A. K. Ciftci
Ankara University
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Publication
Featured researches published by A. K. Ciftci.
International Journal of Modern Physics A | 2004
B. Badelek; C. Blochinger; J. Blumlein; E. Boos; R. Brinkmann; H. Burkhardt; P. Bussey; C. Carimalo; J. Chyla; A. K. Ciftci; W. Decking; A. De Roeck; Fadin; M. Ferrario; A.J. Finch; H. Fraas; F. Franke; M. Galynskii; A. Gamp; I. Ginzburg; Rohini M. Godbole; Ds Gorbunov; G. J. Gounaris; Kaoru Hagiwara; L. Han; R. D. Heuer; C. Heusch; J. Illana; Ilyin; P. Jankowski
High energy photon colliders (γγ,γe) are based on e-e- linear colliders where high energy photons are produced using Compton scattering of laser light on high energy electrons just before the interaction point. This paper is a part of the Technical Design Report of the linear collider TESLA.1 Physics program, possible parameters and some technical aspects of the photon collider at TESLA are discussed.
arXiv: High Energy Physics - Experiment | 2001
B. Badelek; C. Blochinger; J. Blumlein; E. Boos; R. Brinkmann; H. Burkhardt; P. Bussey; C. Carimalo; J. Chyla; A. K. Ciftci; W. Decking; A. De Roeck; V. Fadin; M. Ferrario; A.J. Finch; H. Fraas; F. Franke; M. Galynskii; A. Gamp; I. Ginzburg; Rohini M. Godbole; Ds Gorbunov; G. J. Gounaris; Kaoru Hagiwara; L. Han; R. D. Heuer; C. Heusch; J. Illana; V. Ilyin; P. Jankowski
High energy photon colliders (γγ,γe) are based on e-e- linear colliders where high energy photons are produced using Compton scattering of laser light on high energy electrons just before the interaction point. This paper is a part of the Technical Design Report of the linear collider TESLA.1 Physics program, possible parameters and some technical aspects of the photon collider at TESLA are discussed.
Physics Letters B | 1995
A. Çelikel; A. K. Ciftci; S. Sultansoy
Abstract Arguments favouring the existence of a fourth fermion family in the framework of the Standard Model are given. The masses of the fourth family neutrino, charged lepton and down quark are close to each other within an accuracy of the order of a few GeV and lie between 300–700 GeV. Experiments on the search for these particles are discussed.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995
A. K. Ciftci; S. Sultansoy; Ş. Türköz; O. Yavas
The main parameters of TeV energy γp colliders have been investigated for PHERA+LC, LHC+TESLA and LHC+e-Linac proposals in detail. In this research, the luminosity of γp collisions and the helicity of the high energy γ beam for these colliders are studied in terms of the distance between the conversion region and the collision point as well as γp invariant mass. The main design problems are also discussed.
Physical Review D | 2005
A. K. Ciftci; R. Çiftçi; S. Sultansoy
It is known that flavor democracy favors the existence of the fourth standard model (SM) family. In order to give nonzero masses for the first three-family fermions flavor democracy has to be slightly broken. A parametrization for democracy breaking, which gives the correct values for fundamental fermion masses and, at the same time, predicts quark and lepton Cabibbo-Kobayashi-Maskawa (CKM) matrices in a good agreement with the experimental data, is proposed. The pair productions of the fourth SM family Dirac
arXiv: High Energy Physics - Experiment | 2000
A. K. Ciftci; S. Sultansoy; O. Yavas
({\ensuremath{\nu}}_{4})
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2007
H. Aksakal; A. K. Ciftci; Z. Nergiz; Daniel Schulte; F. Zimmermann
and Majorana
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1999
H. Aktaş; N. Büget; A. K. Ciftci; N. Meriç; S. Sultansoy; O. Yavas
({N}_{1})
Physics Letters B | 1995
A. K. Ciftci; S. Sultansoy; Ş. Türköz
neutrinos at future linear colliders with
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2001
A. K. Ciftci; S. Sultansoy; O. Yavas
\sqrt{s}=500\text{ }\text{ }\mathrm{GeV}