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{{Short description|Quantized periodic motion of atoms in a molecule}}
{{Quantum matter backlink|Molecules}}

'''Quantum molecular vibration''' is the quantized periodic motion of atoms in a [[Physics:Quantum molecular structure|molecule]] relative to one another, with the center of mass of the molecule remaining unchanged. Molecular vibrations are central to [[Physics:Quantum molecular spectroscopy|molecular spectroscopy]], because vibrational transitions produce characteristic infrared and Raman spectra that reveal bond strengths, molecular geometry, symmetry, and chemical structure.

Typical molecular vibrational frequencies range from less than 10<sup>13</sup> Hz to about 10<sup>14</sup> Hz, corresponding to wavenumbers of roughly 300–3000 cm<sup>−1</sup> and wavelengths of about 30–3 µm. These energies usually lie in the infrared region of the electromagnetic spectrum.
<div style="float:right; border:1px solid #e0d890; background:#fff8cc; padding:6px; margin:0 0 1em 1em; width:420px;">
[[File:Anharmonic oscillator.gif|400px]]
<div style="font-size:90%;">A molecular vibration can often be approximated by a harmonic oscillator, but real molecular bonds are anharmonic and can eventually dissociate.</div>
</div>
=Overview=
For a diatomic molecule A–B, the vibrational frequency can be approximated by treating the bond as a spring. In this model,

:<math>\nu = \frac{1}{2 \pi} \sqrt{\frac{k}{\mu}},</math>

where <math>k</math> is the force constant and <math>\mu</math> is the reduced mass,

:<math>\frac{1}{\mu} = \frac{1}{m_A}+\frac{1}{m_B}.</math>

The vibrational wavenumber is

:<math>\tilde{\nu} = \frac{1}{2 \pi c} \sqrt{\frac{k}{\mu}},</math>

where <math>c</math> is the speed of light. Stronger bonds and lighter atoms generally give higher vibrational frequencies.

Vibrations of polyatomic molecules are described in terms of [[Physics:Quantum molecular vibration#Normal coordinates|normal modes]]. These modes are independent collective motions of the nuclei, but each normal mode may involve simultaneous movement of several atoms. A nonlinear molecule with <math>N</math> atoms has <math>3N-6</math> normal modes of vibration, while a linear molecule has <math>3N-5</math> modes because rotation about the molecular axis does not change the nuclear coordinates.<ref>{{cite book |last=Landau |first=L. D. |last2=Lifshitz |first2=E. M. |year=1976 |title=Mechanics |edition=3rd |publisher=Pergamon Press |isbn=0-08-021022-8 |url-access=registration |url=https://archive.org/details/mechanics00land }}</ref>

=Quantum description=
A molecular vibration is excited when the molecule absorbs energy corresponding to the vibration frequency. The energy spacing is approximately

:<math>\Delta E = h\nu,</math>

where <math>h</math> is Planck's constant and <math>\nu</math> is the vibrational frequency. A fundamental vibration occurs when one quantum of vibrational energy is absorbed from the ground vibrational state. When additional quanta are absorbed, overtones may be excited.

To a first approximation, the motion in a normal vibration can be described as [[Physics:Quantum harmonic oscillator|simple harmonic motion]]. In this approximation, the vibrational energy is a quadratic function of the atomic displacement, and the energy levels are evenly spaced:

:<math>E_v = h\nu\left(v+\frac{1}{2}\right),\qquad v=0,1,2,\ldots</math>

where <math>v</math> is the vibrational quantum number.<ref>{{cite book |first=J. M. |last=Hollas |title=Modern Spectroscopy |edition=3rd |publisher=John Wiley |year=1996 |page=21 |isbn=0471965227 }}</ref><ref>{{cite book |first=P. W. |last=Atkins |first2=J. de |last2=Paula |title=Physical Chemistry |edition=8th |publisher=W. H. Freeman |location=New York |year=2006 |pages=[https://archive.org/details/atkinsphysicalch00pwat/page/291 291 and 453] |isbn=0716787598 |url=https://archive.org/details/atkinsphysicalch00pwat/page/291 }}</ref>

In real molecules, vibrations are anharmonic. The first overtone is therefore slightly less than twice the fundamental frequency, and higher overtones require progressively less additional energy. At sufficiently high vibrational excitation, the molecule may dissociate. The potential energy curve of a real bond is therefore better represented by a Morse potential than by a perfect parabola.

=Infrared and Raman spectroscopy=
The vibrational states of a molecule can be probed in several ways. The most direct method is infrared spectroscopy, because vibrational transitions often require energies in the infrared region of the spectrum. A vibration is infrared-active when it changes the molecular dipole moment.

Raman spectroscopy can also measure vibrational frequencies. In Raman spectroscopy, the intensity of a band depends on the change of molecular polarizability with respect to the normal coordinate. Infrared and Raman spectroscopy are complementary: some vibrations that are weak or forbidden in infrared spectroscopy may appear strongly in Raman spectra, and vice versa.

Vibrational excitation can also occur together with electronic excitation. The combined transition is called a vibronic transition and gives vibrational fine structure to electronic spectra, especially for molecules in the gas phase.

Simultaneous excitation of vibration and rotation gives rise to vibration–rotation spectra, also called rovibrational spectra.

=Number of vibrational modes=
For a molecule with <math>N</math> atoms, the positions of all nuclei depend on <math>3N</math> coordinates. These coordinates include translation, rotation, and vibration. Translation corresponds to motion of the center of mass and accounts for three degrees of freedom.

A nonlinear molecule can rotate about three mutually perpendicular axes and therefore has three rotational degrees of freedom. A linear molecule has only two rotational degrees of freedom because rotation about the molecular axis does not change the positions of the nuclei.<ref name=Hollas77>{{cite book |first=J. M. |last=Hollas |title=Modern Spectroscopy |edition=3rd |publisher=John Wiley |year=1996 |page=77 |isbn=0471965227 }}</ref><ref name=Banwell>{{cite book |last=Banwell |first=Colin N. |last2=McCash |first2=Elaine M. |year=1994 |title=Fundamentals of Molecular Spectroscopy |url=https://archive.org/details/isbn_9780077079765 |url-access=registration |edition=4th |publisher=McGraw Hill |isbn=0-07-707976-0 |page=[https://archive.org/details/isbn_9780077079765/page/71 71] }}</ref>

Thus the number of vibrational modes is

:<math>3N-6</math>

for nonlinear molecules, and

:<math>3N-5</math>

for linear molecules.<ref name=Hollas77/><ref name=Banwell/><ref name=Atk460>{{cite book |first=P. W. |last=Atkins |first2=J. de |last2=Paula |title=Physical Chemistry |edition=8th |publisher=W. H. Freeman |location=New York |year=2006 |page=[https://archive.org/details/atkinsphysicalch00pwat/page/460 460] |isbn=0716787598 |url=https://archive.org/details/atkinsphysicalch00pwat/page/460 }}</ref>

A diatomic molecule has one vibrational mode, corresponding to stretching and compression of the single bond.

=Vibrational coordinates=
The coordinate of a normal vibration is a combination of changes in the positions of atoms in the molecule. When the vibration is excited, the coordinate changes approximately sinusoidally with the vibrational frequency.

==Internal coordinates==
Internal coordinates describe molecular motion in terms of changes in bond lengths, bond angles, and relative group orientations. Common internal coordinates include:

* '''Stretching''': a change in the length of a bond, such as C–H or C–C.
* '''Bending''': a change in the angle between two bonds.
* '''Rocking''': a change in angle between a group of atoms and the rest of the molecule.
* '''Wagging''': motion of a group of atoms out of a reference plane.
* '''Twisting''': a change in the angle between two planes defined by groups of atoms.
* '''Out-of-plane motion''': movement of an atom or bond out of a molecular plane.

These internal coordinates do not necessarily correspond directly to normal modes. A normal mode may be a linear combination of several internal coordinates.

==Methylene-group vibrations==
Within a CH<sub>2</sub> group, the two hydrogen atoms can vibrate in several characteristic ways. These are commonly grouped as stretching, bending, rocking, wagging, and twisting motions.

{| class="wikitable"
|-
! Symmetric stretching
! Asymmetric stretching
! Scissoring
|-
| [[Image:Symmetrical stretching.gif]]
| [[Image:Asymmetrical stretching.gif]]
| [[Image:Scissoring.gif]]
|-
! Rocking
! Wagging
! Twisting
|-
| [[Image:Modo rotacao.gif]]
| [[Image:Wagging.gif]]
| [[Image:Twisting.gif]]
|}

=Symmetry-adapted coordinates=
Symmetry-adapted coordinates are constructed by applying projection operators to internal coordinates. The projection operators are built from the character table of the molecular point group.<ref name="Cotton">{{cite book |first=F. A. |last=Cotton |title=Chemical Applications of Group Theory |publisher=Wiley |edition=2nd |year=1971 |location=New York |isbn=0471175706 }}</ref>

For example, the four unnormalized C–H stretching coordinates of ethene may be combined as

:<math>\begin{align}
Q_{s1} &= q_{1} + q_{2} + q_{3} + q_{4},\\
Q_{s2} &= q_{1} + q_{2} - q_{3} - q_{4},\\
Q_{s3} &= q_{1} - q_{2} + q_{3} - q_{4},\\
Q_{s4} &= q_{1} - q_{2} - q_{3} + q_{4}.
\end{align}</math>

Here <math>q_1</math> to <math>q_4</math> are internal coordinates for stretching of the four C–H bonds. Illustrations of symmetry-adapted coordinates for many small molecules can be found in Nakamoto.<ref name="Nakamoto">{{cite book |first=K. |last=Nakamoto |title=Infrared and Raman spectra of inorganic and coordination compounds, Part A |edition=5th |publisher=Wiley |location=New York |year=1997 |isbn=0471163945 }}</ref>

=Normal coordinates=
Normal coordinates, usually denoted <math>Q</math>, describe displacement along normal modes of vibration. Each normal mode has one normal coordinate. Normal modes diagonalize the matrix governing molecular vibrations, so each normal mode behaves as an independent vibration in the harmonic approximation.

If the molecule has symmetry, its normal modes transform according to irreducible representations of the molecular point group. For example, in carbon dioxide, the two C–O stretches are not independent local bond motions. They combine into a symmetric stretch and an asymmetric stretch:

* '''Symmetric stretching''': the two C–O bond lengths change by the same amount.
* '''Asymmetric stretching''': one C–O bond length increases while the other decreases.

When two or more normal coordinates have the same symmetry, mixing occurs and the coefficients of the linear combination cannot be determined by symmetry alone. A full normal-coordinate analysis is then required.

The Wilson GF method is a standard way to calculate normal modes and vibrational frequencies.<ref name="WilsonDeciusCross">{{cite book |first=E. B. |last=Wilson |first2=J. C. |last2=Decius |first3=P. C. |last3=Cross |title=Molecular Vibrations |location=New York |orig-year=1955 |publisher=Dover |year=1995 |isbn=048663941X |url=https://archive.org/details/molecularvibrati00wils }}</ref>

=Newtonian approximation=
Although molecular vibrations are quantum mechanical, their approximate frequencies can often be calculated with Newtonian mechanics. In the harmonic approximation, each vibration is treated as if it were a spring obeying Hooke's law:

:<math>F=-kQ.</math>

By Newton's second law,

:<math>F=\mu\frac{d^2Q}{dt^2},</math>

so the equation of motion becomes

:<math>\mu\frac{d^2Q}{dt^2}+kQ=0.</math>

Its solution is

:<math>Q(t)=A\cos(2\pi\nu t),\qquad \nu={1\over 2\pi}\sqrt{\frac{k}{\mu}}.</math>

In this expression, <math>A</math> is the amplitude, <math>k</math> is the force constant, and <math>\mu</math> is the reduced mass. For a diatomic molecule AB,

:<math>\frac{1}{\mu}=\frac{1}{m_A}+\frac{1}{m_B}.</math>

The use of the reduced mass ensures that the center of mass of the molecule is not affected by the vibration. In the harmonic approximation, the potential energy is quadratic in the normal coordinate:

:<math>V(Q)\approx \frac{1}{2}kQ^2.</math>

The force constant is therefore related to the curvature of the potential energy surface:

:<math>k=\frac{\partial^2 V}{\partial Q^2}.</math>

When two or more normal vibrations have the same symmetry, a full normal coordinate analysis must be performed. In the Wilson GF method, vibrational frequencies are obtained from eigenvalues of the matrix product <math>GF</math>, where <math>G</math> depends on masses and molecular geometry and <math>F</math> depends on force constants.<ref name="WilsonDeciusCross"/><ref name="Gans">{{cite book |first=P. |last=Gans |title=Vibrating Molecules |publisher=Chapman and Hall |location=New York |year=1971 |isbn=0412102900 }}</ref>

=Quantum mechanics=
In quantum mechanics, the harmonic approximation leads to the Schrödinger equation for each normal coordinate. The vibrational energy levels are

:<math>E_v=h\nu\left(v+\frac{1}{2}\right),\qquad v=0,1,2,\ldots</math>

where <math>v</math> is the vibrational quantum number. The difference between adjacent levels is

:<math>\Delta E=h\nu.</math>

For a harmonic oscillator, the basic selection rule is

:<math>\Delta v=\pm 1.</math>

This selection rule explains why the fundamental vibrational transition is strongest in the ideal harmonic approximation. Overtone transitions such as <math>\Delta v=2</math> become possible because real molecules are anharmonic. Anharmonicity also explains hot bands, where transitions begin from already excited vibrational states.

For anharmonic oscillators, vibrational levels may be represented by expansions such as the Dunham expansion. These descriptions account for decreasing level spacings and the approach to molecular dissociation.

=Intensities=
In an infrared spectrum, the intensity of an absorption band is proportional to the change of the molecular dipole moment with respect to the normal coordinate.<ref name="Steele">{{cite book |first=D. |last=Steele |title=Theory of vibrational spectroscopy |publisher=W. B. Saunders |location=Philadelphia |year=1971 |isbn=0721685803 |url-access=registration |url=https://archive.org/details/theoryofvibratio0000stee }}</ref> A vibration is infrared-active when

:<math>\frac{\partial \mu}{\partial Q}\neq 0.</math>

In Raman spectroscopy, the intensity depends on the change in polarizability with respect to the normal coordinate:

:<math>\frac{\partial \alpha}{\partial Q}\neq 0.</math>

This distinction explains why infrared and Raman spectra often provide complementary information about the same molecule.

=Applications=
Molecular vibration is used to interpret infrared and Raman spectra, identify functional groups, determine molecular symmetry, estimate bond strengths, and study molecular structure. It is important in chemical physics, atmospheric spectroscopy, astrochemistry, materials science, plasma diagnostics, and the study of molecular energy transfer.

=See also=
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also/Matter}}

=References=
{{reflist|3}}

=Further reading=
* {{cite book |first=P. M. A. |last=Sherwood |title=Vibrational Spectroscopy of Solids |publisher={{wipe|Cambridge University Press}} |year=1972 |isbn=0521084822 }}

{{Author|Harold Foppele}}

{{Sourceattribution|Physics:Quantum molecular vibration|1}}

Physics:Quantum molecular vibration - Revision history

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