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Quasinormal modes (QNM) are the modes of energy dissipation of a perturbed object or field, i.e. they describe perturbations of a field that decay in time.

Example

A familiar example is the perturbation (gentle tap) of a wine glass with a knife: the glass begins to ring, it rings with a set, or superposition, of its natural frequencies — its modes of sonic energy dissipation. One could call these modes normal if the glass went on ringing forever. Here the amplitude of oscillation decays in time, so we call its modes quasi-normal. To a high degree of accuracy, quasinormal ringing can be approximated by

${\displaystyle \psi (t)\approx e^{-\omega ^{\prime \prime }t}\cos \omega ^{\prime }t}$

where ${\displaystyle \psi \left(t\right)}$ is the amplitude of oscillation, ${\displaystyle \omega ^{\prime }}$ is the frequency, and ${\displaystyle \omega ^{\prime \prime }}$ is the decay rate. The quasinormal frequency is described by two numbers,

${\displaystyle \omega =\left(\omega ^{\prime },\omega ^{\prime \prime }\right)}$

or, more compactly

${\displaystyle \psi \left(t\right)\approx \operatorname {Re} (e^{i\omega t})}$

${\displaystyle \omega =\omega ^{\prime }+i\omega ^{\prime \prime }}$

Here, ${\displaystyle \mathbf {\omega } }$ is what is commonly referred to as the quasinormal mode frequency. It is a complex number with two pieces of information: real part is the temporal oscillation; imaginary part is the temporal, exponential decay.

In certain cases the amplitude of the wave decays quickly, to follow the decay for a longer time one may plot ${\displaystyle \log \left|\psi (t)\right|}$

Mathematical Physics

In theoretical physics, a quasinormal mode is a formal solution of linearized differential equations (such as the linearized equations of general relativity constraining perturbations around a black hole solution) with a complex eigenvalue (frequency).

Black holes have many quasinormal modes (also: ringing modes) that describe the exponential decrease of asymmetry of the black hole in time as it evolves towards the perfect spherical shape.

Recently, the properties of quasinormal modes have been tested in the context of the AdS/CFT correspondence. Also, the asymptotic behavior of quasinormal modes was proposed to be related to the Immirzi parameter in loop quantum gravity, but convincing arguments have not been found yet.

Electromagnetism and photonics

In the first type, high Q factors are achieved with lossless dielectric optical materials, with mode volumes of the order of a cubic wavelength, essentially limited by the diffraction limit. Famous examples of high-Q microcavity with are micropillar cavities, microtoroid resonators, photonic-crystal cavities. In the second type of resonators, the characteristic size is well below the diffraction limit, routinely by 2-3 orders of magnitude. In such small volumes, energies are stored for a small period of time. A tiny piece of dielectric or metallic material, a plasmonic nanoantenna supporting localized surface plasmons essentially behaves as a poor antenna that radiates energy rather than stores it. Thus, as the optical mode becomes deeply sub-wavelength in all three dimensions, independent of its shape, the Q-factor is limited to about 10.

Formally, the resonances (i.e., the quasinormal mode) of an open (with non-Hermitian hamiltonians) electromagnetic micro or nanoresonators are found by solving the time-harmonic source-free Maxwell’s equations with a complex frequency, the real part being the resonance frequency and the imaginary part the damping rate. The damping is due to energy loses via leakage (the cavity is coupled to the open space surrounding it) and/or material absorption. Effective quasinormal modes solvers exist to compute and normalize the modes of plasmonic nanoresonators and photonic cavities. Their proper normalisation leads to the important concepts of mode volume of non-Hermitian (open and lossy) systems. The mode volume directly impact the physics of the interaction of light and electrons with resonance, e.g. the local density of electromagnetic states, Purcell effect, cavity perturbation theory, strong interaction with quantum emitters, superradiance.

Biophysics

In computational biophysics, quasinormal modes, also called quasiharmonic modes, are derived from diagonalizing the matrix of equal-time correlations of atomic fluctuations.

See also

• Resonance (quantum field theory).

References

1. Konoplya, R. A.; Zhidenko, Alexander (2011-07-11). "Quasinormal modes of black holes: From astrophysics to string theory". Reviews of Modern Physics. 83 (3): 793–836. arXiv:1102.4014. Bibcode:2011RvMP...83..793K. doi:10.1103/RevModPhys.83.793.
2. Kokkotas, Kostas D.; Schmidt, Bernd G. (1999-01-01). "Quasi-Normal Modes of Stars and Black Holes". relativity.livingreviews.org. Archived from the original on 2015-12-22. Retrieved 2015-10-29. {{cite web}}: Unknown parameter |deadurl= ignored (|url-status= suggested) (help)
3. Lalanne, P.; Yan, W.; Vynck, K.; Sauvan, C.; Hugonin, J.-P. (2018-04-17). "Light interaction with photonic and plasmonic resonances". Laser & Photonics Reviews. 12 (5): 1700113. doi:10.1002/lpor.201700113.

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