The Cosmic Ray Energetics And Mass (CREAM) is a balloon-borne experiment designed to measure the composition and energy spectra of cosmic rays of charge Z = 1 to 26 up to an energy of ~ 10^15 eV. CREAM had two successful flights on long-duration balloons (LDB) launched from Mc- Murdo Station, Antarctica, in December 2004 and December 2005. CREAM-I achieves a substantial measurement redundancy by employing multiple detector systems, namely a Timing Charge Detector and a Silicon Charge Detector (SCD) for particle identification, and a Transition Radiation Detector and a sampling tungsten/scintillating-fiber ionization calorimeter (CAL) for energy measurement. In this paper, preliminary energy spectra of various elements measured with CAL/SCD during the first 42-day flight are presented.
Deep Dive into Elemental Spectra from the CREAM-I Flight.
The Cosmic Ray Energetics And Mass (CREAM) is a balloon-borne experiment designed to measure the composition and energy spectra of cosmic rays of charge Z = 1 to 26 up to an energy of ~ 10^15 eV. CREAM had two successful flights on long-duration balloons (LDB) launched from Mc- Murdo Station, Antarctica, in December 2004 and December 2005. CREAM-I achieves a substantial measurement redundancy by employing multiple detector systems, namely a Timing Charge Detector and a Silicon Charge Detector (SCD) for particle identification, and a Transition Radiation Detector and a sampling tungsten/scintillating-fiber ionization calorimeter (CAL) for energy measurement. In this paper, preliminary energy spectra of various elements measured with CAL/SCD during the first 42-day flight are presented.
30TH INTERNATIONAL COSMIC RAY CONFERENCE
Elemental Spectra from the CREAM-I Flight
H. S. AHN , P. ALLISON , M. G. BAGLIESI , J. J. BEATTY , G. BIGONGIARI , P. BOYLE ,
J. T. CHILDERS , N. B. CONKLIN , S. COUTU , M. A. DUVERNOIS , O. GANEL , J. H. HAN ,
J. A. JEON , K. C. KIM , J. K. LEE , M. H. LEE , L. LUTZ , P. MAESTRO , A. MALININE ,
P. S. MARROCCHESI , S. MINNICK , S. I. MOGNET , S. NAM , S. NUTTER , I. H. PARK ,
N. H. PARK , E. S. SEO
, R. SINA , S. SWORDY , S. WAKELY , J. WU , J. YANG , Y. S. YOON
,
R. ZEI , S. Y. ZINN .
Inst. for Phys. Sci. and Tech., University of Maryland, College Park, MD 20742 USA
Dept. of Physics, Ohio State University, Columbus, Ohio 43210, USA
Dept. of Physics, University of Siena and INFN, Via Roma 56, 53100 Siena, Italy
Enrico Fermi Institute and Dept. of Physics, University of Chicago, Chicago, IL 60637, USA
School of Physics and Astronomy, University of Minnesota, Minneapolis, MN 55455, USA
Dept. of Physics, Penn State University, University Park, PA 16802, USA
Dept. of Physics, Ewha Womans University, Seoul, 120-750, Republic of Korea
Dept. of Physics, Kent State University Tuscarawas, New Philadelphia, OH 44663, USA
Dept. of Physics and Geology, Northern Kentucky University, Highland Heights, KY 41099, USA
Dept. of Physics, University of Maryland, College Park, MD 20742 USA
hsahn@umd.edu
Abstract:
The Cosmic Ray Energetics And Mass (CREAM) is a balloon-borne experiment designed
to measure the composition and energy spectra of cosmic rays of charge Z = 1 to 26 up to an energy
of
10
eV. CREAM had two successful flights on long-duration balloons (LDB) launched from Mc-
Murdo Station, Antarctica, in December 2004 and December 2005. CREAM-I achieves a substantial
measurement redundancy by employing multiple detector systems, namely a Timing Charge Detector
and a Silicon Charge Detector (SCD) for particle identification, and a Transition Radiation Detector and a
sampling tungsten/scintillating-fiber ionization calorimeter (CAL) for energy measurement. In this paper,
preliminary energy spectra of various elements measured with CAL/SCD during the first 42-day flight are
presented.
Introduction
The Cosmic Ray Energetics And Mass (CREAM)
balloon-borne experiment is designed to investi-
gate the charge and energy spectra of cosmic-
ray nuclei of hydrogen to iron at high energies
up to
10
eV. CREAM has had two success-
ful long-duration balloon (LDB) flights, launched
from McMurdo Station, Antarctica, for 42 days in
2004-2005 (CREAM-I) and 28 days in 2005-2006
(CREAM-II) [1].
In both flights CREAM em-
ployed a 20 radiation length tungsten/scintillating-
fiber sampling calorimeter (CAL), preceded by
a pair of graphite targets providing
0.42 nu-
clear interaction length, to induce hadronic show-
ers from cosmic-ray nuclei, triggering and mea-
suring the energy of those with energy above
10
eV. Each of the 20 active layers was seg-
mented into 50 one-cm-wide ribbons. Signals from
these ribbons were used to reconstruct and extrap-
olate trajectories back to the Silicon Charge Detec-
tor (SCD) of 52
56 pixels, for accurate charge
measurement. Details of the experiment, including
other complementary instruments, namely a Tim-
ing Charge Detector and a Transition Radiation
Detector, can be found in [2].
Various elements have been studied by analyzing
the CREAM-I flight data with CAL/SCD. See [3]
ELEMENTAL SPECTRA FROM THE CREAM-I FLIGHT
for the spectra of hydrogen and helium. In this pa-
per, preliminary energy spectra of cosmic-ray car-
bon and oxygen are presented, and compared with
results from other experiments.
Calibration
CAL was placed in one of CERN’s SPS accelerator
beam-lines, and exposed to a variety of electron,
proton, and nuclear fragment beams to verify both
the instrument’s functionality and the validity of
the simulation model. CAL responses to 150 GeV
electrons were used for absolute calibration, which
is extrapolated to the responses to much higher en-
ergy cosmic rays collected during flight [4].
CREAM-I Flight
During the flight, the payload floated at an aver-
age altitude of 128,000 ft, corresponding to a resid-
ual atmosphere of 3.9 g/cm . The analysis in this
paper has been performed with only a subset of
cosmic-ray events, CAL-triggered by requiring 6
consecutive layers to have energy deposit of more
than
50 MeV in the highest deposit ribbon, and
collected for 23.7 days when both CAL and SCD
operation was stable. Live time fraction is assumed
to be 75%. The dead CAL channels, noisy SCD
pixels, and zero-suppression level in CAL ribbons
have been taken into account in the detector simu-
lations.
Reconstruction
Incident particle trajectory is estimated using
fitting of a straight line through a combination of
CAL hits with highest energy deposit in each layer,
in x-z and y-z, respectively. The combination is
chosen by rejecting any hit that is not consistent
with others to make a straight line. This trajectory
is further improved by including, in the fitting, (1)
selected CAL hits’
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