<?xml version="1.0" encoding="utf-8"?>
<feed xmlns="http://www.w3.org/2005/Atom"><title>USTC IonQNet Group</title><link href="http://lqcc.ustc.edu.cn/iontrap/" rel="alternate"/><link href="http://lqcc.ustc.edu.cn/iontrap/feeds/all-en.atom.xml" rel="self"/><id>http://lqcc.ustc.edu.cn/iontrap/</id><updated>2026-10-03T00:00:00+08:00</updated><entry><title>High optical access (HOA) trap</title><link href="http://lqcc.ustc.edu.cn/iontrap/gallery/high-optical-access-trap.html" rel="alternate"/><published>2026-10-03T00:00:00+08:00</published><updated>2026-10-03T00:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2026-10-03:/iontrap/gallery/high-optical-access-trap.html</id><summary type="html">A miniature blade trap in an all-glass cell, with high-NA optical access from four directions for precise addressing, imaging, readout and optical-tweezer control.</summary><content type="html">&lt;html&gt;&lt;body&gt;&lt;h2 id="four-directions-of-high-na-optical-access"&gt;Four directions of
high-NA optical access&lt;/h2&gt;
&lt;p&gt;Our &lt;a href="https://doi.org/10.1063/5.0043985"&gt;high-optical-access
apparatus (Review of Scientific Instruments, 2021)&lt;/a&gt; places a
miniaturized blade-electrode ion trap in an all-glass cell, opening
optical paths for tightly focused control beams and fluorescence
collection. The geometry supports high-numerical-aperture objectives
from four directions. These objectives provide multi-directional
addressing, ion imaging and quantum-state readout, allowing the optical
system to be configured around the needs of each experiment.&lt;/p&gt;
&lt;h2 id="from-precise-addressing-to-new-quantum-gates"&gt;From precise
addressing to new quantum gates&lt;/h2&gt;
&lt;p&gt;The HOA platform supports our research on ion control with tightly
focused light and optical tweezers. We used its optical access to
develop &lt;a href="https://doi.org/10.1103/PhysRevApplied.22.054003"&gt;low-crosstalk
dual-sided Raman addressing&lt;/a&gt;, then used the optical Magnus effect to
implement &lt;a href="https://doi.org/10.1103/w5l6-wmrl"&gt;addressed
entangling gates with single-sided polarization-gradient control&lt;/a&gt;.
Together with &lt;a href="https://doi.org/10.3788/COL202624.010201"&gt;in-situ
aberration correction using an ion probe&lt;/a&gt;, high-quality focused
fields allow us to select individual qubits and couple to axial motion
along an ion chain.&lt;/p&gt;
&lt;h2 id="optical-control-of-the-crystals-motional-spectrum"&gt;Optical
control of the crystal’s motional spectrum&lt;/h2&gt;
&lt;p&gt;The open optical geometry also allows local optical-tweezer
potentials to be combined with electrical confinement. We have
demonstrated optical control of an ion’s vibrational frequency and are
investigating how local light fields can dynamically reshape the
frequencies and spatial structure of phonon modes in a crystal. This
approach aims to reduce crosstalk from unwanted motional modes and
provide additional control for high-fidelity gates directly within ion
crystals.&lt;/p&gt;
&lt;p&gt;&lt;a href="/pages/researches/trapped-ion-qip.html"&gt;Explore our
trapped-ion quantum computing research →&lt;/a&gt;&lt;/p&gt;
&lt;/body&gt;&lt;/html&gt;</content><category term="gallery"/></entry><entry><title>Optical-tweezer ion gates</title><link href="http://lqcc.ustc.edu.cn/iontrap/gallery/optical-tweezer-ion-gates.html" rel="alternate"/><published>2026-10-03T00:00:00+08:00</published><updated>2026-10-03T00:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2026-10-03:/iontrap/gallery/optical-tweezer-ion-gates.html</id><summary type="html">Tightly focused light opens new ways to address trapped ions, generate entangling gates and control their collective motion.</summary><content type="html">&lt;html&gt;&lt;body&gt;&lt;h2 id="addressed-gates-with-the-optical-magnus-effect"&gt;Addressed gates
with the optical Magnus effect&lt;/h2&gt;
&lt;p&gt;Tightly focused light provides more than a small addressing spot: its
spatially varying polarization offers a new way to couple an ion’s spin
to its motion. Using the optical Magnus effect, we implemented addressed
entangling gates driven by co-propagating Raman light through a single
objective. This geometry simplifies the optical interface while
retaining flexible selection of the ions involved in the gate.&lt;/p&gt;
&lt;p&gt;The work was reported in &lt;a href="https://doi.org/10.1103/w5l6-wmrl"&gt;Physical Review Letters 135,
260604 (2025)&lt;/a&gt;. After correcting for state-preparation and
measurement errors, the measured Bell-state fidelities were
&lt;strong&gt;98.7(1)% in a two-ion chain and 97.2(4)% in a four-ion
chain&lt;/strong&gt;.&lt;/p&gt;
&lt;h2 id="from-precise-addressing-to-phonon-control"&gt;From precise
addressing to phonon control&lt;/h2&gt;
&lt;p&gt;We combine single-sided polarization-gradient control with in-situ
aberration correction and coupling to axial motional modes. Optical
tweezers also provide local potentials for tuning ion motion; building
on demonstrated control of an ion’s vibrational frequency, we are
developing ways to reshape phonon modes within ion crystals and reduce
unwanted motional crosstalk.&lt;/p&gt;
&lt;p&gt;&lt;a href="/pages/researches/trapped-ion-qip.html"&gt;Explore the
trapped-ion quantum computing research →&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;a href="/gallery/high-optical-access-trap.html"&gt;See the high optical
access (HOA) trap →&lt;/a&gt;&lt;/p&gt;
&lt;/body&gt;&lt;/html&gt;</content><category term="gallery"/></entry><entry><title>Yun-Feng Huang</title><link href="http://lqcc.ustc.edu.cn/iontrap/Members/Yun-Feng_Huang.html" rel="alternate"/><published>2026-04-01T10:00:00+08:00</published><updated>2026-04-01T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2026-04-01:/iontrap/Members/Yun-Feng_Huang.html</id><summary type="html">&lt;h2 id="profile"&gt;Profile&lt;/h2&gt;
&lt;p&gt;Yun-Feng Huang is a Researcher in the Department of Optics and
Optical Engineering at the University of Science and Technology of
China. His research interests include quantum communication, photonic
quantum information processing, and trapped-ion quantum information
processing.&lt;/p&gt;
&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;1998-2003, Ph.D. program, Department of Physics, University of
Science and …&lt;/li&gt;&lt;/ul&gt;</summary><content type="html">&lt;h2 id="profile"&gt;Profile&lt;/h2&gt;
&lt;p&gt;Yun-Feng Huang is a Researcher in the Department of Optics and
Optical Engineering at the University of Science and Technology of
China. His research interests include quantum communication, photonic
quantum information processing, and trapped-ion quantum information
processing.&lt;/p&gt;
&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;1998-2003, Ph.D. program, Department of Physics, University of
Science and Technology of China&lt;/li&gt;
&lt;li&gt;1994-1998, B.S., Department of Physics, University of Science and
Technology of China&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="experience"&gt;Experience&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;2009-present, Researcher, Department of Optics and Optical
Engineering, University of Science and Technology of China&lt;/li&gt;
&lt;li&gt;2006-2008, Associate Professor, Department of Physics, University of
Science and Technology of China&lt;/li&gt;
&lt;li&gt;2003-2005, Lecturer, Department of Physics, University of Science
and Technology of China&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="research"&gt;Research&lt;/h2&gt;
&lt;p&gt;Current work focuses on building quantum networks based on
trapped-ion systems, including enhanced trapped-ion nodes, photonic
quantum channels and hybrid quantum networks. His group has carried out
experimental studies with Yb and Ba ions confined in linear ion
traps.&lt;/p&gt;
</content><category term="People"/></entry><entry><title>Chen-Xu Wang</title><link href="http://lqcc.ustc.edu.cn/iontrap/Members/Chen-Xu_Wang.html" rel="alternate"/><published>2026-03-31T20:20:00+08:00</published><updated>2026-03-31T20:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2026-03-31:/iontrap/Members/Chen-Xu_Wang.html</id><content type="html">&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;2021.9-now, University of Science and Technology of China,
Department of Optics and Optical Engineering, Doctor&lt;/li&gt;
&lt;li&gt;2017.8-2021.6, Ocean University of China, Faculty of Information
Science and Engineering, Bachelor&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="research"&gt;Research&lt;/h2&gt;
&lt;p&gt;Quantum information with trapped ions. Quantum simulation, quantum
network, distributed quantum computation.&lt;/p&gt;
</content><category term="People"/></entry><entry><title>Quantum Interface Concept</title><link href="http://lqcc.ustc.edu.cn/iontrap/gallery/quantum-interface-concept.html" rel="alternate"/><published>2026-03-28T10:23:00+08:00</published><updated>2026-03-28T10:23:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2026-03-28:/iontrap/gallery/quantum-interface-concept.html</id><summary type="html">Connecting stationary matter qubits through optical quantum channels.</summary><content type="html">&lt;html&gt;&lt;body&gt;&lt;p&gt;Quantum interfaces connect stationary matter qubits to photons that
carry quantum information between remote nodes. In our research, trapped
ions provide coherent local processing, while cavity interfaces and
frequency conversion connect those processors to optical channels and
other quantum systems.&lt;/p&gt;
&lt;p&gt;&lt;a href="/pages/research.html"&gt;Explore our quantum-network research
→&lt;/a&gt;&lt;/p&gt;
&lt;/body&gt;&lt;/html&gt;</content><category term="gallery"/></entry><entry><title>Hybrid Quantum Network</title><link href="http://lqcc.ustc.edu.cn/iontrap/gallery/hybrid-quantum-network.html" rel="alternate"/><published>2026-03-28T10:21:00+08:00</published><updated>2026-03-28T10:21:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2026-03-28:/iontrap/gallery/hybrid-quantum-network.html</id><summary type="html">Connecting trapped-ion processors and solid-state quantum memories through quantum frequency conversion.</summary><content type="html">&lt;html&gt;&lt;body&gt;&lt;p&gt;Trapped ions provide long-lived coherence and high-fidelity quantum
operations, while solid-state memories store photonic quantum states. We
develop interfaces that combine these capabilities in a hybrid network,
connecting local ion control with remote optical storage.&lt;/p&gt;
&lt;p&gt;Our polarization-preserving frequency converter bridges the 369.5 nm
emission of a ytterbium ion and the 580 nm transition of a
europium-doped crystal memory. A Sagnac loop stabilizes the polarization
components, and off-axis parabolic mirrors provide achromatic coupling
across the wavelength bands (&lt;a href="https://doi.org/10.3788/COL202624.021901"&gt;Chinese Optics Letters,
2026&lt;/a&gt;). The two figures show the network architecture and the
experimental system linking the ion node, frequency converter and
memory.&lt;/p&gt;
&lt;p&gt;Working with Professor Zong-Quan Zhou’s team, we established
ion–memory entanglement between laboratories separated by 75 m and
connected by 90 m of optical fiber. Joint measurements after storage and
retrieval verify quantum correlations across this heterogeneous link.
The experiment is reported in the preprint &lt;a href="https://arxiv.org/abs/2603.05836"&gt;Heterogeneous entanglement
between a trapped ion and a solid-state quantum memory
(arXiv:2603.05836)&lt;/a&gt;, with further details in &lt;a href="/publications/files/thesis/2026_hybrid-quantum-networks-trapped-ions-solid-state-memories_wang-chenxu.pdf"&gt;Chen-Xu
Wang’s doctoral thesis (2026)&lt;/a&gt;. We plan to extend these interfaces to
neutral-atom systems and explore distributed quantum computing across
physical platforms.&lt;/p&gt;
&lt;p&gt;&lt;a href="/pages/researches/hybrid-quantum-network.html"&gt;Explore our
hybrid quantum network research →&lt;/a&gt;&lt;/p&gt;
&lt;/body&gt;&lt;/html&gt;</content><category term="gallery"/></entry><entry><title>Cavity QED Interface</title><link href="http://lqcc.ustc.edu.cn/iontrap/gallery/cavity-qed-interface.html" rel="alternate"/><published>2026-03-28T10:20:00+08:00</published><updated>2026-03-28T10:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2026-03-28:/iontrap/gallery/cavity-qed-interface.html</id><summary type="html">From gold-coated fiber mirrors to needle-trap integration: building high-bandwidth, high-efficiency ion–photon interfaces.</summary><content type="html">&lt;html&gt;&lt;body&gt;&lt;p&gt;We integrate fiber microcavities with needle ion traps to develop
ion–photon interfaces for quantum networks. The small cavity mode volume
enhances ion–cavity coupling, while the fibers provide channels for
collecting and transmitting photons. By designing the mirrors, trapping
geometry and optical coupling together, we aim to build network nodes
that combine high bandwidth with high efficiency.&lt;/p&gt;
&lt;p&gt;The photographs show the hardware behind this interface. Gold coating
on the fiber sides and the outer regions of the end faces provides
electrical shielding while leaving the central optical apertures open.
Two opposing fiber mirrors form a microcavity, which is integrated with
the needle trap inside the vacuum chamber. The fluorescence image of a
single Ba⁺ ion between the mirrors shows the ion confined within this
cavity geometry.&lt;/p&gt;
&lt;p&gt;&lt;a href="/pages/researches/quantum-network-cavity-qed.html"&gt;Explore
quantum networking with cavity QED →&lt;/a&gt;&lt;/p&gt;
&lt;/body&gt;&lt;/html&gt;</content><category term="gallery"/></entry><entry><title>"Transverse Polarization Gradient Entangling Gates for Trapped-Ion Quantum Computation" is published in Physical Review Letters</title><link href="http://lqcc.ustc.edu.cn/iontrap/transverse-polarization-gradient-entangling-gates-trapped-ion.html" rel="alternate"/><published>2025-12-25T10:00:00+08:00</published><updated>2025-12-25T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2025-12-25:/iontrap/transverse-polarization-gradient-entangling-gates-trapped-ion.html</id><summary type="html">&lt;p&gt;Our work “Transverse Polarization Gradient Entangling Gates for
Trapped-Ion Quantum Computation” has been published in &lt;strong&gt;Physical
Review Letters&lt;/strong&gt; as an &lt;strong&gt;Editors’ Suggestion&lt;/strong&gt; on
December 24, 2025.&lt;/p&gt;
&lt;p&gt;We realized high-fidelity entangling gates for trapped ions based on
the polarization gradient of tightly focused light. This scheme
simplifies the current entangling gate …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work “Transverse Polarization Gradient Entangling Gates for
Trapped-Ion Quantum Computation” has been published in &lt;strong&gt;Physical
Review Letters&lt;/strong&gt; as an &lt;strong&gt;Editors’ Suggestion&lt;/strong&gt; on
December 24, 2025.&lt;/p&gt;
&lt;p&gt;We realized high-fidelity entangling gates for trapped ions based on
the polarization gradient of tightly focused light. This scheme
simplifies the current entangling gate configuration and is compatible
with the optical tweezer architecture, holding great significance for
large-scale trapped-ion quantum computation.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;p&gt;&lt;img src="/images/shared/polarization-gradient-gates.webp" style="max-width: 600px;" title="Optical Magnus effect quantum gate" alt="Artistic rendering of the optical Magnus effect quantum gate"&gt;&lt;/p&gt;
&lt;/div&gt;
&lt;h3 id="background-and-challenge"&gt;Background and Challenge&lt;/h3&gt;
&lt;p&gt;Trapped-ion quantum systems, with their ultra-high operation fidelity
and coherence, are one of the leading physical platforms for building
large-scale quantum computers. Ion-array-based quantum computing
architectures, which construct quantum processors through optically
addressing individual ion qubits in parallel, offer the advantages of
high connectivity and parallel computational efficiency. However,
scaling up this architecture faces a fundamental challenge: dense phonon
modes in large ion arrays cause &lt;strong&gt;gate crosstalk&lt;/strong&gt;, making
it difficult to implement high-fidelity entangling gates directly. In
recent years, the international community has proposed using tightly
focused optical tweezer arrays to reshape the ion phonon spectrum and
suppress crosstalk, but demonstrating optical tweezer gates in optically
addressed ion-trap quantum computers has not yet achieved a
breakthrough.&lt;/p&gt;
&lt;h3 id="the-optical-magnus-effect-approach"&gt;The Optical Magnus Effect
Approach&lt;/h3&gt;
&lt;p&gt;Building on years of innovative research and independent development
in trapped-ion quantum computation, our team has realized a novel
entangling gate scheme based on the &lt;strong&gt;optical Magnus
effect&lt;/strong&gt;: analogous to the Magnus effect in fluid dynamics, a
spinning ion in a focused light stream (optical tweezer) experiences a
transverse force — perpendicular to the light propagation direction.
This scheme exploits the transverse field gradient of a tightly focused
laser to create a state-dependent push that establishes quantum
entanglement between ions. This approach eliminates the traditional
complex counter-propagating laser beam configuration, greatly
simplifying the experimental setup and reducing operational
complexity.&lt;/p&gt;
&lt;h3 id="key-results"&gt;Key Results&lt;/h3&gt;
&lt;p&gt;After correcting for state-preparation and measurement errors, we
measured Bell-state fidelities of &lt;strong&gt;98.7(1)%&lt;/strong&gt; in a two-ion
chain and &lt;strong&gt;97.2(4)%&lt;/strong&gt; in a four-ion chain of
&lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; ions. This quantum gate is capable of
achieving fidelities above &lt;strong&gt;99.99%&lt;/strong&gt; in theory. We
analyzed and discussed the main sources of infidelity in the current
experiment, and expect to reduce the gate error by more than an order of
magnitude in future experiments.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/entangling_gates_2025/fig1.jpg" style="max-width: 600px;" title="Experimental setup" alt="Principle of polarization-gradient-based individual addressing"&gt;
&lt;p class="caption"&gt;
Fig. 1. Principle of polarization-gradient-based individual addressing.
An acousto-optic deflector (AOD) generates multiple laser spots through
a high-NA objective lens, producing polarization gradients that enable
spin-dependent forces on individual ions.
&lt;/p&gt;
&lt;/div&gt;
&lt;h3 id="significance"&gt;Significance&lt;/h3&gt;
&lt;p&gt;The key innovation of this technique lies in its excellent
compatibility with optical tweezer gates — since the tweezer operation
itself involves transverse motion — and the significant simplification
of optical configurations, making the optical tweezer gate scheme highly
feasible in experiment. This provides a simpler and more flexible path
toward large-scale, scalable trapped-ion quantum computation.&lt;/p&gt;
&lt;p&gt;Reviewers gave high praise: &lt;em&gt;“This paper demonstrates a successful
combination of optical tweezers with linear ion chains, proposing an
ingenious and powerful mechanism through which two-qubit gate operations
can be realized between arbitrary ion pairs…”&lt;/em&gt; and &lt;em&gt;“The results
of realizing this type of quantum gate are encouraging, and this method
addresses an important challenge in scaling up ion-trap quantum
computation…”&lt;/em&gt;&lt;/p&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1103/w5l6-wmrl"&gt;https://doi.org/10.1103/w5l6-wmrl&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;See also the report by Photon Box (光子盒): &lt;a
href="https://news.qq.com/rain/a/20251225A06IAR00"&gt;https://news.qq.com/rain/a/20251225A06IAR00&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;(Source: China Science Daily, by Min Wang)&lt;/p&gt;
</content><category term="News"/></entry><entry><title>"A neural network assisted ¹⁷¹Yb⁺ quantum magnetometer" is published in npj Quantum Information</title><link href="http://lqcc.ustc.edu.cn/iontrap/neural-network-assisted-yb-quantum-magnetometer.html" rel="alternate"/><published>2022-12-22T10:00:00+08:00</published><updated>2022-12-22T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2022-12-22:/iontrap/neural-network-assisted-yb-quantum-magnetometer.html</id><summary type="html">&lt;p&gt;Our work “A neural network assisted &lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt;
quantum magnetometer” has been published in &lt;strong&gt;npj Quantum
Information&lt;/strong&gt;. We demonstrate the power of combining machine
learning with quantum sensing by integrating neural networks into the
data processing stage of a trapped-ion magnetometer, significantly
extending its operational regime.&lt;/p&gt;
&lt;h3 id="the-challenge"&gt;The Challenge&lt;/h3&gt;
&lt;p&gt;A versatile …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work “A neural network assisted &lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt;
quantum magnetometer” has been published in &lt;strong&gt;npj Quantum
Information&lt;/strong&gt;. We demonstrate the power of combining machine
learning with quantum sensing by integrating neural networks into the
data processing stage of a trapped-ion magnetometer, significantly
extending its operational regime.&lt;/p&gt;
&lt;h3 id="the-challenge"&gt;The Challenge&lt;/h3&gt;
&lt;p&gt;A versatile quantum magnetometer must deliver a readable response
across a wide range of target field parameters. Standard atomic
magnetometers operate in a regime leading to harmonic sensor responses,
where RF target parameters are encoded in simple sinusoidal patterns.
However, when the RF driving induces responses beyond this standard
harmonic behavior — for instance, with large shot noise or in continuous
single-shot measurement scenarios — the simple relationship between
sensor responses and target parameters breaks down, making accurate
field characterization extremely challenging.&lt;/p&gt;
&lt;h3 id="our-approach"&gt;Our Approach&lt;/h3&gt;
&lt;p&gt;We experimentally demonstrated that combining
&lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; atomic sensors with adequately trained
neural networks enables us to investigate target fields in distinct
challenging scenarios. Specifically, we characterized radio frequency
(RF) fields in the presence of large shot noise, including the limit
case of continuous data acquisition via single-shot measurements. The
neural network learns the complex mapping between measured sensor
responses and the underlying field parameters, effectively deciphering
the information contained in non-trivial sensor responses.&lt;/p&gt;
&lt;h3 id="key-results"&gt;Key Results&lt;/h3&gt;
&lt;p&gt;In the scenario of reduced measurement averaging, our neural network
achieved an average estimation accuracy of &lt;strong&gt;98.76%&lt;/strong&gt; with
only 100 measurement shots per data point. Even with as few as 30 shots,
the accuracy remained at &lt;strong&gt;98.31%&lt;/strong&gt;. For continuous
single-shot measurements, the regression between NN outputs and targets
showed correlation coefficients exceeding &lt;strong&gt;R = 0.999&lt;/strong&gt;.
These results demonstrate that the hybridization of machine learning
tools with quantum sensing techniques is a strategy that can be readily
extended to other quantum platforms, such as nitrogen-vacancy centers in
diamond.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/neural_network_magnetometer_2022/fig1.jpg" style="max-width: 600px;" title="Schematic" alt="Schematic of the neural network assisted quantum magnetometer"&gt;
&lt;p class="caption"&gt;
Fig. 1. Energy levels of the &lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; atomic sensor
(a, b), the needle trap configuration (c), and the neural network
architecture (d). The sensor response from the photomultiplier tube
(PMT) is processed through a well-trained neural network to extract RF
field parameters from complex sensor responses.
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;This work was a collaboration with researchers from the University of
the Basque Country (UPV/EHU) in Spain.&lt;/p&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1038/s41534-022-00669-2"&gt;https://doi.org/10.1038/s41534-022-00669-2&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>"Super-resolved Imaging of a Single Cold Atom on a Nanosecond Timescale" is published in Physical Review Letters</title><link href="http://lqcc.ustc.edu.cn/iontrap/super-resolved-imaging-single-cold-atom-nanosecond.html" rel="alternate"/><published>2021-12-24T10:00:00+08:00</published><updated>2021-12-24T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2021-12-24:/iontrap/super-resolved-imaging-single-cold-atom-nanosecond.html</id><summary type="html">&lt;p&gt;Our work “Super-resolved Imaging of a Single Cold Atom on a
Nanosecond Timescale” has been published in &lt;strong&gt;Physical Review
Letters&lt;/strong&gt;. We demonstrate a groundbreaking method to image a
single trapped ion with unprecedented spatial and temporal resolution,
breaking through the optical diffraction limit.&lt;/p&gt;
&lt;h3 id="breaking-the-diffraction-limit"&gt;Breaking the Diffraction
Limit&lt;/h3&gt;
&lt;p&gt;High-resolution optical detection …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work “Super-resolved Imaging of a Single Cold Atom on a
Nanosecond Timescale” has been published in &lt;strong&gt;Physical Review
Letters&lt;/strong&gt;. We demonstrate a groundbreaking method to image a
single trapped ion with unprecedented spatial and temporal resolution,
breaking through the optical diffraction limit.&lt;/p&gt;
&lt;h3 id="breaking-the-diffraction-limit"&gt;Breaking the Diffraction
Limit&lt;/h3&gt;
&lt;p&gt;High-resolution optical detection and imaging of individual particles
in cold atomic systems is essential for directly probing quantum
phenomena such as transport, correlations, and phase transitions.
However, traditional microscopy techniques are fundamentally restricted
by the wavelength-scale diffraction limit, making them unsuitable for
studying wave function details of many-body systems. We brought the
concept of super-resolved microscopy — which has matured as a powerful
tool in biology and chemistry — into the realm of cold atoms.&lt;/p&gt;
&lt;h3 id="our-method-ground-state-depletion-microscopy"&gt;Our Method:
Ground-State Depletion Microscopy&lt;/h3&gt;
&lt;p&gt;We demonstrated &lt;strong&gt;ground-state depletion (GSD)
microscopy&lt;/strong&gt; on a trapped-ion system for the first time. By
combining the GSD control sequence with the qubit-state polarization and
detection methods of &lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; ions, we achieved 2D
super-resolved imaging beyond the optical diffraction limit. The key
innovation is using a high-purity doughnut-shaped laser beam, generated
via a &lt;strong&gt;digital micromirror device (DMD)&lt;/strong&gt; with in-situ
aberration correction, to selectively deplete the ion’s quantum
state.&lt;/p&gt;
&lt;h3 id="results"&gt;Results&lt;/h3&gt;
&lt;p&gt;We achieved a spatial resolution of &lt;strong&gt;175 nm&lt;/strong&gt; using a
NA = 0.1 imaging objective — a &lt;strong&gt;13-fold improvement&lt;/strong&gt;
compared with direct fluorescence imaging. Moreover, the depletion
process can be as short as ~50 ns under strong laser power, enabling us
to take stroboscopic images on nanosecond timescales. We demonstrated
this capability by observing one complete cycle of the ion’s secular
motion within &lt;strong&gt;735 ns&lt;/strong&gt;, achieving a displacement
detection sensitivity of &lt;strong&gt;10 nm&lt;/strong&gt;.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/super_resolved_imaging_2021/fig1.jpg" style="max-width: 600px;" title="Experimental scheme" alt="Super-resolved imaging experimental scheme and setup"&gt;
&lt;p class="caption"&gt;
Fig. 1. Experimental scheme and setup. (a) Energy levels of
&lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; and the three-laser GSD imaging sequence.
(b) A Paul trap with the doughnut beam focused through the top window.
(c) Schematic of the super-resolved imaging process: scanning the
doughnut spot pixel by pixel to build a super-resolved image.
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;Our method provides a powerful tool for probing particle positions,
momenta, correlations, and dynamics in cold atomic systems, and can be
readily extended to neutral atoms in optical tweezers.&lt;/p&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1103/PhysRevLett.127.263603"&gt;https://doi.org/10.1103/PhysRevLett.127.263603&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>"Riemann zeros from Floquet engineering a trapped-ion qubit" is published in npj Quantum Information</title><link href="http://lqcc.ustc.edu.cn/iontrap/riemann-zeros-floquet-engineering-trapped-ion.html" rel="alternate"/><published>2021-07-01T10:00:00+08:00</published><updated>2021-07-01T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2021-07-01:/iontrap/riemann-zeros-floquet-engineering-trapped-ion.html</id><summary type="html">&lt;p&gt;Our work “Riemann zeros from Floquet engineering a trapped-ion qubit”
was published in &lt;strong&gt;npj Quantum Information&lt;/strong&gt; on July 14,
2021. This work bridges quantum physics and number theory by
experimentally measuring the zeros of the Riemann zeta function using a
trapped-ion quantum system.&lt;/p&gt;
&lt;h3 id="background"&gt;Background&lt;/h3&gt;
&lt;p&gt;The Riemann Hypothesis, proposed by Bernhard …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work “Riemann zeros from Floquet engineering a trapped-ion qubit”
was published in &lt;strong&gt;npj Quantum Information&lt;/strong&gt; on July 14,
2021. This work bridges quantum physics and number theory by
experimentally measuring the zeros of the Riemann zeta function using a
trapped-ion quantum system.&lt;/p&gt;
&lt;h3 id="background"&gt;Background&lt;/h3&gt;
&lt;p&gt;The Riemann Hypothesis, proposed by Bernhard Riemann in 1859,
conjectures that all non-trivial zeros of the Riemann zeta function have
their real parts equal to 1/2. As one of the seven Millennium Prize
Problems, its proof would profoundly advance our understanding of prime
number distribution. An intriguing approach to this problem is the
Hilbert-Pólya conjecture, which proposes the existence of a quantum
system whose Hamiltonian eigenvalues correspond one-to-one with the
Riemann zeros.&lt;/p&gt;
&lt;h3 id="our-approach"&gt;Our Approach&lt;/h3&gt;
&lt;p&gt;We proposed, for the first time internationally, a quasi-static
Hamiltonian method. By designing a periodic driving function to modulate
a trapped-ion qubit, we realized quasi-static evolution of the quantum
state. When the driving parameter corresponds to a Riemann zero, the
engineered quasienergies become degenerate and the quantum state remains
frozen at integer multiples of the driving period — a phenomenon known
as &lt;strong&gt;coherent destruction of tunneling&lt;/strong&gt;. This is described
by Floquet theory, where the quasienergies of the periodically driven
system are regulated by the driving parameters. By scanning over the
driving amplitude, the locations of the Riemann zeros can be measured to
a high degree of accuracy.&lt;/p&gt;
&lt;h3 id="results"&gt;Results&lt;/h3&gt;
&lt;p&gt;Using our self-developed trapped-ion system with long coherence
times, we implemented 30-period high-fidelity driving and successfully
measured the &lt;strong&gt;first 80 non-trivial Riemann zeros&lt;/strong&gt; —
improving upon previous work in this field by nearly &lt;strong&gt;two orders
of magnitude&lt;/strong&gt;. Our experimental results provide important
evidence for studying the Hilbert-Pólya conjecture and deepening the
connection between the Riemann Hypothesis and quantum systems.&lt;/p&gt;
&lt;p&gt;Reviewers commented: &lt;em&gt;“I am recommending publication, for several
reasons: the high level of experimental ingenuity required to make the
scheme work; the clear description of theory and experiment; and the
large numbers and high accuracy of the measured zeros.”&lt;/em&gt;&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/riemann_zeros_2021/fig1.jpg" style="max-width: 600px;" title="Experimental procedure" alt="Floquet dynamics in a trapped-ion system"&gt;
&lt;p class="caption"&gt;
Fig. 1. Experimental procedure to measure Floquet dynamics in a
trapped-ion system. (a) The qubit is periodically driven by a microwave
field generated by an AWG. (b) On the Bloch sphere, the qubit is
initialized to |0⟩ and evolves to U(nT)|0⟩ after n periods of driving,
with the freezing of dynamics revealing the Riemann zeros.
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;The first author of this paper is Dr. Ran He from our laboratory.
This work was supported by the Ministry of Science and Technology, NSFC,
CAS, and Anhui Province.&lt;/p&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1038/s41534-021-00446-7"&gt;https://doi.org/10.1038/s41534-021-00446-7&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>"Quantum thermodynamics in adiabatic open systems and its trapped-ion experimental realization" is published in npj Quantum Information</title><link href="http://lqcc.ustc.edu.cn/iontrap/quantum-thermodynamics-adiabatic-open-systems-trapped-ion.html" rel="alternate"/><published>2020-09-18T10:00:00+08:00</published><updated>2020-09-18T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2020-09-18:/iontrap/quantum-thermodynamics-adiabatic-open-systems-trapped-ion.html</id><summary type="html">&lt;p&gt;Our work “Quantum thermodynamics in adiabatic open systems and its
trapped-ion experimental realization” has been published in &lt;strong&gt;npj
Quantum Information&lt;/strong&gt;. In collaboration with our Brazilian
colleagues, we established general formulas for quantum thermodynamics
in adiabatic open systems, bridging quantum adiabatic processes and
thermodynamic adiabatic processes, and verified our theory
experimentally …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work “Quantum thermodynamics in adiabatic open systems and its
trapped-ion experimental realization” has been published in &lt;strong&gt;npj
Quantum Information&lt;/strong&gt;. In collaboration with our Brazilian
colleagues, we established general formulas for quantum thermodynamics
in adiabatic open systems, bridging quantum adiabatic processes and
thermodynamic adiabatic processes, and verified our theory
experimentally using trapped ions.&lt;/p&gt;
&lt;h3 id="motivation"&gt;Motivation&lt;/h3&gt;
&lt;p&gt;Thermodynamics, built upon macroscopic observations of matter, has
achieved tremendous success across many systems. With the development of
quantum technology enabling precise preparation and control of quantum
systems, a fundamental question emerges: &lt;strong&gt;do the laws of
thermodynamics still apply at the quantum scale?&lt;/strong&gt; Quantum
thermodynamics has thus gradually developed, aiming to study the
emergence and limits of thermodynamic laws from the microscopic
perspective of quantum mechanics, addressing long-standing puzzles such
as Maxwell’s demon.&lt;/p&gt;
&lt;h3 id="key-contributions"&gt;Key Contributions&lt;/h3&gt;
&lt;p&gt;Quantum adiabatic processes and thermodynamic adiabatic processes are
fundamental components of quantum theory and thermodynamics,
respectively. Exploring the relationship between them is a fascinating
and complex problem. We derived general formulas for heat, work,
internal energy, and entropy in open quantum systems, and established
that quantum mechanical adiabaticity and thermodynamic adiabaticity are
&lt;strong&gt;generally not equivalent&lt;/strong&gt; — thermal adiabaticity
requires a sufficient condition satisfied by quantum systems
adiabatically evolving under a steady-state trajectory.&lt;/p&gt;
&lt;h3 id="experimental-verification"&gt;Experimental Verification&lt;/h3&gt;
&lt;p&gt;We implemented the experiment using our trapped-ion system. The
trapped ion offers long coherence times, multiple controllable degrees
of freedom (spin and motion), and serves as an ideal platform for
quantum information processing. We developed an innovative solution to
simulate time-dependent decoherence channels by using noise-modulated
carrier frequency, achieving a fidelity of over &lt;strong&gt;99.5%&lt;/strong&gt;
in simulating the quantum decoherence channel. This enabled us to
analyze heat and internal energy in a fully controllable dynamical
process with high-fidelity quantum state manipulation.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/quantum_thermodynamics_2020/fig1.jpg" style="max-width: 600px;" title="Experimental scheme" alt="Experimental scheme for investigating thermodynamics of adiabaticity"&gt;
&lt;p class="caption"&gt;
Fig. 1. Experimental scheme to investigate the thermodynamics of
adiabaticity in open quantum systems. (a) Schematic of the six-needle
Paul trap and relevant energy levels. (b) Experimental microwave
instrument for generating the driving field and controlling the Gaussian
noise as a dephasing channel.
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;Reviewers gave high praise: &lt;em&gt;“The present work would be one of the
very few, and probably the most convincing, theoretical and experimental
discussion on the relation between thermodynamical adiabatic processes
and quantum adiabatic processes in open quantum systems.”&lt;/em&gt;&lt;/p&gt;
&lt;p&gt;The first author is Dr. Chang-Kang Hu, a former PhD student from our
laboratory. This work was supported by MOST, NSFC, CAS, Anhui Province,
and the Postdoctoral Science Fund.&lt;/p&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1038/s41534-020-00300-2"&gt;https://doi.org/10.1038/s41534-020-00300-2&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>"Experimentally testing quantum critical dynamics beyond the Kibble-Zurek mechanism" is published in Communications Physics</title><link href="http://lqcc.ustc.edu.cn/iontrap/experimentally-testing-quantum-critical-dynamics-beyond-kibble-zurek.html" rel="alternate"/><published>2020-02-14T10:00:00+08:00</published><updated>2020-02-14T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2020-02-14:/iontrap/experimentally-testing-quantum-critical-dynamics-beyond-kibble-zurek.html</id><summary type="html">&lt;p&gt;Our work “Experimentally testing quantum critical dynamics beyond the
Kibble-Zurek mechanism” has been published in &lt;strong&gt;Communications
Physics&lt;/strong&gt; (Nature). Building on our earlier Kibble-Zurek
experiment, we go beyond the standard KZM to probe the &lt;strong&gt;full
probability distribution&lt;/strong&gt; of topological defects formed during a
quantum phase transition.&lt;/p&gt;
&lt;h3 id="beyond-the-mean-full-counting-statistics"&gt;Beyond the Mean: Full
Counting …&lt;/h3&gt;</summary><content type="html">&lt;p&gt;Our work “Experimentally testing quantum critical dynamics beyond the
Kibble-Zurek mechanism” has been published in &lt;strong&gt;Communications
Physics&lt;/strong&gt; (Nature). Building on our earlier Kibble-Zurek
experiment, we go beyond the standard KZM to probe the &lt;strong&gt;full
probability distribution&lt;/strong&gt; of topological defects formed during a
quantum phase transition.&lt;/p&gt;
&lt;h3 id="beyond-the-mean-full-counting-statistics"&gt;Beyond the Mean: Full
Counting Statistics&lt;/h3&gt;
&lt;p&gt;The Kibble-Zurek mechanism (KZM) describes the universal dynamics
across a phase transition, predicting that the average number of
topological defects scales as a universal power law with the quench
rate. However, the KZM focuses only on the &lt;strong&gt;mean&lt;/strong&gt; number
of defects. In this work, we aim to validate a much richer prediction:
the measured distribution of kink pairs follows a &lt;strong&gt;Poisson
binomial distribution&lt;/strong&gt;, in which all low-order cumulants scale
with universal power laws.&lt;/p&gt;
&lt;h3 id="quantum-simulation-in-momentum-space"&gt;Quantum Simulation in
Momentum Space&lt;/h3&gt;
&lt;p&gt;We experimentally probed the distribution of kink pairs in a
one-dimensional quantum Ising chain driven across the
paramagnet-ferromagnet quantum phase transition, using a single
&lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; trapped ion as a quantum simulator in
momentum space. Each mode of the quantum Ising model is mapped to a
Landau-Zener crossing, whose dynamics can be simulated with our ion-trap
qubit. By measuring the excitation probability for each mode, we
reconstruct the full counting statistics of topological defects.&lt;/p&gt;
&lt;h3 id="key-results"&gt;Key Results&lt;/h3&gt;
&lt;p&gt;We experimentally verified the universal scaling of the first
cumulants and reported deviations due to noise-induced dephasing of the
trapped ion. Our results establish that the &lt;strong&gt;universal character
of critical dynamics extends beyond KZM&lt;/strong&gt;, from the mean kink
number to the full probability distribution of topological defects —
providing a much more stringent test of universality at quantum phase
transitions.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/kibble_zurek_2020/fig1.jpg" style="max-width: 600px;" title="Experimental setup" alt="Experimental setup for testing quantum critical dynamics"&gt;
&lt;p class="caption"&gt;
Fig. 1. Experimental setup. (a) A single &lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt;
ion trapped in a needle trap. (b) The qubit energy levels. (c) The qubit
is driven by a microwave field, with operations programmed via an
arbitrary waveform generator (AWG).
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;This work was done in collaboration with Fernando Javier Gómez-Ruiz
and Adolfo del Campo from the Donostia International Physics Center,
Spain.&lt;/p&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1038/s42005-020-0306-6"&gt;https://doi.org/10.1038/s42005-020-0306-6&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>"Experimental demonstration of suppressing residual geometric dephasing" is published in Science Bulletin</title><link href="http://lqcc.ustc.edu.cn/iontrap/experimental-demonstration-suppressing-residual-geometric-dephasing.html" rel="alternate"/><published>2019-09-20T10:00:00+08:00</published><updated>2019-09-20T10:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2019-09-20:/iontrap/experimental-demonstration-suppressing-residual-geometric-dephasing.html</id><summary type="html">&lt;p&gt;Our work “Experimental demonstration of suppressing residual
geometric dephasing” has been published in &lt;strong&gt;Science
Bulletin&lt;/strong&gt;. We experimentally demonstrate effective suppression
of residual geometric dephasing — a key obstacle for high-fidelity
geometric quantum gates — using modified dynamical decoupling schemes on
a single trapped &lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; ion.&lt;/p&gt;
&lt;h3 id="the-problem-residual-geometric-dephasing"&gt;The Problem: Residual
Geometric Dephasing&lt;/h3&gt;
&lt;p&gt;The …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work “Experimental demonstration of suppressing residual
geometric dephasing” has been published in &lt;strong&gt;Science
Bulletin&lt;/strong&gt;. We experimentally demonstrate effective suppression
of residual geometric dephasing — a key obstacle for high-fidelity
geometric quantum gates — using modified dynamical decoupling schemes on
a single trapped &lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; ion.&lt;/p&gt;
&lt;h3 id="the-problem-residual-geometric-dephasing"&gt;The Problem: Residual
Geometric Dephasing&lt;/h3&gt;
&lt;p&gt;The geometric phase (Berry phase) is a promising strategy for
fault-tolerant quantum information processing because it depends only on
the geometry of the path executed, not the dynamics. However,
decoherence caused by environmental noise destroys the geometric phase.
Traditional dynamical decoupling sequences such as Spin Echo (SE) and
CPMG can eliminate &lt;strong&gt;dynamic dephasing&lt;/strong&gt; but cannot reduce
&lt;strong&gt;residual geometric dephasing&lt;/strong&gt;, which remains a critical
barrier for high-precision geometric quantum manipulation.&lt;/p&gt;
&lt;h3 id="our-solution"&gt;Our Solution&lt;/h3&gt;
&lt;p&gt;We designed &lt;strong&gt;modified dynamical decoupling schemes&lt;/strong&gt;
that carefully choose the angles of neighboring adiabatic paths on the
Bloch sphere. By varying the tilt angles in the SE and CPMG sequences,
we ensure that the accumulated geometric dephasing in successive
segments cancels out. This is achieved through two schemes:&lt;/p&gt;
&lt;ol type="1"&gt;
&lt;li&gt;&lt;strong&gt;Modified SE&lt;/strong&gt;: Using different slant angles for
neighboring evolution segments so that the geometric dephasing
contributions cancel.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Modified CPMG&lt;/strong&gt;: Separating adiabatic paths into four
parts with swapping π pulses, ensuring zero net geometric
dephasing.&lt;/li&gt;
&lt;/ol&gt;
&lt;h3 id="results"&gt;Results&lt;/h3&gt;
&lt;p&gt;Our experimental results demonstrate that the modified schemes can
reduce the dephasing rate by &lt;strong&gt;more than one order of
magnitude&lt;/strong&gt; compared with traditional dynamical decoupling
schemes in the regime where residual geometric dephasing dominates. We
also investigated the impact of noise intensity and correlation time on
the coherence of the quantum system, confirming that these methods are
effective across a wide range of noise conditions.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/geometric_dephasing_2019/fig1.jpg" style="max-width: 600px;" title="Bloch sphere dynamics" alt="Dynamics of Hamiltonian on Bloch sphere"&gt;
&lt;p class="caption"&gt;
Fig. 1. Dynamics of Hamiltonian H in the Bloch sphere and corresponding
geometric phase. (a) The Hamiltonian H tilted by angle θ evolves around
the z axis, accumulating both dynamic and geometric phases. (b) The spin
echo strategy, where the Hamiltonian rotates in opposite directions,
eliminates dynamic phase and acquires pure geometric phase.
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1016/j.scib.2019.09.007"&gt;https://doi.org/10.1016/j.scib.2019.09.007&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>Mingzhong Ai</title><link href="http://lqcc.ustc.edu.cn/iontrap/Members/Ming-Zhong_Ai.html" rel="alternate"/><published>2018-05-09T00:00:00+08:00</published><updated>2018-05-09T00:00:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2018-05-09:/iontrap/Members/Ming-Zhong_Ai.html</id><summary type="html">&lt;h2 id="personal-data"&gt;Personal data&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;Address: Key Laboratory of Quantum Information, CAS, USTC, Jinzhai
Road #96, Hefei, Anhui, P. R. China, 230026&lt;/li&gt;
&lt;li&gt;Phone: (+86) 18214880012&lt;/li&gt;
&lt;li&gt;E-mail: amz@mail.ustc.edu.cn&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;Ph.D. (enrolled September 2016), Key Lab of Quantum Information,
Department of Optics and Optical Engineering, University of Science and
Technology …&lt;/li&gt;&lt;/ul&gt;</summary><content type="html">&lt;h2 id="personal-data"&gt;Personal data&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;Address: Key Laboratory of Quantum Information, CAS, USTC, Jinzhai
Road #96, Hefei, Anhui, P. R. China, 230026&lt;/li&gt;
&lt;li&gt;Phone: (+86) 18214880012&lt;/li&gt;
&lt;li&gt;E-mail: amz@mail.ustc.edu.cn&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;Ph.D. (enrolled September 2016), Key Lab of Quantum Information,
Department of Optics and Optical Engineering, University of Science and
Technology of China, Hefei, Anhui, China&lt;/li&gt;
&lt;li&gt;2012.9-2016.7 B.Sc., Department of Physics, Shandong University,
Jinan, Shandong, China&lt;/li&gt;
&lt;/ul&gt;
</content><category term="People"/></entry><entry><title>"An Ultraviolet Fiber Fabry–Pérot Cavity for Florescence Collection of Trapped Ions" is published</title><link href="http://lqcc.ustc.edu.cn/iontrap/an-ultraviolet-fiber-fabry-perot-cavity-for-florescence-collection-of-trapped-ions-is-published.html" rel="alternate"/><published>2017-01-22T10:20:00+08:00</published><updated>2017-01-22T10:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2017-01-22:/iontrap/an-ultraviolet-fiber-fabry-perot-cavity-for-florescence-collection-of-trapped-ions-is-published.html</id><summary type="html">&lt;p&gt;Our work “An Ultraviolet Fiber Fabry–Pérot Cavity for Florescence
Collection of Trapped Ions” has been published in &lt;strong&gt;Chinese
Physics Letters&lt;/strong&gt;. We demonstrate a fiber Fabry–Pérot cavity
(FFPC) operating in the ultraviolet range at 369 nm, specifically
designed for enhancing fluorescence collection from trapped
&lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; ions — a key …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work “An Ultraviolet Fiber Fabry–Pérot Cavity for Florescence
Collection of Trapped Ions” has been published in &lt;strong&gt;Chinese
Physics Letters&lt;/strong&gt;. We demonstrate a fiber Fabry–Pérot cavity
(FFPC) operating in the ultraviolet range at 369 nm, specifically
designed for enhancing fluorescence collection from trapped
&lt;sup&gt;171&lt;/sup&gt;Yb&lt;sup&gt;+&lt;/sup&gt; ions — a key technology for building
scalable quantum networks.&lt;/p&gt;
&lt;h3 id="why-fiber-cavities"&gt;Why Fiber Cavities?&lt;/h3&gt;
&lt;p&gt;Trapped ions are an ideal platform for quantum information
processing, but building a large-scale quantum computer and
long-distance quantum communication requires the ability to
&lt;strong&gt;remotely distribute entanglement&lt;/strong&gt; between ions. The key
ingredient is efficient photon collection. A fiber Fabry–Pérot cavity
can provide a large Purcell factor to enhance the photon emission rate
while maintaining high coupling efficiency between the single fiber mode
and the cavity mode — solving the long-standing problem of low photon
collection efficiency.&lt;/p&gt;
&lt;h3 id="technical-achievements"&gt;Technical Achievements&lt;/h3&gt;
&lt;p&gt;We designed the FFPC at the bad cavity limit for fluorescence
enhancement at the &lt;sup&gt;2&lt;/sup&gt;P&lt;sub&gt;1/2&lt;/sub&gt; to
&lt;sup&gt;2&lt;/sup&gt;S&lt;sub&gt;1/2&lt;/sub&gt; transition wavelength of Yb&lt;sup&gt;+&lt;/sup&gt;. The
concave mirror profiles on fiber-end faces were fabricated using
CO&lt;sub&gt;2&lt;/sub&gt; laser machining with spatial filtering, achieving an
averaged eccentricity of only &lt;strong&gt;0.22 ± 0.04&lt;/strong&gt;. The mirrors
were coated for high reflection in the ultraviolet range by ion-beam
sputtering, achieving a coating reflectivity of &lt;strong&gt;99.76%&lt;/strong&gt;
and a finesse of &lt;strong&gt;1300 ± 100&lt;/strong&gt;.&lt;/p&gt;
&lt;h3 id="key-results"&gt;Key Results&lt;/h3&gt;
&lt;p&gt;Based on measured experimental parameters and numerical simulation,
we estimate:&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;&lt;strong&gt;Purcell factor&lt;/strong&gt; &amp;gt; 2.5&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Single-mode fiber collection efficiency&lt;/strong&gt; &amp;gt;
10%&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;These results demonstrate the FFPC’s potential to entangle remote
ions, which is the basis for constructing quantum networks and
developing distributed quantum computation.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/fiber_cavity_2017/fig1.jpg" style="max-width: 600px;" title="FFPC schematic" alt="Fiber Fabry-Pérot cavity schematic and characterization"&gt;
&lt;p class="caption"&gt;
Fig. 1. Schematic diagram of the laser machining setup for fabricating
FFPCs, and surface characterization of the machined fiber-end face using
AFM. The setup uses a CO₂ laser with spatial filtering to produce
concave mirror profiles with high circularity.
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;Find the article here: &lt;a
href="https://doi.org/10.1088/0256-307X/34/1/013701"&gt;https://doi.org/10.1088/0256-307X/34/1/013701&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>"Experimental Trapped-ion Quantum Simulation of the Kibble-Zurek dynamics in momentum space" is published</title><link href="http://lqcc.ustc.edu.cn/iontrap/experimental-trapped-ion-quantum-simulation-of-the-kibble-zurek-dynamics-in-momentum-space-is-published.html" rel="alternate"/><published>2016-09-22T10:20:00+08:00</published><updated>2016-09-22T10:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2016-09-22:/iontrap/experimental-trapped-ion-quantum-simulation-of-the-kibble-zurek-dynamics-in-momentum-space-is-published.html</id><summary type="html">&lt;p&gt;Our work &lt;em&gt;Experimental Trapped-ion Quantum Simulation of the
Kibble-Zurek dynamics in momentum space&lt;/em&gt; was published in
&lt;strong&gt;Scientific Reports&lt;/strong&gt;. This was our group’s first
trapped-ion experiment, following the development of the platform that
began in 2013. We thank our collaborators Le Luo and Adolfo del Campo
for their contributions to …&lt;/p&gt;</summary><content type="html">&lt;p&gt;Our work &lt;em&gt;Experimental Trapped-ion Quantum Simulation of the
Kibble-Zurek dynamics in momentum space&lt;/em&gt; was published in
&lt;strong&gt;Scientific Reports&lt;/strong&gt;. This was our group’s first
trapped-ion experiment, following the development of the platform that
began in 2013. We thank our collaborators Le Luo and Adolfo del Campo
for their contributions to the experiment and theory.&lt;/p&gt;
&lt;h3 id="simulating-a-quantum-phase-transition"&gt;Simulating a quantum
phase transition&lt;/h3&gt;
&lt;p&gt;The Kibble–Zurek mechanism predicts how defects form when a system is
driven through a continuous phase transition. Testing this scaling in a
quantum system requires controlled state preparation, tunable dynamics
and accurate measurements of the resulting excitations.&lt;/p&gt;
&lt;p&gt;We used a single trapped ion to simulate a transverse-field Ising
chain in momentum space. Each momentum mode is represented by a
two-level system, allowing its excitation probability to be measured
separately. Combining these measurements reconstructs the defect density
of the simulated chain.&lt;/p&gt;
&lt;p&gt;The experiment observed the predicted power-law scaling as the system
crossed the quantum critical point at different rates, providing an
experimental test of the Kibble–Zurek mechanism in the quantum
regime.&lt;/p&gt;
&lt;div class="figure" style="max-width: 600px;"&gt;
&lt;img src="/images/news/scientific_report2016/SetUp.jpg" style="max-width: 600px;" title="Experimental setup" alt="Six-needle ion trap, ytterbium-ion qubit levels and microwave control setup"&gt;
&lt;p class="caption"&gt;
Fig. 1. Experimental platform: the six-needle ion trap, the hyperfine
levels used as a qubit, and the microwave control system that drives the
simulated dynamics.
&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;Paper link: &lt;a href="https://doi.org/10.1038/srep33381"&gt;Scientific
Reports 6, 33381 (2016)&lt;/a&gt;&lt;/p&gt;
</content><category term="News"/></entry><entry><title>Ran He</title><link href="http://lqcc.ustc.edu.cn/iontrap/Members/Ran_He.html" rel="alternate"/><published>2016-09-21T10:20:00+08:00</published><updated>2016-09-21T10:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2016-09-21:/iontrap/Members/Ran_He.html</id><summary type="html">&lt;ul&gt;
&lt;li&gt;PhD alumnus&lt;/li&gt;
&lt;li&gt;office:316&lt;/li&gt;
&lt;li&gt;email:heran@mail.ustc.edu.cn&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;Introduction:&lt;/p&gt;
&lt;p&gt;I received my bachelor’s degree from Dalian University of Technology
(DUT). During a summer visit to USTC, I became interested in trapping
single ions and manipulating their quantum states with lasers, and
subsequently joined the ion-trap group as …&lt;/p&gt;</summary><content type="html">&lt;ul&gt;
&lt;li&gt;PhD alumnus&lt;/li&gt;
&lt;li&gt;office:316&lt;/li&gt;
&lt;li&gt;email:heran@mail.ustc.edu.cn&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;Introduction:&lt;/p&gt;
&lt;p&gt;I received my bachelor’s degree from Dalian University of Technology
(DUT). During a summer visit to USTC, I became interested in trapping
single ions and manipulating their quantum states with lasers, and
subsequently joined the ion-trap group as a PhD student. My doctoral
research focused on developing ion traps for confining multiple ions and
addressing them individually.&lt;/p&gt;
&lt;p&gt;In 2017.11 to 2018.11, I visited Jonathan’s ion trap group (TIQI) at
ETH, Zurich as an academic guest.&lt;/p&gt;
</content><category term="People"/></entry><entry><title>Chang-Kang Hu</title><link href="http://lqcc.ustc.edu.cn/iontrap/Members/Chang-Kang_Hu.html" rel="alternate"/><published>2016-09-19T10:20:00+08:00</published><updated>2016-09-19T10:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2016-09-19:/iontrap/Members/Chang-Kang_Hu.html</id><content type="html">&lt;figure&gt;
&lt;img src="../images/people/hckcontacts.png" alt="Chang-Kang Hu" /&gt;
&lt;figcaption aria-hidden="true"&gt;Chang-Kang Hu&lt;/figcaption&gt;
&lt;/figure&gt;
</content><category term="People"/></entry><entry><title>Jin-Ming Cui</title><link href="http://lqcc.ustc.edu.cn/iontrap/Members/Jin-Ming_Cui.html" rel="alternate"/><published>2016-09-19T10:20:00+08:00</published><updated>2016-09-19T10:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2016-09-19:/iontrap/Members/Jin-Ming_Cui.html</id><content type="html">&lt;h2 id="personal-information"&gt;Personal Information&lt;/h2&gt;
&lt;p&gt;&lt;img src="../images/people/personal_card_cui.svg" width="350" /&gt;&lt;/p&gt;
&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;2008.9-2013.6, University of Science and Technology of China,
Department of Optics and Optical Engineering, Doctor&lt;/li&gt;
&lt;li&gt;2004.8-2008.6, University of Science and Technology of China,
Department of Physics, Bachelor&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="research"&gt;Research&lt;/h2&gt;
&lt;p&gt;Quantum information with trapped ions. Quantum simulation, cavity
QED, quantum network, distributed quantum computation.&lt;/p&gt;
</content><category term="People"/></entry><entry><title>Wei-Min Lv</title><link href="http://lqcc.ustc.edu.cn/iontrap/Members/Wei-Min_Lv.html" rel="alternate"/><published>2016-09-19T10:20:00+08:00</published><updated>2016-09-19T10:20:00+08:00</updated><author><name>qng</name></author><id>tag:lqcc.ustc.edu.cn,2016-09-19:/iontrap/Members/Wei-Min_Lv.html</id><summary type="html">&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;2013.9-2016.6, University of Science and Technology of China,
Department of Optics and Optical Engineering, PhD&lt;/li&gt;
&lt;li&gt;2009.8-2013.6, Hefei University of Technology, School of Instrument
Science and Opto-electronic Engineering, Bachelor&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="contact"&gt;Contact&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;Tel: +86 13866664268&lt;/li&gt;
&lt;li&gt;Email: weimin@mail.ustc.edu.cn&lt;/li&gt;
&lt;li&gt;Address: Key Laboratory of Quantum Information, CAS …&lt;/li&gt;&lt;/ul&gt;</summary><content type="html">&lt;h2 id="education"&gt;Education&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;2013.9-2016.6, University of Science and Technology of China,
Department of Optics and Optical Engineering, PhD&lt;/li&gt;
&lt;li&gt;2009.8-2013.6, Hefei University of Technology, School of Instrument
Science and Opto-electronic Engineering, Bachelor&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="contact"&gt;Contact&lt;/h2&gt;
&lt;ul&gt;
&lt;li&gt;Tel: +86 13866664268&lt;/li&gt;
&lt;li&gt;Email: weimin@mail.ustc.edu.cn&lt;/li&gt;
&lt;li&gt;Address: Key Laboratory of Quantum Information, CAS, USTC, 96
Jinzhai Road, Hefei, Anhui 230026, China&lt;/li&gt;
&lt;/ul&gt;
</content><category term="People"/></entry></feed>