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4.4 Temperature and voltage dependence of electron transport

3 min readaugust 7, 2024

Electron transport in molecules is heavily influenced by temperature and voltage. These factors affect how electrons move through materials, impacting everything from to resistance changes.

Understanding these dependencies is crucial for designing and analyzing molecular electronic devices. We'll look at how temperature impacts electron emission and energy distributions, and how voltage drives current flow and reveals .

Thermionic Emission and Thermal Effects

Temperature-Dependent Electron Emission and Transport

Top images from around the web for Temperature-Dependent Electron Emission and Transport
Top images from around the web for Temperature-Dependent Electron Emission and Transport
  • Thermionic emission occurs when electrons gain enough thermal energy to overcome the work function and escape from a material's surface
    • Governed by the Richardson-Dushman equation: J=AT2eWkBTJ = A T^2 e^{-\frac{W}{k_B T}}, where JJ is the emission current density, AA is a material-specific constant, TT is the temperature, WW is the work function, and kBk_B is the Boltzmann constant
    • Commonly observed in vacuum tubes and electron guns (cathode ray tubes)
  • of energy levels leads to a distribution of electron energies around the Fermi level
    • Described by the : f(E)=1e(EEF)/kBT+1f(E) = \frac{1}{e^{(E-E_F)/k_B T}+1}, where f(E)f(E) is the probability of an electron occupying a state with energy EE, EFE_F is the Fermi energy, kBk_B is the Boltzmann constant, and TT is the temperature
    • Results in a smearing of the Fermi edge and a non-zero probability of finding electrons above the Fermi level at finite temperatures

Activation Energy and Temperature-Dependent Resistance

  • is the minimum energy required for a process to occur, such as electron transport or chemical reactions
    • Determines the temperature dependence of the rate of a process according to the : k=AeEakBTk = A e^{-\frac{E_a}{k_B T}}, where kk is the rate constant, AA is a pre-exponential factor, EaE_a is the activation energy, kBk_B is the Boltzmann constant, and TT is the temperature
    • Can be extracted from the slope of an Arrhenius plot, which is a graph of ln(k)\ln(k) vs. 1/T1/T
  • describes the relative change in resistance with temperature
    • Defined as α=1RdRdT\alpha = \frac{1}{R} \frac{dR}{dT}, where α\alpha is the TCR, RR is the resistance, and TT is the temperature
    • Positive TCR (metals) indicates increasing resistance with temperature due to increased electron scattering
    • Negative TCR (semiconductors) indicates decreasing resistance with temperature due to increased from thermal excitation across the bandgap

Voltage-Dependent Transport

Current-Voltage Characteristics and Differential Conductance

  • is the potential difference applied across a device or junction
    • Drives current flow and determines the energy landscape for electron transport
    • Can be used to probe the and transport properties of materials and devices
  • I-V characteristics describe the relationship between current and voltage in a device
    • Provide information about the transport mechanism, such as ohmic (linear) or non-ohmic (non-linear) behavior
    • Can reveal the presence of energy barriers, such as in a Schottky diode or a tunnel junction
  • is the derivative of the current with respect to voltage: G=dIdVG = \frac{dI}{dV}
    • Reflects the local density of states and the transmission probability at a given energy
    • Can be measured using lock-in techniques or numerical differentiation of I-V data
    • Peaks in differential conductance correspond to resonant tunneling through discrete energy levels (quantum dots, molecules)

Non-Linear Transport Phenomena

  • occurs when the current-voltage relationship deviates from ohmic behavior
    • Can arise from various mechanisms, such as voltage-dependent tunneling, space-charge limited current, or field emission
    • Examples include in resonant tunneling diodes and current saturation in field-effect transistors
  • leads to non-linear I-V characteristics in tunnel junctions
    • Described by the : IVe2d2mϕ2I \propto V e^{-2d\sqrt{\frac{2m\phi}{\hbar^2}}}, where II is the current, VV is the voltage, dd is the barrier width, mm is the electron mass, ϕ\phi is the barrier height, and \hbar is the reduced Planck constant
    • Enables the study of electronic structure and transport mechanisms in and nanoscale devices
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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.

© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.
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