38-1 The Photon, the Quantum of Light#
Prompts
How is light quantized? What is a photon? What is the smallest amount of energy a light wave of frequency \(f\) can have?
Write the photon energy formula \(E = hf\) in terms of wavelength \(\lambda\). What is the Planck constant \(h\)?
Describe photon absorption and photon emission by an atom. What happens to the photon in each case?
A 100 W lamp emits visible light (average \(\lambda \approx 550\) nm). Estimate the rate at which photons are emitted. (Hint: \(P = (\text{rate}) \times (\text{energy per photon})\).)
Why did classical wave theory suffice in earlier chapters, but quantum physics becomes essential for single-photon experiments?
Lecture Notes#
Overview#
Quantum physics studies the microscopic world, where many quantities are quantized—they exist only in certain minimum (elementary) amounts or integer multiples thereof.
Light is quantized: electromagnetic radiation exists in elementary amounts called photons. The energy of a photon of frequency \(f\) is \(E = hf\).
Absorption and emission of light occur in discrete events: one photon transfers energy \(hf\) between light and matter.
The classical wave picture (Ch. 33) remains valid for describing propagation; the photon concept is essential when light interacts with matter.
The photon#
In 1905, Einstein proposed that light is quantized. The quantum of light is the photon. For light of frequency \(f\) and wavelength \(\lambda\) (with \(c = f\lambda\)), the energy of a single photon is
where \(h\) is the Planck constant:
The smallest amount of energy a light wave of frequency \(f\) can have is \(hf\)—the energy of one photon. If the wave has more energy, it must be an integer multiple of \(hf\): \(E = nhf\) with \(n = 1, 2, 3, \ldots\). Light cannot have energy \(0.6hf\) or \(75.5hf\).
Wave vs particle
We have treated light as a wave (wavelength, frequency, interference). The photon is a particle-like quantum of that wave. Both descriptions are needed—light exhibits wave-like behavior (diffraction, interference) and particle-like behavior (discrete absorption and emission). This wave–particle duality is a central theme of quantum physics.
Absorption and emission#
When light interacts with matter, the interaction occurs in atoms (or molecules). Each event involves exactly one photon.
Photon absorption: When light of frequency \(f\) is absorbed by an atom, the energy \(hf\) of one photon is transferred from the light to the atom. The photon vanishes; the atom is said to absorb it.
Photon emission: When light of frequency \(f\) is emitted by an atom, an amount of energy \(hf\) is transferred from the atom to the light. A photon appears; the atom is said to emit it.
For an object with many atoms (e.g., sunglasses absorbing light, a lamp emitting light), there are many such absorption or emission events. Each event still involves the transfer of one photon’s worth of energy, \(hf\).
Photon rate, power, and intensity#
If a light source emits power \(P\) at a single frequency \(f\), and each photon has energy \(hf\), the rate at which photons are emitted is
For intensity \(I\) (power per unit area), the rate of photons per unit area is \(I/(hf)\).
Example: lamp
A 100 W lamp emits visible light with average wavelength \(\lambda \approx 550\) nm. Energy per photon: \(E = hc/\lambda \approx (6.6\times 10^{-34})(3\times 10^8)/(550\times 10^{-9}) \approx 3.6\times 10^{-19}\) J. Photon rate: \(R = P/E \approx 100/(3.6\times 10^{-19}) \approx 3\times 10^{20}\) photons/s. Ordinary light involves enormous numbers of photons.
When is quantum physics needed?#
In previous chapters we used classical wave theory for reflection, refraction, interference, and diffraction. That approach works when many photons are involved—the discrete nature of light is averaged out. For single-photon experiments (e.g., sensitive detectors, quantum cryptography), the quantum picture is essential. Modern technology has made such experiments routine in optical engineering.
Summary#
Photon: quantum of light; energy \(E = hf = hc/\lambda\); Planck constant \(h = 6.626\times 10^{-34}\) J·s.
Quantization: light energy exists only in integer multiples of \(hf\).
Absorption: photon transfers \(hf\) to atom; photon vanishes. Emission: atom transfers \(hf\) to light; photon appears.
Photon rate: \(R = P/(hf)\) for power \(P\) at frequency \(f\).