Reflection of Light on Mirrors: Why & How?

Click For Summary
SUMMARY

The discussion centers on the atomic mechanisms behind the reflection of light on mirrors, specifically how photons interact with electrons in materials. It establishes that specular reflection occurs in metals, where electrons in the conduction band collectively oscillate when excited by incoming photons. This collective motion resembles dipole antennas, which leads to the reflection of light across the normal line. The conversation highlights the significance of understanding the atomic scale interactions that govern optical phenomena.

PREREQUISITES
  • Understanding of specular reflection and Snell's law
  • Basic knowledge of photon behavior and wavelength
  • Familiarity with atomic structure and electron behavior in solids
  • Concept of conduction bands in metals
NEXT STEPS
  • Research the principles of Snell's law in optics
  • Study the behavior of photons and their interactions with matter
  • Explore the concept of conduction bands and electron oscillation in metals
  • Investigate the corpuscular theory of light and its historical context
USEFUL FOR

Physicists, materials scientists, and anyone interested in the fundamental principles of light reflection and atomic interactions in optics.

nhmllr
Messages
183
Reaction score
1
I understand why a ball's velocity vector is reflected across the line normal to the wall when it hits the wall. Why does this happen with light and a mirror? What is happening atomically for an atom to take in a photon and spit it out across the normal line?
 
Physics news on Phys.org
(I did post this in the Classical Physics section a few days ago, but I got no helpful replies and figured this would be a better forum.)

I understand why a ball's velocity vector is reflected across the line normal to the wall when it hits the wall. Why does this happen with light and a mirror? Intuitively it makes sense, but what is happening atomically for an atom to take in a photon and spit it out across the normal line?
 
Last edited:
Ohh...I remember something talking about this but I'll have to do some searching...I don't remember if it was in a book I have or on the internet somewhere. I'll see if I can get back to you.
 
Remember that an optical photon has a wavelength of hundreds of nanometers, while an atom is much smaller than this. The photon excites a region of the solid, not just an individual atom.

Specular reflection, in which Snell's law is obeyed, takes place in metals, where some of the electrons pass freely from one atom to another in what is known as the conduction band. The incoming photon excites a collective oscillation of these electrons. The effect of their motion is very similar to the usual simplified picture, of electrons acting as little dipole antennas all in phase.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 57 ·
2
Replies
57
Views
5K
  • · Replies 16 ·
Replies
16
Views
3K
  • · Replies 14 ·
Replies
14
Views
4K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 15 ·
Replies
15
Views
2K
  • · Replies 18 ·
Replies
18
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 15 ·
Replies
15
Views
2K