Introduction to Laser Physics - Laser Physics | Lecture Notes - YNetStudyHub
Laser Physics

Introduction to Laser Physics

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This topic provides an overview of the fundamental principles of laser physics, including the concept of stimulated emission, population inversion, and the basic components of a laser system.

Introduction to Laser Physics – Study Notes


1. What Is a Laser?

Term Meaning
Laser Light Amplification by Stimulated Emission of Radiation.
Coherent Light Photons are in phase (constant phase relationship) and travel in the same direction.
Monochromatic Emission at a very narrow wavelength band (Δλ ≪ λ).
Highly Directional Beam divergence typically < 1 mrad.

2. Fundamental Concepts

2.1. Atomic Energy Levels

  • Ground state (E₁) – lowest energy level, most atoms occupy this at thermal equilibrium.
  • Excited state (E₂) – higher energy level; population can be created by pumping.

2.2. Spontaneous vs. Stimulated Emission

Process Trigger Photon Characteristics
Spontaneous emission Random decay of excited atom Random phase, direction, and polarization
Stimulated emission Incident photon with energy hν = E₂ – E₁ Emitted photon copies phase, direction, and polarization of the stimulating photon

2.3. Population Inversion

  • Condition: N₂ > N₁ (more atoms in excited state than ground state).
  • Required for net gain because stimulated emission must out‑balance absorption.

2.4. Gain Medium

  • Material that provides the active transition (e.g., ruby crystal, Nd:YAG, semiconductor quantum wells, gas mixtures).
  • Characterized by gain coefficient g(ν), which depends on wavelength, pump power, and temperature.

3. Laser Cavity (Resonator)

Component Function
Two mirrors (high‑reflectivity & partially transmitting) Form standing‑wave optical resonator; define allowed longitudinal modes.
Optical cavity length L Determines mode spacing: Δν = c / (2L).
Mode selection Achieved with apertures, etalons, or diffraction gratings to enforce single‑frequency operation.

3.1. Longitudinal Modes

  • Integer number q of half‑wavelengths fits into cavity: q·λ/2 = L.
  • Frequency of mode q: ν_q = q·(c/2L).

3.2. Transverse Modes

  • Spatial field distribution described by Hermite‑Gaussian (TEMₘₙ) or Laguerre‑Gaussian patterns.
  • Fundamental mode TEM₀₀ gives the smallest divergence.

4. Rate‑Equation Model (Simplified)

For a two‑level system:

[ \frac{dN_2}{dt}=R_{\text{pump}} - \frac{N_2}{\tau} - B_{21}, \rho(\nu), (N_2 - N_1) ]

[ \frac{d\Phi}{dt}=B_{21}, \rho(\nu), (N_2 - N_1) - \frac{\Phi}{\tau_c} ]

  • (R_{\text{pump}}) – pump rate (atoms s⁻¹).
  • (τ) – spontaneous lifetime.
  • (B_{21}) – Einstein coefficient for stimulated emission.
  • (ρ(\nu)) – photon density in the cavity.
  • (Φ)
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Unit Syllabus 9 Topics
Introduction to Laser Physics
Laser Emission and Properties
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Laser Pumping Mechanisms
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Laser Cavity Design
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Laser Beam Characteristics
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Laser Applications in Science and Technology
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Laser Safety and Hazards
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Advanced Laser Technologies
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Emerging Trends in Laser Physics
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