419 research outputs found
Nanomechanical Inverse Electromagnetically Induced Transparency and Confinement of Light in Normal modes
We demonstrate the existence of the phenomenon of the inverse
electromagnetically induced transparency (IEIT) in an opto mechanical system
consisting of a nanomechanical mirror placed in an optical cavity. We show that
two weak counter-propagating identical classical probe fields can be completely
absorbed by the system in the presence of a strong coupling field so that the
output probe fields are zero. The light is completely confined inside the
cavity and the energy of the incoming probe fields is shared between the cavity
field and creation of a coherent phonon and resides primarily in one of the
polariton modes. The energy can be extracted by a perturbation of the external
fields or by suddenly changing the of the cavity.Comment: 10 pages, 5 figure
Entangling nanomechanical oscillators in a ring cavity by feeding squeezed light
A scheme is presented for entangling two separated nanomechanical oscillators
by injecting broad band squeezed vacuum light and laser light into the ring
cavity. We work in the resolved sideband regime. We find that in order to
obtain the maximum entanglement of the two oscillators, the squeezing parameter
of the input light should be about 1. We report significant entanglement over a
very wide range of power levels of the pump and temperatures of the
environment.Comment: 13 pages,5 figure
Reactive-Coupling-Induced Normal Mode Splittings in Microdisk Resonators Coupled to Waveguides
We study the optomechanical design introduced by M. Li et al. [Phys. Rev.
Lett. {\bf 103}, 223901 (2009)], which is very effective for investigation of
the effects of reactive coupling. We show the normal mode splitting which is
due solely to reactive coupling rather than due to dispersive coupling. We
suggest feeding the waveguide with a pump field along with a probe field and
scanning the output probe for evidence of reactive-coupling-induced normal mode
splitting.Comment: 4 pages,6 figure
The Electromagnetically Induced Transparency in Mechanical Effects of Light
We consider the dynamical behavior of a nanomechanical mirror in a
high-quality cavity under the action of a coupling laser and a probe laser. We
demonstrate the existence of the analog of electromagnetically induced
transparency (EIT) in the output field at the probe frequency. Our calculations
show explicitly the origin of EIT-like dips as well as the characteristic
changes in dispersion from anomalous to normal in the range where EIT dips
occur. Remarkably the pump-probe response for the opto mechanical system shares
all the features of the Lambda system as discovered by Harris and
collaborators.Comment: 4 pages, 5 figure
Electromagnetically Induced Transparency with Quantized Fields in Optocavity Mechanics
We report electromagnetically induced transparency using quantized fields in
optomechanical systems. The weak probe field is a narrow band squeezed field.
We present a homodyne detection of EIT in the output quantum field. We find
that the EIT dip exists even though the photon number in the squeezed vacuum is
at the single photon level. The EIT with quantized fields can be seen even at
temperatures of the order of 100 mK paving the way for using optomechanical
systems as memory elements.Comment: 6 pages, 5 figure
Electromagnetically Induced Transparency from Two Phonon Processes in Quadratically Coupled Membranes
We describe how electromagnetically induced transparency can arise in
quadratically coupled optomechanical systems. Due to quadratic coupling the
underlying optical process involves a two phonon process in optomechanical
system and this two phonon process makes the mean amplitude, which plays the
role of atomic coherence in traditional EIT, zero. We show how the fluctuation
in displacement can play a role similar to atomic coherence and can lead to
EIT-like effects in quadratically coupled optomechanical systems. We show how
such effects can be studied using the existing optomechanical systems.Comment: 5 pages,4 figure
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