The barrier length in quantum tunneling

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SUMMARY

The discussion centers on the quantum tunneling barrier length and the transmission coefficient T, defined as T = exp(-2sqrt(2m(U-E)/hbar^2)L). Participants clarify that T represents the probability of a single particle successfully tunneling through the barrier, and integrating over distance is unnecessary if all particles possess the same energy. The conversation emphasizes that T is already squared, negating the need for further squaring in calculations.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly quantum tunneling.
  • Familiarity with the transmission coefficient and its mathematical formulation.
  • Knowledge of the variables involved: mass (m), potential energy (U), kinetic energy (E), and reduced Planck's constant (hbar).
  • Basic calculus for interpreting integrals and probabilities.
NEXT STEPS
  • Study the derivation of the transmission coefficient T in quantum mechanics.
  • Explore the implications of the potential barrier height (U) on tunneling probabilities.
  • Learn about the role of particle energy (E) in quantum tunneling scenarios.
  • Investigate the concept of wave function and its relation to tunneling phenomena.
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Physicists, quantum mechanics students, and researchers interested in quantum tunneling and its applications in fields such as quantum computing and nanotechnology.

Alan Ezra
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Hi,

In transmission coefficient T= exp(-2sqrt(2m(U-E)/hbar^2)L), L, as I interpret it, is the distance of the potential barrier. I am wondering if I have N particles all with kinetic energy E, approaching the barrier, can I integrate the transmission coefficient over a distance from infinity to the potential barrier(the charged radius?), and times the number of particles N, to find out how many of them can penetrate the barrier?

Thank you so much for helping me

best regards
alan
 
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Hello Alan, :welcome:

I checked here and found a different expression. Turns out your ##T## is a simplification for sqrt(2m(U-E)/hbar^2)L >> 1 (and you left out a factor 4E(U-E0)/U2 ).

Point is that this is already the probability for transmission, so no need to integrate.
 
BvU said:
Point is that this is already the probability for transmission

Actually ##|T|^2## is the probability for a single particle to make it through the barrier. But as you say, no need to integrate, provided all the particles have the same energy, and therefore the same ##T##.
 
T is already a square. Not to be squared again.
 
BvU said:
Hello Alan, :welcome:

I checked here and found a different expression. Turns out your ##T## is a simplification for sqrt(2m(U-E)/hbar^2)L >> 1 (and you left out a factor 4E(U-E0)/U2 ).

Point is that this is already the probability for transmission, so no need to integrate.

Hi BvU,

Thanks for the help! So should I use the expression
a326086a233dab558664add1292497b9.png
and multiply it by the number of particles to find out the number of particles tunneled through? And so the expression I gave, the simplified one took a approximation for sinh^2?? Is that right? Thanks.
 
BvU said:
T is already a square.

Right you are. I got confused between t and T=|t|2. :oops:
 

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