hole by about 10 to about 30 microns.

8. The modulator of claim 4 wherein the plurality of holes are located outside of the perimeter of a centrally located region of the membrane, which region defines an optical window for receiving the optical signal.

9. The modulator of claim 8 wherein the optical window ranges in diameter from about 25 to about 60 microns.

12. The modulator of claim 4 wherein the membrane is circular in shape.