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Chapter 38: Photons and Quantum Mechanics

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1 Chapter 38: Photons and Quantum Mechanics
Question: What did Albert Einstein win the Nobel Prize in Physics for ? Special Relativity ? General Relativity ? Swedish Academy: The Nobel Prize in Physics 1921 was awarded to Albert Einstein "for his services to Theoretical Physics, and especially for his discovery of the law of the photoelectric effect".

2 Chapter 38: Photons and Quantum Mechanics
Our learning goals in this chapter: To consider the fundamental constituent of light, the photon To study the ejection of an electron by an incident photon, the photoelectric effect To understand how the photon concept explains x-ray production, x-ray scattering (Compton scattering), and e+ e- pair production To interpret light diffraction and interference in the photon picture To introduce the Heisenberg uncertainty principle

3 Photoelectric Effect

4 Photoelectric Effect Interesting fact: Blue light striking cesium causes the cesium to emit electrons. Red light does not. Einstein’s explanation: Light comes in photons. To emit an electron, the cesium atom must absorb a single photon whose energy exceeds the ionization energy of the outermost electron in cesium. A blue photon has enough energy; a red photon does not. Photoelectric effect

5 Photoelectric Effect Apparatus
Done at UH in PHYS274L

6 Photoelectric Effect Master Equations
Maximum kinetic energy of the electron is the energy from the photon minus the “work function” ϕ “Stopping potential” V0 The current at which the photoelectron current stops

7 Photon Quantization Master Equations
where h=6.63 x 10-34J-s Question: How can we express the photon energy in terms of the photon wavelength ? Ans: use f = c/λ (Recall c=λf) Question: What is the photon momentum in terms of wavelength or frequency ? (but wait, the massless photon has momentum ?) From special relativity

8 Einstein’s explanation of the photoelectric effect
A photon carries a discrete amount of energy. For light of frequency f and wavelength λ, this energy is E = hf or E = (hc)/λ, where h is Planck’s constant × 10−34 J • s. This explains how the energy of an emitted electron in the photoelectric effect depends on the frequency of light used (see Figure on the right). The momentum of a photon of wavelength λ is p = h/λ. “Photons are quantized”

9 The photoelectric effect—examples
This is also called ϕ, in the master equation for the PE effect

10 The photoelectric effect— many applications
Photons enter the scope and hit a plate ejecting electrons, which then pass through a disk with millions of tiny channels. The current in each channel is amplified. Night vision scopes Solar cells: by the photoelectric effect, photons excite electrons into the conduction band Solar cells

11 Photon quantization— example
A laser pointer with a power output of 5.00mW emits red light (λ=650nm). a) What is the magnitude of the momentum of each photon ? Since light is quantized we only need the frequency or wavelength for this problem. Could also use E=hc/lambda b) What is the energy of each photon ?

12 Photon quantization— example
A laser pointer with a power output of 5.00mW emits red light (λ=650nm). b) How many photons does the laser pointer emit each second ? Calculated in a) How do we calculate the number of photons per second with this information ? Huge but each photon has a very small energy

13 Photoelectric effect— example (how to determine h)
For a particular cathode material in a photoelectric effect experiment, you measure stopping potentials V0=1.0 V for light of wavelength λ=600nm, 2.0 V for 400nm and 3.0V for 300 nm. a) Determine the work function, ϕ for this material, and then the value of Planck’s constant h. Question: Suppose we plot V0 vs f (frequency). What does the graph look like ? The vertical intercept is -ϕ/e=-1.0V The slope of the graph is h/e

14 Photoelectric effect— example (how to determine h)
For a particular cathode material in a photoelectric effect experiment, you measure stopping potentials V0=1.0 V for light of wavelength λ=600nm, 2.0 V for 400nm and 3.0V for 300 nm. The slope of the graph is h/e Let’s take the 3.0V and -1V (y-intercept) points to calculate the slope.


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