The Hall effect is a phenomenon first discovered by Edwin Hall in 1879 that creates a voltage difference (the Hall voltage) between the current in a conductor and an applied magnetic field. The diversity of this effect requires us to explore more than just the ordinary Hall effect, but also to have a deeper understanding of the existence of gap effects and the differences between them.
The Hall effect is determined by the characteristics of the current in the conductor and is closely related to the type and properties of the charge carriers carried by the current.
The ordinary Hall effect is the voltage difference that occurs on both sides of a conductor when an electric current flows through it and is in a magnetic field perpendicular to the current. This effect can be observed in any homogeneous material. However, compared to the ordinary Hall effect, the void effect occurs within the voids (or holes) in semiconductors or metal plates. When current passes through a contact point located at the boundary of the void, this means that charge flows in the material outside the void.
When this gap effect occurs, a voltage difference appears on different sides of the line connecting the current contacts, depending on the applied magnetic field, and has an opposite sign to that of the ordinary Hall effect. The formation of this condition depends solely on the current injected into the gap, and the generated Hall voltage cannot be explained by the current contribution from outside the conductor.
The observation of the void effect not only demonstrates the diversity of the Hall effect, but also prompts us to re-understand the current behavior in different structures.
Fascinatingly, both Hall effects can be present in the same device, for example by placing a rectangular void inside a thin rectangular element with a boundary, so that both the ordinary Hall effect from the outer boundary and the inverse Hall effect from the inner boundary can be observed simultaneously. In such an installation, the two effects reveal their interconnectedness in a striking way.
The realization of this superposition not only deepens the understanding of the classical Hall effect, but also shows how the behavior of current in different structures affects the generation of electric fields and the response of voltage, allowing researchers to explore more levels of physical mechanisms.
The existence of the Hall effect is closely related to the current characteristics in the conductor. Electric current is carried by many small charge carriers (usually electrons). When a magnetic field is applied, these charges are affected by the Lorentz force and their paths are deflected. This causes an accumulation of charge on one side of the material and a lack of flowing charge on the other side, thus causing an electric field to form within the conducting material.
This asymmetric charge distribution causes the voltage difference to persist as long as current continues to flow.
While the basic idea of the Hall effect applies to many conductors, its manifestations are particularly diverse in semiconductors. For example, the concentration and mobility of carriers are different in n-type and p-type semiconductors, which makes the formula for the Hall coefficient more complicated. In these materials, the Hall effect can also determine the type of charge carrier, whether it is an electron or an electron's "hole."
With these results, researchers can better understand and design semiconductors, which are crucial for many applications, such as optoelectronics and sensor technology.
With the continuous advancement of science and technology, the application areas of the Hall effect are also expanding. From the quantum Hall effect to the spin Hall effect, these new forms of the Hall effect have opened up new research directions in fields such as materials science and quantum computing. Researchers are trying to exploit phenomena that go beyond the traditional Hall effect in order to achieve more precise and flexible technological breakthroughs.
As our understanding of the Hall effect deepens, its applications are becoming more and more widespread, but can we predict another layer of meaning hidden in the material world?