Ultra high energy cosmic ray research with the pierre auger observatory
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Ultra-High Energy Cosmic Ray Research with the Pierre Auger Observatory. Methods, Results, What We Learn, and expansion to Colorado Bill Robinson. Mysteries of Ultra-High Energy Cosmic Rays. What are they made of through the range of energies? What accelerates them?

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Ultra-High Energy Cosmic Ray Research with the Pierre Auger Observatory

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Ultra high energy cosmic ray research with the pierre auger observatory

Ultra-High Energy Cosmic Ray Research with the Pierre Auger Observatory

Methods, Results, What We Learn,

and expansion to Colorado

Bill Robinson


Mysteries of ultra high energy cosmic rays

Mysteries of Ultra-High Energy Cosmic Rays

  • What are they made of through the range of energies?

  • What accelerates them?

  • How energetic can they get?

  • Why do we detect UHECRs that are too energetic to be allowed by current theory?

  • Where do they come from? And why do different detectors get different results?


S swordy auger design report

(S. Swordy, AUGER design report)

power law E-2.8

Above knee:

supernova remnant shocks

Below knee; where from?

Upper limit;

GZK cutoff at

ankle, most

energetic yet

3 E 20 eV or

300 EeV

[1 EeV = 10 E18,

Exaelectron Volt]


Ultra high energy cosmic ray research with the pierre auger observatory

(from http://www.mpi-hd.mpg.de/hfm/CosmicRay/Showers.html)


Simulated longitudinal development of 50 1 eev cascades

Simulated Longitudinal development of 50 1 EeV Cascades

M. Ambrosio et. al., Astroparticle Physics 24, 355-371 (2005).


Interaction depth of shower maximum pao 850 g cm 2 sea level 1000 interstellar space 10 8 ly

Interaction Depth of shower maximum (PAO ~ 850 g/cm^2; sea level = 1000 = interstellar space 10^8 LY)


1 eev anisotropy from akeno

1 EeV Anisotropy from Akeno

Ratio of # of observed events to expected ones in equatorial coordinate.

Solid line = Galactic Plane, G.C. is galactic center. Amplitude: ~ 4%


Galactic region of excess akeno

Galactic region of excess (Akeno)

Ion gyroradius [cgs];

m = mass in proton units

Z = ionization

E = energy in eV

Galactic B = 3 microgauss

R for 1 EeV proton =

~300 pc


Anisotropies in he arrival direction

Anisotropies in HE Arrival Direction

From the Japanese Akeno observatory, above 40 EeV, 1990—2002

But there’s a lot of controversy about this…..


Problems

Problems

  • Shaded circles show clustering within 2.5 degrees; chance probability of 0.9% for just one triple event

  • BUT this is not corroborated by other observatories; when they show anisotropies they are in other directions

  • No sources in arrival directions away from galaxy*

  • Neutrons of 10 EeV have gamma ~ 10 E9, so a range of about 10 kpc; galactic center within range. Immune to field deflections. No anisotropies below 10 E17.9

  • Impossible to detect directly if neutrons are primaries

  • Only Akeno shows galactic center and Cygnus clustering

  • Extremely low flux and contradictory results are good arguments for more observatories using multiple detection methods in different regions

  • Have to separate gamma ray showers from nuclei


Pao fails to find excess

PAO fails to find excess…

10 E17.9 < E < 10 E 18.5, 5 degree windows, GC at cross, line is galactic plane;

2.3 years of Auger data, no abnormally over-dense regions, cannot resolve

probable source at GC (must use gamma rays to investigate)


Gzk cutoff 2003 pre pao

GZK Cutoff? (2003, pre-PAO)

arXiv:hep-ph/o206217 v5 27 Feb 2003, “Has the GZK suppression been discovered?”


Pao south near completion

PAO (south); near completion


Pao hybrid detector

PAO Hybrid Detector


Lonesome water tank and the andes

Lonesome Water Tank and the Andes


Fluorescence telescope enclosure

Fluorescence telescope enclosure


Uhecr energy loss and calibration

UHECR Energy loss and calibration;

Energy loss in the shower;

with Nem = particle density along shower direction x, Nph = photons reaching fluorescence detector, R(x) = distance from shower point x and FD, T(x) = atmospheric transmission (<1)

Energy loss in the shower;

Energy loss in the shower;

Night atmosphere assumed horizontally

Invariant; only steered through zenith

angle, probes to 30 km tracing losses

to molecular and aerosol scattering. Requires clear moonless nights; 14% duty cycle.

Calibrationwith Lidar


Auger fluorescence telescope

Auger fluorescence telescope

Diameter: 2.2 meters

Aperture: 3.8 sq. m.

440 photomultiplier tubes

Schematic shows positions of diffusers for optical calibrations


Central laser facility pao south

Central Laser Facility (PAO South)

  • UV laser (355 nm) fires 7 ns, 7 mJ pulse every 15 minutes to calibrate FDs; scattered luminosity approx. same as strong shower

  • Located equidistant from 3 of the 4 FD eyes

  • Polarization randomized (better than circular)

  • Can fire in any direction

  • Weather checked by instruments every 5 minutes


Pao proposed initial colorado site

PAO proposed initial Colorado site

(Middle of Nowhere)


Conclusion

Conclusion

  • More detectors needed!

  • Colorado site ideal; funding on order of $100 million; room for huge expansion

  • Primary questions remain unresolved

  • Existing PAO works both physically and politically as a model of international cooperation


References

References

Websites:

History of the Air Fluorescence Technique,

www.cosmic-ray.org/reading/fluor.html

Pierre Auger Observatory; www.auger.org and www.augernorth.org

AGASA; www-akeno.icrr.u-tokyo.ac.jp/AGASA/

Interaction Depth www.lbl.gov/abc/cosmic/SKliewer/Cosmic_Rays/Interaction.htm

Journals:

M. Ambrosio et. al., Astroparticle Physics 24, 355-371 (2005).

Pierre Auger Collaboration, arXiv:astro-ph 3, 0607382 (2006).

N. Hayashitda et al., Astroparticle Physics 10, 310 (1999).

J. Bahcall and Eli Waxman, arXiv:hep-ph 5, 0206217 (27 Feb 2003).

A. Filipcic et. al., Astroparticle Physics 18, 502 (2003).

Optical Relative Calibration for Auger Fluorescence Detector, and Performance of the PAO Surface Array, Pune (2005) 00, 101-106

The Central Laser Facility at the PAO, Subm. To Nucl. Inst. Meth. ‘06


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