Patent Application
20100209039
The invention relates to a method and to an apparatus for compensating the polarization-dependent shift of the center frequency in an optical filter comprising an interferometer by way of compensating for the birefringence in at least one waveguide of the interferometer, wherein at least one half-wave plate is inserted into the beam path of the interferometer and at least a section of the at least one waveguide to the right and to the left of the half-wave plate is brought to a pre-selected temperature.
Interferometers of the kind cited in the beginning are used in various applications for the optical data transmission in different applications, e.g. in optical switches, in variable optical attenuators, in optical modulators, in demultiplexers used in OTDM systems, in DPSK methods, in DQPSK methods as well as an array of sensor applications.—These uses typically involve a Mach-Zender interferometer; however, a Michelson interferometer may be used as well.
It is known to integrate Mach-Zender Interferometers together with active or passive components in a planar integrated circuit. Such Mach-Zender interferometers integrated in planar integrated circuits are compact, easy to control and cost effective.
These types of Mach-Zender interferometers, however, exhibit a transfer behavior in optical filters or switches that is a function of the polarization of the incident light. This polarization-dependency restricts the range of application of integrated Mach-Zender interferometers in optical communications engineering at high bandwidths and/or high transmission rates. For applications in DPSK, DQPSK, OTDM or similar systems, the requirements are exceptionally high for polarization-independence of transmission rates in order to achieve reliable demodulation of an arriving data stream. With known Mach-Zender interferometers, which are used as optical filters or switches in planar-integrated circuits, a polarization-dependent shift of the central frequency (PDFS) occurs that is so extensive that the known Mach-Zender interferometers are usually insufficient for the demands of DPSK-, DQPSK and OTDM Systems.
For example, delay-line interferometers (DLIs) are used for the demodulation on the receiver side in OTDM, DPSK or DQPSK systems. The allowable PDFS of such a DLI in a DQPSK system ranges at approximately ±200 MHz for a bit-rate of 40 Gb/s. Such PDFS requires that the birefringence be restricted in the optical paths of the interferometers to approx. ±2×10−6 in the C and L bands.
For Mach-Zender interferometers in planar integrated circuits, the birefringence of the waveguide equals approximately BWG˜10−3, and the PDFS accordingly equals approximately ±100 GHz. This birefringence is primarily induced by tension. Thus, it changes with the temperature on a linear basis. The corresponding slope (in this case, the decrease) S is determined based on S=BWG/ΔTProc, with ΔTProc=Tf−T0 denoting the difference between the final temperature of the production process Tf and the operating temperature T0. The value of S is always negative and ranges at approximately −10−5 K−1 for polymer waveguides; the typical temperature difference ΔTProc amounts approximately 100 K to 200 K.
From the prior art it is known that to restrict the PDFS, a Mach-Zender interferometer must be equipped with a half-wave plate made of polyimide, which must be placed in the center of the transmission path. The half-wave plate thereby causes a rotation of the polarization vector, so that the PDFS may be equalized in the first section of the interferometer and in the second section of the interferometer. Under practical conditions, this equalization is incomplete, so that an interferometer equipped as aforementioned achieves a PDFS of approximately ±1000 MHz. This means that the birefringence equals approximately 10−5.
However, this measure is insufficient to satisfy the demands on the PDFS in a DQPSK system as illustrated above.
The object of the present invention therefore is to provide a method and an apparatus for the diminishment of polarization-dependent shift of the center frequency (PDFS) in optical filters, in order to achieve higher data rates and/or bandwidths in OTDM, DPSK or DQPSK systems compared to conventional optical filters.
The object is solved by a method for compensating polarization-dependent shifts of the central frequency in an optical filter, which comprises an interferometer, by compensation of the birefringence in at least one waveguide of the interferometer, wherein at least one half-wave plate is inserted into the beam path of the interferometer, and at least a section of at least one waveguide is brought to a pre-selected temperature on the right and left of the half-wave plate, and wherein at least one section on the right of the half-wave plate is brought to a first temperature T1 and at least one section on the left of the half-wave plate is brought to a second temperature T2.
Furthermore, the object is solved by providing an interferometer with two arms that each comprise at least one waveguide, wherein a half-wave plate is arranged into both arms of the interferometer, and at least a section of the waveguides of both arms of the interferometer to the right and left of the half-wave plate are in a heat-exchange contact to at least one heating element each, and the heating elements placed in the arm with the larger optical path length of the interferometer to the right and left of the half-wave plate each exhibit a length δ|1 and the heating elements placed in the other arm of the interferometer to the right and left of the half-wave plate each exhibit a length of δ|2=δ|1*L/(L+ΔL).
Useful embodiments of the invention are subject to the dependent claims.
According to the invention, in the method for compensation of polarization-dependent frequency shifts in optical waveguides, at least one half-wave plate is introduced into the beam path and at least a predefined section of the optical waveguide on both sides of the half-wave plate is heated. To do so, at least one section of each waveguide is brought to a pre-selected temperature. This is achieved by delivering heat to the waveguides at the right and left of the half-wave plate by means of at least two heating elements. These heating elements may be embodied as heating electrodes.
According to an embodiment of the invention, the tension-induced birefringence of the waveguide, and thus the Mach-Zender interferometer's residual PDFS following installation of the half-wave plate, may be compensated by bringing at least one section to the right of the half-wave plate to a first temperature T1, and at least one section to the left of the half-wave plate to a second temperature, T2, which differs from T1. Preferably, the sections on each side of the half-wave plate each comprise a plurality of interconnected sections, so that a single section on the right and a single section on the left side of the half-wave plate is heated by the heating elements.
By heating the waveguides, their length and/or the refractive index and/or the tension-induced birefringence changes, so that a remaining asymmetry of the optical paths may be balanced on both the right and left of the half-wave plate by variable heating.
In an embodiment of the invention, the sections to the right and the left of the half-wave plate each feature a heating electrode of equal length δ|1 and their respective temperatures T1 and T2 satisfy the following condition:
T
2
−T
1=(Bres/BWG)*ΔTProc*(L/δ|1),
wherein
Bres: represents the birefringence corresponding to the residual PDSF
BWG: represents the birefringence of the waveguide;
ΔTProc: represents the difference between the process temperature and the ambient temperature and
L: represents the length of the waveguide.
Preferably, the method will be used in an embodiment of the invention, which is distinguished by the fact that the waveguide is integrated into a Mach-Zender interferometer. In this case, the length of the upper arm of the Mach-Zender Interferometer is given by (L+ΔL), so that a temperature difference of the upper arm of the Mach-Zender interferometer may be given by
T
2
−T
1=(Bres/BWG)*ΔTProc*{(L+ΔL)/δ|1},
For a Mach-Zender interferometer with a delay line in a DQPSK receiver, the delay time between both arms of the Mach-Zender interferometer must be equal during the period of the symbol. The heating electrode is used for this purpose, in order to coordinate the differences in optical path lengths. This is achieved by applying the temperature TDLI, which is required to correct the differences in the optical path lengths.
An embodiment of the invention entails the following combination: Applying a temperature of TDLI, reduced by half of the temperature difference ΔT=T2−T1 required for compensating the PDFS to the sections of the waveguide on the right (or left) of the half-wave plate, as well as applying a temperature of TDLI, increased by half of the temperature difference ΔT to the sections of the waveguide to the left (or right) of the half-wave plate. The results from this are temperatures from (TDLI−ΔT/2) and (TDLI+ΔT/2).
For polymer waveguides, only a small electrical power is required due to the high thermo-optical coefficients and the small thermal conductivity of the polymer materials in order to cover a broad tuning range.
If the invention is used in Mach-Zender interferometers, it may be advantageous to install a half-wave plate in the beam path of the waveguides in both arms of the Mach-Zender interferometer. Using this embodiment, the PDFS of the Mach-Zender interferometer may be compensated to a much higher extent than previously known, because pre-selected temperatures may be applied at least to a section of the waveguide both in the upper arm as well as in the lower arm of the Mach-Zender interferometer to the right and left of the half-wave plate, by bringing these sections into a heat-exchange contact with at least one heating element. The complexity of this embodiment is reduced if the waveguides on the right of the half-wave plate in both arms of the Mach-Zender interferometer are brought—at least in a section—to the equal temperature Tr, preferably to Tr=TDLI−ΔT/2, and likewise if the two waveguides on the left of the half-wave plate are brought to the same temperature T1, preferably T1=TDLI+ΔT/2. This may be achieved through the commensurate selection of the lengths of the heated section, or the length of the respective heating elements respectively.
The heated sections on each side of the half-wave plate may comprise several sub-sections. However, preferably a single continuous section will be heated both on the right and left of the half-wave plate. Accordingly, only one heating element is needed on each side for each waveguide. If the length of the heated sections in the upper arm (or the length of the heating element, respectively) both right and left equals δ|1, then the length of the sections heated in the lower arm (or the length of the heating element, respectively) both right and left of the half-wave plate each shall equal δ|2=δ|1*L/(L+ΔL).
According to the invention, it becomes possible to lower the birefringence to 10−5, which is made possible by means of the half-wave plate made of polyimide, even further. As values equal to 10−6 or below may be achieved for the birefringence, the high demands on waveguides in planar integrated circuits in DQPSK systems and other areas may be satisfied.
In a preferred embodiment of the invention, the assembly according to the invention is combined with a data processing device for controlling the temperatures of the heating elements.
A computer program, based on the invention, enables a data processing device, after it has been loaded into the memory of the data processing device, to execute a method for the compensation of polarization-dependent frequency shifts in optical waveguides, wherein the waveguides to the right and left of the half-wave plate may be brought to pre-selected temperatures, at least in a section. The computer program according to the invention additionally may keep the temperatures at a constant level.
Such computer programs may, for example, be available for download (in exchange for a fee or for free, or are openly accessible or password protected) in a data or communications network. The computer programs obtained in this manner may then be made useable through a method by which a computer program is downloaded from an electronic data network, such as from the Internet, for example, onto the data network of the connected data processing device.
In order to execute the method for compensation of polarization-dependent frequency shifts in optical waveguides, it is intended to deploy a computer-readable storage medium in which a program is stored that enables a data processing device (after it has been loaded into the memory of the data processing device) to execute the method for compensation of polarization dependent frequency shifts in optical waveguides wherein at least a section of the waveguide to the right and left of the half-wave plate may be set at pre-selectable temperatures.
The invention is described in greater detail hereinafter, making reference to the figures in the drawings on an embodiment. It illustrates
In
Δφ2=2π/λ*δB2*δ|1,
wherein δ|1 is the length of the heating element 12. The value Δφ1 is always negative, if the temperature increases. Nonetheless, passage through the half-wave plate 11 converts this phase shift into a positive birefringence, which is expressed by +|Δφ1|. The right heating electrode 13 is heated to a temperature T2, which results in a change in the waveguide's birefringence to δB2=|S*(T2−T0)|.
The corresponding phase shift is then:
Δφ2=2π/λ*δB2*δ|1.
The induced polarization phase shift of both heating elements 12, 13 thus may be indicated as follows:
Δφ2−Δφ1=2π/λ*(δB2−δB1)*δ|1.
The remaining PDFS may be viewed as the residual polarization phase shift:
Δ□res=2π/λ*(Bres*(L+ΔL),
wherein L denotes the length of the lower (shorter) arm 17 and (L+ΔL) indicates the upper (longer) arm 16 of the Mach-Zender interferometer.
For a total compensation of the phase shift, the condition Δ□res+(Δφ1−Δφ2)=0 applies, i.e.
2π/λ*Bres*(L+ΔL)=2π/λ*S*(T2−T1)*δ|1,
which yields the following temperature difference for heating elements 12, 13:
T
2
−T
1=(Bres/BWG)*ΔTProc*{(L+ΔL)/δ|1}.
Depending on the sign of Bres, the difference T2−T1 is positive or negative. The Quotient Bres/BWG will lie approximately in the range of 10−2 through 10−3, ΔTProc approximately in the range of 100 K through 200 K, the length factor {(L+ΔL)/δ|1} amounts approximately 10. It can be seen that a temperature difference of only a few degrees is sufficient in order to balance the remaining birefringence of the DLI.
For Mach-Zender interferometers that use a delay line in DQPSK receivers, a heating electrode is needed which compensates the frequency shift between the optical source and the DLI through a precise coordination of the optical path length difference of the delay line. For polymer waveguides, due to the high thermo-optic coefficients and the low thermal conductivity of the polymer material, only a small electrical power is required in order to cover a broad setting range.
In cases in which a half-wave plate 11 is used, the upper heating electrodes 12, 13 for compensating the optical path length are arranged advantageously to the left and right of the half-wave plate 11. The equalization effect for compensation of the PDFS can thereby be reached by heating both heating electrodes 12, 13 to different temperatures. If, for compensation of differences in lengths, the temperature of the waveguide is brought to the value TDLI, and for compensation of the PDFS a temperature difference of ΔT=T2−T1 is required, then an embodiment would entail bringing the heating electrodes 12, 13 to temperatures (TDLI−ΔT/2) resp. (TDLI+ΔT/2). Since no special structure is required, the invention provides a compact and cost-effective solution that uses minimal power consumption.
In order to compensate the PDFS in the entire Mach-Zender interferometer 10, the two heating elements 14, 15 must simultaneously balance the lower arm 17. If the heating elements 14, 15 of the lower arm 17 shall be heated to the same temperature as the heating elements 12, 13 of the upper arm, then the heating elements 14, 15 of the lower arm 17 must exhibit a length of δ|2=δ|1*L/(L+ΔL).
The invention is not restricted to the preferred embodiments presented. Rather, a collection of variations is conceivable, that could make use of the configuration based on the invention, and the method based on the invention, even in essentially different embodiments.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10 2007 031 864.4 | Jul 2007 | DE | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/EP08/57966 | 6/23/2008 | WO | 00 | 4/27/2010 |
