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Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK [email protected] 59 th Krakow School of Theoretical Physics Zakopane June 2019 Probing the Violent Universe with multi-messenger eyes: gravitational waves, high-energy neutrinos, gamma rays, and cosmic rays

Probing the Violent Universe with multi-messenger eyes ...th- · Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK [email protected] 59th Krakow School

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Page 1: Probing the Violent Universe with multi-messenger eyes ...th- · Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK a.a.watson@leeds.ac.uk 59th Krakow School

Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson

University of Leeds, UK [email protected]

59th Krakow School of Theoretical Physics Zakopane June 2019

Probing the Violent Universe with multi-messenger eyes: gravitational waves, high-energy neutrinos,

gamma rays, and cosmic rays

Page 2: Probing the Violent Universe with multi-messenger eyes ...th- · Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK a.a.watson@leeds.ac.uk 59th Krakow School

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Lecture 3

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Astrophysical Models to explain all of this There are many and the data are not very constraining

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Implications of mass result for detection of cosmogenic neutrinos (Ave, Busca, Olinto, aaw, Yamamoto 2005; Hooper, Taylor and Sarkar 2005)

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Neutrino argument and the Ankle Region: Heinze et al. arXiv 1512.05988 (ApJ 2016)

Assume that the TA spectrum measurement and interpretation of pure protons is correct Scan simultaneously over

Spectral index at injection Source Evolution Maximum proton energy

Predict the neutrino flux and compare with IceCube

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3D best fit: log (Emax/GeV) = 10.7 +0.3 /0.1; m = 4.3 +0.4/-0.8; γ = 1.52 +0.35/-0.20

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Heavier composition, à la Auger, is favoured (or some additional component in ankle region)

Auger neutrino limit 2019

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New York and Parisian Ideas: Extragalactic sources

Globus, Allard and Parizot: arXiv 1505.01377

Unger, Farrar and Anchordoqui: arXiv 1505.02153 Acceleration in extragalactic sources surrounded by strong photon fields

Globus et al. Specific GRB model

Unger et al. More generic Fragmentation and propagation studied

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Page 10: Probing the Violent Universe with multi-messenger eyes ...th- · Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK a.a.watson@leeds.ac.uk 59th Krakow School

10 Carlo Crivelli (1430 – 1490): ‘The Annuciation with St Edimus’

National Gallery London

An earlier solution?

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Search for UHE neutrinos at the Auger Observatory

Parente and Zas: Venice Meeting 1996, arXiv 960609

τ at EeV may decay before reaching the ground à Secondary shower (Double Bang event)

Also interactions in mountains or upward-going in earth

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Page 13: Probing the Violent Universe with multi-messenger eyes ...th- · Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK a.a.watson@leeds.ac.uk 59th Krakow School

Search Method for neutrinos

Look for inclined, BUT young, showers

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Searching neutrinos in coincidence with other ‘happenings’ 1.  GW170817 Superbly positioned for Auger neutrino searches -but only upper limits – joint paper with ~4000 others! 2. TXS0506+056

Again no neutrinos seen. Joint paper with IceCube, ANTARES and Auger

No coincidences - YET

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Search for photons Main source is decay of neutral pions Or from exotic ways of producing UHECR Showers with lateral distribution function steeper unusually steep

Xmax unusually deep

Shower front unusually curved

Risetime unusually slow

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Limits rule out exotic models Beginning to test models where protons dominate No signals from specific objects Work continuing to devise more clever methods

Searches from specific sources

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Some success - and of some problems

Hadronic Interactions

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Bristol: Conference on Very High Energy Interactions, January 1963

J G Wilson

Trying to get information about particle interactions from studying

Extensive Air Showers is like trying to get information about the workings of the British Cabinet by reading the

Daily Mirror

AGS 33 GeV CERN PS 28 GeV

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Distribution of Xmax for two energy ranges ICRC 2015

Λη , the attenuation length, is found from the 20% most penetrating events

1196/18090

1384/21270

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Relationship between Λη and proton-air cross-section

25% Helium contamination: σ reduced by -17 and – 16 mb

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Proton-air cross-section as function of energy

Impact of 25% He is included as systematic uncertainty (- 16 mb) Photons have been shown to be < 0.5% at energies of interest: contamination would raise σ by ~ 4.5 mb

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β = 0.9 εc = energy at which pion interaction becomes less probable than decay (~10 GeV) Nµ increases with energy increases with A at given energy

‘The Muon Problem’

Page 32: Probing the Violent Universe with multi-messenger eyes ...th- · Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK a.a.watson@leeds.ac.uk 59th Krakow School

37 stations 71° 3200 g cm-2 54 EeV Fit made to density distribution Energy measured with ~20 % accuracy

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Inclined showers are useful to test models – muons dominate

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33 Maps such as these are compared and fitted to the observations so that the number of muons, Nµ, can be obtained

Average muon density profile of simulated-proton of 1019eV

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35 Predicted muon numbers are under-estimated by 30 to 80% (20% systematic)

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ρ0 → π+ + π-

Thus there is a channel to enhance muon production

Taking energy out of electromagnetic channel will raise depth of shower maximum - slightly lighter primaries

NA62/SHINE

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Similar muon problem to what was seen at LEP?

Page 41: Probing the Violent Universe with multi-messenger eyes ...th- · Ultra High-Energy Cosmic Rays Lecture 3 Alan Watson University of Leeds, UK a.a.watson@leeds.ac.uk 59th Krakow School
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CERN Courier December 2015 ALICE

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JCAP 01 032 2016

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Conclusion in ALICE paper makes assumption about mass composition, in contradiction with cosmic ray data

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Next steps: On the ground TA x4: this will increase area of TA to that of Auger. Operational in next year or so. Fully Sensitive above ~ 30 EeV. Main aim is to increase Statistics on Hot Spot Auger to Auger Prime: 4 m2 of scintillator to allow muon separation: event-by-event mass at highest energies Radio antenna on every tank

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(ii) 4 m2 Scintillators above Water-Cherenkov detectors

Scintillators respond to muons and electromagnetic component Water-Cherenkov detectors absorb all of the em component and are fully sensitive to muons It has been demonstrated with simulations that techniques exist to separate out the muon component

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(iii) Buried Muon Detectors (1.3 m below surface)

60 x 20 m2

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Linsley proposed (1979) that a fluorescence detector should be put into space Eventually led to EUSO (ESA phase A (with Livio Scarsi)) and then to JEM-EUSO Currently module at TA and super-pressure balloon test flights ISS flight Twin satellites: POEMMA: Probe of Extreme Multi-Messenger Astrophysics

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The Future at the Highest Energies – immediate future

•  Separate particles as function of development for anisotropy studies:

FADC parameters with water-Cherenkov detectors Radio detection to measure Xmax , 24 hours per day •  Achieve greater exposures:

TA x 4 Continued operation of Auger Observatory JEM-EUSO and derivatives

•  Composition on shower-by-shower basis at highest energy

with AugerPrime

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Summary of experimental data •  Ankle at ~ 4 EeV and steepening at ~ 50 EeV clearly established •  Strong evidence for dipole anisotropy in Auger data above 8 EeV

•  Weaker evidences (~4 sigma) for coincidence with starburst galaxies above 39 EeV and some evidence (~2.5 sigma) for γAGNs above 60 EeV •  Mass composition getting heavier above the ankle (still some dispute) •  No diffuse neutrinos seen (at level similar to IceCube) nor any from specific events (GW170817 or TX0506+56) •  Hadronic Interactions – more muons seen than predicted

Remains a fascinating field with very exciting prospects!