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The Lorentz oscillator model describes the optical response of bound charges. The model is named after the Dutch physicist
Hendrik Antoon Lorentz Hendrik Antoon Lorentz (; 18 July 1853 – 4 February 1928) was a Dutch physicist who shared the 1902 Nobel Prize in Physics with Pieter Zeeman for the discovery and theoretical explanation of the Zeeman effect. He also derived the Lorent ...
. It is a classical, phenomenological model for materials with characteristic resonance frequencies (or other characteristic energy scales) for optical absorption, e.g. ionic and molecular vibrations, interband transitions (semiconductors), phonons, and collective excitations.


Derivation of electron motion

The model is derived by modeling an electron orbiting a massive, stationary nucleus as a spring-mass-damper system. The electron is modeled to be connected to the nucleus via a hypothetical spring and its motion is damped by via a hypothetical damper. The damping force ensures that the oscillator's response is finite at its resonance frequency. For a time-harmonic driving force which originates from the electric field, Newton’s second law can be applied to the electron to obtain the motion of the electron and expressions for the dipole moment, polarization, susceptibility, and
dielectric function In electromagnetism, the absolute permittivity, often simply called permittivity and denoted by the Greek letter ''ε'' (epsilon), is a measure of the electric polarizability of a dielectric. A material with high permittivity polarizes more in ...
. Equation of motion for electron oscillator: : \mathbf F_ = m\frac : \mathbf F_ + \mathbf F_ + \mathbf F_ = m\frac : \frac \frac - k \mathbf r - \mathbf E(t) = m\frac : \frac + \frac \frac + \omega_0^2 \mathbf r\; = \; \frac \mathbf E(t) where * \mathbf r is the displacement of charge from the rest position, * t is time, * \mathrm \tau is the relaxation time/scattering time, * k is a constant factor characteristic of the spring, * m is the effective mass of the electron, * \omega_0 = \left(k / m \right)^ * \omega_0 is the resonance frequency of the oscillator, * e is the elementary charge, * \mathbf E(t) is the electric field. For time-harmonic fields: :\mathbf E(t) = \mathbf E_0 e^ :\mathbf r(t) = \mathbf r_0 e^ The stationary solution of this equation of motion is: :\mathbf r(\omega) = \frac \mathbf E(\omega) The fact that the above solution is
complex Complex commonly refers to: * Complexity, the behaviour of a system whose components interact in multiple ways so possible interactions are difficult to describe ** Complex system, a system composed of many components which may interact with each ...
means there is a time delay (phase shift) between the driving electric field and the response of the electron’s motion.


Dipole moment

The displacement, \mathbf r , induces a dipole moment, \mathbf p, given by :\mathbf p(\omega) = -e \mathbf r(\omega) = \hat\alpha(\omega) \mathbf E(\omega) \hat \alpha(\omega) is the polarizability of single oscillator, given by :\hat \alpha(\omega)= \frac \frac


Polarization

The polarization \mathbf P is the dipole moment per unit volume. For macroscopic material properties N is the density of charges (electrons) per unit volume. Considering that each electron is acting with the same dipole moment we have the polarization as below :\mathbf P = N \mathbf p = N \hat \alpha(\omega) \mathbf E(\omega)


Electric displacement

The electric displacement \mathbf D is related to the polarization density \mathbf P by :\mathbf D = \hat\varepsilon \mathbf E = \mathbf E + 4\pi \mathbf P = (1 + 4\pi N \hat \alpha) \mathbf E


Dielectric function

The complex dielectric function is given by :\hat \varepsilon(\omega) = 1 + \frac \frac where 4\pi N e^2/m = \omega_p^2 and \omega_p is the so called
plasma frequency Plasma oscillations, also known as Langmuir waves (after Irving Langmuir), are rapid oscillations of the electron density in conducting media such as plasmas or metals in the ultraviolet region. The oscillations can be described as an instability i ...
. In practice, the model is commonly modified to account for multiple absorption mechanisms present in a medium. The modified version is given by :\hat \varepsilon(\omega) = \varepsilon_ + \sum_ \chi_^(\omega; \omega_) where :\chi_^(\omega; \omega_) = \frac and * \varepsilon_ is the value of the dielectric function at infinite frequency, which can be used as an adjustable parameter to account for high frequency absorption mechanisms, * s_ = \omega_p^ f_ and f_ is related to the strength of the jth absorption mechanism, * \Gamma_=1/\tau. Separating the real and imaginary components, :\hat \varepsilon(\omega) = \varepsilon_1(\omega) + \mathrm i \varepsilon_2(\omega) = \left \varepsilon_ + \sum_ \frac \right+ \mathrm i \left \sum_ \frac \right/math>


Complex conductivity

The complex optical conductivity in general is related to the complex dielectric function : \hat \sigma(\omega) = \frac (\hat\varepsilon(\omega) - 1) Substituting the formula of \hat\varepsilon(\omega) in the equation above we obtain :\hat \sigma(\omega) = \frac \frac Separating the real and imaginary components, :\hat \sigma(\omega) = \sigma_1(\omega) + \mathrm i \sigma_2(\omega) = \frac \frac -\mathrm i \frac \frac


References

{{reflist , refs = {{cite book , last1 = Lorentz , first1 = Hendrik Antoon , year = 1909 , title = The theory of electrons and its applications to the phenomena of light and radiant heat , language = en , volume = Bd. XXIX;Bd. 29 , location = New York; Leipzig , publisher = B.G. Teubner , oclc = 535812 {{cite book , last1 = Dressel , first1 = Martin , last2 = Grüner , first2 = George , year = 2002 , title = Electrodynamics of Solids: Optical Properties of Electrons in Matter , chapter = Semiconductors , pages = 136–172 , language = en , location = Cambridge , doi = 10.1017/CBO9780511606168.008 , isbn = 9780521592536 {{cite web , last = Colton , first = John , title = Lorentz Oscillator Model , year = 2020 , website = Brigham Young University, Department of Physics & Astronomy , publisher = Brigham Young University , url = https://physics.byu.edu/faculty/colton/docs/phy442-resources/Lorentz-oscillator-model.pdf , access-date = 2021-11-18 {{cite web , last1 = Almog , first1 = I. F. , last2 = Bradley , first2 = M. S. , last3 = Bulovic , first3 = V. , title = The Lorentz Oscillator and its Applications , year = 2011 , website = Massachusetts Institute of Technology, Department of Electrical Engineering and Computer Science , publisher = Massachusetts Institute of Technology , url = https://ocw.mit.edu/courses/electrical-engineering-and-computer-science/6-007-electromagnetic-energy-from-motors-to-lasers-spring-2011/readings/MIT6_007S11_lorentz.pdf , access-date = 2021-11-24 {{cite journal , last1 = Spitzer , first1 = W. G. , last2 = Kleinman , first2 = D. , last3 = Walsh , first3 = D. , title = Infrared Properties of Hexagonal Silicon Carbide , journal = Physical Review , volume = 113 , issue = 1 , pages = 127–132 , year = 1959 , url = https://doi.org/10.1103/PhysRev.113.127 , doi = 10.1103/PhysRev.113.127 , bibcode = 1959PhRv..113..127S , access-date = 2021-11-24 {{cite journal , last1 = Zhang , first1 = Z. M. , last2 = Lefever-Button , first2 = G. , last3 = Powell , first3 = F. R. , title = Infrared Refractive Index and Extinction Coefficient of Polyimide Films , journal = International Journal of Thermophysics , volume = 19 , issue = 3 , pages = 905–916 , year = 1998 , url = https://doi.org/10.1023/A:1022655309574 , doi = 10.1023/A:1022655309574 , s2cid = 116271335 , access-date = 2021-11-24


See also

* Cauchy equation * Sellmeier equation *
Forouhi–Bloomer model The Forouhi–Bloomer model is a mathematical formula for the frequency dependence of the complex-valued refractive index. The model can be used to fit the refractive index of amorphous and crystalline semiconductor and dielectric materials at ene ...
*
Tauc–Lorentz model The Tauc–Lorentz model is a mathematical formula for the frequency dependence of the complex-valued relative permittivity, sometimes referred to as the dielectric function. The model has been used to fit the complex refractive index of amorphous ...
*
Brendel–Bormann oscillator model The Brendel–Bormann oscillator model is a mathematical formula for the frequency dependence of the complex-valued relative permittivity, sometimes referred to as the dielectric function. The model has been used to fit to the complex refractive in ...
Condensed matter physics Electric and magnetic fields in matter Optics