Laser detuning: Difference between revisions
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==Illustration== |
==Illustration== |
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Let us consider a system with a resonance frequency <math>\omega_0</math> in the optical frequency range of the [[electromagnetic spectrum]], i.e. with frequency of a few THz to a few PHz, or equivalently with a wavelength in the range of 10 nm to 100 μm. If this system is excited by a laser with a frequency <math>\omega_L</math> close to this value, the laser detuning is then defined as:<math display="block">\Delta \omega\ \overset{\underset{\mathrm{def}}{}}{=} \ \omega_L - \omega_0 </math>The |
Let us consider a system with a resonance frequency <math>\omega_0</math> in the optical frequency range of the [[electromagnetic spectrum]], i.e. with frequency of a few THz to a few PHz, or equivalently with a wavelength in the range of 10 nm to 100 μm. If this system is excited by a laser with a frequency <math>\omega_L</math> close to this value, the laser detuning is then defined as:<math display="block">\Delta \omega\ \overset{\underset{\mathrm{def}}{}}{=} \ \omega_L - \omega_0 </math>The most common examples of such resonant systems in the optical frequency range are [[Optical cavity|optical cavities]] (free-space, fiber or [[Optical microcavity|microcavities]]), [[Atom|atoms]], and [[Dielectric|dielectrics]] or [[Semiconductor|semiconductors]]. |
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The laser detuning is important for a resonant system such as a cavity because it determines the phase (modulo 2π) acquired by the laser field per roundtrip. This is important for linear optical processes such as interference and scattering, and extremely important for [[Nonlinear optics|nonlinear optical]] processes because it affects the [[Nonlinear_optics#Phase_matching|phase-matching]] condition. |
The laser detuning is important for a resonant system such as a cavity because it determines the phase (modulo 2π) acquired by the laser field per roundtrip. This is important for linear optical processes such as interference and scattering, and extremely important for [[Nonlinear optics|nonlinear optical]] processes because it affects the [[Nonlinear_optics#Phase_matching|phase-matching]] condition. |
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== Applications == |
== Applications == |
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Revision as of 14:18, 26 November 2018
In optical physics, laser detuning is the tuning of a laser to a frequency that is slightly off from a quantum system's resonant frequency. When used as a noun, the laser detuning is the difference between the resonance frequency of the system and the laser's optical frequency (or wavelength). Lasers tuned to a frequency below the resonant frequency are called red-detuned, and lasers tuned above resonance are called blue-detuned.[1]
Illustration
Let us consider a system with a resonance frequency in the optical frequency range of the electromagnetic spectrum, i.e. with frequency of a few THz to a few PHz, or equivalently with a wavelength in the range of 10 nm to 100 μm. If this system is excited by a laser with a frequency close to this value, the laser detuning is then defined as:The most common examples of such resonant systems in the optical frequency range are optical cavities (free-space, fiber or microcavities), atoms, and dielectrics or semiconductors.
The laser detuning is important for a resonant system such as a cavity because it determines the phase (modulo 2π) acquired by the laser field per roundtrip. This is important for linear optical processes such as interference and scattering, and extremely important for nonlinear optical processes because it affects the phase-matching condition.
Applications
Laser cooling of atoms
Lasers can be detuned in the lab frame so that they are Doppler shifted to the resonant frequency in a moving system, which allows lasers to affect only atoms moving at a specific speed or in a specific direction and makes laser detuning a central tool of laser cooling[2] and magneto-optical traps.[1]
Optomechanics
Similar to the laser cooling of atoms, the sign of the detuning plays an important part in Optomechanical applications[3][4]. In the red detuned regime, the optomechanical system undergoes cooling and coherent energy transfer between the light and the mechanical mode (a "beam splitter"). In the blue-detuned regime, it undergoes heating, mechanical amplification and possibly squeezing and entanglement. The on-resonance case when the laser detuning is zero, can be used for very sensitive detection of mechanical motion, such as used in LIGO.
References
- ^ a b Fritz Riehle (8 May 2006). Frequency Standards: Basics and Applications. John Wiley & Sons. ISBN 978-3-527-60595-8. Retrieved 26 November 2011.
- ^ Harold J. Metcalf; Peter Van der Straten (1999). Laser cooling and trapping. Springer. ISBN 978-0-387-98728-6. Retrieved 26 November 2011.
- ^ Aspelmeyer, M.; Gröblacher, S.; Hammerer, K.; Kiesel, N. (2010-06-01). "Quantum optomechanics—throwing a glance [Invited]". JOSA B. 27 (6): A189–A197. Bibcode:2010JOSAB..27..189A. doi:10.1364/JOSAB.27.00A189. ISSN 1520-8540.
- ^ Aspelmeyer, Markus; Kippenberg, Tobias J.; Marquardt, Florian (2014-12-30). "Cavity optomechanics". Reviews of Modern Physics. 86 (4): 1391–1452. arXiv:1303.0733. Bibcode:2014RvMP...86.1391A. doi:10.1103/RevModPhys.86.1391.
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