Susy at the FPF by Luis A. Anchordoqui, Ignatios Antoniadis, Karim Benakli, Jules Cunat, Dieter Lüst

“…The failure to observe signals of sparticle production at the large hadron collider (LHC) has eroded the central motivation for SUSY breaking at the weak scale. …”
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Study of Nonleptonic Bq∗→DqV and PqD∗ Weak Decays by Qin Chang, Xiaohui Hu, Junfeng Sun, Xiaolin Wang, Yueling Yang

“…Motivated by the powerful capability of measurement for the b hadron decays at LHC and SuperKEKB/Belle-II, the nonleptonic B-∗→DD-∗, Dρ-, DK∗-, πD∗, and KD∗ decays are studied. …”
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Deep(er) reconstruction of imaging Cherenkov detectors with swin transformers and normalizing flow models by C Fanelli, J Giroux, J Stevens

“…At the future electron–ion collider (EIC), the ePIC detector will feature a dual Ring Imaging Cherenkov (RICH) detector in the hadron direction, a Detector of Internally Reflected Cherenkov (DIRC) in the barrel, and a proximity focus RICH in the electron direction. …”
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Study of 1D Strange Charmed Meson Family Using HQET by Pallavi Gupta, A. Upadhyay

“…We study its decay modes variation with hadronic coupling constant gxh and the mixing angle θ. …”
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J/ψ photoproduction and polarization in peripheral Pb−Pb collisions with ALICE by Mallick Dukhishyam

“…Recently, coherent photoproduction of J/ψ has been observed in nucleus–nucleus (A–A) collisions with nuclear overlap, based on the measurement of an excess of production with respect to hadron-production expectations in the very low transverse momentum (pT). …”
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Phenomenology of electroweak portal dark showers: high energy direct probes and low energy complementarity by Hsin-Chia Cheng, Xu-Hui Jiang, Lingfeng Li

“…We focus on dark shower events initiated by various bosons at the Large Hadron Collider (LHC). The most prominent signal is the displaced decay of GeV-scale dark pions as LLPs. …”
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Extracting the femtometer structure of strange baryons using the vacuum polarization effect by The BESIII Collaboration

“…Electromagnetic form factors quantify the structure of hadrons in terms of charge and magnetization distributions. …”
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NNLO PDFs driven by top-quark data by S. Alekhin, M. V. Garzelli, S.-O. Moch, O. Zenaiev

“…Abstract We study the impact of state-of-the-art top-quark data collected at the large hadron collider on parton distribution functions (PDFs). …”
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Big Data Analytics for the ATLAS EventIndex Project with Apache Spark by Álvaro Fernández Casaní, Carlos García Montoro, Santiago González de la Hoz, José Salt, Javier Sánchez, Miguel Villaplana Pérez

“…The ATLAS EventIndex was designed to provide a global event catalogue and limited event-level metadata for ATLAS experiment of the Large Hadron Collider (LHC) and their analysis groups and users during Run 2 (2015-2018) and has been running in production since. …”
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Experimental Results on Charge Fluctuations in Heavy-Ion Collisions by D. K. Mishra, P. Garg, P. K. Netrakanti, L. M. Pant, A. K. Mohanty

“…Deviations are observed in both Sσ and κσ2 for net-proton multiplicity distributions from the Skellam and hadron resonance gas model for sNN<39 GeV. Higher moment results of the net-electric charge and net-kaon do not observe any significant nonmonotonic behavior as a function of collision energy. …”
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Nonperturbative and Thermal Dynamics of Confined Fields in Dual QCD by H. C. Chandola, Deependra Singh Rawat, Dinesh Yadav, H. C. Pandey, H. Dehnen

“…The thermal variation of the profiles of the color electic field is further investigated which indicates the survival of flux tubes even in the thermal domain that leads the possibility of the formation of some exotic states like QGP in the intermediate regime during the quark-hadron phase transition.…”
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Measurement of the production cross section of prompt $$\Xi ^0_{\textrm{c}}$$ Ξ c 0 baryons in p–Pb collisions at $$\sqrt{s_{{\textrm{NN}}}}=5.02$$ s NN = 5.02  TeV by ALICE Collaboration

“…Abstract The transverse momentum ( $$p_{\textrm{T}}$$ p T ) differential production cross section of the promptly produced charm-strange baryon $$\mathrm {\Xi _{c}^{0}}$$ Ξ c 0 (and its charge conjugate $$\overline{\mathrm {\Xi _{c}^{0}}}$$ Ξ c 0 ¯ ) is measured at midrapidity via its hadronic decay into $$\mathrm{\pi ^{+}}\Xi ^{-}$$ π + Ξ - in p–Pb collisions at a centre-of-mass energy per nucleon–nucleon collision $$\sqrt{s_{\textrm{NN}}}~=~5.02$$ s NN = 5.02  TeV with the ALICE detector at the LHC. …”
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Search for Neutrino Signals Correlated with LHAASO Diffuse Galactic Emission by Wenlian Li, Tian-Qi Huang, Donglian Xu, Huihai He

“…The measured muon neutrino intensity at 25 TeV is $4.7{3}_{-2.51}^{+2.53}\times 1{0}^{-14}\,{{\rm{TeV}}}^{-1}\,{{\rm{cm}}}^{-2}\,{{\rm{s}}}^{-1}\,{{\rm{sr}}}^{-1}$ , consistent with the expected neutrino flux assuming that all the diffuse Galactic γ -rays originate from hadronic interactions. In the Galactic plane scan search, the most significant location is found at l  = 63 $\mathop{.}…”
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SymbolNet: neural symbolic regression with adaptive dynamic pruning for compression by Ho Fung Tsoi, Vladimir Loncar, Sridhara Dasu, Philip Harris

“…These capabilities are highly valuable in environments with stringent computational resource constraints, such as high-energy physics experiments at the CERN Large Hadron Collider. However, finding compact expressions for high-dimensional datasets remains challenging due to the inherent limitations of genetic programming (GP), the search algorithm of most symbolic regression (SR) methods. …”
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Improved π 0 , η, η′ transition form factors in resonance chiral theory and their a μ HLbL $$ {a}_{\mu}^{\textrm{HLbL}} $$ contribution by Emilio J. Estrada, Sergi Gonzàlez-Solís, Adolfo Guevara, Pablo Roig

“…Our evaluation of the corresponding pole contributions to the hadronic light-by-light piece of the muon g − 2 read: a μ π 0 − pole = 61.9 ± 0.6 − 1.5 + 2.4 × 10 − 11 $$ {a}_{\mu}^{\pi^0-\textrm{pole}}=\left(61.9\pm {0.6}_{-1.5}^{+2.4}\right)\times {10}^{-11} $$ , a μ η − pole = 15.2 ± 0.5 − 0.8 + 1.1 × 10 − 11 $$ {a}_{\mu}^{\eta -\textrm{pole}}=\left(15.2\pm {0.5}_{-0.8}^{+1.1}\right)\times {10}^{-11} $$ and a μ η ′ − pole = 14.2 ± 0.7 − 0.9 + 1.4 × 10 − 11 $$ {a}_{\mu}^{\eta^{\prime }-\textrm{pole}}=\left(14.2\pm {0.7}_{-0.9}^{+1.4}\right)\times {10}^{-11} $$ , for a total of a μ π 0 + η + η ′ − pole = 91.3 ± 1.0 − 1.9 + 3.0 × 10 − 11 $$ {a}_{\mu}^{\pi^0+\eta +{\eta}^{\prime }-\textrm{pole}}=\left(91.3\pm {1.0}_{-1.9}^{+3.0}\right)\times {10}^{-11} $$ , where the first and second errors are the statistical and systematic uncertainties, respectively.…”
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Characterization of Sleep Structure and Autonomic Dysfunction in REM Sleep Behavior Disorder by Nicla Mandas, Maximiliano Mollura, Giulia Baldazzi, Parisa Sattar, Maria Mura, Elisa Casaglia, Michela Figorilli, Laura Giorgetti, Pietro Mattioli, Francesco Calizzano, Francesco Fama, Dario Arnaldi, Monica Puligheddu, Danilo Pani, Riccardo Barbieri

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Form factors of $$\varLambda _b^0 \rightarrow \varLambda _c(2595)^+$$ Λ b 0 → Λ c ( 2595 ) + within light-cone QCD sum rules by Hui-Hui Duan, Yong-Lu Liu, Qin Chang, Ming-Qiu Huang

“…Utilizing the light-cone QCD sum rules approach, we incorporated the contributions of the lowest two charm baryon states: the ground state $$\varLambda _c$$ Λ c with $$J^P=\frac{1}{2}^+$$ J P = 1 2 + and the excited state $$\varLambda _c(2595)^+$$ Λ c ( 2595 ) + with $$J^P=\frac{1}{2}^-$$ J P = 1 2 - in the hadronic representation of the $$\varLambda _b \rightarrow \varLambda _c(2595)^+$$ Λ b → Λ c ( 2595 ) + transition correlation function. …”
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Elliptic and Quadrangular Flow of Protons in the High-Baryon-Density Region by Shaowei Lan, Zuowen Liu, Like Liu, Shusu Shi

“…In this paper, we use the hadronic transport model SMASH to investigate the elliptic flow (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>v</mi><mn>2</mn></msub></semantics></math></inline-formula>), quadrangular flow (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>v</mi><mn>4</mn></msub></semantics></math></inline-formula>), and their ratio (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>v</mi><mn>4</mn></msub><mo>/</mo><msubsup><mi>v</mi><mrow><mn>2</mn></mrow><mn>2</mn></msubsup></mrow></semantics></math></inline-formula>) in Au+Au collisions at high baryon density. …”
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