This application claims priority to Japanese Patent Application No. 2008-152243, filed Jun. 10, 2008, in the Japanese Patent Office. The Japanese Patent Application No. 2008-152243 is incorporated by reference in its entirety.
The present disclosure relates to a delay interferometer using a spatial optical system, which is used for demodulating a differential phase shift keying signal in optical fiber communication, particularly in optical fiber communication using a dense wavelength division multiplexing (DWDM) system.
In optical fiber communication using a DWDM system, an optical signal which is modulated by the differential phase shift keying method (DPSK) or the differential quadrature phase shift keying method (DQPSK) is mainly transmitted, and a received optical signal is demodulated by a demodulator including a delay interferometer.
As a delay interferometer using a spatial optical system, a Michelson delay interferometer is well known.
A light beam S10 which is incident from incident means is split by a splitting portion 111 into two light beams S1, S12. The light beams S1, S12 are incident on the Michelson delay interferometer. Four interference outputs from the Michelson delay interferometer due to the input light beams S1, S12 are reflected by a mirror 116 or 117, and received by an optical detector 122 or 123 through a lens 118, 119, 120, or 121. These components constitute a demodulator for a DQPSK optical signal.
[Patent Reference 1] JP-A-2007-151026
The mirror 116 or 117 corrects the optical path length difference between the light beams S11, S12 produced by the splitting portion 111. When it is assumed that the optical detector 122 is an optical fiber, axis and angle deviations in the optical axis are produced in the mirror 116 or 117 by position and angle errors of the mirror surface, thereby producing a problem in that the coupling to the optical fiber is hardly performed.
Exemplary embodiments of the present invention provide a delay interferometer in which the difference of optical path lengths to output ports in the delay interferometer can be easily corrected.
The invention is configured in the following manners.
(1) A delay interferometer comprises:
a package including an input port through which input light is received, an A-channel first output port and an A-channel second output port, through which output an A-channel interference output light, and a B-channel first output port and a B-channel second output port, through which output a B-channel interference output light;
a Michelson delay interferometer unit mounted in the package, the Michelson delay interferometer unit including a splitting portion which splits the input light into A and B channels in such a manner that there is an optical path length difference between the A-channel interference output light and the B-channel interference output light, the Michelson delay interferometer unit optically processing the split lights as an input light to form the A-channel interference output light and the B-channel interference output light; and
a first optical path length compensating member which is interposed between the A-channel interference output light or the B-channel interference output light, and the A-channel first output port or the B-channel first output port.
(2) In the delay interferometer of (1), the delay interferometer further includes a second optical path length compensating member which is interposed between the A-channel interference output light or the B-channel interference output light, and the A-channel second output port or the B-channel second output port.
(3) In the delay interferometer of (1) or (2), the first optical path length compensating member and the second optical path length compensating member are rectangular prisms.
(4) In the delay interferometer of any one of (1) to (3), the Michelson delay interferometer unit includes a beam splitter and reflectors which are integrally structured by a same material.
Other features and advantages may be apparent from the following detailed description, the accompanying drawings and the claims.
Hereinafter, the invention will be described in more detail with reference to the drawings.
Referring to
The embodiment operates on the same principle as the Michelson delay interferometer disclosed in Patent Reference 1 shown in
In the Michelson delay interferometer unit 2, the A-channel first interference output light L1A is output from an A-channel first output port 4A disposed in the first sidewall portion 1a, and the A-channel second interference output light L2A is output from an A-channel second output port 5A disposed in the second sidewall portion 1b.
Similarly, the B-channel first interference output light L1B is output from a B-channel first output port 4B disposed in the first sidewall portion 1a, and the B-channel second interference output light L2B is output from a B-channel second output port 5B disposed in the second sidewall portion 1b.
First and second optical path length compensating members 100, 200 are formed by a rectangular prism and placed in the optical paths. First and second optical path length compensating members 100, 200 correct the optical path length difference between output ports. More specifically, first and second optical path length compensating members 100, 200 correct the optical path length difference caused by the splitting portion 21, etc., between the optical path lengths of the A-channel first interference output light L1A and the A-channel second interference output light L2A, and the optical path lengths of the B-channel first interference output light L1B and the B-channel second interference output light L2B. In the rectangular prism, the incident and emission faces for a light flux are substantially parallel to each other, and axis and angle deviations are not produced in the incident light and the emission light of the rectangular prism. Therefore, reduction of characteristics in an optical fiber which receives light can be minimized.
In the embodiment, the first and second optical path length compensating members 100, 200 increase the optical path lengths of the A-channel interference output light. Alternatively, the first and second optical path length compensating members may be inserted into the B channel depending on the design of the splitting portion 21. Namely, the first and second optical path length compensating members are inserted into the channel in which reduction of optical path lengths is performed.
The input light Li which is incident through the input port 3 is passed through a lens to be converted to substantially parallel light, and then incident on the splitting portion 21. The incident substantially parallel light flux is split into transmitted light and reflected light by an NPBS film of the splitting portion 21.
The light transmitted through the NPBS film is totally reflected by a total reflection surface to be formed as an A-channel light flux, and the light reflected by the NPBS film of the splitting portion 21 is formed as a B-channel light flux. As shown in Fig.
As shown in
The transmitted light which is formed by causing the reflected light A-1 to be transmitted through the NPBS film 22b, and the reflected light which is formed by causing the transmitted light A-2 to be reflected by the NPBS film 22b are output as the A-channel first interference output light L1A to the A-channel first output port 4A. At this time, the A-channel first interference output light L1A is the output the Michelson delay interferometer which is determined by the positions of the first and second reflectors 23, 24, i.e., the optical path length difference between the reflected light A-1 and the transmitted light A-2.
Similarly, the reflected light which is formed by causing the reflected light A-1 to be reflected by the NPBS film 22b, and the transmitted light which is formed by causing the transmitted light A-2 to be transmitted through the NPBS film 22b are output as the A-channel second interference output light L2A to the A-channel second output port 5A.
Also with respect to the light flux B shown in
The A-channel first and second interference output light L1A, L2A are supplied into the respective output ports through the first and second optical path length compensating members 100, 200, and the B-channel first and second interference output light L1B, L2B are supplied into the respective output ports through the first and second optical axis shifting members 61, 62.
In the embodiment, the first and second optical path length compensating members 100, 200 have a function of comprehensively correcting the optical path difference between the A and B channels caused by the splitting portion 21, the first and second optical axis shifting members 61, 62, and the like.
In the embodiment, in the package, the first and second optical axis shifting members 61, 62 each configured by a parallel prism are inserted into optical paths of the B-channel first interference output light L1B and the B-channel second interference output light L2B, respectively.
The optical axis shifting members 61, 62 eliminate restrictions of the distances between the ports disposed in the sidewall portions, and reduce the sizes of the components of the Michelson delay interferometer unit 2, thereby contributing to the design of the miniaturized package 1.
A thin-film heater is formed on the A-channel phase adjusting plate 25A which is inserted in the optical path of the reflected light A-1. When an electric power is supplied to the heater, the refractive index of the phase adjusting plate 25A is changed, and the optical path length is equivalently changed, whereby the interference spectrum of the A-channel interference output light can be adjusted. Similarly, the B-channel phase adjusting plate 25B inserted in the optical path of the reflected light B-1 can adjust the interference spectrum of the B-channel interference output light. More specifically, a thin-film heater is formed on the B-channel phase adjusting plate 25B, and when an electric power is supplied to the heater, the refractive index of the phase adjusting plate 25B is changed, and the optical path length is equivalently changed, whereby the interference spectrum of the B-channel interference output light can be adjusted.
In the integrated configuration, the optical path length therein can be equivalently shortened because the material has a high refractive index (for example, about 1.5), and therefore the package size can be further reduced. Also the beam splitter 22 and the first reflector 23 can be integrated with each other. When these components are integrated with each other, it is possible to realize a performance improvement in which the optical path length change due to the difference of the coefficients of thermal expansion is minimized.
Although the embodiment in which the delay interferometer has the configuration where the package has the perpendicular wall portions, and the input and output ports are perpendicularly disposed in the wall portions has been described, the invention is versatile, and is not restricted by the shape of the package.
Number | Date | Country | Kind |
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2008-152243 | Jun 2008 | JP | national |