J. H. Han
University of Maryland, College Park
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Featured researches published by J. H. Han.
The Astrophysical Journal | 2010
H. S. Ahn; P. Allison; M. G. Bagliesi; J. J. Beatty; G. Bigongiari; J.T. Childers; N. B. Conklin; S. Coutu; Michael A. DuVernois; O. Ganel; J. H. Han; J. A. Jeon; K. C. Kim; M.H. Lee; L. Lutz; P. Maestro; A. Malinin; P.S. Marrocchesi; S. Minnick; S. I. Mognet; J. Nam; S. Nam; S. Nutter; I. H. Park; N. Park; E. S. Seo; R. Sina; J. Wu; J. Yang; Y.S. Yoon
The balloon-borne Cosmic Ray Energetics And Mass experiment launched five times from Antarctica has achieved a cumulative flight duration of about 156 days above 99.5% of the atmosphere. The instrument is configured with complementary and redundant particle detectors designed to extend direct measurements of cosmic-ray composition to the highest energies practical with balloon flights. All elements from protons to iron nuclei are separated with excellent charge resolution. Here, we report results from the first two flights of ~70 days, which indicate hardening of the elemental spectra above ~200 GeV/nucleon and a spectral difference between the two most abundant species, protons and helium nuclei. These results challenge the view that cosmic-ray spectra are simple power laws below the so-called knee at ~1015 eV. This discrepant hardening may result from a relatively nearby source, or it could represent spectral concavity caused by interactions of cosmic rays with the accelerating shock. Other possible explanations should also be investigated.
The Astrophysical Journal | 2011
Y.S. Yoon; H. S. Ahn; P. Allison; M. G. Bagliesi; J. J. Beatty; G. Bigongiari; P. J. Boyle; J.T. Childers; N. B. Conklin; S. Coutu; Michael A. DuVernois; O. Ganel; J. H. Han; J. A. Jeon; K. C. Kim; 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. Park; E. S. Seo; R. Sina; Simon P. Swordy; S. P. Wakely
Cosmic-ray proton and helium spectra have been measured with the balloon-borne Cosmic Ray Energetics And Mass experiment flown for 42 days in Antarctica in the 2004–2005 austral summer season. High-energy cosmic-ray data were collected at an average altitude of �38.5 km with an average atmospheric overburden of �3.9 g cm −2 . Individual elements are clearly separated with a charge resolution of �0.15 e (in charge units) and �0.2 e for protons and helium nuclei, respectively. The measured spectra at the top of the atmosphere are represented by power laws with a spectral index of 2.66 ± 0.02 for protons from 2.5 TeV to 250 TeV and –2.58 ± 0.02 for helium nuclei from 630 GeV nucleon −1 to 63 TeV nucleon −1 . They are harder than previous measurements
The Astrophysical Journal | 2009
H. S. Ahn; P. Allison; M. G. Bagliesi; Loius M. Barbier; J. J. Beatty; G. Bigongiari; T. J. Brandt; J.T. Childers; N. B. Conklin; S. Coutu; Michael A. DuVernois; O. Ganel; J. H. Han; J. A. Jeon; K. C. Kim; M.H. Lee; P. Maestro; A. Malinine; P.S. Marrocchesi; S. Minnick; S. I. Mognet; S. Nam; S. Nutter; I. H. Park; N. Park; E. S. Seo; R. Sina; P. Walpole; J. Wu; J. Yang
We present new measurements of the energy spectra of cosmic-ray (CR) nuclei from the second flight of the balloon-borne experiment Cosmic-Ray Energetics And Mass (CREAM). The instrument included different particle detectors to provide redundant charge identification and measure the energy of CRs up to several hundred TeV. The measured individual energy spectra of C, O, Ne, Mg, Si, and Fe are presented up to ~1014 eV. The spectral shape looks nearly the same for these primary elements and it can be fitted to an E –2.66 ± 0.04 power law in energy. Moreover, a new measurement of the absolute intensity of nitrogen in the 100-800 GeV/n energy range with smaller errors than previous observations, clearly indicates a hardening of the spectrum at high energy. The relative abundance of N/O at the top of the atmosphere is measured to be 0.080 ± 0.025 (stat.)±0.025 (sys.) at ~800 GeV/n, in good agreement with a recent result from the first CREAM flight.
The Astrophysical Journal | 2010
H. S. Ahn; P. Allison; M. G. Bagliesi; Loius M. Barbier; J. J. Beatty; G. Bigongiari; T. J. Brandt; J.T. Childers; N. B. Conklin; S. Coutu; Michael A. DuVernois; O. Ganel; J. H. Han; J. A. Jeon; K. C. Kim; Jue-Yeon Lee; M.H. Lee; P. Maestro; A. Malinin; P.S. Marrocchesi; S. Minnick; S. I. Mognet; G. W. Na; J. Nam; S. Nam; S. Nutter; I. H. Park; N. Park; E. S. Seo; R. Sina
We present measurements of the relative abundances of cosmic-ray nuclei in the energy range of 500-3980 GeV/nucleon from the second flight of the Cosmic Ray Energetics And Mass balloon-borne experiment. Particle energy was determined using a sampling tungsten/scintillating-fiber calorimeter, while particle charge was identified precisely with a dual-layer silicon charge detector installed for this flight. The resulting element ratios C/O, N/O, Ne/O, Mg/O, Si/O, and Fe/O at the top of atmosphere are 0.919 ? 0.123stat ? 0.030syst, 0.076 ? 0.019stat ? 0.013syst, 0.115 ? 0.031stat ? 0.004syst, 0.153 ? 0.039stat ? 0.005syst, 0.180 ? 0.045stat ? 0.006syst, and 0.139?? 0.043stat ? 0.005syst, respectively, which agree with measurements at lower energies. The source abundance of N/O is found to be 0.054 ? 0.013stat ? 0.009syst+0.010esc ?0.017. The cosmic-ray source abundances are compared to local Galactic (LG) abundances as a function of first ionization potential and as a function of condensation temperature. At high energies the trend that the cosmic-ray source abundances at large ionization potential or low condensation temperature are suppressed compared to their LG abundances continues. Therefore, the injection mechanism must be the same at TeV/nucleon energies as at the lower energies measured by HEAO-3, CRN, and TRACER. Furthermore, the cosmic-ray source abundances are compared to a mixture of 80% solar system abundances and 20% massive stellar outflow (MSO) as a function of atomic mass. The good agreement with TIGER measurements at lower energies confirms the existence of a substantial fraction of MSO material required in the ~TeV per nucleon region.
IEEE Transactions on Nuclear Science | 2007
S. Nam; H. S. Ahn; P. Allison; M. G. Bagliesi; Loius M. Barbier; J. J. Beatty; G. Bigongiari; T. J. Brandt; J. A. Jeon; J. T. Childers; N. B. Conklin; S. Coutu; Michael A. DuVernois; O. Ganel; J. H. Han; K. C. Kim; M.H. Lee; L. Lutz; P. Maestro; A. Malinine; P.S. Marrocchesi; Stephen Anthony Minnick; S. I. Mognet; Scott Lowry Nutter; I. H. Park; N. Park; E. S. Seo; R. Sina; P. Walpole; J. Wu
The balloon-borne cosmic-ray experiment CREAM (Cosmic Ray Energetics And Mass) has completed two flights in Antarctica, with a combined duration of 70 days. One of the detectors in the payload is the SCD (silicon charge detector) that measures the charge of high energy cosmic rays. The SCD was assembled with silicon sensors. A sensor is a 4 × 4 array of DC-coupled PIN diode pixels with the total active area of 21 × 16 mm2. The SCD used during the first flight (December 2004-January 2005) was a single layer device, then upgraded to a dual layer device for the second flight (December 2005-January 2006), covering the total sensitive area of 779 × 795 mm2. Flight data demonstrated that adding a second layer improved SCD performance, showing excellent particle charge resolution. With a total dissipation of 136 W for the dual layer system, special care was needed in designing thermal paths to keep the detector temperature within its operational range. As a consequence, flight temperatures of the SCD, even at diurnal maximum were kept below 38°C. The SCD mechanical structure was designed to minimize the possibility of damage to the sensors and electronics from the impacts of parachute deployment and landing. The detector was recovered successfully following the flight and is being refurbished for the next flight in 2007. Details of construction, operation, and performance are presented for the dual-layered SCD flown for the second CREAM flight.
CALORIMETRY IN HIGH ENERGY PHYSICS: XII International Conference | 2006
M.H. Lee; H. S. Ahn; P. Allison; M. G. Bagliesi; Loius M. Barbier; J. J. Beatty; G. Bigongiari; P. J. Boyle; T. J. Brandt; J.T. Childers; N. B. Conklin; S. Coutu; Michael A. DuVernois; O. Ganel; J. H. Han; J. A. Jeon; K. C. Kim; L. Lutz; P. Maestro; A. Malinine; P. S. Marrocchesi; S. Minnick; S. I. Mognet; S. Nam; S. Nutter; I. H. Park; N. Park; E. S. Seo; R. Sina; Simon P. Swordy
The Cosmic Ray Energetics And Mass (CREAM) balloon‐borne experiment, designed to directly measure cosmic‐ray particle energies from ∼1011 to ∼1015 eV, had two successful flights since December 2004, with a total duration of 70 days. The CREAM calorimeter is comprised of 20 layers of 1 radiation length (X0) tungsten interleaved with 20 active layers each made up of fifty 1 cm wide scintillating fiber ribbons. The scintillation signals are read out with multi pixel Hybrid Photo Diodes (HPDs), VA32‐HDR2/TA32C ASICs and LTC1400 ADCs. During detector construction, various tests were carried out using radioactive sources, UV‐LEDs, and particle beams. We will present results from these tests and show preliminary results from the two flights.
arXiv: High Energy Astrophysical Phenomena | 2009
P. Maestro; H. S. Ahn; P. Allison; M. G. Bagliesi; Loius M. Barbier; J. J. Beatty; G. Bigongiari; T. J. Brandt; J.T. Childers; N. B. Conklin; S. Coutu; Michael A. DuVernois; O. Ganel; J. H. Han; J. A. Jeon; K. C. Kim; M.H. Lee; A. Malinine; P.S. Marrocchesi; S. Minnick; S. I. Mognet; S. Nam; S. Nutter; I. H. Park; N. Park; E. S. Seo; R. Sina; P. Walpole; J. Wu; J. Yang
During its second Antarctic flight, the CREAM (Cosmic Ray Energetics And Mass) balloon experiment collected data for 28 days, measuring the charge and the energy of cosmic rays (CR) with a redundant system of particle identification and an imaging thin ionization calorimeter. Preliminary direct measurements of the absolute intensities of individual CR nuclei are reported in the elemental range from carbon to iron at very high energy.
IEEE Transactions on Nuclear Science | 2009
Moo Hyun Lee; H. S. Ahn; O. Ganel; J. H. Han; Jin A. Jeon; C.H. Kim; Ki Chun Kim; L. Lutz; A. Malinin; G. W. Na; S. Nam; I. H. Park; Na Hee Park; E. S. Seo; A. Vartanyan; P. Walpole; Jayoung Wu; Jongmann Yang; J.H. Yoo; Y.S. Yoon
Cosmic Ray Energetics And Mass (CREAM) is a balloon-borne experiment to directly measure the elemental spectra of protons to iron nuclei with energies up to ~ 1015 eV. Energies of these cosmic-ray particles are measured by an ionization calorimeter comprised of 20 layers of 1 radiation length thick tungsten plates and 20 layers of 0.5 mm diameter scintillating fibers. Each tungsten plate is 500 times 500 times 3.5 mm3 and the fibers are grouped into fifty 1 cm wide ribbons. After construction, the CREAM-III calorimeter was tested at CERN, the European high energy physics lab, in the H2 beam line of the SPS. Following the CERN test, the calorimeter was integrated into the CREAM-III instrument, and flown successfully in the 3rd flight of the project, during the 2007/8 Antarctic campaign. We present the performance of the CREAM-III calorimeter in lab and beam tests.
Journal of Instrumentation | 2015
Y.S. Hwang; H. J. Kim; T. Anderson; D. Angelaszek; M. Copley; S. Coutu; J. H. Han; H.G. Huh; D.H. Kah; K. C. Kim; K. Kwashnak; M.H. Lee; J. T. Link; L. Lutz; A. Malinin; J. W. Mitchell; S. Nutter; O. Ofoha; H.B. Jeon; H.J. Hyun; H. Park; J.M. Park; P. Patterson; E. S. Seo; J. Wu; Y.S. Yoon
The Cosmic Ray Energetics And Mass (CREAM) mission is planned for launch in 2015 to the International Space Station (ISS) to research high-energy cosmic rays. Its aim is to understand the acceleration and propagation mechanism of high-energy cosmic rays by measuring their compositions. The Top Counting Detector and Bottom Counting Detector (T/BCD) were built to discriminate electrons from protons by using the difference in cascade shapes between electromagnetic and hadronic showers. The T/BCD provides a redundant instrument trigger in flight as well as a low-energy calibration trigger for ground testing. Each detector consists of a plastic scintillator and two-dimensional silicon photodiode array with readout electronics. The TCD is located between the carbon target and the calorimeter, and the BCD is located below the calorimeter. In this paper, we present the design, assembly, and performance of the T/BCD.
Proceedings of 35th International Cosmic Ray Conference — PoS(ICRC2017) | 2017
J.R. Smith; Y Amare; Tyler Anderson; D Angelaszek; N Anthony; K. Cheryian; G.H. Choi; M. Copley; S. Coutu; Laurent Derome; Ludo Eraud; L Hagenau; J. H. Han; H.G. Huh; S. Im; Jina Jeon; Soomin Jeong; K. C. Kim; M.H. Kim; H.Y. Lee; Junghwi Lee; M.H. Lee; J Liang; J. T. Link; L. Lutz; Arturo Menchaca-Rocha; T Mernik; J. W. Mitchell; S. I. Mognet; S. Morton
The balloon-borne Cosmic Ray Energetics And Mass experiment had its third flight (CREAM-III) over Antarctica for 29 days from December 17, 2007 to January 19, 2008. CREAM-III was designed to directly measure the elemental spectra of cosmic-ray nuclei from Hydrogen to Iron in the energy range from 10^12 to 10^15 eV. Energy of incident cosmic rays was measured with a calorimeter that consisted of a densified carbon target directly above a stack of 20 alternating layers of tungsten and scintillating fiber ribbons. Multiple charge measurements were independently made with the silicon charge detector (SCD), Cherenkov Camera (CherCam), and a Timing Charge Detector (TCD) in order to identify particles and minimize backscattering effects from the calorimeter. Compared to previous CREAM flights, the electronic noise of CREAM-III was reduced, significantly lowering the energy threshold. Results from on-going analysis of the energy spectra will be presented.