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Featured researches published by Y. Torun.


arXiv: Accelerator Physics | 2004

NEUTRINO FACTORY AND BETA BEAM EXPERIMENTS AND DEVELOPMENT.

Carl H. Albright; V. Barger; John F. Beacom; E. Black; A. Blondel; S. A. Bogacz; S. J. Brice; S. Caspi; W. Chou; M. Cummings; R. Fernow; D. A. Finley; J. Gallardo; S. Geer; M. C. Goodman; D. A. Harris; Patrick Huber; A. Jansson; C. Johnstone; S. Kahn; Daniel M. Kaplan; H. Kirk; T. Kobilarcik; Manfred Lindner; Kirk T. McDonald; Olga Mena; D. Neuffer; V. Palladino; Robert B. Palmer; K. Paul

The long-term prospects for fully exploring three-flavor mixing in the neutrino sector depend upon an ongoing and increased investment in the appropriate accelerator R&D. Two new concepts have been proposed that would revolutionize neutrino experiments, namely the Neutrino Factory and the Beta Beam facility. These new facilities would dramatically improve our ability to test the three-flavor mixing framework, measure CP violation in the lepton sector, and perhaps determine the neutrino mass hierarchy, and, if necessary, probe extremely small values of the mixing angle {theta}{sub 13}. The stunning sensitivity that could be achieved with a Neutrino Factory is described, together with our present understanding of the corresponding sensitivity that might be achieved with a Beta Beam facility. In the Beta Beam case, additional study is required to better understand the optimum Beta Beam energy, and the achievable sensitivity. Neither a Neutrino Factory nor a Beta Beam facility could be built without significant R&D. An impressive Neutrino Factory R&D effort has been ongoing in the U.S. and elsewhere over the last few years and significant progress has been made towards optimizing the design, developing and testing the required accelerator components, and significantly reducing the cost. The recent progress is described here.


Physical Review D | 2011

Forward Neutron Production at the Fermilab Main Injector

T. Nigmanov; D. Rajaram; Michael J. Longo; U. Akgun; G. Aydin; W. Baker; P. D. Barnes; T. Bergfeld; A. Bujak; D. Carey; E. C. Dukes; F. Duru; Gary J. Feldman; A. Godley; E. Gülmez; Y. O. Günaydin; N. Graf; H. R. Gustafson; L. Gutay; E. P. Hartouni; P. Hanlet; M. Heffner; C. Johnstone; Daniel M. Kaplan; O. Kamaev; J. Klay; M. Kostin; D. J. Lange; A. Lebedev; L. C. Lu

We have measured cross sections for forward neutron production from a variety of targets using proton beams from the Fermilab Main Injector. Measurements were performed for proton beam momenta of 58, 84, and 120 GeV/c. The cross section dependence on the atomic weight (A) of the targets was found to vary as A{sup {alpha}}, where {alpha} is 0.46{+-}0.06 for a beam momentum of 58 GeV/c and 0.54{+-}0.05 for 120 GeV/c. The cross sections show reasonable agreement with FLUKA and DPMJET Monte Carlos. Comparisons have also been made with the LAQGSM Monte Carlo.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2010

Charged kaon mass measurement using the Cherenkov effect

N. Graf; A. Lebedev; R. J. Abrams; U. Akgun; G. Aydin; W. Baker; P. D. Barnes; T. Bergfeld; L. Beverly; A. Bujak; D. Carey; C. Dukes; F. Duru; Gary J. Feldman; A. Godley; E. Gulmez; Y. Gunaydin; H.R. Gustafson; L. Gutay; E. P. Hartouni; P. Hanlet; S. Hansen; M. Heffner; C. Johnstone; Daniel M. Kaplan; O. Kamaev; J. Kilmer; J. Klay; M. Kostin; D. J. Lange

The two most recent and precise measurements of the charged kaon mass use X-rays from kaonic atoms and report uncertainties of 14 ppm and 22 ppm yet dier from each other by 122 ppm. We describe the possibility of an independent mass measurement using the measurement of Cherenkov light from a narrow-band beam of kaons, pions, and protons. This technique was demonstrated using data taken opportunistically by the Main Injector Particle Production experiment at Fermi National Accelerator Laboratory which recorded beams of protons, kaons, and pions ranging in momentum from +37 GeV/c to +63 GeV/c. The measured value is 491.3 1.7 MeV/c 2 , which is within 1.4 of the world average. An improvement of two orders of magnitude in precision would make this technique useful for resolving the ambiguity in the X-ray data and may be achievable in a dedicated experiment.


Physical Review D | 2014

Measurement of charged pion production yields off the NuMI target

J. Paley; M. D. Messier; R. Raja; U. Akgun; D. Asner; G. Aydin; W. Baker; P. D. Barnes; T. Bergfeld; L. Beverly; V. Bhatnagar; B. Choudhary; E. C. Dukes; F. Duru; Gary J. Feldman; A. Godley; N. Graf; J. Gronberg; E. Gulmez; Y. Gunaydin; H. R. Gustafson; E. P. Hartouni; P. Hanlet; M. Heffner; Daniel M. Kaplan; O. Kamaev; J. Klay; Arun Kumar; D. J. Lange; A. Lebedev


Nuclear Physics B - Proceedings Supplements | 2011

Hadronic Cross Sections for Neutrino Production in MIPP

J. Paley; R.L. Abrams; U. Akgun; G. Aydin; W. Baker; P. D. Barnes; T. Bergfeld; A. Bujak; D. Carey; C. Dukes; F. Duru; Gary J. Feldman; Y. Fisyak; N. Graf; A. Godley; Y. Gunaydin; H. R. Gustafson; L. Gutay; E. P. Hartouni; P. Hanlet; M. Heffner; J. Hylen; C. Johnstone; Daniel M. Kaplan; O. Kamaev; J. Klay; M. Kostin; D. J. Lange; A. Lebedev; M. J. Longo


Annual Meeting of the Division of Particles and Fields of the American Physical Society, DPF 2006, and the Annual Fall Meeting of the Japan Particle Physics Community | 2006

The main injector particle production experiment (MIPP) at Fermilab

Holger Meyer; Y. Fisyak; R. Winston; R. J. Peterson; E. Swallow; W. Baker; D. Carey; J. Hylen; C. Johnstone; M. Kostin; H. Meyer; N. Mokhov; A. Para; R. Raja; S. Striganov; Gary J. Feldman; A. Lebedev; S. M. Seun; P. Hanlet; O. Kamaev; Daniel M. Kaplan; H. A. Rubin; N. Solomey; Y. Torun; U. Akgun; G. Aydin; F. Duru; E. Gulmez; Y. Gunaydin; Y. Onel

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Daniel M. Kaplan

Illinois Institute of Technology

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O. Kamaev

Illinois Institute of Technology

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P. Hanlet

Illinois Institute of Technology

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A. Godley

University of South Carolina

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