Optical amplifiers - Test methods -- Part 11-2: Polarization mode dispersion parameter - Poincaré sphere analysis method

Applies to all commercially available optical amplifiers (OAs) including optical fibre amplifiers (OFAs) using active fibres and semiconductor optical amplifiers (SOAs) using semiconductor gain media.

Prüfverfahren für Lichtwellenleiter-Verstärker -- Teil 11-2: Polarisationsmodendispersion - Kugelanalyse nach Poincaré

Amplificateurs optiques - Méthodes d'essai -- Partie 11-2: Paramètre de dispersion en mode de polarisation - Méthode d'analyse par la sphère de Poincaré

S'applique à tous les amplificateurs optiques (AO) disponibles sur le marché, y compris les amplificateurs à fibres optiques (OFA) à fibres actives et les amplificateurs optiques à semi-conducteurs (SOA) qui utilisent un dispositif semi-conducteur pour le gain.

Optični ojačevalniki – Preskusne metode – 11-2. del: Parameter disperzije polarizacijskega načina – Metoda analize s Poincaréjevo kroglo (IEC 61290-11-2:2005)

General Information

Status
Published
Publication Date
31-Oct-2005
Technical Committee
Current Stage
6060 - National Implementation/Publication (Adopted Project)
Start Date
01-Nov-2005
Due Date
01-Nov-2005
Completion Date
01-Nov-2005

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SIST EN 61290-11-2:2005SLOVENSKInovember 2005
STANDARDOptični ojačevalniki – Preskusne metode – 11-2. del: Parameter disperzije polarizacijskega načina – Metoda analize s Poincaréjevo kroglo (IEC 61290-11-2:2005)Optical amplifiers - Test methods - Part 11-2: Polarization mode dispersion parameter - Poincaré sphere analysis method (IEC 61290-11-2:2005)©
Standard je založil in izdal Slovenski inštitut za standardizacijo. Razmnoževanje ali kopiranje celote ali delov tega dokumenta ni dovoljenoReferenčna številkaSIST EN 61290-11-2:2005(en)ICS33.180.30







EUROPEAN STANDARD
EN 61290-11-2 NORME EUROPÉENNE EUROPÄISCHE NORM
May 2005 CENELEC European Committee for Electrotechnical Standardization Comité Européen de Normalisation Electrotechnique Europäisches Komitee für Elektrotechnische Normung
Central Secretariat: rue de Stassart 35, B - 1050 Brussels
© 2005 CENELEC - All rights of exploitation in any form and by any means reserved worldwide for CENELEC members.
Ref. No. EN 61290-11-2:2005 E
ICS 33.180.30
English version
Optical amplifiers –
Test methods Part 11-2: Polarization mode dispersion parameter –
Poincaré sphere analysis method (IEC 61290-11-2:2005)
Amplificateurs optiques –
Méthodes d'essai Partie 11-2: Paramètre de dispersion
en mode de polarisation –
Méthode d'analyse par la sphère
de Poincaré (CEI 61290-11-2:2005)
Prüfverfahren für Lichtwellenleiter-Verstärker Teil 11-2: Polarisationsmodendispersion - Kugelanalyse nach Poincaré (IEC 61290-11-2:2005)
This European Standard was approved by CENELEC on 2005-04-01. CENELEC members are bound to comply with the CEN/CENELEC Internal Regulations which stipulate the conditions for giving this European Standard the status of a national standard without any alteration.
Up-to-date lists and bibliographical references concerning such national standards may be obtained on application to the Central Secretariat or to any CENELEC member.
This European Standard exists in three official versions (English, French, German). A version in any other language made by translation under the responsibility of a CENELEC member into its own language and notified to the Central Secretariat has the same status as the official versions.
CENELEC members are the national electrotechnical committees of Austria, Belgium, Cyprus, Czech Republic, Denmark, Estonia, Finland, France, Germany, Greece, Hungary, Iceland, Ireland, Italy, Latvia, Lithuania, Luxembourg, Malta, Netherlands, Norway, Poland, Portugal, Slovakia, Slovenia, Spain, Sweden, Switzerland and United Kingdom.



EN 61290-11-2:2005 - 2 - Foreword The text of document 86C/640/FDIS, future edition 1 of IEC 61290-11-2, prepared by SC 86C, Fibre optic systems and active devices, of IEC TC 86, Fibre optics, was submitted to the IEC-CENELEC parallel vote and was approved by CENELEC as EN 61290-11-2 on 2005-04-01. The following dates were fixed: – latest date by which the EN has to be implemented
at national level by publication of an identical
national standard or by endorsement
(dop)
2006-01-01 – latest date by which the national standards conflicting
with the EN have to be withdrawn
(dow)
2008-04-01 Annex ZA has been added by CENELEC. __________ Endorsement notice The text of the International Standard IEC 61290-11-2:2005 was approved by CENELEC as a European Standard without any modification. In the official version, for Bibliography, the following notes have to be added for the standards indicated: IEC 60793-1-1 NOTE Harmonized as EN 60793-1-1:2003 (not modified). IEC 60825-1 NOTE Harmonized as EN 60825-1:1994 (not modified). IEC 60825-2 NOTE Harmonized as EN 60825-2:2004 (not modified). IEC 60874-1 NOTE Harmonized as EN 60874-1:1999 (not modified). IEC 61291-1 NOTE Harmonized as EN 61291-1:1998 (not modified). IEC 61291-4 NOTE Harmonized as EN 61291-4:2003 (not modified). __________



- 3 - EN 61290-11-2:2005
Annex ZA
(normative)
Normative references to international publications
with their corresponding European publications The following referenced documents are indispensable for the application of this document. For dated references, only the edition cited applies. For undated references, the latest edition of the referenced document (including any amendments) applies. NOTE Where an international publication has been modified by common modifications, indicated by (mod), the relevant EN/HD applies. Publication Year Title EN/HD Year IEC/TR 61292-5 - 1) Optical amplifiers Part 5: Polarization mode dispersion parameter - General information - -
1) Undated reference.







NORME INTERNATIONALECEIIEC INTERNATIONAL STANDARD 61290-11-2Première éditionFirst edition2005-03 Amplificateurs optiques – Méthodes d'essai – Partie 11-2: Paramètre de dispersion
en mode de polarisation – Méthode d'analyse par la sphère de Poincaré
Optical amplifiers – Test methods – Part 11-2: Polarization mode dispersion parameter – Poincaré sphere analysis method
Pour prix, voir catalogue en vigueur For price, see current catalogue IEC 2005
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Web: www.iec.ch CODE PRIX PRICE CODE M Commission Electrotechnique InternationaleInternational Electrotechnical Commission



61290-11-2  IEC:2005 – 3 –
CONTENTS
FOREWORD.5
1 Scope and object.9 2 Normative references.9 3 Abbreviated terms.11 4 Apparatus.11 4.1 General.11 4.2 Light source.13 4.3 State of polarization generator.15 4.4 Analyser.17 5 Procedure.19 6 Calculations.21 6.1 Poincaré sphere analysis calculations.21 6.2 Display of differential group delay versus wavelength.23 6.3 Average differential group delay.23 6.4 Maximum differential group delay.23 7 Test results.23
Bibliography.25



61290-11-2  IEC:2005 – 5 –
INTERNATIONAL ELECTROTECHNICAL COMMISSION ____________
OPTICAL AMPLIFIERS –
TEST METHODS –
Part 11-2: Polarization mode dispersion parameter – Poincaré sphere analysis method
FOREWORD 1) The International Electrotechnical Commission (IEC) is a worldwide organization for standardization comprising all national electrotechnical committees (IEC National Committees). The object of IEC is to promote international co-operation on all questions concerning standardization in the electrical and electronic fields. To this end and in addition to other activities, IEC publishes International Standards, Technical Specifications, Technical Reports, Publicly Available Specifications (PAS) and Guides (hereafter referred to as “IEC Publication(s)”). Their preparation is entrusted to technical committees; any IEC National Committee interested in the subject dealt with may participate in this preparatory work. International, governmental and non-governmental organizations liaising with the IEC also participate in this preparation. IEC collaborates closely with the International Organization for Standardization (ISO) in accordance with conditions determined by agreement between the two organizations. 2) The formal decisions or agreements of IEC on technical matters express, as nearly as possible, an international consensus of opinion on the relevant subjects since each technical committee has representation from all interested IEC National Committees.
3) IEC Publications have the form of recommendations for international use and are accepted by IEC National Committees in that sense. While all reasonable efforts are made to ensure that the technical content of IEC Publications is accurate, IEC cannot be held responsible for the way in which they are used or for any misinterpretation by any end user. 4) In order to promote international uniformity, IEC National Committees undertake to apply IEC Publications transparently to the maximum extent possible in their national and regional publications. Any divergence between any IEC Publication and the corresponding national or regional publication shall be clearly indicated in the latter. 5) IEC provides no marking procedure to indicate its approval and cannot be rendered responsible for any equipment declared to be in conformity with an IEC Publication. 6) All users should ensure that they have the latest edition of this publication. 7) No liability shall attach to IEC or its directors, employees, servants or agents including individual experts and members of its technical committees and IEC National Committees for any personal injury, property damage or other damage of any nature whatsoever, whether direct or indirect, or for costs (including legal fees) and expenses arising out of the publication, use of, or reliance upon, this IEC Publication or any other IEC Publications.
8) Attention is drawn to the Normative references cited in this publication. Use of the referenced publications is indispensable for the correct application of this publication. 9) Attention is drawn to the possibility that some of the elements of this IEC Publication may be the subject of patent rights. IEC shall not be held responsible for identifying any or all such patent rights. International Standard IEC 61290-11-2 has been prepared by subcommittee 86C: Fibre optic systems and active devices, of IEC technical committee 86: Fibre optics. The text of this standard is based on the following documents: FDIS Report on voting 86C/640/FDIS 86C/660/RVD
Full information on the voting for the approval of this standard can be found in the report on voting indicated in the above table.



61290-11-2  IEC:2005 – 7 –
This publication has been drafted in accordance with the ISO/IEC Directives, Part 2. IEC 61290-11 consists of the following parts under the new general title Optical amplifiers – Test methods: Part 11-1:
Polarization mode dispersion – Jones matrix eigenanalysis method (JME) Part 11-2:
Polarization mode dispersion parameter – Poincaré sphere analysis method Future standards in this series will carry the new general title as cited above. Titles of existing standards in this series will be updated at the time of the next edition. The committee has decided that the contents of this publication will remain unchanged until the maintenance result date indicated on the IEC web site under "http://webstore.iec.ch" in the data related to the specific publication. At this date, the publication will be
• reconfirmed; • withdrawn; • replaced by a revised edition, or • amended.



61290-11-2  IEC:2005 – 9 –
OPTICAL AMPLIFIERS –
TEST METHODS –
Part 11-2: Polarization mode dispersion parameter – Poincaré sphere analysis method
1 Scope and object This part of IEC 61290 applies to all commercially available optical amplifiers (OAs) including optical fibre amplifiers (OFAs) using active fibres and semiconductor optical amplifiers (SOAs) using semiconductor gain media.
Polarization mode dispersion (PMD) causes an optical pulse to spread in the time domain. This dispersion could impair the performance of a telecommunications system. The effect can be related to differential group velocity and corresponding arrival times of different polarization components of the signal. For a narrowband source, the effect can be related to a differential group delay (DGD) between pairs of orthogonally polarized principal states of polarization (PSP). This test method describes a procedure for measuring the PMD of OAs. The measurement result is obtained from the measurement of the normalised Stokes parameters at two closely spaced wavelengths. The mathematical basis together with an example of calculation for the Poincaré sphere analysis (PSA) method to calculate PMD is provided in the technical report IEC 61292-5. The method described herein has been shown to be immune to polarization-dependent gain (PDG) and polarization-dependent loss (PDL) up to approximately 1 dB [‡]. Although the PSA, in practice, is applicable to unpumped (that is, unpowered) OAs, the PSA technique in this standard applies to pumped (that is, powered) OAs only. NOTE All numerical values followed by (‡) are suggested values for which the measurement is assured. Other values may be acceptable but should be verified. 2 Normative references The following referenced documents are indispensable for the application of this document. For dated references, only the edition cited applies. For undated references, the latest edition of the referenced document (including any amendments) applies. IEC 61292-5, Optical amplifiers – Part 5: Polarization mode dispersion parameter – General information



61290-11-2  IEC:2005 – 11 –
3 Abbreviated terms ASE
amplified spontaneous emission DGD
differential group delay DOP
degree of polarization DUT
device (optical amplifier) under test FTSA
Fourier transform spectrum analyser JME
Jones matrix eigenanalysis method OA
optical amplifier OFA
optical fibre amplifier OSA
optical spectrum analyser PDG
polari
...

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