Konstantin Belov. GZK-40, Moscow. Konstantin Belov High Resolution Fly’s Eye (HiRes) Collaboration GZK-40. INR, Moscow. May 17, 2006. measurements by fluorescence.

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Konstantin Belov. GZK-40, Moscow. Konstantin Belov High Resolution Fly’s Eye (HiRes) Collaboration GZK-40. INR, Moscow. May 17, measurements by fluorescence experiments. measurements by fluorescence experiments. Columbia University University of Adelaide University of New Mexico Rutgers University University of Montana Los Alamos National Laboratory University of Tokyo

Konstantin Belov. GZK-40, Moscow. Motivation Compare the measurements from the three fluorescence experiments: Fly’s Eye, HiRes/MIA, and HiRes Stereo. Only fluorescence experiment SEE Xmax. In HiRes energy range ( eV) expect to see a transition between galactic and extragalactic sources: –Expect highest energy galactic cosmic rays to be heavy nuclei (iron); –Expect extragalactic cosmic rays to be light (protons) –Expect transition from mixed to light composition.

Konstantin Belov. GZK-40, Moscow. X max distribution for p, CNO, Fe Heavier primaries develop earlier in the atmosphere. RMS of the X max distribution is different. QGSJet

Konstantin Belov. GZK-40, Moscow. Elongation rate p, CNO, Fe

Konstantin Belov. GZK-40, Moscow. Fly’s Eye detector. Two fluorescence detectors were positioned 3.5 km apart; The effective energy range extended from eV to 3  eV; 5  5 degree pixel size; Geometry of the event was determined by the intersection of the two event-detector planes; Elevation angle range from 0 to 90 degrees; FE II had only partial azimuth coverage

Konstantin Belov. GZK-40, Moscow. HiRes prototype/MIA Hybrid fluorescence - muon array detector; Fourteen mirror prototype of the current HiRes detector had a 1  1 degree pixel size; looked from 3 to 71 degrees in elevation. Was located 3.5 km from the center of the MIA muon array; The muon array sampled a part of muon lateral distribution. 3 km effective area; Energy range from 5  eV to just above eV; Event geometry was determined by using the HiRes event-detector plane and timing from both detectors.

Konstantin Belov. GZK-40, Moscow. HiRes fluorescence detector.

Konstantin Belov. GZK-40, Moscow. Stereo observations. HiRes 1 has 20 operational mirrors in one ring. S/H electronics. FOV 3-17º in elevation, 322º in azimuth HiRes 2 has 42 operational mirrors in two rings. FADC electronics. FOV 3-31º in elevation, 336º in azimuth. Detectors are 12.6 km apart forming a stereo pair. Stereo fixes shower geometry improving resolution. Idealistic view of a stereo event

Konstantin Belov. GZK-40, Moscow. An event of the HiRes displays. HiRes1 – one ring detector HiRes2 – two ring detector

Konstantin Belov. GZK-40, Moscow. Measured shower profile. Event by event: X max in g/cm 2 ; Total energy of the primary particle: Arrival direction Statistically: p-air inelastic cross-section; Mass composition. Measured shower parameters.

Konstantin Belov. GZK-40, Moscow. HiRes stereo and HiRes/MIA data. HiRes/MIA - hybrid experiment. Resolution function estimated from simulations ~ 44 gm/cm 2 HiRes stereo - X max resolution measured, 30 gm/cm 2

Konstantin Belov. GZK-40, Moscow. Fly’s Eye stereo data. Fly’s Eye Stereo - X max resolution ~45 gm/cm 2 measured resolution function

Konstantin Belov. GZK-40, Moscow. Systematic errors All three experiments quote systematic errors ~ 25 gm/cm 2. Dominant contributions –Mirror survey –Cherenkov subtraction –Atmospheric profile –Aerosol corrections Highest energy data is best measurements - most complete profile - minimum Cherenkov subtraction

Konstantin Belov. GZK-40, Moscow. Comparison of Fly’s Eye Stereo and HiRes energy scales Energy scale for all three experiments is consistent (location of ankle and second knee). Energy scale for all three experiments is consistent (location of ankle and second knee).

Konstantin Belov. GZK-40, Moscow. Elongation rate Use HiRes stereo average X max and Fly’s Eye stereo average Xmax above eV. Require a 13 gm/cm 2 upward shift for Fly’s Eye to bring means into agreement Shift all Fly’s eye X max data points by the same amount. Filled circles, HiRes; Triangles, HiRes/MIA, Open circles, Fly’s Eye (shifted).

Konstantin Belov. GZK-40, Moscow. Elongation Rate Simple shift of Fly’s Eye data brings all data into reasonable agreement. Fly’s Eye and HiRes data are in excellent agreement above eV. HiRes/MIA shows earlier transition to “protons”, but point by point discrepancy is small. HiRes/MIA systematics are better understood, however.

Konstantin Belov. GZK-40, Moscow. What about X max distributions?  Are Xmax distribution widths consistent?  Two overlap regions - Fly’s Eye and Hires/MIA in 3x10 17 to 5 x eV bin. - Fly’s Eye and Hires/MIA in 3x10 17 to 5 x eV bin. - Fly’s Eye and HiRes stereo in > eV bin. - Fly’s Eye and HiRes stereo in > eV bin.  No evidence of discrepancy in distribution widths.

Konstantin Belov. GZK-40, Moscow. Triangles: Fly’s Eye Stereo; Circles: HiRes/MIA. Fly’s Eye vs HiRes/MIA X max at 3-5 x eV

Konstantin Belov. GZK-40, Moscow. Triangles: Stereo Fly’s Eye; Circles: HiRes. Fly’s Eye vs HiRes X max > eV

Konstantin Belov. GZK-40, Moscow. Sequence of X max distributions in three increasing energy bins 3-5  10 17, 5-10  and > eV. Red-Fly’s Eye Blue-HiRes/MIA Purple-HiRes stereo

Konstantin Belov. GZK-40, Moscow. Conclusions A simple X max shift brings all three experiments into reasonable agreement. Widths of X max distributions are in agreement. Normalized X max distribution show change to wider distribution above 10 18, consistent with change to protons. Interpretation of elongation rate over limited energy range is problematic - Need large dynamic range in a single experiment!