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Increasing quantum limited sensitivity of
interferometers using electromagnetically
induced transparency
Hunter Rew
Advised by Dr. Eugeniy Mikhailov
What to expect
● Introduction
○ Gravitational wave detection
○ Increasing sensitivity
○ Electromagnetically induced transparency
● Simulation methods and results
● Experimental methods and results
● Conclusions
2
Gravitational Waves
Gravitational waves (GWs) are a
prediction of general relativity.
GWs contract space in one
direction while expanding it in
transverse directions
Copyright: [NASA]
3
Interferometric Gravitational Wave Detectors
GW changes lengths of arms
relative to each other, creating
a phase shift in the light
GW interferometers such as
Advanced LIGO are
approaching the standard
quantum limit
4
Uncertainty and Squeezing
5
Noise in LIGO
Noise sources within LIGO
are frequency dependent
6[Nature Photonics 7, 613–619 (2013) doi:10.1038/nphoton.2013.177]
Electromagnetically Induced Transparency
Opaque media become transparent when optical fields are applied at the
transitions of hyperfine ground states. A dark state is produced from the
superposition of these states.
● Produce narrow linewidths
● Near 100% transmission
● Tunable
7
The Lambda Model
[4]
8
Simulation Methods
● eXtensible Multi-Dimensional Simulator (XMDS)
● SciClone
9
[XMDS]
Simulated EIT (Results)
10
Methods (cont.)
Simulations varied the following parameters:
● Drive Rabi frequency (Ωd
) from 17 to 25 KHz
● 2 photon detuning ( ) with a range based on the given drive
● Time from 0 to 0.1 s
● Media length from 0 to 2 cm
11
Methods (cont.)
Constants:
● Probe Rabi frequency (Ωp
) of 0.1 Hz
● Excited state decay (γ) of 6 MHz
● Ground state decay (γbc
) of 1 Hz
● Particle density of 1015
particles per m3
● Transitions at 794.7 nm
12
Simulated EIT (Definitions)
13
Data is fit to a generalized
Lorentzian
A is the contrast
γ is the linewidth / 2
14
15
16
Region of interest
17
Experimental setup
18
Experimental parameters
● Rubidium cell is roughly 1.5 cm in diameter and 1 cm in length
○ Anti-relaxation coating
● Drive and probe intensities are roughly equal
○ Rabi frequencies from 5 to 30 MHz
● Cell temperatures from 35 to 75 Celsius
○ Particle concentrations from 3 x 1010
to 9 x 1011
● Beam waists from full to 0.8ω0
19
Analysis of experimental data
Data is fit to a generalized
Lorentzian
A is the contrast
γ is the linewidth / 2
20
Experiment vs simulation: contrast vs drive
21
Experiment vs simulation: width vs drive
22
Experiment vs simulation: transmission vs concentration
23
Experiment vs simulation: width vs concentration
24
Experiment vs simulation: contrast vs concentration
25
Varying concentration
26
Reminder of experimental setup
27
Varying beam size
28
Conclusions and future work
● Best contrast: 3.9%
● Best linewidth: 202 Hz
● Experiment and simulation
agree (mostly)
● Low temperatures show
promise
● Low drive intensities show
promise
29
Acknowledgements
● Dr. Eugeniy Mikhailov
● Dr. Irina Novikova
● SciClone
30

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