100% transmission through a potential barrier

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SUMMARY

The discussion centers on the behavior of a particle of energy E incident upon a potential barrier of height V0 and thickness a, specifically when E > V0. It establishes that the transmission coefficient can reach 100% under certain conditions. The conversation explores the implications of destructive and constructive interference, particularly how the path difference of the reflected waves influences the transmission outcomes. The key point is that constructive interference occurs when the path difference is an integral multiple of the wavelength λ', leading to enhanced transmission through the barrier.

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  • Quantum mechanics principles, specifically wave-particle duality
  • Understanding of potential barriers and tunneling phenomena
  • Knowledge of interference patterns in wave physics
  • Familiarity with the concept of transmission coefficients in quantum mechanics
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  • Study the mathematical derivation of the transmission coefficient for quantum tunneling
  • Explore the implications of wave-particle duality in quantum mechanics
  • Learn about the conditions for constructive and destructive interference in wave functions
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Students and professionals in physics, particularly those focusing on quantum mechanics, as well as researchers interested in wave behavior and potential barriers in particle physics.

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A particle of energy ##E## is incident upon a potential barrier of potential ##V_0## and of thickness ##a##. Given that ##E>V_0##, the transmission coefficient is given by

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Screen Shot 2015-12-09 at 8.45.54 am.png

Screen Shot 2015-12-09 at 8.46.09 am.png


If destructive interference occurs when the path difference between the two reflected waves (at points ##x=0## and ##x=a##) is half-integral number of ##\lambda'##, then shouldn't constructive interference occurs when the path difference is integral number of ##\lambda'##?
 
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The extra path length traveled by the wave that reflects off the back side of the barrier is 2a. That wave travels through the barrier, is reflected off the back side, and travels through the barrier again, in the opposite direction.
 
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