Einstein coefficients

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Emission lines and absorption lines compared to a continuous spectrum.

In physics, one thinks of atomic spectral lines from two viewpoints.

  • An emission line is formed when an electron makes a transition from a particular discrete energy level E2 of an atom, to a lower energy level E1, emitting a photon of a particular energy and wavelength. A spectrum of many such photons will show an emission spike at the wavelength associated with these photons.
  • An absorption line is formed when an electron makes a transition from a lower, E1, to a higher discrete energy state, E2, with a photon being absorbed in the process. These absorbed photons generally come from background continuum radiation (the full spectrum of electromagnetic radiation) and a spectrum will show a drop in the continuum radiation at the wavelength associated with the absorbed photons.

The two states must be bound states in which the electron is bound to the atom, so the transition is sometimes referred to as a "bound–bound" transition, as opposed to a transition in which the electron is ejected out of the atom completely ("bound–free" transition) into a continuum state, leaving an ionized atom, and generating continuum radiation.

A photon with an energy equal to the difference E2 - E1 between the energy levels is released or absorbed in the process. The frequency ν at which the spectral line occurs is related to the photon energy by Bohr's frequency condition E2 - E1 = where h denotes Planck's constant.[1][2][3][4][5][6]

Emission and absorption coefficients[edit]

An atomic spectral line refers to emission and absorption events in a gas in which n_2 is the density of atoms in the upper energy state for the line, and n_1 is the density of atoms in the lower energy state for the line.

The emission of atomic line radiation at frequency ν may be described by an emission coefficient \epsilon with units of energy/time/volume/solid angle. ε dt dV dΩ is then the energy emitted by a volume element dV in time dt into solid angle d\Omega. For atomic line radiation:

\epsilon = \frac{h\nu}{4\pi}n_2 A_{21}\,

where A_{21} is the Einstein coefficient for spontaneous emission, which is fixed by the intrinsic properties of the relevant atom for the two relevant energy levels.

The absorption of atomic line radiation may be described by an absorption coefficient \kappa with units of 1/length. The expression κ' dx gives the fraction of intensity absorbed for a light beam at frequency ν while traveling distance dx. The absorption coefficient is given by:

\kappa' = \frac{h\nu}{4\pi}~(n_1 B_{12}-n_2 B_{21}) \,

where B_{12} and B_{21} are the Einstein coefficients for photo absorption and induced emission respectively. Like the coefficient A_{21}, these are also fixed by the intrinsic properties of the relevant atom for the two relevant energy levels. For thermodynamics and for the application of Kirchhoff's law, it is necessary that the total absorption be expressed as the algebraic sum of two components, described respectively by B_{12} and B_{21}, which may be regarded as positive and negative absorption, which are, respectively, the direct photon absorption, and what is commonly called stimulated or induced emission.[7][8][9]

The above equations have ignored the influence of the spectroscopic line shape. To be accurate, the above equations need to be multiplied by the (normalized) spectral line shape, in which case the units will change to include a 1/Hz term.

For conditions of thermodynamic equilibrium, together the number densities n_2 and n_1, the Einstein coefficients, and the spectral energy density provide sufficient information to determine the absorption and emission rates.

Equilibrium conditions[edit]

The number densities n_2 and n_1 are set by the physical state of the gas in which the spectral line occurs, including the local spectral radiance (or, in some presentations, the local spectral radiant energy density). When that state is either one of strict thermodynamic equilibrium, or one of so-called 'local thermodynamic equilibrium',[10][11][12] then the distribution of atomic states of excitation (which includes n_2 and n_1) determines the rates of atomic emissions and absorptions to be such that Kirchhoff's law of equality of radiative absorptivity and emissivity holds. In strict thermodynamic equilibrium, the radiation field is said to be black-body radiation, and is described by Planck's law. For local thermodynamic equilibrium, the radiation field does not have to be a black-body field, but the rate of interatomic collisions must vastly exceed the rates of absorption and emission of quanta of light, so that the interatomic collisions entirely dominate the distribution of states of atomic excitation. Circumstances occur in which local thermodynamic equilibrium does not prevail, because the strong radiative effects overwhelm the tendency to the Maxwell-Boltzmann distribution of molecular velocities. For example, in the atmosphere of the sun, the great strength of the radiation dominates. In the upper atmosphere of the earth, at altitudes over 100 km, the rarity of intermolecular collisions is decisive.

In the cases of thermodynamic equilibrium and of local thermodynamic equilibrium, the number densities of the atoms, both excited and unexcited, may be calculated from the Maxwell–Boltzmann distribution, but for other cases, (e.g. lasers) the calculation is more complicated.

Einstein coefficients[edit]

In 1916, Albert Einstein proposed that there are three processes occurring in the formation of an atomic spectral line. The three processes are referred to as spontaneous emission, stimulated emission, and absorption. With each is associated an Einstein coefficient which is a measure of the probability of that particular process occurring. Einstein considered the case of isotropic radiation of frequency ν, and spectral energy density ρ (ν).[2][13]

Various formulations[edit]

Hilborn has compared various formulations for derivations for the Einstein coefficients, by various authors.[14] For example, Herzberg works with irradiance and wavenumber.[15] Yariv works with energy per unit volume per unit frequency interval;[16] also;[17] this is how the present account is formulated. Mihalas & Weibel-Mihalas work with radiance and frequency;[12] also Chandrasekhar;[18] also Goody & Yung;[19] Loudon uses angular frequency and radiance.[20]

Spontaneous emission[edit]

Main article: Spontaneous emission
Schematic diagram of atomic spontaneous emission

Spontaneous emission is the process by which an electron "spontaneously" (i.e. without any outside influence) decays from a higher energy level to a lower one. The process is described by the Einstein coefficient A21 (s−1) which gives the probability per unit time that an electron in state 2 with energy E_2 will decay spontaneously to state 1 with energy E_1, emitting a photon with an energy E2E1 = . Due to the energy-time uncertainty principle, the transition actually produces photons within a narrow range of frequencies called the spectral linewidth. If n_i is the number density of atoms in state i  then the change in the number density of atoms in state 2 per unit time due to spontaneous emission will be:

\left(\frac{dn_2}{dt}\right)_{\mathrm{spontaneous}}=-A_{21}n_2\,.

The same process results in increasing of the population of the state 1:

\left(\frac{dn_1}{dt}\right)_{\mathrm{spontaneous}}=A_{21}n_2\,.

Stimulated emission[edit]

Main article: Stimulated emission
Schematic diagram of atomic stimulated emission

Stimulated emission (also known as induced emission) is the process by which an electron is induced to jump from a higher energy level to a lower one by the presence of electromagnetic radiation at (or near) the frequency of the transition. From the thermodynamic viewpoint, this process must be regarded as negative absorption. The process is described by the Einstein coefficient B_{21} (J−1 m3 s−2), which gives the probability per unit time per unit spectral energy density of the radiation field that an electron in state 2 with energy E_2 will decay to state 1 with energy E_1, emitting a photon with an energy E2E1 = . The change in the number density of atoms in state 1 per unit time due to induced emission will be:

\left(\frac{dn_1}{dt}\right)_{\mathrm{neg}\,\mathrm{absorb}}=B_{21}n_2 \rho(\nu)


where \rho(\nu) denotes the spectral energy density of the isotropic radiation field at the frequency of the transition (see Planck's law).

Stimulated emission is one of the fundamental processes that led to the development of the laser. Laser radiation is, however, very far from the present case of isotropic radiation.

Photo absorption[edit]

Main article: Absorption (optics)
Schematic diagram of atomic absorption

Absorption is the process by which a photon is absorbed by the atom, causing an electron to jump from a lower energy level to a higher one. The process is described by the Einstein coefficient B_{12} (J−1 m3 s−2), which gives the probability per unit time per unit spectral energy density of the radiation field that an electron in state 1 with energy E_1 will absorb a photon with an energy E2E1 = and jump to state 2 with energy E_2. The change in the number density of atoms in state 1 per unit time due to absorption will be:

\left(\frac{dn_1}{dt}\right)_{\mathrm{pos}\,\mathrm{absorb}}=-B_{12}n_0 \rho(\nu)


Detailed balancing[edit]

The Einstein coefficients are fixed probabilities associated with each atom, and do not depend on the state of the gas of which the atoms are a part. Therefore, any relationship that we can derive between the coefficients at, say, thermodynamic equilibrium will be valid universally.

At thermodynamic equilibrium, we will have a simple balancing, in which the net change in the number of any excited atoms is zero, being balanced by loss and gain due to all processes. With respect to bound-bound transitions, we will have detailed balancing as well, which states that the net exchange between any two levels will be balanced. This is because the probabilities of transition cannot be affected by the presence or absence of other excited atoms. Detailed balance (valid only at equilibrium) requires that the change in time of the number of atoms in level 1 due to the above three processes be zero:

0=A_{21}n_2+B_{21}n_2\rho(\nu)-B_{12}n_1 \rho(\nu)\,

Along with detailed balancing, at temperature T we may use our knowledge of the equilibrium energy distribution of the atoms, as stated in the Maxwell–Boltzmann distribution, and the equilibrium distribution of the photons, as stated in Planck's law of black body radiation to derive universal relationships between the Einstein coefficients.

From the Maxwell–Boltzmann distribution we have for the number of excited atomic species i:

\frac{n_i}{n}= \frac{g_i e^{-E_i/kT}}{Z}

where n is the total number density of the atomic species, excited and unexcited, k is Boltzmann's constant, T is the temperature, g_i is the degeneracy (also called the multiplicity) of state i, and Z is the partition function. From Planck's law of black-body radiation at temperature T we have for the spectral energy density at frequency ν

\rho_\nu(\nu,T)=F(\nu)\frac{1}{e^{h\nu/kT}-1}

where:

F(\nu)=\frac{8\pi h\nu^3}{c^3}[16]

where c is the speed of light and h is Planck's constant.

Substituting these expressions into the equation of detailed balancing and remembering that E2E1 = yields:

A_{21}g_2e^{-h\nu/kT}+B_{21}g_2e^{-h\nu/kT}\frac{F(\nu)}{e^{h\nu/kT}-1}=
B_{12}g_1\frac{F(\nu)}{e^{h\nu/kT}-1}

separating to:

A_{21}g_2(e^{h\nu/kT}-1)+ B_{21}g_2F(\nu)= B_{12}g_1e^{h\nu/kT}F(\nu)\,

The above equation must hold at any temperature, so

A_{21}g_2 = B_{12}g_1F(\nu)\,

and

- A_{21}g_2 + B_{21}g_2F(\nu) = 0\,

Therefore the three Einstein coefficients are interrelated by:

\frac{A_{21}}{B_{21}}=F(\nu)

and

\frac{B_{21}}{B_{12}}=\frac{g_1}{g_2}

When this relation is inserted into the original equation, one can also find a relation between A_{21} and B_{12}, involving Planck's law.

Oscillator strengths[edit]

The oscillator strength f_{12} is defined by the following relation to the cross section a_{12} for absorption:

a_{12}=\frac{\pi e^2}{2 \varepsilon_0 m_e c}\,f_{12}

where e is the electron charge and m_e is the electron mass. This allows all three Einstein coefficients to be expressed in terms of the single oscillator strength associated with the particular atomic spectral line:

B_{12}=\frac{4\pi^2 e^2}{m_e h\nu c}\,f_{12}
B_{21}=\frac{4\pi^2 e^2}{m_e h\nu c}~\frac{g_1}{g_2}~f_{12}
A_{21}=\frac{8\nu^2 \pi^2 e^2}{m_e c^3}~\frac{g_1}{g_2}~f_{12}

In Gaussian units, the A coefficient is in \text{s}^{-1} and the B coefficients are in \text{cm}^2 \text{s}^{-1} \text{erg}^{-1}.

See also[edit]

References[edit]

  1. ^ Bohr 1913
  2. ^ a b Einstein 1916
  3. ^ Sommerfeld 1923, p. 43
  4. ^ Heisenberg 1925, p. 108
  5. ^ Brillouin 1970, p. 31
  6. ^ Jammer 1989, pp. 113, 115
  7. ^ Weinstein, M.A. (1960). On the validity of Kirchhoff's law for a freely radiating body, American Journal of Physics, 28: 123-25.
  8. ^ Burkhard, D.G., Lochhead, J.V.S., Penchina, C.M. (1972). On the validity of Kirchhoff's law in a nonequilibrium environment, American Journal of Physics, 40: 1794-1798.
  9. ^ Baltes, H.P. (1976). On the validity of Kirchhoff's law of heat radiation for a body in a nonequilibrium environment, Chapter 1, pages 1-25 of Progress in Optics XIII, edited by E. Wolf, North-Holland, ISSN 00796638.
  10. ^ Milne, E.A. (1928). The effect of collisions on monochromatic radiative equilibrium, Monthly Notices of the Royal Astronomical Society, 88: 493-502. [1]
  11. ^ Chandrasekhar, S. (1950), p. 7.
  12. ^ a b Mihalas, D., Weibel-Mihalas, B. (1984), pp. 329–330.
  13. ^ Loudon, R. (2000), Section 1.5, pp. 16–19.
  14. ^ Hilborn, R.C. (2002). Einstein coefficients, cross sections, f values, dipole moments, and all that.
  15. ^ Herzberg, G. (1950).
  16. ^ a b Yariv, A. (1967/1989), pp. 171–173.
  17. ^ Garrison, J.C., Chiao, R.Y. (2008), pp. 15–19.
  18. ^ Chandrasekhar, S. (1950), p. 354
  19. ^ Goody, R.M., Yung, Y.L. (1989), pp. 33–35.
  20. ^ Loudon,R. (1973/2000), pp. 16–19.

Cited bibliography[edit]

Other reading[edit]

  • Condon, E.U. and Shortley, G.H. (1964). The Theory of Atomic Spectra. Cambridge University Press. ISBN 0-521-09209-4. 
  • Rybicki, G.B. and Lightman, A.P. (1985). Radiative processes in Astrophysics. John Wiley & Sons, New York. ISBN 0-471-82759-2. 
  • Shu, F.H. (1991). The Physics of Astrophysics - Volume 1 - Radiation. University Science Books, Mill Valley, CA. ISBN 0-935702-64-4. 
  • Robert C. Hilborn (2002). "Einstein coefficients, cross sections, f values, dipole moments, and all that". physics/0202029. 
  • Taylor, M.A. and Vilchez, J.M. (2009). "Tutorial: Exact solutions for the populations of the n-level ion". Pub. Astron. Soc. Pac. 121, 885: 1257–1266. 

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