UNIT 1: Optical Fiber Communication - Short Notes
A. FIBER FUNDAMENTALS & WAVE GUIDING
Ray Theory & Transmission in Optical Fibers
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Step-Index Fiber: Core refractive index \(n_1\) uniform, cladding index \(n_2 < n_1\).
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Meridional Rays: Pass through fiber axis, zigzag path with reflections at core-cladding interface.
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Skew Rays: Do not pass through axis; helical path; more reflections per unit length → higher attenuation.
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Graded-Index Fiber: Core index \(n(r)\) decreases parabolically from center: \(n(r) = n_1 \sqrt{1 - 2\Delta (r/a)^2}\) for \(r \leq a\), where \(\Delta = (n_1 - n_2)/n_1\).
- Rays follow curved paths due to continuous refraction; reduces intermodal dispersion.
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Modes in Planar Dielectric Waveguide:
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Planar slab of thickness \(d\), indices \(n_f\) (film), \(n_s\) (substrate), \(n_c\) (cladding) with \(n_f > n_s > n_c\).
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Modes: Solutions to wave equation satisfying boundary conditions; TE (electric transverse) and TM (magnetic transverse) modes.
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Each mode has cutoff wavelength \(\lambda_c\) above which it becomes leaky. Number of guided modes depends on \(V\)-number for slab: \(V = \frac{2\pi d}{\lambda} \sqrt{n_f^2 - n_s^2}\).
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Normalized Frequency (V-number)
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Definition: \(V = \frac{2\pi a}{\lambda} \sqrt{n_1^2 - n_2^2} = \frac{2\pi a}{\lambda} NA\), where \(a\) = core radius, \(\lambda\) = wavelength.
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Significance: Determines number of guided modes.
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Single-mode condition: \(V < 2.405\) (cutoff for LP\(_{11}\) mode).
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Multimode: \(V > 2.405\).
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Derivation: From wave equation for cylindrical waveguide; \(V\) arises as eigenvalue parameter.
Numerical Aperture (NA) & Acceptance Angle
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Definition: \(NA = \sqrt{n_1^2 - n_2^2}\). Measures light-gathering ability.
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Physical Meaning: Sine of maximum acceptance angle \(\theta_{max}\) in air: \(\sin\theta_{max} = NA\).
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Derivation (Step-Index Fiber):
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Snell’s law at fiber entrance: \(n_0 \sin\theta_0 = n_1 \sin\phi\) (\(n_0\) = air index ≈ 1).
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At core-cladding interface, total internal reflection condition: \(\sin\theta_c = n_2/n_1\), where \(\theta_c\) = critical angle.
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For meridional ray, \(\phi = 90^\circ - \theta_c\) → \(\sin\phi = \cos\theta_c = \sqrt{1 - (n_2/n_1)^2}\).
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Thus, \(\sin\theta_{max} = n_1 \sqrt{1 - (n_2/n_1)^2} = \sqrt{n_1^2 - n_2^2} = NA\).
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Calculation: Given \(n_1, n_2\), compute \(NA\) and \(\theta_{max} = \sin^{-1}(NA)\).
Number of Modes
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Step-Index Multimode Fiber: Total guided modes \(M \approx \frac{V^2}{2}\) (including both polarizations).
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Graded-Index Fiber: \(M \approx \frac{V^2}{2}\) but effective number of modes lower due to graded profile reducing modal dispersion.
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Problems: Compute \(V\) from given \(a, \lambda, n_1, n_2\) (or \(\Delta\)), then \(M\).
[!TIP]
Common Pitfall: In NA derivation, ensure using correct angle \(\phi\) inside core. For graded-index, NA definition same but acceptance cone narrower due to index profile.
B. TRANSMISSION CHARACTERISTICS & SIGNAL DEGRADATION
Attenuation (Losses)
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Absorption Losses:
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Intrinsic: Fundamental material absorption due to electronic band structure (UV: band-to-band; IR: vibrational modes). In silica, IR absorption > 1.6 µm, UV < 0.4 µm.
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Extrinsic: Impurity absorption:
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OH⁻ ions (water peak at 1.38 µm, overtones at 0.95, 1.24 µm).
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Transition metal ions (Fe, Cu, Co) in visible range.
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Reduction: Ultra-pure silica (vapor-phase deposition), dehydration, careful doping.
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Scattering Losses:
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Rayleigh Scattering: Caused by microscopic density/composition fluctuations; loss \(\propto \lambda^{-4}\). Dominant in low-loss windows (e.g., 0.85, 1.3, 1.55 µm).
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Mie Scattering: Due to macroscopic imperfections (diameter variations, bubbles); less wavelength dependent.
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Bending Losses:
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Macrobending: Fiber curved with radius \(R\). Loss occurs when \(R\) less than critical radius \(R_c\). For step-index:
\[ R_c \approx \frac{3\lambda}{4\pi n_1 \Delta} \left( \frac{2a}{\lambda} \right)^{1/2} \quad \text{(approx.)} \]
Loss increases rapidly as \(R\) decreases below \(R_c\).
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Microbending: Small-scale bends (µm scale) from lateral pressure, temperature changes. Causes mode coupling and radiation loss.
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Reduction: Proper cabling, avoid tight bends, use graded-index fiber.
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Core-Cladding Losses: Differential attenuation among modes; higher-order modes often have higher loss.
Dispersion
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Intermodal Dispersion (Modal):
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Cause: Different group velocities for modes in multimode step-index fiber.
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Delay spread: \(\Delta\tau_{inter} = \frac{L n_1 \Delta}{c}\), where \(L\) = length, \(\Delta = (n_1 - n_2)/n_1\).
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Reduction: Use graded-index fiber (parabolic profile equalizes mode delays).
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Intramodal Dispersion (Chromatic):
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Material Dispersion: Wavelength dependence of refractive index \(n(\lambda)\); described by dispersion parameter \(D = -\frac{\lambda}{c} \frac{d^2 n}{d\lambda^2}\) (ps/(nm·km)).
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Waveguide Dispersion: Due to waveguide structure; depends on \(V\)-number and mode.
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Total Intramodal: \(\Delta\tau_{intra} = |D| L \Delta\lambda\), where \(\Delta\lambda\) = source spectral width.
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Overall Pulse Broadening:
\[ \Delta\tau_{total} = \sqrt{\Delta\tau_{inter}^2 + \Delta\tau_{intra}^2} \]
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Bit Rate & Link Distance:
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Maximum bit rate \(B_{max} \approx \frac{0.44}{\Delta\tau_{total}}\) (for NRZ) or \(B = \frac{0.7}{t_{sys}}\) (using rise time budget).
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Link distance limited by dispersion: \(L_{max} \propto \frac{1}{\Delta\tau_{total}}\).
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[!TIP]
Key Formula: For step-index multimode, \(\Delta\tau_{inter} \propto L \Delta\). Graded-index reduces this by factor ~10–100. Material dispersion zero around 1.3 µm for silica.
Nonlinear Effects (Brief)
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SPM (Self-Phase Modulation): Intensity-dependent phase shift.
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XPM (Cross-Phase Modulation): Wavelength channels modulate each other.
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FWM (Four-Wave Mixing): Interaction of multiple wavelengths generating new frequencies. Significant in WDM systems.
C. FIBER FABRICATION & MATERIALS
Fiber Preform Fabrication Techniques
| Method | Process Steps | Advantages |
|---|---|---|
| MCVD (Modified Chemical Vapor Deposition) | 1. SiCl₄, GeCl₄, O₂ inside rotating silica tube.<br>2. Burner moves along tube, depositing soot layer.<br>3. Sinter to form transparent glass.<br>4. Collapse tube to solid preform. | High purity, precise index control, low loss. |
| OVD (Outside Vapor Deposition) | 1. Soot deposited on solid rod from burner.<br>2. Build up porous preform.<br>3. Sinter in furnace to dense glass. | Large preforms, high deposition rate. |
| VAD (Vapor Axial Deposition) | 1. Porous soot built axially on rotating seed rod.<br>2. Simultaneous sintering at deposition zone.<br>3. Continuous process. | No collapse step, high productivity, low cost. |
Fiber Drawing & Coating
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Draw Tower: Preform heated in furnace (~2000°C), fiber drawn at ~1 m/s, coated with UV-cured acrylate.
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Primary Coating: Soft, cushions fiber against microbends.
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Secondary Coating: Hard, protects from abrasion.
D. FIBER CONNECTIONS, SPLICING & MEASUREMENT
Fiber Connectors
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Types:
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FC/PC: Screw-on, ceramic ferrule, physical contact (low reflection).
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ST: Bayonet lock, older multimode.
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SC: Push-pull, high density.
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LC: Small form factor, common in datacenters.
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Parameters:
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Insertion Loss (dB): Loss due to connector (typical 0.2–0.5 dB).
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Return Loss (dB): Reflection back toward source (higher better, >40 dB for PC).
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Fiber Splicing
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Fusion Splicing:
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Fiber ends cleaved (perfect 90°).
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Aligned (microscope/alignment system).
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Arc weld to fuse ends.
- Advantages: Low loss (<0.1 dB), high strength, permanent.
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Mechanical Splicing:
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Alignment via V-grooves, index-matching gel.
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Advantages: Quick, no power needed; higher loss (~0.3 dB).
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Comparison: Fusion superior for permanent, low-loss; mechanical for temporary/repair.
Fiber Characterization & Testing
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Optical Time-Domain Reflectometer (OTDR):
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Principle: Launch short pulse, detect backscattered/reflected light vs. time.
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Working: Pulse → fiber → Rayleigh backscatter + Fresnel reflections → time-gated detector → distance \(z = c t / (2 n)\).
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Trace Interpretation:
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Slope = attenuation (dB/km).
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Spike up = connector/splice loss (backscatter drop).
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Spike down = reflection (e.g., fiber end, break).
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Distance between events = fiber length.
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Measures: Attenuation, splice/connector loss, fiber length, fault location.
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Cut-Back Method:
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Measure output power \(P_{out1}\) from long fiber.
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Cut fiber near output, measure \(P_{out2}\) from short length.
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Attenuation \(\alpha = 10 \log_{10}(P_{out1}/P_{out2}) / (L_1 - L_2)\) (dB/km).
- Accurate but destructive.
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E. SOURCES & DETECTORS
Light Emitting Diodes (LEDs)
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Structure:
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Surface-Emitting (Burrus): p-n junction perpendicular to surface; lens for coupling.
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Edge-Emitting: Similar to laser diode but no feedback; emits from cleaved edge.
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Principle: Electroluminescence—electron-hole recombination in active layer.
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Internal Optical Power Derivation:
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Recombination rate \(R = I / q\) (carriers/sec).
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Internal quantum efficiency \(\eta_{int}\) = fraction recombining radiatively.
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Photon generation rate \(= \eta_{int} R\).
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Internal optical power \(P_{int} = \eta_{int} R \cdot h\nu = \eta_{int} \frac{I}{q} h\nu\).
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\boxed{P_{int} = \eta_{int} \frac{I h\nu}{q}}
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Characteristics: Broad spectrum (~50–100 nm), low modulation bandwidth (~100 MHz), low cost, long life.
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vs Lasers: Lower power, higher dispersion, but no coherence issues.
LASERs (Semiconductor Injection Lasers)
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Principle:
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Population Inversion: Forward bias injects carriers into active region.
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Stimulated Emission: Photon triggers coherent emission.
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Optical Feedback: Cleaved facets form Fabry-Perot cavity; standing waves.
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Structure: Double heterostructure (AlGaAs/GaAs) for carrier confinement; cleaved ends reflect.
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Resonant Frequency & Mode Spacing:
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Cavity length \(L\), effective index \(n\).
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Allowed frequencies: \(\nu_m = m \frac{c}{2nL}\).
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Mode spacing: \(\Delta\nu = \frac{c}{2nL}\).
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\boxed{\Delta\nu = \frac{c}{2nL}}
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Modulation: Direct modulation (bias current varied); limited by chirp and relaxation oscillations.
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vs LEDs: Narrow spectrum (~1–2 nm), high power, high bandwidth (>10 GHz), coherent.
Photodetectors
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PIN Photodiode:
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Structure: p⁺-i-n⁺; intrinsic layer wide depletion region.
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Working: Photons absorbed in depletion region → electron-hole pairs → drift current (photoconductive mode).
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Quantum Efficiency \(\eta\):
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Fraction of incident photons generating collected carriers.
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Derivation: Incident photon flux \(P/(h\nu)\). Fraction absorbed in depletion region of width \(d\): \(1 - e^{-\alpha d}\), where \(\alpha\) = absorption coefficient.
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Including reflection loss \(R\) at surface: \(\eta = (1 - R)(1 - e^{-\alpha d})\).
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\boxed{\eta = (1 - R)(1 - e^{-\alpha d})}
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Responsivity \(R\): \(R = \frac{I_{ph}}{P_{opt}} = \frac{\eta q}{h\nu}\) (A/W).
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Avalanche Photodiode (APD):
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Structure: p⁺-π-n⁺; high field multiplication region (p-π junction).
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Principle: Photogenerated carriers accelerated → impact ionization → avalanche multiplication (gain \(M\)).
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Advantages: Internal gain (10–1000×) → higher sensitivity than PIN.
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Disadvantages: Higher bias (100–400 V), excess noise (statistical variation in multiplication).
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Excess Noise Factor \(F\): \(F = k M + (1-k)(2 - 1/M)\) for electrons (typical \(k \approx 0.02–0.7\)).
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Comparison:
| Parameter | PIN | APD | |---------------|---------|---------| | Gain | 1 | \(M > 1\) | | Bandwidth | High | Lower (avalanche time) | | Noise | Low | Higher (excess noise) | | Bias | Low (5–50 V) | High (100–400 V) | | Sensitivity | Moderate | High |
F. OPTICAL AMPLIFIERS
Erbium-Doped Fiber Amplifier (EDFA)
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Principle:
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Er³⁺ ions doped in fiber core (pump at 980 nm or 1480 nm).
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Pump excites Er³⁺ to higher level → population inversion between \(^4I_{13/2}\) and \(^4I_{15/2}\).
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Signal at 1550 nm stimulates emission → amplification.
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Configurations:
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Co-propagating: Pump and signal same direction.
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Counter-propagating: Pump opposite to signal (reduces ASE noise).
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Bi-directional: Both pumps.
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Amplifier Gain Derivation:
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Small-signal gain \(G = \exp[(\sigma_e N_2 - \sigma_a N_1) L]\), where \(\sigma_e, \sigma_a\) = emission/absorption cross-sections, \(N_1, N_2\) = population densities, \(L\) = doped length.
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With saturation: \(G = \frac{G_0}{1 + P_{sig}/P_{sat}}\), where \(G_0\) = small-signal gain, \(P_{sat}\) = saturation power.
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Conversion Efficiency:
\[ \eta = \frac{P_{sig,out} - P_{sig,in}}{P_{pump,in}} \times 100\% \]
- Derivation from rate equations and power propagation.
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Advantages: High gain (30–40 dB), low noise (4–6 dB), wavelength compatibility with SMF, polarization independent.
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Applications: In-line amplifier, pre-amplifier (before receiver), power booster.
Raman Amplifier
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Principle: Stimulated Raman Scattering (SRS); pump photon (higher frequency) → Stokes photon (lower frequency) + phonon.
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Pump wavelength \(\lambda_p\), signal \(\lambda_s\) with \(\lambda_s > \lambda_p\) (Stokes shift ~13 THz for silica).
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Gain \(G_R = \exp(g_R P_p L_{eff}/A_{eff})\), where \(g_R\) = Raman gain coefficient, \(P_p\) = pump power, \(L_{eff}\) = effective length, \(A_{eff}\) = effective area.
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Types:
- Distributed Raman Amplification (DRA): Pump co-propagates with signal in transmission fiber; extends reach, reduces noise.
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vs EDFA:
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Raman: Broadband (any wavelength), distributed gain, higher noise, requires high pump power.
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EDFA: Fixed band (C/L-band), discrete amplifier, lower noise.
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G. OPTICAL NETWORKING & SYSTEM DESIGN
Wavelength Division Multiplexing (WDM)
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Principle: Multiple wavelengths (channels) transmitted simultaneously on single fiber → multiplies capacity.
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System Components:
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Multiplexer/Demultiplexer: Combine/separate wavelengths.
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AWG (Arrayed Waveguide Grating): Planar lightwave circuit; phased array waveguides.
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Thin-Film Filters: Interference coatings; cascaded for many channels.
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Optical Amplifiers: EDFA/Raman to boost all channels.
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Add-Drop Multiplexers (OADM): Selectively add/drop wavelengths.
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Architecture:
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Point-to-Point: Simple link with MUX/DEMUX at ends.
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OADM Networks: Nodes add/drop channels; enables mesh topologies.
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Applications: Increase link capacity, SONET/SDH augmentation, optical mesh networks.
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MEMS Technology: Micro-electromechanical mirrors for dynamic wavelength switching/tuning in WDM.
SONET / SDH
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Architecture & Hierarchy:
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SONET (US): STS-1 = 51.84 Mbps; STS-3c = 155.52 Mbps (3×STS-1); STS-12c, STS-48c, etc.
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SDH (Int'l): STM-1 = 155.52 Mbps; STM-4 = 622.08 Mbps; STM-16, STM-64.
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STS-3c = STM-1; STS-12c = STM-4; etc.
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Frame Structure:
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SONET STS-1 Frame: 9 rows × 90 columns; first 3 columns = transport overhead (Section, Line, Path).
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SDH STM-1 Frame: 9 rows × 270 columns; overhead similar.
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Byte-Interleaving: Multiplexing by interleaving bytes from lower-rate signals.
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Working: Synchronous multiplexing; all clocks locked to master; overhead bytes for management (error, alarm, routing).
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Comparison: SONET uses STS-1 as base; SDH uses STM-1 (155.52 Mbps). SDH more globally adopted; SONET common in North America.
Passive Optical Networks (PON)
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Architecture:
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OLT (Optical Line Terminal) at central office.
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ODN (Optical Distribution Network): passive splitters (1:32, 1:64).
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ONU/ONT (Optical Network Unit/Terminal) at customer premises.
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Working:
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Downstream: Broadcast from OLT to all ONUs (TDMA not needed); ONUs select by wavelength or time.
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Upstream: TDMA (Time Division Multiple Access); ONUs transmit in assigned slots to avoid collision.
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Types:
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APON/BPON: ATM-based; BPON adds TDM (STM) and protection.
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GPON: GFP framing; higher split ratio (1:128); 2.5 Gbps down, 1.25 Gbps up.
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EPON: Ethernet-based; 1 Gbps symmetric; IEEE 802.3ah.
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Optical Link Design & Power Budget
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Link Power Budget Analysis:
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Transmitter Power \(P_T\) (dBm): Launch power.
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Receiver Sensitivity \(P_R\) (dBm): Minimum power for target BER.
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System Margin \(M_s\) (dB): Allowance for aging, mis-splicing (typically 3–6 dB).
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Total Loss Budget:
\[ P_T - P_R - M_s \geq \text{Total Link Loss} \]
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Total Link Loss = Fiber attenuation (\(\alpha L\)) + Connector loss (\(N_c \cdot \alpha_c\)) + Splice loss (\(N_s \cdot \alpha_s\)) + Safety margin.
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Design: Compute total loss; ensure \(P_T - \text{loss} \geq P_R + M_s\).
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Rise-Time Budget (Digital Links):
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Total system rise time:
\[ t_{sys} = \sqrt{t_{tx}^2 + t_{rx}^2 + t_{inter}^2 + t_{intra}^2} \]
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\(t_{tx}\) = transmitter rise time.
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\(t_{rx}\) = receiver rise time.
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\(t_{inter} = \frac{L n_1 \Delta}{c}\) (step-index multimode).
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\(t_{intra} = |D| L \Delta\lambda\) (chromatic dispersion).
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Maximum bit rate:
\[ B = \frac{0.7}{t_{sys}} \quad \text{(for NRZ)} \]
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Point-to-Point Links: Simple transmitter-fiber-receiver; power budget and rise time budget determine max distance/bit rate.
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Power Penalties: Additional power required due to:
- Modal noise, dispersion, reflections (from connectors), timing jitter.
H. OPTICAL COUPLERS & PASSIVE COMPONENTS
Optical Coupler Parameters
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Splitting Ratio (Coupling Ratio): Fraction of input power directed to each output port (e.g., 50:50, 90:10).
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Insertion Loss: Loss for a particular path; \(IL = -10 \log_{10}(P_{out}/P_{in})\) (dB).
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Excess Loss: Loss beyond ideal splitting; \(EL = P_{in} - (P_{out1} + P_{out2})\) (dB).
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Cross-talk (Isolation): Unwanted coupling from one port to another; \(XT = -10 \log_{10}(P_{leak}/P_{in})\) (dB).
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Directionality: Isolation between input and wrong output (reverse direction).
Types of Couplers
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Fused Biconical Taper (FBT):
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Two fibers fused and tapered; evanescent coupling.
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Advantages: Low cost, good for 2×2 couplers.
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Disadvantages: Wavelength dependent, sensitive to temperature.
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Planar Lightwave Circuit (PLC):
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Waveguides on silica/silicon substrate; lithography.
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Advantages: Wavelength independent, stable, scalable (1×N).
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Used in PON splitters, AWGs.
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[!TIP]
Exam Focus: NA derivation, attenuation mechanisms (especially OH⁻ peak), OTDR trace reading, EDFA gain, link power budget calculation, SONET/SDH frame overhead, PIN quantum efficiency derivation. Always box final formulas.