 | Real crystals are three-dimensional and we must consider their band structure in three dimensions, too. |
| | Of course, we must consider the reciprocal lattice, and, as always if we look at electronic properties, use the Wigner-Seitz cell (identical to the 1st Brillouin zone) as the unit cell. |
| | There is no way to express quantities that change as a function of three coordinates graphically, so we look at a two dimensional crystal first (which, incidentally, do exist in semiconductor physics). |
| The qualitative recipe for obtaining the band structure of a two-dimensional lattice using the slightly adjusted parabolas of the free electron gas model is simple: |
| | Construct the parabolas along major directions of the reciprocal lattice, interpolate in between, and fold them back into the first Brillouin zone. How this can be done for the free electron gas is shown in an illustration module. |
| | An example – taken from "Harrison" – may look like this: |
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| | The lower part (the "cup") is contained in the 1st Brillouin zone, the upper part (the "top") comes from the second BZ, but is now folded back into the first one. It thus would carry a different band index. This could be continued ad infinitum; but Brillouin zones with energies well above the Fermi energy are of no real interest. |
| | The lower part shows tracings along major directions. Evidently, they contain most of the relevant information in condensed form. It is clear, e.g., that this structure has no band gap. |
| It would be sufficient for most purposes to know the En(k) curves – the dispersion relations – along the major directions of the reciprocal lattice (n is the band index) (see quantum mechanics script as well). |
| | This is exactly what is done when real band diagrams of crystals are shown. Directions are chosen that lead from the center of the Wigner-Seitz unit cell – or the Brillouin zones in the more generalized picture – to special symmetry points. These points are labeled according to the following rules: |
| | - Points (and lines) inside the Brillouin zone are denoted with Greek letters.
- Points on the surface of the Brillouin zone with Roman letters.
- The center of the Wigner-Seitz cell is always denoted by a G
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| | For cubic reciprocal lattices, the points with a high symmetry on the Wigner-Seitz cell are the intersections of the Wigner Seitz cell with the low-indexed directions in the cubic elementary cell. |
| | We use the following nomenclature: ( red for fcc, blue for bcc): |
| | The intersection point with the [100] direction is called X ( H); the line G X is called D. The intersection point with the [110] direction is called K (N); the line GK is called S. The intersection point with the [111] direction is called L (P); the line GL is called L . |
| The picture above already used this kind of labelling. Since the tracing of the dispersion curve can be done on different levels – corresponding to the 1st, second, etc. Brillouin zone – the points are often indexed with the number of the Brillouin zone they use. |
| | This may look like this: |
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| | The top pictures show the elementary cell of the diamond lattice or of the ZnS type lattice; the lower left picture the Bravais lattice of the fcc type and the primitive (non-cubic) lattice which is an equally valid, if less symmetric, representation of the fcc lattice.. |
| | The lower right picture shows the cubic reciprocal lattice of the cubic fcc lattice (which is a bcc lattice) and the Wigner-Seitz cells (identical with the first Brillouin zone) which also represent the reciprocal lattice |
| We now can draw the band diagrams along all kinds of lines – not only from G to some point on the Brillouin zone, but also from point to point, e.g., from L to K or to some other points not yet labeled. An example for the fcc structure and the free electron gas approximation is shown below. |
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| | The first Brillouin zone with the proper indexing of the relevant points and some dispersion parabola along prominent directions are shown. The picture is taken from Hummel's book. |
| | The indexing of the various branches is a bit more complicated than in the illustration example for reasons explained below. |
| Contemplate this picture a bit and then ask yourself: |
| | - Do I find this picture alarming ? ("Gee, if even the most simple situation produces such a complicated structure, I'm never going to understand it)
- Do I find this picture exciting? ("Gee, what a wealth of information one can get in a simple diagram if you pick a smart way of representation").
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| | Yes, it is a bit confusing at first. But do not despair: If you need it, if you work with it, you will quickly catch on! |
| It is standard praxis to join the single diagram at appropriate points and to draw band diagrams by showing two branches starting from G to major points and to continue from there as already practiced above. |
| | The band diagram of Si, e.g., then assumes its standard form: |
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| | The indexing of the major points in the Brillouin zone is more complex than described so far – it is more than just a band index. This reflects the fact that there is no unique choice of the G point, or that the the band structure allows certain symmetry operations without changing. The indexing follows rules of group theory displaying the symmetries, but shall not be described here. |
| | The band structure as shown in this standard diagram contains a tremendous amount of information; at this level it is, e.g., evident that: |
| | Si has a band gap of about 1 eV. |
| | Si is an indirect semiconductor because the maximum of the valence band (at G) does not coincide with the minimum of the conduction band (to the left of X). |
| There is, however, a lot more information encoded in this diagram, as we will see later. |
| Of course, the question remains how the band structures of real-world materials can be obtained. However, concerning both measurementes and calculations, this is a rather involved subject of its own; we do not treat it here. |
| | To get at least a coarse feeling about how involved such calculations are, you may have a look at some really advanced module where the theoretical basics and the available software are presented. |
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© H. Föll (Semiconductors - Script)
FAQs
Band structures are a representation of the allowed electronic energy levels of solid materials and are used to better inform their electrical properties. A band structure is a 2D representation of the energies of the crystal orbitals in a crystalline material.
How to read band structure diagrams? ›
In a band diagram the vertical axis is energy while the horizontal axis represents real space. Horizontal lines represent energy levels, while blocks represent energy bands. When the horizontal lines in these diagram are slanted then the energy of the level or band changes with distance.
What is band structure in DFT? ›
[57] applied DFT simulation to calculate the electronic band structure of silicon nanowire (Si50H40) grounded structure, using Generalized Gradient Approximation (GGA-PBE) functional. The band structure is the change of the Kohn-Sham eigenvalues in the Brillouin zone (BZ) along a specific k-point path.
What is the band structure calculation? ›
Band structure calculations refer to the computational methods used to analyze and predict the electronic properties of metal-hydrogen systems, providing insights into their microscopic behavior.
What is band representation? ›
The band representation characterizes the symmetry of all the electronic states of. an energy band. Any band representation coincides with a so-called simple band representation.
What is the band theory explained? ›
band theory, in solid-state physics, theoretical model describing the states of electrons, in solid materials, that can have values of energy only within certain specific ranges. The behaviour of an electron in a solid (and hence its energy) is related to the behaviour of all other particles around it.
How do you measure experimental band structure? ›
The electronic band structure is commonly studied by angular resolved photoelectron spectroscopy(ARUPS). ARUPS gives you the joint density of states from the valence bands. By assuming free electron states for the unoccupied states you obtain the density of occupied states.
What are high symmetry points for band structure? ›
High-symmetry points are special points in the BZ that are invariant under one or more symmetry operations of the crystal lattice. These points can be used to define a path through the BZ, and the band structure can be calculated along this path.
What is the gamma point in band structure? ›
The gamma point is the center of the Brillouin zone (k=(0,0,0)). It is most commonly encountered in the context of phonon or electron dispersions (ω or E vs k relations), but the same concepts show up when describing dispersion relations of various collective excitations (e.g. magnons).
What do you mean by band structure? ›
1 Band structures. Electronic band structures of a solid, or band structures, in short, describe the energy that electrons have and are responsible for the explanation of the electrical properties of a material.
The E-k curve of valence and conduction bands is a parabola because the net energy of an electron or hole is a parabolic function of its wave number. This is derived from the De-Broglie Wave-Particle Duality theory.
What is the meaning of banded structure? ›
noun. : a geological structure characterized by an arrangement of different minerals in layers that appear as bands in cross section (as in a fissure vein) or of different colors or textures in layers in a rock consisting of one mineral (as in onyx marble)
What is the bandwidth of a band structure? ›
The difference in energy between the highest and lowest allowed levels within a given band is the bandwidth, and the difference in energy between the highest level of one band and the lowest level of the band above it is the band gap.
How do you calculate band depth? ›
obtain band depth, a continuum hull was matched to the original spectral profile, and this continuum was removed from the original spectral profile to get normalized reflectance; we then subtracted these continuum-removed reflectance values from one to get the band depth profile.
What is the formula for band ratio? ›
To calculate band ratios, you specify a numerator band and a denominator band. The band ratio is the numerator divided by the denominator.
What type of structure is the IT band? ›
The IT band runs along the outside of the thigh, from just above the hip to just below the knee, and is made up of fascia, an elastic connective tissue found throughout the body.
What is the manifestation of band structure due to? ›
Thus, the manifestation of band structure in solids is due to Pauli's exclusion principle.
What is the work function of the band structure? ›
The valence bands are filled with electrons up to the Fermi energy (EF). The energy difference between Fermi energy and vacuum level corresponds to the work function (Φ). The work function corresponds to the minimum amount of energy needed to remove an electron from the metal.
What is the structure of the A band and the I band? ›
These striations appear as alternate dark and light bands that stretch across the muscle fibre. These dark and light bands are called A-bands and I-bands respectively. The A-band is made up of myosin filaments whereas the I-band is made up of actin filaments alone. A-Bands are the anisotropic bands of the sarcomere.
