- Franck-Condon principle
The

**Franck-Condon principle**is a rule inspectroscopy andquantum chemistry that explains the intensity ofvibronic transition s. Vibronic transitions are the simultaneous changes in electronic and vibrational energy levels of a molecule due to the absorption or emission of aphoton of the appropriate energy. The principle states that during anelectronic transition , a change from one vibrationalenergy level to another will be more likely to happen if the two vibrationalwave functions overlap more significantly.**Overview**The Franck-Condon principle has a well-established

semiclassical interpretation based on the original contributions ofJames Franck [Franck 1927] .Electronic transition s are essentially instantaneous compared with the time scale of nuclear motions, therefore if the molecule is to move to a new vibrational level during the electronic transition, this new vibrational level must be instantaneously compatible with the nuclear positions and momenta of the vibrational level of the molecule in the originating electronic state. In the semiclassical picture of vibrations (oscillations) of a simple harmonic oscillator, the necessary conditions can occur at the turning points, where the momentum is zero.\ 0 end{matrix}

The spin-independent part of the initial integral is here "approximated" as a product of two integrals :$intint\; \{\; psi\; \_v\text{'}^\; *\; \}\; \{\; psi\; \_e\text{'}^\; *\; \}\; \backslash boldsymbol\{mu\}\; \_e\; psi\; \_e\; psi\; \_v\; d\; au\_e\; d\; au\_napprox\; int\{\; psi\; \_v\text{'}^\; *\; \}\; psi\; \_vd\; au\_n\; int\; \{\; psi\; \_e\text{'}^\; *\; \}\; \backslash boldsymbol\{mu\}\; \_e\; psi\; \_e\; d\; au\_e\; .$This factorization would be exact if the integral $int\; \{\; psi\; \_e\text{'}^\; *\; \}\; \backslash boldsymbol\{mu\}\; \_e\; psi\; \_e\; d\; au\_e$ over the spatial coordinates of the electrons would not depend on the nuclear coordinates. However, in the Born-Oppenheimer approximation $psi\_e,$ and $psi\text{'}\_e,$ do depend (parametrically) on the nuclear coordinates, so that the integral (a so-called "transition dipole surface") is a function of nuclear coordinates. Since the dependence is usually rather smooth its neglect (i.e., the assumption that the transition dipole surface is independent of nuclear coordinates, called the "Condon approximation") is often allowed.

The first integral after the plus sign is equal to zero because electronic wavefunctions of different states are orthogonal. Remaining is the product of three integrals. The first integral is the vibrational overlap integral, also called the

**Franck-Condon factor**. The remaining two integrals contributing to the probability amplitude determine the electronic spatial and spin selection rules.The Franck-Condon principle is a statement on allowed

**vibrational**transitions between two "different" electronic states, other quantum mechanicalselection rules may lower the probability of a transition or prohibit it altogether. Rotational selection rules have been neglected in the above derivation. Rotational contributions can be observed in the spectra of gases but are strongly suppressed in liquids and solids.It should be clear that the quantum mechanical formulation of the Franck-Condon principle is the result of a series of approximations, principally the electrical dipole transition assumption and the Born-Oppenheimer approximation. Weaker magnetic dipole and electric

quadrupole electronic transitions along with the incomplete validity of the factorization of the total wavefunction into nuclear, electronic spatial and spin wavefunctions means that the selection rules, including the Franck-Condon factor, are not strictly observed. For any given transition, the value of**"P**" is determined by all of the selection rules, however spin selection is the largest contributor, followed by electronic selection rules. The**Franck-Condon factor**only "weakly" modulates the intensity of transitions, i.e., it contributes with a factor on the order of 1 to the intensity of bands whose order of magnitude is determined by the other selection rules. The table below gives the range of extinction coefficients for the possible combinations of allowed and forbidden spin and orbital selection rules.**Franck-Condon metaphors in spectroscopy**The Franck-Condon principle, in its canonical form, applies only to changes in the vibrational levels of a molecule in the course of a change in electronic levels by either absorption or emission of a photon. The physical intuition of this principle is anchored by the idea that the nuclear coordinates of the atoms constituting the molecule do not have time to change during the very brief amount of time involved in an electronic transition. However, this physical intuition can be, and is indeed, routinely extended to interactions between light absorbing or emitting molecules (

chromophore s) and their environment. Franck-Condonmetaphors are appropriate because molecules often interact strongly with surrounding molecules, particularly in liquids and solids, and these interactions modify the nuclear coordinates of the chromophore in ways which are closely analogous to the molecular vibrations considered by the Franck-Condon principle.**Franck-Condon principle for phonons**The closest Franck-Condon

analogy is due to the interaction ofphonons —quanta of lattice vibrations— with the electronic transitions of chromophores embedded as impurities the lattice. In this situation, transitions to higher electronic levels can take place when the energy of the photon corresponds to the purely electronic transition energy or to the purely electronic transition energy plus the energy of one or more lattice phonons. In the low-temperature approximation, emission is from the zero-phonon level of the excited state to the zero-phonon level of the ground state or to higher phonon levels of the ground state. Just like in the Franck-Condon principle, the probability of transitions involving phonons is determined by the overlap of the phonon wavefunctions at the initial and final energy levels. For the Franck-Condon principle applied to phonon transitions, the label of the horizontal axis of Figure 1 is replaced in Figure 6 with the configurational coordinate for anormal mode . The lattice mode $q\_i$ potential energy in Figure 6 is represented as that of a harmonic oscillator, and the spacing between phonon levels ($hbar\; Omega\; \_i$)is determined by lattice parameters. Because the energy of single phonons is generally quite small, zero- or few-phonon transitions can only be observed at temperatures below about 40kelvins .:See

Zero-phonon line and phonon sideband for further details and references.**Franck-Condon principle in solvation**Franck-Condon considerations can also be applied to the electronic transitions of chromophores dissolved in liquids. In this use of the Franck-Condon metaphor, the vibrational levels of the chromophores, as well as interactions of the chromophores with phonons in the liquid, continue to contribute to the structure of the absorption and emission spectra, but these effects are considered separately and independently.

Consider chromophores surrounded by

solvent molecules. These surrounding molecules may interact with the chromophores, particularly if the solvent molecules are polar. This association between solvent andsolute is referred to assolvation and is a stabilizing interaction, that is, the solvent molecules can move and rotate until the energy of the interaction is minimized. The interaction itself involveselectrostatic andvan der Waals forces and can also includehydrogen bonds . Franck-Condon principles can be applied when the interactions between the chromophore and the surrounding solvent molecules are different in the ground and in the excited electronic state. This change in interaction can originate, for example, due to different dipole moments in these two states. If the chromophore starts in its ground state and is close to equilibrium with the surrounding solvent molecules and then absorbs a photon that takes it to the excited state, its interaction with the solvent will be far from equilibrium in the excited state. This effect is analogous to the original Franck-Condon principle: the electronic transition is very fast compared with the motion of nuclei—the rearrangement of solvent molecules in the case of solvation—. We now speak of a vertical transition, but now the horizontal coordinate is solvent-solute interaction space. This coordinate axis is often labeled as "Solvation Coordinate" and represents, somewhat abstractly, all of the relevant dimensions of motion of all of the interacting solvent molecules.In the original Franck-Condon principle, after the electronic transition, the molecules which end up in higher vibrational states immediately begin to relax to the lowest vibrational state. In the case of solvation, the solvent molecules will immediately try to rearrange themselves in order to minimize the interaction energy. The rate of solvent relaxation depends on the

viscosity of the solvent. Assuming the solvent relaxation time is short compared with the lifetime of the electronic excited state, emission will be from the lowest solvent energy state of the excited electronic state. For small-molecule solvents such aswater ormethanol at ambient temperature, solvent relaxation time is on the order of some tens ofpicosecond s whereas chromophore excited state lifetimes range from a few picoseconds to a fewnanoseconds . Immediately after the transition to the ground electronic state, the solvent molecules must also rearrange themselves to accommodate the new electronic configuration of the chromophore. Figure 7 illustrates the Franck-Condon principle applied to solvation. When thesolution is illuminated by with light corresponding to the electronic transition energy, some of the chromophores will move to the excited state. Within this group of chromophores there will be a statistical distribution of solvent-chromophore interaction energies, represented in the figure by aGaussian distribution function. The solvent-chromophore interaction is drawn as a parabolic potential in both electronic states. Since the electronic transition is essentially instantaneous on the time scale of solvent motion (vertical arrow), the collection of excited state chromophores is immediately far from equilibrium. The rearrangement of the solvent molecules according to the new potential energy curve is represented by the curved arrows in Figure 7. Note that while the electronic transitions are quantized, the chromophore-solvent interaction energy is treated as a classical continuum due to the large number of molecules involved. Although emission is depicted as taking place from the minimum of the excited state chromophore-solvent interaction potential, significant emission can take place before equilibrium is reached when the viscosity of the solvent is high or the lifetime of the excited state is short. The energy difference between absorbed and emitted photons depicted in Figure 7 is the solvation contribution to theStokes shift .**References**Journal links may require subscription.

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author = Condon, E.

year = 1926

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author = Condon, E.

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author = Condon, E.

year = 1928

title = Nuclear motions associated with electron transitions in diatomic molecules

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author = Birge, R. T.

year = 1926

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author = Noyes, W. A.

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title = The correlation of spectroscopy and photochemistry

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author = Coolidge, A. S, James, H. M. and Present, R. D.

year = 1936

title = A study of the Franck-Condon Principle

journal =Journal of Chemical Physics

volume = 4

pages = 193–211

doi = 10.1063/1.1749818 [*http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=JCPSA6000004000003000193000001&idtype=cvips&gifs=yes Link*]

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last = Herzberg | first = Gerhard

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title = The spectra and structures of simple free radicals

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last = Harris | first = Daniel C.

coauthors = Michael D. Bertolucci

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title = Symmetry and spectroscopy

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last = Bernath | first = Peter F.

year = 1995

title = Spectra of Atoms and Molecules (Topics in Physical Chemistry)

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last = Atkins | first = P. W.

coauthors = R. S. Frieman

year = 1999

title = Molecular Quantum Mechanics

location = Oxford

publisher = Oxford University Press

id = ISBN 0-19-855947-X**ee also***

Born-Oppenheimer approximation

*Molecular electronic transition

*Ultraviolet-visible spectroscopy

*Quantum harmonic oscillator

*Morse potential

*Vibronic coupling

*Zero-phonon line and phonon sideband

*Sudden approximation **External links*** http://www.iupac.org/goldbook/F02510.pdf

* http://www.life.uiuc.edu/govindjee/biochem494/Abs.html

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