TIA SP3696-2000 Accelerated Measurement of BER and Q-Factor in Digital Optical Transmission Systems Using the Sinusoidal Interference Method Comment Period Expires July 26 2000 TIA.pdf
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1、STDaEIA SP NO 3b7b-ENGL 2000 3234hDO 065h520 295 811 May 26,2000 2500 Wilson Boulevard, Suite 300 Arlington, VA 22201 703/907-7700 FAX 703/907-7727 Representing the telecommunications industry in association with the Electromc Industries Alliance Copyright Telecommunications Industry Association Pro
2、vided by IHS under license with EIANot for ResaleNo reproduction or networking permitted without license from IHS-,-,-PLEASE FILL OUT AND SIGN THIS FORM AND RETURN IT WITH ANY COMMENTS TO: Billie Zidek-Comer Telecommunications Industry Assoc. 2500 Wilson Blvd., Suite 300 Arlington, VA 22201 -3834 (F
3、AX: 703/907-7727) SUBJECT: Standards Proposal No. 3696, Proposed New Standard “Accelerated Measurement of BER and Q-Factor in Digital Optical Transmission Systems Using the Sinusoidal Interference Method” (if approved, to be published as TWEL4-526-8) COMMENT PERIOD EXPIRES: JULY 26,2000 PRODUCER I G
4、ENERAL INTEREST of the relevance of this This information is re -page 2- Copyright Telecommunications Industry Association Provided by IHS under license with EIANot for ResaleNo reproduction or networking permitted without license from IHS-,-,- - STD.EIA SP NO 3696-ENGL 2000 3234600 065h522 068 H NO
5、TICE This document is a TWEIA Engineering Standards Proposal, rather than an interim or final Standard. It is published for purposes of comment and is subject to further review and modification by the TLA Technical Standards Subcommittee (TSSC), which may accept or reject the Standards Proposal. Acc
6、ordingly, readers of this Standards Proposal are cautioned against contained therein prior to the adoption of a final standard. TMIA disc1 responsibility for the consequences of such reliance. ion or TELECOMMUNICATIONS INDUSTRY 2500 Wilson Boulevard Copyright Telecommunications Industry Association
7、Provided by IHS under license with EIANot for ResaleNo reproduction or networking permitted without license from IHS-,-,- STD=EIA SP NO 3bqb-ENGL 2000 W 3234b00 Ob5b523 TT4 I1Ip SP-3696 (To be TINEIA-526-8) Section Sinusoidal Interference Meth 1 Introduction 2 Normative references 3 Appartus OFSTP-8
8、 Accelerated Measurement of BER and Q-Fa Digital Optical Transmission Systems U 5 4 S 5 P 3 4 b 4 erpretation ts 9 8 9 oidal Interference Method by Optical Injection 6 for the Sinusoidal Interference Method by Electrical Injection 7 b Result from the Sinusoidal Interference Method 10 11 R vs Optical
9、 Power for Three Methods A Comparison between OFSTP-8 and IEC and ITU requirements 12 RLN, TIA SC F0-2.1,5/00 I Copyright Telecommunications Industry Association Provided by IHS under license with EIANot for ResaleNo reproduction or networking permitted without license from IHS-,-,-STD*EIA SP NO 3bq
10、b-ENGL 2000 3234600 065652Y 930 1911 SP-3696 (To be TINEIA-526-8) OFSTP-8 Accelerated Measurement of BER and Q-Factor in Digital Optical Transmission Systems Using the Si n u soi d al 1 n te rfe re n ce Method of very low bit-error ratios educe the time required to 1 espe it-rates. The usual methods
11、 can -i2 in which optical power is varied, in this varying disturbance, representing noise, is I noise, shot noise, reflection-induced noise, laser se, crosstalk, jitter, etc. The sum of all noise sources tribution. The technique may not be applicable if the BER is astic processes, such as rare impu
12、lse noise. Its applicability with amplified spontaneous emission (ASE) is under study. The r or not a BER “floor“ is present. Such a floor is due to the signal- ,eing almost independent of the input power to the receiver. The method artificially degrades the di ita1 channel in a controlled manner, t
13、hereby raising the BER to a range (such as IO- to IO- ) within which the measurement time is substantially reduced. Values of BER vs. the amount of artificial degradation are recorded and then extrapolated to the poiiit of zero artificial degradation. The results of the optical sinsusoidal ?o RLN, T
14、IA SC FO-2.1, 5/00 3 Previous page is blank Copyright Telecommunications Industry Association Provided by IHS under license with EIANot for ResaleNo reproduction or networking permitted without license from IHS-,-,-SP-3696 (To be TINEIA-526-8) interference method and the variable threshold method of
15、 OFSTPQ have been shown to agree with each other. 1.2.1 Sinusoidal interference method: This method optically or electrically adds an interfering sinusoidal signal to the digital signal at a point before the receiver (Rx) decision circuit to increase the measured BER. The measurements taken at sever
16、al value The sinusoid can be injected into the Rx optically, by adding it to the o the sinusoid electrically requires electrical access to the circuitry of the The optical method works for an ac-coupled Rx only; the electri dc-coupled Rx. 2 Normative references asurement equipment: a BER pattern gth
17、 similar to the system under test and capable of being modulated at a in the passband of the Rx under test. This serves as an “interfering laser”. 3.1.3 An optical splitter/combiner with split ratios typically between 5050 and 1090, and with fiber compatible with that of the system and the interferi
18、ng laser. 3.1.4 An analog optical receiver capable of detecting frequencies within the passband of the system under test, used to confirm proper operation of the interfering laser. RLN, TIA SC FO-2.1,5/00 4 Copyright Telecommunications Industry Association Provided by IHS under license with EIANot f
19、or ResaleNo reproduction or networking permitted without license from IHS-,-,-STD-EIA SP NO 3676-ENGL 2000 3234600 0656526 703 118 SP-3696 (To be TINEIA-526-8) 4 Sampling and specimens The specimen is a fiber optic digital system consisting of a digital transmitter (Tx) receiver (Rx). In between the
20、m is either a fiber link consisting of fiber or cable passive or active components (if an operational link is to be tested) or a attenuator (if the Tx/k pair alone is to be tested). 5 Procedure 5.1 Refer to Figure 1. Sinusoidal Interference Method (Optical O 5.1.1 Place the combiner with one input I
21、 Connect the output port to the Rx and th modulated by the sinewave generator. Con 5.1.2 Adjust the Tx the attenuator is use the duration oft 5.1.3 Choose and not harmonicallv r( ratio or the modulation depth of the interfering laser a step at a time by adjusting the output level of the sinewave gen
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