Fiber Optic Communication Fundamentals Section
1 Fiber optics -- Snell’s law -- Total Internal Refraction -- Wave Theory -- Model Dispersion -- Material (Chromatic) Dispersion -- Advantage of Fiber Optic Communication
Section 2 Laser Physics -- Quantum Theory -- Spontaneous Emission -- Stimulated Emission -- Population Inversion -- Cavity Resonance -- Laser Beam
Section 3 Photo-detectors -- Photo-electron effect -- Photomultipliers -- Semiconductor Photodiodes
Section 1 Fiber Optics -- Significance of Optics Fiber * It keeps the light inside the fiber and sends it to where we want it to go Optics Fiber
Sun
Earth
-- Reflection and Refraction, Snell’ Law Snell’s
Law * n1 Sinθ I = n2 Sinθ
r
n1 n2
-- Total Internal Refraction Critical
Angle * The incidence angle which has 900 refraction angle n2 n1 * Sin θ r = (n1/ n2) Sinθ
I
-- Wave Theory Maxwell’s
Equations * ∇ × E = - B/t * ∇ × H = D/t *∇ •D=0 *∇ •B=0 * Optical fiber is a wave guide. Different fiber just imposes different boundary conditions to the equations.
-- Model Dispersion Modes
of optical fiber * One typical thing for modes is that they have different velocities of propagation along the fiber. mode 1 mode 2
-- Model Dispersion Model
Dispersion, Multi-mode fiber * For multi-mode fiber, signal riding on difference modes for propagation. * The velocity difference of modes creates model dispersion
-- Model Dispersion Single
mode fiber * Only one mode is allowed to exist for propagation. * The diameter of the core is small enough to only allow the fundamental mode to survive. * No model dispersion but the energy flow along the fiber is limited because of the small core diameter.
-- Material (Chromatic) Dispersion
white
Prism
red blue
•
Refraction Index is frequency dependent. Sin θ r = (n1(f)/ n2(f)) Sinθ I
•
V = C/n(f)
•
-- Material (Chromatic) Dispersion Difference
of refraction index causes difference of propagation velocity of light along the fiber. Even for a single mode fiber, if the light source is not monochromatic, there still exists dispersion due to frequency dependence of the refraction index of material. Low line width laser beam is important as the light source of fiber optic communication.
-- Advantage of Fiber Optic Communication
Huge Capacity * Capacity for one channel (correspondence to one wavelength) 1542nm wavelength, f=c/(1542nm) = 1.95 x 1014 Hz = 195 THz. Possible bit rate ≤ 2f. * Capacity due to DWDM
No Electrical Connection, No Electromagnetic Interference Distance between repeaters, regenerators *Direct connection distance cable typical bandwidth Thick-net coax 10-100Mbps Multimode fiber 100 Single-mode-fiber 100-2400Mbps
distance 500 2km 40km
Section 2 Laser Physics LASER
*Light Amplified Stimulated Emission Radiation
-- Quantum Theory
Light is particle which is composed of photons. * The energy of a single photon = hf. Internal energy of atoms and molecules are quantized called energy levels. A photon emission or absorption corresponding to a transition of energy levels. E2 * hf = E2 – E1 E1
-- Spontaneous Emission Particles
(atoms, molecules) in their higher energy levels tend to jump back to the ground state (lower energy level states) by themselves.
-- Stimulated Emission Jump
Stimulated by another photon whose energy equals to the gap of the energy levels. E2 hf = E2 – E1 E1
Same
kind of photon, same direction.
-- Population Inversion More
populated in higher energy level instead of ground state (lower energy levels). Optical pump
-- Cavity Resonance Selected
wavelength meets the condition of resonance of the cavity.
-- Laser beam Same
frequency (narrow line width), same direction.
Section 3 Photo-detectors Change
the photon signal to electrical. Have region of wavelength sensitivity.
-- Photon electron effect If
the energy of a photon is larger than the work function of the metal. Than one photon electron is created.
hf ≥ Eg
-- Photomultipliers Avalanche
effect. Dynodes Anode
Cathode -v
Output
-- Semiconductor Photodiode Depletion
Light
region and photo-current v p -
intrinsic
n +
d End-illuminated p-I-n photodiode
End