2. Quantum Mechanics 102 Tunneling and its Applications

3. Interference of Waves and the Double Slit Experiment  Waves spreading out from two points, such as waves passing through two slits, will interfere d Wave crest Wave trough Spot of constructive interference Spot of destructive interference

4. Interpretation  The probability of finding a particle in a particular region within a particular time interval is found by integrating the square of the wave function:  P (x,t) =  |  (x,t)| 2 dx =  |  (x)| 2 dx  |  (x)| 2 dx is called the “probability density; the area under a curve of probability density yields the probability the particle is in that region  When a measurement is made, we say the wave function “collapses” to a point, and a particle is detected at some particular location

5. Particle in a box  (x) = B sin (n  x/a)  (x) |  (x)| 2 n=2 n=3  Only certain wavelengths  = 2a/n are allowed  Only certain momenta p = h/ = hn/2a are allowed  Only certain energies E = p 2 /2m = h 2 n 2 /8ma 2 are allowed - energy is QUANTIZED  Allowed energies depend on well width

6. What about the real world?  Solution has non-trivial form, but only certain states (integer n) are solutions  Each state has one allowed energy, so energy is again quantized  Energy depends on well width a  Can pick energies for electron by adjusting a |  (x)| 2 n=1 n=2 x

7. Putting Several Wells Together  How does the number of energy bands compare with the number of energy levels in a single well?  As atom spacing decreases, what happens to energy bands?  What happens when impurities are added?

8. Quantum wells  An electron is trapped since no empty energy states exist on either side of the well

9. Escaping quantum wells  Classically, an electron could gain thermal energy and escape  For a deep well, this is not very probable

10. Escaping quantum wells  Thanks to quantum mechanics, an electron has a non-zero probability of appearing outside of the well  This happens more often than thermal escape

11. What if free electron encounters barrier? Do Today’s Activity

12. What Have You Seen?  What happens when electron energy is less than barrier height?  What happens when electron energy is greater than barrier height?  What affects tunneling probability? T  e –2kL k = [8  2m(E pot – E)] ½ /h

13. A classical diode  According to classical physics, to get to the holes on the other side of the junction, the conduction electrons must first gain enough energy to get to the conduction band on the p-side  This does not happen often once the energy barrier gets large  Applying a bias increases the current by decreasing the barrier

14. A tunnel diode  According to quantum physics, electrons could tunnel through to holes on the other side of the junction with comparable energy to the electron  This happens fairly often  Applying a bias moves the electrons out of the p-side so more can tunnel in

15. Negative resistance  As the bias is increased, however, the energy of the empty states in the p-side decreases  A tunneling electron would then end up in the band gap - no allowed energy  So as the potential difference is increased, the current actually decreases = negative R

16. No more negative resistance  As bias continues to increase, it becomes easier for conduction electrons on the n-side to surmount the energy barrier with thermal energy  So resistance becomes positive again

17. The tunneling transistor Only electrons with energies equal to the energy state in the well will get through

18. The tunneling transistor As the potential difference increases, the energy levels on the positive side are lowered toward the electron’s energy Once the energy state in the well equals the electron’s energy, the electron can go through, and the current increases.

19. The tunneling transistor The current through the transistor increases as each successive energy level reaches the electron’s energy, then decreases as the energy level sinks below the electron’s energy

20. Randomness  Consider photons going through beam splitters  NO way to predict whether photon will be reflected or transmitted! (Color of line is NOT related to actual color of laser; all beams have same wavelength!)

21. Randomness Revisited  If particle/probabilistic theory correct, half the intensity always arrives in top detector, half in bottom  BUT, can move mirror so no light in bottom! (Color of line is NOT related to actual color of laser; all beams have same wavelength!)

22. Interference effects  Laser light taking different paths interferes, causing zero intensity at bottom detector  EVEN IF INTENSITY SO LOW THAT ONE PHOTON TRAVELS THROUGH AT A TIME  What happens if I detect path with bomb? No interference, even if bomb does not detonate!

23. Interpretation  Wave theory does not explain why bomb detonates half the time  Particle probability theory does not explain why changing position of mirrors affects detection  Neither explains why presence of bomb destroys interference  Quantum theory explains both!  Amplitudes, not probabilities add - interference  Measurement yields probability, not amplitude - bomb detonates half the time  Once path determined, wavefunction reflects only that possibility - presence of bomb destroys interference

24. Quantum Theory meets Bomb  Four possible paths: RR and TT hit upper detector, TR and RT hit lower detector (R=reflected, T=transmitted)  Classically, 4 equally-likely paths, so prob of each is 1/4, so prob at each detector is 1/4 + 1/4 = 1/2  Quantum mechanically, square of amplitudes must each be 1/4 (prob for particular path), but amplitudes can be imaginary or complex!  e.g.,

25. Adding amplitudes  Lower detector:  Upper detector:

26. What wave function would give 50% at each detector?  Must have |a| = |b| = |c| = |d| = 1/4  Need |a + b| 2 = |c+d| 2 = 1/2