Apparatus for selectively blocking WDM channels

Description

FIELD OF THE INVENTION

This invention relates to the field of wavelength division multiplex (WDM) optical communication. More particularly, this invention relates to the field of wavelength division multiplex (WDM) optical communication where there is a need to selectively block at least one WDM channel.

BACKGROUND OF THE INVENTION

In WDM (wavelength division multiplex) optical communication, multiple wavelengths of light each carry a communication signal. Each of the multiple wavelengths of light forms a WDM channel. In DWDM (dense WDM) optical communication, a subset of the WDM optical communication, the WDM channels are spaced closer together. A typical DWDM application operates at a wavelength band about 1,550 mm, has 90 channels, and has spacing of 0.4 nm between adjacent channels.

In the WDM optical communication there is a need to selectively block at least one of the WDM channels. In order to block a WDM channel, a dynamic range between a blocked WDM channel and non-blocked WDM channels must be at least 30 dB. Preferably, the dynamic range between the blocked WDM channel and the non-blocked WDM channels must be at least 40 dB. There is also a need to selectively equalize a power level of each of the non-blocked WDM channels.

What is needed is a method of selectively blocking WDM channels, which is fast, which is cost efficient, and which reduces a power level of a blocked WDM channel by at least 30 dB.

SUMMARY OF THE INVENTION

An embodiment of the present invention is an apparatus for selectively blocking WDM channels. The apparatus for selectively blocking WDM channels comprises a light modulator, a diffraction grating, and a transform lens. The light modulator comprises an array of pixels. Each pixel of the light modulator is selectively operable to direct light into a first mode and a second mode. The first mode directs the light to an output. The second mode directs the light away from the output. The diffraction grating is operable to receive the WDM channels from an input and to disperse the WDM channels into a range of angles. The transform lens couples the diffraction grating to the light modulator. The diffraction grating is operable to transform the range of angles of the WDM channels into a range of spatially distinct positions along the array of pixels of the light modulator without overlap of two of the WDM channels on an individual pixel. In operation, the light modulator directs at least one of the WDM channels into the second mode while directing a remainder of the WDM channels into the first mode.

Embodiments of the present invention can also allow equalization of the non-blocked channels by utilizing a variable reflectivity of the light modulator to partially relect and partially diffract those non-blocked WDM channels which are to be equalized to a reference level.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates the preferred selective blocking filter of the present invention.

FIG. 2 illustrates a grating light valve type device of the present invention.

FIG. 3 illustrates the grating light valve type device of the present invention in a reflection mode.

FIG. 4 illustrates the grating light valve type device of the present invention in a diffraction mode.

FIG. 5 illustrates a first alternative selective blocking filter of the present invention.

FIG. 6 illustrates an angled facet of a transceiver optical fiber of a circulator of the present invention.

FIGS. 7A and 7B illustrate a second alternative selective blocking filter of the present invention.

FIGS. 8A and 8B graphically illustrate test results from operation of the second alternative selective blocking filter of the present invention.

FIG. 9A illustrates a third alternative selective blocking filter of the present invention.

FIG. 9B illustrates the polarization diversity module included in the third alternative selective blocking filter.

FIG. 9C illustrates a side view of the grating light valve type device operating in first order retro.

DETAILED DESCRIPTION OF THE EMBODIMENTS

Embodiments of the present invention selectively block WDM (wavelength division multiplex) channels. In a WDM communication system, various wavelengths of light each carry information. The various wavelengths of light are referred to as WDM channels. The WDM channels are separated by a channel separation. For example, in a telecom C band having WDM channels from 1,527 to 1,563 nm with a channel separation of 0.4 run (or 50 GHz), 90 individual WDM channels each individually carry information. Applying the present invention to such a WDM communication system allows selective blocking of one or more of the 90 individual WDM channels.

The preferred selective blocking filter of the present invention is illustrated in FIG. 1. The preferred selective blocking filter 10 comprises a circulator 12, a first collimation lens 14, a first diffraction grating 16, a first transform lens 18, a grating light valve type device 20, and first electronics 22. The circulator 12 comprises an input optical fiber 24, a transceiver optical fiber 26, and an output optical fiber 28. The first collimation lens 14 couples the circulator 12 to the first diffraction grating 16. The first transform lens 18 couples the first diffraction grating 16 to the grating light valve type device 20. Preferably, a transform lens focal length f_t separates the first diffraction grating 16 from the first transform lens 18. Preferably, the transform lens focal length f_t separates the first transform lens 18 from the grating light valve type device 20. The first electronics 22 couple to the grating light valve type device 20.

The grating light valve type device 20 of the present invention is illustrated in FIG. 2. The grating light valve type device 20 preferably comprises elongated elements 32 suspended by first and second posts, 34 and 36, above a substrate 38. The elongated elements 32 comprise a conducting and reflecting surface 40. The substrate 38 comprises a conductor 42. In operation, the grating light valve type device 20 operates to produce modulated light selected from a reflection mode and a diffraction mode.

A cross-section of the grating light valve type device 20 of the present invention is further illustrated in FIGS. 3 and 4. The grating light valve type device 20 comprises the elongated elements 32 suspended above the substrate 38. The elongated elements comprise the conducting and reflecting surface 40 and a resilient material 44. The substrate 38 comprises the conductor 42.

FIG. 3 depicts the grating light valve type device 20 in the reflection mode. In the reflection mode, the conducting and reflecting surfaces 40 of the elongated elements 32 form a plane so that incident light I reflects from the elongated elements 32 to produce reflected light R.

FIG. 4 depicts the grating light valve type device 20 in the diffraction mode. In the diffraction mode, an electrical bias causes alternate ones of the elongated elements 32 to move toward the substrate 38. The electrical bias is applied between the reflecting and conducting surfaces 40 of the alternate ones of the elongated elements 32 and the conductor 42. The electrical bias results in a height difference of a quarter wavelength λ/4 of the incident light I between the alternate ones of the elongated elements 32 and non-biased ones of the elongated elements 32. The height difference of the quarter wavelength λ/4 produces diffracted light including plus one and minus one diffraction orders, D₊₁ and D₋₁.

FIGS. 3 and 4 depict the grating light valve type device 20 in the reflection and diffraction modes, respectively. For a deflection of the alternate ones of the elongated elements 32 of less than a quarter wavelength λ/4, the incident light I both reflects and diffracts producing the reflected light R and the diffracted light including the plus one and minus one diffraction orders, D₊₁ and D₋₁. In other words, by deflecting the alternate ones of the elongated elements less than the quarter wavelength λ/4, the grating light valve type device 20 produces a variable reflectivity.

It will be readily apparent to one skilled in the art that the conducting and reflecting surface 40 can be replaced by a multilayer dielectric reflector and a conducting element where the conducting element is buried within each of the elongated elements 32 or within just the alternate ones of the elongated elements 32.

While FIGS. 2, 3, and 4 depict the grating light valve type device 20 having six of the elongated elements 32, the grating light valve type device 20 preferably includes more of the elongated elements 32. By providing more of the elongated elements 32, the elongated elements 32 are able to function as groups, which are referred to as pixels.

It will be readily apparent to one skilled in the art that the term “pixel” is used here in the context of an element of a light modulator rather than its more specific definition of a picture element of a display.

In operation of the preferred selective blocking filter 10 (FIG. 1), an input signal 46 comprising the WDM channels enters the input optical fiber 24 of the circulator 12 and exits the transceiver optical fiber 26. The first collimation lens 14 collimates the WDM channels. The first diffraction grating 16 disperses the WDM channels into a range of angles. The first transform lens 18 transforms the range of angles of the WDM channels into a range of spatially distinct positions along the grating light valve type device 20, which comprises an array of pixels. No two WDM channels on the grating light valve type device 20 overlap.

The grating light valve type device 20, driven by the first electronics 22, directs at least one of the WDM channels into the diffraction mode while directing a remainder of the WDM channels into the reflection mode. The reflection mode returns the remainder of the WDM channels along a reverse path to the transceiver optical fiber 26 of the circulator 12. The diffraction mode causes the at least one WDM channel to not follow the reverse path to the circulator 12. The reverse path comprises the first transform lens 18, the first diffraction grating 16, and the first collimation lens 14. The circulator 12 directs the remainder of the WDM channels out of the output optical fiber 28 of the circulator as an output signal 48.

In an alternative mode of operation, the function of the reflection mode and the diffraction mode can be exchanged. For example, the diffraction mode returns the remainder of the WDM channels along the reverse path to the transceiver optical fiber 26 of the circulator 12, and the reflection mode causes the at least one WDM channel to not follow the reverse path to the circulator 12.

In order to successfully achieve WDM channel blocking, a dynamic range between the at least one WDM channel and the remainder of the WDM channels at the output optical fiber 28 must be at least 30 dB. Preferably, the dynamic range between the at least one WDM channel and the remainder of the WDM channels at the output optical fiber 28 is at least 40 dB.

The dynamic range is met by first and second aspects of the present invention. The first aspect is not overlapping any two WDM channels on an individual pixel of the grating light valve type device 20 by spatially separating the WDM channels at distinct positions along the grating light valve type device 20. This is accomplished by using high resolution optical components for the first collimation lens 14, the first diffraction grating 16, and the first transform lens 18.

The second aspect is a modulator dynamic range provided by the grating light valve type device 20. In the reflection mode, the grating light valve type device 10 reflects the incident light I to form the reflected light R (FIG. 3). In the diffraction mode, the grating light valve type device 10 diffracts the incident light I to form the diffracted light including the plus one and minus one diffraction orders, D₊₁ and D₋₁ (FIG. 4). In the diffraction mode, however, a small amount of light is directed into the reflected mode. The modulator dynamic range is a ratio of a power level of the reflected light in the reflection mode to a power level of the small amount of reflected light in the diffraction mode. The grating light valve type device 20 has a modulator dynamic range that is at least 30 dB. By careful design and fabrication, including maintaining narrow gaps between the adjacent ones of the elongated elements 32 of the grating light valve type device 20, the grating light valve type device 20 provides a modulator dynamic range of 40 dB.

In an alternative operation of the preferred selective blocking filter 10, the remainder of the WDM channels are equalized to a reference level in addition to blocking the at least one WDM channel. The alternative operation utilizes the variable reflectivity capability of grating light valve type device 20 to partially reflect and partially diffract those WDM channels of the remainder of the WDM channels which must be reduced in power in order to equalize the remainder of the WDM channels to the reference level.

A first alternative selective blocking filter of the present invention is illustrated in FIG. 5. The first alternative selective blocking filter 50 comprises the circulator 12, a second collimation lens 52, a second diffraction grating 54, a mirror 56, a second transform lens 58, the grating light valve type device 20, and second electronics 60. The second collimation lens 52 couples the circulator 12 to the diffraction grating 54. The diffraction grating 54 couples to the mirror 56. The second transform lens 58 couples the diffraction grating 54 to the grating light valve type device 20. Preferably, the transform lens 58 is positioned so that a virtual pivot 61 of the diffraction grating 54 is located at a transform lens focal length f_t. Preferably, the transform lens 58 is also positioned so that the grating light valve type device 20 is located at the transform lens focal length f_t. The second electronics 60 couple to the grating light valve type device 20.

In operation of the first alternative selective blocking filter 50, the circulator 12 directs the WDM channels to the collimation lens 52, which collimates the WDM channels onto the diffraction grating 54. The diffraction grating 54 disperses the WDM channels into a first range of angles. The mirror 56 reflects the first range of angles of the WDM channels back to the diffraction grating 54, which further disperses the WDM channels into a second range of angles. The transform lens 58 transforms the second range of angles of the WDM channels into spatially distinct positions along the grating light valve type device 20.

The grating light valve type device 20, driven by the second electronics 60, directs at least one of the WDM channels into the diffraction mode while directing a remainder of the WDM channels into the reflection mode. The reflection mode returns the remainder of the WDM channels along a second reverse path to the transceiver optical fiber 26 of the circulator 12. The diffraction mode causes the at least one WDM channel to not follow the second reverse path to the circulator 12. The second reverse path comprises the second transform lens 58, the second diffraction grating 54, the mirror 56, and the second collimation lens 52.

Comparing the first alternative selective blocking filter 50 to the preferred selective blocking filter 10 it is seen that the first alternative selective blocking filter 50 operates similarly to the preferred selective blocking filter 10 with first and second exceptions. The first exception is that the mirror 56 of the first alternative selective blocking filter causes a double pass of the WDM channels on the diffraction grating 54 before the WDM channels reach the grating light valve type device 20. The second exception is that the mirror 56 causes the double pass of the remainder of the WDM channels on the diffraction grating 54 along the second reverse path from the grating light valve type device 20 to the circulator 12. The double pass enhances the spatially distinct positions of the WDM channels along the grating light valve type device 20. This allows for a smaller physical layout for the first alternative selective blocking filter 50 over the preferred selective blocking filter 10. However, the first alternative selective blocking filter 50 incurs a slight loss in efficiency over the preferred selective blocking filter 10 due to the two reflections from the mirror 56 and due to the double pass of the second diffraction grating 54.

A fiber end of the transceiver optical fiber 26 of the circulator 12 is further illustrated in FIG. 6. The fiber end 62 of the transceiver optical fiber 26 preferably includes an angled facet having an angle 64 from a cross-cut of the transceiver optical fiber 26. The angle 64 reduces back reflection in the first alternative selective blocking filter 50, which enhances performance of the first alternative selective blocking filter 50. Preferably, the angle 64 is 8°, which provides a 3.6° beam deviation. Alternatively, the angle 64 is larger or smaller. Further alternatively, the angle 64 is zero.

A second alternative selective blocking filter of the present invention is illustrated in FIGS. 7A and 7B. The second alternative selective blocking filter 70 comprises the circulator 12, a third collimation lens 72, a third diffraction grating 74, a third transform lens 76, the grating light valve type device 20, a quarter wave plate 78, a retro lens 80, a retro mirror 82, and third electronics 84. The third collimation lens 72 couples the circulator 12 to the third diffraction grating 74. The third transform lens 76 couples the third diffraction grating 74 to the grating light valve type device 20. The third transform lens 76 also couples the grating light valve type device 20 the quarter wave plate 78. The retro lens 80 couples the quarter wave plate 78 to the retro mirror 82. The third electronics 84 couple to the grating light valve type device 20.

FIGS. 7A and 7B depict a plan view of the second alternative selective blocking filter 70 of the present invention. FIG. 7A depicts a first ray trace from the circulator 12 to the grating light valve type device 20. FIG. 7B depicts a second ray trace from the grating light valve type device 20 to the retro mirror 82.

It will be readily apparent to one skilled in the art that the third diffraction grating 74 lies in the first ray trace (FIG. 7A) and not the second ray trace (FIG. 7B).

In operation of the second alternative selective blocking filter 70, the WDM channels couple from the circulator 12 to the grating light valve type device 20 via the third collimation lens 72, the third diffraction grating 74, and the third transform lens 76 as depicted by the first ray trace in FIG. 7A. The grating light valve type device 20, driven by the third electronics 84, directs at least one of the WDM channels into the diffraction mode while directing the remainder of the WDM channels into the reflection mode. The remainder of the WDM channels are directed to the retro mirror 82 via the third transform lens 76, the quarter wave plate 78, and the retro lens 80 as depicted by the second ray trace in FIG. 7B. The retro mirror 82 reflects the remainder of the WDM channels back to grating light valve type device 20 via the retro lens 80, the quarter wave plate 78, and the third transform lens 76. The grating light valve type device 20 then directs the remainder of the WDM channels back to the circulator 12 via the third transform lens 76, the diffraction grating 74, and the third collimation lens 72.

The second alternative selective blocking filter 70 provides a double pass of the grating light valve type device 20. Because of the double pass of the grating light valve type device 20, the second alternative selective blocking filter 70 exhibits an ultrahigh attenuation of a blocked WDM channel.

Since the remainder of the WDM channels pass through the quarter wave plate 78 twice, the quarter wave plate 78 provides an orthogonal rotation of a polarization of the remainder of the WDM channels. This feature provides a mechanism for compensating for a polarization dependent loss in the second alternative selective blocking filter 70. By orienting an optic axis of the quarter wave plate 78 at 45° to the polarization that exhibits a worst polarization loss, the worst polarization loss is reduced by half.

Thus, advantages of the second alternative selective blocking filter 70 are that it exhibits the ultrahigh attenuation of the blocked WDM channel and it compensates for polarization dependent loss. A disadvantage of the second alternative selective blocking filter 70 is that it is less efficient due to the reflection from the retro mirror 82 and due to the double pass of the grating light valve type device 20.

FIGS. 8A and 8B graphically illustrate test results from operation of the second alternative selective blocking filter 70 of the present invention. FIG. 8A graphically depicts the test results for a control test. In the control test, eight WDM channels on a channel spacing of 0.4 nm were passed through the second alternative selective blocking filter 70. In the control test, none of the eight WDM channels were blocked. FIG. 8B graphically depicts the test results for a blocking test. In the blocking test, a single WDM channel at 1547.72 run was blocked while seven remaining WDM channels were transmitted. In the blocking test, the single WDM channel exhibited a power reduction of 38 dB.

A third alternative selective blocking filter of the present invention is illustrated in FIG. 9A. The third alternative selective blocking filter 90 comprises the circulator 12, a polarization diversity (PD) module 92, a fourth diffraction grating 94, a fourth transform lens 96, the grating light valve type device 20, and fourth electronics 98. The PD module 92 couples the circulator 12 to the fourth diffraction grating 94. The fourth transform lens 96 couples the fourth diffraction grating 94 to the grating light valve type device 20. Preferably, a transform lens focal length ft separates the fourth diffraction grating 94 from the fourth transform lens 96. Preferably, the transform lens focal length f_t separates the fourth transform lens 96 from the grating light valve type device 20. The fourth electronics 98 couple to the grating light valve type device 20. The grating light valve type device 20 is positioned perpendicular to the optical axis.

FIG. 9B further illustrates the PD module 92. The PD module 92 comprises a fourth collimation lens 100, a polarization splitter 102 and a half-wave plate 104. The fourth collimation lens 100 couples the optical fiber 26 of the circulator 12 (FIG. 9A) to the polarization splitter 102. The half-wave plate 104 couples an optical path from the polarization splitter 102 to the fourth diffraction grating 94.

In operation of the third alternative selective blocking filter 90, the circulator 12 directs the WDM channels to the PD module 92. The WDM channels are received by the PD module 92 as diverging light beams from the optical fiber 26. The diverging light is received by the fourth collimation lens 100 and directed as collimated light to the polarization splitter 102. The polarization splitter 102 is preferably a crystal capable of splitting an input light beam into two light beams with orthogonal polarization states to each other. The polarization splitter 102 receives the collimated light from the fourth collimation lens 100 and splits the collimated light into a first split light 101 and a second split light 103. The first split light 101 and the second split light 103 are orthogonal to each other. Preferably, the first split light 101 is polarized perpendicular to the page of the FIG. 9B, and the second split light 103 is polarized parallel to the page of the FIG. 9B. The polarization of the first split light 101 is directed along an upper optical path and the second split light is directed along a lower optical path, as illustrated in FIG. 9B. The lower optical path is coupled to the half-wave plate 104 such that the half-wave plate 104 receives the second split light 103 from the polarization splitter 102. The half-wave plate 104 provides an orthogonal rotation of a polarization of the second split light 103. In this manner, the first split light 101 and the second split light 103 exit the PD module 92 with the same polarization.

The first split light 101 and the second split light 103 are coupled to the grating light valve type device 20 via the diffraction grating 94 and the fourth transform lens 96 as depicted by the optical path illustrated in FIG. 9A. Although two optical paths are illustrated leaving the PD module 92 in FIG. 9B, only one optical path is illustrated leaving the PD module 92 in FIG. 9A. This is because FIG. 9A shows a top down view of the PD module 92 relative to the view illustrated in FIG. 9B. As such, the two beams leaving the PD module 92 in FIG. 9B are stacked vertically, as viewed in FIG. 9A, and only one beam is shown. The first split light 101 and the second split light 103 in FIG. 9B, viewed as the single light beam in FIG. 9A, propagates from the diffractive grating 94 to the fourth transform lens 96 off-axis to the optical axis, and arrives off-center at the fourth transform lens 96. The beams are refracted by the transform lens 96 and directed onto the grating light valve type device 20 at an angle approximately one-half the first order diffraction angle.

The grating light valve type device 20, driven by the fourth electronics 98, directs at least one of the WDM channels into the diffraction mode while directing a remainder of the WDM channels into the reflection mode. Preferably, the third alternative selective blocking filter 90 uses first order retro operation of the grating light valve type device 20. FIG. 9C illustrates a side view of the grating light valve type device 20 operating in first order retro. As previously described in relation to the preferred, first alternative and second alternative selective blocking filters 10, 50, 70, an incident light impinges normal to the grating light valve type device 20 and first order diffracted light is diffracted at a first order diffraction angle θ₁. In the third alternative selective blocking filter 90, incident light impinges the grating light valve type device 20 off-axis. Preferably, the incident light impinges the grating light valve type device 20 at an angle of about θ₁/2. In first order retro operation, reflected light is reflected off-axis while the plus first order diffracted light is diffracted at an angle of about θ₁/2. In other words, the plus first order diffracted light is diffracted at the same angle as the incident light impinging the grating light valve type device 20. In this third alternative embodiment, the incident light comprises the first split light 101 along the upper optical path and the second split light 103 along the lower optical path. In reference to FIG. 9C, the first split light 101 angles toward the grating light valve type device 20 from a position above the plane of FIG. 9C and in the plane of the incident light IN. Similarly, the second split light 103 angles toward the grating light valve type device 20 from a position below the plane of FIG. 9C and in the plane of the incident light IN. Preferably, the upper optical path and the lower optical path form mirror images of each other about the plane of the grating light valve type device 20 in FIG. 9C.

First split light 101 impinging the grating light valve type device 20 while in the diffraction mode is directed along a reverse path that comprises the lower optical path. In other words, the first split light 101 is directed to the grating light valve type device 20 along the upper optical path and, if the grating light valve type device 20 is in the diffraction mode, then the first split light 101 is directed away from the grating light valve type device 20 along the lower optical path. Similarly, second split light 103 impinging the grating light valve type device 20 while in the diffraction mode is directed along a reverse path that comprises the upper optical path. The reverse path along the upper optical path comprises the fourth transform lens 96, the fourth diffraction grating 94, the polarization splitter 102 and the fourth collimation lens 100. The reverse path along the lower optical path comprises the fourth transform lens 96, the fourth diffraction grating 94, the half-wave plate 104, the polarization splitter 102 and the fourth collimation lens 100. Once the second split light 103 returns through the half-wave plate 104, the first and second split light 101, 103 are orthogonal to each other. The polarization splitter 102 then recombines the first and second split light 101, 103 into an output signal. The output signal is directed to the optical fiber 26 via the fourth collimation lens 100.

The primary purpose of the polarization diversity module 92 is to suppress polarization dependent loss (PDL). Polarization diversity also enables the use of a highly dispersive grating and a fine pitch grating light valve type device, which both allow for a compact optics design. The PD module 92 can be fabricated reliably and economically.

In an alternative operation of the alternative selective blocking filters 50, 70 and 90, the remainder of the WDM channels are equalized to a reference level in addition to blocking the at least one WDM channel. The alternative operation utilizes the variable reflectivity capability of grating light valve type device 20 to partially reflect and partially diffract those WDM channels of the remainder of the WDM channels which must be reduced in power in order to equalize the remainder of the WDM channels to the reference level.

It will be readily apparent to one skilled in the art that other various modifications may be made to the embodiments without departing from the spirit and scope of the invention as defined by the appended claims.