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How does the width of a potential barrier affect the tunneling probability of a particle, assuming all other parameters remain constant?



The tunneling probability of a particle through a potential barrier decreases exponentially with the width of the barrier, assuming all other parameters (such as the particle's energy, the barrier height, and the particle's mass) remain constant. This means that even a small increase in the barrier width can result in a significant decrease in the probability that the particle will tunnel through the barrier. The relationship between tunneling probability (T) and barrier width (W) is approximately described by the equation T ≈ exp(-2√(2m(V-E))W/ħ), where m is the mass of the particle, V is the potential energy of the barrier, E is the energy of the particle, and ħ is the reduced Planck constant. From this equation, it is clear that the tunneling probability is exponentially dependent on the barrier width (W). Therefore, a wider barrier leads to a dramatically reduced probability of tunneling. This exponential dependence explains why tunneling is typically only significant for very narrow barriers, such as those encountered at the atomic or molecular level. The wider the barrier, the less likely the particle is to tunnel through it, as the wave function decays more rapidly within the barrier.