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Electric field sensing near the surface microstructure of an atom chip using cold Rydberg atoms

This thesis reports experimental observations of electric fields using Rydberg atoms, including dc field measurements near the surface of an atom chip, and demonstration of
measurement techniques for ac fields far from the surface. Associated theoretical results
are also presented, including Monte Carlo simulations of the decoherence of Rydberg states
in electric field noise as well as an analytical calculation of the statistics of dc electric field
inhomogeneity near polycrystalline metal surfaces.

DC electric fields were measured near the heterogeneous metal and dielectric surface of
an atom chip using optical spectroscopy on cold atoms released from the trapping potential.
The fields were attributed to charges accumulating in the dielectric gaps between the wires
on the chip surface. The field magnitude and direction depend on the details of the dc
biasing of the chip wires, suggesting that fields may be minimized with appropriate biasing.

Techniques to measure ac electric fields were demonstrated far from the chip surface,
using the decay of a coherent superposition of two Rydberg states of cold atoms. We have
used the decay of coherent Rabi oscillations to place some bounds on the magnitude and
frequency dependence of ac field noise.

The rate of decoherence of a superposition of two Rydberg states was calculated with
Monte Carlo simulations. The states were assumed to have quadratic Stark shifts and the
power spectrum of the electric field noise was assumed to have a power-law dependence
of the form 1/f^κ. The decay is exponential at long times for both free evolution of the
superposition and and Hahn spin-echo sequences with a π refocusing pulse applied to
eliminate the effects of low-frequency field noise. This decay time may be used to calculate
the magnitude of the field noise if κ is known.

The dc field inhomogeneity near polycrystalline metal surfaces due to patch potentials
on the surface has been calculated, and the rms field scales with distance to the surface as
1/z^2. For typical evaporated metal surfaces the magnitude of the rms field is comparable
to the image field of an elementary charge near the surface.

Identiferoai:union.ndltd.org:WATERLOO/oai:uwspace.uwaterloo.ca:10012/7593
Date January 2013
CreatorsCarter, Jeffrey David
Source SetsUniversity of Waterloo Electronic Theses Repository
LanguageEnglish
Detected LanguageEnglish
TypeThesis or Dissertation

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