1. LIGHT and MATTER Chapters 11 & 12

2. Originally performed by Young (1801) to demonstrate the wave-nature of light. Has now been done with electrons, neutrons, He atoms among others. D θ d Detecting screen Incoming coherent beam of particles (or light) y Alternative method of detection: scan a detector across the plane and record number of arrivals at each point. THE DOUBLE-SLIT EXPERIMENT For particles we expect two peaks, for waves an interference pattern

3. PHOTOELECTRIC EFFECT When UV light is shone on a metal plate in a vacuum, it emits charged particles (Hertz 1887), which were later shown to be electrons by J.J. Thomson (1899). Electric field E of light exerts force F=-eE on electrons. As intensity of light increases, force increases, so KE of ejected electrons should increase. Electrons should be emitted whatever the frequency ν of the light, so long as E is sufficiently large For very low intensities, expect a time lag between light exposure and emission, while electrons absorb enough energy to escape from material Classical expectations Hertz J.J. Thomson I Vacuum chamber Metal plate Collecting plate Ammeter Potentiostat Light, frequency ν

4. COMPTON SCATTERING X-ray source Target Crystal (selects wavelength) Collimator (selects angle) θ Compton (1923) measured intensity of scattered X-rays from solid target, as function of wavelength for different angles. He won the 1927 Nobel prize. Result: peak in scattered radiation shifts to longer wavelength than source. Amount depends on θ (but not on the target material).

5. But what actually happened? http://phet.colorado.edu/en/simulation/photoelectric Energy of emitted electrons did not depend on the intensity of the light Each material had a unique cut-off frequency The graph of stopping voltage versus frequency was a straight line of slope = “h”. PHOTOELECTRIC EFFECT

6. Free electrons must escape

7. Gradient = h

8. Work Function W = hf o where h = 6.63 X 10 -34 js -1 and f o is the threshold frequency Ek (max) = ½ mv max 2 = hf –W = max KE of released electrons Where hf = incident photon energy W = work function

9. Momentum?

10. Longer wavelength?

11. Momentum of a photon

12. De Broglie and matter waves

13. Electron and X-rays

14. Cricket balls

15. If light can exhibit particle like behaviour, can matter exhibit wavelike behaviour? http://www.youtube.com/watch?v=uPPyYhHOPb0 De BROGLIE WAVELENGTH

16. What is Light? What is Matter? WAVE-PARTICLE DUALITY In 1924 Einstein wrote:- “ There are therefore now two theories of light, both indispensable, and … without any logical connection.” Evidence for wave-nature of light Diffraction and interference Evidence for particle-nature of light Photoelectric effect Compton effect

17. SAC Can you sketch a diagram illustrating the double slit interference experiment? Can you explain why light passing through two narrow slits produces a pattern? Do you know why double slit interference supports the wave theory of light? Can you describe the photoelectric effect experiment ie. how it was conducted, the apparatus used and what results were obtained? Do you know why the wave theory could not explain the photoelectric effect? Can you sketch a diagram of an electron diffraction experiment? Do you know how this experiment showed that particles can behave like waves?

18. Photoelectric Effect Number 1 Higher intensity light produced greater values of the maximum photocurrent the maximum photocurrent was directly proportional to the light intensity Number 2 This minimum voltage which causes all electrons to turn back is called the stopping voltage. Number 3 Brighter light did not increase the kinetic energy of the electrons emitted from the cathode

19. Photoelectric Effect 4.The stopping voltage depended on both the frequency of the light and on the material of the electrode. In fact, for each material there was a minimum frequency required for electrons to be ejected. Below this cut-off frequency no electrons were ever ejected, no matter how intense the light or how long the electrode was exposed to the light. Above this frequency a photocurrent could always be detected. The photocurrent could be detected as quickly as 10-9 s after turning on the light source. This time interval was independent of the brightness of the light source.

20. The Electron Volt

21. Photoelectric Effect

23. Atomic Viewpoint

24. Were deflected by magnetic fields Could push a paddle wheel and carried momentum Could pass through metals without damaging them Travelled more slowly than light Were negatively charged Carried energy Travelled in straight lines Cathode Rays

26. Emission Spectra

28. Emission vs Absorption Spectra

29. Emission Spectrum

30. Absorption Spectrum

31. Equations