{"id":55,"date":"2018-01-14T20:51:28","date_gmt":"2018-01-14T20:51:28","guid":{"rendered":"http:\/\/134.169.6.169\/milq\/?page_id=55"},"modified":"2026-07-22T20:27:25","modified_gmt":"2026-07-22T18:27:25","slug":"11-tunneleffekt","status":"publish","type":"page","link":"https:\/\/www.milq.info\/en\/mehr\/11-tunneleffekt\/","title":{"rendered":"Lesson 11: The tunnel effect"},"content":{"rendered":"
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11.1 The tunnel effect<\/a>\u00a0–\u00a011.2 Progress check<\/a>\u00a0–\u00a011.3 Summary of Chapter 11: The tunnel effect<\/a>\u00a0–\u00a0\u00a0–\u00a0<\/p>\n

\u201cIn the quantum world, it is possible to quickly wangle yourself through an energetically forbidden zone.<\/em>\u201d (Richard Feynman)<\/p>\n

This chapter deals with the quantum theoretical background of this citation. The Nobel Prize for Binnig and Rohrer in 1986 puts the scanning tunneling microscope at the center of the applications of the tunnel effect.<\/p>\n

This chapter contains the fundamentals of, and general information on the tunnel effect, but also makes proposals as to how the tunnel effect can be discussed in schools.<\/p>\n

11.1 The tunnel effect<\/h3>\n

The potential well, in which the electrons are in bound states, was considered in Section 10.1. The potential barrier emerges from the potential well by reflection about the horizontal axis (cf. Fig. 11.1). The potential barrier causes the quantum objects to behave in a completely different way than is the case with the potential well. The bound states with quantized energy levels are missing, for example.<\/p>\n

\"\"<\/p>\n

Fig. 11.1: Potential curve\u00a0\"V_{(x)}\" and total energy \"E \le V_0\"<\/p>\n

In classical physics, the barrier is an obstacle for any particle, and it cannot be overcome if the total energy \"E\" of the particle is less than the height \"V_0\" of the barrier. The situation is different in quantum mechanics:<\/p>\n

A wave coming in from the left is partially reflected, but the remainder passes though the barrier into region III. This happens although region II is forbidden for the quantum object from an energy point of view. The solution of the Schr\u00f6dinger equation provides more details:<\/p>\n

The Schr\u00f6dinger equation for the potential barrier and its solution<\/strong><\/p>\n

The Schr\u00f6dinger equation<\/p>\n

  <\/span>   <\/span>\"\[ \left( \hat{E}_{kin} + V_{(x)} \right) \psi_{(x)} = E \cdot \psi_{(x)} \]\"<\/p>\n

in regions I, II and III is:<\/p>\n\n\n\n\n\n
Region I<\/td>\nRegion II<\/td>\nRegion III<\/td>\n<\/tr>\n
\"\displaystyle {-\frac{\hbar^2}{2m} \frac{d^2}{dx^2} \psi = E \cdot \psi}\"<\/td>\n\"\displaystyle {- \left( \frac{\hbar^2}{2m} \frac{d^2}{dx^2} + V_0 \right) \psi = E \cdot \psi}\"<\/td>\n\"\displaystyle {- \frac{\hbar^2}{2m} \frac{d^2}{dx^2} \psi = E \cdot \psi}\"<\/td>\n<\/tr>\n
rearranged:
\n\"\displaystyle {\frac{d^2}{dx^2} \psi = -\frac{2mE}{\hbar^2} \cdot \psi}\"<\/td>\n		rearranged:
\n\"\displaystyle {\frac{d^2}{dx^2} \psi = - \frac{2m(E-V_o)}{\hbar^2} \cdot \psi}\"<\/td>\n		rearranged:
\n\"\displaystyle {\frac{d^2}{dx^2} \psi = - \frac{2mE}{\hbar^2} \cdot \psi}\"<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

Each of the equations has two independent solution functions. To obtain a solution for the whole region, the parts of the solution have to be suitably combined so that the transitions are continuous and continuously differentiable. One of the possible overall solutions has the following form:<\/p>\n

\"\psi_{(x)} = \left\lbrace<\/p>\n

with<\/p>\n

  <\/span>   <\/span>\"\[ k_1 = \frac{1}{\hbar} \sqrt{2mE} \hspace{15pt} \text{and} \hspace{15pt} k_2 = \frac{1}{\hbar} \sqrt{2m(V_0-E)} \]\"<\/p>\n

Here, only the exponentially decreasing partial solution has been used for region II. In this case, the intensity in region III is only a fraction of the intensity in region I. To a good approximation, this low intensity in region III can be considered as that part of the main wave of region I which has tunneled through.<\/p>\n

Why is this only an approximation?<\/a><\/p>\n

To determine the degree of transmission T, the intensities (squares of the absolute value of the wave function) of the corresponding regions are determined and expressed as a ratio. For the wave function stated above we obtain:<\/p>\n

  <\/span>   <\/span>\"\[ \displaystyle{ T = e^{- \sqrt{2m(V_0-E)} \frac{2a}{\hbar}}} \]\"<\/p>\n

The degree of transmission \"T\" is a measure of how well the barrier can be tunneled through: The higher the barrier compared to the total energy, the lower is the probability that the barrier is tunneled through.<\/p>\n

The tunnel effect in nature and technology<\/a><\/p>\n

The tunnel effect in schools<\/a><\/p>\n

11.2 Progress check<\/h3>\n

After working through Chapter 11, you should be able to answer the following questions:<\/p>\n