Population inversion
1. What It Is
Population inversion = a non-equilibrium condition where upper laser level population exceeds lower:
This is opposite to thermal equilibrium where . With , stimulated emission dominates absorption ⇒ net amplification:
Without inversion, net absorption (attenuation). Inversion is necessary (not sufficient; also need gain > cavity loss) for laser oscillation.
2. Why Not Two-Level System (impossibility)
In a strict two-level system pumped by same photons , rates: . At steady state with large , at best (equalization), never because absorption and stimulated emission have same — pumping equalizes. So two levels cannot give CW inversion with same pump.
3. How to Achieve — Three- and Four-Level Schemes
- Three-level (Ruby): Ground , pump to (broad), fast non-radiative decay to upper laser level (metastable), laser .
- Needs >50% of ground population pumped to to invert vs (since lower is ground) ⇒ high threshold, pulsed often.
- Four-level (Nd:YAG, He-Ne): Pump , fast decay to (upper), laser , fast decay (empty). Lower laser level nearly empty ⇒ easy inversion (small already >), low threshold, CW possible.
So practical lasers use 3 or 4 levels with a metastable upper laser level (long lifetime vs spontaneous) to store population.
4. Worked Checks
Thermal at 300K for λ=600 nm: hν/kT≈ (6.6e-34·5e14)/(1.38e-23·300)≈80 ⇒ N2/N1≈e^{-80}∼10^{-35} negligible.
Three-level Ruby: need pump to lift >50% atoms to E2; pulsed flashlamp does; CW would need huge power.
Four-level He-Ne: pump excites He, transfers to Ne E2; lower Ne E1 quickly empties to ground via collisions ⇒ inversion with small pump.
5. Exam Points
- Define inversion and why needed for net stimulated emission — 5 marks, very frequent.
- Explain why two-level cannot invert (equal ) — 5 marks, very frequent.
- Compare three vs four-level with diagram and threshold difference — 5-7 marks, very frequent.
- Mention metastable state lifetime — 3 marks.