Materials Science: Unit II(a): Electrical Properties of Materials

Tunneling

Electrical Properties of Materials

According to classical ideas, a particle striking a hard wall has no chance of leaking through it.

TUNNELING

• According to classical ideas, a particle striking a hard wall has no chance of leaking through it. But, the behaviour of a quantum particle is different due to the wave nature associated with it.

• We know that when an electromagnetic wave strikes at the interface of two media, it is partly reflected and partly transmitted through he interface and enters the second medium.

• In a similar way the de Broglie wave also has a possibility of getting partly reflected from the boundary of the potential well and partly penetrating through the barrier.

• Fig. 2.9 shows a particle with energy E < V approaching potential barrier of height V.

• An electron of total energy E approaches the barrier from the left. From the view-point of classical physics, the electron would be reflected from the barrier because its energy E is less than V.

• For the particle to overcome the potential barrier, it must have an energy equal to or greater than V.


Quantum mechanics leads to an entirely new result. It shows that there is a finite chance for the electron to leak to the other side of the barrier.

It is noted that the electron tunneled through the potential barrier and hence in quantum mechanics, this phenomenon is called tunneling.

The transmission of electrons through the barrier is known as barrier penetration.

Materials Science: Unit II(a): Electrical Properties of Materials : Tag: : Electrical Properties of Materials - Tunneling


Materials Science: Unit II(a): Electrical Properties of Materials



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