WO2014070219A1

WO2014070219A1 - A fabry-perot interference electro-optic modulating device

Info

Publication number: WO2014070219A1
Application number: PCT/US2013/025028
Authority: WO
Inventors: Steven Miller
Original assignee: Unipixel Displays, Inc.
Priority date: 2012-10-30
Filing date: 2013-02-07
Publication date: 2014-05-08
Also published as: TW201416787A

Abstract

An optical modulating device, comprising an optical modulator that comprises a first reflective layer, a second reflective layer, and an electro-optical polymer (EOP) layer deposed between the first and second reflective layers, wherein the combination of the first reflective layer, the EOP layer, and the second reflective layer forms a Fabry-Perot cavity. The optical modulating device also comprising a voltage generator coupled to the optical modulator.

Description

A FABRY-PEROT INTERFERENCE ELECTRO-OPTIC

MODULATING DEVICE

CROSS-REFERENCE TO RELATED APPLICATION

[0001] The present application claims priority to U.S. Provisional Patent Application No. 61/720,192, filed on October 30, 2012 (Attorney Docket No. 291 1 -05100); which is hereby incorporated herein by reference.

BACKGROUND

[0002] Fabry-Perot cavities may be used in a wide range of optical devices and systems. They can be used as interferometers in spectroscopy systems and as laser cavity feedback systems, for example. The Fabry-Perot cavity is attractive for optical devices and systems due to its ability to select a wavelength for reinforcement while causing most other wavelengths to destructively interfere with one another. This finesse, or tuning capability, of the Fabry-Perot cavity may also be used as a reflective or transmissive switch for a desired wavelength.

[0003] The use of a Fabry-Perot cavity as a switch may allow the cavity to be used to modulate a light signal, which may also be used in optical communication systems. The Fabry-Perot cavity as a modulator may be implemented in any type of optical communication system that modulates a signal. Additionally, the Fabry-Perot cavity may be used as a transmission modulator by modulating a signal that passes through the cavity, or it may be used as a reflective modulator by modulating a signal being reflected by the Fabry-Perot cavity.

SUMMARY

[0004] The devices disclosed herein may in large part involve an optical modulating device, comprising an optical modulator that comprises a first reflective layer, a second reflective layer, and an electro-optical polymer (EOP) layer deposed between the first and second reflective layers, wherein the combination of the first reflective layer, the EOP layer, and the second reflective layer forms a Fabry-Perot cavity. The optical modulating device also comprises a voltage generator coupled to the optical modulator. [0005] The devices and systems may also involve a modulating retro-reflector (MRR), comprising a corner cube retro-reflector (CCR) comprising at least three sides, wherein one side of the CCR comprises a Fabry-Perot modulator, and a signal generator coupled to the CCR. The Fabry-Perot modulator comprises a first layer, a second layer and an electro-optical polymer (EOP) material, wherein the index of refraction of the EOP material is changeable by varying an applied voltage from the signal generator.

[0006] The devices and systems may alternatively involve an optical communication system, comprising a laser source, an optical detector, and an optical modulator, comprising a first layer that is conductive and reflective, a second layer that is conductive and reflective, an electro-optical polymer (EOP) deposed between the first and second layers, wherein the EOP's index of refection is altered when an electric field is applied across it. The optical communication system also comprises a signal generator coupled to the optical modulator and a communication module coupled to the signal generator.

BRIEF DESCRIPTION OF THE DRAWINGS

[0007] For a detailed description of exemplary embodiments of the invention, reference will now be made to the accompanying drawings in which:

[0008] Figure 1 illustrates an embodiment of a Fabry-Perot optical modulator;

[0009] Figure 2 illustrates a predicted device performance curve for a Fabry-Perot optical modulator;

[0010] Figure 3 illustrates a modulator side of a free space optical communication system utilizing a Fabry-Perot optical modulator; and

[0011] Figure 4 illustrates a transceiver side of a free space optical communication system.

NOTATION AND NOMENCLATURE

[0012] Certain terms are used throughout the following description and claims to refer to particular system components. As one skilled in the art will appreciate, companies may refer to a component by different names. This document does not intend to distinguish between components that differ in name but not function. In the following discussion and in the claims, the terms "including" and "comprising" are used in an open-ended fashion, and thus should be interpreted to mean "including, but not limited to... ." Also, the term "couple" or "couples" is intended to mean either an indirect or direct connection. Thus, if a first device couples to a second device, that connection may be through a direct connection, or through an indirect connection via other devices and connections.

DETAILED DESCRIPTION

[0013] The following discussion is directed to various embodiments of the disclosure. Although one or more of these embodiments may be preferred, the embodiments disclosed should not be interpreted, or otherwise used, as limiting the scope of the disclosure, including the claims. In addition, one skilled in the art will understand that the following description has broad application, and the discussion of any embodiment is meant only to be exemplary of that embodiment, and not intended to intimate that the scope of the disclosure, including the claims, is limited to that embodiment.

[0014] A Fabry-Perot cavity conventionally comprises two reflective surfaces separated by an optical path length. In a Fabry-Perot interferometer the gap enclosed by the mirrors usually comprises air and may be mechanically varied, e.g. by moving one of the mirrors with respect to the other mirror. In a Fabry-Perot etalon, the mirrors are usually held fixed, for example by means of a spacer, for which, e.g., quartz, or glass may commonly be used, with the mirrors on opposite sides of the spacer. Common gap widths for an interferometer may vary from several micrometers to several centimeters. Considerably greater gap widths are customary when the Fabry- Perot cavity is employed as a laser resonance cavity, but may also be dependent on the wavelength of the laser. For some applications, including modulators, gap widths may be on the order of one to several micrometers. The gap widths of all Fabry-Perot cavities, be they etalons or interferometers, may be dependent on the wavelength of the light being targeted for reinforcement.

[0015] Two types of mirrors may be used in producing Fabry-Perot cavities. Thin Film Stacks (TFS) made of a material that may not exhibit substantial reflectance as a single layer are combined to produce varying amounts of reflectivity, which may be used as mirrors. The index of refraction of the TFS material may determine the number and thickness of the layers to give the desired reflectivity. Secondly, mirrors comprising a single layer of a reflective material, usually metal or metal compounds, may be used. The mirrors may be plane parallel, but curved-mirror systems are known as well, notably as laser cavities and as spectrum analyzers.

[0016] Fabry-Perot cavities, which may be resonant optical cavities, have an overall reflectance dependent upon the two mirrors' reflectances, Ri and R₂, and the index of refraction of the gap material, which is disposed between the two mirrors, plus some other factors, which may be represented by the following formula:

Reflectance (R,A,0,n,h) = (R(1 -A)² + 4RAsin(5/2)²)/ ((1 -RA)² + 4RAsin(5/2)²) (Eq.

1 )

where

and is the effective reflectance of the cavity mirrors 1 and 2, with Ri representing the reflectivity of mirror 1 and R₂ representing the reflectivity of mirror 2, λ isthe target wavelength of the light in the cavity, Θ isthe angle of propagation within the cavity with respect to the surface normal, n isthe cavity's internal refractive index, h isthe physical thickness of the cavity material, and A isthe loss per pass due to absorption of the gap material. The quantity δ in the above equation isa phase shift factor and is given by 5=(4nnhcos Θ)/ λ.

[0017] The reflectance therefore has minima when δ=2ηηπ and maxima when δ=2(ηη+½)π, where m is an integer, i.e., when the sine factors are zero and one, respectively. Therefore, a Fabry-Perot cavity may be designed using equation 1 to reflect an incident light beam of a specific wavelength by the proper selection of the cavity material's index of refraction, the reflectivity values of the two mirrors, and the cavity's thickness. All other wavelengths may be trapped, or absorbed, by the gap material due to destructive interference within the cavity or multiple internal reflections leading to the absorption of the light due to the absorption characteristic of the gap material.

[0018] In general, any of the quantities R, λ, θ, n or h may serve as an adjustable parameter to tune the cavity. In accordance with various embodiments, the refractive index of the cavity gap material may be adjusted to tune the Fabry-Perot cavity. Alternatively or additionally, the thickness of the cavity, h, may also be adjusted to tune the cavity. A Fabry-Perot cavity may be tuned so that it reflects a desired wavelength and attenuates or absorbs other wavelengths. This may be used so that the Fabry- Perot may be used in an optical communication system, as a laser cavity, or in a spectrometer so that a desired wavelength is amplified or selected out of a broadband signal. Alternatively, the Fabry-Perot cavity may be tuned to a wavelength so that the cavity may be used as a switch for light of that wavelength.

[0019] The linear electro-optic effect may only occur in an anisotropic birefringent material (e.g., where the molecules have different symmetries for different spatial axes) which has at least 2 different indexes of refraction, referred to as an ordinary index and an extraordinary index. The electro-optic effect can be induced by including an anisotropic material between two electrodes of spacing, d, and applying a voltage, V, across the electrodes to generate an electric field having an electric field strength of E=V/d. The linear electro-optic effect may be a change in the index of refraction, Δη, (shown in equation 2, below) that may be proportional to the magnitude of an externally applied electric field, E, and the electro-optic coefficient, r, which depends on the molecular axis of the material.

Δη = ½^*(n³)^*r^*E = ½^*(n3)^*r^*V/d

(Eq. 2)

[0020] By combining the reflective characteristics of the Fabry-Perot cavity with a gap material displaying the electro-optical effect, a Fabry-Perot cavity may be designed to change its level of reflectivity for a given wavelength. As discussed above, the cavity's reflectivity may be a function of the gap material's index of refraction. Thus, by designing the cavity to reflect a specific wavelength using a gap material's intrinsic index of refraction, the cavity may also absorb, trap, or cause internal destructive interference for the same wavelength by changing the gap material index of refraction. The gap material's index of refection may be altered by applying a voltage across it when using a gap material that displays the linear electro-optical effect. The ability to alter the gap material's index of refraction may allow the Fabry- Perot cavity to be tuned to a different wavelength. Stated differently, the Fabry-Perot cavity may be de-tuned from the designed for wavelength. Thus, by switching an applied voltage on and off, then Fabry-Perot cavity may be switched between reflecting the wavelength and absorbing the wavelength. As such, the Fabry-Perot cavity may function as an optical switch.

[0021] Disclosed herein are a device and a system implementing a Fabry-Perot cavity as an optical modulator. The Fabry-Perot optical modulator may comprise two mirrors, one on each side of an electro-optical polymer gap material. The electro- optical polymer gap material may display the linear electro-optical effect, which may allow the gap material's index of refraction to be changed by applying an electric field across it. The Fabry-Perot optical modulator may be used in optical communication systems to modulate an impinging light beam and the modulator may be used in a reflective or transmissive system. The Fabry-Perot optical modulator may modulate a light signal by shuttering it in accordance with an applied data signal so that the shuttered light signal carries the data from the data signal. [0022] FIG. 1 illustrates an embodiment of a Fabry-Perot optical modulator 100. The optical modulator 100 comprises a first reflective layer 102, a second reflective layer 104, an electro-optical polymer (EOP) layer 106, a substrate 108, and may be coupled to a voltage generator 1 10. The first and second reflective layers may be mirrors of the Fabry-Perot optical modulator 100. The second reflective layer 104 may have a normally high reflectivity (at least higher than the reflectivity of the first reflective layer 102), e.g. a reflectivity, R₂, of around 0.98, and the second reflective layer 104 may also be conductive. The second reflective layer 104 may be mounted onto the substrate 108, or it may be a surface of the substrate 108, or it may be the surface of substrate 108 coated with a conductive and reflective material, for example gold, aluminum, or silver, but any highly reflective and conductive material may work. The substrate 108 may be at least 5 microns thick, but may be thicker depending on any external parameters required for the optical modulator 100.

[0023] The first reflective layer 102 may also be conductive but may have a lower reflectivity than the second reflective layer 104. For example, the reflectivity, of the first reflective layer 102 may be 0.7 to 0.8 in embodiments in which the reflectivity of the second reflective layer 104 is 0.9 or greater. One way to obtain this level of reflectivity is by keeping the first reflective layer 102 relatively thin, e.g. around 30 nanometers. However, the reflectivity and, conversely, the absorption, of the first reflective layer 102 may also be a function of material used to form the first reflective layer 102. The amount of absorption may also depend on the thickness of the material. In various embodiments, aluminum may provide the best optical properties due to its reflective and transmissive properties. In various other embodiments, materials such as silicon with an aluminum or gold layer may be used as the first and second reflective layers.

[0024] Both the reflective layer 102 and the reflective layer 104 may have flat surfaces and may be parallel to each other. Both layers may also serve as electrodes, which allow the formation of an electric field through EOP layer 106 when applying a voltage to the reflective layers by the voltage generator 1 10. The voltage may be any suitable voltage such as a voltage in the range from 5 to 100 volts across EOP layer 106, depending on the layer's thickness and composition.

[0025] The EOP layer 106 may have an average thickness, h, of, for example, about 5 microns due to preparation requirements involving poling of the EOP material. Poling is the process of applying a high voltage across the EOP while the temperature of the EOP is near its glass transition temperature. The EOP layer 106 may be formed of organic electro-optic polymers which may contain many nonlinear optically active molecules, i.e., chromophores. Chromophores are molecules composed of strong electron donors, strong electron acceptors, and bridge in such a way that the electron density may be polarized easily through extended conjugation in response to an applied electric field. The extended conjugation may allow the electrons to move across the bridge so they collect in one area, or side, of the molecule, thus causing it to polarize. These chromophores may be dispersed in a compatible and optically inactive (transparent) matrix such as a polymer. In such bulk material constructed from many molecularly asymmetric (dipolar) chromophores, the added need for overall noncentrosymmetry imposes the additional requirement of molecular alignment in order to achieve a finite macroscopic second-order nonlinear optical activity. This alignment can be achieved by a poling process under very high electrical field strength up to 100-200 V/micron at a glass transition temperature of the matrix polymer. The nonlinear optical property may be achieved after a successful poling process and characterized herein as EO coefficient (r33). The r33 is the tensor element that may be used to calculate the magnitude of refractive index change obtained for an applied electric field and may be expressed in units of picometers per volt (pm/V). The tensor element may be a function of the molecular axis of the material and may represent the electro-optic coefficient of the material.

[0026] The change in the index of refraction of resulting chromophore-doped EOP may be proportional to the magnitude of an externally applied electric field, as discussed above in relation to the linear electro-optical effect. Omitting the vector nature of the physical quantities, the effect of an external electric field on the index of refraction of an EOP material may be described in the linear relationship (similar to Eq. 2, above): Δη = n^{3 *} r₃₃ ^* E/2

(Eq. 3) where Δη may be the change in the index of refraction, n may be the index of refraction of the EOP layer 106, r33 may be the electro-optic coefficient, and E may be the applied electric field strength. Per equation 3, the change of the index of refraction may not only be related to r33, but also related to the refractive index of the EOP and the applied electrical field strength. A typical value for the r33 of the EOP layer 106 may be 100-200 pm/V at a wavelength of 1310 nm. The measure of index of refraction may be wavelength dependent because it represents a ratio of the velocity of light in a medium to the velocity of light in air. [0027] As discussed above, the EOP layer 106 may have an average thickness of, for example, 5 microns. Such a thickness, in light of an r33 of 100-200 pm/V, may only need an electric field of 5 V/micron in order to change the layer's index of refraction. At such an electric field, the EOP layer's 106 index of refraction may change by 0.00123 using an r33 of 100 pm/V. This change in the index of refraction of the EOP layer 106 may be enough to affect the wavelength for which the Fabry-Perot optical modulator may be tuned.

[0028] In accordance with various embodiments, the voltage generator 1 10 may be coupled to the Fabry-Perot optical modulator 100 at the first and second reflective layers. The voltage generator 1 10 may be used to apply a voltage to the Fabry-Perot optical modulator 100, and the applied voltage may alter the EOP layer's 106 index of refraction as described in reference to Eq. 2 above. By changing the refractive index of the EOP layer 106 the reflectivity of the Fabry-Perot optical modulator 100, per Eq. 1 above, may be changed. Thus, without applying a voltage, the Fabry-Perot optical modulator 100 may reflect an impinging light signal of the designed wavelength. The light signal may be reflected because the Fabry-Perot optical modulator 100 may cause the light signal to be reinforced within the cavity by setting up a standing wave at the incident light's wavelength. On the other hand, when applying a voltage, the Fabry-Perot optical modulator 100 may cause the impinging light signal to eliminate itself within the cavity through destructive interference - this may also be referred to as trapping the light or absorbing the light. Alternatively, the Fabry-Perot optical modulator 100 may be designed to be reflective when applying a voltage and absorptive without an applied voltage.

[0029] FIG. 2 illustrates a device performance curve 200 for the Fabry-Perot optical modulator 100. The device performance curve 200 illustrates the calculated reflectance of Fabry-Perot optical modulator 100 versus different index of refraction values for the EOP layer 106. As can be seen in device performance curve 200, if the EOP layer's 106 index of refraction is modulated from between about 1 .6025 to around 1 .615, the reflectivity of the EOP layer 106 may be altered from around 0.25 to around 0.98. Thus, when the EOP layer's 106 index of refection is around 1 .6025, the overall reflectivity of the Fabry-Perot optical modulator 100 may be low, which may cause it to absorb impinging light. Yet, when the EOP layer's 106 index of refraction is around 1 .615, the overall reflectivity of the Fabry-Perot optical modulator 100 may be high, which may cause it to reflect impinging light. [0030] Using the voltage generator 1 10 to switch the index of refraction of the EOP layer 106 between the above two values, may cause the Fabry-Perot modulator 100 to switch between reflection and absorption of an impinging light, which may cause the light to be modulated. If the switching of the Fabry-Perot optical modulator's 100 reflectivity is done in accordance with an applied data signal, by way of voltage generator 1 10, then an impinging light signal may be reflected as a modulated light signal. In accordance with various embodiments, the Fabry-Perot modulator 100 may be transmissive and a transmitted light signal may be modulated.

[0031] FIG. 3 illustrates a modulator side 300 of a free space optical communication system (FSOCS). The modulator side of the FSOCS 300 comprises a collection lens 304, a corner cube retro-reflector (CCR) 306, and a signal generator 310 coupled to the CCR 306. The combination of the CCR 306 and the signal generator may be referred to as a modulating retro-reflector. The CCR 306 may comprise three sides so that light incident upon it is reflected back in the direction in which the light came. For the modulator side of the FSOCS 300 to modulate light signals, one side of the CCR 306 may comprise a Fabry-Perot optical modulator, such as the Fabry-Perot optical modulator 100.

[0032] The collection lens 304 may reduce the incident beam profile down to a smaller size onto the CCR 306. The collection lens 304 may also collect a beam as it is reflected off of the CCR 306 and direct it toward the other side of the FSOCS 300, such as the transceiver side 400 described below. The collection lens 304 may also expand the reflected beam to reduce the beam's intensity so to avoid engendering any animals or humans that may cross the beams path. The combination of the collection lens 304 and the CCR 306 may reflect, or return, the reflected beam back toward the other side of the FSOCS with a reduced amount of active steering of either the modulator side 300 or a transceiver side of the FSOCS, if any at all. The lack of active steering may be due to the wide operating angle the combination of the collection lens 304, a collection lens that may be associated with the transceiver side, and the inherent characteristic of the CCR 306 for returning a beam in the direction it was received.

[0033] By covering one side of the CCR 306 with a Fabry-Perot optical modulator, for example Fabry-Perot optical modulator 100, a light beam incident onto the CCR 306 may be modulated by varying, or switching, a voltage applied to the Fabry-Perot optical modulator side of the CCR 306 by signal generator 310. By using the index of refraction switching characteristics as shown in FIG. 2, the CCR 306 may modulate an impinging light beam by reflecting a beam back for an amount of time no voltage is applied to the CCR 306 and by absorbing, or trapping, a light beam for an amount of time a voltage is applied to the CCR 306. Thus, by varying the applied voltage by a data signal using the signal generator 310, a modulated signal may be reflected by the modulator side of the FSOCS 300.

[0034] In accordance with various embodiments, the laser source associated with transceiver side of the FSOCS 300 may generate a light beam aimed at, and incident upon, the collection lens 304 - this may be represented by incident beam 302 in FIG. 3. The collection lens 304 may reduce incident beam 302 down to a smaller profile onto the CCR 306. Using a signal generator 310 attached to the CCR 306 to vary a voltage applied to the side of the CCR 306 comprising the Fabry-Perot optical modulator, the index of refraction of the EOP layer 106 may be changed, which results in the reflectivity of the CCR 306 being changed. By modulating the EOP layer's index of refraction in accordance with FIG. 2, which causes the Fabry-Perot optical modulator to switch between being reflective and being absorptive, the incident light beam 302 may be reflected and modulated by the CCR 306 - shown by modulated light beam 308 in FIG. 3. The modulated beam 308 may be collected by the collection lens 304, expanded, and directed back to the detector housed in the other side of the FSOCS.

[0035] By combining two sides of a FSOCS, optical communication may take place between two points separated by several kilometers. Additionally, the modulator, since housed away from the laser source and detector, may only require a small amount of power due to the Fabry-Perot optical modulator's 100 potential low operating voltage requirements, as discussed above. Thus, only one side of a FSOCS, the transceiver side, may require appreciable amounts of power to operate the laser source and the detector, whereas the modulator side may be low power.

[0036] Figure 4 illustrates a transceiver side 400 of a free space optical communication system. Transceiver side 400 comprises a laser source 402, a beam splitter 404, a detector 406, and a collection lens 408. The laser source 402 may generate the laser beam 412 that may propagate through the beam splitter 404 before being collected and focused by collection lens 408. The collection lens 408 may aim the laser beam 412 toward a modulator side of a FSOCS, such as the modulator side 300. The laser beam 412 may be collected by the modulator side of a FSOCS, modulated, and then sent back toward the transceiver side 400 of a FSOCS. The laser beam 412 may be similar to incident light beam 302 of FIG. 3. The modulated laser beam 410 denotes the modulated and returned laser beam from the modulator side of a FSOCS and may be similar to modulated beam 308 of FIG. 3. The modulated laser beam 410 may be collected by collection lens 408 and focused onto the beam splitter 404. The beam splitter 404 may direct a portion of the modulated beam to the detector 406 so that signal the modulated beam 410 is carrying is relayed by the FSOCS. The combination of the collection lens 304 and the collection lens 408 may allow light to be received by the both sides of a FSOCS within a range of angles (e.g., ± 25° off of normal) that may reduce or negate the need for any active beam steering for a FSOCS.

[0037] The above discussion is meant to be illustrative of the principles and various embodiments of the present invention. Numerous variations and modifications will become apparent to those skilled in the art once the above disclosure is fully appreciated. It is intended that the following claims be interpreted to embrace all such variations and modifications.

Claims

CLAIMS What is claimed is:

1 . An optical modulating device, comprising: an optical modulator, comprising: a first reflective layer; a second reflective layer; and an electro-optical polymer (EOP) layer deposed between the first and second reflective layers, wherein the combination of the first reflective layer, the EOP layer, and the second reflective layer forms a Fabry-Perot cavity; and a voltage generator coupled to the optical modulator.

2. The optical modulating device of claim 1 , wherein the reflectivity of the first layer is less than the reflectivity of the second layer.

3. The optical modulating device of claim 1 , wherein the first and second reflective layers are conductive.

4. The optical modulating device of claim 1 , wherein the EOP layer's index of refraction is changeable by applying an electric field to the optical cavity using the voltage generator.

5. The optical modulating device of claim 1 , wherein the optical modulator's reflectivity is altered when the EOP layer's index of refraction is changed.

6. The optical modulating device of claim 1 , wherein the optical modulator reflects an impinging light beam when no voltage is applied by the voltage generator and the optical modulator absorbs the impinging light beam when a voltage is applied by the voltage generator.

7. The optical modulating device of claim 1 , wherein the impinging light beam is modulated by the optical modulator by switching the voltage generator in accordance to a varying data signal.

8. A modulating retro-reflector (MRR), comprising: a corner cube retro-reflector (CCR) comprising at least three sides, wherein one side of the CCR comprises a Fabry-Perot modulator; and a signal generator coupled to the CCR; wherein the Fabry-Perot modulator comprises a first layer, a second layer and an electro-optical polymer (EOP) material, wherein the index of refraction of the EOP material is changeable by varying an applied voltage from the signal generator.

9. The MRR of claim 8, wherein the EOP material is deposed between the first and second layers.

10. The MRR of claim 8, wherein both the first layer and the second layer are reflective and conductive.

1 1 . The MRR of claim 8, wherein the reflectivity of the first layer is less than the reflectivity of the second layer.

12. The MRR of claim 8, wherein the second layer is also the side of the CCR that comprises the Fabry-Perot modulator.

13. The MRR of claim 8, wherein the signal generator is coupled to the first and second reflectors so that an electric field is produced across the EOP material when a voltage is applied.

14. The MRR of claim 8, wherein an impinging light strikes the first layer of the Fabry-Perot modulator and is reflected when no voltage is applied.

15. The MRR of claim 8, wherein an impinging light is absorbed by the Fabry-Perot modulator when a voltage is applied.

16. The MRR of claim 8, wherein an impinging light signal is modulated when the signal generator applies a varying voltage signal to the Fabry-Perot modulator.

17. An optical communication system, comprising: a laser source; an optical detector; an optical modulator, comprising: a first layer that is conductive and reflective; a second layer that is conductive and reflective; an electro-optical polymer (EOP) deposed between the first and second layers, wherein the EOP's index of refection is altered when an electric field is applied across it; a signal generator coupled to the optical modulator; and a communication module coupled to the signal generator.

18. The optical communication system of claim 17, wherein a light beam incident onto the first layer is reflected when no voltage is applied to the optical modulator by the signal generator.

19. The optical communication system of claim 17, wherein a light beam incident onto the first layer is absorbed when a voltage is applied to the optical modulator by the signal generator.

20. The optical communication system of claim 17, wherein a light beam incident onto the optical modulator is modulated when the communication module applies a data signal to the signal generator causing the signal generator to modulate a voltage applied to the optical modulator is accordance to the data signal.