D.E. Wagoner
Fermilab
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Featured researches published by D.E. Wagoner.
Nuclear Instruments and Methods in Physics Research | 1984
B. Cox; G. Hale; P.O. Mazur; R.L. Wagner; D.E. Wagoner; H. Areti; S. Conetti; P. Lebrun; Timothy A. Ryan; J.E. Brau; R. Gearhart
We have measured the response of an electromagnetic shower counter constructed from the new scintillation glass (SCG1-C, Ohara Optical Glass, Inc.) to positrons in the energy range 2 to 17.5 GeV. We have measured the energy resolution of this 18.4 radiation length detector plus its attendant SF5 lead glass shower counter array to be ¿/E = (1.64 ± 0.14)% + (1.13 ± 0.33)%/¿E with the constant term dominated by variations in the conversion point of the positron and shower leakage. We found this counter to be linear over the energy range examined. We have also measured the light output of the SCG1-C counter relative to light output of the SF5 lead glass guard blocks using 17.5 GeV positrons. We find that the SCG1-C counter produces 5.10 ± 0.30 more light at the phototube than the SF5 lead glass counters.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1985
D.E. Wagoner; B. Cox; D.J. Judd; G. Hale; P.O. Mazur; C. T. Murphy; R. Rameika; F. Turkot; S. Conetti; M. Haire; P. Lebrun; C. Leroy; Timothy A. Ryan; L. Turnbull; R. Gearhart; S. Tzamarias
We report the measurement of the energy resolution of a 4×4 array of SCG1-C scintillation glass counters (Ohara Optical Glass Manufacturing Co., Ltd.) exposed to positrons in the energy range of 1 to 25 GeV. Each element of the array was 20.5 radiation lengths long. The resolution of the array was measured both with and without a 3.5 radiation length SCG1-C scintillation glass active converter and 0.2 radiation length hodoscopes used to measure shower position. We obtained an energy resolution ¿/E = (1.63 + 1.46/¿E)% without the active converter and ¿/E = (0.64 + 3.94/¿E)% with the active converter. Performing a partial correction for the average energy loss in the 0.2 radiation length hodoscopes resulted in an energy resolution of ¿/E = (0.50 + 3.43/¿/E)% for the active converter measurement. We also report on the measurement of the absolute number of photons produced by 1 GeV showers, the optical attenuation length for the light produced by showers, the fraction of the total light output that is due to Cerenkov light relative to scintillation light for showers, and the radiation darkening sensitivity of the scintillation glass.
Nuclear Instruments and Methods in Physics Research | 1984
B. Cox; G. Hale; P.O. Mazur; R.L. Wagner; D.E. Wagoner; H. Areti; S. Conetti; P. Lebrun; Timothy A. Ryan; R. Gearhart
We have measured the centroids of high energy electromagnetic showers initiated by positrons in the energy range 2 to 17.5 GeV with a fine grained scintillation hodoscope composed of seven 1 cm wide elements placed behind a 3.6 radiation length (15 cm) converter composed of SCG1-C scintillation glass. A simple first moment calculation using the ionization observed in each element of this hodoscope yields a shower position resolution as a function of energy of: ¿(mm) ¿ 0.7 ± 5.6/¿E(GeV). We present results on the energy dependence of the shower profiles and the ionization measured by this hodoscope.
IEEE Transactions on Nuclear Science | 1984
D.E. Wagoner; B. Cox; D.J. Judd; G. Hale; P.O. Mazur; C. T. Murphy; R. Rameika; F. Turkot; S. Conetti; M. Haire; P. Lebrun; C. Leroy; Timothy A. Ryan; L. Turnbull; R. Gearhart; S. Tzamarias
We report the measurement of the energy resolution of a 4×4 array of SCG1-C scintillation glass counters (Ohara Optical Glass Manufacturing Co., Ltd.) exposed to positrons in the energy range of 1 to 25 GeV. Each element of the array was 20.5 radiation lengths long. The resolution of the array was measured both with and without a 3.5 radiation length SCG1-C scintillation glass active converter and 0.2 radiation length hodoscopes used to measure shower position. We obtained an energy resolution ?/E = (1.63 + 1.46/?E)% without the active converter and ?/E = (0.64 + 3.94/?E)% with the active converter. Performing a partial correction for the average energy loss in the 0.2 radiation length hodoscopes resulted in an energy resolution of ?/E = (0.50 + 3.43/?/E)% for the active converter measurement. We also report on the measurement of the absolute number of photons produced by 1 GeV showers, the optical attenuation length for the light produced by showers, the fraction of the total light output that is due to Cerenkov light relative to scintillation light for showers, and the radiation darkening sensitivity of the scintillation glass.
IEEE Transactions on Nuclear Science | 1984
G. Theodosiou; W. Kononenko; W. Selove; D. Owen; B. Cox; D.E. Wagoner
We have been able to observe and measure both the direct Cherenkov (C) and the Scintillation (S) light components from scintillating glass, distinctly separated in time. This has important implications for hadron calorimetry, electron/hadron separation and low energy particle identification.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1985
B. Cox; C.M. Jenkins; D.J. Judd; G. Hale; P.O. Mazur; C. T. Murphy; R. Rameika; F. Turkot; D.E. Wagoner; S. Conetti; M. Haire; P. Lebrun; C. Leroy; Timothy A. Ryan; D. Stairs; L. Turnbull; R. Gearhart; M. Abolins; D. Owen; S. Tzamarias
An SCG1-C scintillation glass detector consisting of a 3.5 radiation length SCG1-C active converter followed by scintillation and gas tube hodoscopes and a 4 × 4 array of a 20.5 radiation length SCG1-C counters has been exposed to pions in the 4–14 GeV/c momentum range. The response of this detector to pions is compared with the response to electrons of the same momentum in order to study the capability of such a detector to distinguish the two types of particles. Using only longitudinal and tranverse shower development criteria, the electrons and pions can be separated such that on average 1.1 × 10−1 of all pions in the range of 4–14 Gev/c would be misidentified as electrons of any energy. If the momentum of the incident particle is known and can be used in the identification technique, this average fraction is reduced to 6.4 × 10−3 of all pions misidentified as electrons of the same momentum.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1985
R. Rameika; B. Cox; C.M. Jenkins; D.J. Judd; G. Hale; P.O. Mazur; C. T. Murphy; F. Turkot; D.E. Wagoner; S. Conetti; M. Haire; P. Lebrun; C. Leroy; Timothy A. Ryan; L. Turnbull; R. Gearhart; C.H. Shen
A hodoscope has been constructed from 100 μm diameter wires and brass tubes (1.2 × 0.7 cm2 cross section) filled with a mixture of argon, ethane and ethyl alcohol. It has been tested in the saturated avalanche mode in an SCG1-C electromagnetic shower detector to determine its properties for the measurement of the position and size of electromagnetic showers. Two of these tube hodoscopes were positioned 3.5 radiation lengths deep in the detector and the profiles of 1–25 GeV electromagnetic showers were measured. Simultaneous measurements were performed using a plane of twenty, 0.5 cm wide scintillation counters positioned immediately behind the gas tube hodoscope. In addition the transition between saturated avalanche and limited streamer modes was observed for the tube hodoscopes.
IEEE Transactions on Nuclear Science | 1983
B. Cox; G. Hale; P.O. Mazur; R.L. Wagner; D.E. Wagoner; H. Areti; S. Conetti; P. Lebrun; Timothy A. Ryan; J.E. Brau; R. Gearhart
We have measured the response of an electromagnetic shower counter constructed from the new scintillation glass (SCG1-C, Ohara Optical Glass, Inc.) to positrons in the energy range 2 to 17.5 GeV. We have measured the energy resolution of this 18.4 radiation length detector plus its attendant SF5 lead glass shower counter array to be ?/E = (1.64 ± 0.14)% + (1.13 ± 0.33)%/?E with the constant term dominated by variations in the conversion point of the positron and shower leakage. We found this counter to be linear over the energy range examined. We have also measured the light output of the SCG1-C counter relative to light output of the SF5 lead glass guard blocks using 17.5 GeV positrons. We find that the SCG1-C counter produces 5.10 ± 0.30 more light at the phototube than the SF5 lead glass counters.
IEEE Transactions on Nuclear Science | 1989
C.M. Jenkins; M. Arenton; T. Chen; S. Conetti; B. Cox; S. Delchamps; B. Etemadi; L. Fortney; K. Guffey; M. Haire; P. Ioannu; D.J. Judd; C. Kourkoumelis; I. Koutentakis; J. Kuzminski; K.W. Lai; A. Manousakis-Katsikakis; He Mao; A. Marchionni; P.O. Mazur; C. T. Murphy; T. Pramantiotis; R. Rameika; L.K. Resvanis; M. Rosati; J. Rosen; C.H. Shen; Q. Shen; A. Simard; R. Smith
A fine-grain hodoscope to measure the position of showers in the outer (>52 cm) region of the E-705 electromagnetic calorimeter is described. The hodoscope is constructed with two layers of vertical conducting plastic tubes for the X position measurement of showers. Y position measurement of showers was accomplished by cathode-induced horizontal strips. A 50/50-ethane mixture bubbled through isopropyl alcohol at 0 degrees C was circulated through the tubes in parallel. The tubes were operated at +1.925 kV on the wire (below the region of saturated avalanche) in the limited proportionality mode. The hodoscope is described, and results are presented for the position resolution, shower width, and charge detected as a function of calibration electron energy. >
IEEE Transactions on Nuclear Science | 1984
R. Rameika; B. Cox; C.M. Jenkins; D.J. Judd; G. Hale; P.O. Mazur; C. T. Murphy; F. Turkot; D.E. Wagoner; S. Conetti; M. Haire; P. Lebrun; C. Leroy; Timothy A. Ryan; L. Turnbull; R. Gearhart; C.H. Shen
A hodoscope has been constructed from 100 ¿m diameter wires and brass tubes (1.2 × 0.7 cm2 cross section) filled with a mixture of argon, ethane and ethyl alchohol. It has been tested in the saturated avalanche mode in an SCG1-C electromagnetic shower detector to determine its properties for the measurement of the position and size of electromagnetic showers. Two of these tube hodoscopes were positioned 3.5 radiation lengths deep in the detector and the profiles of 1-25 GeV electromagnetic showers were measured. Simultaneous measurements were performed using a plane of twenty, 0.5 cm wide scintillation counters positioned immediately behind the gas tube hodoscope. In addition the transition between saturated avalanche and limited streamer modes has been measured for the tube hodoscopes.