---
title: "Why laser needs population inversion"
subject: "Engineering Physics"
chapter: 6
key: "semester_1/engineering_physics:population-inversion-laser-necessity"
source: https://www.bctengineer.com/q/semester_1/engineering_physics/population-inversion-laser-necessity
site: BCT Engineering
---

# Why laser needs population inversion

Engineering Physics · Chapter 6: Laser and Fiber Optics

- Asked in: 2069 Chaitra, 5 marks
- Video: [Requirements for laser: Population Inversion, Pumping and Metastable State](https://www.youtube.com/watch?v=Ox4IPUaigG0) — Physics Jessy
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_1/engineering_physics/population-inversion-laser-necessity
- Whole chapter: https://www.bctengineer.com/md/semester_1/engineering_physics/chapter-6

## Question

What is population inversion? Explain why laser action cannot occur without population inversion between atomic levels?

## Short answer

Population inversion occurs when a higher energy level has more atoms than a lower one (N₂ > N₁), contrary to thermal equilibrium. Laser action cannot occur without it because net amplification requires stimulated emission to dominate absorption; the net gain rate is Bρ(N₂−N₁), so N₂ > N₁ is essential for light amplification.

## Answer

#### Population inversion
Population inversion is the condition in which the number of atoms N₂ in a higher energy level exceeds the number N₁ in a lower level (N₂ > N₁), which is the opposite of the thermal equilibrium situation.

#### Why laser action needs it
Three radiative processes occur between levels 1 and 2 (E₂ − E₁ = hν):
- **Absorption:** rate = B₁₂ N₁ ρ(ν)
- **Stimulated emission:** rate = B₂₁ N₂ ρ(ν)
- **Spontaneous emission:** rate = A₂₁ N₂ (random phase and direction)

where ρ(ν) is the energy density of the radiation, and Einstein showed B₁₂ = B₂₁.

1. Net gain from an incident beam: (stimulated emission) − (absorption) = B ρ (N₂ − N₁).
2. Amplification of light requires stimulated emission to beat absorption, so N₂ > N₁.
3. At thermal equilibrium, Boltzmann's law gives N₂/N₁ = exp(−hν/kT), which is always less than 1. For red light (632.8 nm) at 300 K, hν = 1.96 eV and kT = 0.0259 eV, so N₂/N₁ = e⁻⁷⁵·⁸ ≈ 10⁻³³. Almost every atom is in the lower level.
4. With N₂ < N₁ a beam of light is **absorbed** more than it is amplified; the intensity falls along the medium. At best, with N₂ = N₁ the medium is transparent (absorption equals stimulated emission), and no net gain is possible.
5. Spontaneous emission alone produces incoherent light, not a laser beam.
6. To get N₂ > N₁, atoms are pumped to a **metastable** upper level (lifetime about 10⁻³ s instead of 10⁻⁸ s), where they stay long enough to build up a larger population than the lower level. This needs at least three levels, since a two-level system cannot be inverted (pumping stops once N₁ = N₂).
7. With inversion the medium has gain: the intensity grows as I = I₀ e^(γx), and with mirrors feeding the beam back, the gain exceeds the losses and laser oscillation starts.

Hence laser action (Light Amplification by Stimulated Emission of Radiation) cannot occur without population inversion.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What is population inversion?
   A. Equal numbers of atoms in two levels (N2 = N1)
   B. All atoms in the ground state
   C. More atoms in a higher level than in a lower level (N2 > N1)
   D. More atoms in the lower level than the upper (N2 < N1)
   Answer: C. Inversion is the opposite of the thermal-equilibrium situation, where the lower level is more populated. (Key point: Definition)

2. If N2 = N1 between two levels, what happens to an incident beam?
   A. The beam is amplified slightly
   B. The medium is transparent: absorption equals stimulated emission, so no net gain
   C. The beam is strongly absorbed
   D. Spontaneous emission turns it into a laser beam
   Answer: B. Net gain is B rho (N2 - N1), which is zero when N2 = N1. (Key point: Equal populations)

3. Why can thermal equilibrium never provide the needed inversion?
   A. Boltzmann's law gives N2/N1 = exp(-hν/kT), always less than 1
   B. Because B12 is much larger than B21
   C. Because spontaneous emission stops at equilibrium
   D. Because at equilibrium N2 = N1 exactly
   Answer: A. The exponential of a negative number is below 1, so most atoms sit in the lower level (about 10^-33 ratio for red light at 300 K). (Key point: Thermal equilibrium)

4. Why are atoms pumped to a metastable upper level?
   A. Its short lifetime makes emission faster
   B. It makes absorption stronger than stimulated emission
   C. It removes the need for mirrors
   D. Its long lifetime (~10^-3 s) lets population build up above the lower level
   Answer: D. Atoms stay long enough in a metastable level to accumulate and exceed the lower-level population. (Key point: Metastable level)

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