نتایج جستجو برای: 6 mev electron beam

تعداد نتایج: 1335450  

2009
M. Lavalle P. G. Fuochi A. Martelli U. Corda A. Kovács K. Mehta F. Kuntz S. Plumeri

An easy-to-use and robust energy monitoring device has been developed for reliable detection of dayto-day small variations in the electron beam energy, a critical parameter for quality control and quality assurance in industrial radiation processing. It has potential for using on-line, thus providing real-time information. Its working principle is based on the measurement of currents, or charge...

2000
C. Vermare D. C. Moir G. J. Seitz

By using the OTR angular distribution property [1], it is possible to extract the energy and the angular dispersion of several kinds of beam [2]. Recently, Le Sage et al. [3] succeeded in producing a transverse phase-space mapping of a 100 MeV electron beam by coupling an interferometric measurement and a ’’mask’’ technique. We present the first OTR time resolved angular distribution measuremen...

Introduction: In clinical electron beams, most of bremsstrahlung radiation is produced by various linac head structures. This bremsstrahlung radiation dose is influenced by the geometry and construction of every component of the linac treatment head structures. Thus, it can be expected that the amount of the contaminated photon dose due to bremsstrahlung radiation varies among different linacs,...

2000
James F. Mccarrick Arthur C. Paul Stephen Sampayan Li-Fang Wang John T. Weir

We have modified the single pulse target experimental facility[1] on the Experimental Test Accelerator II (ETAII) to perform the double pulse target experiments to validate the DARHT-II[2, 3] multi-pulse target concept. The 1.15 MeV, 2 kA Snowtron injector will provide the first electron pulse. The 6 MeV, 2 kA ETA-II beam will be used as the probe beam. Our modeling indicates that the ETA-II/Sn...

2015
NASHAAT A. DEIAB SHAYMAA Z. ABDEL KADER MOHAMED EL-NAGDY Nashaat A. Deiab

Purpose: This study was to investigate the effect of irregularity in shape of field size of electron beam on the percentage depth dose and the output factor. Study the variety of the Percentage Depth Dose (PDD) and the output factors for rectangular and small field sizes when one of field dimensions less than the Practical Range (Rp) of the electron energy used. Compare the measured output fact...

2001
T. J. ORZECHOWSKI

High-power free electron lasers (FEL’s) can be realized using induction linear accelerators as the source of the electron beam. These accelerators are currently capable of producing intense cwrents (102-104 A) at moderately high energy (1-50 MeV). Experiments using a 500 A, 3.3 MeV beam have produced 80 MW of radiation at 34.6 GHz and are in good agreement with theoretical analysis. Future expe...

Journal: :iranian journal of radiation research 0
n. jabbari department of medical physics and imaging, urmia university of medical sciences, urmia, iran h. nedaie department of radiotherapy, cancer institute, tehran university of medical science, tehran, iran a. zeinali department of medical physics and imaging, urmia university of medical sciences, urmia, iran

background: understanding of the incident electron energy and angular distributions from clinical electron accelerators (linacs) is important for dosimetry and treatment planning. the most important goals of this study were to evaluate the energy fluence and angular distributions of electron beams from a neptun 10pc linac using the monte carlo (mc) code. materials and methods: the linac electro...

Journal: :iranian journal of radiation research 0
s.r.m. mahdavi department of medical physics, tehran university of medical sciences, tehran, iran m. mahdavi department of physics, faculty of basic sciences, mazandaran university, babolsar, iran h. alijanzadeh department of physics, faculty of basic sciences, mazandaran university, babolsar, iran m. zabihzadeh department of medical physics, joundishapour university of medical sciences, ahvaz, iran a. mostaar department of medical physics, faculty of medicine, shahid beheshti university of medical sciences, tehran, iran

background: two protocols of aapm tg-51 and iaea trs-398 were compared followed by a measurement and monte carlo simulation of beam quality correction factor, kq, aapm tg-51 and iaea trs-398 protocols were compared for the absorbed dose to water for dw, and kq parameters. materials and methods: dose measurements by either protocols were performed with cylindrical and plane parallel chambers for...

Journal: :Physical review letters 2016
D Abbott P Adderley A Adeyemi P Aguilera M Ali H Areti M Baylac J Benesch G Bosson B Cade A Camsonne L S Cardman J Clark P Cole S Covert C Cuevas O Dadoun D Dale H Dong J Dumas E Fanchini T Forest E Forman A Freyberger E Froidefond S Golge J Grames P Guèye J Hansknecht P Harrell J Hoskins C Hyde B Josey R Kazimi Y Kim D Machie K Mahoney R Mammei M Marton J McCarter M McCaughan M McHugh D McNulty K E Mesick T Michaelides R Michaels B Moffit D Moser C Muñoz Camacho J-F Muraz A Opper M Poelker J-S Réal L Richardson S Setiniyaz M Stutzman R Suleiman C Tennant C Tsai D Turner M Ungaro A Variola E Voutier Y Wang Y Zhang

The Polarized Electrons for Polarized Positrons experiment at the injector of the Continuous Electron Beam Accelerator Facility has demonstrated for the first time the efficient transfer of polarization from electrons to positrons produced by the polarized bremsstrahlung radiation induced by a polarized electron beam in a high-Z target. Positron polarization up to 82% have been measured for an ...

Journal: :Physical review letters 2014
G Sarri D J Corvan W Schumaker J M Cole A Di Piazza H Ahmed C Harvey C H Keitel K Krushelnick S P D Mangles Z Najmudin D Symes A G R Thomas M Yeung Z Zhao M Zepf

We report on the generation of a narrow divergence (θ_{γ}<2.5  mrad), multi-MeV (E_{max}≈18  MeV) and ultrahigh peak brilliance (>1.8×10^{20}  photons s^{-1} mm^{-2}  mrad^{-2} 0.1% BW) γ-ray beam from the scattering of an ultrarelativistic laser-wakefield accelerated electron beam in the field of a relativistically intense laser (dimensionless amplitude a_{0}≈2). The spectrum of the generated ...

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