Neven Simicevic
Louisiana Tech University
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Featured researches published by Neven Simicevic.
Physical Review C | 2006
L. Yuan; M. Sarsour; Toshinobu Miyoshi; Zhengmao Zhu; Abdellah Ahmidouch; D. Androic; T. Angelescu; R. Asaturyan; S. Avery; Oliver Keith Baker; I. Bertovic; H. Breuer; Roger Carlini; J. Cha; Robert E. Chrien; M. E. Christy; L. Cole; S. Danagoulian; D. Dehnhard; M. Elaasar; A. Empl; R. Ent; H. Fenker; Yu Fujii; M. Furic; L. Gan; K. Garrow; Ashot Gasparian; P. Gueye; M. Harvey
A pioneering experiment in {lambda} hypernuclear spectroscopy, undertaken at the Thomas Jefferson National Accelerator Facility (J Lab), was recently reported. The experiment used the high precision, continuous electron beam at JLab, and a special arrangement of spectrometer magnets to measure the hypernuclear spectrum from C and {sup 7}Li targets using the (e,eK{sup +}) reaction. The {sub {lambda}}{sup 12}B spectrum found in this investigation was previously published, but is reported here in more detail, with improved resolution. In addition, the results of a {sub {lambda}}{sup 7}He spectrum also obtained in the experiment, are shown. This latter spectrum indicates the need for a more detailed few-body calculation of the hypernucleus and the reaction process. The success of the experiment demonstrates the potential of the (e,eK{sup +}) reaction for high resolution spectroscopy of hypernuclear spectra.
Physical Review Letters | 2013
S. N. Nakamura; A. Matsumura; Y. Okayasu; T. Seva; V. M. Rodriguez; P. Baturin; L. Yuan; A. Acha; A. Ahmidouch; D. Androic; A. Asaturyan; R. Asaturyan; Oliver Keith Baker; F. Benmokhtar; P. Bosted; R. Carlini; Chen Chen; M. E. Christy; L. Cole; S. Danagoulian; A. Daniel; V. Dharmawardane; K. S. Egiyan; M. Elaasar; R. Ent; H. Fenker; Y. Fujii; M. Furic; L. Gan; D. Gaskell
An experiment with a newly developed high-resolution kaon spectrometer and a scattered electron spectrometer with a novel configuration was performed in Hall C at Jefferson Lab. The ground state of a neutron-rich hypernucleus, (Λ)(7)He, was observed for the first time with the (e, eK+) reaction with an energy resolution of ~0.6 MeV. This resolution is the best reported to date for hypernuclear reaction spectroscopy. The (Λ)(7)He binding energy supplies the last missing information of the A = 7, T = 1 hypernuclear isotriplet, providing a new input for the charge symmetry breaking effect of the ΛN potential.
Physics in Medicine and Biology | 2005
Neven Simicevic; Donald T. Haynie
Ultra-wideband (UWB) electromagnetic pulses of nanosecond duration, or nanopulses, are of considerable interest to the communications industry and are being explored for various applications in biotechnology and medicine. The propagation of a nanopulse through biological matter has been computed using the finite difference-time domain (FDTD) method. The approach required the reparametrization of existing Cole-Cole model-based descriptions of dielectric properties of biological matter in terms of the Debye model without loss of accuracy. Several tissue types have been considered. Results show that the electromagnetic field inside biological tissue depends on incident pulse rise time and width. Rise time dominates pulse behaviour inside tissue as conductivity increases. It has also been found that the amount of energy deposited by 20 kV m(-1) nanopulses is insufficient to change the temperature of the exposed material for pulse repetition rates of 1 MHz or less, consistent with recent experimental results.
Physics in Medicine and Biology | 2008
Neven Simicevic
With an increase in the application of ultra-wideband (UWB) electromagnetic pulses in the communications industry, radar, biotechnology and medicine, comes an interest in UWB exposure safety standards. Despite an increase of the scientific research on bioeffects of exposure to non-ionizing UWB pulses, characterization of those effects is far from complete. A numerical computational approach, such as a finite-difference time domain (FDTD) method, is required to visualize and understand the complexity of broadband electromagnetic interactions. The FDTD method has almost no limits in the description of the geometrical and dispersive properties of the simulated material, it is numerically robust and appropriate for current computer technology. In this paper, a complete calculation of exposure of the human eye to UWB electromagnetic pulses in the frequency range of 3.1-10.6, 22-29 and 57-64 GHz is performed. Computation in this frequency range required a geometrical resolution of the eye of 0.1 mm and an arbitrary precision in the description of its dielectric properties in terms of the Debye model. New results show that the interaction of UWB pulses with the eye tissues exhibits the same properties as the interaction of the continuous electromagnetic waves (CWs) with the frequencies from the pulses frequency spectrum. It is also shown that under the same exposure conditions the exposure to UWB pulses is from one to many orders of magnitude safer than the exposure to CW.
Physics in Medicine and Biology | 2005
Neven Simicevic
Ultra-wideband (UWB) electromagnetic pulses of nanosecond duration, or nanopulses, have recently been approved by the Federal Communications Commission for a number of different applications. They are also being explored for applications in biotechnology and medicine. The simulation of the propagation of a nanopulse through biological matter, previously performed using a two-dimensional finite-difference time-domain (FDTD) method, has been extended here into a full three-dimensional computation. To account for the UWB frequency range, the geometrical resolution of the exposed sample was 0.25 mm and the dielectric properties of biological matter were accurately described in terms of the Debye model. The results obtained from the three-dimensional computation support the previously obtained results: the electromagnetic field inside a biological tissue depends on the incident pulse rise time and width, with increased importance of the rise time as the conductivity increases; no thermal effects are possible for the low pulse repetition rates, supported by recent experiments. New results show that the dielectric sample exposed to nanopulses behaves as a dielectric resonator. For a sample in a cuvette, we obtained the dominant resonant frequency and the Q-factor of the resonator.
IEEE Transactions on Instrumentation and Measurement | 2010
Rastko R. Selmic; Atindra K. Mitra; Shravan Challa; Neven Simicevic
Ultra-wideband (UWB) signals exhibit different characteristics upon propagation through matter compared with narrow-band signals. The latter keeps a sinusoidal shape during different forms of signal propagation. The behavior of narrow-band signals does not apply to UWB signals in many cases. Presently, the possibilities for development of UWB signaling technology remain largely unexplored. Few applications have been developed due to strict regulations by the Federal Communications Commission (FCC). In this paper, we describe a series of experiments that have been carried out to determine the behavior of UWB signals and their properties. A transverse electromagnetic (TEM) horn antenna has been made for radiating UWB signals. A procedure for propagating UWB signals through a liquid medium of given salt concentration has been demonstrated, providing a basis for studying UWB signal propagation in biological matter. A new pulsewidth definition was adopted, which is suitable for propagated UWB signals.
Journal of Mathematical Modelling and Algorithms | 2005
Shengjun Su; Weizhong Dai; Donald T. Haynie; Raja Nassar; Neven Simicevic
Short duration, fast rise time ultra-wideband (UWB) electromagnetic pulses (“nanopulses”) are generated by numerous electronic devices in use today. Moreover, many new technologies involving nanopulses are under development and expected to become widely available soon. Study of nanopulse bioeffects is needed to probe their useful range in possible biomedical and biotechnological applications, and to ensure human safety. In this work we develop a computational approach to investigate electromagnetic fields in biological cells exposed to nanopulses. The simulation is based on a z-transformation of the electric displacement and a second-order Taylor approximation of a Cole–Cole expression for the frequency dependence of the dielectric properties of tissues, useful for converting from the frequency domain to the time domain. Maxwell’s equations are then calculated using the finite difference time domain method (FDTD), coupled with a perfectly matched layer to eliminate reflections from the boundary. Numerical results for a biological cell model are presented and discussed.
international symposium on electromagnetic compatibility | 2008
Neven Simicevic
Despite an increase in the application of ultra-wideband (UWB) electromagnetic pulses in the communications industry, radar, biotechnology and medicine, characterization of bioeffects of exposure to non-ionizing UWB radiation is far from complete. In this paper the finite-difference time domain (FDTD) method is used to calculate the bioeffects resulting from the exposure of a human eye to UWB electromagnetic pulses in the frequency range of 3.1-10.6, 22-29, and 57-64 GHz. The results show that the interaction of UWB pulse with the eye tissues exhibits the same properties as the interaction of the continuous electromagnetic wave (CW) with frequency from the pulsepsilas power spectrum. It is also shown that under the same exposure conditions the exposure to UWB pulses is from one to many orders of magnitude safer than the exposure to CW.
Physical Review Letters | 2012
D. Androic; D.S. Armstrong; J. Arvieux; S. L. Bailey; D. Beck; E. J. Beise; J. Benesch; F. Benmokhtar; L. Bimbot; J. Birchall; P. Bosted; H. Breuer; C. L. Capuano; Y. C. Chao; A. Coppens; C. A. Davis; C. Ellis; G. Flores; G. B. Franklin; C. Furget; D. Gaskell; M. T. Gericke; J. Grames; G. Guillard; J. Hansknecht; T. Horn; M. K. Jones; P. M. King; W. Korsch; S. Kox
The parity-violating (PV) asymmetry of inclusive π- production in electron scattering from a liquid deuterium target was measured at backward angles. The measurement was conducted as a part of the G0 experiment, at a beam energy of 360 MeV. The physics process dominating pion production for these kinematics is quasifree photoproduction off the neutron via the Δ0 resonance. In the context of heavy-baryon chiral perturbation theory, this asymmetry is related to a low-energy constant d(Δ)- that characterizes the parity-violating γNΔ coupling. Zhu et al. calculated d(Δ)- in a model benchmarked by the large asymmetries seen in hyperon weak radiative decays, and predicted potentially large asymmetries for this process, ranging from A(γ)-=-5.2 to +5.2u2009u2009ppm. The measurement performed in this work leads to A(γ)-=-0.36±1.06±0.37±0.03u2009u2009ppm (where sources of statistical, systematic and theoretical uncertainties are included), which would disfavor enchancements considered by Zhu et al. proportional to V(ud)/V(us). The measurement is part of a program of inelastic scattering measurements that were conducted by the G0 experiment, seeking to determine the N-Δ axial transition form factors using PV electron scattering.
Journal of Physics: Conference Series | 2011
O. Hashimoto; Y. Fujii; D. Honda; M. Kaneta; F. Kato; D. Kawama; N. Maruyama; A. Matsumura; S. N. Nakamura; Hiroshi Nomura; K. Nonaka; A. Ohtani; Y. Okayasu; M. Osaka; M. Oyamada; M. Sumihama; H. Tamura; Oliver Keith Baker; L. Cole; M. E. Christy; P. Gueye; Cynthia Keppel; L. Tang; L. Yuan; A. Acha; P. Baturin; W. Boeglin; L. Kramer; P. Markowitz; P. Pamela
The binding energy of 7ΛHe has been obtained for the first time with reaction spectroscopy using the (e, eK+) reaction at Jefferson Labs Hall C. A comparison among the binding energies of the A = 7 T = l iso-triplet hypernuclei, 7ΛHe, 7ΛLi*and 7ΛBe, is made and possible charge symmetry breaking (CSB) in the ΛN potential is discussed. For 7ΛHe and 7ΛBe, the shifts in binding energies are opposite to those predicted by a recent cluster model calculation, which assumes that the unexplained part of the binding energy difference between 4ΛH and 4ΛHe, is due to the CSB of the ΛN potential. Further examination of CSB in light hypernuclear systems is required both experimentally and theoretically.