EP1585953A1 - Multi-signal determination of polarization dependent characteristic - Google Patents
Multi-signal determination of polarization dependent characteristicInfo
- Publication number
- EP1585953A1 EP1585953A1 EP03795021A EP03795021A EP1585953A1 EP 1585953 A1 EP1585953 A1 EP 1585953A1 EP 03795021 A EP03795021 A EP 03795021A EP 03795021 A EP03795021 A EP 03795021A EP 1585953 A1 EP1585953 A1 EP 1585953A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- signal
- polarization
- stimulus
- under test
- code
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
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- 230000010287 polarization Effects 0.000 title claims abstract description 162
- 230000001419 dependent effect Effects 0.000 title claims abstract description 37
- 230000003287 optical effect Effects 0.000 claims abstract description 49
- 230000004044 response Effects 0.000 claims abstract description 44
- 238000012360 testing method Methods 0.000 claims abstract description 41
- 238000000034 method Methods 0.000 claims abstract description 19
- 238000011156 evaluation Methods 0.000 claims description 13
- 239000011159 matrix material Substances 0.000 claims description 9
- 238000012545 processing Methods 0.000 claims description 3
- 238000004445 quantitative analysis Methods 0.000 claims 2
- 238000005259 measurement Methods 0.000 abstract description 11
- 239000006185 dispersion Substances 0.000 abstract description 2
- 230000005540 biological transmission Effects 0.000 description 5
- 230000008859 change Effects 0.000 description 4
- 238000004891 communication Methods 0.000 description 4
- 239000000835 fiber Substances 0.000 description 4
- 238000001228 spectrum Methods 0.000 description 4
- 238000004458 analytical method Methods 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 230000009466 transformation Effects 0.000 description 2
- 238000012512 characterization method Methods 0.000 description 1
- 238000005388 cross polarization Methods 0.000 description 1
- 238000009795 derivation Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- 239000000284 extract Substances 0.000 description 1
- 239000002075 main ingredient Substances 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 239000013307 optical fiber Substances 0.000 description 1
- 230000000717 retained effect Effects 0.000 description 1
- 230000009897 systematic effect Effects 0.000 description 1
- 230000001131 transforming effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/33—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
- G01M11/337—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face by measuring polarization dependent loss [PDL]
Definitions
- the present invention relates to the measurement of optical devices having single or multiple ports and comprising one or more optically active or passive components.
- the invention relates to a determination of polarization dependent characteristic of these devices.
- a method of measuring multi-port optical devices is known from EP-A-1235062. Testing optically active or passive devices exhibiting polarization dependent characteristic has become an increasingly important task in optical communications measurement industry. With ongoing increase of distances in optical transmission communication systems, mechanical stress or temperature induced birefringence, e.g., in optical fibers, are growingly affecting polarization characteristic of a signal that is input to the communication system, i.e. to one or more optical devices.
- Optical devices affected by polarization changes are among others, e.g., switches, cross-connects, attenuators, fiber optic couplers, filters, isolators, amplifiers, or passive fiber optic transmission lines. Changes in the state of polarization of a signal input to optical devices may result in unwanted signal fluctuations. Characterization of an optical device with respect to polarization therefore is one of the main goals when improving optical transmission systems.
- a method of measuring polarization mode dispersion (PMD) is known from US-A-6, 144,450. SUMMARY OF
- An optical device under test having at least one input and at least one output is applied with a stimulus signal, which is superimposed with characteristic identification portions, each of said portions being set into a different state of polarization by means of a plurality of polarization units.
- This stimulus signal is introduced to the system by means of a signal application unit, which - according to a preferred embodiment - may comprise one or more optical signal sources, e.g. a tunable laser source, but the stimulus signal may also be introduced from an external source.
- the signal application unit forwards the stimulus signal to each of the plurality of polarization units.
- Each of said polarization units is designed to set the stimulus signal forwarded from the signal application unit into a unique state of polarization.
- a state of polarization set by a first polarization unit differs from another state of polarization set by a second polarization unit.
- Polarization units as described in this document may comprise polarization controllers.
- One known and commonly available product is the Agilent 8169 A polarization controller of the applicant Agilent Technologies.
- Polarization controllers as being usable in the present system may either be designed to set an incoming optical signal into a fixed state of polarization or may be designed to apply adjustable, variable polarization characteristic to said signal. What is important is, that a single stimulus signal is introduced by the application unit and is applied - or split - towards each of the polarization units, each of said polarization units setting the stimulus signal separately into a unique state of polarization, which differs from that of another polarization unit within the present set.
- a characteristic identification portion is attached to each of the polarized stimulus signals.
- one modulation unit affecting said identification portion is each associated with one of the polarization units.
- a characteristic identification portion within said stimulus signal uniquely corresponds to a state of polarization applied to the signal by means of the polarization unit.
- the stimulus signal as being applied by the signal application unit comprises a carrier portion having a carrier frequency.
- Said modulation unit is designed to apply the characteristic identification portion by means of frequency, amplitude or phase modulation to a stimulus signal.
- the identification portion is represented by mixture frequencies located in side bands of the carrier frequency.
- the uniquely polarized and identifiable stimulus signal split towards each of the polarization units is then superimposed for being input to the optical device under test.
- the superimposed signal comprises a carrier portion having multiple components with differing states of polarization each portion being characterized by one unique frequency.
- the DUT to be tested with the stimulus signal provided as explained above may have one or more in- and outputs, and may be embodied as any kind of active or passive optical device.
- Gain systems such as amplifiers, or fiber optic couplers, filters, attenuators, switches, cross-connects, isolators, etc. or even polarization controllers itself maybe examined with respect to polarization characteristic using the system and the method of the present invention.
- the invention is not restricted to devices as listed above, rather the invention is applicable to any device, or system of devices including long transmission line systems, which exhibit polarization change characteristic, in particular polarization dependent loss, which will be explained in embodiments below.
- the response signal associated with the stimulus signal by means of the DUT is received by a signal receiving unit.
- the signal receiving unit comprises an optical power meter for measuring the response signal.
- the signal receiving unit may comprise a semiconductor diode as a sensor element, e.g., InGaAs-diodes for a wavelength range 850 - 1700 nm, Ge-diodes for 600 - 1650 nm or Si-diodes for 400 - 1000 nm.
- each of the individual frequencies may be associated with one of said states of polarization.
- the receiving unit is therefore enabled to trace the identification portion originating from the stimulus signal from within the response signal. Due to the polarization characteristic of the optical device, the polarized identification portions are affected by loss or gain characteristic. With the help of the signal receiving unit, each of the polarized identification portions traced within the response signal can be measured.
- the measured values of the polarized identification portions e.g. the power of each component
- SOP ⁇ loss- or gain-change of the applied states of polarizations
- Mueller-method can be used to evaluate the maximum and minimum signal power and therefrom, e.g., the polarization dependent loss (PDL) or gain (PDG).
- the evaluation unit may comprise a PC, workstation or other logical processing unit, the user interface, and/or a memory.
- PDL polarization dependent loss
- PDG gain
- a matrix e.g., the so-called Mueller-matrix
- Mueller-matrix is set up relating each of the components of the four states of polarization prior and after passing the DUT to each other.
- the corresponding linear equation system is then solved by means of the evaluation unit, wherein the polarization dependent loss can easily be represented by the matrix coefficients.
- a main ingredient is that the stimulus signal is split into a plurality of portions, each portion being supplied with an additional identification portion and a unique state of polarization.
- the state of polarization is recovered by means of the identification portion and is then measured.
- the coefficients can be derived with just one measurement cycle, i.e. a single shot of said stimulus signal.
- Prior art methods employed serial measurement techniques (in time). Thus, few efforts are necessary; in particular, less time and calibration work is needed to characterize an optical device.
- the invention can be partly or entirely embodied or supported by one or more suitable software programs, which can be stored on or otherwise provided by any kind of data carrier, and which might be executed in or by any suitable data processing unit.
- Software programs or routines are preferably applied to receive the measured values of the polarized signal components from the response signal, compare each of the components with corresponding values known or measured from the stimulus signal and then solve a linear equation system relating the components to each other.
- Fig. 1 shows a schematic illustration of a first embodiment of the present invention
- FIG. 2 show a schematic illustration of a second embodiment of the present invention
- Fig. 3 shows a signal spectrum with states of polarization each of the stimulus signal and the response signal that is generated by the system shown in Fig. 2.
- Fig. 1 shows a schematic illustration of a first embodiment of the present invention providing a system for determining polarization dependent characteristic of an optical device under test 10 (DUT).
- an optical stimulus signal 6 of a TLS 4 is provided to a first coupler 105.
- the first coupler 105 has 4 output ports and splits the optical signal 6 into 4 parts 6a, 6b, 6c and 6d.
- Each signal part 6a, 6b, 6c and 6d is modulated by modulation units 27, 29, 127 and 129, respectively.
- the first signal 6a is modulated using a first binary code code 1
- the second signal part is modulated using a second binary code code 2
- the third signal part is modulated using a third binary code code 3
- the fourth signal part is modulated using a fourth binary code code 4.
- Codes 1 , 2, 3 and 4 are orthogonal to each other.
- each coded signal 6a ' , 6b ' , 6c ' , 6d ' receives a defined polarization by polarization controllers 27a, 29b, 127c, 129d in the path of the coded signal 6a ' , 6b ' , 6c', 6d', respectively.
- the resulting polarized signals 6a “ , 6b “ , 6c “ , 6d " are then combined at a coupler 135 and provided as a superimposed signal 136 to a DUT 10.
- modulation units 27, 29, 127, 129 intensity modulators e.g. LiNb0 3 - based
- a response signal 140 leaving the DUT 10 is then detected at a detector 44.
- a detector signal 48 containing coded signals for main polarizations and cross polarization is then provided to a correlation unit 52 containing four correlators 52-1 , 52-2, 52-3 and 52-4.
- Each correlator 52-1 , 52-2, 52-3 and 52-4 is demodulating the signal 48 by multiplying signal 48 with the codes code 1 , code 2, code 3 and code 4, respectively.
- the results of the demodulation is then provided by the correlation unit 52 at output ports a, b, c and d of the correlators 52-1 , 52-2, 52-3 and 52-4, respectively.
- Fig. 2 shows a schematic representation of a second embodiment.
- An optical stimulus signal S a is generated by a tunable laser source 4.
- the wavelength may be tuned over a limited wavelength range in order to investigate polarization effects of DUT 10 that further depend on wavelength.
- the stimulus signal S a is input to a first polarization unit 20, which may be a polarization controller, for setting the signal into a predetermined state of polarization (signal S ).
- a first polarization unit 20 which may be a polarization controller, for setting the signal into a predetermined state of polarization (signal S ).
- This step is performed since optical modulation units such as a Mach-Zehnder based on LiNb0 3 as well as the subsequent polarization units generally work polarization dependent. Consequently, the influence of systematic errors on the measurement results can considerably be reduced.
- polarization controller 20 polarizes signal S a linearly with angle 90 degrees.
- the resulting spectrum is depicted with its attached state of polarization in Fig. 3.
- the signal attains the form
- ⁇ c is a carrier frequency
- the resulting signal S5 is then applied in parallel - or split - to each one of a set of modulation units 30-1 ... 30-4.
- a set of four modulation units is implemented.
- These modulation units modulate stimulus signal SK . by means of, e.g., amplitude, phase or frequency modulation. While the spectrum of polarized signal SK is represented by one or more carrier frequencies, the corresponding carrier portion signal SK. is thus supplemented with each an unique identification portion to give modulated stimulus signals S c ⁇ 1 ... S c -4.
- a modulation frequency 1 - ⁇ m is applied to the stimulus signal SK that enters modulation unit 30-1
- a modulation frequency of 4- ⁇ m is applied to the stimulus signal SK. that enters modulation unit 30-2.
- Each of the modulated stimulus signals is then forwarded to one of a set of polarization units 40-1 ... 40-4, which each may be embodied, e.g., as a polarization controller.
- Stimulus signal S c -1 is retained in its state of polarization, i.e. linear vertical (90°) polarization.
- Stimulus signal S c -2 is converted to linear diagonal (45°) polarization
- Stimulus signal S c -3 is converted to linear horizontal (0°) polarization
- Stimulus signal S c -4 is converted to circular polarization.
- Each of the four separated stimulus signals S c -1 ... S c -4 now has a unique pair of modulation frequencies and states of polarization.
- the polarized, modulated signals are denoted as S ⁇ -l ... Srj-4 in
- a frequency selective receiver 60 receives a response signal R a from DUT 10.
- said receiver 60 is adjustable in selecting desired frequency ranges by comprising an optical/electrical signal transformation unit (by means of, e.g., a semiconductor diode) with corresponding electrical filters having filter wavelength ranges according to the current needs. Accordingly, it becomes possible to select the identification portion of the transformed signal in order to trace and recover an indication of one of the stimulus signals S ⁇ -l ... S ⁇ j-4 within the (electrically transformed) response signals R -1... Rtr 4 - It is clear to a person skilled in the art of optical communications measurement device techniques that instead of using one adjustable frequency selective receiver four or more frequency selective receivers 60 may be employed in parallel, each of them being fed with an input DUT response signal coming from a coupler, which splits the response signal R a into at least four different parts.
- an optical/electrical signal transformation unit by means of, e.g., a semiconductor diode
- Each signal measured by the power meter 70 (bandpass larger than 2 times the maximum of the modulation frequency) comprises the following frequency dependent characteristic signals:
- Tp 0 denotes a loss of power for the respective polarized signal
- PDL is the maximum change in transmission of an optical component versus all possible input polarization states.
- EQ e.g. by a similar measurement with a power meter prior to inputting the signal into the DUT 10
- com the intensity is measured
- the polarization dependent characteristic of the DUT 10 can be derived.
- An evaluation unit 80 extracts the measured power values and starts a detailed analysis of these results based on the concept of the Mueller matrix, which describes a transition of states of polarization due to, e.g., an optical element:
- SO represents the power
- S1 the amount of linear horizontal polarization
- S2 that of +/- 45° linear horizontal polarization
- S3 the amount of left or right hand circular polarization.
- the relation between the Stokes vector of the stimulus input signal and that of the output response signal can be expressed by a linear equation system which is represented by a 4x4 matrix, also called the Mueller- Matrix.
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- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
Abstract
Description
Claims
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| EP03795021A EP1585953A1 (en) | 2002-09-13 | 2003-07-25 | Multi-signal determination of polarization dependent characteristic |
Applications Claiming Priority (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| PCT/EP2002/010285 WO2004025878A1 (en) | 2002-09-13 | 2002-09-13 | Coded polarization-dependent analyzing |
| WOPCT/EP02/10285 | 2002-09-13 | ||
| PCT/EP2003/050335 WO2004025242A1 (en) | 2002-09-13 | 2003-07-25 | Multi-signal determination of polarization dependent characteristic |
| EP03795021A EP1585953A1 (en) | 2002-09-13 | 2003-07-25 | Multi-signal determination of polarization dependent characteristic |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| EP1585953A1 true EP1585953A1 (en) | 2005-10-19 |
Family
ID=35034648
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP03795021A Withdrawn EP1585953A1 (en) | 2002-09-13 | 2003-07-25 | Multi-signal determination of polarization dependent characteristic |
Country Status (1)
| Country | Link |
|---|---|
| EP (1) | EP1585953A1 (en) |
-
2003
- 2003-07-25 EP EP03795021A patent/EP1585953A1/en not_active Withdrawn
Non-Patent Citations (1)
| Title |
|---|
| See references of WO2004025242A1 * |
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