Cavity Optomechanics: Nano- and Micromechanical Resonators by Markus Aspelmeyer, Tobias J. Kippenberg, Florian Marquardt

By Markus Aspelmeyer, Tobias J. Kippenberg, Florian Marquardt

During the previous couple of years cavity-optomechanics has emerged as a brand new box of analysis. This hugely interdisciplinary box stories the interplay among micro and nano mechanical platforms and lightweight. attainable functions variety from novel high-bandwidth mechanical sensing units in the course of the new release of squeezed optical or mechanical states to even assessments of quantum thought itself. this is often one of many first books during this quite younger box. it really is aimed toward scientists, engineers and scholars who are looking to receive a concise creation to the state-of-the-art within the box of hollow space optomechanics. it's important to researchers in nano technology, quantum optics, quantum info, gravitational wave detection and different innovative fields. attainable purposes comprise organic sensing, frequency comb functions, silicon photonics and so forth. The technical content material should be available to those that have familiarity with easy undergraduate physics.

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Extra info for Cavity Optomechanics: Nano- and Micromechanical Resonators Interacting with Light

Example text

These conditions are already suggested by Eq. , large mechanical quality factor Q; S XoutY (ω) means large radiation pressure, achieved at large intracavity field and small mass. 11) → 0, and φopt (ω) ≈ − 21 arctan → 0. Since the field quadrature δ X out at φ = 0 is just at the shot-noise limit (see Eq. 8)), one has that squeezing is achieved only within a narrow interval for the homodyne phase around φopt (ω), of width ∼ 2 φopt (ω) ∼ arctan 2/S XoutY (ω) . This extreme phase dependence is a general and well-known property of quantum squeezing, which is due to the Heisenberg principle: the width of the interval of 2 S out X Y (ω) 30 (a) K.

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