BS EN 62150-4:2010
Current
The latest, up-to-date edition.
Fibre optic active components and devices. Test and measurement procedures Relative intensity noise using a time-domain optical detection system
Hardcopy , PDF
English
02-28-2010
INTRODUCTION
1 Scope
2 Normative references
3 Terms, definitions and abbreviations
4 Apparatus
5 Test procedure
6 Test results
Annex A (informative) - Background on laser intensity noise
Bibliography
Annex ZA (normative) - Normative references to international
publications with their corresponding European
publications
Describes test and measurement procedures for relative intensity noise (RIN).
Committee |
GEL/86/3
|
DevelopmentNote |
Supersedes 08/30179611 DC. (02/2010)
|
DocumentType |
Standard
|
Pages |
18
|
PublisherName |
British Standards Institution
|
Status |
Current
|
Supersedes |
This part of IEC 62150 specifies test and measurement procedures for relative intensity noise (RIN). It applies to lasers, laser transmitters, and the transmitter portion of transceivers. This procedure examines whether the device or module satisfies the appropriate performance specification. The procedure is applicable to single longitudinal mode (SLM). An optional section of the procedure presents a controlled return loss to the device-under-test, but is only applicable to devices coupled to SMF.
The method described in this standard, using a time-domain detection system, provides a single value for RIN that averages the noise over the transmission bandwidth. The measurement is made on a modulated laser capturing the RIN value under normal operating conditions. It also measures RINOMA, an alternative definition, as described in IEEE 802.3-2005.
An alternative RIN measurement method uses a photoreceiver and electrical spectrum analyzer and provides RIN vs. electrical frequency. This method provides a RIN value averaged over particular electrical band determined by a filter. For a filter bandwidth and characteristic that duplicates the filtering in a transmission system, this technique provides a result that is appropriate to determine the noise for such a system.
This method is based on the measurement of total intensity noise including and does attempt to subtract the effects of thermal and shot noise.
Background on laser intensity noise is given in Annex A.
Standards | Relationship |
IEC 62150-4:2009 | Identical |
EN 62150-4:2010 | Identical |
EN 62007-2:2009 | Semiconductor optoelectronic devices for fibre optic system applications - Part 2: Measuring methods |
IEEE 802.3-2012 | IEEE Standard for Ethernet |
IEC 62007-2:2009 | Semiconductor optoelectronic devices for fibre optic system applications - Part 2: Measuring methods |
EN 61280-2-2:2012/AC:2015 | FIBRE OPTIC COMMUNICATION SUBSYSTEM TEST PROCEDURES - PART 2-2: DIGITAL SYSTEMS - OPTICAL EYE PATTERN, WAVEFORM AND EXTINCTION RATIO MEASUREMENT (IEC 61280-2-2:2012) |
IEC 61300-3-6:2008 | Fibre optic interconnecting devices and passive components - Basic test and measurement procedures - Part 3-6: Examinations and measurements - Return loss |
IEC 61280-2-2:2012 | Fibre optic communication subsystem test procedures - Part 2-2: Digital systems - Optical eye pattern, waveform and extinction ratio measurement |
EN 61300-3-6:2009 | Fibre optic interconnecting devices and passive components - Basic test and measurement procedures - Part 3-6: Examinations and measurements - Return loss |
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