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Wireless millikelvin interconnects for superconducting quantum hardware
Authors:
Kristopher Barr,
Mingyan Zhong,
Euan Parry,
Manoj Stanley,
Qusay Al-Taai,
Paniz Foshat,
Kaveh Delfanazari,
Martin Weides,
Nick M. Ridler,
Chong Li,
Alessandro Rossi
Abstract:
Scalable quantum computing is limited by the dense network of electrical interconnects linking cryogenic quantum processors to room-temperature control electronics. To overcome this bottleneck, considerable effort has focused on cryogenic CMOS electronics and microwave-to-optical transduction, aiming to reduce wiring complexity and thermal loading. Wireless interconnects have recently emerged as a…
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Scalable quantum computing is limited by the dense network of electrical interconnects linking cryogenic quantum processors to room-temperature control electronics. To overcome this bottleneck, considerable effort has focused on cryogenic CMOS electronics and microwave-to-optical transduction, aiming to reduce wiring complexity and thermal loading. Wireless interconnects have recently emerged as a promising complementary approach, yet their compatibility with superconducting quantum hardware remains largely unexplored. Here, we demonstrate the wireless excitation of a superconducting microwave resonator of the type routinely employed for qubit readout, operating at millikelvin temperatures inside a dilution refrigerator. By directly comparing wired and wireless operation within the same cryogenic environment, we show that wireless coupling preserves the intrinsic resonator response while revealing parasitic electromagnetic pathways arising from stray radiation within the cryostat enclosure. These results establish a framework for the co-design of wireless interconnects, cryogenic packaging and superconducting quantum hardware.
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Submitted 15 July, 2026;
originally announced July 2026.
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Boronization-enabled I-mode on EAST tokamak with an expanded density window and favorable-configuration access
Authors:
X. M. Zhong,
X. L. Zou,
A. D. Liu,
L. Q. Xu,
B. Zhang,
C. Zhou,
J. P. Qian,
X. Z. Gong,
Y. T. Song,
G. Zhuang,
W. X. Shi,
L. T. Gao,
S. F. Wang,
Y. H. Guan,
G. Z. Zuo,
T. Q. Jia,
Y. X. Cheng,
S. X. Wang,
K. N. Geng,
H. L. Zhao,
EAST I-mode Working Group,
EAST Team
Abstract:
I-mode is a promising confinement regime for future fusion reactors because it combines enhanced energy confinement with L-mode-like particle transport and naturally ELM-free operation. Previous EAST I-mode studies were performed exclusively under lithium-conditioned wall conditions. Here we report the first systematic experimental investigation of I-mode under boronized wall conditions on EAST an…
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I-mode is a promising confinement regime for future fusion reactors because it combines enhanced energy confinement with L-mode-like particle transport and naturally ELM-free operation. Previous EAST I-mode studies were performed exclusively under lithium-conditioned wall conditions. Here we report the first systematic experimental investigation of I-mode under boronized wall conditions on EAST and compare it with an existing lithium-conditioned I-mode database at the same toroidal field, $B_t = 2.47$\,T. The boronized-wall dataset exhibits a substantially broader accessible density range, with the Greenwald fraction extending from $f_{\mathrm{GW}} = 0.26 - 0.77$ , compared with $f_{\mathrm{GW}} = 0.35 - 0.54$ under lithiation. A higher normalized $\mathrm{D}_α$ emission suggests that enhanced edge recycling may contribute to this density extension. A striking increase in favorable-configuration I-mode is also observed: $51\%$ boronized-wall discharges are obtained in favorable-configuration, compared with only $8\%$ lithium-conditioned discharges. These favorable-configuration cases are concentrated at high density and exhibit a deeper radial electric-field($E_r$) well and stronger $\mathbf{E_r}\times\mathbf{B}$ velocity shear. When ETRO is present, the associated transition between electron and ion turbulence is similar under the two wall conditions, although ETRO occurs less frequently ($15\%$) under boronization. An empirical EAST I-mode energy confinement scaling at fixed $B_t$ is obtained, $τ_E = 3.29 I_p^{0.51 \pm 0.10} P_{\mathrm{loss}}^{-0.53 \pm 0.05} \bar{n}_e^{0.08 \pm 0.07}$, indicating weaker power degradation than IPB98(y,2) H-mode scaling and a weak density dependence. These results show that boronization can broaden the operational space of EAST I-mode and support the development of reactor-relevant ELM-free scenarios.
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Submitted 14 July, 2026;
originally announced July 2026.
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Enhancing Neutrinoless Double-Beta Decay Sensitivity of Liquid-Xenon Time Projection Chamber with Augmented Convolutional Neural Network
Authors:
E. Aprile,
J. Aalbers,
K. Abe,
M. Adrover,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
S. R. Armbruster,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
R. M. Braun,
G. Bruni,
G. Bruno,
R. Budnik,
C. Cai,
C. Capelli,
J. M. R. Cardoso,
A. P. Cimental Chávez
, et al. (151 additional authors not shown)
Abstract:
Dual-phase time projection chamber (TPC) that employs a multi-ton-scale liquid xenon (LXe) target mass is a pioneering detector technology to search for dark matter. Beyond its advantage in dark matter direct detection efforts, the natural xenon target allows it to search for the neutrinoless double-beta decay ($0νββ$) process, which would violate lepton number conservation and indicate that neutr…
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Dual-phase time projection chamber (TPC) that employs a multi-ton-scale liquid xenon (LXe) target mass is a pioneering detector technology to search for dark matter. Beyond its advantage in dark matter direct detection efforts, the natural xenon target allows it to search for the neutrinoless double-beta decay ($0νββ$) process, which would violate lepton number conservation and indicate that neutrinos are Majorana particles. However, such $0νββ$ searches have been limited by gamma-ray backgrounds originating from the detector materials. In this work, we designed an augmented convolutional neural network (A-CNN) model to extract additional event-topology information from detector data. Using simulation and calibration data from XENONnT, a leading LXe TPC experiment, our model achieved over 60% background rejection while maintaining 90% signal acceptance. This rejection power improves XENONnT's projected sensitivity of the $^{136}$Xe $0νββ$ search by about 40%. The implementation of A-CNN in the data analysis of future liquid xenon observatories, such as XLZD, will further enhance their sensitivities for $0νββ$ with $^{136}$Xe.
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Submitted 20 March, 2026;
originally announced March 2026.
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Light Dark Matter Search with 7.8 Tonne-Year of Ionization-Only Data in XENONnT
Authors:
E. Aprile,
J. Aalbers,
K. Abe,
M. Adrover,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
S. R. Armbruster,
F. Arneodo,
L. Baudis,
M. Bazyk,
V. Beligotti,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
R. M. Braun,
G. Bruni,
G. Bruno,
R. Budnik,
C. Cai,
C. Capelli,
J. M. R. Cardoso
, et al. (152 additional authors not shown)
Abstract:
We report on a blinded search for dark matter (DM) using ionization-only (S2-only) signals in XENONnT with a total exposure of $7.83\mathrm{tonne}\times\mathrm{year}$ over 579 days in three science runs. Dedicated background suppression techniques and the first complete S2-only background model in XENONnT provide sensitivity to nuclear recoils of [0.5, 5.0] $\mathrm{keV_\mathrm{nr}}$ and electroni…
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We report on a blinded search for dark matter (DM) using ionization-only (S2-only) signals in XENONnT with a total exposure of $7.83\mathrm{tonne}\times\mathrm{year}$ over 579 days in three science runs. Dedicated background suppression techniques and the first complete S2-only background model in XENONnT provide sensitivity to nuclear recoils of [0.5, 5.0] $\mathrm{keV_\mathrm{nr}}$ and electronic recoils of [0.04, 0.7] $\mathrm{keV_\mathrm{ee}}$. No significant excess over the expected background is observed, and we set 90\% confidence level upper limits on spin-independent DM--nucleon and spin-dependent DM--neutron scattering for DM masses between 3 and 8 $\mathrm{GeV}/c^2$, as well as on DM--electron scattering, axion-like particles, and dark photons, improving on previous constraints. For spin-independent DM--nucleon scattering, we exclude cross sections above $6.0\times10^{-45} $cm$^2$ at a DM mass of 5 $\mathrm{GeV}/c^2$, pushing the XENONnT sensitivity closer to the region where coherent elastic neutrino-nucleus scattering ($\text{CE}ν\text{NS}$) becomes an irreducible background.
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Submitted 30 July, 2026; v1 submitted 16 January, 2026;
originally announced January 2026.
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Controllable Lateral Optical Forces on Janus Particles in Fluid Media
Authors:
Ziheng Xiu,
Yue Chai,
Pengyu Wen,
Chun Meng,
Min-Cheng Zhong,
Yu-Xuan Ren,
Daohong Song,
Hrvoje Buljan,
Liqin Tang,
Zhigang Chen
Abstract:
Optical forces - studied since the earliest days of laser physics - continue to reveal rich dynamics and enable powerful tools for manipulation of objects on micro- and nanoscales, and even individual atoms. Lateral optical forces, which act perpendicular to the direction of beam propagation, are particularly intriguing but have largely been restricted to interface geometries such as air - water b…
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Optical forces - studied since the earliest days of laser physics - continue to reveal rich dynamics and enable powerful tools for manipulation of objects on micro- and nanoscales, and even individual atoms. Lateral optical forces, which act perpendicular to the direction of beam propagation, are particularly intriguing but have largely been restricted to interface geometries such as air - water boundaries. Here, we realize tunable lateral optical force entirely within a fluid environment by using Janus particles: dielectric microspheres half-coated with gold. We show that the lateral optical force arises from scattering asymmetry induced by the asymmetric structure of the particles; it can be tuned by adjusting the polarization angle of a linearly polarized beam, but also particle parameters including their size and orientation. Experimentally, we directly observe fully reversible lateral propulsion of Janus particles in water merely by rotating the polarization direction, in excellent agreement with theoretical predictions. These results establish a new mechanism for programmable, polarization-controlled optical manipulation, with promising implications for biophotonics, microfluidics, and active soft-matter systems.
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Submitted 4 January, 2026;
originally announced January 2026.
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The Wiener Path Integral Interpretation of the 3:1 Combat Rule
Authors:
Wei Liang,
Ming Zhong
Abstract:
The Wiener path integral framework is proposed to model military combat dynamics by incorporating the neglected stochastic effects to the Lanchester's square law. This framework is applied to evaluate the empirical 3:1 combat rule, which posits that an attacker requires a threefold force superiority to achieve victory. Specifically, the attacker's winning probability is computed utilizing a semi-a…
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The Wiener path integral framework is proposed to model military combat dynamics by incorporating the neglected stochastic effects to the Lanchester's square law. This framework is applied to evaluate the empirical 3:1 combat rule, which posits that an attacker requires a threefold force superiority to achieve victory. Specifically, the attacker's winning probability is computed utilizing a semi-analytical Rayleigh-Ritz method. Numerical results demonstrate that the validity of the rule critically depends on specific parameter regimes, primarily contingent upon the relative combat effectiveness ratio between the opposing forces and the tolerance for attrition. This work establishes a physics-informed theoretical bridge between statistical mechanics and military operations research for analyzing uncertain combat systems.
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Submitted 26 December, 2025;
originally announced December 2025.
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The Least Action-Augmented Lanchester Model
Authors:
Wei Liang,
Han Hu,
Lijie Sun,
Pingxing Chen,
Ming Zhong
Abstract:
The principle of least action, a fundamental principle in variational mechanics with broad applicability to classical physical systems, is employed to formulate a novel attrition model for combat dynamics. This formulation extends the Lanchester's square law through second-order temporal derivatives by requiring the resultant Euler-Lagrange equation to coincide with the classical Lanchester's equa…
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The principle of least action, a fundamental principle in variational mechanics with broad applicability to classical physical systems, is employed to formulate a novel attrition model for combat dynamics. This formulation extends the Lanchester's square law through second-order temporal derivatives by requiring the resultant Euler-Lagrange equation to coincide with the classical Lanchester's equation. Initial conditions at a specified temporal point enable determination of subsequent system evolution through action minimization, while terminal boundary conditions permit backward reconstruction of combat trajectories. The model's validity is examined through historical analysis of WWII engagements: the Battle of Kursk and the Battle of Iwo Jima. Comparative studies with conventional Lanchester's square models demonstrate marked improvements in predictive accuracy regarding force strength progression, particularly in capturing non-linear attrition patterns characteristic of prolonged engagements.
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Submitted 16 December, 2025;
originally announced December 2025.
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Combined Effects of Transient Ionizing and Electromagnetic Pulse on Vertical NPN Bipolar Transistor
Authors:
Meiqing Zhong,
Cui Meng,
Yinong Liu,
Lanfeng Yuan,
Chicheng Liu,
Bolun Feng,
Maoxing Zhang
Abstract:
Combined effects of transient ionizing and electromagnetic pulse on vertical NPN bipolar transistor were experimentally investigated under pulsed X-ray irradiation. Technology computer-aided design (TCAD) simulation method was also employed to explore the underlying physical mechanisms. The results demonstrate that the combined effect of a positive pulse injected into the collector (CEMP) and puls…
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Combined effects of transient ionizing and electromagnetic pulse on vertical NPN bipolar transistor were experimentally investigated under pulsed X-ray irradiation. Technology computer-aided design (TCAD) simulation method was also employed to explore the underlying physical mechanisms. The results demonstrate that the combined effect of a positive pulse injected into the collector (CEMP) and pulsed X-ray irradiation exceeds the linear superposition of their individual effects. Conversely, the combined effect of a positive pulse injected into the base (BEMP) and pulsed X-ray irradiation aligns closely with the results observed under BEMP acting alone. Mechanism analysis reveals that when CEMP and pulsed X-ray irradiation act simultaneously, there is a significant increase in both the drift photocurrent at the collector junction and the diffusion photocurrent near the collector junction. However, when BEMP and pulsed X-ray irradiation act simultaneously, these photocurrent components remain small, leading to a combined effect similar to the results observed when BEMP acts alone. These findings provide critical insights for the radiation-hardening design of bipolar circuits in harsh radiation environments.
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Submitted 1 December, 2025;
originally announced December 2025.
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Development & Characterization of Electrodes for large-scale Xenon Time Projection Chambers
Authors:
A. Elykov,
S. Vetter,
V. H. S. Wu,
A. Deisting,
K. Eitel,
R. Gumbsheimer,
M. Kara,
S. Lichter,
S. Lindemann,
T. Luce,
Y. Ma,
J. Müller,
K. Müller,
K. Ni,
U. Oberlack,
M. Schumann,
P. Shagin,
K. Valerius,
M. Zhong
Abstract:
Dual-phase liquid xenon time projection chambers are the core detector elements of many experiments that conduct searches for Dark Matter and rare events, as well as in neutrino and high-energy physics. As part of this detector technology, high-voltage electrodes are instrumental for the generation of observable signals and their physical interpretation. Thus, electrode design and manufacturing ha…
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Dual-phase liquid xenon time projection chambers are the core detector elements of many experiments that conduct searches for Dark Matter and rare events, as well as in neutrino and high-energy physics. As part of this detector technology, high-voltage electrodes are instrumental for the generation of observable signals and their physical interpretation. Thus, electrode design and manufacturing has to fulfill stringent requirements, and their production is associated with significant engineering challenges. In this work we describe the successful development of electrodes on the 1.5 m-scale, from their design and simulation to subsequent assembly and high-voltage testing in a gaseous argon environment. The produced electrodes were recently installed as an anode and a cathode during an upgrade to the XENONnT experiment.
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Submitted 14 January, 2026; v1 submitted 20 November, 2025;
originally announced November 2025.
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Efficient High-Accuracy PDEs Solver with the Linear Attention Neural Operator
Authors:
Ming Zhong,
Zhenya Yan
Abstract:
Neural operators offer a powerful data-driven framework for learning mappings between function spaces, in which the transformer-based neural operator architecture faces a fundamental scalability-accuracy trade-off: softmax attention provides excellent fidelity but incurs quadratic complexity $\mathcal{O}(N^2 d)$ in the number of mesh points $N$ and hidden dimension $d$, while linear attention vari…
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Neural operators offer a powerful data-driven framework for learning mappings between function spaces, in which the transformer-based neural operator architecture faces a fundamental scalability-accuracy trade-off: softmax attention provides excellent fidelity but incurs quadratic complexity $\mathcal{O}(N^2 d)$ in the number of mesh points $N$ and hidden dimension $d$, while linear attention variants reduce cost to $\mathcal{O}(N d^2)$ but often suffer significant accuracy degradation. To address the aforementioned challenge, in this paper, we present a novel type of neural operators, Linear Attention Neural Operator (LANO), which achieves both scalability and high accuracy by reformulating attention through an agent-based mechanism. LANO resolves this dilemma by introducing a compact set of $M$ agent tokens $(M \ll N)$ that mediate global interactions among $N$ tokens. This agent attention mechanism yields an operator layer with linear complexity $\mathcal{O}(MN d)$ while preserving the expressive power of softmax attention. Theoretically, we demonstrate the universal approximation property, thereby demonstrating improved conditioning and stability properties. Empirically, LANO surpasses current state-of-the-art neural PDE solvers, including Transolver with slice-based softmax attention, achieving average $19.5\%$ accuracy improvement across standard benchmarks. By bridging the gap between linear complexity and softmax-level performance, LANO establishes a scalable, high-accuracy foundation for scientific machine learning applications.
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Submitted 19 October, 2025;
originally announced October 2025.
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Asymmetric integrable turbulence and rogue wave statistics for the derivative nonlinear Schrödinger equation
Authors:
Ming Zhong,
Weifang Weng,
Zhenya Yan
Abstract:
We investigate the asymmetric integrable turbulence and rogue waves (RWs) emerging from the modulation instability (MI) of plane waves for the DNLS equation. The \(n\)-th moments and ensemble-averaged kinetic and potential energy exhibit oscillatory convergence towards their steady-state values. Specifically, the amplitudes of oscillations for these indexes decay asymptotically with time as \(t^{-…
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We investigate the asymmetric integrable turbulence and rogue waves (RWs) emerging from the modulation instability (MI) of plane waves for the DNLS equation. The \(n\)-th moments and ensemble-averaged kinetic and potential energy exhibit oscillatory convergence towards their steady-state values. Specifically, the amplitudes of oscillations for these indexes decay asymptotically with time as \(t^{-1.36}\), while the phase shifts demonstrate a nonlinear decay with a rate of \(t^{-0.78}\). The frequency of these oscillations is observed to be twice the maximum growth rate of MI. These oscillations can be classified into two distinct types: one is in phase with ensemble-averaged potential energy modulus $|\langle H_4\rangle|$, and the other is anti-phase. At the same time, this unity is also reflected in the wave-action spectrum \( S_k(t) \) for a given \( k \), the auto-correlation function \( g(x,t) \) for a given \( x \), as well as the PDF \( P(I,t) \). The critical feature of the turbulence is the wave-action spectrum, which follows a power-law distribution of \( |k+3|^{-α} \) expect for $k=-3$. Unlike the NLS equation, the turbulence in the DNLS setting is asymmetric, primarily due to the asymmetry between the wave number of the plane wave from the MI and the perturbation wave number.. As the asymptotic peak value of \( S_k \) is observed at \( k = -3 \), the auto-correlation function exhibits a nonzero level as \( x \to \pm L/2 \). The PDF of the wave intensity asymptotically approaches the exponential distribution in an oscillatory manner. However, during the initial stage of the nonlinear phase, MI slightly increases the occurrence of RWs. This happens at the moments when the potential modulus is at its minimum, where the probability of RWs occurring in the range of \( I\in [12, 15] \) is significantly higher than in the asymptotic steady state.
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Submitted 16 October, 2025;
originally announced October 2025.
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Robustness of One-to-Many Interdependent Higher-order Networks Against Cascading Failures
Authors:
Cheng Qian,
Dandan Zhao,
Bo Zhang,
Ming Zhong,
Jianmin Han,
Shenghong Li,
Hao Peng,
Wei Wang
Abstract:
In the real world, the stable operation of a network is usually inseparable from the mutual support of other networks. In such an interdependent network, a node in one layer may depend on multiple nodes in another layer, forming a complex one-to-many dependency relationship. Meanwhile, there may also be higher-order interactions between multiple nodes within a layer, which increases the connectivi…
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In the real world, the stable operation of a network is usually inseparable from the mutual support of other networks. In such an interdependent network, a node in one layer may depend on multiple nodes in another layer, forming a complex one-to-many dependency relationship. Meanwhile, there may also be higher-order interactions between multiple nodes within a layer, which increases the connectivity within the layer. However, existing research on one-to-many interdependence often neglects intra-layer higher-order structures and lacks a unified theoretical framework for inter-layer dependencies. Moreover, current research on interdependent higher-order networks typically assumes idealized one-to-one inter-layer dependencies, which does not reflect the complexity of real-world systems. These limitations hinder a comprehensive understanding of how such networks withstand failures. Therefore, this paper investigates the robustness of one-to-many interdependent higher-order networks under random attacks. Depending on whether node survival requires at least one dependency edge or multiple dependency edges, we propose four inter-layer interdependency conditions and analyze the network's robustness after cascading failures induced by random attacks. Using percolation theory, we establish a unified theoretical framework that reveals how higher-order interaction structures within intra-layers and inter-layer coupling parameters affect network reliability and system resilience. Additionally, we extend our study to partially interdependent hypergraphs. We validate our theoretical analysis on both synthetic and real-data-based interdependent hypergraphs, offering insights into the optimization of network design for enhanced reliability.
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Submitted 28 September, 2025;
originally announced September 2025.
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Uncertain data assimilation for urban wind flow simulations with OpenLB-UQ
Authors:
Mingliang Zhong,
Dennis Teutscher,
Adrian Kummerländer,
Mathias J. Krause,
Martin Frank,
Stephan Simonis
Abstract:
Accurate prediction of urban wind flow is essential for urban planning, pedestrian safety, and environmental management. Yet, it remains challenging due to uncertain boundary conditions and the high cost of conventional CFD simulations. This paper presents the use of the modular and efficient uncertainty quantification (UQ) framework OpenLB-UQ for urban wind flow simulations. We specifically use t…
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Accurate prediction of urban wind flow is essential for urban planning, pedestrian safety, and environmental management. Yet, it remains challenging due to uncertain boundary conditions and the high cost of conventional CFD simulations. This paper presents the use of the modular and efficient uncertainty quantification (UQ) framework OpenLB-UQ for urban wind flow simulations. We specifically use the lattice Boltzmann method (LBM) coupled with a stochastic collocation (SC) approach based on generalized polynomial chaos (gPC). The framework introduces a relative-error noise model for inflow wind speeds based on real measurements. The model is propagated through a non-intrusive SC LBM pipeline using sparse-grid quadrature. Key quantities of interest, including mean flow fields, standard deviations, and vertical profiles with confidence intervals, are efficiently computed without altering the underlying deterministic solver. We demonstrate this on a real urban scenario, highlighting how uncertainty localizes in complex flow regions such as wakes and shear layers. The results show that the SC LBM approach provides accurate, uncertainty-aware predictions with significant computational efficiency, making OpenLB-UQ a practical tool for real-time urban wind analysis.
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Submitted 25 August, 2025;
originally announced August 2025.
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OpenLB-UQ: An Uncertainty Quantification Framework for Incompressible Fluid Flow Simulations
Authors:
Mingliang Zhong,
Adrian Kummerländer,
Shota Ito,
Mathias J. Krause,
Martin Frank,
Stephan Simonis
Abstract:
Uncertainty quantification (UQ) is crucial in computational fluid dynamics to assess the reliability and robustness of simulations, given the uncertainties in input parameters. OpenLB is an open-source lattice Boltzmann method library designed for efficient and extensible simulations of complex fluid dynamics on high-performance computers. In this work, we leverage the efficiency of OpenLB for lar…
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Uncertainty quantification (UQ) is crucial in computational fluid dynamics to assess the reliability and robustness of simulations, given the uncertainties in input parameters. OpenLB is an open-source lattice Boltzmann method library designed for efficient and extensible simulations of complex fluid dynamics on high-performance computers. In this work, we leverage the efficiency of OpenLB for large-scale flow sampling with a dedicated and integrated UQ module. To this end, we focus on non-intrusive stochastic collocation methods based on generalized polynomial chaos and Monte Carlo sampling. The OpenLB-UQ framework is extensively validated in convergence tests with respect to statistical metrics and sample efficiency using selected benchmark cases, including two-dimensional Taylor--Green vortex flows with up to four-dimensional uncertainty and a flow past a cylinder. Our results confirm the expected convergence rates and show promising scalability, demonstrating robust statistical accuracy as well as computational efficiency. OpenLB-UQ enhances the capability of the OpenLB library, offering researchers a scalable framework for UQ in incompressible fluid flow simulations and beyond.
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Submitted 19 August, 2025;
originally announced August 2025.
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WIMP Dark Matter Search using a 3.1 Tonne-Year Exposure of the XENONnT Experiment
Authors:
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
S. R. Armbruster,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
A. Brown,
G. Bruno,
R. Budnik,
C. Cai,
C. Capelli,
J. M. R. Cardoso,
A. P. Cimental Chávez,
A. P. Colijn,
J. Conrad
, et al. (153 additional authors not shown)
Abstract:
We report on a search for weakly interacting massive particle (WIMP) dark matter (DM) via elastic DM-xenon-nucleus interactions in the XENONnT experiment. We combine datasets from the first and second science campaigns resulting in a total exposure of 3.1 tonne-years. In a blind analysis of nuclear recoil events with energies above $3.8\,\mathrm{keV_{NR}}$, we find no significant excess above back…
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We report on a search for weakly interacting massive particle (WIMP) dark matter (DM) via elastic DM-xenon-nucleus interactions in the XENONnT experiment. We combine datasets from the first and second science campaigns resulting in a total exposure of 3.1 tonne-years. In a blind analysis of nuclear recoil events with energies above $3.8\,\mathrm{keV_{NR}}$, we find no significant excess above background. We set new upper limits on the spin-independent WIMP-nucleon scattering cross section for WIMP masses above $10\,\mathrm{GeV}/c^2$ with a minimum of $1.7\,\times\,10^{-47}\,\mathrm{cm^2}$ at $90\,\%$ confidence level for a WIMP mass of $30\,\mathrm{GeV}/c^2$. We achieve a best median sensitivity of $1.4\,\times\,10^{-47}\,\mathrm{cm^2}$ for a $41\,\mathrm{GeV}/c^2$ WIMP. Compared to the result from the first XENONnT science dataset, we improve our sensitivity by a factor of up to 1.8.
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Submitted 16 December, 2025; v1 submitted 25 February, 2025;
originally announced February 2025.
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Radon Removal in XENONnT down to the Solar Neutrino Level
Authors:
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
A. Brown,
G. Bruno,
R. Budnik,
C. Cai,
C. Capelli,
J. M. R. Cardoso,
A. P. Cimental Chávez,
A. P. Colijn,
J. Conrad,
J. J. Cuenca-García
, et al. (147 additional authors not shown)
Abstract:
The XENONnT experiment has achieved an exceptionally low $^\text{222}$Rn activity concentration within its inner 5.9$\,$tonne liquid xenon detector of (0.90$\,\pm\,$0.01$\,$stat.$\,\pm\,$0.07 sys.)$\,μ$Bq/kg, equivalent to about 430 $^\text{222}$Rn atoms per tonne of xenon. This was achieved by active online radon removal via cryogenic distillation after stringent material selection. The achieved…
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The XENONnT experiment has achieved an exceptionally low $^\text{222}$Rn activity concentration within its inner 5.9$\,$tonne liquid xenon detector of (0.90$\,\pm\,$0.01$\,$stat.$\,\pm\,$0.07 sys.)$\,μ$Bq/kg, equivalent to about 430 $^\text{222}$Rn atoms per tonne of xenon. This was achieved by active online radon removal via cryogenic distillation after stringent material selection. The achieved $^\text{222}$Rn activity concentration is five times lower than that in other currently operational multi-tonne liquid xenon detectors engaged in dark matter searches. This breakthrough enables the pursuit of various rare event searches that lie beyond the confines of the standard model of particle physics, with world-leading sensitivity. The ultra-low $^\text{222}$Rn levels have diminished the radon-induced background rate in the detector to a point where it is for the first time comparable to the solar neutrino-induced background, which is poised to become the primary irreducible background in liquid xenon-based detectors.
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Submitted 25 April, 2025; v1 submitted 6 February, 2025;
originally announced February 2025.
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Low-Energy Nuclear Recoil Calibration of XENONnT with a $^{88}$YBe Photoneutron Source
Authors:
XENON Collaboration,
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
A. Brown,
G. Bruno,
R. Budnik,
C. Cai,
C. Capelli,
J. M. R. Cardoso,
A. P. Cimental Chávez,
A. P. Colijn,
J. Conrad
, et al. (147 additional authors not shown)
Abstract:
Characterizing low-energy, keV-range nuclear recoils near the detector threshold is one of the major challenges for large direct dark matter detectors. To that end, we have successfully used a Yttrium-Beryllium photoneutron source that emits 152 keV neutrons for the calibration of the light and charge yields of the XENONnT experiment for the first time. After data selection, we accumulated 474 eve…
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Characterizing low-energy, keV-range nuclear recoils near the detector threshold is one of the major challenges for large direct dark matter detectors. To that end, we have successfully used a Yttrium-Beryllium photoneutron source that emits 152 keV neutrons for the calibration of the light and charge yields of the XENONnT experiment for the first time. After data selection, we accumulated 474 events from 183 hours of exposure with this source. The expected background was $55 \pm 12$ accidental coincidence events, estimated using a dedicated 152 hour background calibration run with a Yttrium-PVC gamma-only source and data-driven modeling. From these calibrations, we extracted the light (charge) yield for liquid xenon at our field strength of 23 V/cm between 0.3 (0.7) keV$_{\rm NR}$ and 5.0 keV$_{\rm NR}$. This calibration is crucial for accurately measuring the solar $^8$B neutrino coherent elastic neutrino-nucleus scattering and searching for light dark matter particles with masses below 12 GeV/c$^2$.
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Submitted 30 April, 2026; v1 submitted 11 December, 2024;
originally announced December 2024.
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Two-dimensional fractional discrete NLS equations: dispersion relations, rogue waves, fundamental and vortex solitons
Authors:
Ming Zhong,
Boris A. Malomed,
Jin Song,
Zhenya Yan
Abstract:
We introduce physically relevant new models of two-dimensional (2D) fractional lattice media accounting for the interplay of fractional intersite coupling and onsite self-focusing. Our approach features novel discrete fractional operators based on an appropriately modified definition of the continuous Riesz fractional derivative. The model of the 2D isotropic lattice employs the discrete fractiona…
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We introduce physically relevant new models of two-dimensional (2D) fractional lattice media accounting for the interplay of fractional intersite coupling and onsite self-focusing. Our approach features novel discrete fractional operators based on an appropriately modified definition of the continuous Riesz fractional derivative. The model of the 2D isotropic lattice employs the discrete fractional Laplacian, whereas the 2D anisotropic system incorporates discrete fractional derivatives acting independently along orthogonal directions with different Lévy indices (LIs). We derive exact linear dispersion relations (DRs), and identify spectral bands that permit linear modes to exist, finding them to be similar to their continuous counterparts, apart from differences in the wavenumber range. Additionally, the modulational instability in the discrete models is studied in detail, and, akin to the linear DRs, it is found to align with the situation in continuous models. This consistency highlights the nature of our newly defined discrete fractional derivatives. Furthermore, using Gaussian inputs, we produce a variety of rogue-wave structures. By means of numerical methods, we systematically construct families of 2D fundamental and vortex solitons, and examine their stability. Fundamental solitons maintain the stability due to the discrete nature of the interactions, preventing the onset of the critical and supercritical collapse. On the other hand, vortex solitons are unstable in the isotropic lattice model. However, the anisotropic one -- in particular, its symmetric version with equal LIs acting in both directions -- maintains stable vortex solitons with winding numbers $S=1$ and $S=3$. The detailed results stress the robustness of the newly defined discrete fractional Laplacian in supporting well-defined soliton modes in the 2D lattice media.
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Submitted 8 December, 2024;
originally announced December 2024.
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The neutron veto of the XENONnT experiment: Results with demineralized water
Authors:
XENON Collaboration,
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
A. Brown,
G. Bruno,
R. Budnik,
C. Cai,
C. Capelli,
J. M. R. Cardoso,
A. P. Cimental Chávez,
A. P. Colijn,
J. Conrad
, et al. (145 additional authors not shown)
Abstract:
Radiogenic neutrons emitted by detector materials are one of the most challenging backgrounds for the direct search of dark matter in the form of weakly interacting massive particles (WIMPs). To mitigate this background, the XENONnT experiment is equipped with a novel gadolinium-doped water Cherenkov detector, which encloses the xenon dual-phase time projection chamber (TPC). The neutron veto (NV)…
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Radiogenic neutrons emitted by detector materials are one of the most challenging backgrounds for the direct search of dark matter in the form of weakly interacting massive particles (WIMPs). To mitigate this background, the XENONnT experiment is equipped with a novel gadolinium-doped water Cherenkov detector, which encloses the xenon dual-phase time projection chamber (TPC). The neutron veto (NV) tags neutrons via their capture on gadolinium or hydrogen, which release $γ$-rays that are subsequently detected as Cherenkov light. In this work, we present the key features and the first results of the XENONnT NV when operated with demineralized water in the initial phase of the experiment. Its efficiency for detecting neutrons is $(82\pm 1)\,\%$, the highest neutron detection efficiency achieved in a water Cherenkov detector. This enables a high efficiency of $(53\pm 3)\,\%$ for the tagging of WIMP-like neutron signals, inside a tagging time window of $250\,\mathrm{μs}$ between TPC and NV, leading to a livetime loss of $1.6\,\%$ during the first science run of XENONnT.
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Submitted 18 December, 2024; v1 submitted 6 December, 2024;
originally announced December 2024.
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Phase-field model of alloy solidification far from chemical equilibrium at the solid-liquid interface
Authors:
Kaihua Ji,
Mingwang Zhong,
Alain Karma
Abstract:
We further develop a recently introduced phase-field model of rapid alloy solidification [Ji et al., PRL 2023]. This model utilizes enhanced solute diffusivity within the spatially diffuse interface region to quantitatively capture solute trapping with a larger interface width, thereby making simulations on experimentally relevant length and time scales computationally feasible. The main developme…
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We further develop a recently introduced phase-field model of rapid alloy solidification [Ji et al., PRL 2023]. This model utilizes enhanced solute diffusivity within the spatially diffuse interface region to quantitatively capture solute trapping with a larger interface width, thereby making simulations on experimentally relevant length and time scales computationally feasible. The main developments presented here include testing the robustness of different variational formulations, extending the model to concentrated alloys by incorporating solid and liquid free energies from thermodynamic databases, as illustrated for hypoeutectic Al-Ag alloys with CALPHAD, extending convergence tests as a function of interface width to 3D, and carrying out simulations in both 2D and 3D to examine existing theories of microstructure development. Our results indicate that the simplest variational formulation that interpolates the bulk free-energy density between its solid and liquid forms is the most robust. Remarkably, for hypoeutectic Al-Ag alloys, this formulation yields a high-velocity nonequilibrium phase diagram that is independent of interface width, thereby demonstrating that the framework of enhanced solute diffusivity can be non-trivially extended to concentrated alloys. Other variational formulations have restricted ranges of materials or processing parameters that can be reliably modeled. We use 2D simulations to construct high-velocity microstructure selection maps for dilute Al-Cu alloys. Furthermore, 3D simulations demonstrate a good convergence similar to that observed in 2D as a function of interface width. Full 3D simulations reveal that the standard theory of absolute stability is a good predictor of the upper critical velocity beyond which steady-state growth becomes unstable, despite the different morphological manifestations of this instability in 2D and 3D.
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Submitted 7 August, 2025; v1 submitted 12 November, 2024;
originally announced November 2024.
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Neutrinoless Double Beta Decay Sensitivity of the XLZD Rare Event Observatory
Authors:
XLZD Collaboration,
J. Aalbers,
K. Abe,
M. Adrover,
S. Ahmed Maouloud,
D. S. Akerib,
A. K. Al Musalhi,
F. Alder,
L. Althueser,
D. W. P. Amaral,
C. S. Amarasinghe,
A. Ames,
B. Andrieu,
N. Angelides,
E. Angelino,
B. Antunovic,
E. Aprile,
H. M. Araújo,
J. E. Armstrong,
M. Arthurs,
M. Babicz,
D. Bajpai,
A. Baker,
M. Balzer,
J. Bang
, et al. (419 additional authors not shown)
Abstract:
The XLZD collaboration is developing a two-phase xenon time projection chamber with an active mass of 60 to 80 t capable of probing the remaining WIMP-nucleon interaction parameter space down to the so-called neutrino fog. In this work we show that, based on the performance of currently operating detectors using the same technology and a realistic reduction of radioactivity in detector materials,…
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The XLZD collaboration is developing a two-phase xenon time projection chamber with an active mass of 60 to 80 t capable of probing the remaining WIMP-nucleon interaction parameter space down to the so-called neutrino fog. In this work we show that, based on the performance of currently operating detectors using the same technology and a realistic reduction of radioactivity in detector materials, such an experiment will also be able to competitively search for neutrinoless double beta decay in $^{136}$Xe using a natural-abundance xenon target. XLZD can reach a 3$σ$ discovery potential half-life of 5.7$\times$10$^{27}$ yr (and a 90% CL exclusion of 1.3$\times$10$^{28}$ yr) with 10 years of data taking, corresponding to a Majorana mass range of 7.3-31.3 meV (4.8-20.5 meV). XLZD will thus exclude the inverted neutrino mass ordering parameter space and will start to probe the normal ordering region for most of the nuclear matrix elements commonly considered by the community.
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Submitted 30 April, 2025; v1 submitted 23 October, 2024;
originally announced October 2024.
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The XLZD Design Book: Towards the Next-Generation Liquid Xenon Observatory for Dark Matter and Neutrino Physics
Authors:
XLZD Collaboration,
J. Aalbers,
K. Abe,
M. Adrover,
S. Ahmed Maouloud,
D. S. Akerib,
A. K. Al Musalhi,
F. Alder,
L. Althueser,
D. W. P. Amaral,
C. S. Amarasinghe,
A. Ames,
B. Andrieu,
N. Angelides,
E. Angelino,
B. Antunovic,
E. Aprile,
H. M. Araújo,
J. E. Armstrong,
M. Arthurs,
M. Babicz,
A. Baker,
M. Balzer,
J. Bang,
E. Barberio
, et al. (419 additional authors not shown)
Abstract:
This report describes the experimental strategy and technologies for XLZD, the next-generation xenon observatory sensitive to dark matter and neutrino physics. In the baseline design, the detector will have an active liquid xenon target of 60 tonnes, which could be increased to 80 tonnes if the market conditions for xenon are favorable. It is based on the mature liquid xenon time projection chambe…
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This report describes the experimental strategy and technologies for XLZD, the next-generation xenon observatory sensitive to dark matter and neutrino physics. In the baseline design, the detector will have an active liquid xenon target of 60 tonnes, which could be increased to 80 tonnes if the market conditions for xenon are favorable. It is based on the mature liquid xenon time projection chamber technology used in current-generation experiments, LZ and XENONnT. The report discusses the baseline design and opportunities for further optimization of the individual detector components. The experiment envisaged here has the capability to explore parameter space for Weakly Interacting Massive Particle (WIMP) dark matter down to the neutrino fog, with a 3$σ$ evidence potential for WIMP-nucleon cross sections as low as $3\times10^{-49}\rm\,cm^2$ (at 40 GeV/c$^2$ WIMP mass). The observatory will also have leading sensitivity to a wide range of alternative dark matter models. It is projected to have a 3$σ$ observation potential of neutrinoless double beta decay of $^{136}$Xe at a half-life of up to $5.7\times 10^{27}$ years. Additionally, it is sensitive to astrophysical neutrinos from the sun and galactic supernovae.
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Submitted 28 October, 2025; v1 submitted 22 October, 2024;
originally announced October 2024.
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Model-independent searches of new physics in DARWIN with a semi-supervised deep learning pipeline
Authors:
J. Aalbers,
K. Abe,
M. Adrover,
S. Ahmed Maouloud,
L. Althueser,
D. W. P. Amaral,
B. Andrieu,
E. Angelino,
D. Antón Martin,
B. Antunovic,
E. Aprile,
M. Babicz,
D. Bajpai,
M. Balzer,
E. Barberio,
L. Baudis,
M. Bazyk,
N. F. Bell,
L. Bellagamba,
R. Biondi,
Y. Biondi,
A. Bismark,
C. Boehm,
K. Boese,
R. Braun
, et al. (209 additional authors not shown)
Abstract:
We present a novel deep learning pipeline to perform a model-independent, likelihood-free search for anomalous (i.e., non-background) events in the proposed next generation multi-ton scale liquid Xenon-based direct detection experiment, DARWIN. We train an anomaly detector comprising a variational autoencoder and a classifier on extensive, high-dimensional simulated detector response data and cons…
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We present a novel deep learning pipeline to perform a model-independent, likelihood-free search for anomalous (i.e., non-background) events in the proposed next generation multi-ton scale liquid Xenon-based direct detection experiment, DARWIN. We train an anomaly detector comprising a variational autoencoder and a classifier on extensive, high-dimensional simulated detector response data and construct a one-dimensional anomaly score optimised to reject the background only hypothesis in the presence of an excess of non-background-like events. We benchmark the procedure with a sensitivity study that determines its power to reject the background-only hypothesis in the presence of an injected WIMP dark matter signal, outperforming the classical, likelihood-based background rejection test. We show that our neural networks learn relevant energy features of the events from low-level, high-dimensional detector outputs, without the need to compress this data into lower-dimensional observables, thus reducing computational effort and information loss. For the future, our approach lays the foundation for an efficient end-to-end pipeline that eliminates the need for many of the corrections and cuts that are traditionally part of the analysis chain, with the potential of achieving higher accuracy and significant reduction of analysis time.
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Submitted 9 May, 2026; v1 submitted 1 October, 2024;
originally announced October 2024.
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XENONnT Analysis: Signal Reconstruction, Calibration and Event Selection
Authors:
XENON Collaboration,
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
D. Antón Martin,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
A. Brown,
G. Bruno,
R. Budnik,
J. M. R. Cardoso,
A. P. Cimental Chávez,
A. P. Colijn,
J. Conrad,
J. J. Cuenca-García
, et al. (143 additional authors not shown)
Abstract:
The XENONnT experiment, located at the INFN Laboratori Nazionali del Gran Sasso, Italy, features a 5.9 tonne liquid xenon time projection chamber surrounded by an instrumented neutron veto, all of which is housed within a muon veto water tank. Due to extensive shielding and advanced purification to mitigate natural radioactivity, an exceptionally low background level of (15.8 $\pm$ 1.3) events/(to…
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The XENONnT experiment, located at the INFN Laboratori Nazionali del Gran Sasso, Italy, features a 5.9 tonne liquid xenon time projection chamber surrounded by an instrumented neutron veto, all of which is housed within a muon veto water tank. Due to extensive shielding and advanced purification to mitigate natural radioactivity, an exceptionally low background level of (15.8 $\pm$ 1.3) events/(tonne$\cdot$year$\cdot$keV) in the (1, 30) keV region is reached in the inner part of the TPC. XENONnT is thus sensitive to a wide range of rare phenomena related to Dark Matter and Neutrino interactions, both within and beyond the Standard Model of particle physics, with a focus on the direct detection of Dark Matter in the form of weakly interacting massive particles (WIMPs). From May 2021 to December 2021, XENONnT accumulated data in rare-event search mode with a total exposure of one tonne $\cdot$ year. This paper provides a detailed description of the signal reconstruction methods, event selection procedure, and detector response calibration, as well as an overview of the detector performance in this time frame. This work establishes the foundational framework for the `blind analysis' methodology we are using when reporting XENONnT physics results.
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Submitted 13 September, 2024;
originally announced September 2024.
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Suppression of soliton collapses, modulational instability, and rogue-wave excitation in two-Lévy-index fractional Kerr media
Authors:
Ming Zhong,
Yong Chen,
Zhenya Yan,
Boris A. Malomed
Abstract:
s in laser systems with two fractional-dispersion/diffraction terms, quantified by their Lévy indices, $α_{1}\, α_{2}\in (1, 2]$, and self-focusing or defocusing Kerr nonlinearity. Some fundamental solitons are obtained by means of the variational approximation, which are verified by comparison with numerical results. We find that the soliton collapse, exhibited by the one-dimensional cubic fracti…
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s in laser systems with two fractional-dispersion/diffraction terms, quantified by their Lévy indices, $α_{1}\, α_{2}\in (1, 2]$, and self-focusing or defocusing Kerr nonlinearity. Some fundamental solitons are obtained by means of the variational approximation, which are verified by comparison with numerical results. We find that the soliton collapse, exhibited by the one-dimensional cubic fractional nonlinear Schrödinger equation with only one Lévy index $α=1$, can be suppressed in the two-Lévy-index fractional nonlinear Schrödinger system. Stability of the solitons is also explored against collisions with Gaussian pulses and adiabatic variation of the system parameters. Modulation instability of continuous waves is investigated in the two-Lévy-index system too. In particular, the modulation instability may occur in the case of the defocusing nonlinearity when two diffraction coefficients have opposite signs. Using results for the modulation instability, we produce first- and second-order rogue waves on top of continuous waves, for both signs of the Kerr nonlinearity.
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Submitted 2 September, 2024;
originally announced September 2024.
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Two-stage initial-value iterative physics-informed neural networks for simulating solitary waves of nonlinear wave equations
Authors:
Jin Song,
Ming Zhong,
George Em Karniadakis,
Zhenya Yan
Abstract:
We propose a new two-stage initial-value iterative neural network (IINN) algorithm for solitary wave computations of nonlinear wave equations based on traditional numerical iterative methods and physics-informed neural networks (PINNs). Specifically, the IINN framework consists of two subnetworks, one of which is used to fit a given initial value, and the other incorporates physical information an…
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We propose a new two-stage initial-value iterative neural network (IINN) algorithm for solitary wave computations of nonlinear wave equations based on traditional numerical iterative methods and physics-informed neural networks (PINNs). Specifically, the IINN framework consists of two subnetworks, one of which is used to fit a given initial value, and the other incorporates physical information and continues training on the basis of the first subnetwork. Importantly, the IINN method does not require any additional data information including boundary conditions, apart from the given initial value. Corresponding theoretical guarantees are provided to demonstrate the effectiveness of our IINN method. The proposed IINN method is efficiently applied to learn some types of solutions in different nonlinear wave equations, including the one-dimensional (1D) nonlinear Schrödinger equations (NLS) equation (with and without potentials), the 1D saturable NLS equation with PT -symmetric optical lattices, the 1D focusing-defocusing coupled NLS equations, the KdV equation, the two-dimensional (2D) NLS equation with potentials, the 2D amended GP equation with a potential, the (2+1)-dimensional KP equation, and the 3D NLS equation with a potential. These applications serve as evidence for the efficacy of our method. Finally, by comparing with the traditional methods, we demonstrate the advantages of the proposed IINN method.
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Submitted 2 September, 2024;
originally announced September 2024.
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First Indication of Solar $^8$B Neutrinos via Coherent Elastic Neutrino-Nucleus Scattering with XENONnT
Authors:
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
A. Brown,
G. Bruno,
R. Budnik,
C. Cai,
C. Capelli,
J. M. R. Cardoso,
A. P. Cimental Chávez,
A. P. Colijn,
J. Conrad,
J. J. Cuenca-García
, et al. (142 additional authors not shown)
Abstract:
We present the first measurement of nuclear recoils from solar $^8$B neutrinos via coherent elastic neutrino-nucleus scattering with the XENONnT dark matter experiment. The central detector of XENONnT is a low-background, two-phase time projection chamber with a 5.9 t sensitive liquid xenon target. A blind analysis with an exposure of 3.51 t$\times$yr resulted in 37 observed events above 0.5 keV,…
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We present the first measurement of nuclear recoils from solar $^8$B neutrinos via coherent elastic neutrino-nucleus scattering with the XENONnT dark matter experiment. The central detector of XENONnT is a low-background, two-phase time projection chamber with a 5.9 t sensitive liquid xenon target. A blind analysis with an exposure of 3.51 t$\times$yr resulted in 37 observed events above 0.5 keV, with ($26.4^{+1.4}_{-1.3}$) events expected from backgrounds. The background-only hypothesis is rejected with a statistical significance of 2.73 $σ$. The measured $^8$B solar neutrino flux of $(4.7_{-2.3}^{+3.6})\times 10^6 \mathrm{cm}^{-2}\mathrm{s}^{-1}$ is consistent with results from the Sudbury Neutrino Observatory. The measured neutrino flux-weighted CE$ν$NS cross section on Xe of $(1.1^{+0.8}_{-0.5})\times10^{-39} \mathrm{cm}^2$ is consistent with the Standard Model prediction. This is the first direct measurement of nuclear recoils from solar neutrinos with a dark matter detector.
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Submitted 23 November, 2024; v1 submitted 5 August, 2024;
originally announced August 2024.
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Dynamics of discrete solitons in the fractional discrete nonlinear Schrödinger equation with the quasi-Riesz derivative
Authors:
Ming Zhong,
Boris A. Malomed,
Zhenya Yan
Abstract:
We elaborate a fractional discrete nonlinear Schrödinger (FDNLS) equation based on an appropriately modified definition of the Riesz fractional derivative, which is characterized by its Lévy index (LI). This FDNLS equation represents a novel discrete system, in which the nearest-neighbor coupling is combined with long-range interactions, that decay as the inverse square of the separation between l…
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We elaborate a fractional discrete nonlinear Schrödinger (FDNLS) equation based on an appropriately modified definition of the Riesz fractional derivative, which is characterized by its Lévy index (LI). This FDNLS equation represents a novel discrete system, in which the nearest-neighbor coupling is combined with long-range interactions, that decay as the inverse square of the separation between lattice sites. The system may be realized as an array of parallel quasi-one-dimensional Bose-Einstein condensates composed of atoms or small molecules carrying, respectively, a permanent magnetic or electric dipole moment. The dispersion relation (DR) for lattice waves and the corresponding propagation band in the system's linear spectrum are found in an exact form for all values of LI. The DR is consistent with the continuum limit, differing in the range of wavenumbers. Formation of single-site and two-site discrete solitons is explored, starting from the anti-continuum limit and continuing the analysis in the numerical form up to the existence boundary of the discrete solitons. Stability of the solitons is identified in terms of eigenvalues for small perturbations, and verified in direct simulations. Mobility of the discrete solitons is considered too, by means of an estimate of the system's Peierls-Nabarro potential barrier, and with the help of direct simulations. Collisions between persistently moving discrete solitons are also studied.
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Submitted 17 July, 2024;
originally announced July 2024.
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XENONnT WIMP Search: Signal & Background Modeling and Statistical Inference
Authors:
XENON Collaboration,
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
D. Antón Martin,
F. Arneodo,
L. Baudis,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
K. Boese,
A. Brown,
G. Bruno,
R. Budnik,
J. M. R. Cardoso,
A. P. Cimental Chávez,
A. P. Colijn,
J. Conrad,
J. J. Cuenca-García,
V. D'Andrea
, et al. (139 additional authors not shown)
Abstract:
The XENONnT experiment searches for weakly-interacting massive particle (WIMP) dark matter scattering off a xenon nucleus. In particular, XENONnT uses a dual-phase time projection chamber with a 5.9-tonne liquid xenon target, detecting both scintillation and ionization signals to reconstruct the energy, position, and type of recoil. A blind search for nuclear recoil WIMPs with an exposure of 1.1 t…
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The XENONnT experiment searches for weakly-interacting massive particle (WIMP) dark matter scattering off a xenon nucleus. In particular, XENONnT uses a dual-phase time projection chamber with a 5.9-tonne liquid xenon target, detecting both scintillation and ionization signals to reconstruct the energy, position, and type of recoil. A blind search for nuclear recoil WIMPs with an exposure of 1.1 tonne-years (4.18 t fiducial mass) yielded no signal excess over background expectations, from which competitive exclusion limits were derived on WIMP-nucleon elastic scatter cross sections, for WIMP masses ranging from 6 GeV/$c^2$ up to the TeV/$c^2$ scale. This work details the modeling and statistical methods employed in this search. By means of calibration data, we model the detector response, which is then used to derive background and signal models. The construction and validation of these models is discussed, alongside additional purely data-driven backgrounds. We also describe the statistical inference framework, including the definition of the likelihood function and the construction of confidence intervals.
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Submitted 3 June, 2025; v1 submitted 19 June, 2024;
originally announced June 2024.
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I-mode Plasma Confinement Improvement by Real-time Lithium Injection and its Classification on EAST Tokamak
Authors:
X. M. Zhong,
X. L. Zou,
A. D. Liu,
Y. T. Song,
G. Zhuang,
H. Q. Liu,
L. Q. Xu,
E. Z. Li,
B. Zhang,
G. Z. Zuo,
Z. Wang,
C. Zhou,
J. Zhang,
W. X. Shi,
L. T. Gao,
S. F. Wang,
W. Gao,
T. Q. Jia,
Q. Zang,
H. L. Zhao,
M. Wang,
H. D. Xu,
X. J. Wang,
X. Gao,
X. D. Lin
, et al. (3 additional authors not shown)
Abstract:
I-mode is a promising regime for future fusion reactors due to the high energy confinement and the moderate particle confinement. However, the effect of lithium, which has been widely applied for particle recycling and impurity control, on I-mode plasma is still unclear. Recently, experiments of real-time lithium powder injection on I-mode plasma have been carried out in EAST Tokamak. It was found…
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I-mode is a promising regime for future fusion reactors due to the high energy confinement and the moderate particle confinement. However, the effect of lithium, which has been widely applied for particle recycling and impurity control, on I-mode plasma is still unclear. Recently, experiments of real-time lithium powder injection on I-mode plasma have been carried out in EAST Tokamak. It was found that the confinement performance of the I-mode can be improved by the lithium powder injection, which can strongly reduce electron turbulence (ET) and then trigger ion turbulence (IT). Four different regimes of I-mode have been identified in EAST. The Type I I-mode plasma is characterized by the weakly coherent mode (WCM) and the geodesic-acoustic mode (GAM). The Type II I-mode is featured as the WCM and the edge temperature ring oscillation (ETRO). The Type III I-mode corresponds to the plasma with the co-existence of ETRO, GAM, and WCM. The Type IV I-mode denotes the plasma with only WCM but without ETRO and GAM. It has been observed that WCM and ETRO are increased with lithium powder injection due to the reduction of ion and electron turbulence, and the enhancement of the pedestal electron temperature gradient. EAST experiments demonstrate that lithium powder injection is an effective tool for real-time control and confinement improvement of I-mode plasma.
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Submitted 10 April, 2024;
originally announced April 2024.
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Offline tagging of radon-induced backgrounds in XENON1T and applicability to other liquid xenon detectors
Authors:
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
E. J. Brookes,
A. Brown,
G. Bruno,
R. Budnik,
T. K. Bui,
J. M. R. Cardoso,
A. P. Cimental Chavez,
A. P. Colijn,
J. Conrad
, et al. (142 additional authors not shown)
Abstract:
This paper details the first application of a software tagging algorithm to reduce radon-induced backgrounds in liquid noble element time projection chambers, such as XENON1T and XENONnT. The convection velocity field in XENON1T was mapped out using $^{222}\text{Rn}$ and $^{218}\text{Po}$ events, and the root-mean-square convection speed was measured to be $0.30 \pm 0.01$ cm/s. Given this velocity…
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This paper details the first application of a software tagging algorithm to reduce radon-induced backgrounds in liquid noble element time projection chambers, such as XENON1T and XENONnT. The convection velocity field in XENON1T was mapped out using $^{222}\text{Rn}$ and $^{218}\text{Po}$ events, and the root-mean-square convection speed was measured to be $0.30 \pm 0.01$ cm/s. Given this velocity field, $^{214}\text{Pb}$ background events can be tagged when they are followed by $^{214}\text{Bi}$ and $^{214}\text{Po}$ decays, or preceded by $^{218}\text{Po}$ decays. This was achieved by evolving a point cloud in the direction of a measured convection velocity field, and searching for $^{214}\text{Bi}$ and $^{214}\text{Po}$ decays or $^{218}\text{Po}$ decays within a volume defined by the point cloud. In XENON1T, this tagging system achieved a $^{214}\text{Pb}$ background reduction of $6.2^{+0.4}_{-0.9}\%$ with an exposure loss of $1.8\pm 0.2 \%$, despite the timescales of convection being smaller than the relevant decay times. We show that the performance can be improved in XENONnT, and that the performance of such a software-tagging approach can be expected to be further improved in a diffusion-limited scenario. Finally, a similar method might be useful to tag the cosmogenic $^{137}\text{Xe}$ background, which is relevant to the search for neutrinoless double-beta decay.
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Submitted 19 June, 2024; v1 submitted 21 March, 2024;
originally announced March 2024.
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The XENONnT Dark Matter Experiment
Authors:
XENON Collaboration,
E. Aprile,
J. Aalbers,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
M. Balata,
L. Baudis,
A. L. Baxter,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
E. J. Brookes,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
T. K. Bui
, et al. (170 additional authors not shown)
Abstract:
The multi-staged XENON program at INFN Laboratori Nazionali del Gran Sasso aims to detect dark matter with two-phase liquid xenon time projection chambers of increasing size and sensitivity. The XENONnT experiment is the latest detector in the program, planned to be an upgrade of its predecessor XENON1T. It features an active target of 5.9 tonnes of cryogenic liquid xenon (8.5 tonnes total mass in…
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The multi-staged XENON program at INFN Laboratori Nazionali del Gran Sasso aims to detect dark matter with two-phase liquid xenon time projection chambers of increasing size and sensitivity. The XENONnT experiment is the latest detector in the program, planned to be an upgrade of its predecessor XENON1T. It features an active target of 5.9 tonnes of cryogenic liquid xenon (8.5 tonnes total mass in cryostat). The experiment is expected to extend the sensitivity to WIMP dark matter by more than an order of magnitude compared to XENON1T, thanks to the larger active mass and the significantly reduced background, improved by novel systems such as a radon removal plant and a neutron veto. This article describes the XENONnT experiment and its sub-systems in detail and reports on the detector performance during the first science run.
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Submitted 13 August, 2025; v1 submitted 15 February, 2024;
originally announced February 2024.
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Design and performance of the field cage for the XENONnT experiment
Authors:
E. Aprile,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
E. J. Brookes,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
T. K. Bui,
C. Cai,
J. M. R. Cardoso,
D. Cichon
, et al. (139 additional authors not shown)
Abstract:
The precision in reconstructing events detected in a dual-phase time projection chamber depends on an homogeneous and well understood electric field within the liquid target. In the XENONnT TPC the field homogeneity is achieved through a double-array field cage, consisting of two nested arrays of field shaping rings connected by an easily accessible resistor chain. Rather than being connected to t…
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The precision in reconstructing events detected in a dual-phase time projection chamber depends on an homogeneous and well understood electric field within the liquid target. In the XENONnT TPC the field homogeneity is achieved through a double-array field cage, consisting of two nested arrays of field shaping rings connected by an easily accessible resistor chain. Rather than being connected to the gate electrode, the topmost field shaping ring is independently biased, adding a degree of freedom to tune the electric field during operation. Two-dimensional finite element simulations were used to optimize the field cage, as well as its operation. Simulation results were compared to ${}^{83m}\mathrm{Kr}$ calibration data. This comparison indicates an accumulation of charge on the panels of the TPC which is constant over time, as no evolution of the reconstructed position distribution of events is observed. The simulated electric field was then used to correct the charge signal for the field dependence of the charge yield. This correction resolves the inconsistent measurement of the drift electron lifetime when using different calibrations sources and different field cage tuning voltages.
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Submitted 21 September, 2023;
originally announced September 2023.
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Search for events in XENON1T associated with Gravitational Waves
Authors:
XENON Collaboration,
E. Aprile,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antoń Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
E. J. Brookes,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
T. K. Bui,
C. Cai,
J. M. R. Cardoso
, et al. (138 additional authors not shown)
Abstract:
We perform a blind search for particle signals in the XENON1T dark matter detector that occur close in time to gravitational wave signals in the LIGO and Virgo observatories. No particle signal is observed in the nuclear recoil, electronic recoil, CE$ν$NS, and S2-only channels within $\pm$ 500 seconds of observations of the gravitational wave signals GW170104, GW170729, GW170817, GW170818, and GW1…
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We perform a blind search for particle signals in the XENON1T dark matter detector that occur close in time to gravitational wave signals in the LIGO and Virgo observatories. No particle signal is observed in the nuclear recoil, electronic recoil, CE$ν$NS, and S2-only channels within $\pm$ 500 seconds of observations of the gravitational wave signals GW170104, GW170729, GW170817, GW170818, and GW170823. We use this null result to constrain mono-energetic neutrinos and Beyond Standard Model particles emitted in the closest coalescence GW170817, a binary neutron star merger. We set new upper limits on the fluence (time-integrated flux) of coincident neutrinos down to 17 keV at 90% confidence level. Furthermore, we constrain the product of coincident fluence and cross section of Beyond Standard Model particles to be less than $10^{-29}$ cm$^2$/cm$^2$ in the [5.5-210] keV energy range at 90% confidence level.
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Submitted 27 October, 2023; v1 submitted 20 June, 2023;
originally announced June 2023.
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Characteristics of the edge temperature ring oscillation during stationary improved confnement mode in EAST
Authors:
A. D. Liu,
X. L. Zou,
X. M. Zhong,
Y. T. Song,
M. K. Han,
Y. M. Duan,
H. Q. Liu,
T. B. Wang,
E. Z. Li,
L. Zhang,
X. Feng,
G. Zhuang,
EAST I-mode working group
Abstract:
I-mode is a natural ELMy-free regime with H-mode like improved energy confnement and L-mode like particle confnement, making it an attractive scenario for future tokamak based fusion reactors. A kind of low frequency oscillation was widely found and appeared to be unique in I-mode, with the frequency between stationary zonal flow and geodesic-acoustic mode (GAM) zonal flow. In EAST, 90 percent I-m…
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I-mode is a natural ELMy-free regime with H-mode like improved energy confnement and L-mode like particle confnement, making it an attractive scenario for future tokamak based fusion reactors. A kind of low frequency oscillation was widely found and appeared to be unique in I-mode, with the frequency between stationary zonal flow and geodesic-acoustic mode (GAM) zonal flow. In EAST, 90 percent I-mode shots have such mode, called edge temperature ring oscillation (ETRO). The mode probably plays an important role during I-mode development and sustainment, while investigations are needed to clarify the differences between ETRO and the similar mode named as low frequency edge oscillation (LFEO) in AUG and C-Mod, especially whether it is still GAM. In the paper, the ETRO characteristics in EAST were investigated in detail and most do not agree with GAM, including that 1) during L-I transition with edge Te and Ti both increasing, ETRO has a smaller frequency than GAM; 2) ETRO has distinct harmonics in various diagnostics; 3) The magnetic component of ETRO is dominated by m = 1 structure; 4) ETRO is accompanied by turbulence transition between electron-scale and ion-scale; 5) As I-mode approaching to H-mode, ETRO frequency would decrease rapidly with Te increasing. These features imply that ETRO is probably caused by the stationary zonal flow with fnite frequency. Moreover, other damping mechanisms need to be involved besides collision in the Imode edge region. It was found that modest fueling could decrease the ETRO intensity with the I-mode confnement sustaining, suggesting that supersonic molecular beam injection (SMBI) could be used as an effective tool to control ETRO.
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Submitted 14 June, 2023;
originally announced June 2023.
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Searching for Heavy Dark Matter near the Planck Mass with XENON1T
Authors:
E. Aprile,
K. Abe,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
E. J. Brookes,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
T. K. Bui,
C. Cai,
J. M. R. Cardoso,
D. Cichon
, et al. (142 additional authors not shown)
Abstract:
Multiple viable theoretical models predict heavy dark matter particles with a mass close to the Planck mass, a range relatively unexplored by current experimental measurements. We use 219.4 days of data collected with the XENON1T experiment to conduct a blind search for signals from Multiply-Interacting Massive Particles (MIMPs). Their unique track signature allows a targeted analysis with only 0.…
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Multiple viable theoretical models predict heavy dark matter particles with a mass close to the Planck mass, a range relatively unexplored by current experimental measurements. We use 219.4 days of data collected with the XENON1T experiment to conduct a blind search for signals from Multiply-Interacting Massive Particles (MIMPs). Their unique track signature allows a targeted analysis with only 0.05 expected background events from muons. Following unblinding, we observe no signal candidate events. This work places strong constraints on spin-independent interactions of dark matter particles with a mass between 1$\times$10$^{12}\,$GeV/c$^2$ and 2$\times$10$^{17}\,$GeV/c$^2$. In addition, we present the first exclusion limits on spin-dependent MIMP-neutron and MIMP-proton cross-sections for dark matter particles with masses close to the Planck scale.
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Submitted 21 April, 2023;
originally announced April 2023.
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First Dark Matter Search with Nuclear Recoils from the XENONnT Experiment
Authors:
XENON Collaboration,
E. Aprile,
K. Abe,
F. Agostini,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
M. Bazyk,
L. Bellagamba,
R. Biondi,
A. Bismark,
E. J. Brookes,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
T. K. Bui,
C. Cai
, et al. (141 additional authors not shown)
Abstract:
We report on the first search for nuclear recoils from dark matter in the form of weakly interacting massive particles (WIMPs) with the XENONnT experiment which is based on a two-phase time projection chamber with a sensitive liquid xenon mass of $5.9$ t. During the approximately 1.1 tonne-year exposure used for this search, the intrinsic $^{85}$Kr and $^{222}$Rn concentrations in the liquid targe…
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We report on the first search for nuclear recoils from dark matter in the form of weakly interacting massive particles (WIMPs) with the XENONnT experiment which is based on a two-phase time projection chamber with a sensitive liquid xenon mass of $5.9$ t. During the approximately 1.1 tonne-year exposure used for this search, the intrinsic $^{85}$Kr and $^{222}$Rn concentrations in the liquid target were reduced to unprecedentedly low levels, giving an electronic recoil background rate of $(15.8\pm1.3)~\mathrm{events}/(\mathrm{t\cdot y \cdot keV})$ in the region of interest. A blind analysis of nuclear recoil events with energies between $3.3$ keV and $60.5$ keV finds no significant excess. This leads to a minimum upper limit on the spin-independent WIMP-nucleon cross section of $2.58\times 10^{-47}~\mathrm{cm}^2$ for a WIMP mass of $28~\mathrm{GeV}/c^2$ at $90\%$ confidence level. Limits for spin-dependent interactions are also provided. Both the limit and the sensitivity for the full range of WIMP masses analyzed here improve on previous results obtained with the XENON1T experiment for the same exposure.
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Submitted 5 August, 2023; v1 submitted 26 March, 2023;
originally announced March 2023.
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Message passing approach to analyze the robustness of hypergraph
Authors:
Hao Peng,
Cheng Qian,
Dandan Zhao,
Ming Zhong,
Jianmin Han,
Runchao Li,
Wei Wang
Abstract:
Hypergraph networks are closer to real life because they can reflect higher-order interactions, so researchers have begun using them to build models for real-world networks. The mean-field approach is the current tool for studying the percolation problem on hypergraph networks. However, we found that when there is a loop in the hypergraph network, the calculated results using this approach deviate…
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Hypergraph networks are closer to real life because they can reflect higher-order interactions, so researchers have begun using them to build models for real-world networks. The mean-field approach is the current tool for studying the percolation problem on hypergraph networks. However, we found that when there is a loop in the hypergraph network, the calculated results using this approach deviate from the real results. Therefore, in this paper, we rephrase the percolation on the hypergraph network as a message passing process, thus obtaining a message passing approach. Our proposed approach has been tested in several hypergraph networks with loops, and the experimental results are more accurate than those under the mean-field approach. This is helpful to analyze and understand the robustness of hypergraph networks with loops. In addition, we also specifically analyzed how four different types of loops affect the accuracy of the experiment. Our proposed message passing approach also provides another way to study percolation on hypergraph networks.
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Submitted 28 February, 2023;
originally announced February 2023.
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Low Energy Electronic Recoils and Single Electron Detection with a Liquid Xenon Proportional Scintillation Counter
Authors:
Jianyang Qi,
Noah Hood,
Abigail Kopec,
Yue Ma,
Haiwen Xu,
Min Zhong,
Kaixuan Ni
Abstract:
Liquid xenon (LXe) is a well-studied detector medium to search for rare events in dark matter and neutrino physics. Two-phase xenon time projection chambers (TPCs) can detect electronic and nuclear recoils with energy down to kilo-electron volts (keV). In this paper, we characterize the response of a single-phase liquid xenon proportional scintillation counter (LXePSC), which produces electrolumin…
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Liquid xenon (LXe) is a well-studied detector medium to search for rare events in dark matter and neutrino physics. Two-phase xenon time projection chambers (TPCs) can detect electronic and nuclear recoils with energy down to kilo-electron volts (keV). In this paper, we characterize the response of a single-phase liquid xenon proportional scintillation counter (LXePSC), which produces electroluminescence directly in the liquid, to detect electronic recoils at low energies. Our design uses a thin (10 - 25 $μ$m diameter), central anode wire in a cylindrical LXe target where ionization electrons, created from radiation particles, drift radially towards the anode, and electroluminescence is produced. Both the primary scintillation (S1) and electroluminescence (S2) are detected by photomultiplier tubes (PMTs) surrounding the LXe target. Up to 17 photons are produced per electron, obtained with a 10 $μ$m diameter anode wire, allowing for the highly efficient detection of electronic recoils from beta decays of a tritium source down to roughly 1 keV. Single electrons, from photo-emission of the cathode wires, are observed at a gain of 1.8 photoelectrons (PE) per electron. The delayed signals following the S2 signals are dominated by single-photon-like hits, without evidence for electron signals observed in the two-phase xenon TPCs. We discuss the potential application of such a LXePSC for reactor neutrino detection via Coherent Elastic Neutrino Nucleus Scattering (CE$ν$NS).
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Submitted 19 June, 2023; v1 submitted 28 January, 2023;
originally announced January 2023.
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The Triggerless Data Acquisition System of the XENONnT Experiment
Authors:
E. Aprile,
J. Aalbers,
K. Abe,
F. Agostini,
S. Ahmed Maouloud,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
L. Bellagamba,
R. Biondi,
A. Bismark,
E. J. Brookes,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
T. K. Bui,
C. Cai,
J. M. R. Cardoso
, et al. (140 additional authors not shown)
Abstract:
The XENONnT detector uses the latest and largest liquid xenon-based time projection chamber (TPC) operated by the XENON Collaboration, aimed at detecting Weakly Interacting Massive Particles and conducting other rare event searches. The XENONnT data acquisition (DAQ) system constitutes an upgraded and expanded version of the XENON1T DAQ system. For its operation, it relies predominantly on commerc…
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The XENONnT detector uses the latest and largest liquid xenon-based time projection chamber (TPC) operated by the XENON Collaboration, aimed at detecting Weakly Interacting Massive Particles and conducting other rare event searches. The XENONnT data acquisition (DAQ) system constitutes an upgraded and expanded version of the XENON1T DAQ system. For its operation, it relies predominantly on commercially available hardware accompanied by open-source and custom-developed software. The three constituent subsystems of the XENONnT detector, the TPC (main detector), muon veto, and the newly introduced neutron veto, are integrated into a single DAQ, and can be operated both independently and as a unified system. In total, the DAQ digitizes the signals of 698 photomultiplier tubes (PMTs), of which 253 from the top PMT array of the TPC are digitized twice, at $\times10$ and $\times0.5$ gain. The DAQ for the most part is a triggerless system, reading out and storing every signal that exceeds the digitization thresholds. Custom-developed software is used to process the acquired data, making it available within $\mathcal{O}\left(10\text{ s}\right)$ for live data quality monitoring and online analyses. The entire system with all the three subsystems was successfully commissioned and has been operating continuously, comfortably withstanding readout rates that exceed $\sim500$ MB/s during calibration. Livetime during normal operation exceeds $99\%$ and is $\sim90\%$ during most high-rate calibrations. The combined DAQ system has collected more than 2 PB of both calibration and science data during the commissioning of XENONnT and the first science run.
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Submitted 21 December, 2022;
originally announced December 2022.
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Low-energy Calibration of XENON1T with an Internal $^{37}$Ar Source
Authors:
E. Aprile,
K. Abe,
F. Agostini,
S. Ahmed Maouloud,
M. Alfonsi,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
L. Bellagamba,
R. Biondi,
A. Bismark,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
T. K. Bui,
C. Cai,
C. Capelli,
J. M. R. Cardoso
, et al. (139 additional authors not shown)
Abstract:
A low-energy electronic recoil calibration of XENON1T, a dual-phase xenon time projection chamber, with an internal $^{37}$Ar source was performed. This calibration source features a 35-day half-life and provides two mono-energetic lines at 2.82 keV and 0.27 keV. The photon yield and electron yield at 2.82 keV are measured to be (32.3$\pm$0.3) photons/keV and (40.6$\pm$0.5) electrons/keV, respecti…
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A low-energy electronic recoil calibration of XENON1T, a dual-phase xenon time projection chamber, with an internal $^{37}$Ar source was performed. This calibration source features a 35-day half-life and provides two mono-energetic lines at 2.82 keV and 0.27 keV. The photon yield and electron yield at 2.82 keV are measured to be (32.3$\pm$0.3) photons/keV and (40.6$\pm$0.5) electrons/keV, respectively, in agreement with other measurements and with NEST predictions. The electron yield at 0.27 keV is also measured and it is (68.0$^{+6.3}_{-3.7}$) electrons/keV. The $^{37}$Ar calibration confirms that the detector is well-understood in the energy region close to the detection threshold, with the 2.82 keV line reconstructed at (2.83$\pm$0.02) keV, which further validates the model used to interpret the low-energy electronic recoil excess previously reported by XENON1T. The ability to efficiently remove argon with cryogenic distillation after the calibration proves that $^{37}$Ar can be considered as a regular calibration source for multi-tonne xenon detectors.
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Submitted 21 March, 2023; v1 submitted 25 November, 2022;
originally announced November 2022.
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A Review of NEST Models for Liquid Xenon and Exhaustive Comparison to Other Approaches
Authors:
M. Szydagis,
J. Balajthy,
G. A. Block,
J. P. Brodsky,
E. Brown,
J. E. Cutter,
S. J. Farrell,
J. Huang,
A. C. Kamaha,
E. S. Kozlova,
C. S. Liebenthal,
D. N. McKinsey,
K. McMichael,
R. McMonigle,
M. Mooney,
J. Mueller,
K. Ni,
G. R. C. Rischbieter,
K. Trengove,
M. Tripathi,
C. D. Tunnell,
V. Velan,
S. Westerdale,
M. D. Wyman,
Z. Zhao
, et al. (1 additional authors not shown)
Abstract:
This paper will discuss the microphysical simulation of interactions in liquid xenon, the active detector medium in many leading rare-event searches for new physics, and describe experimental observables useful for understanding detector performance. The scintillation and ionization yield distributions for signal and background will be presented using the Noble Element Simulation Technique (NEST),…
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This paper will discuss the microphysical simulation of interactions in liquid xenon, the active detector medium in many leading rare-event searches for new physics, and describe experimental observables useful for understanding detector performance. The scintillation and ionization yield distributions for signal and background will be presented using the Noble Element Simulation Technique (NEST), which is a toolkit based on experimental data and simple, empirical formulae, which mimic previous microphysics modeling, but are guided by data. The NEST models for light and charge production as a function of the particle type, energy, and electric field will be reviewed, as well as models for energy resolution and final pulse areas. NEST will be compared to other models or sets of models, and vetted against real data, with several specific examples pulled from XENON, ZEPLIN, LUX, LZ, PandaX, and table-top experiments used for calibrations.
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Submitted 19 December, 2024; v1 submitted 19 November, 2022;
originally announced November 2022.
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An approximate likelihood for nuclear recoil searches with XENON1T data
Authors:
E. Aprile,
K. Abe,
F. Agostini,
S. Ahmed Maouloud,
M. Alfonsi,
L. Althueser,
B. Andrieu,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
L. Bellagamba,
R. Biondi,
A. Bismark,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
C. Capelli,
J. M. R. Cardoso,
D. Cichon,
B. Cimmino
, et al. (129 additional authors not shown)
Abstract:
The XENON collaboration has published stringent limits on specific dark matter -nucleon recoil spectra from dark matter recoiling on the liquid xenon detector target. In this paper, we present an approximate likelihood for the XENON1T 1 tonne-year nuclear recoil search applicable to any nuclear recoil spectrum. Alongside this paper, we publish data and code to compute upper limits using the method…
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The XENON collaboration has published stringent limits on specific dark matter -nucleon recoil spectra from dark matter recoiling on the liquid xenon detector target. In this paper, we present an approximate likelihood for the XENON1T 1 tonne-year nuclear recoil search applicable to any nuclear recoil spectrum. Alongside this paper, we publish data and code to compute upper limits using the method we present. The approximate likelihood is constructed in bins of reconstructed energy, profiled along the signal expectation in each bin. This approach can be used to compute an approximate likelihood and therefore most statistical results for any nuclear recoil spectrum. Computing approximate results with this method is approximately three orders of magnitude faster than the likelihood used in the original publications of XENON1T, where limits were set for specific families of recoil spectra. Using this same method, we include toy Monte Carlo simulation-derived binwise likelihoods for the upcoming XENONnT experiment that can similarly be used to assess the sensitivity to arbitrary nuclear recoil signatures in its eventual 20 tonne-year exposure.
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Submitted 13 October, 2022;
originally announced October 2022.
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Spontaneous symmetry breaking and ghost states supported by the fractional nonlinear Schrödinger equation with focusing saturable nonlinearity and PT-symmetric potential
Authors:
Ming Zhong,
Li Wang,
Pengfei Li,
Zhenya Yan
Abstract:
We report a novel spontaneous symmetry breaking phenomenon and ghost states existed in the framework of the fractional nonlinear Schrödinger (FNLS) equation with focusing saturable nonlinearity and PT-symmetric potential. The continuous asymmetric soliton branch bifurcates from the fundamental symmetric one as the power exceeds some critical value. Intriguingly, the symmetry of fundamental soliton…
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We report a novel spontaneous symmetry breaking phenomenon and ghost states existed in the framework of the fractional nonlinear Schrödinger (FNLS) equation with focusing saturable nonlinearity and PT-symmetric potential. The continuous asymmetric soliton branch bifurcates from the fundamental symmetric one as the power exceeds some critical value. Intriguingly, the symmetry of fundamental solitons is broken into two branches of asymmetry solitons (alias ghost states) with complex conjugate propagation constants, which is solely in fractional media. Besides, the dipole (antisymmetry) and tripole solitons are also studied numerically. Moreover, we analyze the influences of fractional Lévy index and saturable nonlinear parameters on the symmetry breaking of solitons in detail. And the stability of fundamental soliton, asymmetric, dipole and tripole solitons are explored via the linear stability analysis and direct propagations. Moreover, we explore the elastic/semi-elastic collision phenomena between symmetric and asymmetric solitons. Meanwhile, we find the stable excitations from the fractional diffraction with saturation nonlinearity to integer-order diffraction with Kerr nonlinearity via the adiabatic excitations of parameters. These results will provide some theoretical basis for the study of spontaneous symmetry breaking phenomena and related physical experiments in the fractional media with PT-symmetric potentials.
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Submitted 1 October, 2022;
originally announced October 2022.
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Data-driven soliton mappings for integrable fractional nonlinear wave equations via deep learning with Fourier neural operator
Authors:
Ming Zhong,
Zhenya Yan
Abstract:
In this paper, we firstly extend the Fourier neural operator (FNO) to discovery the soliton mapping between two function spaces, where one is the fractional-order index space $\{ε|ε\in (0, 1)\}$ in the fractional integrable nonlinear wave equations while another denotes the solitonic solution function space. To be specific, the fractional nonlinear Schrödinger (fNLS), fractional Korteweg-de Vries…
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In this paper, we firstly extend the Fourier neural operator (FNO) to discovery the soliton mapping between two function spaces, where one is the fractional-order index space $\{ε|ε\in (0, 1)\}$ in the fractional integrable nonlinear wave equations while another denotes the solitonic solution function space. To be specific, the fractional nonlinear Schrödinger (fNLS), fractional Korteweg-de Vries (fKdV), fractional modified Korteweg-de Vries (fmKdV) and fractional sine-Gordon (fsineG) equations proposed recently are studied in this paper. We present the train and evaluate progress by recording the train and test loss. To illustrate the accuracies, the data-driven solitons are also compared to the exact solutions. Moreover, we consider the influences of several critical factors (e.g., activation functions containing Relu$(x)$, Sigmoid$(x)$, Swish$(x)$ and $x\tanh(x)$, depths of fully connected layer) on the performance of the FNO algorithm. We also use a new activation function, namely, $x\tanh(x)$, which is not used in the field of deep learning. The results obtained in this paper may be useful to further understand the neural networks in the fractional integrable nonlinear wave systems and the mappings between two spaces.
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Submitted 29 August, 2022;
originally announced September 2022.
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Physics-Informed Neural Networks with Adaptive Localized Artificial Viscosity
Authors:
E. J. R. Coutinho,
M. Dall'Aqua,
L. McClenny,
M. Zhong,
U. Braga-Neto,
E. Gildin
Abstract:
Physics-informed Neural Network (PINN) is a promising tool that has been applied in a variety of physical phenomena described by partial differential equations (PDE). However, it has been observed that PINNs are difficult to train in certain "stiff" problems, which include various nonlinear hyperbolic PDEs that display shocks in their solutions. Recent studies added a diffusion term to the PDE, an…
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Physics-informed Neural Network (PINN) is a promising tool that has been applied in a variety of physical phenomena described by partial differential equations (PDE). However, it has been observed that PINNs are difficult to train in certain "stiff" problems, which include various nonlinear hyperbolic PDEs that display shocks in their solutions. Recent studies added a diffusion term to the PDE, and an artificial viscosity (AV) value was manually tuned to allow PINNs to solve these problems. In this paper, we propose three approaches to address this problem, none of which rely on an a priori definition of the artificial viscosity value. The first method learns a global AV value, whereas the other two learn localized AV values around the shocks, by means of a parametrized AV map or a residual-based AV map. We applied the proposed methods to the inviscid Burgers equation and the Buckley-Leverett equation, the latter being a classical problem in Petroleum Engineering. The results show that the proposed methods are able to learn both a small AV value and the accurate shock location and improve the approximation error over a nonadaptive global AV alternative method.
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Submitted 15 March, 2022;
originally announced March 2022.
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A Next-Generation Liquid Xenon Observatory for Dark Matter and Neutrino Physics
Authors:
J. Aalbers,
K. Abe,
V. Aerne,
F. Agostini,
S. Ahmed Maouloud,
D. S. Akerib,
D. Yu. Akimov,
J. Akshat,
A. K. Al Musalhi,
F. Alder,
S. K. Alsum,
L. Althueser,
C. S. Amarasinghe,
F. D. Amaro,
A. Ames,
T. J. Anderson,
B. Andrieu,
N. Angelides,
E. Angelino,
J. Angevaare,
V. C. Antochi,
D. Antón Martin,
B. Antunovic,
E. Aprile,
H. M. Araújo
, et al. (572 additional authors not shown)
Abstract:
The nature of dark matter and properties of neutrinos are among the most pressing issues in contemporary particle physics. The dual-phase xenon time-projection chamber is the leading technology to cover the available parameter space for Weakly Interacting Massive Particles (WIMPs), while featuring extensive sensitivity to many alternative dark matter candidates. These detectors can also study neut…
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The nature of dark matter and properties of neutrinos are among the most pressing issues in contemporary particle physics. The dual-phase xenon time-projection chamber is the leading technology to cover the available parameter space for Weakly Interacting Massive Particles (WIMPs), while featuring extensive sensitivity to many alternative dark matter candidates. These detectors can also study neutrinos through neutrinoless double-beta decay and through a variety of astrophysical sources. A next-generation xenon-based detector will therefore be a true multi-purpose observatory to significantly advance particle physics, nuclear physics, astrophysics, solar physics, and cosmology. This review article presents the science cases for such a detector.
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Submitted 4 March, 2022;
originally announced March 2022.
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Application and modeling of an online distillation method to reduce krypton and argon in XENON1T
Authors:
E. Aprile,
K. Abe,
F. Agostini,
S. Ahmed Maouloud,
M. Alfonsi,
L. Althueser,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
L. Bellagamba,
A. Bernard,
R. Biondi,
A. Bismark,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
C. Capelli,
J. M. R. Cardoso,
D. Cichon,
B. Cimmino
, et al. (129 additional authors not shown)
Abstract:
A novel online distillation technique was developed for the XENON1T dark matter experiment to reduce intrinsic background components more volatile than xenon, such as krypton or argon, while the detector was operating. The method is based on a continuous purification of the gaseous volume of the detector system using the XENON1T cryogenic distillation column. A krypton-in-xenon concentration of…
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A novel online distillation technique was developed for the XENON1T dark matter experiment to reduce intrinsic background components more volatile than xenon, such as krypton or argon, while the detector was operating. The method is based on a continuous purification of the gaseous volume of the detector system using the XENON1T cryogenic distillation column. A krypton-in-xenon concentration of $(360 \pm 60)$ ppq was achieved. It is the lowest concentration measured in the fiducial volume of an operating dark matter detector to date. A model was developed and fit to the data to describe the krypton evolution in the liquid and gas volumes of the detector system for several operation modes over the time span of 550 days, including the commissioning and science runs of XENON1T. The online distillation was also successfully applied to remove Ar-37 after its injection for a low energy calibration in XENON1T. This makes the usage of Ar-37 as a regular calibration source possible in the future. The online distillation can be applied to next-generation experiments to remove krypton prior to, or during, any science run. The model developed here allows further optimization of the distillation strategy for future large scale detectors.
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Submitted 14 June, 2022; v1 submitted 22 December, 2021;
originally announced December 2021.
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Emission of Single and Few Electrons in XENON1T and Limits on Light Dark Matter
Authors:
E. Aprile,
K. Abe,
F. Agostini,
S. Ahmed Maouloud,
M. Alfonsi,
L. Althueser,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
L. Bellagamba,
A. Bernard,
R. Biondi,
A. Bismark,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
C. Capelli,
J. M. R. Cardoso,
D. Cichon,
B. Cimmino
, et al. (130 additional authors not shown)
Abstract:
Delayed single- and few-electron emissions plague dual-phase time projection chambers, limiting their potential to search for light-mass dark matter. This paper examines the origins of these events in the XENON1T experiment. Characterization of the intensity of delayed electron backgrounds shows that the resulting emissions are correlated, in time and position, with high-energy events and can effe…
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Delayed single- and few-electron emissions plague dual-phase time projection chambers, limiting their potential to search for light-mass dark matter. This paper examines the origins of these events in the XENON1T experiment. Characterization of the intensity of delayed electron backgrounds shows that the resulting emissions are correlated, in time and position, with high-energy events and can effectively be vetoed. In this work we extend previous S2-only analyses down to a single electron. From this analysis, after removing the correlated backgrounds, we observe rates < 30 events/(electron*kg*day) in the region of interest spanning 1 to 5 electrons. We derive 90% confidence upper limits for dark matter-electron scattering, first direct limits on the electric dipole, magnetic dipole, and anapole interactions, and bosonic dark matter models, where we exclude new parameter space for dark photons and solar dark photons.
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Submitted 2 September, 2024; v1 submitted 22 December, 2021;
originally announced December 2021.
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Material radiopurity control in the XENONnT experiment
Authors:
E. Aprile,
K. Abe,
F. Agostini,
S. Ahmed Maouloud,
M. Alfonsi,
L. Althueser,
E. Angelino,
J. R. Angevaare,
V. C. Antochi,
D. Antón Martin,
F. Arneodo,
L. Baudis,
A. L. Baxter,
L. Bellagamba,
R. Biondi,
A. Bismark,
A. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
C. Capelli,
J. M. R. Cardoso,
D. Cichon,
B. Cimmino,
M. Clark
, et al. (128 additional authors not shown)
Abstract:
The selection of low-radioactive construction materials is of the utmost importance for rare-event searches and thus critical to the XENONnT experiment. Results of an extensive radioassay program are reported, in which material samples have been screened with gamma-ray spectroscopy, mass spectrometry, and $^{222}$Rn emanation measurements. Furthermore, the cleanliness procedures applied to remove…
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The selection of low-radioactive construction materials is of the utmost importance for rare-event searches and thus critical to the XENONnT experiment. Results of an extensive radioassay program are reported, in which material samples have been screened with gamma-ray spectroscopy, mass spectrometry, and $^{222}$Rn emanation measurements. Furthermore, the cleanliness procedures applied to remove or mitigate surface contamination of detector materials are described. Screening results, used as inputs for a XENONnT Monte Carlo simulation, predict a reduction of materials background ($\sim$17%) with respect to its predecessor XENON1T. Through radon emanation measurements, the expected $^{222}$Rn activity concentration in XENONnT is determined to be 4.2$\,(^{+0.5}_{-0.7})\,μ$Bq/kg, a factor three lower with respect to XENON1T. This radon concentration will be further suppressed by means of the novel radon distillation system.
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Submitted 26 January, 2023; v1 submitted 10 December, 2021;
originally announced December 2021.