Max Planck Institute for Nuclear Physics
The effective electron neutrino mass can be determined by analyzing the endpoint region of the 163^{163}Ho electron capture spectrum, provided a measurement with high energy resolution and high statistics using calorimetric techniques. Here, the Electron Capture in 163^{163}Ho collaboration, ECHo, presents an analysis of the most precise 163^{163}Ho spectrum currently available, obtained with the ECHo-1k experiment and comprising about 200 million events. A very low background rate of B=9.1(1.3)×106B=9.1(1.3)\times 10^{-6} /eV/pixel/day was achieved allowing for a reliable analysis of the endpoint region. The derived endpoint energy Q=2862(4)Q = 2862(4) eV is in excellent agreement with the one independently determined via Penning-trap mass spectrometry of Q=2863.2(6)Q=2863.2(6) eV [1]. The upper limit of the effective electron neutrino mass is improved by almost a factor 2 compared to the lowest current value [2], reaching m_{\nu_\mathrm{e}} < 15 eV/c2{^2} (90\% credible interval).
The influence of extraterrestrial particles like cosmic radiation (CR) on the chemistry and ozone density in the Earth stratosphere is not well investigated and normally neglected in stratospheric chemistry models. Here we present the commissioning of a lab-based apparatus which aims at simulating conditions in the stratosphere in order to get better insight into the reactions induced by the secondary-particle showers from high-energetic CR which can reach low altitudes. Admixtures of ozone and the halocarbon CHClF2 (R22, chlorodifluoromethane) to atmospheric gases (N2, O2, Ar) were exposed to a glow discharge in the total pressure regime of a few hPa. According to the mass spectrometric analysis of the gas composition the discharge initiates significant ozone depletion by a factor four in the absence of R22. This depletion is strongly enhanced to two orders of magnitude in the presence of R22. The possible underlying reactions are discussed.
We report observations of the ultra-high-energy gamma-ray source LHAASO J2108++5157, utilizing VERITAS, HAWC, Fermi-LAT, and XMM-Newton. VERITAS has collected \sim 40 hours of data that we used to set ULs to the emission above 200 GeV. The HAWC data, collected over 2400\sim 2400 days, reveal emission between 3 and 146 TeV, with a significance of 7.5 σ7.5~\sigma, favoring an extended source model. The best-fit spectrum measured by HAWC is characterized by a simple power-law with a spectral index of 2.45±0.11stat2.45\pm0.11_{stat}. Fermi-LAT analysis finds a point source with a very soft spectrum in the LHAASO J2108+5157 region, consistent with the 4FGL-DR3 catalog results. The XMM-Newton analysis yields a null detection of the source in the 2 - 7 keV band. The broadband spectrum can be interpreted as a pulsar and a pulsar wind nebula system, where the GeV gamma-ray emission originates from an unidentified pulsar, and the X-ray and TeV emission is attributed to synchrotron radiation and inverse Compton scattering of electrons accelerated within a pulsar wind nebula. In this leptonic scenario, our X-ray upper limit provides a stringent constraint on the magnetic field, which is 1.5 μ\lesssim 1.5\ \muG.
University of Illinois at Urbana-Champaign logoUniversity of Illinois at Urbana-ChampaignUniversity of Pittsburgh logoUniversity of PittsburghUniversity of California, Santa Barbara logoUniversity of California, Santa BarbaraSLAC National Accelerator LaboratoryHarvard University logoHarvard UniversityImperial College London logoImperial College LondonUniversity of OklahomaDESYUniversity of Manchester logoUniversity of ManchesterUniversity of ZurichUniversity of BernUC Berkeley logoUC BerkeleyUniversity of Oxford logoUniversity of OxfordNikhefIndiana UniversityPusan National UniversityScuola Normale SuperioreCornell University logoCornell UniversityUniversity of California, San Diego logoUniversity of California, San DiegoNorthwestern University logoNorthwestern UniversityUniversity of GranadaCERN logoCERNArgonne National Laboratory logoArgonne National LaboratoryFlorida State UniversitySeoul National University logoSeoul National UniversityHuazhong University of Science and Technology logoHuazhong University of Science and TechnologyUniversity of Wisconsin-Madison logoUniversity of Wisconsin-MadisonUniversity of PisaLawrence Berkeley National Laboratory logoLawrence Berkeley National LaboratoryPolitecnico di MilanoUniversity of LiverpoolUniversity of IowaDuke University logoDuke UniversityUniversity of GenevaUniversity of GlasgowUniversity of Warwick logoUniversity of WarwickIowa State UniversityKarlsruhe Institute of Technology logoKarlsruhe Institute of TechnologyUniversità di Milano-BicoccaTechnische Universität MünchenOld Dominion UniversityTexas Tech UniversityDurham University logoDurham UniversityNiels Bohr InstituteCzech Technical University in PragueUniversity of OregonUniversity of AlabamaSTFC Rutherford Appleton LaboratoryLawrence Livermore National LaboratoryUniversity of California, Santa Cruz logoUniversity of California, Santa CruzUniversity of SarajevoJefferson LabTOBB University of Economics and TechnologyUniversity of California RiversideUniversity of HuddersfieldCEA SaclayRadboud University NijmegenUniversitá degli Studi dell’InsubriaHumboldt University BerlinINFN Milano-BicoccaUniversità degli Studi di BresciaIIT GuwahatiDaresbury LaboratoryINFN - PadovaINFN MilanoUniversità degli Studi di BariCockcroft InstituteHelwan UniversityINFN-TorinoINFN PisaINFN-BolognaBrookhaven National Laboratory (BNL)INFN Laboratori Nazionali del SudINFN PaviaMax Planck Institute for Nuclear PhysicsINFN TriesteINFN Roma TreINFN GenovaFermi National Accelerator Laboratory (Fermilab)INFN BariINFN-FirenzeINFN FerraraPunjab Agricultural UniversityEuropean Spallation Source (ESS)Fusion for EnergyInternational Institute of Physics (IIP)INFN-Roma La SapienzaUniversit degli Studi di GenovaUniversit di FerraraUniversit degli Studi di PadovaUniversit di Roma La SapienzaRWTH Aachen UniversityUniversit di TorinoSapienza Universit di RomaUniversit degli Studi di FirenzeUniversit degli Studi di TorinoUniversit di PaviaUniversit Di BolognaUniversit degli Studi Roma Tre
This review, by the International Muon Collider Collaboration (IMCC), outlines the scientific case and technological feasibility of a multi-TeV muon collider, demonstrating its potential for unprecedented energy reach and precision measurements in particle physics. It presents a comprehensive conceptual design and R&D roadmap for a collider capable of reaching 10+ TeV center-of-mass energy.
The Nobel prize in physics 2015 has been awarded "... for the discovery of neutrino oscillations which show that neutrinos have mass". While SuperKamiokande (SK), indeed, has discovered oscillations, SNO observed effect of the adiabatic (almost non-oscillatory) flavor conversion of neutrinos in the matter of the Sun. Oscillations are irrelevant for solar neutrinos apart from small νe\nu_e regeneration inside the Earth. Both oscillations and adiabatic conversion do not imply masses uniquely and further studies were required to show that non-zero neutrino masses are behind the SNO results. Phenomena of oscillations (phase effect) and adiabatic conversion (the MSW effect driven by the change of mixing in matter) are described in pedagogical way.
Improving gamma-hadron separation is one of the most effective ways to enhance the performance of ground-based gamma-ray observatories. With over a decade of continuous operation, the High-Altitude Water Cherenkov (HAWC) Observatory has contributed significantly to high-energy astrophysics. To further leverage its rich dataset, we introduce a machine learning approach for gamma-hadron separation. A Multilayer Perceptron shows the best performance, surpassing traditional and other Machine Learning based methods. This approach shows a notable improvement in the detector's sensitivity, supported by results from both simulated and real HAWC data. In particular, it achieves a 19\% increase in significance for the Crab Nebula, commonly used as a benchmark. These improvements highlight the potential of machine learning to significantly enhance the performance of HAWC and provide a valuable reference for ground-based observatories, such as Large High Altitude Air Shower Observatory (LHAASO) and the upcoming Southern Wide-field Gamma-ray Observatory (SWGO).
We find that biorthogonal quantum mechanics with a scalar product that counts both absorbed and emitted particles leads to covariant position operators with localized eigenvectors. In this manifestly covariant formulation the probability for a transition from a one-photon state to a position eigenvector is the first order Glauber correlation function, bridging the gap between photon counting and the sensitivity of light detectors to electromagnetic energy density. The position eigenvalues are identified as the spatial parameters in the canonical quantum field operators and the position basis describes an array of localized devices that instantaneously absorb and re-emit bosons.
Michigan State University logoMichigan State UniversityUniversity of UtahShanghai Jiao Tong University logoShanghai Jiao Tong UniversityStanford University logoStanford UniversityPennsylvania State UniversityUniversity of Maryland logoUniversity of MarylandUniversity of Tokyo logoUniversity of TokyoUniversity of Wisconsin-Madison logoUniversity of Wisconsin-MadisonLos Alamos National LaboratoryUniversity of RochesterUniversity of New MexicoChulalongkorn UniversityMichigan Technological UniversityInstitute of Nuclear Physics, Polish Academy of SciencesUniversidad de GuadalajaraUniversidad Nacional Autonoma de MexicoMax Planck Institute for Nuclear PhysicsUniversidad Politecnica de PachucaNational Astronomical Research Institute of Thailand (Public Organization)Universidad Autonoma de ChiapasBenemerita Universidad Autonoma de PueblaCentro de Investigacion y de Estudios Avanzados del IPNInstituto Politecnico NacionalTsung-Dao Lee Institute & School of Physics and Astronomy, Shanghai Jiao Tong UniversityCalifornia University of PennsylvaniaUniversidad Michoacana de San Nicolas de HidalgoUniversidad Autonoma del Estado de HidalgoInstituto Nacional de Astrofısica Optica y ElectronicaTHOUGHTNatural Science Research Institute, University of SeoulInstituto de F´ısica Corpuscular, CSIC, Universitat de Val`encia1. Department of Physics and Astronomy, University of Utah, Salt Lake City, UT, USA -> University of Utah2. Physics Division, Los Alamos National Laboratory, Los Alamos, NM, USA -> Los Alamos National Laboratory3. Instituto de F´ısica, Universidad Nacional Aut´onoma de M´exico, Ciudad de Mexico, Mexico -> Universidad Nacional Aut´onoma de M´exico4. Universidad Aut´onoma de Chiapas, Tuxtla Guti´errez, Chiapas, M´exico -> Universidad Aut´onoma de Chiapas5. Universidad Michoacana de San Nicol´as de Hidalgo, Morelia, Mexico -> Universidad Michoacana de San Nicol´as de Hidalgo6. Instituto de Geof´ısica, Universidad Nacional Aut´onoma de M´exico, Ciudad de Mexico, Mexico -> Universidad Nacional Aut´onoma de M´exico (already listed)7. Department of Physics, Pennsylvania State University, University Park, PA, USA -> Pennsylvania State University8. Institute of Nuclear Physics Polish Academy of Sciences, PL-31342 IFJ-PAN, Krakow, Poland -> Institute of Nuclear Physics Polish Academy of Sciences9. Department of Physics & Astronomy, University of Rochester, Rochester, NY , USA -> University of Rochester10. Department of Physics, Stanford University: Stanford, CA 94305–4060, USA -> Stanford University11. Department of Physics, University of Maryland, College Park, MD, USA -> University of Maryland12. Instituto Nacional de Astrof´ısica, ´Optica y Electr´onica, Puebla, Mexico -> Instituto Nacional de Astrof´ısica, ´Optica y Electr´onica13. Instituto de Astronom´ıa, Universidad Nacional Aut´onoma de M´exico, Ciudad de Mexico, Mex-ico -> Universidad Nacional Aut´onoma de M´exico (already listed)14. Departamento de F´ısica, Centro Universitario de Ciencias Exactase Ingenierias, Universidad de Guadalajara, Guadalajara, Mexico -> Universidad de Guadalajara15. Institute for Cosmic Ray Research, University of Tokyo: 277-8582 Chiba, Kashiwa, Kashi-wanoha, 5 Chome-1-5 -> University of Tokyo16. Department of Physics, University of Wisconsin-Madison, Madison, WI, USA -> University of Wisconsin-Madison17. Department of Physics, Michigan Technological University, Houghton, MI, USA -> Michigan Technological University18. Max-Planck Institute for Nuclear Physics, 69117 Heidelberg, Germany -> Max-Planck Institute for Nuclear Physics19. Department of Physics, Faculty of Science, Chulalongkorn University, 254 Phayathai Road, Pathumwan, Bangkok 10330, Thailand -> Chulalongkorn University20. National Astronomical Research Institute of Thailand (Public Organization), Don Kaeo, MaeRim, Chiang Mai 50180, Thailand -> National Astronomical Research Institute of Thailand (Public Organization)21. Erlangen Centre for Astroparticle Physics, Friedrich-Alexander-Universit¨at Erlangen-N¨urnberg, Erlangen, Germany -> Friedrich-Alexander-Universit¨at Erlangen-N¨urnberg22. Department of Physics and Astronomy, Michigan State University, East Lansing, MI, USA -> Michigan State University23. Universidad Politecnica de Pachuca, Pachuca, Hgo, Mexico -> Universidad Politecnica de Pachuca24. Facultad de Ciencias F´ısico Matem´aticas, Benem´erita Universidad Aut´onoma de Puebla, Puebla, Mexico -> Benem´erita Universidad Aut´onoma de Puebla25. Centro de Investigaci´on en Computaci´on, Instituto Polit´ecnico Nacional, M´exico City, M´exico. -> Instituto Polit´ecnico Nacional26. Dept of Physics and Astronomy, University of New Mexico, Albuquerque, NM, USA -> University of New Mexico27. Universidad Aut´onoma del Estado de Hidalgo, Pachuca, Mexico -> Universidad Aut´onoma del Estado de Hidalgo28. Instituto de Ciencias Nucleares, Universidad Nacional Aut´onoma de Mexico, Ciudad de Mexico, Mexico -> Universidad Nacional Aut´onoma de Mexico (already listed)29. Natural Science Research Institute, University of Seoul, Seoul, Republic Of Korea -> University of Seoul30. Instituto de F´ısica Corpuscular, CSIC, Universitat de Val`encia, E-46980, Paterna, Valencia, Spain -> Universitat de Val`encia31. Department of Chemistry and Physics, California University of Pennsylvania, California, Penn-sylvania, USA -> California University of Pennsylvania32. Physics Department, Centro de Investigacion y de Estudios Avanzados del IPN, Mexico City, DF, Mexico -> Centro de Investigacion y de Estudios Avanzados del IPN33. Tsung-Dao Lee Institute & School of Physics and Astronomy, Shanghai Jiao Tong U -> Tsung-Dao Lee InstituteFriedrich-Alexander Universität, Erlangen-Nürnberg":
Cosmic rays with energies up to a few PeV are known to be accelerated within the Milky Way. Traditionally, it has been presumed that supernova remnants were the main source of very-high-energy cosmic rays but theoretically it is difficult to get protons to PeV energies and observationally there simply is no evidence to support the remnants as sources of hadrons with energies above a few tens of TeV. One possible source of protons with those energies is the Galactic Center region. Here we report observations of 1-100 TeV gamma rays coming from the 'Cygnus Cocoon', which is a superbubble surrounding a region of OB2 massive star formation. These gamma rays are likely produced by 10-1000 TeV freshly accelerated CRs originating from the enclosed star forming region Cygnus OB2. Hitherto it was not known that such regions could accelerate particles to these energies. The measured flux is likely originated by hadronic interactions. The spectral shape and the emission profile of the Cocoon changes from GeV to TeV energies, which reveals the transport of cosmic particles and historical activity in the superbubble.
Very-high-energy (0.1-100 TeV) gamma-ray emission was observed in HAWC data from the lobes of the microquasar SS 433, making them the first set of astrophysical jets that were resolved at TeV energies. In this work, we update the analysis of SS 433 using 2,565 days of data from the High Altitude Water Cherenkov (HAWC) observatory. Our analysis reports the detection of a point-like source in the east lobe at a significance of 6.6σ6.6\,\sigma and in the west lobe at a significance of 8.2σ8.2\,\sigma. For each jet lobe, we localize the gamma-ray emission and identify a best-fit position. The locations are close to the X-ray emission sites "e1" and "w1" for the east and west lobes, respectively. We analyze the spectral energy distributions and find that the energy spectra of the lobes are consistent with a simple power-law dN/dEEα\text{d}N/\text{d}E\propto E^{\alpha} with α=2.440.120.04+0.13+0.04\alpha = -2.44^{+0.13+0.04}_{-0.12-0.04} and α=2.350.110.03+0.12+0.03\alpha = -2.35^{+0.12+0.03}_{-0.11-0.03} for the east and west lobes, respectively. The maximum energy of photons from the east and west lobes reaches 56 TeV and 123 TeV, respectively. We compare our observations to various models and conclude that the very-high-energy gamma-ray emission can be produced by a population of electrons that were efficiently accelerated.
The recent breakthroughs in the distribution of quantum information and high-precision time and frequency (T&F) signals over long-haul optical fibre networks have transformative potential for physically secure communications, resilience of Global Navigation Satellite Systems (GNSS) and fundamental physics. However, so far these capabilities remain confined to isolated testbeds, with quantum and T&F signals accessible, for example in Germany, to only a few institutions. We propose the QTF-Backbone: a dedicated national fibre-optic infrastructure in Germany for the networked distribution of quantum and T&F signals using dark fibres and specialized hardware. The QTF-Backbone is planned as a four-phase deployment over ten years to ensure scalable, sustainable access for research institutions and industry. The concept builds on successful demonstrations of high-TRL time and frequency distribution across Europe, including PTB-MPQ links in Germany, REFIMEVE in France, and the Italian LIFT network. The QTF-Backbone will enable transformative R&D, support a nationwide QTF ecosystem, and ensure the transition from innovation to deployment. As a national and European hub, it will position Germany and Europe at the forefront of quantum networking, as well as time and frequency transfer.
We reveal a new source of CP-violation in the electroweak sector that is free of any experimental bounds, and we highlight the possible implications for baryogenesis.
A calculation of the QED vacuum polarization potential in the Coulomb field of a pointlike nucleus was presented in an earlier publication by the author and his collaborators. Corrections up to order α2(Zα)7\alpha^2 (Z\alpha)^7 were evaluated, where ZZ is the nuclear charge number and ZαZ\alpha is treated as an independent variable. These corrections correspond to two-loop Feynman graphs with proper propagators of fermions in the external field. The calculation employed a reduction to free QED, leading to free QED Feynman graphs with up to eight independent loops. The method of calculation is described here in detail.
Radiation reaction describes the effective force experienced by an accelerated charge due to radiation emission. Quantum effects dominate charge dynamics and radiation production[1][2] for charges accelerated by fields with strengths approaching the Schwinger field, Esch=\mathbf{E_{sch}=}\textbf{\SI[detect-weight]{1.3e18}{\volt\per\metre}[3]. Such fields exist in extreme astrophysical environments such as pulsar magnetospheres[4], may be accessed by high-power laser systems[5-7], dense particle beams interacting with plasma[8], crystals[9], and at the interaction point of next generation particle colliders[10]. Classical radiation reaction theories do not limit the frequency of radiation emitted by accelerating charges and omit stochastic effects inherent in photon emission[11], thus demanding a quantum treatment. Two quantum radiation reaction models, the quantum-continuous[12] and quantum-stochastic[13] models, correct the former issue, while only the quantum-stochastic model incorporates stochasticity[12]. Such models are of fundamental importance, providing insight into the effect of the electron self-force on its dynamics in electromagnetic fields. The difficulty of accessing conditions where quantum effects dominate inhibited previous efforts to observe quantum radiation reaction in charged particle dynamics with high significance. We report the first direct, high significance (>5σ)(>5{\sigma}) observation of strong-field radiation reaction on charged particles. Furthermore, we obtain strong evidence favouring the quantum radiation reaction models, which perform equivalently, over the classical model. Robust model comparison was facilitated by a novel Bayesian framework which inferred collision parameters. This framework has widespread utility for experiments where parameters governing lepton-laser collisions cannot be directly measured, including those using conventional accelerators.
Gamma-ray binaries are systems composed of a compact object orbiting a massive companion star. The interaction between these two objects can drive relativistic outflows, either jets or winds, in which particles can be accelerated to energies reaching hundreds of tera-electronvolts (TeV). It is however still debated where and under which physical conditions particles are accelerated in these objects and ultimately whether protons can be accelerated up to PeV energies. Among the well-known gamma-ray binaries, LS 5039 is a high-mass X-ray binary (HMXB) with an orbital period of 3.9 days that has been observed up to TeV energies by the High Energy Stereoscopic System (H.E.S.S.). In this work, we present new observations of LS 5039 obtained with the High Altitude Water Cherenkov (HAWC) observatory. Our data reveal that the gamma-ray spectrum of LS 5039 extends up to 200 TeV with no apparent spectral cut-off. Furthermore, we confirm, with a confidence level of 4.7{\sigma}, that the emission between 2 TeV and 118 TeV is modulated by the orbital motion of the system, which indicates that these photons are likely produced within or near the binary orbit where they can undergo absorption by the stellar photons. In a leptonic scenario, the highest energy photons detected by HAWC can be emitted by ~200 TeV electrons inverse Compton scattering stellar photons, which would require an extremely efficient acceleration mechanism operating within LS 5039. Alternatively, a hadronic scenario could explain the data through proton-proton or proton-{\gamma} collisions of protons accelerated to peta-electronvolt (PeV) energies.
We present a summary of recent tests and measurements of hadronic interaction properties with air showers. This report has a special focus on muon density measurements. Several experiments reported deviations between simulated and recorded muon densities in extensive air showers, while others reported no discrepancies. We combine data from eight leading air shower experiments to cover shower energies from PeV to tens of EeV. Data are combined using the z-scale, a unified reference scale based on simulated air showers. Energy-scales of experiments are cross-calibrated. Above 10 PeV, we find a muon deficit in simulated air showers for each of the six considered hadronic interaction models. The deficit is increasing with shower energy. For the models EPOS-LHC and QGSJet-II.04, the slope is found significant at 8 sigma.
Microquasars are laboratories for the study of jets of relativistic particles produced by accretion onto a spinning black hole. Microquasars are near enough to allow detailed imaging of spatial features across the multiwavelength spectrum. The recent extension of the spatial morphology of a microquasar, SS 433, to TeV gamma rays \cite{abeysekara2018very} localizes the acceleration of electrons at shocks in the jet far from the black hole \cite{hess2024ss433}. Here we report TeV gamma-ray emission from another microquasar, V4641~Sgr, which reveals particle acceleration at similar distances from the black hole as SS~433. Additionally, the gamma-ray spectrum of V4641 is among the hardest TeV spectra observed from any known gamma-ray source and is detected up to 200 TeV. Gamma rays are produced by particles, either electrons or hadrons, of higher energies. Because electrons lose energy more quickly the higher their energy, such a spectrum either very strongly constrains the electron production mechanism or points to the acceleration of high-energy hadrons. This observation suggests that large-scale jets from microquasars could be more common than previously expected and that microquasars could be a significant source of Galactic cosmic rays. high energy gamma-rays also provide unique constraints on the acceleration mechanisms of extra-Galactic cosmic rays postulated to be produced by the supermassive black holes and relativistic jets of quasars. The distance to quasars limits imaging studies due to insufficient angular resolution of gamma-rays and due to attenuation of the highest energy gamma-rays by the extragalactic background light.
Many powerful tests of the Standard Model of particle physics and searches for new physics with precision atomic spectroscopy are plagued by our lack of knowledge of nuclear properties. Ideally, such properties may be derived from precise measurements of the most sensitive and theoretically best-understood observables, often found in hydrogen-like systems. While these measurements are abundant for the electric properties of nuclei, they are scarce for the magnetic properties, and precise experimental results are limited to the lightest of nuclei. Here, we focus on 9^9Be which offers the unique possibility to utilize comparisons between different charge states available for high-precision spectroscopy in Penning traps to test theoretical calculations typically obscured by nuclear structure. In particular, we perform the first high-precision spectroscopy of the 1s1s hyperfine and Zeeman structure in hydrogen-like 9^9Be3+^{3+}. We determine its effective Zemach radius with an uncertainty of 500500 ppm, and its bare nuclear magnetic moment with an uncertainty of 0.60.6 parts-per-billion (ppb) - uncertainties unmatched beyond hydrogen. Moreover, we compare to measurements conducted on the three-electron charge state 9^9Be+^{+}, which, for the first time, enables testing the calculation of multi-electron diamagnetic shielding effects of the nuclear magnetic moment at the ppb level. In addition, we test quantum electrodynamics (QED) methods used for the calculation of the hyperfine splitting. Our results serve as a crucial benchmark essential for transferring high-precision results of nuclear magnetic properties across different electronic configurations.
Supernova remnants (SNRs) are widely considered to be accelerators of cosmic rays (CR). They are also expected to produce very-high-energy (VHE; E>100E > 100 GeV) gamma rays through interactions of high-energy particles with the surrounding medium and photon fields. They are, therefore, promising targets for observations with ground-based imaging atmospheric Cherenkov telescopes like the H.E.S.S. telescope array. VHE gamma-ray emission has already been discovered from a number of SNRs, establishing them as a prominent source class in the VHE domain. Of particular interest are the handful of SNRs whose X-ray spectra are dominated by non-thermal synchrotron emission, such as the VHE gamma-ray emitters RX J0852.0-4622 (Vela Jr.) and RX J1713-3946. The shell-type SNRs G1.9+0.3 and G330.2+1.0 also belong to this subclass and are further notable for their young ages (1\leq 1 kyr), especially G1.9+0.3, which was recently determined to be the youngest SNR in the Galaxy (100\sim100 yr). These unique characteristics motivated investigations with H.E.S.S. to search for VHE gamma rays. The results of the H.E.S.S. observations and analyses are presented, along with implications for potential particle acceleration scenarios.
Solar neutrino studies triggered and largely motivated the major developments in neutrino physics in the last 50 years. Theory of neutrino propagation in different media with matter and fields has been elaborated. It includes oscillations in vacuum and matter, resonance flavor conversion and resonance oscillations, spin and spin-flavor precession, etc. LMA MSW has been established as the true solution of the solar neutrino problem. Parameters theta12 and Delta_m21^2 have been measured; theta13 extracted from the solar data is in agreement with results from reactor experiments. Solar neutrino studies provide a sensitive way to test theory of neutrino oscillations and conversion. Characterized by long baseline, huge fluxes and low energies they are a powerful set-up to search for new physics beyond the standard 3nu paradigm: new neutrino states, sterile neutrinos, non-standard neutrino interactions, effects of violation of fundamental symmetries, new dynamics of neutrino propagation, probes of space and time. These searches allow us to get stringent, and in some cases unique bounds on new physics. We summarize the results on physics of propagation, neutrino properties and physics beyond the standard model obtained from studies of solar neutrinos.
The unexpectedly high flux of cosmic ray positrons detected at Earth may originate from nearby astrophysical sources, dark matter, or unknown processes of cosmic-ray secondary production. We report the detection, using the HighAltitude Water Cherenkov Observatory (HAWC), of extended tera-electron volt gamma-ray emission coincident with the locations of two nearby middle-aged pulsars (Geminga and PSR B0656+14). The HAWC observations demonstrate that these pulsars are indeed local sources of accelerated leptons, but the measured tera-electron volt emission profile constrains the diffusion of particles away from these sources to be much slower than previously assumed. We demonstrate that the leptons emitted by these objects are therefore unlikely to be the origin of the excess positrons, which may have a more exotic origin.
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