Comb wavelength division multiplexer

Information

  • Patent Grant
  • 6608719
  • Patent Number
    6,608,719
  • Date Filed
    Thursday, October 26, 2000
    24 years ago
  • Date Issued
    Tuesday, August 19, 2003
    21 years ago
Abstract
The invention discloses a comb wavelength division multiplexer, comprising: an input device at input side, a polarization splitter, a λ/2 phase delay wave plate; a birefringent crystal filter; and a reflective parallel light polarization splitter for reflecting an incident light beam from the birefringent crystal filter into the birefringent crystal filter again, and passing the reflected light beam through the λ/2 phase delay wave plate and the polarization splitter to an output side, so that the input side and the output side are a same side. The invention uses only one-stage filter to obtain a two-stage filtering effect. The channel isolation factor is improved and the size of the apparatus is reduced (FIG. 2).
Description




FIELD OF THE INVENTION




The invention generally relates to optical communication systems) and more particularly, to a Comb Wavelength Division Multiplexer for optical communications.




BACKGROUND OF THE INVENTION




As optical telecommunication technology develops, information transmitted through optical fiber expands, and the full optical network grows, higher requirements are set for technologies like DWDM, optical passive devices. At present time, DWDM is implemented with grating, light waveguide, interference filter, birefringent filter and the like, but since density of channel are getting denser and denser, a better device is needed to multiplex or demultiplex signal. For example, DWDM may use the wavelength division device with birefringent crystal filter. Current design adopts one-stage filter to reduce the size of the device, but channel separation is poor. However, if two birefringent crystal filter element groups are applied to improve performance, the construction of two-stage filter is very complicated and the cost is expensive.




The invention overcomes above-mentioned problems with a new wavelength division device. A purpose of the invention is to obtain a two-stage filter effect with only one group of birefringent filters by light reflection The device has a reduced size and a better channel separation.




According to one aspect of the invention, a reflective parallel light polarization splitter


6


of the comb wavelength division multiplexer comprises a polarization splitter


6


-


1


and a right-angle prism


6


-


2


, a slant side of the right-angle prism is parallel to a surface of the polarization splitter.




According to another aspect of the invention, a reflective parallel light polarization splitter


6


of the comb wavelength division multiplexer comprises a λ/2 phase delay wave plate


6


-


3


,


6


-


4


disposed symmetrically in front of a polarization splitter


6


-


1


, a λ/4 phase delay wave plate


6


-


5


, and a flat mirror


6


-


2


.




One feature of the above-mentioned comb wavelength division multiplexer is an I/O device comprising a three-core collimator and trapezoid prism, or comprising a three-collimator array.




Another feature of the above-mentioned comb wavelength division multiplexer is that a PMD compensator


3


be disposed between the polarization splitter


2


and the λ/4 phase delay wave plate device.




One advantage of the invention is duplicative use of a birefringent crystal filter element group by reflection to attain a dual-stage filtering effect, the channel isolation degree is greater than one-stage filter, the number of elements is lesser and package size is smaller. The second advantage is that the construction is independent on the polarization of input light. The third advantage is that the construction provides PMD compensation and eliminate PMD effect of device on the system. A device of wavelength division multiplexer of the invention can couple DWDM signals of odd channel and even channel into different fibers, so that the channel spacing is doubled and the signals are demultiplexed. The device can also couple signals of two channels into one fiber to realize multiplexing. If changing the birefringent filter in the device, we may also obtain devices like optical attenuator, optical modulator and optical 1×2 switcher with high isolation degree.




SUMMARY OF THE INVENTION




The invention provides a comb wavelength division multiplexer, comprising: an input device at input side; a polarization splitter; a λ/2 phase delay wave plate; a birefringent crystal filter; and a reflective parallel light polarization splitter for reflecting an incident light beam from the birefringent crystal filter into the birefringent crystal filter again, and passing the reflected light beam through the λ/2 phase delay wave plate and the polarization splitter to an output side, so that the input side and the output side are a same side;




The invention still provides a comb wavelength division multiplexer, comprising: an input device at input side, a polarization splitter; a λ/2 phase delay wave plate; a birefringent crystal filter; a mirror; a λ/4 phase delay wave plate; a polarization splitter; and two λ/2 phase delay wave plates, said two λ/2 phase delay wave plates are disposed respectively in an reflective optical path in front of the polarization splitter: said λ/4 phase delay wave plate is disposed between the polarization splitter and the mirror.











BRIEF DESCRIPTION OF THE DRAWINGS




The invention will be explained in further detail with reference to the accompanying drawings, in which:





FIG. 1

is a construction of the first embodiment of the invention,





FIG. 2

is a vertical view of light path of the embodiment in

FIG. 1

;





FIG. 3

shows a side view of light path of PMD compensator;





FIG. 4

is a schematic diagram of the construction of the second embodiment of the invention;





FIG. 5

is a vertical view of light path of the embodiment in

FIG. 4

;




FIG.


6


and

FIG. 7

are two embodiments with collimator array of the invention,





FIG. 8

is a construction of the collimator array in FIG.


6


and

FIG. 7

;





FIG. 9

is a transmission spectrum of the one-stage filter; and





FIG. 10

is a transmission spectrum of the two-stage filter.











In these FIGURES, reference number


1


represents I/O section,


1


-


1


is three-core collimator,


1


-


2


is trapezoid prism,


1


-


3


is three-core collimator array reference number


2


represents polarization splitter,


3


represents PMD compensation element,


4


is λ/2 phase delay element,


5


is the birefringent crystal filtering element group,


6


is the reflective parallel light polarization splitter,


6


-


1


is polarization splitter,


6


-


2


is comer cube prism,


6


-


3


and


6


-


4


are λ/2 phase delay elements,


6


-


5


represents λ/4 phase delay element,


6


-


7


represents flat mirror.




In

FIG. 2

, an input light includes wavelength channels


1


and wavelength channels


2


. The wavelength channels


1


refer to a sequence of wavelengths which has its phase changed to [2Kπ] when getting out of the birefringent crystal filtering element group


5


; the wavelength channels


2


refer to a sequence of wavelength which has its phase changed to [(2K+1)π] when getting out of the birefringent crystal filtering element group


5


. Light beam L


101


passes through polarization splitter


2


, and then divided into light beam L


106


A and light beam L


106


A, wherein the polarization direction of light beam L


106


B passing through a glass plate


3


and a λ/2 phase delay wave plate


4


is same as that of light beam L


106


A; at the same time, the light path difference of L


106


B and L


106


A are compensated, that is to say, the PMD caused by polarization splitter is compensated, a principle of the compensation will be explained latter in detail. Since the characterizations of L


106


A and L


106


B are identical with each other in the latter half of the path, only one of them will be described hereafter. After light beam L


106


passes through birefringent filtering element group


5


, the wavelength channels


1


and


2


have different polarization direction due to their different phase changes. In light beam L


108


, the polarization direction of wavelength channels


1


is perpendicular to the paper, while the polarization direction of wavelength channels


2


is parallel to the paper. After light beam L


108


passes through polarization splitter


6


, the wavelength channels


1


and


2


are divided into light beams L


111


and L


110


; the two light beams exchange their positions after passing through prism


6


-


2


. Since their different polarization states with the effect of polarization splitter


6


-


1


, light beam L


110


turns back as light beam L


109


, light beam L


111


normally passing through polarization splitter


6


-


1


turns back as light beam L


107


. Light beams L


107


and L


109


pass through the birefringent filtering element group


5


again to obtain a two-stage filtering effect. At the same time, the light beam L


107


of wavelength channels


1


remains unchanged polarization as light beam L


104


, the light beam L


109


of wavelength channels


2


changes to light beam L


105


with polarization perpendicular to the paper; as a result, light beams L


104


, L


105


and L


106


have a same polarization direction, and a same polarization plane; light beams L


104


and L


105


will be two light beams L


102


and L


103


that are parallel to light beam L


101


and in a same plane with each other after they pass through devices


4


,


3


and


2


. Then they will be coupled to three single-core collimator array, or pass through a trapezoid prism


1


-


2


and be coupled into a three-core collimator


1


-


1


; when manufacturing, we may put device


1


-


2


between device


4


and device


5


to spare space. In

FIG. 5

, the descriptions with respect to light beams L


201


, L


206


A, L


206


B, L


206


and L


208


are same with those with respect to light beams L


101


, L


106


A, L


106


B, L


106


and L


108


in FIG.


2


. Light beam L


210


is wavelength channels


2


, light beam L


211


is wavelength channels


1


, their phases change λ/2 after passing through λ/4 phase delay element


6


-


5


, flat mirror


6


-


2


, their polarization direction change 90° relative to the original polarization direction, but the polarization direction will be same with the original polarization direction after they pass through λ/2 phase delay elements


6


-


3


and


6


-


4


respectively; light beam L


207


is wavelength channels


2


, and light beam L


209


is wavelength channels


1


. The polarization direction of light beam L


207


will be perpendicular to the paper after passing through birefringent filtering element group


5


, while the polarization direction of light beam L


209


will have no change. Therefore, light beams L


204


, L


205


and L


206


will have a same polarization direction and be in a same polarization plane, from here on, their light path is same as that in

FIG. 2

, light beams L


204


and L


205


will be two light beams L


202


and L


203


that are parallel to light beam L


201


and in a same plane with each other after they pass through devices


4


,


3


and


2


.

FIG. 3

is a side view of light path of the two embodiments when light beam pass through compensator


3


. It shows the light path when light has passed through a polarization splitter and a PMD compensator, and also shows a PMD compensation effect.

FIG. 8

is a collimation lens array


1


-


3


. There is V-shaped slot used to fix fiber on section


1


-


3


-


1


, section


1


-


3


-


2


is a collimation lens.




FIG.


9


and

FIG. 10

are transmission spectra of the one-stage filter and the two-stage filter, using the birefringent crystal filtering element group that has three 7 mm YVO


4


crystals lined up. The distance between the two transmission peaks is about 100 GHz. The table below shows a comparison between the two spectra:





















−0.5 dB




−1.0 dB




−3.0 dB




−25.0 dB




−30.0 dB











One-stage Filter




0.45




0.55




0.76




1.35




1.40






Two-stage Filter




0.37




0.45




0.62




1.15




1.21














The above descriptions and the drawings provide two embodiments with two different wavelength division device of the invention. One embodiment adopts a comer cube prism as a reflection body; the other uses a flat mirror as a reflection body.

FIG. 1

relates to a reflective parallel light polarization splitter with a comer cube prism. The light beams are of opposite direction before and after reflection, but still on a same plane. The spacing distance of two light beams after reflection is determined by birefringent crystal and dependent on the optical axis direction, length, and birefringent index of the crystal. The crystal, for example, may be YVO


4


, TiO


2


, a-BBO, CaCO


3


, etc., if 10 mm YVO


4


crystal is used, the spacing distance will be 1 mm.

FIG. 4

relates to a reflective parallel light polarization splitter with a flat mirror and a λ/4 phase delay element. Because a 45° axis direction and a λ/4 phase delay element are applied, the polarization states of two light beams after separation change 90° angle. In order to have them turn to original state, λ/2 phase delay elements


6


-


3


and


6


-


4


with 45° axis direction are added.




The invention adopts a construction that can compensate PMD caused by the polarization splitter. In the polarization splitter, because the path of light O and the path of light E are very different, PMD is caused. We have to compensate the path of the light beam that passes a short path, so as to eliminate PMD. For example, in order to compensate a PMD caused by a 7 mm YVO


4


polarization splitter with 45° axis direction, we first calculate the path difference of O light and E light to be about 0.67 mm, If using K


9


glass element to make compensation, the element must be 1.24 mm in thickness.




In such a reflective wavelength division device, if we modify the birefringent filtering element group by electro-optic modulation, magneto-optic modulation or other modulation device, we may obtain a reflective optical switcher. We only need replace the filter element group with a phase-delay-controllable birefringent crystal, e.g. liquid crystal, to obtain an optical switcher.



Claims
  • 1. A comb wavelength division multiplexer having an input side including an input device, said multiplexer comprising:a first polarization splitter (2) optically coupled to the input device; a first λ/2 phase delay means (4) optically coupled to said polarization splitter; a birefringent crystal filter (5) optically coupled to said λ/2 phase delay means and said first polarization splitter; and a reflective polarization splitter device (6) including a second polarization splitter (6-1), said reflective polarization splitter device being optically coupled to said birefringent crystal filter for splitting an incident light beam from the birefringent crystal filter into respective polarized beams, and reflecting said respective polarized beams back through said birefringent crystal filter and said first polarization splitter to an output device on the input side, wherein a three-core collimator and trapezoid prism provides the input device and said output device.
Priority Claims (1)
Number Date Country Kind
0114440 A Mar 2000 CN
US Referenced Citations (10)
Number Name Date Kind
5471340 Cheng et al. Nov 1995 A
5606439 Wu Feb 1997 A
5724165 Wu Mar 1998 A
5768005 Cheng et al. Jun 1998 A
5808763 Duck et al. Sep 1998 A
5930418 Chang Jul 1999 A
5930422 Cheng Jul 1999 A
6005697 Wu et al. Dec 1999 A
6097869 Chang et al. Aug 2000 A
6212313 Li Apr 2001 B1
Foreign Referenced Citations (3)
Number Date Country
1193124 Sep 1998 CN
0884615 Jun 1998 EP
9100535 Jul 1990 WO