Lei Xiao’s research while affiliated with Southeast University and other places

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Publications (87)


Photonic Chiral State Transfer near the Liouvillian Exceptional Point
  • Article

April 2025

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11 Reads

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1 Citation

Physical Review Letters

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Konghao Sun

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[...]

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Peng Xue


Photonic chiral state transfer near the Liouvillian exceptional point
  • Preprint
  • File available

January 2025

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41 Reads

As branch-point singularities of non-Hermitian matrices, the exceptional points (EPs) exhibit unique spectral topology and criticality, with intriguing dynamic consequences in non-Hermitian settings. In open quantum systems, EPs also emerge in the Liouvillian spectrum, but their dynamic impact often pertains to the transient dynamics and is challenging to demonstrate. Here, using the flexible control afforded by single-photon interferometry, we study the chiral state transfer when the Liouvillian EP is parametrically encircled. Reconstructing the density-matrix evolution by experimentally simulating the quantum Langevin equation, we show that the chirality of the dynamics is only present within an intermediate encircling timescale and dictated by the landscape of the Liouvillian spectrum near the EP. However, the chirality disappears at long times as the system always relaxes to the steady state. We then demonstrate the universal scaling of the chirality with respect to the encircling time. Our experiment confirms the transient nature of chiral state transfer near a Liouvillian EP in open quantum systems, while our scheme paves the way for simulating general open-system dynamics using single photons.

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Quantum teleportation protocols
a Standard teleportation, where the message encoded by ψR is transmitted from the sender Alice to receiver Bob. The protocol is enabled by implementing Θ0, which involves a Bell measurement on ψR ⊗ ρAB followed by unitary operations on Bob’s system B; b Teleportation with embezzling catalyst, where Alice and Bob have an additional catalyst τCC′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\tau }_{C{C}^{{\prime} }}$$\end{document} undergoing a transformation Λ∈LOCC(RAC:BC′)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\Lambda \in {{{\rm{LOCC}}}}(RAC:B{C}^{{\prime} })$$\end{document} and coming back slightly changed. The state τCC′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\tau }_{C{C}^{{\prime} }}$$\end{document} assists in improving the performance of teleportation protocol. Alice holds the part above the dashed line and Bob holds the part below it.
The LOCC operation ΛCS defined in Eq. (22)
We use a visual example with n = 4 to illustrate the convex-split lemma. Each color represents a different state: red for ρ, white for τ, and blue for the maximally entangled state ϕ⁺. The circle portrays a uniform mixture of 4 concentric circles. Each concentric circle, from the innermost to the outermost, is designated as the t-th layer, with t ranging from 1 to 4, and represents a quantum state. For instance, every concentric circle in (a) stands for a tensor product state of the form ρ1 ⊗ τ2 ⊗ τ3 ⊗ τ4, where i ∈ 1, …, 4 denotes systems AiBi. In (b), we take layer 2 as an illustration, depicting τ1 ⊗ ρ2 ⊗ τ3 ⊗ τ4. Finally, (c) showcases the state ϕ1+⊗τ2⊗τ3⊗τ4\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\phi }_{1}^{+}\otimes {\tau }_{2}\otimes {\tau }_{3}\otimes {\tau }_{4}$$\end{document}. The symbol ≈ indicates that the purified distance between the quantum states depicted in (b) and (c) is at most η=2k/4+P(τ,ϕ+)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\eta =\sqrt{{2}^{k}/4}+P(\tau ,{\phi }^{+})$$\end{document}.
The comparison of nmin(SI/d2,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }({{{{\mathcal{S}}}}}_{{\mathbb{I}}/{d}^{2}},\epsilon )$$\end{document} and nmin(Sζi,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }({{{{\mathcal{S}}}}}_{{\zeta }_{i}},\epsilon )$$\end{document}
In (a), we sketch our idea and visualize the relation between the maximally mixed state I/d2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\mathbb{I}}/{d}^{2}$$\end{document} and the four random full-ranked states ζi with i ∈ {1, 2, 3, 4}. Each point of the line represents a possible τ considered in Eq. (24). In (b) to (e), the red and blue bar graphs respectively represent the number of copies of τ, with the red dotted line indicating the percentage of copy reduction, i.e., ϑ(ϵ), defined in Eq. (47).
The comparison of nmin(SI/d2,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }({{{{\mathcal{S}}}}}_{{\mathbb{I}}/{d}^{2}},\epsilon )$$\end{document} and nmin(N,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }(N,\epsilon )$$\end{document}
Here we choose the initial state as the one considered in Eq. (45) and take N full-ranked states randomly, to construct τ (see Eq. (24)) and compare the number of copies that are needed to achieve higher fidelity in (a). Investigation of descent ratio ϑ(N, ϵ) (see Eq. (49)) with respect to different N is shown in (b).
The comparison of nmin(SI/d2,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }({{{{\mathcal{S}}}}}_{{\mathbb{I}}/{d}^{2}},\epsilon )$$\end{document} and nmin(100,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }(100,\epsilon )$$\end{document}
a illustrates the required copies for enhancing average fidelity in entangled initial states. Left for 0.75, right for 0.80. The red and blue bar graphs illustrate the copies of τ (see Eq. (24)) corresponding to nmin(SI/d2,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }({{{{\mathcal{S}}}}}_{{\mathbb{I}}/{d}^{2}},\epsilon )$$\end{document} and nmin(100,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }(100,\epsilon )$$\end{document}, respectively. b The case of separable initial states, improved to 0.7. Here, the red and blue bar graphs represent the average fidelity before and after embezzling. In both (a) and (b), the red dashed line indicates the percentage reduction in copies of nmin(100,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }(100,\epsilon )$$\end{document} compared to nmin(SI/d2,ϵ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${n}_{\min }({{{{\mathcal{S}}}}}_{{\mathbb{I}}/{d}^{2}},\epsilon )$$\end{document}. The random states selected by us are provided in Supplementary Tables 1 and 2.

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Teleportation with embezzling catalysts

October 2024

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37 Reads

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4 Citations

Quantum teleportation is the process of transferring quantum information using classical communication and pre-shared entanglement. This process can benefit from the use of catalysts, which are ancillary entangled states that can enhance teleportation without being consumed. While chemical catalysts undergoing deactivation invariably exhibit inferior performance compared to those unaffected by deactivation, quantum catalysts, termed embezzling catalysts, that are subject to deactivation, may outperform their non-deactivating counterparts. In this work, we present teleportation protocols with embezzling catalysts that can achieve arbitrarily high fidelity. This enables the teleported state to closely approximate the original message state with arbitrary precision, while maintaining arbitrarily small variations in the catalytic system through the use of finite-dimensional embezzling catalysts. We show that some embezzling catalysts are universal, meaning that they can improve the teleportation fidelity for any pre-shared entanglement. We also explore methods to reduce the dimension of catalysts without increasing catalyst consumption, an essential step towards realizing quantum catalysis in practice.


Non-Hermitian Sensing in the Absence of Exceptional Points

October 2024

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40 Reads

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7 Citations

Physical Review Letters

Open systems possess unique potentials in high-precision sensing, yet the majority of previous studies rely on the spectral singularities known as "exceptional points." Here, we theoretically propose and experimentally demonstrate universal non-Hermitian sensing in the absence of exceptional points. The scheme makes use of the intrinsic sensitivity of a non-Hermitian probe to weak external fields, which can be understood as the direct consequence of non-Hermiticity. We confirm the basic mechanism by simulating the sensor-field dynamics using photon interferometry, and, as a concrete example, demonstrate the enhanced sensing of signals encoded in the setting angle of a wave plate. While the sensitivity of the probe is ultimately limited by the measurement noise, we find the non-Hermitian sensor showing superior performance under background noises that cannot be suppressed through repetitive measurements. Our experiment opens the avenue of enhanced sensing without exceptional points, complementing existing efforts aimed at harnessing the unique features of open systems.


Photonic Non-Abelian Braid Monopole

October 2024

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56 Reads

Monopoles and braids are exotic but elusive aspects of fundamental theories of light and matter. In lattice systems, monopoles of band-structure degeneracies are subject to well-established no-go (doubling) theorems that appear to universally apply in closed Hermitian systems and open non-Hermitian systems alike. However, the non-Abelian braid topology of non-Hermitian multi-band systems provides a remarkable loophole to these constraints. Here we make use of this loophole, and experimentally implement, for the first time, a monopole degeneracy in a non-Hermitian three-band system in the form of a single third-order exceptional point. We explicitly demonstrate the intricate braiding topology and the non-Abelian fusion rules underlying the monopole degeneracy. The experiment is carried out using a new design of single-photon interferometry, enabling eigenstate and spectral resolutions for non-Hermitian multi-band systems with widely tunable parameters. Thus, the union of state-of-the-art experiments, fundamental theory, and everyday concepts such as braids paves the way toward the highly exotic non-Abelian topology unique to non-Hermitian settings.


Observation of Non-Hermitian Edge Burst in Quantum Dynamics

August 2024

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85 Reads

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31 Citations

Physical Review Letters

The non-Hermitian skin effect, by which the eigenstates of the Hamiltonian are predominantly localized at the boundary, has revealed a strong sensitivity of non-Hermitian systems to the boundary condition. Here we experimentally observe a striking boundary-induced dynamical phenomenon known as the non-Hermitian edge burst, which is characterized by a sharp boundary accumulation of loss in non-Hermitian time evolutions. In contrast to the eigenstate localization, the edge burst represents a generic non-Hermitian dynamical phenomenon that occurs in real time. Our experiment, based on photonic quantum walks, not only confirms the prediction of the phenomenon, but also unveils its complete space-time dynamics. Our observation of edge burst paves the way for studying the rich real-time dynamics in non-Hermitian topological systems.


Experimental revival of an unknown state from the past in quantum walks

August 2024

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4 Reads

National Science Review

The physical process in the macroscopic world unfolds along a single time direction, while the evolution of a quantum system is reversible in principle. How to recover a quantum system to its past state is a complex issue of both fundamental and practical interests. In this article, we experimentally demonstrate a novel method for recovering the state in quantum walks (QWs), also known as full-state revival. Moreover, we observe two other important phenomena in QWs, recurrence and periodicity, via simplifying and repeatedly implementing the scheme, respectively. Our experiments show that obtaining these phenomena requires neither any information of the initial state nor full information of the coin operations. Our work sheds new light on quantum state engineering and recovery, and the initialization of quantum devices based on QWs.


Citations (53)


... The transition from real to complex spectra occurs at EPs, where a pair of eigenstates coalesce [40][41][42][43][44][45]. Even in situations without PT symmetry, non-Hermitian systems with non-reciprocal elements can exhibit purely real eigenenergies under OBC, which can be explained by the non-Bloch PT -symmetry theory [19,46,47]. More recently, researchers have demonstrated that non-Bloch PT symmetry serves as a comprehensive framework for understanding PT symmetry in the presence of NHSE [19,48,49]. ...

Reference:

Geometric meaning of high-order exceptional points in non-Hermitian Su–Schrieffer–Heeger model
Non-Bloch parity-time-symmetric phase transition in quantum walks
  • Citing Article
  • November 2024

Physical Review A

... It serves as the foundation of a modern society, enabling the development of technological landscapes. Entering the spotlight, quantum communication [1][2][3][4][5][6][7] is emerging as a revolutionary field that uses the principles of quantum mechanics to achieve unprecedented levels of security and efficiency, signaling a new era in data transmission. Nowadays, quantum information can already be transmitted from satellites to the ground [8][9][10][11], and quantum networks are being established within cities [12][13][14]. ...

Teleportation with embezzling catalysts

... This results in a substantially stronger response to perturbations of system parameters compared to Hermitian many-body systems. Such enhanced sensitivity has been experimentally demonstrated in various physical platforms, including superconducting qubits [50], trapped ions [51,52], optical cavity [53], photonic systems [54][55][56][57] and NV centers [58], among others. Therefore, it is essential to comprehend the significance of critical points in non-Hermitian Hamiltonians in order to develop quantum sensors, much like in the Hermitian situation. ...

Non-Hermitian Sensing in the Absence of Exceptional Points
  • Citing Article
  • October 2024

Physical Review Letters

... In non-Hermitian lossy quantum systems, the edge burst is characterized by anomalously high particle leakage near a boundary, supported by novel algebraic long-ranged decay of wavefunction amplitudes in the bulk. Beyond the canonical single-particle setting [26,27], the interplay of the edge burst with interacting many-body physics is uncharted terrain in both theory and experiments. ...

Observation of Non-Hermitian Edge Burst in Quantum Dynamics
  • Citing Article
  • August 2024

Physical Review Letters

... These models elucidate the nature of topological phase transitions in non-Hermitian quantum walks. Experiments in photonic setups have supported the presence of topological phases through observations of topological edge states [29,30] and non-Hermitian bulk-boundary correspondence [31], and have shown how the spectral topology affects the dynamics [32]. Robust entanglement can be an indicator of the topological phases in non-Hermitian quantum walks [11], in a similar way as in Hermitian quantum walks [33,34]. ...

Self acceleration from spectral geometry in dissipative quantum-walk dynamics

... pass preparations, transformations, and unsharp measurements [5], contrasting with the Kochen-Specker theorem that primarily focuses on projective measurements. Since then, generalised contextuality has been proved to subsume or be related to many common notions of nonclassicality [4,10,18,[26][27][28][29][30][31][32][33], while challenging the nonclassical status of some phenomena [34][35][36][37][38]. Within the generalized contextuality framework -and therefore throughout this manuscript -a theory or scenario therein is deemed classical when it can be explained by a generalized noncontextual ontological model. ...

Experimental investigation of contextual robustness and coherence in state discrimination

Physical Review A

... The 2 × 2 matrix generating the dynamics is non-Hermitian and has imaginary instantaneous eigenvalues whenever k < a /a and real eigenvalues otherwise. Matrices with this structure and unitary transformations of them appear frequently in the study of non-Hermitian quantum systems [70][71][72][73][74][75]. Note that these Bogoliubov equations are simply parametric oscillators in disguise [76]. ...

Experimental Observation of the Yang-Lee Quantum Criticality in Open Quantum Systems
  • Citing Article
  • April 2024

Physical Review Letters

... In Section 5, we derive, for the first time, exact expressions for the population of the postselected PT -symmetric subspace for both N = 2 and N = 3. In contrast, prior studies have relied on numerical computations and experimentation [66][67][68][69] to embed the PT -symmetric subsystem into a Hermitian Hamiltonian. We show that for N = 2 states, the proposed method has the same probability of success as conventional unambiguous quantum state discrimination [13]. ...

Demonstration of PTPT\mathcal{P}\mathcal{T}-symmetric quantum state discrimination

Quantum Information Processing

... There are two typical kinds of non-Hermitian systems, where the non-Hermiticity comes from the gain-and-loss and nonreciprocality, respectively. Extensive intriguing properties unique to these non-Hermitian systems have been discovered, such as exceptional points [5][6][7][8][9][10][11][12], new topological phases and invariants [13][14][15][16][17][18][19][20][21][22][23], the non-Hermitian skin effect (NHSE) [13,[24][25][26][27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42] and mobility ring [43,44]. The so-called NHSE is manifested as skin modes (eigenstates) localized near the boundaries and profoundly modifies the bulk-boundary correspondence in non-Hermitian systems [13]. ...

Demonstration of reversed non-Hermitian skin effect via quantum walks on a ladder

... Therefore, the QMA-EUR can accurately predict the measurement outcomes of the two observables Q 1 and Q 2 (even with zero uncertainty) when A and B are maximally entangled. This uncertainty relation has been experimentally verified [15][16][17][18] and has significant applications in quantum information science [9,[19][20][21][22][23]. Additionally, recent studies [24][25][26][27] further explored the QMA-EUR and its lower bound to enhance their accuracy and applicability. ...

Experimental investigation of conditional majorization uncertainty relations in the presence of quantum memory
  • Citing Article
  • November 2023

Physical Review A