33.180.30 光纤放大器 标准查询与下载

DIN EN 62148-15:2015 光纤有源元件及器件.封装和接口标准.第15部分:离散垂直型控表面发射激光封装(IEC 62148-15-2014).德文版本EN 62148-15-2014

Fibre optic active components and devices - Package and interface standards - Part 15: Discrete vertical cavity surface emitting laser packages (IEC 62148-15:2014); German version EN 62148-15:2014

BS EN 61290-1:2015 光学放大器 试验方法 功率和增益参数

Optical amplifiers. Test methods. Power and gain parameters

EN 61290-1:2015 光放大器 测试方法 第1部分：功率和增益参数

IEC 61290-1:2014 applies to all commercially available optical amplifiers (OAs) and optically amplified subsystems. It applies to OAs using optically pumped fibres (OFAs based on either rare-earth doped fibres or on the Raman effect), semiconductors (SOAs), and waveguides (POWAs). The object of this standard is to establish uniform requirements for accurate and reliable measurements of the following OA parameters, as defined in Clause 3 of IEC 61291-1:2012: - nominal output signal power; - gain; - reverse gain; - maximum gain; - maximum gain wavelength; - maximum gain variation with temperature; - gain wavelength band; - gain wavelength variation; - gain stability; - polarization-dependent gain; - large-signal output stability; - saturation output power; - maximum output signal power; - maximum total output power. The object of this standard is specifically directed to single-channel amplifiers. For multichannel amplifiers, one should refer to the IEC 61290-10 series. Keywords: optical amplifiers (OAs), optically pumped fibres (OFAs), semiconductors (SOAs), and waveguides (POWAs)

Optical amplifiers - Test methods - Part 1: Power and gain parameters

IEC 61290-1-3:2015 光学放大器.试验方法.第1-3部分:光功率参数和增益参数.光功率计法

Optical amplifiers - Test methods - Part 1-3: Power and gain parameters - Optical power meter method

DIN EN 62149-9:2015 纤维光学有源元件和器件. 性能标准. 第9部分: 晶种反射半导体光放大器收发器 (IEC 62149-9-2014); 德文版本EN 62149-9-2014

Fibre optic active components and devices - Performance standards - Part 9: Seeded reflective semiconductor optical amplifier transceivers (IEC 62149-9:2014); German version EN 62149-9:2014

GSO IEC 61290-11-1:2014 光放大器 测试方法 第11-1部分：偏振模式色散参数 琼斯矩阵自动分析 (JME)

This part of IEC 61290 applies to all commercially available optical amplifiers (OAs), including optical fibre amplifiers (OFAs) using active fibres, semiconductor optical amplifiers (SOAs), and planar waveguide optical amplifiers (PWOAs). 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). Other information about PMD may be found in IEC 61282-9 in general and in IEC 61292-5 on OAs in particular. This test method describes a procedure for measuring the PMD of OAs. The measurement result is obtained from the measurement of the normalized Stokes parameters at two closely spaced wavelengths. The test method described herein requires a polarized signal at the input of the polarimeter with a degree of polarization (DOP) of at least 25 %. Although the test source is highly polarized, the DOP at the output of the OA is reduced by amplified spontaneous emission (ASE). Annex A analyses the impact of ASE on the DOP. In order to assure an accurate measurement, the DOP is measured as part of the measurement procedure. 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 Jones matrix eigenanalysis (JME) test method is in principle also applicable to unpumped (that is, unpowered) OAs, the JME technique in this standard applies to pumped (that is, powered) OAs only.

Optical amplifiers - Test methods - Part 11-1: Polarization mode dispersion parameter - Jones matrix eigenanalysis (JME)

GSO IEC 61290-4-2:2014 光放大器 测试方法 第4-2部分：传输增益系数 宽带源方法

This part of IEC 61290-4 applies to optical amplifiers (OAs) and optically amplified elementary sub-systems. More specifically, it applies to OAs using active fibres (optical fibre amplifiers, OFAs) containing rare-earth dopants, such as erbium doped fibre amplifiers (EDFAs), presently commercially available, as indicated in IEC 61291-1. The object of this part of IEC 61290-4 is to establish uniform requirements for accurate and reliable measurements, by means of the broadband source method, of the transient response of OFAs to dynamic changes in their input power, as defined in IEC 61290-4-1:2011. The broadband source method is different from the two-wavelength method described in IEC 61290-4-1:– in that the saturating signal is not located at a single wavelength, but is rather spread out across the entire specified DWDM transmission band of the OFA-under-test (e.g. the C-Band, 1 525 nm to 1 565 nm). Thus, this method may be relevant to the characterization of transient events where the DWDM signals that are added or dropped are more or less uniformly spread across the transmission band. The difference between the two measurement methods is discussed in more detail in Annex A.

Optical amplifiers - Test methods - Part 4-2: Gain transient parameters - Broadband source method

GSO IEC 61290-11-2:2014 光放大器测试方法 第11-2部分：偏振模色散参数庞加莱球分析方法

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.

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

GSO IEC 61290-10-2:2014 光放大器 测试方法 第10-2部分：多通道参数 使用门控分光光度计的脉冲法

This part of IEC 61290 applies to optical fibre amplifiers (OFA) using active fibres, containing rare-earth dopants, currently commercially available. The object of this International Standard is to establish uniform requirements for accurate and reliable measurements of the signal-spontaneous noise figure as defined in IEC 61291-1. The test method independently detects amplified signal power and amplified spontaneous emission (ASE) power by launching optical pulses into the OFA under test. The ASE level is measured by synchronously measuring the power on an optical spectrum analyzer (OSA) during the optical pulse off period. The average optical signal level is measured by random sampling in the OSA. Such measurement is possible because the gain response of the rare-earth doped OFA is relatively slow, particularly in Er-doped OFA. However, since the OFA gain dynamics vary with amplifier types, operating conditions, and control schemes, the gain dynamics should be carefully considered when applying the present test method to various OFA. The manufacturer of the OFA should present data validating the required modulation frequency to limit the error to

Optical amplifiers - Test methods - Part 10-2: Multichannel parameters - Pulse method using a gated optical spectrum analyzer

GSO IEC 61290-6-1:2014 光纤放大器基本规范 第6-1部分：泵浦泄漏参数的测试方法光信号分路器

This part of IEC 61290 applies to optical fibre amplifiers (OFAs) using active fibres, containing rare-earth dopants, presently commercially available. The object of this standard is to establish uniform requirements for accurate and reliable measurements, by means of the optical demultiplexer test method, of the following OFA parameters, as defined in clause 3 of IEC 61291-1: a) pump leakage to output; b) pump leakage to input. NOTE – All numerical values followed by (‡) are currently under consideration.

Optical fibre amplifiers - Basic specification - Part 6-1: Test methods for pump leakage parameters - Optical demultiplexer

GSO IEC 61290-3-1:2014 光放大器 测试方法 第3-1部分：噪声形状参数 光谱分析仪方法

This part of IEC 61290 applies to commercially available optical amplifiers (OAs) such as optical fibre amplifiers (OFAs), semiconductor optical amplifiers (SOAs) and planar waveguide amplifiers (PWOAs) as classified in IEC 61292-3. The object of this standard is to establish uniform requirements for accurate and reliable measurements, by means of the optical spectrum analyzer (OSA) test method, of the following OA parameters, as defined in IEC 61291-1: a) signal-spontaneous noise figure; b) forward amplified spontaneous emission (ASE) power level. The methods described in this part of IEC 61290 apply to single-channel stimulus only. Two alternatives for determining the signal-spontaneous beat noise are possible, namely the ASE direct interpolation technique (DI) and the polarization nulling with interpolation technique (PN). The accuracy of the DI technique will suffer when the slope of the OA spectral ASE curve has large wavelength dependence, as in the case of an OA with an internal narrowband ASE suppressing filter. The accuracy of the DI technique degrades at high input power level due to the spontaneous emission from the laser source(s). Annex A provides guidance on the limits of this technique for high input power. NOTE 1 All numerical values marked with (‡) are suggested values for which the measurement is assured. Other values may be acceptable but should be verified. NOTE 2 General aspects of noise figure test methods are reported in IEC 61290-3.

Optical amplifiers - Test methods - Part 3-1: Noise figure parameters - Optical spectrum analyzer method

GSO IEC 61290-4-1:2014 光放大器 测试方法 第4-1部分：传输增益系数 双波长方法

This part of IEC 61290-4 applies to erbium-doped fibre amplifiers (EDFAs) and optically amplified elementary sub-systems. It applies to OAs using active fibres (optical fibre amplifiers, OFAs), containing rare-earth dopants. These amplifiers are commercially available and widely deployed in service provider networks. The object of this part of IEC 61290-4 is to provide the general background for EDFA transients and related parameters, and to describe a standard test method for accurate and reliable measurement of the following transient parameters: • Channel addition/removal transient gain overshoot and transient net gain overshoot • Channel addition/removal transient gain undershoot and transient net gain undershoot • Channel addition/removal gain offset • Channel addition/removal transient gain response time constant (settling time)

Optical amplifiers - Test methods - Part 4-1: Gain transient parameters - Two-wavelength method

GSO IEC 62148-4:2014 有源光纤器件和组件 包装和适配器的标准规范 第4部分：PN 1x9 塑料光纤收发器

This part of IEC 62148 covers the physical interface specifications for the PN 1x9 transceiver family for plastic optical fibre.

Fibre optic active components and devices - Package and interface standards - Part 4: PN 1x9 plastic optical fibre transceivers

GSO IEC 61291-1:2014 光放大器 第1部分：通用规范

This part of IEC 61291 applies to all commercially available optical amplifiers (OAs) and optically amplified assemblies. It applies to OAs using optically pumped fibres (OFAs based either on rare-earth doped fibres or on the Raman effect), semiconductors (SOAs), and waveguides (POWAs). The object of this standard is: – to establish uniform requirements for transmission, operation, reliability and environmental properties of OAs; – to provide assistance to the purchaser in the selection of consistently high-quality OA products for his particular applications. Parameters specified for OAs are those characterizing the transmission, operation, reliability and environmental properties of the OA seen as a “black box” from a general point of view. In the sectional and detail specifications a subset of these parameters will be specified according to the type and application of the particular OA device or assembly.

Optical amplifiers - Part 1: Generic specification

GSO IEC 61290-10-1:2014 光放大器 测试方法 第10-1部分：多通道参数 使用光开关和光谱分析仪的脉冲方法

This part of IEC 61290 applies to optical amplifiers (OAs) using active fibres and waveguides, containing rare-earth dopants, currently commercially available. The object of this standard is to establish uniform requirements for accurate and reliable measurements of the signal-spontaneous noise figure as defined in IEC 61291-1. The test method independently detects amplified signal power and amplified spontaneous emission (ASE) power by launching optical pulses into the OA under test and synchronously detecting "on" and "off" levels of the output pulses by using an optical sampling switch and an optical spectrum analyzer (OSA). Such measurement is possible because the gain response of the rare-earth doped OA is relatively slow, particularly in Er-doped OAs. However, since the OA gain dynamics vary with amplifier types, operating conditions and control schemes, the gain dynamics should be carefully considered when applying the present test method to various OA. The manufacturer of the OA should present data validating the required modulation frequency to limit the error to

Optical amplifiers - Test methods - Part 10-1: Multichannel parameters - Pulse method using an optical switch and optical spectrum analyzer

GSO IEC 61290-5-1:2014 光放大器 测试方法 第5-1部分：反射率参数 光谱仪方法

This part of IEC 61290 applies to all commercially available optical amplifiers (OAs) and optically amplified sub-systems. It applies to OAs using optically pumped fibres (OFAs based on either rare-earth doped fibres or on the Raman effect), semiconductor OAs (SOAs), and waveguides (POWAs)

Optical amplifiers - Test methods - Part 5-1: Reflectance parameters - Optical spectrum analyzer method

GSO IEC 61290-7-1:2014 光放大器 测试方法 第7-1部分：带外插入损耗 滤波光功率计方法

This part of IEC 61290 applies to optical amplifiers (OAs) using active fibres presently commercially available containing rare-earth dopants. The object of this standard is to establish uniform requirements for accurate and reliable measurements, by means of the filtered optical power meter test method, of the following OA parameters, as defined in IEC 61291-1: a) out-of-band insertion loss; b) out-of-band reverse insertion loss. NOTE 1 The out-of-band insertion loss of an OA is highly dependent on the amplifier configuration and the out-ofband wavelength. NOTE 2 All numerical values followed by (‡) are suggested values.

Optical amplifiers - Test methods - Part 7-1: Out-of-band insertion losses - Filtered optical power meter method

GSO IEC 62129-2:2014 波长/光频率计的校准 第2部分：单波长米歇尔森干涉仪

This part of IEC 62129 is applicable to instruments measuring the vacuum wavelength or optical frequency emitted from sources that are typical for the fibre-optic communications industry. These sources include Distributed Feedback (DFB) laser diodes, External Cavity lasers and single longitudinal mode fibre-type sources. It is assumed that the optical radiation will be coupled to the wavelength meter by a single-mode optical fibre. The standard describes the calibration of wavelength meters to be performed by calibration laboratories or by wavelength meter manufacturers. This standard is part of the IEC 62129 series on the calibration of wavelength/optical frequency measurement instruments. Refer to IEC 62129 for the calibration of optical spectrum analyzers.

Calibration of wavelength/optical frequency measurement instruments - Part 2: Michelson interferometer single wavelength meters

GSO IEC 61290-3:2014 光纤放大器基本规范 第3部分：噪声轮廓参数的测试方法

This International Standard applies to all commercially available optical amplifiers (OAs), including OAs using optically pumped fibres (OFAs based on either rare-earth doped fibres or on the Raman effect), semiconductor optical amplifiers (SOAs) and planar waveguide optical amplifiers (PWOAs). The object of this standard is to provide the general background for OA noise figure parameters measurements and to indicate those IEC standard test methods for accurate and reliable measurements of the following OA parameters, as defined in IEC 61291-1: a) noise figure (NF); b) noise factor (F); c) multiple path interference (MPI) figure of merit; d) signal-spontaneous noise figure; e) (equivalent) spontaneous-spontaneous optical bandwidth (Bsp-sp); f) forward amplified spontaneous emission (ASE) power level; g) reverse ASE power level; h) ASE bandwidth. This standard addresses measurement of OAs that are to be used for amplifying single channels, that is signals from a single transmitter. Testing of OAs for multichannel use involves additional considerations, such as: the number, wavelengths and relative power of the signals, the ability to measure signals simultaneously and to measure the ASE between channels. NOTE Methods for measurement of OAs for multichannel use are included in the IEC 61290-10 series.

Optical amplifiers - Test methods - Part 3: Noise figure parameters

GSO IEC 61290-5-2:2014 光放大器 测试方法 第5-2部分：反射率参数 电谱分析仪方法

This part of IEC 61290 applies to optical fibre amplifiers (OFAs) using active fibres, containing rare-earth dopants, presently commercially available. The object of this part of IEC 61290 is to establish uniform requirements for accurate and reliable measurements, by means of the electrical spectrum analyser test method, of the following OFA parameters, as defined in IEC 61291-1: a) input reflectance; b) output reflectance. NOTE 1 All numerical values followed by (‡) are currently under study. NOTE 2 The measurement uncertainty should be better than ±1 dB.

Optical amplifiers - Test methods - Part 5-2: Reflectance parameters - Electrical spectrum analyser method