Results from the Pierre Auger Observatory

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L. Cazón Hadron-Hadron & Cosmic-Rays interactions at multi-TeV energies. Trento,2-Dez-2010 1 Results from the Pierre Auger Observatory L. Cazon, for the Pierre Auger Collaboration LIP, Portugal

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Results from the Pierre Auger Observatory. L. Cazon , for the Pierre Auger Collaboration LIP, Portugal. UHECRs. How / where are they produced ? What is their composition ? How do they interact ?. UHECRs : those with energies greater than 10 18 eV 1 particle/km 2 /year. - PowerPoint PPT Presentation

Transcript of Results from the Pierre Auger Observatory

Page 1: Results from the  Pierre Auger Observatory

L. Cazón Hadron-Hadron & Cosmic-Rays interactions at multi-TeV energies.

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Results from the Pierre Auger Observatory

L. Cazon, for the Pierre Auger Collaboration LIP, Portugal

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UHECRs

UHECRs : those with energies greater than 1018 eV

1 particle/km2/year

L. Cazón Hadron-Hadron & Cosmic-Rays interactions at multi-TeV energies.

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How/where are they produced?

What is their composition?

How do they interact?

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Very Interesting region

L. Cazón 3Simple model for extragalactic B. B=1 nG, Lcoh=1 MPc

Galactic and extragalactig B fields bend the CR trajectories.

At the highest energies, UHECR point back to the sources.

GZK Horizons: Only sources within 100 Mpc will reach us. Anisotropies are expected.

D. Allard et al

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Latitude 35 S – Longitude 69 W

1400m a.s.l. X=870 g cm2

Data taking since 2004

Installation completed in 2008

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Fluorescence detectors4 building with 6 telescopes eachTelescope f.o.v. 30 x 30 deg~10% duty cycleProvides High Accuracy

Surface detectors1600 Cherenkov stations spaced 1.5 kmArea of 3000 km2

100% duty cycleProvides Large Statistics

The Pierre Auger Observatory

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SD detectors

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PMT µe

Diffusive tyvek

Water Cerenkov Detectors give signal proportional to their track lengh in waterDifficult to separate different particle types.Some indirect methods

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FD detectors

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20 x 22 pixels440 Photonis XP3062Pixel f.o.v. = 1.5 x 1.5 deg

Collect Fluorescence light emited by the shower. Mainly the central region of the EM cascade.

shuttersfilters + corrector ringcameraelectronics cratemirror

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Hybrid Detector: Large and accurate

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The energy is independent of simulations except for the energy carried by neutrinos and muons.

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Resolution SD & FD

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The systematic uncertainties on the energy scale EFD sum up to 22%.The largest uncertainties are given by the absolute fluorescence yield (14%), the absolute calibration of the fluorescence telescopes (9%)and the uncertainty due to the reconstruction method of the longitudinal shower profile (10%).

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Energy Calibration of SD with FD

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Calibration does not depend on hadronic interaction modelsSystematical error 22%energy resolution 17%

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Energy Spectrum

Auger data shows a flux supression at the highest energies

Cutoff significant with >20 sigma

L. Cazón 10

PLB 685 (2010) 239

γ=3.26±0.04γ =2.55±0.04

log10 (E1/2/eV)=19.61 ± 0.03

log10 (Eankle /eV)=18.60 ± 0.01

This feature is compatible with:

GZK

Sources running out of power

It combines FD and SD spectrum.

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Spectrum comparison

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PLB 685 (2010) 239

In agreement with energy scale systematics

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Xmax analysis

L. Cazón 12

PRL 104 (2010) 091101

Single: D10=33 ± 2 g/cm2/decadeχ2/ndf = 35/11

+35

Broken: D10=105 – 21 g/cm2/decadelog10 (Ebreak/eV) = 18.24 ± 0.05D10=24 ± 3 g/cm2/decadeχ2/ndf = 9.7/9

3754 events

If hadronic interactions do no change much over less than 2 decades, this change on D10 would imply a change on composition around the ankle.

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Comparison with MC

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PRL 104 (2010) 091101

Data show either a change on composition towards heavier nucei or a change in the hadronic models

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Correlation with AGNScience318:938-943,2007

12/15 events correlated in the exploratory scan, 3.2 expected. P<1E-8Difficult to estimate real probability, thus confirmation required with an independent data set.

Prescription was set.8/13 events found to correlate.• Null hypothesis (Isotropy of UHECR) rejected at 99% CL• Large correlation (~70%) with extragalactic matter (traced by AGN)

VCV catalogue is not complete: over/undersampled across the sky

A correlation with the AGNs does not necessarily mean that AGNs are the sources!!!AGNs act as tracers of the regions where the sources are.

(z<0.018, alpha=3.1 deg, E>57 EeV)

Angular resolution ~1 deg

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Update

L. Cazón 15

Astroparticle Physics 34 (2010) 314–326

69 events observed (up to 31.12.2009; 20370 km2 sr y)14.5 correlations expected if isotropy. 29 observed.

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Astroparticle Physics 34 (2010) 314–326

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Hot spot

L. Cazón 17

At 3.8 Mpc distance, Cen A is the closest AGN. Obvious source candidate.

Separation angle (deg)

Astroparticle Physics 34 (2010) 314–326

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Other catalogs

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2MRS galaxies

Swift-BAT AGNs Comparisons with flux limited (unbiased) catalogs show that there are multiple astrophysical models of anisotropy arising from the distribution of matter in the nearby universe which are fully consistent with the observed distribution of arrival directions.

Smoothed maps

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Neutrinos

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Neutrino Limits

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Photon limits

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Astropart. Phys. 31 (2009) 399

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Number of muons

L. Cazón 22

Hybrids

Smoothing

Muon jump

Universality

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Number of muons

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ICRC09, Lodz 2009

Hybrids

Muon Jump

Universality

Smoothing

It also implies an energy scaling (different from FD)

(Universality)

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Conclusions• Flux suppression of UHECR unequivocally established

• GZK? Sources running out of power?

• UHECR anisotropy at 99% CL

• Light primaries? Heavy primaries with weak B? Sources closeby?

• Composition: intriguing results

• Heavier? Failing models? Cross sections?

• Top down models

disfavored

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AnisotropyIsotropy

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Back up slides

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Acceptance

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CIC Method

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Resolution SD & FD

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The systematic uncertainties on the energy scale EFD sum up to 22%.The largest uncertainties are given by the absolute fluorescence yield (14%), the absolute calibration of the fluorescence telescopes (9%)and the uncertainty due to the reconstruction method of the longitudinal shower profile (10%).

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