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Electromagnetic spectrum and the LASER

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E 2<br />

r(n)<br />

E 1<br />

Laser principles I. Stimulated emission<br />

Elementary radiative processes:<br />

1. Absorption 2. Spontaneous emission 3. Stimulated emission<br />

B 12<br />

•Frequency of transition:<br />

n 12=N 1B 12r(n)<br />

•�E= E 2-E 1=hn<br />

energy quantum<br />

is absorbed.<br />

N 2<br />

N 1<br />

Explanation: two-state atomic or molecular system<br />

E 1, E2 : energy levels, E2>E1<br />

r(n) : spectral power density of external field<br />

N 1, N2 : number of atoms, molecules on <strong>the</strong> given energy level<br />

B 12, A21, B21: transition probabilities between energy levels (Einstein coefficients), B12 = B21<br />

A 21<br />

•Frequency of transition:<br />

n 21=N 2A 21<br />

•E 2-E 1 photons<br />

radiate independently<br />

in all directions.<br />

r(n)<br />

B 21<br />

•Frequency of transition:<br />

n 21=N 2B 21r(n)<br />

•Upon external stimulation.<br />

•Field energy increases.<br />

•Phase, direction <strong>and</strong><br />

frequency of emitted <strong>and</strong><br />

external photons are identical.<br />

Laser principles III. Optical resonance<br />

End mirror<br />

Pumping<br />

Active medium<br />

d=n�/2<br />

Partially<br />

transparent mirror<br />

Resonator:<br />

•two, parallel planar (or concave) mirrors<br />

•Couples part of <strong>the</strong> optical power back in <strong>the</strong> active medium<br />

•Positive feedback -> self-excitation -> resonance<br />

Types of laser<br />

Based on active medium:<br />

1. Solid state lasers<br />

Crystals or glasses doped with metal ions; Ruby, Nd-YAG, Ti-zaphire<br />

Red - infrared spectral range; CW, Q-switched modes, high power<br />

2. Gas lasers<br />

Best known: He-Ne laser (10 He/Ne). Small energy, wide use<br />

CO 2 laser: CO 2-N 2-He mixture; �~10 µm; enormous power (100 W)<br />

Laser beam<br />

3. Dye lasers<br />

Dilute solution of organic dyes (e.g., rhodamine, coumarine); pumped with ano<strong>the</strong>r laser<br />

Large power (in Q-switched mode); Tunable<br />

4. Semiconductor lasers<br />

No need for resonator mirrors (internal reflection)<br />

Red, IR spectral range. Large CW power (up to 100 W)<br />

Beam characteristics not ideal. Wide use due to small size.<br />

Laser principles II. Population inversion<br />

•Amplification depends<br />

on <strong>the</strong> relative population<br />

of energy levels<br />

E 1<br />

E 0<br />

A<br />

F<br />

Active<br />

medium F+dF<br />

dz<br />

Thermal equilibrium Population inversion<br />

•Population inversion only<br />

in multiple-state systems!<br />

•Pumping: electric,<br />

optical, chemical energy<br />

1. Small divergence<br />

Parallel, collimated beam<br />

E 2<br />

Pumping<br />

E 0<br />

E 1<br />

E 0<br />

E 1<br />

Fast relaxation<br />

Metastable state<br />

Properties of laser<br />

2. High power<br />

In continuous (CW) mode: tens, hundreds of watts (e.g., CO 2)<br />

Q-switched mode: instantaneous power is enormous (GW)<br />

Large spatial power density due to small divergence<br />

3. Small spectral width<br />

“Monochrome”<br />

Large spectral power density<br />

4. Polarized<br />

5. Possibility of very short pulses<br />

ps, fs<br />

Laser transition<br />

6. Coherence<br />

phase equivalence, ability for interference<br />

Temporal coherence (phase equivalence of photons emitted at different times)<br />

Spatial coherence (phase equivalence across beam diameter)<br />

4

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