IEC TR 61282-3-2006 Fibre optic communication system design guides - Part 3 Calculation of polarisation mode dispersion《纤维光学通信系统设计指南.第3部分 偏振模散射计算》.pdf

《IEC TR 61282-3-2006 Fibre optic communication system design guides - Part 3 Calculation of polarisation mode dispersion《纤维光学通信系统设计指南.第3部分 偏振模散射计算》.pdf》由会员分享，可在线阅读，更多相关《IEC TR 61282-3-2006 Fibre optic communication system design guides - Part 3 Calculation of polarisation mode dispersion《纤维光学通信系统设计指南.第3部分 偏振模散射计算》.pdf（40页珍藏版）》请在麦多课文档分享上搜索。

1、 TECHNICAL REPORT IEC TR 61282-3Second edition 2006-10Fibre optic communication system design guides Part 3: Calculation of link polarization mode dispersion Reference number IEC/TR 61282-3:2006(E) Publication numbering As from 1 January 1997 all IEC publications are issued with a designation in the

2、 60000 series. For example, IEC 34-1 is now referred to as IEC 60034-1. Consolidated editions The IEC is now publishing consolidated versions of its publications. For example, edition numbers 1.0, 1.1 and 1.2 refer, respectively, to the base publication, the base publication incorporating amendment

3、1 and the base publication incorporating amendments 1 and 2. Further information on IEC publications The technical content of IEC publications is kept under constant review by the IEC, thus ensuring that the content reflects current technology. Information relating to this publication, including its

4、 validity, is available in the IEC Catalogue of publications (see below) in addition to new editions, amendments and corrigenda. Information on the subjects under consideration and work in progress undertaken by the technical committee which has prepared this publication, as well as the list of publ

5、ications issued, is also available from the following: IEC Web Site (www.iec.ch) Catalogue of IEC publications The on-line catalogue on the IEC web site (www.iec.ch/searchpub) enables you to search by a variety of criteria including text searches, technical committees and date of publication. On-lin

6、e information is also available on recently issued publications, withdrawn and replaced publications, as well as corrigenda. IEC Just Published This summary of recently issued publications (www.iec.ch/online_news/ justpub) is also available by email. Please contact the Customer Service Centre (see b

7、elow) for further information. Customer Service Centre If you have any questions regarding this publication or need further assistance, please contact the Customer Service Centre: Email: custserviec.ch Tel: +41 22 919 02 11 Fax: +41 22 919 03 00 TECHNICAL REPORT IEC TR 61282-3Second edition 2006-10F

8、ibre optic communication system design guides Part 3: Calculation of link polarization mode dispersion PRICE CODE IEC 2006 Copyright - all rights reserved No part of this publication may be reproduced or utilized in any form or by any means, electronic or mechanical, including photocopying and micro

9、film, without permission in writing from the publisher. International Electrotechnical Commission, 3, rue de Varemb, PO Box 131, CH-1211 Geneva 20, Switzerland Telephone: +41 22 919 02 11 Telefax: +41 22 919 03 00 E-mail: inmailiec.ch Web: www.iec.ch V For price, see current catalogue Commission Ele

10、ctrotechnique Internationale International Electrotechnical Commission 2 TR 61282-3 IEC:2006(E) CONTENTS FOREWORD.3 INTRODUCTION.5 1 Scope.6 2 Basic design models for total system PMD performance6 2.1 Notation.6 2.2 Calculation of system PMD 7 3 Calculation of cabled fibre PMD 9 3.1 General .9 3.2 M

11、ethod 1: Calculating PMD Q , the PMD link design value11 3.3 Method 2: Calculating the probability of exceeding DGD max 14 3.4 Equivalence of methods.18 4 Calculation of optical component PMD 20 5 Summary of acronyms and symbols 20 Annex A (informative) PMD concatenation fundamentals 22 Annex B (inf

12、ormative) Combining Maxwell extrema from two populations26 Annex C (informative) Worked example30 Annex D (informative) Relationship of probability to system performance31 Annex E (informative) Concatenation experiment32 Bibliography34 Figure 1 Various passing distributions 15 Figure 2 Worst case ap

13、proach assumption .17 Figure 3 Convolution of two Diracs .17 Figure 4 Equivalence envelopes for method 1/2 defaults.19 Figure A.1 Sum of randomly rotated elements.25 Figure A.2 Sum of randomly rotated elements.25 Table 1 Probability based on wavelength average.9 Table 2 Acronyms and definitions .21

14、Table 3 Symbols and clause of definition 21 Table E.1 Concatenation math verification33 TR 61282-3 IEC:2006(E) 3 INTERNATIONAL ELECTROTECHNICAL COMMISSION _ FIBRE OPTIC COMMUNICATION SYSTEM DESIGN GUIDES Part 3: Calculation of link polarization mode dispersion FOREWORD 1) The International Electrote

15、chnical 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 t

16、his 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 Nationa

17、l 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

18、) 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 fr

19、om 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 h

20、eld 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

21、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 Publicat

22、ion. 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, propert

23、y 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 thi

24、s 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

25、 all such patent rights. The main task of IEC technical committees is to prepare International Standards. However, a technical committee may propose the publication of a technical report when it has collected data of a different kind from that which is normally published as an International Standard

26、, for example “state of the art“. IEC 61282-3, which is a technical report, has been prepared by subcommittee 86C: Fibre optic systems and active devices, of IEC technical committee 86: Fibre optics. This second edition cancels and replaces the first edition published in 2002. It is a technical revi

27、sion that includes the following significant changes: a) the title has been changed to better reflect its applicability to links; b) Equations (1) and (2) were simplified in order to align with agreements in the ITU-T. 4 TR 61282-3 IEC:2006(E) The text of this technical report is based on the follow

28、ing documents: Enquiry draft Report on voting 86C/701/DTR 86C/720/RVC Full information on the voting for the approval of this technical report can be found in the report on voting indicated in the above table. This publication has been drafted in accordance with the ISO/IEC Directives, Part 2. A lis

29、t of all parts of the IEC 61282 series, published under the general title Fibre optic communication system design guides, can be found on the IEC website. The committee has decided that the contents of this publication will remain unchanged until the maintenance result date indicated on the IEC web

30、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. A bilingual version of this publication may be issued at a later date. TR 61282-3 IEC:2006(E) 5 INTRODUCTION Po

31、larization mode dispersion (PMD) is usually described in terms of a differential group delay (DGD), which is the time difference between the principal states of polarization of an optical signal at a particular wavelength and time. PMD in cabled fibres and optical components causes an optical pulse

32、to spread in the time domain, which may impair the performance of a fibre optic telecommunication system, as defined in IEC 61281-1. 6 TR 61282-3 IEC:2006(E) FIBRE OPTIC COMMUNICATION SYSTEM DESIGN GUIDES Part 3: Calculation of link polarization mode dispersion 1 Scope This part of IEC 61282 provide

33、s guidelines for the calculation of polarization mode dispersion (PMD) in fibre optic systems to accommodate the statistical variation of PMD and differential group delay (DGD) in optical fibre cables and components. This technical report describes methods for calculating PMD due to optical fibre ca

34、bles and optical components in an optical link. The calculations are compatible with those documented in the outdoor optical fibre cable specification IEC 60794-3. Example calculations are given to illustrate the methods for calculating total optical link PMD from typical cable and optical component

35、 data. The calculations include the statistics of concatenating individual optical fibre cables drawn from a specified distribution. The calculations assume that all components have PMD equal to the maximum specified value. The calculations described cover first order PMD only. The following subject

36、 areas are currently beyond the scope of this technical report, but remain under study: calculation of second and higher order PMD; accommodation of components with polarization dependent loss (PDL) if it is assumed that PDL is negligible in optical fibre cables; system impairments (power penalty) d

37、ue to PMD; interaction with chromatic dispersion and other nonlinear effects. Measurement of PMD is beyond the scope of this technical report. Methods of measurement of PMD of optical fibre and cable are given in IEC 60793-1-48. The measurement of optical amplifier PMD is in IEC 61290-11-1. The meas

38、urement of component PMD is in IEC 61300-3-32. Measurement of link PMD is given in 61280-4-4. A general theory and guidance on measurements is given in 61282-9. 2 Basic design models for total system PMD performance 2.1 Notation For cabled fibre and components with randomly varying DGD, the PMD freq

39、uency domain measurement is based on averaging the individual DGD values for a range of wavelengths. The probability density function of DGD values is known to be Maxwell for fibre, and is assumed to be Maxwell, in effect, for components. The single parameter for the Maxwell distribution scales with

40、 the PMD value. For long fibre and cable (typically longer than 500 m to 1 000 m), the PMD value is divided by the square root of the length to obtain the PMD coefficient. For components, the PMD value is reported without normalization. The following terms and meanings will be used to distinguish th

41、e various expressions: DGD value The differential group delay at a time and wavelength (ps) PMD value The wavelength average of DGD values (ps) PMD coefficient The length normalised PMD (ps/sqrt(km) DGD coefficient The length normalised DGD (ps/sqrt(km) TR 61282-3 IEC:2006(E) 7 NOTE The term “DGD co

42、efficient” is used only in some of the calculations. The physical square root length dependence of the PMD value does not apply to DGD. Deterministic components are those for which the DGD may vary with wavelength, but not appreciably with time. The variation in wavelength may be complex, depending

43、on the number and characteristics of the sub-components within. For these types of components, either the maximum DGD is reported or the wavelength average is reported as the PMD value. For components with multiple paths, such as an optical demultiplexer, the maximum DGD of the different paths shoul

44、d be reported as the PMD value. 2.2 Calculation of system PMD PMD values of randomly varying elements can be added in quadrature. Annex A shows the basis of this, as well as one basis for concluding that the Maxwell distribution is appropriate to describe the distribution of DGD values. Annex A desc

45、ribes the concatenation in terms of the addition of rotated polarization dispersion vectors (pdv) which are, for randomly varying components, assumed to be random in magnitude and direction over both time and wavelength. For deterministic components, the evolution of the pdv with wavelength may be q

46、uite complex, but for each wavelength, there is a value that does not vary appreciably with time. Analysis of the relationships in Annex A shows that deterministic components that are randomly aligned in combination with random elements behave like random components. For randomly varying components

47、such as fibre, the statistics of DGD variation imply that there is little wavelength dependence of the PMD value. This leads to an equivalence between PMD measurement methods such as Jones Matrix Eigenanalysis (JME) and interferometric methods (IT) where the wavelength ranges of the two are differen

48、t. For deterministic elements, there can be distinct dependence of both the DGD and PMD on the wavelength range. Therefore for these elements, when doing calculations which combine both randomly varying and deterministic elements, the combined values are only representative of the wavelength overlap

49、. The relationships of Annex A also show an analysis for an assumption that the deterministic components are randomly aligned. For this assumption, the DGD values are time randomised across the wavelengths by the fibre. The random alignment of these components with respect to the other elements leads to the following conclusions for deterministic components. The quadrature addition of PMD values can be used to calculate the