8 results on '"V. Nazaryan"'
Search Results
2. Longitudinal-transverse separations of deep-inelastic structure functions at low Q(2) for hydrogen and deuterium
- Author
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R. Asaturyan, J. A. Dunne, A. K. Opper, D. G. Meekins, V. Tvaskis, L Lapikás, J. W. Martin, L. Cole, H. C. Fenker, Ross Milner, A. Uzzle, K. McIlhany, K. Garrow, I. Niculescu, A. Gasparian, B Moreland, V Nazaryan, D. H. Potterveld, H. E. Jackson, B. W. Filippone, J. Arrington, Yoichi Sato, Rolf Ent, M. E. Christy, W. F. Vulcan, Geoffrey Smith, K Spurlock, S. Stepanyan, M Boswell, H. Mkrtchyan, G. van der Steenhoven, P. E. Bosted, A. Cochran, J. H. Mitchell, A. Bruell, Oliver Keith Baker, A. F. Lung, W Seo, Y. Liang, J Crowder, S. A. Wood, D. J. Mack, C. E. Keppel, B. Zihlmann, V. Tadevosian, E. R. Kinney, V. Ziskin, R. B. Piercey, H. P. Blok, Wolfgang Lorenzon, B Rose, J. Gomez, and (Astro)-Particles Physics
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Physics ,Range (particle radiation) ,Hydrogen ,Scattering ,Structure function ,General Physics and Astronomy ,chemistry.chemical_element ,Particle accelerator ,Deep inelastic scattering ,law.invention ,Transverse plane ,Deuterium ,chemistry ,law ,Atomic physics - Abstract
We report on a study of the longitudinal to transverse cross section ratio, R=σL/σT, at low values of x and Q2, as determined from inclusive inelastic electron-hydrogen and electron-deuterium scattering data from Jefferson Laboratory Hall C spanning the four-momentum transfer range 0.06
- Published
- 2007
- Full Text
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3. SU-E-T-470: Beam Performance of the Radiance 330 Proton Therapy System
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F Wang, V Alexandrov, V Nazaryan, J Flanz, and H Nazaryan
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Physics ,Optics ,business.industry ,Radiance ,Dosimetry ,Isocenter ,Bragg peak ,General Medicine ,Beam emittance ,business ,Intensity modulation ,Proton therapy ,Beam (structure) - Abstract
Purpose: The ProTom Radiance 330 proton radiotherapy system is a fully functional, compact proton radiotherapy system that provides advanced proton delivery capabilities. It supports three-dimensional beam scanning with energy and intensity modulation. A series of measurements have been conducted to characterize the beam performance of the first installation of the system at the McLaren Proton Therapy Center in Flint, Michigan. These measurements were part of the technical commissioning of the system. Select measurements and results are presented. Methods: The Radiance 330 proton beam energy range is 70–250 MeV for treatment, and up to 330 MeV for proton tomography and radiography. Its 3-D scanning capability, together with a small beam emittance and momentum spread, provides a highly efficient beam delivery. During the technical commissioning, treatment plans were created to deliver uniform maps at various energies to perform Gamma Index analysis. EBT3 Gafchromic films were irradiated using the Planned irradiation maps. Bragg Peak chamber was used to test the dynamic range during a scan in one layer for high (250 MeV) and Low (70 MeV) energies. The maximum and minimum range, range adjustment and modulation, distal dose falloff (80%–20%), pencil beam spot size, spot placement accuracy were also measured. The accuracy testingmore » included acquiring images, image registration, receiving correction vectors and applying the corrections to the robotic patient positioner. Results: Gamma Index analysis of the Treatment Planning System (TPS) data vs. Measured data showed more than 90% of points within (3%, 3mm) for the maps created by the TPS. At Isocenter Beam Size (One sigma) < 3mm at highest energy (250 MeV) in air. Beam delivery was within 0.6 mm of the intended target at the entrance and the exit of the beam, through the phantom. Conclusion: The Radiance 330 Beam Performance Measurements have confirmed that the system operates as designed with excellent clinical performance specifications. Hovakim Nazaryan, Vahagn Nazaryan and Fuhua Wang are employees of ProTom International, Inc. who contributed to the development and completed the technical commissioning of the Radiance 330 proton therapy delivery system manufactured by ProTom International.« less
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- 2014
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4. Measurement of Pion Transparency in Nuclei
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R. Asaturyan, P. Gueye, Pete Markowitz, G. M. Huber, H. Gao, A. Lung, H. C. Fenker, C. E. Keppel, L. Cole, V. Nazaryan, A. Borissov, S. Stepanyan, D. Gaskell, A. Gasparian, M. K. Jones, Liguang Tang, V. Tadevosyan, B. Hu, W. Lorenzon, H. Mkrtchyan, D. G. Meekins, Oliver Keith Baker, M. E. Christy, S. A. Wood, R. Carlini, Geoffrey Smith, C. Jackson, Kevin Fissum, W. F. Vulcan, D. J. Mack, and J. Arrington
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Nuclear physics ,Physics ,Particle physics ,Pion ,Factorization ,Proton ,Meson ,Color transparency ,Parton ,Transparency (data compression) ,Measure (mathematics) - Abstract
We propose to measure pion electroproduction off {sup 1}H, {sup 2}, {sup 12}C, {sup 64}Cu, and {sup 197}Au, and extract the pion transparency through the nuclear medium between Q{sup 2} = 1 and 5 (GeV/c){sup 2}. The pion transparency is predicted to be a signature of the onset of nuclear filtering and/or Color Transparency. Recent experiments have reported evidence for Color Transparency effects at Q{sup 2} approx 10 (GeV/c){sup 2}. The occurrence of nuclear filtering could potentially explain the apparent discrepancy between (proton) nuclear transparencies found in quasielastic A(e,e'p) and A(p,2p) experiments. The occurrence of these effects is an effective signature of the approach to the factorization regime in meson electroproduction experiments, necessary for the access to Generalized Parton Distributions. Measurable effects of approx. 40% are predicted for this region of Q{sup 2}. The proposed experiment seeks to measure the pion transparency with 5-10% uncertainties, dominated by systematics, up to Q{sup 2} = 5 (GeV/c){sup 2}.
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- 2001
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5. SU-E-T-77: Determination of KQ Factor for PTW Bragg Peak Chamber Used in Proton Pencil Beam Dose Calibration
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Narayan Sahoo, W Hsi, Mark Pankuch, V Nazaryan, B. Arjomandy, and V Kozlyuk
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Physics ,Proton ,business.industry ,Sobp ,Bragg peak ,General Medicine ,Synchrotron ,Pencil (optics) ,law.invention ,Nuclear magnetic resonance ,Optics ,law ,Dosimetry ,business ,Proton therapy ,Beam (structure) - Abstract
Purpose: Dose calibration protocols such as AAPM TG51 for photons and IAEA TR389 for protons recommend using specific KQ quality factor for different ionization chambers for absolute dosimtery in radiation therapy beams. However, there is no quality factor for Bragg Peak chambers (BPC) which are used for proton pencil beams. We have investigated a method to determine the KQ value for this chamber for proton pencil beam dose calibration.Method and Material: A uniform scanning proton beam from a cyclotron accelerator was used to irradiate a PTW‐BPC and an ADCL calibrated IBA‐PPC05 parallel plate chamber (PPC) to obtain the Nw × KQ factor for BPC. Distinctly, measurements of number of protons and the dose were measured simultaneously using the BPC, a Faraday cup, and EBT3 film dosimetry using a single proton pencil beam with a synchrotron accelerator. The calibration of film absolute dosimetry was assessed in a calibrated proton beam with a SOBP width of 10‐cm and range of 16‐cm. The Nw for BPC was determined using TG21 protocol against a PTW‐PPC in a high energy electron beam. Results: Our analysis indicates that KQ for BPC is equal to 1.08 with an uncertainty of ±1%. Independent measurements of the same chamber at different cyclotron proton center produced an agreement of 0.4% for Nw x KQ factor. However, the determination of Nw. KQ of different chamber using a synchrotron proton therapy center disagreed by 6%. The Nw obtained from TG21 protocol was in agreement with manufacturer value to within 0.2%. Conclusion: This investigation produced some results that suggest that there is a possible dose rate dependency of BPC in proton beams. This Result is currently under investigation, but it is believed that the KQ factor is not affected by this dependency.
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- 2013
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6. ChemInform Abstract: MOLECULAR REARRANGEMENTS. XVIII. DETERMINATION OF THE RELATIVE MIGRATION CAPACITY OF BROMINE AND CHLORINE DURING THE OXIDATION OF GEM-BROMOCHLOROOLEFINS BY PER ACIDS
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M. V. Nazaryan and G. M. Shakhnazaryan
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Bromine ,Chemistry ,Inorganic chemistry ,Chlorine ,Organic chemistry ,chemistry.chemical_element ,General Medicine - Published
- 1978
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7. Variations in the RBE for cell killing along the depth-dose profile of a modulated proton therapy beam.
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Britten RA, Nazaryan V, Davis LK, Klein SB, Nichiporov D, Mendonca MS, Wolanski M, Nie X, George J, and Keppel C
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- Animals, Cell Death radiation effects, Cell Line, Tumor, Cricetinae, Dose-Response Relationship, Radiation, Humans, Linear Energy Transfer, Radiation Tolerance, Radiometry, Relative Biological Effectiveness, X-Rays, Proton Therapy
- Abstract
Considerable evidence now exists to show that that the relative biological effectiveness (RBE) changes considerably along the proton depth-dose distribution, with progressively higher RBE values at the distal part of the modulated, or spread out Bragg peak (SOBP) and in the distal dose fall-off (DDF). However, the highly variable nature of the existing studies (with regards to cell lines, and to the physical properties and dosimetry of the various proton beams) precludes any consensus regarding the RBE weighting factor at any position in the depth-dose profile. We have thus conducted a systematic study on the variation in RBE for cell killing for two clinical modulated proton beams at Indiana University and have determined the relationship between the RBE and the dose-averaged linear energy transfer (LETd) of the protons at various positions along the depth-dose profiles. Clonogenic assays were performed on human Hep2 laryngeal cancer cells and V79 cells at various positions along the SOBPs of beams with incident energies of 87 and 200 MeV. There was a marked variation in the radiosensitivity of both cell lines along the SOBP depth-dose profile of the 87 MeV proton beam. Using Hep2 cells, the D(0.1) isoeffect dose RBE values (normalized against (60)Co) were 1.46 at the middle of SOBP, 2.1 at the distal end of the SOBP and 2.3 in the DDF. For V79 cells, the D(0.1) isoeffect RBE for the 87 MEV beam were 1.23 for the proximal end of the SOBP: 1.46 for the distal SOBP and 1.78 for the DDF. Similar D(0.1) isoeffect RBE values were found for Hep2 cells irradiated at various positions along the depth-dose profile of the 200 MeV beam. Our experimentally derived RBE values were significantly correlated (P = 0.001) with the mean LETd of the protons at the various depths, which confirmed that proton RBE is highly dependent on LETd. These in vitro data suggest that the RBE of the proton beam at certain depths is greater than 1.1, a value currently used in most treatment planning algorithms. Thus, the potential for increased cell killing and normal tissue damage in the distal regions of the proton SOBP may be greater than originally thought.
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- 2013
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8. Experimental constraints on polarizability corrections to hydrogen hyperfine structure.
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Nazaryan V, Carlson CE, and Griffioen KA
- Abstract
We present a state-of-the-art evaluation of the polarizability corrections--the inelastic nucleon corrections--to the hydrogen ground-state hyperfine splitting using analytic fits to the most recent data. We find a value Delta(pol)=1.3+/-0.3 ppm. This is 1-2 ppm smaller than the value of Delta(pol) deduced using hyperfine splitting data and elastic nucleon corrections obtained from modern form factor fits.
- Published
- 2006
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