BS EN 61300-3-43:2009 BSI British Standards Fibre optic interconnecting devices and passive components – Basic test and measurement procedures Part 3-43: Examinations and measurements – Mode transfer function measurement for fibre optic sources NO COPYING WITHOUT BSI PERMISSION EXCEPT AS PERMITTED BY COPYRIGHT LAW raising standards worldwide™ BRITISH STANDARD BS EN 61300-3-43:2009 National foreword This British Standard is the UK implementation of EN 61300-3-43:2009 It is identical to IEC 61300-3-43:2009 It supersedes DD IEC/PAS 61300-3-43:2006 which is withdrawn The UK participation in its preparation was entrusted by Technical Committee GEL/86, Fibre optics, to Subcommittee GEL/86/2, Fibre optic interconnecting devices and passive components A list of organizations represented on this committee can be obtained on request to its secretary This publication does not purport to include all the necessary provisions of a contract Users are responsible for its correct application © BSI 2009 ISBN 978 580 56660 ICS 33.180.20 Compliance with a British Standard cannot confer immunity from legal obligations This British Standard was published under the authority of the Standards Policy and Strategy Committee on 31 July 2009 Amendments issued since publication Amd No Date Text affected BS EN 61300-3-43:2009 EUROPEAN STANDARD EN 61300-3-43 NORME EUROPÉENNE April 2009 EUROPÄISCHE NORM ICS 33.180.20 English version Fibre optic interconnecting devices and passive components Basic test and measurement procedures Part 3-43: Examinations and measurements Mode transfer function measurement for fibre optic sources (IEC 61300-3-43:2009) Dispositifs d'interconnexion et composants passifs fibres optiques Méthodes fondamentales d'essais et de mesures Partie 3-43: Examens et mesures Mesures de la fonction de transfert de modes pour les sources fibres optiques (CEI 61300-3-43:2009) Lichtwellenleiter Verbindungselemente und passive Bauteile Grundlegende Prüf- und Messverfahren Teil 3-43: Untersuchungen und Messungen Messung der Moden-Transferfunktion bei Lichtwellenleiterquellen (IEC 61300-3-43:2009) This European Standard was approved by CENELEC on 2009-04-01 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, Bulgaria, Cyprus, the Czech Republic, Denmark, Estonia, Finland, France, Germany, Greece, Hungary, Iceland, Ireland, Italy, Latvia, Lithuania, Luxembourg, Malta, the Netherlands, Norway, Poland, Portugal, Romania, Slovakia, Slovenia, Spain, Sweden, Switzerland and the United Kingdom CENELEC European Committee for Electrotechnical Standardization Comité Européen de Normalisation Electrotechnique Europäisches Komitee für Elektrotechnische Normung Central Secretariat: avenue Marnix 17, B - 1000 Brussels © 2009 CENELEC - All rights of exploitation in any form and by any means reserved worldwide for CENELEC members Ref No EN 61300-3-43:2009 E BS EN 61300-3-43:2009 EN 61300-3-43:2009 -2- Foreword The text of document 86B/2780/FDIS, future edition of IEC 61300-3-43, prepared by SC 86B, Fibre optic interconnecting devices and passive components, of IEC TC 86, Fibre optics, was submitted to the IEC-CENELEC parallel vote and was approved by CENELEC as EN 61300-3-43 on 2009-04-01 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) 2010-01-01 – latest date by which the national standards conflicting with the EN have to be withdrawn (dow) 2012-04-01 Annex ZA has been added by CENELEC Endorsement notice The text of the International Standard IEC 61300-3-43:2009 was approved by CENELEC as a European Standard without any modification BS EN 61300-3-43:2009 -3- EN 61300-3-43:2009 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 When an international publication has been modified by common modifications, indicated by (mod), the relevant EN/HD applies Publication Year Title EN/HD Year Optical fibres Part 1-20: Measurement methods and test procedures - Fibre geometry EN 60793-1-20 2002 2) IEC 60793-1-20 - 1) IEC 61300-1 - 1) Fibre optic interconnecting devices and passive components - Basic test and measurement procedures Part 1: General and guidance EN 61300-1 2003 2) IEC 61300-3-4 - 1) Fibre optic interconnecting devices and passive components - Basic test and measurement procedures Part 3-4: Examinations and measurements Attenuation EN 61300-3-4 2001 2) ｗｗｗ．ｂｚｆｘｗ．ｃｏｍ 1) Undated reference 2) Valid edition at date of issue BS EN 61300-3-43:2009 –2– 61300-3-43 © IEC:2009(E) CONTENTS Scope .5 Normative references .5 General description Theory 5 4.1 Alternative method 4.2 Mode power distribution 4.3 Constraints Apparatus 5.1 General 5.2 Test sample 5.3 Sample positioning device .9 5.4 Optical system 10 5.5 Camera 10 5.6 Video digitiser 10 5.7 Calibration 10 Procedure 11 6.1 Mounting and aligning the sample 11 6.2 Optimisation 11 6.3 Acquiring the data 11 Calculations 11 7.1 Background level subtraction 11 7.2 Location of centroid of intensity profile 12 7.3 Differentiating the intensity profile 12 7.4 Computing the MTF 13 Results 14 ｗｗｗ．ｂｚｆｘｗ．ｃｏｍ Annex A (informative) 16 Bibliography 18 Figure – Example of normalised MTF Figure – Example of normalised MPD Figure – Schematic of measurement apparatus Figure – Location of fibre centre using symmetry computation 13 Figure A.1 – Sensitivity of MTF and MPD to core diameter 16 Figure A.2 – Sensitivity of MTF and MPD to profile factor 17 BS EN 61300-3-43:2009 61300-3-43 © IEC:2009(E) –5– FIBRE OPTIC INTERCONNECTING DEVICES AND PASSIVE COMPONENTS – BASIC TEST AND MEASUREMENT PROCEDURES – Part 3-43: Examinations and measurements – Mode transfer function measurement for fibre optic sources Scope This part of IEC 61300 describes the method for measuring the mode transfer function (MTF) to be used in characterising the launch conditions for measurements of attenuation and or return loss of multimode passive components The MTF may be measured at the operational wavelengths 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 61300-1, Fibre optic interconnecting devices and passive components – Basic test and measurement procedures – Part 1: General and guidance ｗｗｗ．ｂｚｆｘｗ．ｃｏｍ IEC 61300-3-4, Fibre optic interconnecting devices and passive components – Basic test and measurement procedures – Part 3-4: Examination and measurements – Attenuation IEC 60793-1-20, Optical fibres – Part 1-20: Measurement methods and test procedures – Fibre geometry General description The modal distribution launched into multimode fibre can vary widely with different light sources This variation in launched modal distribution can result in significant differences in measured attenuation in the same component The MTF test method gives information about the launched modal distribution (LMD) condition in a measured component The MTF test method is based on a measurement of the near-field intensity distribution in the fibre [ 1], [2] Theory For a fibre with a power-law index profile n(r), given by, α ⎡ ⎛r⎞ ⎤ n( r ) = n1⎢1 − 2Δ⎜ ⎟ ⎥ ⎢⎣ ⎝ a ⎠ ⎥⎦ 0,5 where a is the fibre core radius; α is the profile factor (α = for a parabolic profile); _ Figures in square brackets refer to the Bibliography ⎛r⎞ ⎜ ⎟ ≤1 ⎝a⎠ (1) BS EN 61300-3-43:2009 61300-3-43 © IEC:2009(E) –6– Δ is the relative index difference, given by n − n22 Δ= 2n12 (2) where n is the index at fibre centre; n is the cladding index The near-field intensity profile in the fibre I ( r ) may be determined from an integration of the mode transfer function MTF( δ ) in the fibre, as follows (ignoring constants): Δ I( r ) = ( δ ) × dδ ∫ MTF α (3) ( a) Δr where δ is the normalised propagation constant; r/a is the normalised radial position Differentiating both sides gives the MTF as follows (ignoring constants): ⎡ dI ( r ) ⎤ MTF ( δ ) = ⎢ × ⎥ α r −1 ⎦ δ = Δ (r ⎣ dr (4) ｗｗｗ．ｂｚｆｘｗ．ｃｏｍ )α a The MTF is usually plotted as in terms of the principal mode number m divided by the maximum principal mode number M, where m ⎡δ ⎤ = M ⎢⎣ Δ ⎥⎦ ( 2+α ) 2α ⎡r ⎤ =⎢ ⎥ ⎣a⎦ ( +α ) (5) The term (m/M) is usually referred to as the relative mode number, or the normalised mode number The maximum principle mode number M, is given by M= α ⎛ n1 2πa ⎞ ⎜ ⎟ Δ α +2⎝ λ ⎠ (6) A typical normalised MTF plot is shown in Figure 1, where it can be seen, in this example, that normalised mode numbers up to about 0,6 are equally filled and higher order modes are progressively less well-filled BS EN 61300-3-43:2009 61300-3-43 © IEC:2009(E) –7– 1,0 Normalised MTF 0,75 0,50 0,25 0,0 0,0 0,2 0,4 0,6 0,8 1,0 Normalised mode number IEC 2371/08 Figure – Example of normalised MTF 4.1 Alternative method If the profile factor, α, in Equation (4) is not known, then an alternative expression for MTF can be used ｗｗｗ．ｂｚｆｘｗ．ｃｏｍ It is known[ 3] that in a fully-filled fibre (i.e MTF=1 for all mode numbers) the near-field intensity profile, I o , is approximately the same shape as the square of the refractive index profile, n(r) Furthermore, the term r α -1 Equation (4) is equal (ignoring constants) to the differential of n(r)2 and so Equation(4) can be rewritten as: ⎡ dI ( r ) ⎤ × MTF ( δ ) = ⎢ ⎥ dr dI ( r ) dr o ⎣ ⎦ δ = Δ (r )2 a (7) where a value of α=2 has been assumed in order to compute values for the normalised mode number Thus the MTF is equal to the ratio of the derivative of the intensity profile under test to the derivative of the intensity profile of the same fibre under fully-filled conditions 4.2 Mode power distribution For graded index multimode fibre the number of discrete modes in a particular mode group is proportional to the principal mode number Thus higher-order mode groups contain more modes and therefore will carry more light if all the modes are equally excited This can be represented by the mode power distribution (MPD), defined as: MPD( m ) = MTF ( m ) × m (8) Because of this relationship of modes within mode groups, the MPD transform effectively displays the relative power in the mode groups An example of a normalised MPD is shown in Figure 2, where it can be seen, in this case, that the peak power level occurs around 0,65 normalised mode number BS EN 61300-3-43:2009 61300-3-43 © IEC:2009(E) –8– 1,0 Normalised MPD 0,75 0,50 0,25 0,0 0,0 0,2 0,4 0,6 0,8 Normalised mode number 1,0 IEC 2372/08 Figure – Example of normalised MPD 4.3 Constraints The MTF measurement method described herein is only valid under certain conditions, as follows: ｗｗｗ．ｂｚｆｘｗ．ｃｏｍ • modes within a mode group carry the same power; • there are random phases between the propagating modes It has been found[4] that both these conditions can be simultaneously met if the line-width Δλ of the source is sufficiently broad, leading to the so-called "mode-continuum approximation", given by: Δλ λ ≥ 2Δ a × k0 × N (10) where λ is the optical wavelength; k0 = 2π/λ; N is the group index, given by N = n1 − λ × dn1 dλ (11) Typically, for a 50 μm core diameter fibre, with 0,21 numerical aperture, then Δλ > 0,5 nm at 850 nm and Δλ > 1,0 nm at 300 nm satisfy this condition If the source line-width does not meet this criterion then interference between propagating modes may take place, resulting in "speckle" in the near-field image The method can, however, still be applied to such sources by gently shaking, or somehow agitating, the fibre under test so as to cause a temporal averaging of the speckle pattern In this case, it is important to ensure the near-field is azimuthally symmetric This can be achieved by checking that the MTFs measured at 45° intervals around the fibre coincide with each other[5] • The peak of the MPD occurs at a normalised mode number of