Universita di Perugia
The NA62 experiment reports the branching ratio measurement BR$(K^+ \rightarrow \pi^+ \nu\bar{\nu}) = (10.6^{+4.0}_{-3.4} |_{\rm stat} \pm 0.9_{\rm syst}) \times 10 ^{-11}$ at 68% CL, based on the observation of 20 signal candidates with an expected background of 7.0 events from the total data sample collected at the CERN SPS during 2016-2018. This provides evidence for the very rare K+π+ννˉK^+ \rightarrow \pi^+ \nu\bar{\nu} decay, observed with a significance of 3.4σ\sigma. The experiment achieves a single event sensitivity of (0.839±0.054)×1011(0.839\pm 0.054)\times 10^{-11}, corresponding to 10.0 events assuming the Standard Model branching ratio of (8.4±1.0)×1011(8.4\pm1.0)\times10^{-11}. This measurement is also used to set limits on BR(K+π+XK^+ \to \pi^+ X), where XX is a scalar or pseudo-scalar particle. Details are given of the analysis of the 2018 data sample, which corresponds to about 80% of the total data sample.
Binary-black-hole (BBH) mergers can take place close to a supermassive black hole (SMBH) while being in a bound orbit around the SMBH. In this paper, we study such bound triple systems and show that including the strong gravity effects of describing the SMBH with a Kerr metric can significantly modify the dynamics, as compared to a Newtonian point particle description of the SMBH. We extract the dynamics of the system, using a quadrupole approximation to the tidal forces due to the SMBH. We exhibit how the gyroscope precession is built into this dynamics, and find the secular Hamiltonian by both averaging over the inner and outer orbits, the latter being the orbit of the BBH around the SMBH. We study the long-time-scale dynamics, including the periastron precession and GW radiation-reaction of the binary system, finding that the strong gravity effects of the SMBH can enhance the von Zeipel-Lidov-Kozai mechanism, resulting in more cycles, higher maximum eccentricity, and thereby a shorter merger time, particularly when the binary is close to, or at, the innermost stable orbit of the SMBH. We end with an analysis of the peak frequency of the GW emission from the binary system, highlighting possible observable signatures in the LISA and ET frequency bands.
We study e+e- --> pi+pi-h_c at center-of-mass energies from 3.90 GeV to 4.42 GeV using data samples collected with the BESIII detector operating at the Beijing Electron Positron Collider. The Born cross sections are measured at 13 energies, and are found to be of the same order of magnitude as those of e+e- --> pi+pi-J/psi but with a different line shape. In the \pi^\pm h_c mass spectrum, a distinct structure, referred to as Z_c(4020), is observed at 4.02 GeV/c^2. The Z_c(4020) carries an electric charge and couples to charmonium. A fit to the \pi^\pm h_c invariant mass spectrum, neglecting possible interferences, results in a mass of (4022.9\pm 0.8\pm 2.7) MeV/c^2 and a width of (7.9\pm 2.7\pm 2.6) MeV for the Z_c(4020), where the first errors are statistical and the second systematic. No significant Z_c(3900) signal is observed, and upper limits on the Z_c(3900) production cross sections in \pi^\pm h_c at center-of-mass energies of 4.23 and 4.26 GeV are set.
University of MississippiUniversity of CincinnatiCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of Cambridge logoUniversity of CambridgeMonash University logoMonash UniversityNational Astronomical Observatory of JapanVanderbilt UniversityUniversita di PisaUniversity of Southern California logoUniversity of Southern CaliforniaNikhefGeorgia Institute of Technology logoGeorgia Institute of TechnologyUniversity of Science and Technology of China logoUniversity of Science and Technology of ChinaStanford University logoStanford UniversityUniversity of WarsawUniversity of British Columbia logoUniversity of British ColumbiaUniversita di PerugiaNorthwestern University logoNorthwestern UniversityUniversity of Texas at Austin logoUniversity of Texas at AustinUniversit‘a di Napoli Federico IIUniversity of Florida logoUniversity of FloridaINFN Sezione di PisaRutherford Appleton LaboratoryUniversity of Minnesota logoUniversity of MinnesotaUniversity of Maryland logoUniversity of MarylandThe Australian National UniversityUniversity of Tokyo logoUniversity of TokyoThe Pennsylvania State University logoThe Pennsylvania State UniversityGran Sasso Science InstituteUniversity of Massachusetts AmherstUniversity of RochesterUniversity of Western AustraliaUniversity of SheffieldCardiff UniversityUniversity of GlasgowUniversit`a degli Studi di PadovaUniversity of PortsmouthSyracuse UniversityUniversity of SannioTexas Tech UniversityUniversity of BirminghamWashington State UniversityUniversity of OregonNational Tsing-Hua UniversityUniversity of AdelaideUniversite Libre de BruxellesMissouri University of Science and TechnologyUniversit\"at HamburgUniversity of California, Santa Cruz logoUniversity of California, Santa CruzUniversitat de ValenciaVirgoLIGOUniversity of Massachusetts DartmouthUniversit`a di FirenzeInstitut d'Astrophysique de ParisUniversity of the Balearic IslandsUniversity of MontanaUniversit`a di TrentoUniversit`a di RomaUniversit`a di Roma Tor VergataUniversite de LyonUniversit`a di CamerinoLeibniz Universit\"at HannoverUniversit´e de MontpellierUniversit´e de NiceUniversit\"a di SassariUniversit´a di Milano-BicoccaUniversité Paris-SaclayUniversită di GenovaUniversita' di SienaUniversita di Roma ‘La Sapienza’
The second Gravitational-Wave Transient Catalog reported on 39 compact binary coalescences observed by the Advanced LIGO and Advanced Virgo detectors between 1 April 2019 15:00 UTC and 1 October 2019 15:00 UTC. We present GWTC-2.1, which reports on a deeper list of candidate events observed over the same period. We analyze the final version of the strain data over this period with improved calibration and better subtraction of excess noise, which has been publicly released. We employ three matched-filter search pipelines for candidate identification, and estimate the astrophysical probability for each candidate event. While GWTC-2 used a false alarm rate threshold of 2 per year, we include in GWTC-2.1, 1201 candidates that pass a false alarm rate threshold of 2 per day. We calculate the source properties of a subset of 44 high-significance candidates that have an astrophysical probability greater than 0.5. Of these candidates, 36 have been reported in GWTC-2. If the 8 additional high-significance candidates presented here are astrophysical, the mass range of events that are unambiguously identified as binary black holes (both objects 3M\geq 3M_\odot) is increased compared to GWTC-2, with total masses from $\sim 14 M_\odotforGW190924021846to for GW190924_021846 to \sim 182 M_\odot$ for GW190426_190642. The primary components of two new candidate events (GW190403_051519 and GW190426_190642) fall in the mass gap predicted by pair instability supernova theory. We also expand the population of binaries with significantly asymmetric mass ratios reported in GWTC-2 by an additional two events (the mass ratio is less than 0.650.65 and 0.440.44 at 90%90\% probability for GW190403_051519 and GW190917_114630 respectively), and find that 2 of the 8 new events have effective inspiral spins \chi_\mathrm{eff} > 0 (at 90%90\% credibility), while no binary is consistent with \chi_\mathrm{eff} < 0 at the same significance.
The Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose, large size, liquid scintillator experiment under construction in China. JUNO will perform leading measurements detecting neutrinos from different sources (reactor, terrestrial and astrophysical neutrinos) covering a wide energy range (from 200 keV to several GeV). This paper focuses on the design and development of a test protocol for the 20-inch PMT underwater readout electronics, performed in parallel to the mass production line. In a time period of about ten months, a total number of 6950 electronic boards were tested with an acceptance yield of 99.1%.
CNRS logoCNRSUniversity of MississippiUniversity of CincinnatiCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of VictoriaINFN Sezione di NapoliSLAC National Accelerator LaboratoryHarvard University logoHarvard UniversityVanderbilt UniversityCarnegie Mellon University logoCarnegie Mellon UniversityImperial College London logoImperial College LondonUniversita di PisaUniversity of Manchester logoUniversity of ManchesterUniversity of Notre Dame logoUniversity of Notre DameUC Berkeley logoUC BerkeleyNikhefStanford University logoStanford UniversityUniversity of Bristol logoUniversity of BristolUniversity of EdinburghINFN logoINFNOhio State UniversityMcGill University logoMcGill UniversityUniversity of British Columbia logoUniversity of British ColumbiaUniversita di PerugiaYale University logoYale UniversityUniversity of WisconsinUniversity of Texas at Austin logoUniversity of Texas at AustinUniversit‘a di Napoli Federico IISouthern Methodist UniversityINFN Sezione di PisaRutherford Appleton LaboratoryUniversity of Pennsylvania logoUniversity of PennsylvaniaJohns Hopkins University logoJohns Hopkins UniversityUniversity of Maryland logoUniversity of MarylandColorado State UniversityUniversity of ColoradoLawrence Berkeley National Laboratory logoLawrence Berkeley National LaboratoryPurdue University logoPurdue UniversityUniversity of LiverpoolUniversity of IowaMIT logoMITCEA logoCEAPrinceton University logoPrinceton UniversityQueen Mary University of London logoQueen Mary University of LondonUniversity of Warwick logoUniversity of WarwickUniversitat de BarcelonaUniversity of Texas at DallasIowa State UniversityUniversity of LouisvilleUniversity of California at Los AngelesMount Holyoke CollegeUniversity of New MexicoUniversity of BirminghamUniversity of TennesseeUniversity of South CarolinaUniversity of OregonLaboratori Nazionali di FrascatiUniversity of BergenUniversity of MassachusettsBrunel UniversityLawrence Livermore National LaboratoryUniversity of Puerto RicoINFN, Sezione di TorinoBudker Institute of Nuclear PhysicsUniversity of California, Santa Cruz logoUniversity of California, Santa CruzIN2P3INFN, Sezione di MilanoUniversit`a di TorinoINFN Sezione di PerugiaINFN - Sezione di PadovaProvidence CollegeINFN-Sezione di GenovaUniversit`a di Roma TreLaboratoire Leprince-RinguetINFN Sezione di RomaUniversity of California at IrvineUniversity of California at Santa BarbaraUniversity of California at RiversideINFN Sezione di Roma 2University of California at San DiegoUniversite de MontrealUniversit`a di Roma Tor VergataUniversit`a di TriesteUniversit`a di BariTechnische Universitat DresdenState University of New York, Stony BrookUniversit´e Paris DiderotLaboratoire de l'Accelerateur LineaireLaboratoire de Physique Nucleaire et de Hautes EnergiesLaboratoire d’Annecy-le-Vieux de Physique des ParticulesState University of New York, AlbanyRuhr-Universitat BochumLaboratoire APCRoyal Holloway and Bedford New CollegeUniversitat DortmundINFN (Sezione di Bari)INFN Sezione di UdineUniversit’e Paris-Sud 11Universit´a di UdineINFN Sezione di Roma 3Forschungszentrum GarchingUniversität KarlsruheUniversità di FerraraLudwig-Maximilians-Universität MünchenINFN-Sezione di FerraraUniversitȁt HeidelbergUniversite Paris-VIUniversită di GenovaUniversit de SavoieUniversita di Milano`Ecole PolytechniqueUniversita di Roma ‘La Sapienza’Universita' di PadovaINFN Sezione di Trieste
We report on an improved measurement of the Cabibbo-Kobayashi-Maskawa {\it CP}-violating phase γ\gamma through a Dalitz plot analysis of neutral DD meson decays to KS0π+πK_S^0 \pi^+ \pi^- and KS0K+KK_S^0 K^+ K^- in the processes BDKB^\mp \to D K^\mp, BDKB^\mp \to D^* K^\mp with DDπ0,DγD^* \to D\pi^0,D\gamma, and BDKB^\mp \to D K^{*\mp} with KKS0πK^{*\mp} \to K_S^0 \pi^\mp. Using a sample of 383 million BBˉB\bar{B} pairs collected by the BABAR detector, we measure γ=(76±22±5±5)\gamma=(76 \pm 22 \pm 5 \pm 5)^\circ (mod 180180^\circ), where the first error is statistical, the second is the experimental systematic uncertainty and the third reflects the uncertainty on the description of the Dalitz plot distributions. The corresponding two standard deviation region is 29^\circ < \gamma < 122^\circ. This result has a significance of direct {\it CP} violation (γ0\gamma \ne 0) of 3.0 standard deviations.
A search for the K+π+XK^{+}\rightarrow\pi^{+}X decay, where XX is a long-lived feebly interacting particle, is performed through an interpretation of the K+π+ννˉK^{+}\rightarrow\pi^{+}\nu\bar{\nu} analysis of data collected in 2017 by the NA62 experiment at CERN. Two ranges of XX masses, 00-110MeV/c2110\,\text{MeV}/c^{2} and 154154-260MeV/c2260\,\text{MeV}/c^{2}, and lifetimes above 100ps100\,\text{ps} are considered. The limits set on the branching ratio, BR(K+π+X)\text{BR}(K^{+}\rightarrow\pi^{+}X), are competitive with previously reported searches in the first mass range, and improve on current limits in the second mass range by more than an order of magnitude.
We find the exact solution for a finite size Giant Magnon in the SU(2)×SU(2)SU(2)\times SU(2) sector of the string dual of the N=6\mathcal{N}=6 superconformal Chern-Simons theory recently constructed by Aharony, Bergman, Jafferis and Maldacena. The finite size Giant Magnon solution consists of two magnons, one in each SU(2)SU(2). In the infinite size limit this solution corresponds to the Giant Magnon solution of arXiv:0806.4959. The magnon dispersion relation exhibits finite-size exponential corrections with respect to the infinite size limit solution.
A search for heavy neutral lepton (NN) production in K+e+NK^+\to e^+N decays using the data sample collected by the NA62 experiment at CERN in 2017--2018 is reported. Upper limits of the extended neutrino mixing matrix element Ue42|U_{e4}|^2 are established at the level of 10910^{-9} over most of the accessible heavy neutral lepton mass range 144--462 MeV/c2c^2, with the assumption that the lifetime exceeds 50 ns. These limits improve significantly upon those of previous production and decay searches. The Ue42|U_{e4}|^2 range favoured by Big Bang Nucleosynthesis is excluded up to a mass of about 340 MeV/c2c^2.
A sample of 1.69×1071.69\times 10^7 fully reconstructed π0γe+e\pi^0\to\gamma e^+e^- decay candidates collected by the NA48/2 experiment at CERN in 2003--2004 is analysed to search for the dark photon (AA') production in the $\pi^0\to\gamma A'decayfollowedbytheprompt decay followed by the prompt A'\to e^+e^-$ decay. No signal is observed, and an exclusion region in the plane of the dark photon mass mAm_{A'} and mixing parameter ε2\varepsilon^2 is established. The obtained upper limits on ε2\varepsilon^2 are more stringent than the previous limits in the mass range $9~{\rm MeV}/c^2
The Jiangmen Underground Neutrino Observatory (JUNO) is a large neutrino detector currently under construction in China. Thanks to the tight requirements on its optical and radio-purity properties, it will be able to perform leading measurements detecting terrestrial and astrophysical neutrinos in a wide energy range from tens of keV to hundreds of MeV. A key requirement for the success of the experiment is an unprecedented 3% energy resolution, guaranteed by its large active mass (20 kton) and the use of more than 20,000 20-inch photo-multiplier tubes (PMTs) acquired by high-speed, high-resolution sampling electronics located very close to the PMTs. As the Front-End and Read-Out electronics is expected to continuously run underwater for 30 years, a reliable readout acquisition system capable of handling the timestamped data stream coming from the Large-PMTs and permitting to simultaneously monitor and operate remotely the inaccessible electronics had to be developed. In this contribution, the firmware and hardware implementation of the IPbus based readout protocol will be presented, together with the performances measured on final modules during the mass production of the electronics.
The Jiangmen Underground Neutrino Observatory (JUNO) is a large neutrino detector currently under construction in China. JUNO will be able to study the neutrino mass ordering and to perform leading measurements detecting terrestrial and astrophysical neutrinos in a wide energy range, spanning from 200 keV to several GeV. Given the ambitious physics goals of JUNO, the electronic system has to meet specific tight requirements, and a thorough characterization is required. The present paper describes the tests performed on the readout modules to measure their performances.
University of MississippiUniversity of CincinnatiTechnische Universitat DortmundCalifornia Institute of Technology logoCalifornia Institute of TechnologyINFN Sezione di NapoliSLAC National Accelerator LaboratoryHarvard University logoHarvard UniversityImperial College London logoImperial College LondonUniversita di PisaUniversity of Manchester logoUniversity of ManchesterUniversity of Notre Dame logoUniversity of Notre DameUC Berkeley logoUC BerkeleyNikhefUniversity of EdinburghOhio State UniversityMcGill University logoMcGill UniversityUniversity of British Columbia logoUniversity of British ColumbiaUniversita di PerugiaUniversit‘a di Napoli Federico IIINFN Sezione di PisaRutherford Appleton LaboratoryJohns Hopkins University logoJohns Hopkins UniversityUniversity of Maryland logoUniversity of MarylandColorado State UniversityUniversity of ColoradoLawrence Berkeley National Laboratory logoLawrence Berkeley National LaboratoryUniversity of LiverpoolUniversity of IowaMIT logoMITCEA logoCEAPrinceton University logoPrinceton UniversityNovosibirsk State UniversityQueen Mary University of London logoQueen Mary University of LondonICREAIowa State UniversityUniversity of LouisvilleUniversitat Aut`onoma de BarcelonaUniversity of OregonRoyal Holloway, University of LondonUniversity of BergenUniversity of MassachusettsBrunel UniversityLawrence Livermore National LaboratoryIndian Institute of Technology GuwahatiBudker Institute of Nuclear PhysicsUniversity of California, Santa Cruz logoUniversity of California, Santa CruzINFN, Sezione di MilanoINFN Sezione di PerugiaLAPPINFN - Sezione di PadovaScuola Normale Superiore di PisaINFN-Sezione di GenovaINFN Sezione di RomaHarvey Mudd CollegeUniversity of California at IrvineUniversity of California at Santa BarbaraUniversity of California at RiversideHumboldt-Universitat zu BerlinUniversite de MontrealUniversit`a di BariLaboratori Nazionali di Frascati dell’INFNTechnische Universitat DresdenLaboratoire de l'Accelerateur LineaireJohannes Gutenberg Universit\"at MainzRuhr-Universitat BochumUniversitat RostockINFN (Sezione di Bari)Laboratoire d'Annecy-le-Vieux de Physique des Particules (LAPP)Universit´e Pierre et Marie Curie-Paris6Universit´e Denis Diderot-Paris7Università di FerraraINFN-Sezione di FerraraUniversitȁt HeidelbergUniversită di GenovaUniversit de SavoieUniversita di Milano`Ecole PolytechniqueUniversita di Roma ‘La Sapienza’Universita' di Padova
Based on the full BaBar data sample, we report improved measurements of the ratios R(D(*)) = B(B -> D(*) Tau Nu)/B(B -> D(*) l Nu), where l is either e or mu. These ratios are sensitive to new physics contributions in the form of a charged Higgs boson. We measure R(D) = 0.440 +- 0.058 +- 0.042 and R(D*) = 0.332 +- 0.024 +- 0.018, which exceed the Standard Model expectations by 2.0 sigma and 2.7 sigma, respectively. Taken together, our results disagree with these expectations at the 3.4 sigma level. This excess cannot be explained by a charged Higgs boson in the type II two-Higgs-doublet model. We also report the observation of the decay B -> D Tau Nu, with a significance of 6.8 sigma.
We find the exact solution for a finite size Giant Magnon in the SU(2)×SU(2)SU(2)\times SU(2) sector of the string dual of the N=6\mathcal{N}=6 superconformal Chern-Simons theory recently constructed by Aharony, Bergman, Jafferis and Maldacena. The finite size Giant Magnon solution consists of two magnons, one in each SU(2)SU(2). In the infinite size limit this solution corresponds to the Giant Magnon solution of arXiv:0806.4959. The magnon dispersion relation exhibits finite-size exponential corrections with respect to the infinite size limit solution.
University of MississippiUniversity of CincinnatiCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of Pittsburgh logoUniversity of PittsburghINFN Sezione di NapoliSLAC National Accelerator LaboratoryHarvard University logoHarvard UniversityImperial College London logoImperial College LondonUniversita di PisaUniversity of Manchester logoUniversity of ManchesterUniversity of Notre Dame logoUniversity of Notre DameUC Berkeley logoUC BerkeleyNikhefOhio State UniversityMcGill University logoMcGill UniversityUniversity of British Columbia logoUniversity of British ColumbiaUniversita di PerugiaUniversit‘a di Napoli Federico IIUniversity of Florida logoUniversity of FloridaINFN Sezione di PisaRutherford Appleton LaboratoryJohns Hopkins University logoJohns Hopkins UniversityUniversity of Maryland logoUniversity of MarylandColorado State UniversityUniversity of ColoradoLawrence Berkeley National Laboratory logoLawrence Berkeley National LaboratoryUniversity of LiverpoolUniversity of Massachusetts AmherstUniversity of IowaMIT logoMITCEA logoCEANovosibirsk State UniversityQueen Mary University of London logoQueen Mary University of LondonUniversitat de BarcelonaTU DortmundIowa State UniversityDalhousie UniversityUniversity of OregonUniversity of BergenLawrence Livermore National LaboratoryIndian Institute of Technology GuwahatiBudker Institute of Nuclear PhysicsINFN, Laboratori Nazionali di FrascatiUniversity of California, Santa Cruz logoUniversity of California, Santa CruzINFN, Sezione di MilanoINFN Sezione di PerugiaCNRS/IN2P3LAPPINFN - Sezione di PadovaScuola Normale Superiore di PisaINFN-Sezione di GenovaLaboratoire Leprince-RinguetINFN Sezione di RomaHarvey Mudd CollegeUniversity of California at IrvineUniversity of Southern MississippiUniversity of California at Santa BarbaraHumboldt-Universitat zu BerlinUniversit`a di BariTechnische Universitat DresdenUniversit´e Paris DiderotLaboratoire de l'Accelerateur LineaireLaboratoire de Physique Nucleaire et de Hautes EnergiesJohannes Gutenberg Universit\"at MainzRuhr-Universitat BochumUniversitat RostockINFN (Sezione di Bari)Laboratoire d'Annecy-le-Vieux de Physique des Particules (LAPP)Universit’e Paris-Sud 11Universite´ Pierre et Marie CurieUniversità di FerraraINFN-Sezione di FerraraUniversitȁt HeidelbergUniversită di GenovaUniversit de SavoieUniversita di Milano`Ecole PolytechniqueUniversita di Roma ‘La Sapienza’Universita' di Padova
Based on the full BaBar data sample, we report improved measurements of the ratios R(D(*)) = B(B -> D(*) Tau Nu)/B(B -> D(*) l Nu), where l is either e or mu. These ratios are sensitive to new physics contributions in the form of a charged Higgs boson. We measure R(D) = 0.440 +- 0.058 +- 0.042 and R(D*) = 0.332 +- 0.024 +- 0.018, which exceed the Standard Model expectations by 2.0 sigma and 2.7 sigma, respectively. Taken together, our results disagree with these expectations at the 3.4 sigma level. This excess cannot be explained by a charged Higgs boson in the type II two-Higgs-doublet model. We also report the observation of the decay B -> D Tau Nu, with a significance of 6.8 sigma.
Institute for Computational and Data SciencesCNRS logoCNRSAcademia SinicaUniversity of Cambridge logoUniversity of CambridgeMonash University logoMonash UniversityNational Central UniversityUniversita di PisaUniversity of Chicago logoUniversity of ChicagoNikhefGeorgia Institute of Technology logoGeorgia Institute of Technologythe University of Tokyo logothe University of TokyoPusan National UniversityStanford University logoStanford UniversityUniversity of Bristol logoUniversity of BristolUniversity of Copenhagen logoUniversity of CopenhagenThe Chinese University of Hong Kong logoThe Chinese University of Hong KongUniversity of MelbourneINFN logoINFNUniversity of WarsawUniversita di PerugiaNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterLouisiana State UniversityInternational Centre for Theoretical Sciences, Tata Institute of Fundamental ResearchUniversit‘a di Napoli Federico IIUniversity of Florida logoUniversity of FloridaUniversity of Minnesota logoUniversity of MinnesotaUniversity of Maryland logoUniversity of MarylandSeoul National University logoSeoul National UniversityNational Taiwan Normal UniversityThe Pennsylvania State University logoThe Pennsylvania State UniversityRochester Institute of TechnologyChennai Mathematical InstituteKing’s College London logoKing’s College LondonIndian Institute of Technology, BombayScuola Superiore MeridionaleNational Changhua University of EducationCharles Sturt UniversityAustralian National University logoAustralian National UniversityUniversity of Western AustraliaUniversity of GlasgowHigh Energy Accelerator Research Organization (KEK)The Graduate University for Advanced Studies (SOKENDAI)Universit`a degli Studi di GenovaWigner Research Centre for PhysicsUniversity of Alabama in HuntsvilleSyracuse UniversityNicolaus Copernicus Astronomical Center, Polish Academy of SciencesObservatoire de ParisInstituto Nacional de Pesquisas EspaciaisIndian Institute of Technology DelhiUniversitat de les Illes BalearsLomonosov Moscow State UniversitySouthwest Jiaotong UniversityUniversity of BirminghamNational Cheng Kung UniversityColl`ege de FranceNiels Bohr InstituteWashington State UniversityINFN, Laboratori Nazionali del Gran SassoGran Sasso Science Institute (GSSI)University of OregonCalifornia State University, FullertonNational Tsing-Hua UniversityBar Ilan UniversityUniversity of AdelaideUniversite Libre de BruxellesIndian Institute of Technology GandhinagarUniversit`a di BolognaMax Planck Institute for Gravitational Physics (Albert Einstein Institute)Universite catholique de LouvainUniversitat de ValenciaResonac CorporationInstitute for Plasma ResearchInter-University Centre for Astronomy and AstrophysicsWest Virginia UniversityCNR-SPINInstituto de Astrofísica de AndalucíaObservatoire de la Cˆote d’AzurIJCLabLaboratoire Kastler BrosselUniversity of ToyamaUniversit`a di Roma TreLaboratoire Charles CoulombUniversity of SzegedUniversity of Wisconsin–MilwaukeeNational Synchrotron Radiation Research CenterKorea Institute of Science and Technology InformationUniversite de StrasbourgLIGO Hanford ObservatoryUniversit‘a di SalernoLIGO, California Institute of TechnologyUniversit\'e C\^ote d'AzurLUTHThe University of Texas Rio Grande ValleyNational Astronomical Observatory of Japan (NAOJ)National Institute for Mathematical SciencesLIGO Livingston ObservatoryIP2I LyonLeibniz Universit\"at HannoverUniversit´e de MontpellierUniversit\`a degli Studi di Urbino ‘Carlo Bo’Laboratoire de l'Accelerateur LineaireUniversit`e de Li`egeLaboratoire de Physique des 2 Infinis Ir`ene Joliot-CurieInstitut FOTONUniversit`a degli Studi di UdineEuropean Gravitational Observatory (EGO)Inje UniversityUniversite du Littoral - Cote d’OpaleLaboratoire d’Annecy de Physique des Particules (LAPP)Universit`a della Campania “Luigi Vanvitelli”Universit´e Paris Cit´eIPHC UMR 7178Key Laboratory of Quantum Optics and Quantum InformationUniversit`a di Cassino e del Lazio MeridionaleUniversit`a degli Studi di SannioCentre Scientifique et Technique du BˆatimentDirectorate of Knowledge Management in Healthcare, Sree Chitra Tirunal Institute for Medical Sciences and TechnologyInstitute for Astronomical ScienceUniversit´e Claude Bernard (Lyon 1)Friedrich-Schiller-Universität JenaÉ́cole normale supérieureUniversita di ParmaUniversité Paris-SaclayUniversită di CagliariUniversità degli Studi di Napoli “Parthenope”Universita' di SienaUniv-RennesINAF Osservatorio Astronomico di PadovaUniversita di Roma ‘La Sapienza’Universita' di PadovaUniversité PSLSorbonne Université
We search for gravitational-wave signals associated with gamma-ray bursts detected by the Fermi and Swift satellites during the second half of the third observing run of Advanced LIGO and Advanced Virgo (1 November 2019 15:00 UTC-27 March 2020 17:00 UTC).We conduct two independent searches: a generic gravitational-wave transients search to analyze 86 gamma-ray bursts and an analysis to target binary mergers with at least one neutron star as short gamma-ray burst progenitors for 17 events. We find no significant evidence for gravitational-wave signals associated with any of these gamma-ray bursts. A weighted binomial test of the combined results finds no evidence for sub-threshold gravitational wave signals associated with this GRB ensemble either. We use several source types and signal morphologies during the searches, resulting in lower bounds on the estimated distance to each gamma-ray burst. Finally, we constrain the population of low luminosity short gamma-ray bursts using results from the first to the third observing runs of Advanced LIGO and Advanced Virgo. The resulting population is in accordance with the local binary neutron star merger rate.
This proceedings contains our considerations made during and after fruitful discussions held at EuCAIFCon 2025. We explore the use of deep reinforcement learning for autonomous locking of Fabry-Perot optical cavities in non-linear regimes, with relevance to gravitational-wave detectors. A custom Gymnasium environment with a time-domain simulator enabled training of agents such as deep deterministic policy gradient, achieving reliable lock acquisition for both low- and high-finesse cavities, including Virgo-like parameters. We also discuss possible improvements with Twin Delayed DDPG, Soft Actor Critic and meta-reinforcement learning, as well as strategies for low-latency execution and off-line policy updates to address hardware limitations. These studies lay the groundwork for future deployment of reinforcement learning-based control in real optical setups.
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The LIGO detection of the gravitational wave transient GW150914, from the inspiral and merger of two black holes with masses $\gtrsim 30\, \text{M}_\odot$, suggests a population of binary black holes with relatively high mass. This observation implies that the stochastic gravitational-wave background from binary black holes, created from the incoherent superposition of all the merging binaries in the Universe, could be higher than previously expected. Using the properties of GW150914, we estimate the energy density of such a background from binary black holes. In the most sensitive part of the Advanced LIGO/Virgo band for stochastic backgrounds (near 25 Hz), we predict ΩGW(f=25Hz)=1.10.9+2.7×109\Omega_\text{GW}(f=25 Hz) = 1.1_{-0.9}^{+2.7} \times 10^{-9} with 90\% confidence. This prediction is robustly demonstrated for a variety of formation scenarios with different parameters. The differences between models are small compared to the statistical uncertainty arising from the currently poorly constrained local coalescence rate. We conclude that this background is potentially measurable by the Advanced LIGO/Virgo detectors operating at their projected final sensitivity.
Complex organic molecules have been observed for decades in the interstellar medium. Some of them might be considered as small bricks of the macromolecules at the base of terrestrial life. It is hence particularly important to understand organic chemistry in Solar-like star forming regions. In this article, we present a new observational project: SOLIS (Seeds Of Life In Space). This is a Large Project at the IRAM-NOEMA interferometer, and its scope is to image the emission of several crucial organic molecules in a sample of Solar-like star forming regions in different evolutionary stage and environments. Here, we report the first SOLIS results, obtained from analysing the spectra of different regions of the Class 0 source NGC1333-IRAS4A, the protocluster OMC-2 FIR4, and the shock site L1157-B1. The different regions were identified based on the images of formamide (NH2CHO) and cyanodiacetylene (HC5N) lines. We discuss the observed large diversity in the molecular and organic content, both on large (3000-10000 au) and relatively small (300-1000 au) scales. Finally, we derive upper limits to the methoxy fractional abundance in the three observed regions of the same order of magnitude of that measured in few cold prestellar objects, namely ~10^-12-10^-11 with respect to H2 molecules.
A sample of 3120 K±π±μ+μK^\pm\to\pi^\pm\mu^+\mu^- decay candidates with (3.3±0.7)(3.3\pm0.7)% background contamination has been collected by the NA48/2 experiment at the CERN SPS, allowing a detailed study of the decay properties. The branching ratio was measured to be BR=(9.62±0.25)×108{\rm BR}=(9.62\pm0.25)\times 10^{-8}. The form factor W(z)W(z), where z=(Mμμ/MK)2z=(M_{\mu\mu}/M_K)^2, was parameterized according to several models. In particular, the slope of the linear form factor W(z)=W0(1+δz)W(z)=W_0(1+\delta z) was measured to be δ=3.11±0.57\delta=3.11\pm0.57. Upper limits of 2.9×1022.9\times 10^{-2} and 2.3×1022.3\times 10^{-2} on possible charge asymmetry and forward-backward asymmetry were established at 90% CL. An upper limit {\rm BR}(K^\pm\to\pi^\mp\mu^\pm\mu^\pm)<1.1\times 10^{-9} was established at 90% CL for the rate of the lepton number violating decay.
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