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🔋College Physics I – Introduction Unit 30 Review

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30.5 Applications of Atomic Excitations and De-Excitations

30.5 Applications of Atomic Excitations and De-Excitations

Written by the Fiveable Content Team • Last updated August 2025
Written by the Fiveable Content Team • Last updated August 2025
🔋College Physics I – Introduction
Unit & Topic Study Guides

Atomic Excitations and De-Excitations

When electrons jump between energy levels in an atom, they absorb or emit photons. These transitions are the basis for technologies ranging from fluorescent microscopes to lasers to holograms. This section covers how those transitions work and why they matter.

Quantum Mechanics and Atomic Transitions

Electrons in an atom can only occupy specific, discrete energy levels dictated by quantum mechanics. When an electron gains or loses energy, it jumps between these levels. There are three key types of transitions:

  • Absorption: An electron absorbs a photon whose energy exactly matches the gap between two levels, jumping to a higher energy state.
  • Spontaneous emission: An electron in an excited state randomly drops to a lower level, releasing a photon. The photon's energy equals the energy difference between the two levels: E=hfE = hf, where hh is Planck's constant and ff is the photon's frequency.
  • Stimulated emission: An incoming photon causes an excited electron to drop to a lower level, emitting a second photon that is identical to the first in wavelength, phase, and direction. This is the mechanism that makes lasers possible.
Process and applications of fluorescence, Frontiers | A Comprehensive Review of Fluorescence Correlation Spectroscopy

Fluorescence

In fluorescence, an atom or molecule absorbs a high-energy photon and gets excited. Rather than returning directly to the ground state, the electron often loses a small amount of energy to internal processes (like vibrations in a molecule) before emitting a photon. The emitted photon therefore has a longer wavelength (lower energy) than the absorbed photon.

This shift in wavelength is useful because you can filter out the excitation light and see only the fluorescent glow. Key applications include:

  • Spectroscopy: Analyzing the wavelengths of fluorescent light reveals information about energy levels and molecular structure.
  • Fluorescence microscopy: Biological samples are tagged with fluorescent dyes that bind to specific structures (cell membranes, particular proteins), allowing researchers to image them with high sensitivity.
  • Fluorescent labeling: Molecules of interest are tagged with fluorescent markers for tracking. This is widely used in DNA sequencing and drug discovery.
Process and applications of fluorescence, Frontiers | Laboratory Microprobe X-Ray Fluorescence in Plant Science: Emerging Applications and ...

Metastable States

Most excited states are short-lived: electrons typically drop back down in nanoseconds. A metastable state is an excited state with an unusually long lifetime, on the order of milliseconds to seconds. The transition back to the ground state is "forbidden" by quantum selection rules, meaning it's not truly impossible but is very unlikely, so the electron lingers.

Metastable states matter because they:

  • Act as intermediate steps in multi-step excitation processes (used in atomic clocks and plasma displays)
  • Enable population inversion, which is essential for laser operation. Because electrons stay in metastable states longer, you can build up a large population of excited atoms before they decay.
  • Allow atoms or molecules to store energy temporarily, which is important in energy transfer processes and photochemical reactions

Laser Operation

A laser (Light Amplification by Stimulated Emission of Radiation) produces a beam of light that is coherent (all waves in phase), monochromatic (single wavelength), and highly directional. Here's how it works, step by step:

  1. Pumping: An external energy source (called the pump) excites electrons in the active medium to a higher energy level. The pump can be an electrical current, a flashlamp, or even another laser.
  2. Population inversion: The pump pushes enough electrons into a metastable excited state that more electrons are in the excited state than in the ground state. Under normal thermal equilibrium, the ground state always has the most electrons, so this is a non-equilibrium condition that must be actively maintained.
  3. Stimulated emission: A photon passing through the medium encounters an excited electron and stimulates it to emit an identical photon. Now there are two photons traveling together, in phase and in the same direction.
  4. Optical amplification: The active medium sits between two highly reflective mirrors (an optical resonator, often called a Fabry-Pérot cavity). Photons bounce back and forth, triggering more stimulated emission with each pass. One mirror is slightly less reflective, allowing a fraction of the light to escape as the laser beam.

The active medium determines the laser's wavelength. Common types include gas lasers (like helium-neon), solid-state lasers (like Nd:YAG), and semiconductor diode lasers.

Population inversion is the critical requirement. Without it, absorption dominates over stimulated emission, and the medium dims the light instead of amplifying it.

Holography

Holography is a technique that records and reconstructs the full wavefront of light scattered from an object, producing a true three-dimensional image. Unlike a photograph, which captures only intensity, a hologram also captures the phase of the light.

How a hologram is created:

  1. A laser beam is split into two: a reference beam and an object beam.
  2. The object beam illuminates the object, and the scattered light reaches a recording medium (like a photographic plate).
  3. The reference beam also reaches the recording medium, where it overlaps with the object beam.
  4. The two beams create an interference pattern of bright and dark fringes, which is recorded on the medium. This pattern encodes both the intensity and phase information.

To view the hologram, you illuminate it with the reference beam. The recorded interference pattern diffracts the light, reconstructing the original wavefront so your eyes perceive a 3D image.

Three physics principles are central to holography:

  • Interference: The superposition of two waves produces regions of constructive interference (bright) and destructive interference (dark).
  • Diffraction: Light bends around structures in the hologram's recorded pattern, redirecting it to reconstruct the image.
  • Coherence: The light source must have a constant phase relationship over time and space. Lasers provide the high coherence needed for stable interference patterns. Ordinary light sources are too incoherent to produce usable holograms.

Practical applications of holography include:

  • Security: Holograms on credit cards, banknotes, and product packaging are difficult to counterfeit because they require precise optical setups to produce.
  • Data storage: Holographic memory can store information in three dimensions, achieving very high data densities.
  • Holographic displays: 3D images viewable without special glasses, used in applications like automotive head-up displays.
  • Interferometry: Comparing holograms taken at different times reveals tiny surface deformations, vibrations, or changes in refractive index. This is used for non-destructive testing and strain analysis in engineering.