Optical: systems and elements – Optical modulator – Light wave temporal modulation
Reexamination Certificate
2001-02-20
2003-11-04
Mai, Huy (Department: 2873)
Optical: systems and elements
Optical modulator
Light wave temporal modulation
C359S291000, C359S248000, C359S260000
Reexamination Certificate
active
06643052
ABSTRACT:
FIELD OF THE INVENTION
The present invention pertains generally to optical communications, and more particularly to a micro-mechanical optical modulator.
BACKGROUND OF THE INVENTION
FIG. 1
 depicts passive optical network 
100
. Network 
100
 includes central office or head-end terminal 
102
, splitter 
110
, wavelength routing device 
112
 and a plurality of network units 
114
i
, i=1−n, interrelated as shown.
Central office 
102
 includes transmitter 
104
 and receiver 
118
. Transmitter 
104
 incorporates active optical source 
106
, such as a multi-frequency laser or light-emitting diode. Transmitter 
104
 generates optical signal 
108
, which is a wavelength division multiplexed (“WDM”) signal. WDM signals comprise multiple independent data channels, each of which is assigned to a distinct optical wavelength. Central office 
102
 sends information over WDM optical signal 
108
 to the plurality of network units 
114
1
-
114
n
, which each receive information over one of the distinct wavelengths.
Wavelength routing device 
112
 de-multiplexes WDM signal 
108
 into its constituent spectral components (optical wavelengths) 
108
i
, i=1−n, such that the spectral components 
108
i 
are spatially separated from one another. Each spatially-separated spectral component 
108
i 
is then routed, over waveguides 
113
i
, i=1−n, to the appropriate network unit 
114
i 
as a function of wavelength. In some embodiments, the waveguides are optical fibers.
With reference to 
FIG. 2
, waveguide 
109
i 
delivers spectral component 
108
i 
to splitter 
220
 in network unit 
114
i
. Splitter 
220
 routes a first portion 
222
 of the power of spectral component 
108
i 
to receiver 
226
, and a second portion 
224
 to transmitter 
228
.
Information is advantageously sent in packets to network unit 
114
i 
via spectral component 
108
i
. The packets contain information (ie., television programming, incoming e-mail, etc.) for processing as well as continuous wave (“CW”) light or “optical chalkboard” which can be modulated with information. First portion 
222
 of spectral component 
108
i 
is converted to an electrical signal that is representative, in part, of the information contained in the packet. The electrical signal is then routed to processing electronics, not shown. Optical modulator 
230
 in transmitter 
228
 modulates information on the CW light that is contained in second portion 
224
, generating modulated (ie., information-carrying) spectral component 
116
i
. The information modulated onto the CW light can be, for example, phone message 
232
 or information 
234
 destined for the Internet.
Modulated spectral components 
116
i
, i=1−n, returned from network units 
114
1
-
114
n
, are multiplexed by wavelength routing device 
112
 into WDM signal 
116
. Splitter 
110
 routes signal 
116
 to receiver 
118
 in central office 
102
.
Optical modulator 
230
 that is used in network 
100
 can be a micro-mechanical optical modulator. This type of modulator typically uses optical interference principles to vary the signal strength of an optical signal (e.g., a carrier signal, such as the CW light of second portion 
224
 of spectral component 
108
i
). One well-known implementation of such a modulator is depicted in FIG.
3
.
Modulator 
230
 depicted in 
FIG. 3
 incorporates a movable mirror, realized as movable layer or membrane 
344
 that is supported by supports 
346
 above fixed multi-layer mirror 
342
. The fixed multi-layer mirror is disposed on substrate 
340
. Membrane 
344
 forms a Fabry-Perot cavity, well known in the art, with underlying fixed mirror 
342
. Membrane 
344
 and fixed mirror 
342
 are electrically connected to controlled voltage source 
350
.
In operation, controlled voltage source 
350
 applies a voltage across membrane 
344
 and fixed mirror 
342
 thereby generating an electrostatic force. This force draws membrane 
344
 toward fixed mirror 
342
 along vector 
452
, as depicted in FIG. 
4
. When the applied voltage is withdrawn, membrane 
344
 returns to the quiescent or unactuated position depicted in FIG. 
3
.
As membrane 
344
 moves toward fixed mirror 
342
, the size of the Fabry-Perot cavity (i.e., the size of gap 
448
 between membrane 
344
 and fixed mirror 
342
) changes. This change is accompanied by a change in the reflectivity of modulator 
230
. The optical interference principle that governs this behavior is described with reference to FIG. 
5
.
In a typical prior art modulator, membrane 
344
 has an optical thickness that is an odd integer multiple of one-quarter of the operating wavelength (“&lgr;/4”) of the modulator. Fixed multi-layer mirror 
342
 consists of anti-reflection layer 
554
 and coating layer 
556
 that each have an optical thickness that is an odd integer multiple of &lgr;/4. Membrane 
344
 and coating layer 
556
 have a refractive index that is equal to the refractive index of substrate 
340
. Anti-reflection layer 
554
 has a refractive index that is about equal to the square root of the refractive index of the substrate 
340
. See, Marxer et al., “MHz Opto-Mechanical Modulator,” Transducers '95—Eurosensors IX, The 8
th 
International Conference on Solid-State Sensors and Actuators, and Eurosensors IX, Stockholm, Sweden, Jun. 25-29, 1995, pp. 289-292.
In a modulator that is configured as described above, modulator reflectivity is at a high value (i.e., a relative maxima) when the size of gap 
448
 is an odd integer multiple of &lgr;/4. This configuration generates a constructive interference condition since the round trip distance of the optical signal from membrane 
344
, across gap 
448
, over coating layer 
556
 and back again is an integer multiple of &lgr;. That is, the optical signal is in-phase.
Conversely, modulator reflectivity is reduced to zero (i.e., a relative minima) when the size of gap 
448
 is zero or an even integer multiple of &lgr;/4. This configuration generates a destructive interference condition since the round trip distance of the optical signal is an integer multiple of 3&lgr;/2-180 degrees out of phase.
FIGS. 6 and 7
 depict the performance of micro-mechanical modulator 
230
 having the layer arrangement and layer characteristics shown in FIG. 
5
 and that is designed for a wavelength, &lgr;, of 1570 nanometers.
FIG. 6
 depicts reflectivity as a function of wavelength for modulator 
230
 wherein membrane 
344
 is silicon and a substrate 
340
 is silicon. Plot 
658
 shows the maximum reflectivity condition wherein the size of gap 
448
 is an odd integer multiple of &lgr;/4—in this case, 3&lgr;/4. For this particular configuration, maximum reflectivity is shown to be about 97 percent. Plot 
660
 shows the minimum reflectivity condition wherein the size of gap 
448
 is an even integer multiple of &lgr;/4—in this case, 2&lgr;/4. For this particular configuration, minimum reflectivity is zero at the design wavelength of 1570 nanometers.
FIG. 7
 depicts reflectivity as a function of wavelength for modulator 
230
 wherein membrane 
344
 is silicon and substrate 
340
 is germanium. Plot 
762
 shows the maximum reflectivity condition wherein the size of gap 
448
 is an odd integer multiple of &lgr;/4, which, again, is 3&lgr;/4. For this configuration, maximum reflectivity is, as before, about 97 percent. Plot 
764
 shows the minimum reflectivity condition wherein the size of gap 
448
 is an even integer multiple of &lgr;/4, here, 2&lgr;/4. Minimum reflectivity is zero at the design wavelength of 1570 nanometers.
FIGS. 6 and 7
 demonstrate that silicon and germanium can be used interchangeably as the substrate with substantially no impact on modulator performance. 
FIGS. 6 and 7
 also illustrate a shortcoming of this particular modulator arrangement. Specifically, while insertion loss is minimized for the modulator configuration described above, the operating bandwidth is relatively narrow. That is, minimum reflectivity rises relatively rapidly with deviations from the design wavelength (e.g., 1570 nanometers) so that contrast (ie., the ratio of the maximum reflect
Aralight, Inc.
DeMont & Breyer LLC
Mai Huy
Tra Tuyen
LandOfFree
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