MapYourTech Complete Banner - Scoped CSS
Tag

EDFAs

Browsing
Fundamentals of Noise Figure in Optical Amplifiers

Noise figure (NF) is a critical parameter in optical amplifiers that quantifies the degradation of signal-to-noise ratio during amplification. In multi-span optical networks, the accumulated noise from cascaded amplifiers ultimately determines system reach, capacity, and performance.

While amplifiers provide the necessary gain to overcome fiber losses, they inevitably add amplified spontaneous emission (ASE) noise to the signal. The noise contribution from each amplifier accumulates along the transmission path, with early-stage amplifiers having the most significant impact on the end-to-end system performance.

Understanding the noise behavior in cascaded amplifier chains is fundamental to optical network design. This article explores noise figure fundamentals, calculation methods, and the cumulative effects in multi-span networks, providing practical design guidelines for optimizing system performance.

Definition and Physical Meaning

Noise figure is defined as the ratio of the input signal-to-noise ratio (SNR) to the output SNR of an amplifier, expressed in decibels (dB):

NF = 10 log₁₀(SNRin / SNRout) dB

Alternatively, it can be expressed using the noise factor F (linear scale):

NF = 10 log₁₀(F) dB

In optical amplifiers, the primary noise source is amplified spontaneous emission (ASE), which originates from spontaneous transitions in the excited gain medium. Instead of being stimulated by the input signal, these transitions occur randomly and produce photons with random phase and direction.

Noise Figure Fundamentals Optical Amplifier Clean signal SNRin Signal + ASE noise SNRout ASE generation NF = 10 log₁₀(SNRin / SNRout) dB = 10 log₁₀(1 + PASE/(G·Psignal)) dB

Quantum Limit and Physical Interpretation

Even a theoretically perfect amplifier has a quantum-limited minimum noise figure of 3dB. This fundamental limit exists because the amplification process inherently introduces at least half a photon of noise per mode.

The noise figure is related to several physical parameters:

  • Spontaneous Emission Factor (nsp): Represents the quality of population inversion in the active medium
  • Population Inversion: The ratio of atoms in excited states versus ground states
  • Quantum Efficiency: How efficiently pump power creates population inversion
NF = 2·nsp·(1-1/G)

As gain (G) becomes large, this approaches: NF = 2·nsp, with a theoretical minimum of 3dB when nsp = 1.

Factors Affecting Noise Figure

Gain and Population Inversion

The population inversion level directly affects the noise figure. Higher inversion leads to lower ASE and therefore lower noise figure. Key relationships include:

  • Gain Level: Higher gain typically results in better inversion and lower NF up to a saturation point
  • Pump Power: Increased pump power improves inversion up to a saturation level
  • Gain Medium Length: Longer gain medium increases available gain but can increase NF if inversion is not maintained throughout

Input Power Dependence

Noise figure varies with input signal power:

  • At very low input powers, the gain can be higher but the effective NF may increase due to insufficient saturation
  • At high input powers, gain saturation occurs, leading to a higher effective NF
  • The optimal input power range for lowest NF is typically 10-15dB below the saturation input power
Noise Figure vs. Input Power Input Power (dBm) -30 -20 -10 0 +10 Noise Figure (dB) 4 5 6 7 8 9 High NF region (Low input power) Optimal operating region High NF region (Gain saturation)

Wavelength Dependence

Noise figure typically varies across the operating wavelength band:

  • The wavelength dependence follows the gain spectrum of the amplifier
  • In typical optical amplifiers, NF is often lowest near the peak gain wavelength
  • Edge wavelengths generally experience higher NF due to lower inversion and gain
  • This wavelength dependence can impact system design, especially for wideband applications

Temperature Effects

Temperature significantly impacts noise figure performance:

  • Higher temperatures typically increase NF due to reduced population inversion efficiency
  • Temperature-dependent cross-sections in the gain medium affect both gain and noise performance
  • Thermal management is critical for maintaining consistent NF performance, especially in high-power amplifiers

EDFA Specifications

In optical networks, various EDFA designs are available with specific noise figure performance characteristics:

Application Typical NF Range Typical Gain Range
Metro access 6.0-7.0dB 12-21dB
Metro/regional 5.5-6.5dB 14-22dB
Regional with mid-stage access 5.5-7.5dB 15-28dB
Long-haul with mid-stage access 5.0-7.0dB 25-37dB
Regional single-stage 5.0-6.0dB 15-28dB
Long-haul single-stage 5.0-6.0dB 25-37dB
Ultra-short span booster 15.0-17.0dB 5-7dB

Temperature Sensitivity

Noise figure is temperature sensitive, with performance typically degrading at higher temperatures due to:

  • Reduced pump efficiency
  • Changes in population inversion
  • Increased thermal noise contributions

Most optical amplifiers are designed to operate in accordance with standard telecom environmental specifications like ETS 300 019-1-3 Class 3.1E for environmental endurance.

Cascaded Amplifiers and Noise Accumulation

In optical networks, signals typically pass through multiple amplifiers as they traverse through fiber spans. Understanding how noise accumulates in these multi-span systems is critical for designing networks that meet performance requirements.

Friis' Formula and Cascaded Amplifier Systems

The noise accumulation in a chain of optical amplifiers follows Friis' formula, which was originally developed for electronic amplifiers but applies equally to optical systems:

Ftotal = F1 + (F2-1)/G1 + (F3-1)/(G1·G2) + ... + (Fn-1)/(G1·G2···Gn-1)

Where:

  • Ftotal is the total noise factor (linear, not in dB)
  • Fi is the noise factor of the i-th amplifier
  • Gi is the gain (linear) of the i-th amplifier

In optical systems, this formula must account for span losses between amplifiers:

Ftotal = F1 + (L1·F2-1)/G1 + (L1·L2·F3-1)/(G1·G2) + ...

Where Li represents the span loss (linear) between amplifiers i and i+1.

Cascaded Amplifier System Amp 1 NF₁ = 5dB Span 1 Loss = 20dB Amp 2 NF₂ = 5dB Span 2 Loss = 20dB Amp 3 NF₃ = 5dB Span N Amp N NFₙ = 5dB Accumulated Noise OSNR final ≈ P launch − L span − NF − 10log 10 (N) − 58

Key Insights from Friis' Formula

The most significant insight from Friis' formula is that the first amplifier has the most substantial impact on the overall noise performance. Each subsequent amplifier's noise contribution is reduced by the gain of all preceding amplifiers.

Practical implications include:

  • Always use the lowest noise figure amplifier at the beginning of a chain
  • The impact of noise figure improvements diminishes for amplifiers later in the chain
  • Pre-amplifiers are more critical for noise performance than boosters
  • Mid-stage components (like DCFs) should have minimal loss to preserve good noise performance

OSNR Evolution in Multi-span Systems

The optical signal-to-noise ratio (OSNR) evolution through a multi-span system can be approximated by:

OSNRdB ≈ Plaunch - α·L - NF - 10·log10(N) - 10·log10(Bref) + 58

Where:

  • Plaunch is the launch power per channel (dBm)
  • α is the fiber attenuation coefficient (dB/km)
  • L is the span length (km)
  • NF is the amplifier noise figure (dB)
  • N is the number of spans
  • Bref is the reference bandwidth for OSNR measurement (typically 0.1nm)
  • 58 is a constant that accounts for physical constants (h𝜈)

The key insight from this equation is that OSNR degrades by 3dB each time the number of spans doubles (10·log10(N) term). This creates a fundamental limit to transmission distance in amplified systems.

Practical Example: OSNR Calculation in a Multi-span System

Consider a 10-span system with the following parameters:

  • Launch power: +1dBm per channel
  • Span length: 80km
  • Fiber loss: 0.2dB/km (total span loss = 16dB)
  • Amplifier gain: 16dB (exactly compensating span loss)
  • Amplifier noise figure: 5dB
  • Reference bandwidth: 0.1nm (~12.5GHz at 1550nm)

Step 1: Calculate the OSNR for a single span:

OSNR1-span = +1 - 16 - 5 - 10·log10(1) - 10·log10(12.5) + 58
= +1 - 16 - 5 - 0 - 11 + 58 = 27dB

Step 2: Calculate the OSNR degradation due to multiple spans:

OSNR degradation = 10·log10(N) = 10·log10(10) = 10dB

Step 3: Calculate the final OSNR:

OSNR10-spans = OSNR1-span - 10·log10(N) = 27 - 10 = 17dB

With a typical OSNR requirement of 12-15dB for modern coherent transmission formats, this system has adequate margin for reliable operation. However, extending to 20 spans would reduce OSNR by another 3dB to 14dB, approaching the limit for reliable operation.

Multi-Stage Amplifier Design

Based on the principles of Friis' formula, multi-stage amplifiers with optimal noise performance typically follow a design where:

Multi-Stage Amplifier Design Optimal Design Low NF Pre-Amp Power Amp Component NF = 4.5dB G = 15dB Loss = 1dB NF = 6.5dB G = 15dB Impact if First Stage NF = 6.5dB: Overall NF increases by ~2dB Impact if Second Stage NF = 8.5dB: Overall NF increases by only ~0.2dB

Key design principles include:

  • Low-Noise First Stage: The first stage should be optimized for low noise figure, even at the expense of output power capability
  • Power-Optimized Second Stage: The second stage can focus on power handling and efficiency once the SNR has been established by the first stage
  • Minimal Mid-Stage Loss: Any passive components (filters, isolators, etc.) between stages should have minimal insertion loss to avoid degrading the noise performance

EDFA Models and Cascaded Performance

Various types of optical amplifiers are designed with cascaded performance in mind:

Type Mid-Stage Features Design Optimization
Variable gain with mid-stage access Mid-stage access for DCF Optimized for regional networks
High-gain variable gain with mid-stage access Mid-stage access for DCF Optimized for high-gain applications
Variable gain with mid-stage access
and C/T filters
Mid-stage access for DCF Optimized for high-power applications
with OSC handling

Typical mid-stage dispersion compensation fiber (DCF) parameters tracked in optical networks include dispersion value, PMD, and tilt, which are critical for maintaining overall system performance.

Automatic Laser Shutdown (ALS) and Safety

In high-power multi-span systems, safety mechanisms like Automatic Laser Shutdown (ALS) are implemented to prevent hazardous conditions during fiber breaks or disconnections:

  • ALS triggers when LOS (Loss Of Signal) is detected on a line port
  • During ALS, EDFAs are disabled except for periodic 30-second probing intervals at reduced power (20dBm)
  • Normal operation resumes only after signal restoration for at least 40 seconds

Modern optical amplifiers feature ALS functionality with configurable parameters to ensure both optimal performance and safety in cascaded environments.

Network Applications and Optimization Strategies for Optical Amplifiers

Different segments of optical networks have varying requirements for noise figure performance based on their application, reach requirements, and economic considerations.

Network Segment Requirements

Noise Figure Requirements by Network Segment Access Short reach High splitting loss Metro/Regional Medium reach Mixed node types Long-haul Extended reach Many cascaded amps Typical NF Req: 6-7 dB (Less critical) Typical NF Req: 5-6 dB (Balanced design) Typical NF Req: 4-5 dB (Highly critical) Design Focus: • Cost efficiency • Size/integration Design Focus: • Flexibility • Dynamic range Design Focus: • Minimal NF • Optimized cascade

Access Networks

Access networks are generally tolerant of higher noise figures (6-7dB) because:

  • They involve fewer amplifiers in cascade
  • They often operate with higher channel powers
  • Transmission distances are relatively short
  • Cost sensitivity is higher than performance optimization

Metro/Regional Networks

Metro and regional networks require balanced NF performance (5-6dB) with:

  • Good dynamic range to handle varying traffic patterns
  • Flexibility to support different node configurations
  • Moderate reach capabilities (typically 4-10 spans)
  • Reasonable cost-performance trade-offs

Long-haul Networks

Long-haul and submarine networks demand optimized low-NF designs (4-5dB) due to:

  • Large number of amplifiers in cascade (often 10-20+)
  • Need to maximize reach without electrical regeneration
  • Requirement to support advanced modulation formats
  • Justification for premium components due to overall system economics

Economic Implications of Noise Figure

Improving noise figure comes with cost implications that must be carefully evaluated:

NF Improvement Typical Cost Increase Performance Benefit Economic Justification
6.0dB → 5.5dB +5-10% ~10% reach increase Generally cost-effective
5.5dB → 5.0dB +10-15% ~10% reach increase Often justified for long-haul
5.0dB → 4.5dB +15-25% ~10% reach increase Specialty applications only
4.5dB → 4.0dB +30-50% ~10% reach increase Rarely justified economically

The economic tradeoffs include:

  • Capital vs. Operating Expenses: Higher-quality, lower-NF amplifiers cost more initially but may reduce the need for additional amplifier sites and regeneration points
  • Upgrade Paths: Better NF provides margin for future capacity upgrades with more advanced modulation formats
  • Lifecycle Considerations: Premium amplifiers may maintain better performance over their operational lifetime, delaying replacement needs
  • System Capacity: Improved NF can enable higher capacity through better OSNR margin, often at lower cost than adding new fiber routes

Operational Optimization Strategies

For system operators using EDFAs, several practical optimization strategies can help maximize performance:

1. Gain Optimization

Modern optical amplifiers support different operation modes with specific gain management approaches:

  • Automatic Mode: Maintains output power per channel based on saturation power and maximum channel count settings
  • Semi-automatic Mode: Maintains a fixed output power per channel
  • Constant Gain Mode: Maintains a fixed gain regardless of input power variations
  • Automatic Power Control (APC) Mode: Provides automatic power control for specialized applications
  • Automatic Current Control (ACC) Mode: Provides precise pump current control for specialized applications

Advanced amplifiers implement specific algorithms for gain control that include careful monitoring of required gain versus actual gain, with alarms for out-of-range or out-of-margin conditions.

2. Tilt Management

Spectral tilt management is crucial for maintaining consistent OSNR across all channels:

  • Modern EDFAs automatically adjust tilt to compensate for fiber and component tilt
  • SRS (Stimulated Raman Scattering) tilt compensation is included for high-power systems
  • Built-in tilt values are stored in amplifier memory and used as reference points
  • For ultra-short span boosters and extended C-band amplifiers, specialized tilt algorithms account for fiber type

3. Temperature Control

Optical amplifiers typically specify operational temperature ranges in accordance with telecom standards like ETS 300 019-1-3 Class 3.1E, emphasizing the importance of controlling environmental conditions to maintain optimal performance.

4. Fiber Plant Optimization

Several fiber plant parameters impact noise figure performance:

  • Span Loss: Monitored and alarmed when outside expected range
  • Mid-stage Loss: For dual-stage amplifiers, carefully managed for optimal performance
  • Transmission Fiber Type: Configuration option that affects SRS tilt compensation
  • DCF Parameters: Dispersion, PMD, and tilt tracked in network control protocols

Noise Figure Design Guidelines

  1. Place Highest Quality First: Always use the lowest noise figure amplifiers at the beginning of the chain where they have the most impact
  2. Budget Wisely: Budget 0.5-1.0dB extra margin for each amplifier to account for aging and temperature variations over the system lifetime
  3. Consider Total Cost: Evaluate the total cost impact of NF improvements, including reduced regeneration needs and extended reach capabilities
  4. Monitor Trends: Establish baseline NF measurements and monitor for gradual degradation that might indicate pump laser aging
  5. Balance Requirements: Balance NF with other parameters like output power, gain flatness, and dynamic range based on specific application needs
  6. Test Under Load: Validate NF performance under realistic channel loading conditions, not just with a single test wavelength

Future Trends in Noise Figure Technology

Future Trends in Noise Figure Technology AI-Optimized Amplifiers Machine Learning Parameter Optimization Advanced Materials Novel Dopants & Co-dopants Engineered Glass Structures Integrated Photonics On-Chip Amplification Hybrid Integration Quantum Approaches Quantum-Enhanced Amplification Phase-Sensitive Designs

Emerging technologies for noise figure optimization include:

  • AI-Driven Optimization: Machine learning algorithms that dynamically adjust amplifier parameters based on real-time network conditions
  • Advanced Material Science: New dopant materials and glass compositions that enable better population inversion and reduced spontaneous emission
  • Integrated Photonics: Silicon photonics and other integrated platforms that combine amplification with filtering and control functions
  • Quantum-Enhanced Amplification: Phase-sensitive amplification and other quantum approaches that can theoretically break the 3dB quantum noise limit
  • Distributed Intelligence: Network-wide optimization that coordinates multiple amplifiers for global noise minimization

EDFA Implementation Examples

Metro Network Design

A typical metro network implementation might include:

  • Terminal nodes using fixed-gain boosters and pre-amplifiers
  • FOADM nodes using low-gain pre-amplifiers
  • Flexible OADM nodes employing medium-gain boosters

Regional Network Design

For regional networks, typical designs include:

  • Terminal nodes with AWG Mux/DeMux and EDFAs for amplification
  • Modern terminals with WSS for automatic equalization
  • ROADM nodes employing pre-amplifiers with mid-stage access for DCF compensation and boosters
  • In-line amplifier nodes (ILAN) using EDFAs to compensate for transmission fiber and DCF loss

Specialized Applications

Some specialized EDFA designs address unique requirements:

  • Ultra-short span boosters: Very high output power (26dBm) with narrow gain range (5-7dB)
  • High-power pre-amps: For ROADM applications with specialized eye-safety verification process
  • Pluggable EDFAs: For applications requiring compact, modular amplification in form factors like CFP2

Conclusion

Noise figure is a fundamental parameter that sets ultimate performance limits for optical amplifier systems. Modern EDFA families demonstrate a comprehensive approach to addressing various network requirements with optimized designs for different applications.

Key takeaways include:

  • Noise figure quantifies an amplifier's SNR degradation, with a quantum-limited minimum of 3dB
  • In cascaded configurations, noise accumulates according to Friis' formula, with early-stage amplifiers having the most significant impact
  • Network operators can optimize NF through proper pump power settings, gain optimization, temperature control, and careful wavelength planning
  • Multi-stage designs with low-NF first stages offer the best overall performance for critical applications
  • Economic considerations must balance the additional cost of lower-NF amplifiers against improved system reach and capacity

The evolution of EDFA technology reflects the ongoing refinement of noise figure optimization techniques, with newer designs and features continually addressing the evolving requirements of optical networks.

In the world of fiber-optic communication, the integrity of the transmitted signal is critical. As an optical engineers, our primary objective is to mitigate the attenuation of signals across long distances, ensuring that data arrives at its destination with minimal loss and distortion. In this article we will discuss into the challenges of linear and nonlinear degradations in fiber-optic systems, with a focus on transoceanic length systems, and offers strategies for optimising system performance.

The Role of Optical Amplifiers

Erbium-doped fiber amplifiers (EDFAs) are the cornerstone of long-distance fiber-optic transmission, providing essential gain within the low-loss window around 1550 nm. Positioned typically between 50 to 100 km apart, these amplifiers are critical for compensating the fiber’s inherent attenuation. Despite their crucial role, EDFAs introduce additional noise, progressively degrading the optical signal-to-noise ratio (OSNR) along the transmission line. This degradation necessitates a careful balance between signal amplification and noise management to maintain transmission quality.

OSNR: The Critical Metric

The received OSNR, a key metric for assessing channel performance, is influenced by several factors, including the channel’s fiber launch power, span loss, and the noise figure (NF) of the EDFA. The relationship is outlined as follows:

osnrformula

Where:

  • is the number of EDFAs the signal has passed through.
  •  is the power of the signal when it’s first sent into the fiber, in dBm.
  • Loss represents the total loss the signal experiences, in dB.
  • NF is the noise figure of the EDFA, also in dB.

Increasing the launch power enhances the OSNR linearly; however, this is constrained by the onset of fiber nonlinearity, particularly Kerr effects, which limit the maximum effective launch power.

The Kerr Effect and Its Implications

The Kerr effect, stemming from the intensity-dependent refractive index of optical fiber, leads to modulation in the fiber’s refractive index and subsequent optical phase changes. Despite the Kerr coefficient () being exceedingly small, the combined effect of long transmission distances, high total power from EDFAs, and the small effective area of standard single-mode fiber (SMF) renders this nonlinearity a dominant factor in signal degradation over transoceanic distances.

The phase change induced by this effect depends on a few key factors:

  • The fiber’s nonlinear coefficient .
  • The signal power , which varies over time.
  • The transmission distance.
  • The fiber’s effective area .

kerr

This phase modulation complicates the accurate recovery of the transmitted optical field, thus limiting the achievable performance of undersea fiber-optic transmission systems.

The Kerr effect is a bit like trying to talk to someone at a party where the music volume keeps changing. Sometimes your message gets through loud and clear, and other times it’s garbled by the fluctuations. In fiber optics, managing these fluctuations is crucial for maintaining signal integrity over long distances.

Striking the Right Balance

Understanding and mitigating the effects of both linear and nonlinear degradations are critical for optimising the performance of undersea fiber-optic transmission systems. Engineers must navigate the delicate balance between maximizing OSNR for enhanced signal quality and minimising the impact of nonlinear distortions.The trick, then, is to find that sweet spot where our OSNR is high enough to ensure quality transmission but not so high that we’re deep into the realm of diminishing returns due to nonlinear degradation. Strategies such as carefully managing launch power, employing advanced modulation formats, and leveraging digital signal processing techniques are vital for overcoming these challenges.

 

When we talk about the internet and data, what often comes to mind are the speeds and how quickly we can download or upload content. But behind the scenes, it’s a game of efficiently packing data signals onto light waves traveling through optical fibers.If you’re an aspiring telecommunications professional or a student diving into the world of fiber optics, understanding the allocation of spectral bands is crucial. It’s like knowing the different climates in a world map of data transmission. Let’s explore the significance of these bands as defined by ITU-T recommendations and what they mean for fiber systems.

#opticalband

The Role of Spectral Bands in Single-Mode Fiber Systems

Original O-Band (1260 – 1360 nm): The journey of fiber optics began with the O-band, chosen for ITU T G.652 fibers due to its favorable dispersion characteristics and alignment with the cut-off wavelength of the cable. This band laid the groundwork for optical transmission without the need for amplifiers, making it a cornerstone in the early days of passive optical networks.

Extended E-Band (1360 – 1460 nm): With advancements, the E-band emerged to accommodate the wavelength drift of uncooled lasers. This extended range allowed for greater flexibility in transmissions, akin to broadening the canvas on which network artists could paint their data streams.

Short Wavelength S-Band (1460 – 1530 nm): The S-band, filling the gap between the E and C bands, has historically been underused for data transmission. However, it plays a crucial role in supporting the network infrastructure by housing pump lasers and supervisory channels, making it the unsung hero of the optical spectrum.

Conventional C-Band (1530 – 1565 nm): The beloved C-band owes its popularity to the era of erbium-doped fiber amplifiers (EDFAs), which provided the necessary gain for dense wavelength division multiplexing (DWDM) systems. It’s the bread and butter of the industry, enabling vast data capacity and robust long-haul transmissions.

Long Wavelength L-Band (1565 – 1625 nm): As we seek to expand our data highways, the L-band has become increasingly important. With fiber performance improving over a range of temperatures, this band offers a wider wavelength range for signal transmission, potentially doubling the capacity when combined with the C-band.

Ultra-Long Wavelength U-Band (1625 – 1675 nm): The U-band is designated mainly for maintenance purposes and is not currently intended for transmitting traffic-bearing signals. This band ensures the network’s longevity and integrity, providing a dedicated spectrum for testing and monitoring without disturbing active data channels.

Historical Context and Technological Progress

It’s fascinating to explore why we have bands at all. The ITU G-series documents paint a rich history of fiber deployment, tracing the evolution from the first multimode fibers to the sophisticated single-mode fibers we use today.

In the late 1970s, multimode fibers were limited by both high attenuation at the 850 nm wavelength and modal dispersion. A leap to 1300 nm in the early 1980s marked a significant drop in attenuation and the advent of single-mode fibers. By the late 1980s, single-mode fibers were achieving commercial transmission rates of up to 1.7 Gb/s, a stark contrast to the multimode fibers of the past.

The designation of bands was a natural progression as single-mode fibers were designed with specific cutoff wavelengths to avoid modal dispersion and to capitalize on the low attenuation properties of the fiber.

The Future Beckons

With the ITU T G.65x series recommendations setting the stage, we anticipate future applications utilizing the full spectrum from 1260 nm to 1625 nm. This evolution, coupled with the development of new amplification technologies like thulium-doped amplifiers or Raman amplification, suggests that the S-band could soon be as important as the C and L bands.

Imagine a future where the combination of S+C+L bands could triple the capacity of our fiber infrastructure. This isn’t just a dream; it’s a realistic projection of where the industry is headed.

Conclusion

The spectral bands in fiber optics are not just arbitrary divisions; they’re the result of decades of research, development, and innovation. As we look to the horizon, the possibilities are as wide as the spectrum itself, promising to keep pace with our ever-growing data needs.

Reference

https://www.itu.int/rec/T-REC-G/e

The main advantages and drawbacks of EDFAs are as follows.

Advantages

  • Commercially available in C band (1,530 to 1,565 nm) and L band (1,560 to 1,605) and up to  84-nm range at the laboratory stage.
  • Excellent coupling: The amplifier medium is an SM fiber;
  • Insensitivity to light polarization state;
  • Low sensitivity to temperature;
  • High gain: > 30 dB with gain flatness < ±0.8 dB and < ±0.5 dB in C and L band, respectively, in the scientific literature and in the manufacturer documentation
  • Low noise figure: 4.5 to 6 dB
  • No distortion at high bit rates;
  • Simultaneous amplification of wavelength division multiplexed signals;
  • Immunity to crosstalk among wavelength multiplexed channels (to a large extent)

Drawbacks

  • Pump laser necessary;
  • Difficult to integrate with other components;
  • Need to use a gain equalizer for multistage amplification;
  • Dropping channels can give rise to errors in surviving channels:dynamic control of amplifiers is  necessary.

A short discussion on 980nm and 1480nm pump based EDFA

Introduction

The 980nm pump needs three energy level for radiation while 1480nm pumps can excite the ions directly to the metastable level .edfa

(a) Energy level scheme of ground and first two excited states of Er ions in a silica matrix. The sublevel splitting and the lengths of arrows representing absorption and emission transitions are not drawn to scale. In the case of the 4 I11/2 state, s is the lifetime for nonradiative decay to the I13/2 first excited state and ssp is the spontaneous lifetime of the 4 I13/2 first excited state. (b) Absorption coefficient, a, and emission coefficient, g*, spectra for a typical aluminum co-doped EDF.

The most important feature of the level scheme is that the transition energy between the I15/2 ground state and the I13/2 first excited state corresponds to photon wavelengths (approximately 1530 to 1560 nm) for which the attenuation in silica fibers is lowest. Amplification is achieved by creating an inversion by pumping atoms into the first excited state, typically using either 980 nm or 1480 nm diode lasers. Because of the superior noise figure they provide and their superior wall plug efficiency, most EDFAs are built using 980 nm pump diodes. 1480 nm pump diodes are still often used in L-band EDFAs although here, too, 980 nm pumps are becoming more widely used.

Though pumping with 1480 nm is used and has an optical power conversion efficiency which is higher than that for 980 nm pumping, the latter is preferred because of the following advantages it has over 1480 nm pumping.

  • It provides a wider separation between the laser wavelength and pump wavelength.
  • 980 nm pumping gives less noise than 1480nm.
  • Unlike 1480 nm pumping, 980 nm pumping cannot stimulate back transition to the ground state.
  • 980 nm pumping also gives a higher signal gain, the maximum gain coefficient being 11 dB/mW against 6.3 dB/mW for the 1.48
  • The reason for better performance of 980 nm pumping over the 1.48 m pumping is related to the fact that the former has a narrower absorption spectrum.
  • The inversion factor almost becomes 1 in case of 980 nm pumping whereas for 1480 nm pumping the best one gets is about 1.6.
  • Quantum mechanics puts a lower limit of 3 dB to the optical noise figure at high optical gain. 980 nm pimping provides a value of 3.1 dB, close to the quantum limit whereas 1.48  pumping gives a value of 4.2 dB.
  • 1480nm pump needs more electrical power compare to 980nm.

Application

The 980 nm pumps EDFA’s are widely used in terrestrial systems while 1480nm pumps are used as Remote Optically Pumped Amplifiers (ROPA) in subsea links where it is difficult to put amplifiers.For submarine systems, remote pumping can be used in order not to have to electrically feed the amplifiers and remove electronic parts.Nowadays ,this is used in pumping up to 200km.

The erbium-doped fiber can be activated by a pump wavelength of 980 or 1480 nm but only the second one is used in repeaterless systems due to the lower fiber loss at 1.48 mm with respect to the loss at 0.98 mm. This allows the distance between the terminal and the remote amplifier to be increased.

In a typical configuration, the ROPA is comprised of a simple short length of erbium doped fiber in the transmission line placed a few tens of kilometers before a shore terminal or a conventional in-line EDFA. The remote EDF is backward pumped by a 1480 nm laser, from the terminal or in-line EDFA, thus providing signal gain

Vendors

Following are the vendors that manufactures 980nm and 1480nm EDFAs