photons and fibres lecturer : professor laurie cahill

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PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

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Page 1: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

PHOTONS AND FIBRES

Lecturer : Professor Laurie Cahill

Page 2: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

PHOTONS AND FIBRES

What is light?

Is light a particle or a wave?

What is a photon?

Page 3: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

HISTORY

Newton - Light is a stream of corpuscles

Huygens, Maxwell,Young - Light travels in waves

Planck - Thermal radiation comprises discrete packets of energy called quanta

Einstein

Page 4: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

EINSTEIN (1905)

Light is similarly quantised

hfE E is the energy of the light quanta, later called photonsh is Planck’s constantf is the frequency of the light

This explains the photoelectric effect

Page 5: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

THE PHOTOELECTRIC EFFECT

The maximum KE of each emitted electron depends on the frequency of the incident light, not the intensity.More photons produce more emitted electrons

(Source: D. A. Neamen)

Page 6: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

WORK FUNCTION OF A METAL SURFACE

(Source : A. Beiser)

Page 7: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

De BROGLIE (1924)

hc

hfc

Ep

Momentum of a photon

Wavelength of a particle Hence matter waves and the Wave-

Particle Duality p

h

Page 8: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

DOUBLE SLIT EXPERIMENT

Similar experimental result (over time) if we use photons or electrons

Page 9: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

WAVES OR PARTICLES?

If light only consists of waves, how come we can only generate and detect discrete photons?If light consists only of particles, how does a photon passing through one slit know about the other slit being open?

Feynman - Consider all possible paths and assign amplitudes and probabilities to “particles” .

Page 10: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

COMMUNICATION USING LIGHT

END VIEWAXIAL CROSS-SECTION

Consider a light ray entering a glass rod

Page 11: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

RAYS IN A CIRCULAR FIBRE

Exercise: Find an expression for the acceptance angle for rays through the axis (Hint apply Snell’s Law).

a

0n 1n2n

1n2n

Cladding

Core

END VIEWAXIAL CROSS-SECTION

Answer : 2

122

21 )()sin( nna

Page 12: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

COMPARISON OF MULTIMODE AND SINGLE MODE FIBRE GEOMETRIES

Can not use ray analysis for SMF - use only modal analysis

Can use ray analysis

Not a ray!

Page 13: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

CAUSES OF FIBRE LOSS

Page 14: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

FIBRE ATTENUATION

Loss in db =

in

out

P

P10log10

Page 15: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

OPTICAL FIBRE LINK

(Source: D. M. Spirit & M. J. Mahoney)

Page 16: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

COMPARISON OF MULTIMODE AND SINGLE MODE FIBRE GEOMETRIES

Can not use ray analysis for SMF - use only modal analysis

Can use ray analysis

Not a ray!

Page 17: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

DIFFERENT PATH LENGTHS IN MULTIMODE FIBRES

The velocity in the z direction depends on the angle of the ray

A spread of path lengths gives a spread of arrival times

This spreads a sharp pulse and limits the bit-rate

1n

c

zV

cos1n

cvz

Use ray analysis:

Page 18: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

ADVANTAGES OF OPTICAL FIBRES

1. LOW LOSS2. HIGH BANDWIDTH3. LOW MATERIAL PRICE4. LOW WEIGHT5. LOW EMI (INTERFERENCE)

Page 19: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

GENERATION AND DETECTION OF PHOTONS

Emission

Stimulated Emission

Detection

hfEE

hfE

12

Page 20: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

ENERGY LEVELS IN A SUITABLE

SEMICONDUCTOR

Photodiode LED Laser Diode

Page 21: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

DETECTION OF PHOTONS

Page 22: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

REQUIREMENTS FOR LASING

Source: Ghatak

•Population inversion

•Optical gain

•Mirrors

Page 23: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

EARLY LASER DIODE

Source: Ghatak

Page 24: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

LIGHT CONCENTRATED IN ACTIVE REGION OF LASER

Page 25: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

LIGHT POWER VS CURRENT

Page 26: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

SPECTRA OF LED AND LASER DIODE

Page 27: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

SINGLE AND MULTIMODE LASER DIODES

Page 28: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

DISPERSION (PULSE SPREADING) IN SMF

Since velocity depends on n, a small change in n with wavelength can affect the arrival time of signals of differentwavelengths and cause them to overlap.

Page 29: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

SINGLE MODE FIBRE DISPERSION

(Source: D. M. Spirit & M. J. Mahoney)

Page 30: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

INTERSYMBOL INTERFERENCE

Dispersion (pulse spreading) can cause pulses to overlap and limit bit-rate

(Source: G. Keiser)

Page 31: PHOTONS AND FIBRES Lecturer : Professor Laurie Cahill

PHOTONS AND FIBRES

What is a photon?

“All these fifty years of conscious brooding have brought me no nearer to the answer to the question, “What are light quanta (photons)?”

Albert Einstein