## Effect of Point Defects on the Fermi Level Position in CZT Crystal
Point defects in
Cadmium Zinc Telluride (CZT) crystals can significantly influence the
Fermi level position, which plays a critical role in determining the electrical and electronic properties of the material. The
Fermi level represents the energy level at which the probability of finding an electron is 50% at absolute zero temperature. The position of the Fermi level in the bandgap dictates the
carrier concentration and the
type of conductivity (n-type or p-type) in the crystal.
Point defects, which include
vacancies,
interstitials, and
antisite defects, can introduce localized energy states within the
bandgap of CZT. These defects influence the
electronic structure by creating shallow or deep levels that can either donate or accept electrons, thereby affecting the position of the Fermi level.
## 1. Vacancies
Vacancies are point defects where an atom is missing from its normal lattice position. In CZT, vacancies can occur in the
cadmium,
zinc, or
tellurium sublattices, and each type of vacancy can have a different impact on the Fermi level position.
*
Cadmium Vacancies (V\_Cd): Cadmium vacancies are donor defects, meaning they tend to
donate electrons to the conduction band, increasing the electron concentration. As a result,
n-type behavior is promoted. The introduction of Cd vacancies causes the Fermi level to move closer to the
conduction band, making it easier for electrons to be thermally excited into the conduction band.
*
Zinc Vacancies (V\_Zn): Zinc vacancies are typically acceptor defects. They can
accept electrons from the valence band, which leads to
p-type behavior by creating hole states in the valence band. This causes the Fermi level to shift towards the
valence band, favoring hole conduction.
*
Tellurium Vacancies (V\_Te): Tellurium vacancies in CZT are often neutral or weakly charged, but they can also contribute to either
n-type or p-type conductivity, depending on the interaction with other defects. The position of the Fermi level can be influenced based on the relative concentrations of the various vacancy types.
## 2. Interstitials
Interstitials are defects in which atoms occupy positions between the normal lattice sites. In CZT,
interstitial cadmium (Cd\_i),
interstitial zinc (Zn\_i), and
interstitial tellurium (Te\_i) can all form.
*
Cadmium Interstitials (Cd\_i): These are often considered
donor defects. They can donate electrons into the conduction band, promoting
n-type behavior. The introduction of Cd interstitials would shift the Fermi level
upwards toward the conduction band.
*
Zinc Interstitials (Zn\_i): Zinc interstitials tend to act as
acceptor defects. When zinc atoms are placed at interstitial sites, they can trap electrons, promoting
p-type behavior and pushing the Fermi level
downward towards the valence band.
*
Tellurium Interstitials (Te\_i): Tellurium interstitials are neutral or can contribute to both n-type and p-type conduction. The effect of Te interstitials on the Fermi level depends on their concentration and their interaction with other defects.
## 3. Antisite Defects
Antisite defects occur when an atom is positioned on a site normally occupied by a different type of atom. For example, a
cadmium atom on a zinc site (Cd\_Zn) or a
zinc atom on a cadmium site (Zn\_Cd).
*
Cadmium on Zinc Site (Cd\_Zn): This antisite defect behaves as a
donor, releasing electrons into the conduction band and increasing
n-type behavior. This defect causes the Fermi level to move
closer to the conduction band.
*
Zinc on Cadmium Site (Zn\_Cd): This defect acts as an
acceptor, capturing electrons and promoting
p-type conductivity. The Fermi level shifts
closer to the valence band due to the formation of hole states.
## 4. Deep Defects and Mid-Gap States
Point defects in CZT can create deep levels within the
bandgap. These deep defects do not significantly contribute to conduction but can significantly alter the position of the Fermi level, especially at high defect concentrations.
*
Deep-Level Defects: These are typically related to
vacancies,
antisite defects, or
impurities. These defects create states that act as traps for electrons or holes. These traps do not directly affect the charge carrier concentration but influence the
position of the Fermi level by altering the relative occupancy of states within the bandgap. For instance, a high density of deep-level defects can pin the Fermi level, preventing it from freely adjusting based on the intrinsic material properties.
*
Electron Trap States: If deep defects act as
electron traps, the Fermi level may shift
upward towards the conduction band, effectively increasing the electron density in the conduction band. Conversely,
hole trap states can pull the Fermi level
downward, promoting hole conduction.
## 5. Overall Impact of Point Defects on the Fermi Level
The overall impact of point defects on the Fermi level in CZT crystals depends on:
1.
Type and Concentration of Defects: A higher concentration of donor defects, such as cadmium vacancies or cadmium interstitials, tends to shift the Fermi level closer to the conduction band, promoting
n-type conductivity. On the other hand, a high concentration of acceptor defects, such as zinc vacancies or zinc interstitials, shifts the Fermi level toward the valence band, promoting
p-type conductivity.
2.
Compensation Effects: The effects of various defects can be
compensatory. For example, the introduction of both donor and acceptor defects may result in a
neutral Fermi level or minimal shift, depending on the balance between the two types of defects.
3.
Temperature and Electrical Biasing: The position of the Fermi level can also vary with
temperature and
biasing conditions. For example,
thermal excitation may promote electrons from deep traps to the conduction band, causing a shift in the Fermi level at high temperatures. Similarly, applying an
external bias can alter the Fermi level's position by creating an electric field that affects charge carrier distribution.
## 6. Summary
*
Cadmium vacancies (V\_Cd) and
cadmium interstitials (Cd\_i) typically act as
donors, promoting
n-type conductivity and shifting the Fermi level toward the conduction band.
*
Zinc vacancies (V\_Zn) and
zinc interstitials (Zn\_i) are generally
acceptors, promoting
p-type conductivity and pulling the Fermi level toward the valence band.
*
Tellurium-related defects, such as
Te vacancies (V\_Te) or
interstitials (Te\_i), can have more complex effects, often depending on the specific type of defect and the surrounding conditions.
*
Antisite defects (e.g.,
Cd\_Zn and
Zn\_Cd) behave as donors or acceptors, depending on which element is misplaced.
* The Fermi level may be
pinned or
shifted by the presence of deep-level defects that introduce mid-gap states.
Understanding the effects of point defects on the Fermi level is crucial for tuning the
electrical properties of CZT crystals, especially for their use in
detectors and other
electronic applications. The goal is to carefully control defect concentrations and types to optimize performance and minimize undesirable charge carrier recombination or trapping.
CdZnTe Association (CdZnTe.com)
https://www.cdznte.com/blog/how-do-point-defects-affect-the-fermi-level-position-in-czt-crystal.html
