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🧗‍♀️Semiconductor Physics Unit 3 Review

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3.4 Temperature dependence of carrier concentration

🧗‍♀️Semiconductor Physics
Unit 3 Review

3.4 Temperature dependence of carrier concentration

Written by the Fiveable Content Team • Last updated September 2025
Written by the Fiveable Content Team • Last updated September 2025
🧗‍♀️Semiconductor Physics
Unit & Topic Study Guides

Temperature dependence of carrier concentration is crucial in semiconductor physics. It affects electrical properties, device performance, and operation across different temperatures. Understanding this relationship is key to designing and optimizing semiconductor devices for various applications.

The intrinsic carrier concentration increases exponentially with temperature, while extrinsic semiconductors show more complex behavior. Dopant ionization, carrier mobility, and conductivity all change with temperature, impacting device characteristics and performance in diodes, transistors, and other semiconductor components.

Intrinsic carrier concentration

  • Intrinsic carrier concentration is a fundamental property of semiconductors that describes the number of electrons and holes in the material at thermal equilibrium
  • It is a key parameter in determining the electrical properties of semiconductors and is essential for understanding the behavior of semiconductor devices
  • The intrinsic carrier concentration is highly dependent on temperature and the material's bandgap energy

Temperature dependence

  • The intrinsic carrier concentration increases exponentially with temperature due to the increased thermal energy available for electrons to be excited from the valence band to the conduction band
  • The relationship between intrinsic carrier concentration ($n_i$) and temperature ($T$) is given by: $n_i = \sqrt{N_c N_v} \exp(-E_g/2k_BT)$, where $N_c$ and $N_v$ are the effective density of states in the conduction and valence bands, $E_g$ is the bandgap energy, and $k_B$ is the Boltzmann constant
  • At higher temperatures, more electrons are excited across the bandgap, leading to a higher intrinsic carrier concentration (silicon, germanium)

Bandgap energy

  • The bandgap energy is the minimum energy required for an electron to be excited from the valence band to the conduction band
  • Materials with larger bandgap energies have lower intrinsic carrier concentrations at a given temperature compared to those with smaller bandgap energies
  • The bandgap energy determines the intrinsic carrier concentration and the temperature range over which a semiconductor can operate effectively (silicon: 1.12 eV, germanium: 0.67 eV)

Density of states

  • The density of states describes the number of available energy states per unit volume and energy in the conduction and valence bands
  • The effective density of states in the conduction band ($N_c$) and valence band ($N_v$) are proportional to $T^{3/2}$ and play a role in determining the intrinsic carrier concentration
  • A higher density of states near the band edges leads to a higher intrinsic carrier concentration at a given temperature (III-V semiconductors, II-VI semiconductors)

Extrinsic semiconductors

  • Extrinsic semiconductors are created by adding impurities (dopants) to intrinsic semiconductors to control their electrical properties
  • Doping introduces additional energy levels within the bandgap, which can donate electrons to the conduction band (n-type) or accept electrons from the valence band (p-type)
  • The carrier concentration in extrinsic semiconductors is dominated by the concentration of dopants and depends on the temperature and the dopant ionization energy

Dopant ionization

  • Dopant ionization is the process by which dopant atoms release or accept electrons, contributing to the carrier concentration in the semiconductor
  • The ionization energy is the energy required to ionize the dopant atoms, which is typically much smaller than the bandgap energy
  • At low temperatures, not all dopant atoms are ionized, leading to a reduced carrier concentration (freeze-out region)

Freeze-out vs exhaustion regions

  • In the freeze-out region, the carrier concentration is limited by the incomplete ionization of dopant atoms at low temperatures
  • As the temperature increases, more dopant atoms become ionized, and the carrier concentration increases until it reaches the dopant concentration (exhaustion region)
  • In the exhaustion region, all dopant atoms are ionized, and the carrier concentration is equal to the dopant concentration, independent of temperature

Saturation of carrier concentration

  • At high temperatures, the carrier concentration in extrinsic semiconductors saturates at the dopant concentration
  • Once all dopant atoms are ionized, further increases in temperature do not significantly affect the carrier concentration
  • The saturation of carrier concentration occurs at lower temperatures for dopants with smaller ionization energies (shallow dopants) compared to those with larger ionization energies (deep dopants)

Fermi level position

  • The Fermi level is a hypothetical energy level that represents the average energy of electrons in a semiconductor
  • The position of the Fermi level relative to the conduction and valence bands determines the carrier concentrations and the semiconductor's electrical properties
  • The Fermi level position depends on temperature, doping concentration, and the type of semiconductor (intrinsic or extrinsic)

Temperature dependence

  • In intrinsic semiconductors, the Fermi level lies near the middle of the bandgap and moves closer to the conduction or valence band as the temperature increases
  • In extrinsic semiconductors, the Fermi level position depends on the type and concentration of dopants and shifts towards the conduction band (n-type) or valence band (p-type) as the temperature increases
  • At high temperatures, the Fermi level in extrinsic semiconductors approaches the intrinsic Fermi level position

Intrinsic vs extrinsic semiconductors

  • In intrinsic semiconductors, the Fermi level is determined by the balance between the electron and hole concentrations, which are equal at thermal equilibrium
  • In extrinsic semiconductors, the Fermi level position is determined by the type and concentration of dopants, which create an imbalance between the electron and hole concentrations
  • The Fermi level in n-type semiconductors lies closer to the conduction band, while in p-type semiconductors, it lies closer to the valence band

Bandgap narrowing effects

  • Bandgap narrowing occurs in heavily doped semiconductors due to the increased interaction between dopant atoms and the semiconductor lattice
  • The reduced bandgap leads to a shift in the Fermi level position and an increase in the intrinsic carrier concentration
  • Bandgap narrowing effects are more pronounced in heavily doped regions of semiconductor devices (emitter regions in bipolar junction transistors)

Carrier mobility

  • Carrier mobility is a measure of how easily charge carriers (electrons and holes) can move through a semiconductor under the influence of an electric field
  • The mobility depends on the scattering mechanisms that limit carrier motion, such as lattice scattering and impurity scattering
  • Higher carrier mobility leads to better electrical conductivity and improved device performance

Lattice scattering

  • Lattice scattering is caused by the interaction between charge carriers and the thermal vibrations of the semiconductor lattice (phonons)
  • As the temperature increases, the thermal vibrations become more intense, leading to increased lattice scattering and reduced carrier mobility
  • Lattice scattering is the dominant scattering mechanism at high temperatures

Impurity scattering

  • Impurity scattering is caused by the interaction between charge carriers and the ionized dopant atoms in the semiconductor
  • The scattering rate depends on the dopant concentration and the charge state of the dopant atoms
  • Impurity scattering is the dominant scattering mechanism at low temperatures and in heavily doped semiconductors

Temperature dependence of mobility

  • The overall carrier mobility is determined by the combined effects of lattice scattering and impurity scattering
  • At low temperatures, impurity scattering dominates, and the mobility increases with temperature as the thermal energy helps carriers overcome the potential barriers created by ionized dopants
  • At high temperatures, lattice scattering dominates, and the mobility decreases with temperature due to increased thermal vibrations

Minority carrier concentration

  • Minority carriers are the less abundant type of charge carriers in a semiconductor (electrons in p-type, holes in n-type)
  • The minority carrier concentration is much lower than the majority carrier concentration in extrinsic semiconductors
  • Minority carriers play a crucial role in the operation of bipolar devices, such as diodes and transistors

Relation to majority carriers

  • In thermal equilibrium, the product of the electron and hole concentrations is equal to the square of the intrinsic carrier concentration: $np = n_i^2$
  • This relation holds for both intrinsic and extrinsic semiconductors
  • In extrinsic semiconductors, the minority carrier concentration can be calculated from the majority carrier concentration using this relation

Temperature dependence

  • The minority carrier concentration increases exponentially with temperature, following the same temperature dependence as the intrinsic carrier concentration
  • At higher temperatures, the minority carrier concentration approaches the intrinsic carrier concentration
  • The temperature dependence of the minority carrier concentration is important for the operation of bipolar devices at different temperatures

Low injection vs high injection

  • Low injection conditions occur when the injected minority carrier concentration is much smaller than the majority carrier concentration
  • In low injection, the minority carrier concentration is determined by the equilibrium conditions and is not affected by the injected carriers
  • High injection conditions occur when the injected minority carrier concentration is comparable to or larger than the majority carrier concentration
  • In high injection, the minority carrier concentration is dominated by the injected carriers, and the semiconductor properties can deviate from their equilibrium values

Conductivity and resistivity

  • Conductivity is a measure of a semiconductor's ability to conduct electric current, while resistivity is a measure of its resistance to current flow
  • The conductivity and resistivity of a semiconductor depend on the carrier concentrations and mobilities
  • Understanding the factors that affect conductivity and resistivity is essential for designing and optimizing semiconductor devices

Carrier concentration effects

  • The conductivity is directly proportional to the sum of the electron and hole concentrations, weighted by their respective mobilities: $\sigma = q(n\mu_n + p\mu_p)$
  • In extrinsic semiconductors, the conductivity is dominated by the majority carrier concentration and mobility
  • Increasing the dopant concentration leads to higher conductivity, as long as the dopants are fully ionized

Mobility effects

  • The conductivity is directly proportional to the carrier mobilities, which determine how easily electrons and holes can move through the semiconductor
  • Higher carrier mobilities lead to higher conductivity and lower resistivity
  • The mobility effects on conductivity become more significant in heavily doped semiconductors, where impurity scattering can limit the carrier mobility

Temperature dependence

  • The temperature dependence of conductivity and resistivity is determined by the combined effects of carrier concentration and mobility
  • In the freeze-out region, the conductivity increases with temperature as more dopants become ionized and contribute to the carrier concentration
  • In the exhaustion region, the conductivity is determined by the temperature dependence of the carrier mobility, which typically decreases with increasing temperature due to enhanced lattice scattering

Applications in devices

  • The temperature dependence of carrier concentration, Fermi level position, mobility, and conductivity plays a crucial role in the operation and performance of semiconductor devices
  • Understanding these dependencies is essential for designing and optimizing devices for specific applications and operating conditions
  • Some common applications include diodes, bipolar junction transistors (BJTs), and metal-oxide-semiconductor field-effect transistors (MOSFETs)

Diodes and rectifiers

  • The temperature dependence of the carrier concentration and Fermi level position affects the forward and reverse characteristics of diodes
  • At higher temperatures, the increased intrinsic carrier concentration leads to higher reverse leakage currents and reduced rectification efficiency
  • Temperature compensation techniques, such as using wide-bandgap semiconductors or optimizing the doping profiles, can improve the temperature stability of diodes and rectifiers

Bipolar junction transistors (BJTs)

  • The temperature dependence of minority carrier concentration and mobility affects the current gain and switching speed of BJTs
  • At higher temperatures, the increased minority carrier concentration leads to higher base currents and reduced current gain
  • The temperature dependence of mobility affects the collector current and the transistor's frequency response
  • Proper biasing and design techniques can help minimize the temperature sensitivity of BJTs

Metal-oxide-semiconductor field-effect transistors (MOSFETs)

  • The temperature dependence of carrier concentration and mobility affects the threshold voltage and the drain current of MOSFETs
  • At higher temperatures, the increased intrinsic carrier concentration can lead to higher off-state leakage currents and reduced on/off current ratios
  • The temperature dependence of mobility affects the drain current and the transistor's switching speed
  • Advanced device structures, such as high-k dielectrics and metal gates, can help improve the temperature stability of MOSFETs