Atom-light couplers with one, two and ten billion atoms
Abstract
Devices that harness the surprising properties of quantum systems
at scale hold the possibility of revolutionary advances in
information technology. Algorithms for quantum computers can take
advantage of quantum parallelism to solve problems that are
intractable with classical hardware, including prime
factorization and simulating chemical processes. A quantum
communication network that carries qubits instead of bits can
leverage the irreversibility of projective measurement to
guarantee secure communication. Because quantum states are
fragile, building such devices requires exquisite control over
many isolated quantum systems. One of the most critical
capabilities is the interaction of stationary and flying qubits.
In this thesis we consider how to engineer atom-light
interactions as an interface for networked quantum systems.
Quantum atom-light couplers require the efficient and reversible
interaction of atomic and optical qubits, but the natural
interaction of atoms and photons is weak. It is this very lack of
interaction between light and its environment that makes light
such an excellent carrier of quantum information. There are three
promising strategies for stronger coherent atom-light
interactions. First, the light field may be confined to a cavity
so that it interacts with the atom over a longer time. Second,
the light field may be focussed to a small spot with high
aperture optics and matched to the natural atomic radiation
pattern. Third, we may pass the light field through an ensemble
of many atoms and store the qubit in a distributed state. In
practice, atom-light couplers employ some combination of all
three strategies. We will focus our research on the second two
approaches: first by coupling one and two trapped ions with high
aperture optics, and then operating a quantum optical memory with
an ensemble of approximately 10 billion neutral
atoms.
Atoms that have been ionized and trapped in a common
electromagnetic potential are an advanced few-qubit computation
platform. Qubit states are associated with an electronic
excitation at each atom, controlled coherently with lasers, and
made to interact in two (or many) qubit gates by mutual Coulomb
repulsion. One path to quantum advantage with ion-trap quantum
processors is to scale small qubit registers by distributing
entanglement with photonic interconnects. We consider the
feasible efficiency of free-space atom-light couplers for atomic
dipole transitions, and derive the atomic image by common
free-space couplers.
We couple a trapped-ion register with high-aperture lenses and
operate a single trapped ion as a photon source. We model the
dynamic character of the source and show spin-orbit coupling in
the single-photon spatial mode. Although the total collection
efficiency is only approximately 0.01, the source has exceptional
photon-number purity A = (1.9 +/- 0:2) * 10^-3 such that the
higher-order quantum nature of the field persists even after most
of the field has been discarded. We derive an efficient quantum
non-Gaussian witness and surpass it, the first such demonstration
for a trapped-atom single-photon source. We entangle two trapped
atoms by single-photon detection, and observe an interference
pattern in the spatial mode of the bipartite state. Constructive
interference between the entangled components enhances the
emission probability by up to 29%, an example of collective
enhancement by a two-atom ensemble.
The efficiency of free-space atom-light couplers is limited by
our capability to engineer high-precision, high-aperture optics.
We fabricate ultra-precise hemispheric mirrors with numerical
aperture 0.996 by single point diamond turning. The mirrors are
amongst the smoothest hemispheric surfaces ever manufactured with
root-mean-square (RMS) errors consistently below 25 nm. The
smoothest of our mirrors has a RMS error of 14 nm and
peak-to-valley error of 88 nm. A mirror with this surface is
capable of suppressing or enhancing the spontaneous emission of
an atom into free space by 96% in a proposed quantum
electrodynamics experiment. We show how these mirrors, with a
simple modification, can shape the spatial mode of a trapped atom
by similar vacuum-mode engineering. We derive a near-hemispheric
mirror coupling scheme that should be 72% efficient with mirrors
as precise as ours. We design an ion trap for use with such
high-aperture optics.
With careful conditioning and control, ensembles of many atoms
can be made to store and release photonic qubits on demand. Such
optical quantum memories leverage the collective interaction of a
light field with many billions of atoms to achieve storage and
recall efficiencies approaching unity. We show how stationary
light fields for photonic phase gates can be generated in
optically deep ensembles, an effect which has since been
observed.
We implement the gradient echo memory (GEM) scheme in an
ultra-high optical depth cold-atom ensemble. The performance of a
practical quantum memory is contingent on the chosen qubit
encoding. We extend the GEM protocol to allow the simultaneous
storage of frequency separated signals and demonstrate that this
`dual-rail' memory is suitable for high-fidelity frequency
qubits. Dual-rail signals are recalled with 35% efficiency, 82%
interference fringe visibility and 6 degrees of phase stability.
We describe how the fidelity of the scheme is limited by
frequency-dependent polarization rotation and how this may be
addressed in an improved configuration. Finally, we demonstrate
single-rail storage by GEM with 87% efficiency and 1 ms memory
lifetime. Our memory surpasses the no-cloning limit for up to 600
us of storage, out-performing an optical fibre delay line by a
factor of six. This is the first quantum memory to beat this
important benchmark.
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