The development of quantum mechanics makes possible the discovery of new effects, impossible from a classical viewpoint. Perhaps the most popular is the tunnel, where making a quick comparison and bad, it's like throwing a ball at a wall to cross it without touching it. This is how it appears from an analysis of a similar situation, through the Schrödinger equation .
quantum Wall
Consider first what is meant by " wall" and what happens to an electron when it arrives. The energy of a particle is always the sum of its kinetic energy and potential energy. Thus, energy will always be equal to or greater than the potential. The cases in which the energy is lower than potential from classical physics, states represent unattainable by a particle. Thus, the point at which the total energy equals the potential represents a "turning point , the particle can not move forward, but must go back. Is the equivalent of a "wall ."
quantum Wall
Consider first what is meant by " wall" and what happens to an electron when it arrives. The energy of a particle is always the sum of its kinetic energy and potential energy. Thus, energy will always be equal to or greater than the potential. The cases in which the energy is lower than potential from classical physics, states represent unattainable by a particle. Thus, the point at which the total energy equals the potential represents a "turning point , the particle can not move forward, but must go back. Is the equivalent of a "wall ."
In the figure, the electron energy above is greater than the step, and both are superior, losing a bit of kinetic energy. Below the electron instead he should go back after reaching the point where its energy is equal to the potential energy, and therefore its kinetic energy is zero at that point.
Consider the situation of the second electron from the quantum point of view, with the Schrödinger equation.
The equation to solve is:
whose solution we saw in the previous entry , is a combination of sine and cosine. The combination of sine and cosine, by Euler's formula is equivalent to an exponential function imaginary and more useful for the analysis that follows. Thus, the wave function can be expressed generally as:
As we saw earlier, k (the wave vector ) is related to the angular momentum and therefore the sense that the particle moves. A + means that moves in the direction of x increasing (going from left to right). The sign - describes a movement in the opposite direction. As the picture has been raised, we are in the first case, ie, the electron moves from left to right, whereas in the wave function describes the first term ( k positive). Therefore, in our case, you should choose B = 0 to cancel the second term.
Let's see the two regions of space that defines the step. On the left, (EV) is a positive quantity (total energy greater than the potential), and the wave equation represents a free electron (an imaginary exponential, or a combination of sine and cosine). In contrast, in the right area, (EV) is negative (energy less than the potential energy), the wave vector is imaginary , and the wave function represents a real exponentially decreasing. That is, although it is a forbidden zone as classical physics, in quantum mechanics a particle can exist in that area, but with a diminishing likelihood as deeply into the wall.
The distance that an electron can penetrate into the forbidden zone before your chance is almost nil, depends on the difference between energy and the value of the potential. The greater the difference EV, the probability falls more rapidly. In the extreme case in which V tends to infinity, the penetration depth tends to zero, ie, the electron does not enter into the wall (as we assumed when we spoke of quantum well).
The tunnel effect
Therefore, a particle can penetrate a wall of potential, something impossible according to classical physics. A particle can penetrate a distance (small), although the probability of finding the particle at that location decreases as depth. What if the potential wall finishes before this probability is terminated, or reduced too?. In this case, the "other side " from the wall of the wave function again described by a free electron. It is therefore possible that an electron reaches a barrier, the cross, and appears on the other side of it, with a certain probability, although less than it did before crossing the barrier.
The probability of crossing the barrier depends on the mass of the particle, the barrier height, but above all, of its width. The typical distances that probability is sufficient to tunnel is in the order of angstroms and nanometers. Alpha decay
The emission of alpha particles is related to the tunnel effect. An alpha particle is an atom composed of 2 protons and 2 neutrons, not electrons. Corresponds to a nucleus of helium 4 (4 I 2 +). An atom with a large number of protons and neutrons keeps these particles stuck together by the strong interaction. An outline of the potential energy inside an atom is as follows:
There is an area of \u200b\u200bpotential barrier at the transition between the strong interaction domain and the electrostatics. Overcoming this barrier would require making a lot of energy. However, an alpha particle is able to cross the barrier by tunnel effect, breaking up the nucleus to which it belonged.
The scanning tunneling microscope
The tunnel is now the basis of some devices such as diodes, lasers and detectors. But one of the most important is related to the surface microscopy.
View STM: Scanning tunneling microscope