260 research outputs found

    Searches for Neutrinos from Gamma-Ray Bursts Using the IceCube Neutrino Observatory

    Get PDF
    Gamma-ray bursts (GRBs) are considered as promising sources of ultra-high-energy cosmic rays (UHECRs) due to their large power output. Observing a neutrino flux from GRBs would offer evidence that GRBs are hadronic accelerators of UHECRs. Previous IceCube analyses, which primarily focused on neutrinos arriving in temporal coincidence with the prompt gamma-rays, found no significant neutrino excess. The four analyses presented in this paper extend the region of interest to 14 days before and after the prompt phase, including generic extended time windows and targeted precursor searches. GRBs were selected between 2011 May and 2018 October to align with the data set of candidate muon-neutrino events observed by IceCube. No evidence of correlation between neutrino events and GRBs was found in these analyses. Limits are set to constrain the contribution of the cosmic GRB population to the diffuse astrophysical neutrino flux observed by IceCube. Prompt neutrino emission from GRBs is limited to ≲1% of the observed diffuse neutrino flux, and emission on timescales up to 104 s is constrained to 24% of the total diffuse flux.Peer Reviewe

    Data-driven modeling of electron recoil nucleation in PICO C3F8 bubble chambers

    Full text link
    [EN] The primary advantage of moderately superheated bubble chamber detectors is their simultaneous sensitivity to nuclear recoils from weakly interacting massive particle (WIMP) dark matter and insensitivity to electron recoil backgrounds. A comprehensive analysis of PICO gamma calibration data demonstrates for the first time that electron recoils in C3F8 scale in accordance with a new nucleation mechanism, rather than one driven by a hot spike as previously supposed. Using this semiempirical model, bubble chamber nucleation thresholds may be tuned to be sensitive to lower energy nuclear recoils while maintaining excellent electron recoil rejection. The PICO-40L detector will exploit this model to achieve thermodynamic thresholds as low as 2.8 keV while being dominated by single-scatter events from coherent elastic neutrino-nucleus scattering of solar neutrinos. In one year of operation, PICO-401, can improve existing leading limits from PICO on spin-dependent WIMP-proton coupling by nearly an order of magnitude for WIMP masses greater than 3 GeV c(-2) and will have the ability to surpass all existing non-xenon bounds on spin-independent WIMP-nucleon coupling for WIMP masses from 3 to 40 GeV c(-2).The PICO Collaboration wishes to thank SNOLAB and its staff for support through underground space, logistical and technical services. SNOLAB operations are supported by the Canada Foundation for Innovation and the Province of Ontario Ministry of Research and Innovation, with underground access provided by Vale at the Creighton mine site. We wish to acknowledge the support of the Natural Sciences and Engineering Research Council of Canada (NSERC) and the Canada Foundation for Innovation (CFI) for funding. We acknowledge the support from National Science Foundation (NSF) (Grants No. 0919526, No. 1506337, No. 1242637, No. 1205987, and No. 1806722). We acknowledge that this work is supported by the U.S. Department of Energy (DOE) Office of Science, Office of High Energy Physics (under Award No. DE-SC-0012161), by DGAPA-UNAM (PAPIIT No. IA100118) and Consejo Nacional de Ciencia y Tecnología (CONACyT, M¿exico, Grants No. 252167 and No. A1-S-8960), by the Department of Atomic Energy (DAE), Government of India, under the Centre for AstroParticle Physics II project (CAPP-II) at the Saha Institute of Nuclear Physics (SINP), European Regional Development Fund¿Project ¿Engineering Applications of Microworld Physics¿ (Project No. CZ.02.1.01/0.0/0.0/ 16_019/0000766), and the Spanish Ministerio de Ciencia, Innovación y Universidades (Red Consolider MultiDark, Grant No. FPA2017-90566-REDC). This work is partially supported by the Kavli Institute for Cosmological Physics at the University of Chicago through NSF Grant No. 1125897, and an endowment from the Kavli Foundation and its founder Fred Kavli. We also wish to acknowledge the support from Fermi National Accelerator Laboratory under Contract No. DE-AC02-07CH11359, and Pacific Northwest National Laboratory, which is operated by Battelle for the U.S. Department of Energy under Contract No. DE-AC05- 76RL01830. We also thank Compute Canada [75] and the Center for Advanced Computing, ACENET, Calcul Qu¿ebec, Compute Ontario, and WestGrid for computational support.Amole, C.; Ardid Ramírez, M.; Arnquist, I.; Asner, DM.; Baxter, D.; Behnke, E.; Bressler, M.... (2019). Data-driven modeling of electron recoil nucleation in PICO C3F8 bubble chambers. Physical Review D: covering particles, fields, gravitation, and cosmology. 100(8):1-18. https://doi.org/10.1103/PhysRevD.100.082006S1181008Amole, C., Ardid, M., Arnquist, I. J., Asner, D. M., Baxter, D., Behnke, E., … Chen, C. J. (2019). Dark matter search results from the complete exposure of the PICO-60 C3F8 bubble chamber. Physical Review D, 100(2). doi:10.1103/physrevd.100.022001Agnese, R., Anderson, A. J., Aramaki, T., Arnquist, I., Baker, W., Barker, D., … Bowles, M. A. (2017). Projected sensitivity of the SuperCDMS SNOLAB experiment. Physical Review D, 95(8). doi:10.1103/physrevd.95.082002Amaudruz, P.-A., Baldwin, M., Batygov, M., Beltran, B., Bina, C. E., Bishop, D., … Broerman, B. (2018). First Results from the DEAP-3600 Dark Matter Search with Argon at SNOLAB. Physical Review Letters, 121(7). doi:10.1103/physrevlett.121.071801Arnaud, Q., Asner, D., Bard, J.-P., Brossard, A., Cai, B., Chapellier, M., … Zampaolo, M. (2018). First results from the NEWS-G direct dark matter search experiment at the LSM. Astroparticle Physics, 97, 54-62. doi:10.1016/j.astropartphys.2017.10.009Aguilar-Arevalo, A., Amidei, D., Bertou, X., Butner, M., Cancelo, G., … Castañeda Vázquez, A. (2016). Search for low-mass WIMPs in a 0.6 kg day exposure of the DAMIC experiment at SNOLAB. Physical Review D, 94(8). doi:10.1103/physrevd.94.082006Aalseth, C. E., Acerbi, F., Agnes, P., Albuquerque, I. F. M., Alexander, T., Alici, A., … Ardito, R. (2018). DarkSide-20k: A 20 tonne two-phase LAr TPC for direct dark matter detection at LNGS. The European Physical Journal Plus, 133(3). doi:10.1140/epjp/i2018-11973-4Jungman, G., Kamionkowski, M., & Griest, K. (1996). Supersymmetric dark matter. Physics Reports, 267(5-6), 195-373. doi:10.1016/0370-1573(95)00058-5Bertone, G., Hooper, D., & Silk, J. (2005). Particle dark matter: evidence, candidates and constraints. Physics Reports, 405(5-6), 279-390. doi:10.1016/j.physrep.2004.08.031Feng, J. L. (2010). Dark Matter Candidates from Particle Physics and Methods of Detection. Annual Review of Astronomy and Astrophysics, 48(1), 495-545. doi:10.1146/annurev-astro-082708-101659Duncan, F., Noble, A. J., & Sinclair, D. (2010). The Construction and Anticipated Science of SNOLAB. Annual Review of Nuclear and Particle Science, 60(1), 163-180. doi:10.1146/annurev.nucl.012809.104513Behnke, E., Behnke, J., Brice, S. J., Broemmelsiek, D., Collar, J. I., … Conner, A. (2012). First dark matter search results from a 4-kgCF3Ibubble chamber operated in a deep underground site. Physical Review D, 86(5). doi:10.1103/physrevd.86.052001Behnke, E., Behnke, J., Brice, S. J., Broemmelsiek, D., Collar, J. I., … Conner, A. (2014). Erratum: First dark matter search results from a 4-kgCF3Ibubble chamber operated in a deep underground site [Phys. Rev. D86, 052001 (2012)]. Physical Review D, 90(7). doi:10.1103/physrevd.90.079902Aubin, F., Auger, M., Genest, M.-H., Giroux, G., Gornea, R., Faust, R., … Storey, C. (2008). Discrimination of nuclear recoils from alpha particles with superheated liquids. New Journal of Physics, 10(10), 103017. doi:10.1088/1367-2630/10/10/103017Zacek, V. (1994). Search for dark matter with moderately superheated liquids. Il Nuovo Cimento A, 107(2), 291-298. doi:10.1007/bf02781560Amole, C., Ardid, M., Asner, D. M., Baxter, D., Behnke, E., Bhattacharjee, P., … Broemmelsiek, D. (2016). Dark matter search results from the PICO-60CF3Ibubble chamber. Physical Review D, 93(5). doi:10.1103/physrevd.93.052014Amole, C., Ardid, M., Arnquist, I. J., Asner, D. M., Baxter, D., Behnke, E., … Campion, P. (2017). Dark Matter Search Results from the PICO−60 C3F8 Bubble Chamber. Physical Review Letters, 118(25). doi:10.1103/physrevlett.118.251301Amole, C., Ardid, M., Arnquist, I. J., Asner, D. M., Baxter, D., Behnke, E., … Brice, S. J. (2016). Improved dark matter search results from PICO-2L Run 2. Physical Review D, 93(6). doi:10.1103/physrevd.93.061101Amole, C., Ardid, M., Asner, D. M., Baxter, D., Behnke, E., Bhattacharjee, P., … Broemmelsiek, D. (2015). Dark Matter Search Results from the PICO-2LC3F8Bubble Chamber. Physical Review Letters, 114(23). doi:10.1103/physrevlett.114.231302Hasert, F. J., Faissner, H., Krenz, W., Von Krogh, J., Lanske, D., Morfin, J., … Lemonne, J. (1973). Search for elastic muon-neutrino electron scattering. Physics Letters B, 46(1), 121-124. doi:10.1016/0370-2693(73)90494-2Hasert, F. J., Kabe, S., Krenz, W., Von Krogh, J., Lanske, D., Morfin, J., … Sacton, J. (1973). Observation of neutrino-like interactions without muon or electron in the gargamelle neutrino experiment. Physics Letters B, 46(1), 138-140. doi:10.1016/0370-2693(73)90499-1Behnke, E., Benjamin, T., Brice, S. J., Broemmelsiek, D., Collar, J. I., … Cooper, P. S. (2013). Direct measurement of the bubble-nucleation energy threshold in aCF3Ibubble chamber. Physical Review D, 88(2). doi:10.1103/physrevd.88.021101Tenner, A. G. (1963). Nucleation in bubble chambers. Nuclear Instruments and Methods, 22, 1-42. doi:10.1016/0029-554x(63)90224-6Kozynets, T., Fallows, S., & Krauss, C. B. (2019). Modeling emission of acoustic energy during bubble expansion in PICO bubble chambers. Physical Review D, 100(5). doi:10.1103/physrevd.100.052001Seitz, F. (1958). On the Theory of the Bubble Chamber. Physics of Fluids, 1(1), 2. doi:10.1063/1.1724333Behnke, E., Collar, J. I., Cooper, P. S., Crum, K., Crisler, M., Hu, M., … Tschirhart, R. (2008). Spin-Dependent WIMP Limits from a Bubble Chamber. Science, 319(5865), 933-936. doi:10.1126/science.1149999Barnabé-Heider, M., Di Marco, M., Doane, P., Genest, M.-H., Gornea, R., Guénette, R., … Noulty, R. (2005). Response of superheated droplet detectors of the PICASSO dark matter search experiment. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 555(1-2), 184-204. doi:10.1016/j.nima.2005.09.015Ziegler, J. F., Ziegler, M. D., & Biersack, J. P. (2010). SRIM – The stopping and range of ions in matter (2010). Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, 268(11-12), 1818-1823. doi:10.1016/j.nimb.2010.02.091Bressler, M., Campion, P., Cushman, V. S., Morrese, A., Wagner, J. M., Zerbo, S., … Dahl, C. E. (2019). A buffer-free concept bubble chamber for PICO dark matter searches. Journal of Instrumentation, 14(08), P08019-P08019. doi:10.1088/1748-0221/14/08/p08019Agostinelli, S., Allison, J., Amako, K., Apostolakis, J., Araujo, H., Arce, P., … Barrand, G. (2003). Geant4—a simulation toolkit. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 506(3), 250-303. doi:10.1016/s0168-9002(03)01368-8Pozzi, S. A., Padovani, E., & Marseguerra, M. (2003). MCNP-PoliMi: a Monte-Carlo code for correlation measurements. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 513(3), 550-558. doi:10.1016/j.nima.2003.06.012Archambault, S., Aubin, F., Auger, M., Beleshi, M., Behnke, E., … Behnke, J. (2011). New insights into particle detection with superheated liquids. New Journal of Physics, 13(4), 043006. doi:10.1088/1367-2630/13/4/043006Glaser, D. A. (1954). Progress report on the development of bubble chambers. Il Nuovo Cimento, 11(S2), 361-368. doi:10.1007/bf02781098Fabian, B. N., Place, R. L., Riley, W. A., Sims, W. H., & Kenney, V. P. (1963). Density of Particle Tracks in the Hydrogen Bubble Chamber. Review of Scientific Instruments, 34(5), 484-495. doi:10.1063/1.1718415Willis, W. J., Fowler, E. C., & Rahm, D. C. (1957). Bubble Density in a Propane Bubble Chamber. Physical Review, 108(4), 1046-1047. doi:10.1103/physrev.108.1046Hahn, B., & Hugentobler, E. (1960). Relativistic increase in bubble density in a CBrF3 bubble chamber. Il Nuovo Cimento, 17(6), 983-985. doi:10.1007/bf02732145Brown, J. L., Glaser, D. A., & Perl, M. L. (1956). Liquid Xenon Bubble Chamber. Physical Review, 102(2), 586-587. doi:10.1103/physrev.102.586Baxter, D., Chen, C. J., Crisler, M., Cwiok, T., Dahl, C. E., Grimsted, A., … Zhang, J. (2017). First Demonstration of a Scintillating Xenon Bubble Chamber for Detecting Dark Matter and Coherent Elastic Neutrino-Nucleus Scattering. Physical Review Letters, 118(23). doi:10.1103/physrevlett.118.231301Durup, J., & Platzman, R. L. (1961). Role of the Auger effect in the displacement of atoms in solids by ionizing radiation. Discussions of the Faraday Society, 31, 156. doi:10.1039/df9613100156Schönfeld, E., & Janßen, H. (2000). Calculation of emission probabilities of X-rays and Auger electrons emitted in radioactive disintegration processes. Applied Radiation and Isotopes, 52(3), 595-600. doi:10.1016/s0969-8043(99)00216-xStrigari, L. E. (2009). Neutrino coherent scattering rates at direct dark matter detectors. New Journal of Physics, 11(10), 105011. doi:10.1088/1367-2630/11/10/105011Lewin, J. D., & Smith, P. F. (1996). Review of mathematics, numerical factors, and corrections for dark matter experiments based on elastic nuclear recoil. Astroparticle Physics, 6(1), 87-112. doi:10.1016/s0927-6505(96)00047-3Fitzpatrick, A. L., Haxton, W., Katz, E., Lubbers, N., & Xu, Y. (2013). The effective field theory of dark matter direct detection. Journal of Cosmology and Astroparticle Physics, 2013(02), 004-004. doi:10.1088/1475-7516/2013/02/004Anand, N., Fitzpatrick, A. L., & Haxton, W. C. (2014). Weakly interacting massive particle-nucleus elastic scattering response. Physical Review C, 89(6). doi:10.1103/physrevc.89.065501Gresham, M. I., & Zurek, K. M. (2014). Effect of nuclear response functions in dark matter direct detection. Physical Review D, 89(12). doi:10.1103/physrevd.89.123521Gluscevic, V., Gresham, M. I., McDermott, S. D., Peter, A. H. G., & Zurek, K. M. (2015). Identifying the theory of dark matter with direct detection. Journal of Cosmology and Astroparticle Physics, 2015(12), 057-057. doi:10.1088/1475-7516/2015/12/057Aprile, E., Aalbers, J., Agostini, F., Alfonsi, M., Althueser, L., Amaro, F. D., … Baudis, L. (2019). Constraining the Spin-Dependent WIMP-Nucleon Cross Sections with XENON1T. Physical Review Letters, 122(14). doi:10.1103/physrevlett.122.141301Akerib, D. S., Alsum, S., Araújo, H. M., Bai, X., Bailey, A. J., Balajthy, J., … Biesiadzinski, T. P. (2017). Limits on Spin-Dependent WIMP-Nucleon Cross Section Obtained from the Complete LUX Exposure. Physical Review Letters, 118(25). doi:10.1103/physrevlett.118.251302Fu, C., Cui, X., Zhou, X., Chen, X., Chen, Y., … Fang, D. (2017). Spin-Dependent Weakly-Interacting-Massive-Particle–Nucleon Cross Section Limits from First Data of PandaX-II Experiment. Physical Review Letters, 118(7). doi:10.1103/physrevlett.118.071301Behnke, E., Besnier, M., Bhattacharjee, P., Dai, X., Das, M., Davour, A., … Zacek, V. (2017). Final results of the PICASSO dark matter search experiment. Astroparticle Physics, 90, 85-92. doi:10.1016/j.astropartphys.2017.02.005Aartsen, M. G., Ackermann, M., Adams, J., Aguilar, J. A., Ahlers, M., Ahrens, M., … Ansseau, I. (2017). Search for annihilating dark matter in the Sun with 3 years of IceCube data. The European Physical Journal C, 77(3). doi:10.1140/epjc/s10052-017-4689-9Choi, K., Abe, K., Haga, Y., Hayato, Y., Iyogi, K., Kameda, J., … Nakahata, M. (2015). Search for Neutrinos from Annihilation of Captured Low-Mass Dark Matter Particles in the Sun by Super-Kamiokande. Physical Review Letters, 114(14). doi:10.1103/physrevlett.114.141301Ruppin, F., Billard, J., Figueroa-Feliciano, E., & Strigari, L. (2014). Complementarity of dark matter detectors in light of the neutrino background. Physical Review D, 90(8). doi:10.1103/physrevd.90.083510Felizardo, M., Girard, T. A., Morlat, T., Fernandes, A. C., Ramos, A. R., Marques, J. G., … Marques, R. (2014). The SIMPLE Phase II dark matter search. Physical Review D, 89(7). doi:10.1103/physrevd.89.072013Adrián-Martínez, S., Albert, A., André, M., Anton, G., Ardid, M., Aubert, J.-J., … Basa, S. (2016). Limits on dark matter annihilation in the sun using the ANTARES neutrino telescope. Physics Letters B, 759, 69-74. doi:10.1016/j.physletb.2016.05.019Adrián-Martínez, S., Albert, A., André, M., Anton, G., Ardid, M., Aubert, J.-J., … Basa, S. (2016). A search for Secluded Dark Matter in the Sun with the ANTARES neutrino telescope. Journal of Cosmology and Astroparticle Physics, 2016(05), 016-016. doi:10.1088/1475-7516/2016/05/016Aprile, E., Aalbers, J., Agostini, F., Alfonsi, M., Althueser, L., Amaro, F. D., … Bauermeister, B. (2018). Dark Matter Search Results from a One Ton-Year Exposure of XENON1T. Physical Review Letters, 121(11). doi:10.1103/physrevlett.121.111302Akerib, D. S., Alsum, S., Araújo, H. M., Bai, X., Bailey, A. J., Balajthy, J., … Biesiadzinski, T. P. (2017). Results from a Search for Dark Matter in the Complete LUX Exposure. Physical Review Letters, 118(2). doi:10.1103/physrevlett.118.021303Agnes, P., Albuquerque, I. F. M., Alexander, T., Alton, A. K., Araujo, G. R., Asner, D. M., … Batignani, G. (2018). Low-Mass Dark Matter Search with the DarkSide-50 Experiment. Physical Review Letters, 121(8). doi:10.1103/physrevlett.121.081307Agnes, P., Albuquerque, I. F. M., Alexander, T., Alton, A. K., Araujo, G. R., Ave, M., … Biery, K. (2018). DarkSide-50 532-day dark matter search with low-radioactivity argon. Physical Review D, 98(10). doi:10.1103/physrevd.98.102006Agnese, R., Anderson, A. J., Aralis, T., Aramaki, T., Arnquist, I. J., Baker, W., … Bauer, D. A. (2018). Low-mass dark matter search with CDMSlite. Physical Review D, 97(2). doi:10.1103/physrevd.97.022002Agnese, R., Aramaki, T., Arnquist, I. J., Baker, W., Balakishiyeva, D., Banik, S., … Binder, T. (2018). Results from the Super Cryogenic Dark Matter Search Experiment at Soudan. Physical Review Letters, 120(6). doi:10.1103/physrevlett.120.061802Hehn, L., Armengaud, E., Arnaud, Q., Augier, C., Benoît, A., Bergé, L., … Yakushev, E. (2016). Improved EDELWEISS-III sensitivity for low-mass WIMPs using a profile likelihood approach. The European Physical Journal C, 76(10). doi:10.1140/epjc/s10052-016-4388-yTolman, R. C. (1949). The Effect of Droplet Size on Surface Tension. The Journal of Chemical Physics, 17(3), 333-337. doi:10.1063/1.1747247Kirkwood, J. G., & Buff, F. P. (1949). The Statistical Mechanical Theory of Surface Tension. The Journal of Chemical Physics, 17(3), 338-343. doi:10.1063/1.1747248Xue, Y.-Q., Yang, X.-C., Cui, Z.-X., & Lai, W.-P. (2010). The Effect of Microdroplet Size on the Surface Tension and Tolman Length. The Journal of Physical Chemistry B, 115(1), 109-112. doi:10.1021/jp108431

    Performance of the D-Egg Optical Sensor for the IceCube Upgrade

    Get PDF
    New optical sensors called the "D-Egg" have been developed for cost-effective instrumentation for the IceCube Upgrade. With two 8-inch high QE photomultipliers, they offer increased effective photocathode area while retaining as much of the successful IceCube Digital Optical Module (DOM) design as possible. Mass production of D-Eggs has started in 2020. By the end of 2021, there will be 310 D-Eggs produced with 288 deployed in the IceCube Upgrade. The D-Egg readout system uses advanced technologies in electronics and computing power. Each of the two PMT signals is digitized using ultra-low-power 14-bit ADCs with a sampling frequency of 250-MSPS, enabling seamless and lossless event recording from single-photon signals to signals exceeding 200pe within 10ns, as well as flexible event triggering. In this paper, we report the single photon detection performance as well as the multiple photon recording capability of D-Eggs from the mass production line which have been evaluated with the built-in DAQ system

    New Flux Limits in the Low Relativistic Regime for Magnetic Monopoles at IceCube

    Get PDF
    Magnetic monopoles are hypothetical particles that carry magnetic charge. Depending on their velocity, different light production mechanisms exist to facilitate detection. In this work, a previously unused light production mechanism, luminescence of ice, is introduced. This light production mechanism is nearly independent of the velocity of the incident magnetic monopole and becomes the only viable light production mechanism in the low relativistic regime (0.1-0.55c). An analysis in the low relativistic regime searching for magnetic monopoles in seven years of IceCube data is presented. While no magnetic monopole detection can be claimed, a new flux limit in the low relativistic regime is presented, superseding the previous best flux limit by 2 orders of magnitude

    Combining Maximum-Likelihood with Deep Learning for Event Reconstruction in IceCube

    Get PDF
    The field of deep learning has become increasingly important for particle physics experiments, yielding a multitude of advances, predominantly in event classification and reconstruction tasks. Many of these applications have been adopted from other domains. However, data in the field of physics are unique in the context of machine learning, insofar as their generation process and the laws and symmetries they abide by are usually well understood. Most commonly used deep learning architectures fail at utilizing this available information. In contrast, more traditional likelihood-based methods are capable of exploiting domain knowledge, but they are often limited by computational complexity. In this contribution, a hybrid approach is presented that utilizes generative neural networks to approximate the likelihood, which may then be used in a traditional maximum-likelihood setting. Domain knowledge, such as invariances and detector characteristics, can easily be incorporated in this approach. The hybrid approach is illustrated by the example of event reconstruction in IceCube

    A Search for Neutrinos from Decaying Dark Matter in Galaxy Clusters and Galaxies with IceCube

    Get PDF
    The observed dark matter abundance in the Universe can be explained with non-thermal, heavy dark matter models. In order for dark matter to still be present today, its lifetime has to far exceed the age of the Universe. In these scenarios, dark matter decay can produce highly energetic neutrinos, along with other Standard Model particles. To date, the IceCube Neutrino Observatory is the world’s largest neutrino telescope, located at the geographic South Pole. In 2013, the IceCube collaboration reported the first observation of high-energy astrophysical neutrinos. Since then, IceCube has collected a large amount of astrophysical neutrino data with energies up to tens of PeV, allowing us to probe the heavy dark matter models using neutrinos. We search the IceCube data for neutrinos from decaying dark matter in galaxy clusters and galaxies. The targeted dark matter masses range from 10 TeV to 10 PeV. In this contribution, we present the method and sensitivities of the analysis

    Testing Hadronic Interaction Models with Cosmic Ray Measurements at the IceCube Neutrino Observatory

    Get PDF
    The IceCube Neutrino Observatory provides the opportunity to perform unique measurements of cosmic-ray air showers with its combination of a surface array and a deep detector. Electromagnetic particles and low-energy muons (∼GeV) are detected by IceTop, while a bundle of high-energy muons (>~400 GeV) can be measured in coincidence in IceCube. Predictions of air-shower observables based on simulations show a strong dependence on the choice of the high-energy hadronic interaction model. By reconstructing different composition-dependent observables, one can provide strong tests of hadronic interaction models, as these measurements should be consistent with one another. In this work, we present an analysis of air-shower data between 2.5 and 80 PeV, comparing the composition interpretation of measurements of the surface muon density, the slope of the IceTop lateral distribution function, and the energy loss of the muon bundle, using the models Sibyll 2.1, QGSJet-II.04 and EPOS-LHC. We observe inconsistencies in all models under consideration, suggesting they do not give an adequate description of experimental data. The results furthermore imply a significant uncertainty in the determination of the cosmic-ray mass composition through indirect measurements

    First Search for Unstable Sterile Neutrinos with the IceCube Neutrino Observatory

    Get PDF
    We present a search for an unstable sterile neutrino by looking for a matter-induced signal in eight years of atmospheric νμ\nu_\mu data collected from 2011 to 2019 at the IceCube Neutrino Observatory. Both the (stable) three-neutrino and the 3+1 sterile neutrino models are disfavored relative to the unstable sterile neutrino model, though with pp-values of 2.5\% and 0.81\%, respectively, we do not observe evidence for 3+1 neutrinos with neutrino decay. The best-fit parameters for the sterile neutrino with decay model from this study are Δm412=6.72.5+3.9eV2\Delta m_{41}^2=6.7^{+3.9}_{-2.5}\,\rm{eV}^2, sin22θ24=0.330.17+0.20\sin^2 2\theta_{24}=0.33^{+0.20}_{-0.17}, and g2=2.5π±1.5πg^2=2.5\pi\pm1.5\pi, where gg is the decay-mediating coupling. The preferred regions from short-baseline oscillation searches are excluded at 90\% C.L

    Design of a Robust Fiber Optic Communications System for Future IceCube Detectors

    Get PDF
    In this work we discuss ongoing development of a hybrid fiber/copper data and timing infrastructure for the future IceCube-Gen2 detector. The IceCube Neutrino Observatory is a kilometer-scale detector operating with 86 strings of modules. These modules communicate utilizing a custom protocol to mitigate the signaling challenges of long distance copper cables. Moving past the limitations of a copper-based backbone will allow larger future IceCube detectors with extremely precise timing and a large margin of excess throughput to accommodate innovative future modules. To this end, the upcoming IceCube Upgrade offers an opportunity to deploy a pathfinder for the new fiber optic infrastructure, called the Fiber Test System. This design draws on experience from AMANDA and IceCube and incorporates recently matured technologies such as ruggedized fibers and White Rabbit timing to deliver robust and high-performance data and timing transfer

    Graph Neural Networks for low-energy event classification & reconstruction in IceCube

    Get PDF
    corecore