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An electron with initial kinetic energy 5.0 eV encounters a barrier with height \(U_{0}\) and width 0.60 \(\mathrm{nm} .\) What is the transmission coefficient if (a) \(U_{0}=7.0 \mathrm{eV} ;\) (b) \(U_{0}=9.0 \mathrm{eV} ;\) (c) \(U_{0}=\) 13.0 \(\mathrm{eV} ?\)

Short Answer

Expert verified
(a) T ≈ 0.135; (b) T ≈ 0.015; (c) T ≈ 0.00036

Step by step solution

01

Determine the Wave Number inside the Barrier

The wave number inside the barrier for a particle of energy less than the barrier height is given by:\[ k = \frac{\sqrt{2m(U_0 - E)}}{\hbar} \]where \( m = 9.11 \times 10^{-31} \text{ kg} \) is the mass of the electron, \( \hbar = 1.05 \times 10^{-34} \text{ J} \cdot \text{s} \) is the reduced Planck's constant, \( U_0 \) is the barrier height, and \( E = 5.0 \text{ eV} = 8.0 \times 10^{-19} \text{ J} \) is the initial kinetic energy. You need to calculate \( k \) for each value of \( U_0 \).
02

Calculate the Transmission Coefficient

The transmission coefficient \( T \) can be calculated using the formula:\[ T = \left(1 + \frac{U_0^2 \sinh^2(kL)}{4E(U_0 - E)}\right)^{-1} \]For each \( U_0 \), compute \( \sinh(kL) \) where \( L = 0.60 \times 10^{-9} \text{ m} \). Substitute \( k \) from Step 1 into the expression to find the transmission coefficient for each case.
03

Apply Calculations for Case (a) \(U_0=7.0 \, \text{eV}\)

1. Convert \( U_0 = 7.0 \, \text{eV} \) to joules: \( U_0 = 7.0 \times 1.6 \times 10^{-19} \, \text{J} \).2. Calculate the wave number \( k \) using the formula from Step 1.3. Find the transmission coefficient \( T \) using the formula from Step 2.
04

Apply Calculations for Case (b) \(U_0=9.0 \, \text{eV}\)

1. Convert \( U_0 = 9.0 \, \text{eV} \) to joules: \( U_0 = 9.0 \times 1.6 \times 10^{-19} \, \text{J} \).2. Calculate the wave number \( k \) using the formula from Step 1.3. Find the transmission coefficient \( T \) using the formula from Step 2.
05

Apply Calculations for Case (c) \(U_0=13.0 \, \text{eV}\)

1. Convert \( U_0 = 13.0 \, \text{eV} \) to joules: \( U_0 = 13.0 \times 1.6 \times 10^{-19} \, \text{J} \).2. Calculate the wave number \( k \) using the formula from Step 1.3. Find the transmission coefficient \( T \) using the formula from Step 2.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Wave Number
In quantum mechanics, the wave number is a crucial concept used to describe the behavior of a particle, particularly when encountering a potential barrier. The wave number (\( k \)) inside a barrier gives us an insight into how the wave function oscillates in a region where a particle has less energy than the barrier height. It is calculated using:\[ k = \frac{\sqrt{2m(U_0 - E)}}{\hbar} \]where:
  • \( m \) is the mass of the particle (e.g., electron),
  • \( U_0 \) is the height of the barrier (potential energy),
  • \( E \) is the kinetic energy of the particle,
  • \( \hbar \) is the reduced Planck's constant.
The wave number is essential for determining how likely a particle is to tunnel through a barrier rather than being reflected back. For an electron with a given kinetic energy encountering different potential barriers, calculating the wave number helps us understand how deep the particle's wave function penetrates the barrier.
Transmission Coefficient
The transmission coefficient (\( T \)) measures the probability that a particle with a given energy will tunnel through a potential barrier instead of being reflected. Tunneling is a distinctive quantum phenomenon where particles move through a barrier they classically shouldn't be able to cross. The formula for the transmission coefficient is:\[T = \left(1 + \frac{U_0^2 \sinh^2(kL)}{4E(U_0 - E)}\right)^{-1}\]where:
  • \( U_0 \) is the barrier potential,
  • \( \sinh \) is the hyperbolic sine function,
  • \( k \) is the wave number (found in the previous section),
  • \( L \) is the width of the barrier,
  • \( E \) is the kinetic energy of the particle.
The transmission coefficient is particularly useful in fields like semiconductor technology and nuclear fusion, where understanding and predicting tunneling probability is crucial. A lower transmission coefficient means the particle is more likely to be reflected, while a higher value indicates a greater chance of tunneling through the barrier.
Barrier Height
In quantum mechanics, the barrier height (\( U_0 \)) is the potential energy of the barrier that a particle encounters. It is a vital factor in determining whether a particle such as an electron can tunnel through a barrier. If the particle's kinetic energy is less than the barrier height, classical physics predicts the particle would not pass through. However, quantum tunneling allows for a non-zero probability of transmission.Barrier height directly influences the wave number and transmission coefficient. As it increases, it becomes more difficult for the particle wave function to penetrate deeply into the barrier. This naturally lowers the probability of tunneling through the barrier, decreasing the transmission coefficient. Understanding barrier height is essential in contexts like quantum tunneling microscopes, which rely on the tunneling principle to visualize atomic details beyond conventional techniques.
Kinetic Energy
Kinetic energy (\( E \)) represents the energy that a particle possesses due to its motion. In the context of quantum tunneling, it is crucial because it influences both the wave number and the transmission coefficient, defining the particle's interaction with the barrier.For an electron encountering a barrier:
  • If the kinetic energy is greater than the barrier height, transmission is almost assured with minimal reflection.
  • When kinetic energy is less than the barrier height, quantum mechanics comes into play, allowing for the possibility of tunneling.
Changes in kinetic energy directly affect the wave number and the transmission coefficient. Higher kinetic energy can lead to smaller wave numbers and higher transmission probabilities, meaning particles can tunnel more easily through a barrier. This nuanced understanding of kinetic energy is pivotal in the design of electronic components like tunnel diodes that exploit tunneling for fast switching characteristics.

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Most popular questions from this chapter

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