Tunneling effect or barrier penetrability

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    Barrier Tunneling
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SUMMARY

The discussion centers on the tunneling effect and barrier penetrability in quantum mechanics, specifically addressing the behavior of wavefunctions at potential barriers. It is established that the wavefunction for a free particle must remain continuous at the barrier, exhibiting exponential decay within the barrier when the energy (E) is less than the potential (V). This results in a reduced probability of finding the particle outside the barrier, despite no energy loss. The relationship between probability and energy is clarified, emphasizing that knowing the probability of a particle's location does not directly inform about its energy.

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  • Understanding of quantum mechanics principles, particularly wavefunctions
  • Familiarity with potential barriers and tunneling phenomena
  • Knowledge of the mathematical representation of wavefunctions, including exponential decay
  • Concept of energy levels in quantum systems
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The wavefunction associated with a free particle must be continuous at the barrier and will show an exponential decay inside the barrier. Why it shows an exponential decay inside the barrier? After coming out of the barrier, there is reduced probability for the particle. When there is no loss of energy after coming out of the barrier why there is reduced probability?
 
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The wave function goes as e^ikx (plus or minus depending on direction). We have that k is real for E>V, and k is imaginary for E<V. Outside of the barrier, the wave function oscillates, but inside the barrier E<V, so we have that the wave function is exponential decay.

As for the energy, if the barrier is loss-less, then the energy has a % probability to be reflected or transmitted just like the particle. The energy is a property of the particle after all.
 
logearav said:
The wavefunction associated with a free particle must be continuous at the barrier and will show an exponential decay inside the barrier. Why it shows an exponential decay inside the barrier? After coming out of the barrier, there is reduced probability for the particle. When there is no loss of energy after coming out of the barrier why there is reduced probability?

Where does the probability appear in the expression for the particle energy? Those two concepts are distinct. Knowing the probability that a particle will be found in a region of space does not necessarily tell you anything about its energy.
 

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