UNIT 5: OPTICAL FIBRE COMMUNICATION – SHORT NOTES
1. FIBER OPTICS FUNDAMENTALS
Numerical Aperture (NA)
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Definition: A measure of the light-gathering ability of an optical fiber. It defines the maximum angle of incidence at the fiber input face for which light will be guided.
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Derivation (Step-Index Fiber):
For light entering from air (n₀=1) into a fiber core (n₁) surrounded by cladding (n₂), the condition for Total Internal Reflection (TIR) at the core-cladding interface is:
$$n_1 \sin \theta_1 \geq n_2$$
Using Snell's law at the air-core interface: $$\displaystyle \sin \theta_0 = n_1 \sin \theta_1 $$.
Combining and solving for the maximum acceptance angle $$\displaystyle \theta_{0(max)} $$:
$$n_0 \sin \theta_{0(max)} = \sqrt{n_1^2 - n_2^2}$$
Therefore, **Numerical Aperture (NA) is:**
$$\boxed{NA = \sqrt{n_1^2 - n_2^2}}$$
For a medium other than air (refractive index n₀), the maximum acceptance angle is given by:
$$\sin \theta_{0(max)} = \frac{\sqrt{n_1^2 - n_2^2}}{n_0}$$
- Critical Angle ($$\displaystyle \theta_c $$): The angle of incidence at the core-cladding interface beyond which TIR occurs.
$$\boxed{\theta_c = \sin^{-1}\left(\frac{n_2}{n_1}\right)}$$
- Relation: $$\displaystyle NA = n_1 \sqrt{2\Delta} $$ (for small $\Delta$, where $$\displaystyle \Delta = \frac{n_1 - n_2}{n_1} $$).
[!TIP] Exam Focus: NA derivation is very frequent. Remember NA depends only on n₁ and n₂. For a fiber in a medium other than air, NA is defined as $$\displaystyle n_0 \sin \theta_{0(max)} $$.
Modes of Propagation
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Mode: A specific solution to Maxwell's equations satisfying boundary conditions, representing a distinct path of light propagation.
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Planar Dielectric Waveguide: Supports Transverse Electric (TE) and Transverse Magnetic (TM) modes. Modes are designated by the number of field zeros (m for TE/TM).
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Step-Index Fiber (Cylindrical): Modes are hybrid (HE/EH). The exact solution involves Bessel functions. The number of guided modes (M) is approximately:
$$\boxed{M \approx \frac{V^2}{2}} \quad \text{(for large V, step-index)}$$
- Normalized Frequency (V-number): A dimensionless parameter determining the number of modes.
$$\boxed{V = \frac{2\pi a}{\lambda} \sqrt{n_1^2 - n_2^2} = \frac{2\pi a}{\lambda} \cdot NA}$$
where `a` = core radius, `λ` = operating wavelength.
* **Significance:**
* V < 2.405 → **Single-mode operation** (only fundamental mode HE₁₁ propagates).
* V >> 2.405 → **Multimode operation**.
- Graded-Index Fiber: Number of modes is also proportional to V² but with a different constant. For a parabolic profile, $$\displaystyle M \approx \frac{g}{g+2} \frac{V^2}{2} $$ (g = profile parameter).
| Fiber Type | V-Number Condition | Approx. Number of Modes (M) |
|---|---|---|
| Step-Index Multimode | V >> 2.405 | $$\displaystyle M \approx V^2/2 $$ |
| Graded-Index Multimode | V >> 2.405 | $$\displaystyle M \approx \frac{g}{g+2} \cdot \frac{V^2}{2} $$ |
| Single-Mode | V < 2.405 | M = 1 (fundamental mode only) |
[!TIP] Common Pitfall: The exact cutoff for single-mode is V=2.405. For V slightly above this, a second mode (LP₁₁) may leak (leaky mode). Use V < 2.405 for guaranteed single-mode.
Ray Theory of Light Transmission
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Step-Index Fiber:
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Meridional Rays: Pass through the fiber axis. Simple analysis using TIR.
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Skew Rays: Do not pass through the axis; follow a helical path. They have a longer path length than meridional rays with the same θ₀.
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Axial Rays: θ₀ = 0, travel straight along the axis.
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Acceptance Cone: Light entering within the cone of half-angle $$\displaystyle \theta_{0(max)} $$ is guided. Solid angle of acceptance = $$\displaystyle \pi (NA)^2 $$.
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Graded-Index Fiber: Ray path is continuously curved due to gradual index change. Rays follow sinusoidal paths. This reduces intermodal dispersion as higher-order rays travel faster in the lower-index outer core.
Dispersion
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Definition: Broadening of an optical pulse as it travels along the fiber, limiting the maximum data rate.
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Intermodal (Modal) Dispersion: Occurs in multimode fibers due to different group velocities of different modes.
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Step-Index: Very high. Pulse broadening $$\displaystyle \Delta \tau_{inter} \approx \frac{L n_1 \Delta}{c} $$.
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Graded-Index: Greatly reduced. For ideal parabolic profile, $$\displaystyle \Delta \tau_{inter} \approx 0 $$.
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Intramodal (Chromatic) Dispersion: Occurs in all fibers (single-mode and multimode) because different wavelengths travel at different speeds.
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Material Dispersion: Due to wavelength dependence of refractive index (n). Zero-dispersion wavelength for silica ~1.27 µm.
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Waveguide Dispersion: Due to wavelength dependence of the mode propagation constant. Arises from the waveguide structure itself. Can be engineered to shift zero-dispersion wavelength.
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Total Chromatic Dispersion: $$\displaystyle D_{total} = D_{material} + D_{waveguide} $$ (units: ps/(nm·km)).
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Polarization Mode Dispersion (PMD): In single-mode fibers, due to birefringence (asymmetry/stress), the two orthogonal polarization states travel at slightly different speeds. A random, statistical effect. $$\displaystyle \Delta \tau_{PMD} = PMD_{coeff} \cdot \sqrt{L} $$.
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Pulse Broadening & Bandwidth: Total RMS pulse broadening: $$\displaystyle \Delta \tau_{total} = \sqrt{\Delta \tau_{inter}^2 + \Delta \tau_{chrom}^2 + \Delta \tau_{PMD}^2} $$.
- Bandwidth-Distance Product (BL): $$\displaystyle B \cdot L \approx \frac{0.44}{\Delta \tau_{total}} $$ (for NRZ). A key system performance metric.
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Rise Time Budget: For a link with multiple sections (transmitter, fiber, receiver), total RMS rise time:
$$\boxed{\Delta t_{r(system)} = \sqrt{\Delta t_{r(tx)}^2 + \Delta t_{r(fiber)}^2 + \Delta t_{r(rx)}^2}}$$
where $$\displaystyle \Delta t_{r(fiber)} = \Delta \tau_{total} $$.
[!TIP] Key Formula: For step-index multimode fiber, intermodal dispersion limit: $$\displaystyle B \cdot L \leq \frac{0.44 c}{n_1 \Delta} $$. Chromatic dispersion limit: $$\displaystyle B \cdot L \leq \frac{0.44}{|D_{total}| \Delta \lambda} $$.
2. ATTENUATION AND LOSS MECHANISMS
Attenuation coefficient $\alpha$ (dB/km) = 10 log₁₀(P_in/P_out).
| Loss Mechanism | Cause | Wavelength Dependence | Reduction Techniques |
|---|---|---|---|
| Intrinsic Absorption | Fundamental material properties: <br>• Electronic: UV absorption (bandgap). <br>• Vibrational (IR): Infrared absorption due to molecular vibrations (Si-O bond). | High in UV & IR regions. Minimum at 1.55 µm (for silica). | Material choice (low-loss glasses like silica). Operate at low-loss windows (0.85, 1.3, 1.55 µm). |
| Extrinsic Absorption | Impurity absorption: <br>• OH⁻ ions: Strong peak at 2.73 µm (1st overtone at 1.38 µm). <br>• Transition metals (Fe, Cu): Broad absorption bands. | OH⁻ peak at 1.38 µm is critical for 1.55 µm window. | Ultra-pure materials, dehydration during manufacturing (MCVD). |
| Rayleigh Scattering | Microscopic density fluctuations frozen into the glass during solidification. | $$\displaystyle \alpha_{Rayleigh} \propto \frac{1}{\lambda^4} $$. Dominant loss mechanism in low-loss window. | Cannot be eliminated. Use larger core fibers? (No, increases other losses). Fundamental limit. |
| Mie Scattering | Scattering from inhomogeneities comparable to λ (e.g., imperfections, large particles). | Weak wavelength dependence. | Improved manufacturing control (cleanroom). |
| Macrobending Losses | Bending radius too large → some modes' incident angles fall below critical angle → radiation loss. | Increases as bend radius decreases. | Minimum bend radius specification. |
| Microbending Losses | Small-scale, microscopic bends (1-10 mm wavelength) due to cabling stress, temperature changes. | Can be severe at specific wavelengths. | Proper cable design, protective coatings, loose tube construction. |
| Fresnel Reflection | Index mismatch at fiber endfaces. | Independent of λ. | Index-matching gel, angled physical contact (APC) connectors. |
[!TIP] Critical Calculation: Critical Radius of Curvature ($$\displaystyle R_c $$) for large bending losses:
$$\boxed{R_c \approx \frac{3\lambda}{4\pi n_1 \sqrt{2\Delta}}}$$
Loss increases sharply when bend radius < $$\displaystyle R_c $$.
3. FIBER FABRICATION TECHNIQUES
| Technique | Process Steps | Advantages | Limitations |
|---|---|---|---|
| MCVD (Modified Chemical Vapor Deposition) | 1. Soot Deposition: SiCl₄/GeCl₄ + O₂ → SiO₂/GeO₂ soot inside rotating silica tube.<br>2. Sintering: Heat (1500-1800°C) collapses soot into transparent glass layer.<br>3. Collapse: Tube collapsed into solid preform rod. | High purity, precise index profile control, low loss. | Slow, limited to small core/cladding diameters. |
| VAD (Vapor Axial Deposition) | 1. Soot Deposition: Reactants (SiCl₄, GeCl₄, O₂) flow axially onto a rotating seed rod.<br>2. Sintering: Soot vitrifies as it builds up.<br>3. Preform: Solid rod grown axially. | Very high deposition rate, large-diameter preforms possible. | More complex gas flow control, potential for higher OH⁻. |
| OVD (Outside Vapor Deposition) | 1. Soot Deposition: Soot deposited on a target rod from the outside.<br>2. Consolidation: Soot tube is sintered in a furnace to form a solid preform. | Simple, high deposition rate, large preforms. | Purity slightly lower than MCVD, soot layer control. |
[!TIP] Exam Comparison: MCVD is inside-out (deposits on tube inner wall),