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Fermi surface

physical science Maturity 9-11 Next article →

In condensed matter physics, the Fermi surface is a vital concept. It is a surface in reciprocal space that separates filled electron states from empty ones at zero temperature. This surface is essential because it dictates how a material responds to electric, magnetic, or thermal gradients. Essentially, electric currents are caused by changes in the occupancy of states near the Fermi energy. Because of this, the shape of the Fermi surface determines much of a metal's behavior. The study of these surfaces is a specific field called fermiology.

The existence of a Fermi surface comes from the Pauli exclusion principle. This rule states that no two fermions, such as electrons, can occupy the same quantum state. At absolute zero temperature, the enthalpy of electrons must be at its minimum. This means electrons cannot change states because there are no unoccupied lower energy states available. Therefore, all the lowest energy states must be saturated. Electrons fill up every available state below a certain energy level. This maximum energy level is known as the Fermi energy. In momentum space, these particles fill a volume, and the boundary of that volume is the Fermi surface.

The specific shape of the Fermi surface is not always a simple sphere. It is derived from the symmetry and periodicity of the crystalline lattice. It also depends on how electronic energy bands are occupied. For an ideal Fermi gas, the surface is a sphere with a radius determined by the valence electron concentration. However, complex crystal structures create intricate shapes. For example, graphite has an anisotropic Fermi surface. This means its shape varies depending on the direction. Graphite shows both electron and hole pockets where multiple bands cross the Fermi energy.

graphiteFS
graphiteFS

In some metals, the Fermi surface radius is actually larger than the first Brillouin zone. The Brillouin zone is a specific area used to describe the patterns of atoms in a crystal. To manage this, scientists use an extended-zone scheme or a reduced-zone scheme. In a reduced-zone scheme, wavevectors are shown modulo the reciprocal lattice vectors. This keeps the representation closer to the origin in reciprocal space. If a material's Fermi level falls within a gap between energy bands, it will not have a Fermi surface. Such a material is classified as either an insulator or a semiconductor, depending on the size of that bandgap.

Scientists have developed several ways to measure these surfaces experimentally. One method involves observing how transport properties oscillate in strong magnetic fields. This includes the de Haas–van Alphen effect, which involves magnetic susceptibility. It also includes the Shubnikov–de Haas effect, which involves resistivity. These oscillations occur because energy levels are quantized in a plane perpendicular to a magnetic field. Lev Landau first predicted these new states, which are called Landau levels. Later, Lars Onsager proved that the period of these oscillations relates to the cross-section of the Fermi surface.

Fermi surface of Copper measured with 2D ACAR
Fermi surface of Copper measured with 2D ACAR

To observe these oscillations, researchers need very large magnetic fields. The circumference of the cyclotron orbit must be smaller than the mean free path of the particles. Because of this requirement, experiments are often held at specialized facilities. These include the High Field Magnet Laboratory in the Netherlands and the National High Magnetic Field Laboratory in the United States. Another direct technique is angle-resolved photoemission spectroscopy, or ARPES. ARPES allows researchers to resolve the electronic structure of crystals in momentum-energy space.

Fermi surface of BSCCO exp
Fermi surface of BSCCO exp

A third method is called Angular Correlation of electron-positron Annihilation Radiation, or ACAR. This technique uses a positron to probe the momentum density of electrons. When a positron annihilates with an electron, the radiation carries information about the electron's momentum. ACAR is useful because it does not require ultra-high vacuum, cryogenic temperatures, or high magnetic fields. However, it does require samples with a low concentration of vacancies. In 1978, researchers used this to determine a smeared Fermi surface in a 30% alloy.

Fermi surface of BSCCO exp
Fermi surface of BSCCO exp

Understanding the Fermi surface helps explain why certain materials undergo phase changes. Solids with a large density of states at the Fermi level can become unstable at low temperatures. They often form new ground states to release energy. This process involves opening a gap at the Fermi surface. Notable examples of these states include superconductors, which carry electricity without resistance. Other examples include ferromagnets, Jahn–Teller distortions, and spin density waves. By studying fermiology, scientists gain deep insights into the fundamental nature of matter.

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File:Fermi surface of Copper measured with 2D ACAR.jpg
Fermi surface of Copper measured with 2D ACAR.jpg
File:graphiteFS.png
graphiteFS.png
File:Fermi surface of BSCCO exp.jpg
Fermi surface of BSCCO exp.jpg
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