Potential barrier
1. What a Potential Barrier Is
Consider 1D potential step/barrier:
Particle energy incident from left. Classically: if , transmit over; if , reflect, cannot enter barrier. Quantum: wave penetrates, even has non-zero transmission (tunneling, next topic); has partial reflection even above barrier due to wave mismatch.
2. TISE in Three Regions
Let
in I/III (free),
if (propagating inside), or
imaginary if (evanescent, decaying).
General solutions:
- I:
(incident + reflected)
- II:
if , or
decaying/growing if (physically keep decaying).
- III:
(transmitted only, no incoming from +∞)
Apply continuity and at and (where jumps finite) ⇒ solve for (reflection amplitude ) and () ⇒ reflection
, transmission
with .
3. Results
- :
— oscillates with ; at resonance when (barrier transparent like Fabry-Perot). Even with enough energy, some reflection — unlike classical.
- : replace ⇒
⇒
for thick barrier — exponential decay, not zero (next topic tunneling).
4. Worked Checks
(a) High barrier V0=2E, a=1 nm, electron E=1 eV: κ=√(2m(V0-E))/ħ=√(2·9.1e-31·1.6e-19)/1.05e-34≈5.1e9 m⁻¹ ⇒ κa≈5.1 ⇒ T≈ e^{-10.2}·factor≈3e-5 small but not zero ✓
(b) At resonance k2 a=π ⇒ T=1 even though V0≠0 ⇒ resonant tunneling.
(c) Classical would predict T=0 for E<V0, but quantum gives ~e^{-2κa}.
5. Exam Points
- Sketch step/barrier — 3 marks, frequent.
- Write TISE solutions in three regions with — 5 marks, very frequent.
- State continuity of at boundaries — 3 marks.
- Give formula for and mention resonance — 5 marks, frequent.
- Mention for preview — 3 marks.