Static and dynamic wavelength routing via the gradient optical force
By J. Rosenberg, Qiang Lin, Kerry J. Vahala, Oskar J. Painter. 2009
187 citations recorded by the source corpus.
We propose and demonstrate an all-optical wavelength routing approach that uses a tuning mechanism based upon the optical gradient force in a specially designed nano-optomechanical system. The resulting mechanically compliant 'spiderweb' resonator realizes seamless wavelength routing over a range of 3,000 times the intrinsic channel width, with a tuning efficiency of 309 GHz mW^(-1), a switching time of less than 200 ns, and 100% channel quality preservation over the entire tuning range. These results indicate the potential for radiation pressure actuated devices to be used in a variety of photonics applications, such as channel routing/switching, buffering, dispersion compensation, pulse trapping/release and widely tunable lasers.
Subfields: Atomic and Molecular Physics, and Optics, Electrical and Electronic Engineering
View Paper: https://www.semanticscholar.org/paper/17ce20b72d0badeeb1245aa788e0c6ede919e857
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Atomic and Molecular Physics, and Optics
- Herre S. J. van der Zant
- Menno Poot
- Darrick E. Chang
- Oskar J. Painter
- Florian Marquardt
- H. Jeff Kimble
- D. van Thourhout
- James S. Douglas
In Electrical and Electronic Engineering
- Herre S. J. van der Zant
- Menno Poot
- Oskar J. Painter
- A. Safavi-Naeini
- Florian Marquardt
- D. van Thourhout
- Darrick E. Chang
- Kerry J. Vahala
Citations in the corpus
- Quantum matter built from nanoscopic lattices of atoms and photons (2018, background): “…the type of spin interaction (of exchange type) is fixed, as is the interaction range L for a given structure design, unless the structure itself exhibits some dynamic tunability [for example, via piezoeletric strain (Wong et al., 2004) or optomechanical forces (Rosenberg, Lin, and Painter, 2009)].”
- Mechanical systems in the quantum regime (2011, background): “e spring constant of the resonator to kR = k0 − ∂Frad/∂u; the so-called optical spring [224, 225, 226, 227, 228, 39, 229, 230]. Similar to displacement-proportionalfeedback this can cool the resonator[39, 64, 231] and can even lead to bistability of the resonator position [225]. A much stronger cool”
- Slowing and stopping light using an optomechanical crystal array (2010, background): “The possibility of using optomechanical systems to facilitate major tasks in classical optical networks has been suggested in several recent proposals [20, 25, 35].”
- Coherent mixing of mechanical excitations in nano-optomechanical structures (2009, background): “More recently[19, 20, 21, 22, 23, 24], it has been realized that guided wave nanostructures can also be used to generate extremely large per-photon optical forces via the gradient optical force[25].”
- Optomechanical device actuation through the optical gradient force (2010, background): “, there is only a 'point contact' between both resonators, whereas for the vertically coupled ring resonator”
- Generalized non-reciprocity in an optomechanical circuit via synthetic magnetism and reservoir engineering (2016, background): “Optomechanical systems [14], involving the coupling of light intensity to mechanical motion via radiation pressure, are a particularly promising venue for studying synthetic fields, as they can be used to create the requisite large optical nonlinearities [15].”