Methods to Calculate OSNR for Optical Communications

Table of Contents

1. Introduction to OSNR in Optical Communications

Optical Signal-to-Noise Ratio (OSNR) is a critical parameter in optical communication systems that directly impacts the system's performance and bit error rate (BER). In C+L band networks where signals are transmitted across both the C-Band (1530-1570nm) and L-Band (1570-1610nm) spectral ranges, calculating OSNR requires specialized methods that account for the unique characteristics of each band and their interactions.

Typical OSNR vs. Transmission Distance

The document outlines several key aspects of OSNR calculation for optical networks, with particular emphasis on C+L band networks. These calculations must account for various factors including:

2. Basic OSNR Calculation Methods

2.1 Fundamental Equations

OSNR is fundamentally the ratio of signal power to noise power, typically measured in a standard reference bandwidth (often 0.1nm or 12.5GHz). For optical systems, several standard equations are used to calculate OSNR.

Basic OSNR Definition:
OSNR = Psignal / Pnoise (linear scale)
OSNR(dB) = 10 × log10(Psignal / Pnoise)

Where:

  • Psignal is the optical signal power
  • Pnoise is the noise power in the reference bandwidth
OSNR for a chain of amplifiers:
1/OSNRtotal = 1/OSNR1 + 1/OSNR2 + ... + 1/OSNRn

This formula shows how OSNR accumulates through a cascade of amplifiers in an optical transmission system.

OSNR from ASE Noise:
OSNR = Psignal / (N × h × v × Δf × G)

Where:

  • N is the spontaneous emission factor (typically 1-2)
  • h is Planck's constant
  • v is the optical frequency
  • Δf is the reference bandwidth
  • G is the amplifier gain

2.2 Fiber Span OSNR

In optical networks, the OSNR for a fiber span considers the relationship between the input power, fiber loss, and amplifier characteristics.

Fiber Span Diagram

From the document, we can see that the fiber span OSNR calculation must consider:

  • The optimal power (Popt) being injected into the fiber span
  • Insertion losses between components (IL1, IL2)
  • Fiber span loss (FSL) which varies by fiber type
  • Amplifier gains and saturation powers
Fiber Span OSNR Calculation:
OSNRspan = Pin - FSL - NF - 10log10(Δf) + 58

Where:

  • Pin is the input power to the fiber (dBm)
  • FSL is the fiber span loss (dB)
  • NF is the noise figure of the downstream amplifier (dB)
  • Δf is the reference bandwidth (typically 0.1nm or 12.5GHz)
  • 58 is a constant for normalization (dB)

3. Advanced OSNR Calculation Methods

3.1 EDFA Operation Impact

From the document, EDFAs play a crucial role in determining the OSNR of optical systems. The document specifically mentions several EDFAs for C+L networks:

  • OA_SGC and OA_SGEC: C-Band Dual EDFA for C+L Networks (with and without DGE)
  • OA_SGL and OA_SGEL: L-Band Dual EDFA for C+L Networks (with and without DGE)

EDFA operation impacts OSNR calculation in several key ways:

EDFA Gain Settings

According to the document, each EDFA can operate in two gain modes:

  • Low-Gain mode: Gain range = 15 – 28dB
  • High-Gain mode: Gain range = 23 – 37dB

The selection of gain mode affects the OSNR calculation through the relationship between gain, saturation, and noise generation.

EDFA Output Power

The document states that EDFAs operate in saturation with specific output powers:

  • OA_SGxC: 2.2dBm per 50GHz channel
  • OA_SGxL: 2.7dBm per 50GHz channel

These power levels directly impact the OSNR through the signal power component.

EDFA Gain Display Calculation (from document section 9.6):

For C-Band EDFAs (OA_SGxC and OA_LSGxC):

Gain(dB) = 22.0 – Input C-Band Total Power(dBm)

For L-Band EDFAs (OA_SGxL and OA_LSGxL):

Gain(dB) = 22.5 – Input L-Band Total Power(dBm)

These equations show how the EDFA gain is automatically adjusted based on input power, which directly affects the OSNR calculation.

3.2 Simulation Types (BOL/EOL)

The document describes how OSNR must be calculated for different simulation scenarios:

From section 7 of the document, each path should be simulated separately for:

  • BOL (Beginning of Life): Minimum span loss condition
  • EOL (End of Life): Maximum span loss condition (includes 3dB margin)

These different conditions affect the OSNR calculations by changing the effective fiber loss and other parameters.

For C-Band, the document specifies:

C-Band Minimum Span loss scenario (BOL):

  • BOL fiber loss (without margin)
  • No L-Band channels (minimum SRS loss)

C-Band Maximum Span loss scenario (EOL):

  • EOL fiber loss (with 3dB margin)
  • Full L-Band (maximum SRS loss)

For L-Band, the document specifies:

L-Band Minimum Span loss scenario (BOL):

  • BOL fiber loss (without margin)
  • Full C-Band (maximum SRS loss)

L-Band Maximum Span loss scenario (EOL):

  • EOL fiber loss (with 3dB margin)
  • No C-Band channels (minimum SRS loss)
OSNR Comparison Between BOL and EOL Conditions

3.3 C-Band OSNR Calculations

For C-Band transmission, the document provides specific formulas for calculating signal propagation under different conditions, which directly impact OSNR.

C-Band Minimum Loss Transmission (BOL):
Pout(fj) = Pin(fj) - α*L – Fiber_Tilt*(fj – fmidC)/4.8

Where:

  • fj is the frequency of the jth channel (THz)
  • α is the fiber attenuation coefficient (BOL)
  • L is the fiber length (km)
  • Fiber_Tilt(dB) is the Fiber Tilt_C(BOL) of the fiber
  • fmidC = 193.735THz is the C-Band middle channel
C-Band Maximum Loss Transmission (EOL):
Pout(fj) = Pin(fj) - α*L - {0.008*R*[PC(mW) + PL(mW)]*(0.22/α)}*c – Fiber_Tilt*(fj – fmidC)/4.8

Where:

  • α is the fiber attenuation coefficient (EOL with 3dB margin)
  • R is the fiber type factor
  • PC(mw) = 10^[PC(dBm)/10] (PC is the total C-Band power at the fiber input)
  • PL(mw) = min{0.92*PC(mw), 140}
  • c = sqrt{[PL(mw)/[PC(mW) +PL(mw)]}

These equations account for both the standard fiber attenuation and the impact of stimulated Raman scattering (SRS) between C and L bands, which affects the OSNR.

3.4 L-Band OSNR Calculations

Similar to C-Band, the document provides specific formulas for L-Band transmission that impact OSNR calculations.

L-Band Maximum Loss Transmission (EOL):
Pout(fj) = Pin(fj) - α*L – Fiber_Tilt_L*(fj – fmidL)/4.8

Where:

  • fj is the frequency of the jth channel (THz)
  • α is the fiber attenuation coefficient (EOL)
  • L is the fiber length (km)
  • Fiber_Tilt_L(EOL)(dB) is the maximum loss L-Band Fiber Tilt of the fiber
  • fmidL = 188.475THz is the L-Band middle channel
L-Band Minimum Loss Transmission (BOL):
Pout(fj) = Pin(fj) - α*L+{0.006*R*[PC(mW) + PL(mW)]*(0.22/α)}*L – Fiber_Tilt_L*(fj – fmidL)/4.8

Where:

  • α is the fiber attenuation coefficient (BOL without margin)
  • R is the fiber type factor
  • PL(mw) = 10^[PL(dBm)/10] (PL is the total L-Band power at the fiber input)
  • PC(mw) = 1.09*PL(mw)
  • L = sqrt{[PC(mw)/[PC(mW) +PL(mw)]}

Note the key difference in the SRS term between C-Band and L-Band equations: for L-Band, the SRS actually provides gain in some scenarios (positive term in the BOL case), which improves OSNR.

4. Optimal Power Calculation

4.1 Optimal Power vs. Span Loss

The document emphasizes that optimal power settings are crucial for maximizing OSNR. Section 8.1 states that "The power injected into the transmission fiber should optimize the span GOSNR." The optimal power depends on:

  • Transmission fiber type and attenuation coefficient
  • Span loss
  • Insertion loss of components within the fiber span
Optimal Power vs. Span Loss (G.652 Fiber)
Equation for Optimal Power (from section 8.1.2):
Popt(dBm) = min{ A + IL1 + 0.35*(FSL+IL2), Psat-10log10(96)}

Where:

  • FSL is the span loss in dB (from fiber input to next EDFA)
  • A is the fiber type coefficient
  • IL1 is the loss from the OA_SGxC output to the transmission fiber input
  • IL2 is the loss between the fiber output and the next adjacent OA_SGxC
  • Psat is the saturation power of the EDFA

4.2 Fiber Type Impact

The fiber type significantly impacts the optimal power and therefore the OSNR. According to the document, the fiber type coefficient (A) varies as follows:

Fiber Type A Coefficient (dBm)
G.652 -6.7
LEAF -8.6
TW-Reach -8.9
TW-RS -8.9
G.654 -5.5
G.653 -14

The document further specifies that C-Band and L-Band have different optimal power calculations:

C-Band Optimal Power:
Popt_C = min{A + IL1 + 0.35*[FSL(EOL) + IL2], Psat(C)-10log10(96)}
L-Band Optimal Power:
Popt_L = min{A + IL1 + 0.35*[FSL(EOL) - 1 + IL2], Psat(L)-10log10(96)}

Note that the L-Band calculation includes a "-1" term in the span loss component, reflecting the different propagation characteristics of the L-Band.

5. Fiber Tilt Considerations

5.1 Tilt Calculation Methods

The document explains in section 8.2 that fiber tilt is a critical factor in OSNR calculations, as it affects the relative power levels across the spectrum. The tilt is caused by:

  • Wavelength Dependent Loss (WDL)
  • Stimulated Raman Scattering (SRS) effects

The fiber tilt factor (R) varies by fiber type:

Fiber Type R Factor
G.652 1.0
LEAF 1.2
TW-Reach 1.5
TW-RS 1.6
G.654 0.85
G.653 2.0

The document provides detailed formulas for calculating fiber tilt in different scenarios:

C-Band BOL Tilt:
Fiber_Tilt_C(BOL) = [0.009*R*PC(mW)*(0.22/α)] + WDL*L

Where:

  • R is the fiber type factor
  • PC(mW) = 10^[(Popt_C + 19.8 - IL1)/10]
  • α (dB) is the fiber attenuation coefficient @ BOL (without margin)
  • WDL = 0.0075dB/km
  • L = fiber span length (km)
C-Band EOL Tilt:
Fiber_Tilt_C(EOL) = {0.009*R*[PC(mW) + PL(mW)]*(0.22/α)} + WDL*L

Where:

  • PC(mW) = 10^[(Popt_C + 19.8 - IL1)/10]
  • PL(mW) = min{0.92*PC(m), 140}
  • α (dB) is the fiber attenuation coefficient @ EOL (with margin)
L-Band BOL Tilt:
Fiber_Tilt_L(BOL) = {0.009*R*[PC(mW) + PL(mW)]*(0.22/α)} - WDL*L

Where:

  • PL(mW) = 10^[(Popt_L + 19.8 - IL1)/10]
  • PC(mW) = 1.09*PL(mW)
  • α (dB) is the fiber attenuation coefficient @ BOL (without margin)
L-Band EOL Tilt:
Fiber_Tilt_L(EOL) = [0.009*R*PL(mW)*(0.22/α)] - WDL*L

Where:

  • PL(mW) = 10^[(Popt_L + 19.8 - IL1)/10]
  • α (dB) is the fiber attenuation coefficient @ EOL (with margin)
Fiber Tilt Comparison Across Fiber Types

5.2 Tilt Compensation

The document explains in section 9.3.2 that EDFAs must compensate for fiber tilt to maintain flat channel power, which is crucial for optimizing OSNR across all channels:

EDFA Output Tilt Setting:
The OA_SGxC/L output Tilt should be equal to the -Fiber_Tilt where Fiber_Tilt is the Tilt of the downstream transmission fiber.

This tilt compensation ensures that the signal arriving at the next EDFA has a flat spectrum, which helps maintain consistent OSNR across all channels.

For ROADM pre-amplifiers, the document specifies in requirement #84 that the tilt should be set to 0dB, as these amplifiers have different requirements compared to in-line amplifiers.

Additionally, for EDFAs with Dynamic Gain Equalizers (DGE), the document provides a detailed formula for power equalization:

Power Equalization Target (section 9.4):
Pgoal(fj) = Psat - 10*log10(96) + Fiber_Tilt*[fj – fmidX]/4.8 + 10log10(BWj/50) + offset(fj)

Where:

  • fj is the channel frequency (in THz)
  • Psat is the EDFA saturation power (22dBm for OA_SGEC, 22.5dBm for OA_SGEL)
  • Fiber_Tilt is the relevant downstream Fiber Tilt (BOL/EOL, C or L), according to the simulation type
  • fmidX is the relevant Band middle channel: fmid_C = 193.735THz, fmid_L = 188.475THz
  • BWj is the channel Bandwidth (GHz)
  • Offset(fj) is the power offset of the channel (usually = 0dB)

6. Stimulated Raman Scattering (SRS) Impact

The document extensively addresses the impact of Stimulated Raman Scattering (SRS) on OSNR calculations, particularly for C+L band networks. SRS causes power transfer from higher frequency channels (C-Band) to lower frequency channels (L-Band), affecting the OSNR in both bands.

SRS Impact Diagram

Key SRS effects identified in the document that impact OSNR calculation:

C-Band Impact

For C-Band, SRS results in power depletion, especially at the lower wavelength edge of the C-Band. This depletion:

  • Reduces signal power, potentially degrading OSNR
  • Creates a tilt in the C-Band spectrum that must be compensated
  • Is more severe when the L-Band is fully populated

From the EOL simulations in section 10.1.2, we see the SRS impact quantified as:

{0.008*R*[PC(mW) + PL(mW)]*(0.22/α)}*c

This term represents the additional loss in C-Band channels due to SRS.

L-Band Impact

For L-Band, SRS results in power gain, especially at the higher wavelength edge of the L-Band. This gain:

  • Increases signal power, potentially improving OSNR
  • Creates a tilt in the L-Band spectrum in the opposite direction to C-Band
  • Is more significant when the C-Band is fully populated

From the BOL simulations in section 10.2.2, we see the SRS impact quantified as:

{0.006*R*[PC(mW) + PL(mW)]*(0.22/α)}*L

This term represents the additional gain in L-Band channels due to SRS.

SRS Impact on OSNR in C+L Band Networks

7. Amplifier Systems and OSNR

7.1 EDFA-based Systems

The document describes several EDFA types and their operation modes that impact OSNR calculations:

Standard EDFAs in the document include:

  • OA_SGC/OA_SGEC: C-Band Dual EDFA for C+L Networks
  • OA_SGL/OA_SGEL: L-Band Dual EDFA for C+L Networks

These operate with gain ranges of:

  • Low-Gain mode: 15 – 28dB
  • High-Gain mode: 23 – 37dB

OSNR impact from standard EDFAs is determined by:

  • Saturation power (22dBm for C-Band, 22.5dBm for L-Band)
  • Gain setting based on span loss
  • Optimum output power calculation (as detailed in section 9.3)

Raman-Optimized EDFAs in the document include:

  • OA_LSGC/OA_LSGEC: C-Band Raman-Optimized EDFA
  • OA_LSGL/OA_LSGEL: L-Band Raman-Optimized EDFA

These operate with different gain ranges:

  • Low-Gain mode: 9 – 17dB
  • High-Gain mode: 12 – 28dB

These EDFAs are specifically designed to work with Raman amplifiers (OA_HRCL) and have different OSNR characteristics due to the reduced gain requirements.

The document also describes the ROADMI_20CL integrated card which includes:

  • ROADMI_20CL (ROADM component)
  • OA_BoosterC (integrated EDFA)
  • High Power Pluggable EDFA (pre-amplifier)

The OA_BoosterC has specific parameters that affect OSNR:

  • Gain range: 18.0 - 25.0 dB
  • Saturation power: 22.0 dBm
  • Minimum input power: -25 dBm
  • Maximum input power: 4 dBm

The document specifies that EDFA output VOA attenuation impacts OSNR through the following formula (section 9.5):

EDFA VOA Attenuation:
VOA_attenuation(dB) = max{Psat(dBm) – 10log10(96) – Popt(dBm), 0}

The document further specifies in Req#82 that "Both the ASE noise and the nonlinear noise at the EDFA output should be attenuated by VOA_Attenuation(dB) such that both OSNR and GOSNR will be kept unmodified." This indicates that VOA attenuation should apply equally to signal and noise.

7.2 Raman Amplification

The document describes the OA_HRCL C+L Raman Amplifier in section 11, which provides simultaneous amplification of both C and L-Bands. This has significant implications for OSNR calculations.

Raman Amplification System

Key characteristics of the OA_HRCL that impact OSNR calculations:

  • Fixed gain of 13 dB (as specified in Table 11.1)
  • Distributed amplification that improves OSNR compared to discrete EDFAs
  • Different optimal power requirements for fiber spans with Raman amplification

The document provides modified optimal power formulas for spans with Raman amplification in section 11.3:

C-Band Optimal Power with Raman Amplification:
Popt_C(dBm) = min { AR + BR*SL(EOL), Psat-10*log10(96)}

Where AR and BR are coefficients that vary based on fiber type and span loss (detailed in Table 11.2a)

L-Band Optimal Power with Raman Amplification:
Popt_L(dBm) = min { AR + 1 + BR*SL(EOL), Psat-10*log10(96)}

Where AR and BR are coefficients that vary based on fiber type and span loss (detailed in Table 11.2b)

The document notes that use of Raman amplification is recommended for spans with EOL loss ≥ 26dB (default threshold in Req#103). This suggests that Raman amplification provides OSNR benefits primarily for longer or higher-loss spans.

8. Practical Considerations and Best Practices

Based on the document, several practical considerations emerge for optimizing OSNR in optical networks:

EDFA Configuration Guidelines

  • Select appropriate gain mode (high/low) based on span loss
  • Use EDFAs with DGE (Dynamic Gain Equalizer) for ILAN sites to ensure flat spectrum
  • When using Raman amplification, ensure the following EDFA has DGE capability (Req#112)
  • Configure appropriate tilt compensation to counteract fiber tilt

Network Planning for Optimal OSNR

  • Deploy Raman amplification for spans with loss ≥ 26dB
  • Consider fiber type impact on OSNR - G.654 offers better performance than G.653
  • Account for both BOL and EOL conditions in planning
  • Consider cross-band SRS effects when planning channel loadings

Monitoring Considerations

  • Monitor total C+L power on shared ports (Req#66)
  • Watch for "low-input Power" alarms on EDFAs (Req#99)
  • Monitor for "High span-loss" alarms on spans with Raman amplifiers (Req#100)
  • Re-simulate paths whenever fiber properties change (Req#87)

C+L Band Interactions

  • Account for SRS power transfer from C-Band to L-Band
  • Remember that L-Band OSNR is better with full C-Band loading
  • Consider that C-Band OSNR is worse with full L-Band loading
  • Plan wavelength assignments to minimize cross-band interference
Best Practices Impact on OSNR Performance

Important: When calculating OSNR, always consider both the signal propagation equations and the amplifier operation characteristics. The document provides detailed formulas for both aspects, recognizing that OSNR is influenced by the complex interplay between fiber types, spectral bands, power levels, and amplification strategies.