Measuring nanomechanical motion with a microwave cavity interferometer
By C. Regal, John Teufel, Konrad W. Lehnert. 2008
464 citations recorded by the source corpus.
Measurements of the position of a nanoscale beam using a microwave cavity detector represents a promising step towards being able to measure displacements at the quantum limit.
Subfields: Atomic and Molecular Physics, and Optics, Electrical and Electronic Engineering
View Paper: https://www.semanticscholar.org/paper/797eba5ef94da87f252fa376a5860958d92fa63b
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
- Steven M. Girvin
- Robert J. Schoelkopf
- Michel H. Devoret
- A. Clerk
- John Clarke
- Franco Nori
- Florian Marquardt
- Herre S. J. van der Zant
In Electrical and Electronic Engineering
- A. Clerk
- Florian Marquardt
- Yun-Feng Xiao
- John Clarke
- Menno Poot
- Yong‐Chun Liu
- B. Kubala
- Michel H. Devoret
Citations in the corpus
- The optomechanical instability in the quantum regime (2008, background): “This includes driven LC circuits coupled to cantilevers [22], singleelectron transistors (SET) and microwave cavities coupled to nanobeams [23]–[30], as well as clouds of cold atoms in an optical lattice inside a cavity [31]–[33].”
- Mechanical systems in the quantum regime (2011, methodology): “5 · 103 19 [50]”
- Electromagnetically induced transparency in optical microcavities (2017, background): “Various experimental systems existing such interactions are proposed and investigated, including FP cavities [94, 95], whispering-gallery microcavities [96–99], microring cavities [100], photonic crystal cavities [101– 104], membranes [105–108], nanostrings [109], nanorods [110–112], hybrid plasmoni”
- The physics of superconducting microwave resonators (2008, methodology): “3 Coupling nanomechanical resonators to microwave resonators A superconducting microwave resonator is also used in an recent experiment to read out the motion of a nanomechanical beam, or the quantum mechanical state of a mechanical harmonic oscillator[36].”
- Noiseless non-reciprocity in a parametric active device (2010, methodology): “For this choice of parameters, we obtain the scatteringmatrix of the complete device as Stotal= 0 0 0 i 0 0 −i 0 i 0 0 0 0 i 0 0 (4)”