Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeVThe first collider search for dark matter arising from a strongly coupled hidden sector is presented and uses a data sample corresponding to 138 fb-1, collected with the CMS detector at the CERN…CMS Collaboration·Dec 21, 2021SaveLearn
Determination of Proton Parton Distribution Functions using ATLAS DataUsing differential cross-section data of inclusive W and Z/γ boson production and of their production in association with jets, and differential cross-section data of top-quark pair…Zhiqing Zhang·Dec 21, 2021SaveLearn
Search for baryon and lepton number violating decays D0 pe+ and D0 pe-Using an electron-positron collision data sample corresponding to an integrated luminosity of 2.93~fb-1 collected with the BESIII detector at a center-of-mass energy of 3.773 GeV, we search for…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 21, 2021SaveLearn
Constraints on the CKM angle γ from B Dh decays using D→ h hπ0 final statesA data sample collected with the LHCb detector corresponding to an integrated luminosity of 9 fb-1 is used to measure eleven CP violation observables in B Dh decays, where h is…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 20, 2021SaveLearn
A background-free optically levitated charge sensorOptically levitated macroscopic objects are a powerful tool in the field of force sensing, owing to high sensitivity, absolute force calibration, environmental isolation and the advanced degree of…Nadav Priel, Alexander Fieguth, Charles P. Blakemore et al.·Dec 20, 2021SaveLearn
First test of Lepton Flavor Universality in the charmed baryon decays 0c - + using data of the Belle experimentWe present the first observation of the c0 - μ+ μ decay and present measurements of the branching fraction ratios of the $c0 -…Belle Collaboration, Y. B. Li, C. P. Shen et al.·Dec 20, 2021SaveLearn
B boson search at KLOE/KLOE-2Following the many contributions, KLOE-2 has done to Dark Matter (DM) searches, an alternative model, where the Dark Force mediator is a hypothetical leptophobic B boson, in contra-position to the U…Elena Perez del Rio·Dec 19, 2021SaveLearn
Search for flavor-changing neutral current interactions of the top quark and the Higgs boson decaying to a bottom quark-antiquark pair at s = 13 TeVA search for flavor-changing neutral current interactions of the top quark (t) and the Higgs boson (H) is presented. The search is based on a data sample corresponding to an integrated luminosity of…CMS Collaboration·Dec 17, 2021SaveLearn
Measurement of the production cross section for Z + b jets in proton-proton collisions at s = 13 TeVThe measurement of the cross section for the production of a Z boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision…CMS Collaboration·Dec 17, 2021SaveLearn
Modelling and computational improvements to the simulation of single vector-boson plus jet processes for the ATLAS experimentThis paper presents updated Monte Carlo configurations used to model the production of single electroweak vector bosons (W, Z/γ*) in association with jets in proton-proton collisions for…ATLAS Collaboration·Dec 17, 2021SaveLearn
Comparisons and challenges of modern neutrino-scattering experiments (TENSIONS 2019 report)A set of comparisons among neutrino interaction experiments (MiniBooNE, MINERvA, T2K, and MicroBooNE) is presented. This gives a broad view of the field of neutrino-nucleus interactions. The emphasis…M. Buizza Avanzini, M. Betancourt, D. Cherdack et al.·Dec 16, 2021SaveLearn
Measurement of the inclusive tt production cross section in proton-proton collisions at s = 5.02 TeVThe top quark pair production cross section is measured in proton-proton collisions at a center-of-mass energy of 5.02 TeV. The data were collected in a special LHC low-energy and low-intensity run…CMS Collaboration·Dec 16, 2021SaveLearn
Inclusive and differential cross-sections measurements in the single top tW e-mu channel with CMSInclusive and normalised differential cross sections measurements are presented for the production of single top quarks in association with a W boson, in proton-proton collisions at a centre-of-mass…Alejandro Soto Rodríguez·Dec 16, 2021SaveLearn
A note on blind technique for new physics searches in particle physicsThis paper attempts to classify various blinding strategies used in particle physics. It argues that the blinding technique is not used consistently throughout searches for new physics. More…S. V. Chekanov·Dec 16, 2021SaveLearn
A Search for the Cosmic Ray Boosted Sub-GeV Dark Matter at the PandaX-II ExperimentWe report a novel search for the cosmic ray boosted dark matter using the 100~tonne·day full data set of the PandaX-II detector located at the China Jinping Underground Laboratory. With the…Xiangyi Cui, Abdusalam Abdukerim, Zihao Bo et al.·Dec 16, 2021SaveLearn
Identification of charm jets at LHCbThe identification of charm jets is achieved at LHCb for data collected in 2015-2018 using a method based on the properties of displaced vertices reconstructed and matched with jets. The performance…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 15, 2021SaveLearn
Feed-forward neural network unfoldingA feed-forward neural network is demonstrated to efficiently unfold the energy distribution of protons and alpha particles passing through passive material. This model-independent approach works with…Ming-Liang Wong, Andrew Edmonds, Chen Wu·Dec 15, 2021SaveLearn
A search for an unexpected asymmetry in the production of e+ μ- and e- μ+ pairs in proton-proton collisions recorded by the ATLAS detector at s = 13 TeVThis search, a type not previously performed at ATLAS, uses a comparison of the production cross sections for e+ μ- and e- μ+ pairs to constrain physics processes beyond the Standard…ATLAS Collaboration·Dec 15, 2021SaveLearn
Domain-informed neural networks for interaction localization within astroparticle experimentsThis work proposes a domain-informed neural network architecture for experimental particle physics, using particle interaction localization with the time-projection chamber (TPC) technology for dark…Shixiao Liang, Aaron Higuera, Christina Peters et al.·Dec 15, 2021SaveLearn
Precision measurement of forward Z boson production in proton-proton collisions at s = 13 TeVA precision measurement of the Z boson production cross-section at s = 13 TeV in the forward region is presented, using pp collision data collected by the LHCb detector, corresponding to…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 14, 2021SaveLearn
Cross section measurements of the e+e- D*+D*- and e+e- D*+D- processes at center-of-mass energies from 4.085 to 4.600 GeVThe Born cross sections of the e+e- D*+D*- and e+e- D*+D- processes are measured using e+e- collision data collected with the BESIII experiment at center-of-mass…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 13, 2021SaveLearn
Search for Highly-Ionizing Particles in pp Collisions at the LHC's Run-1 Using the Prototype MoEDAL DetectorA search for highly electrically charged objects (HECOs) and magnetic monopoles is presented using 2.2 fb-1 of p - p collision data taken at a centre of mass energy (ECM) of 8 TeV by the MoEDAL…B. Acharya, J. Alexandre, P. Benes et al.·Dec 10, 2021SaveLearn
Transverse-single-spin asymmetries of charged pions at midrapidity in transversely polarized p+p collisions at s=200 GeVIn 2015, the PHENIX collaboration has measured single-spin asymmetries for charged pions in transversely polarized proton-proton collisions at the center of mass energy of s=200 GeV. The…U. A. Acharya, C. Aidala, Y. Akiba et al.·Dec 10, 2021SaveLearn
Accessing glue through photoproduction measurements at GlueXPhotoproduction experiments are a key tool in the investigation of the spectrum of hadronic states and the way gluons contribute to this spectrum. The GlueX experiment, located at Jefferson Lab,…Peter Pauli·Dec 10, 2021SaveLearn
Evidence for WW/WZ vector boson scattering in the decay channel produced in association with two jets in proton-proton collisions at s = 13 TeVEvidence is reported for electroweak (EW) vector boson scattering in the decay channel of two weak vector bosons WV (V = W or Z), produced in association with two parton jets. The search…CMS Collaboration·Dec 10, 2021SaveLearn