Zobrazeno 1 - 10
of 26
pro vyhledávání: '"I. Ziaeian"'
Autor:
C. Hill, Dipti, K. Heinola, A. Dubois, N. Sisourat, A. Taoutioui, H. Agueny, K. Tőkési, I. Ziaeian, C. Illescas, A. Jorge, L. Méndez, A.S. Kadyrov, N.W. Antonio, A.M. Kotian, T. Kirchner, A.C.K. Leung, J. Ko, J.K. Lee, O. Marchuk, M.G. O’Mullane, E. Litherland-Smith, G.I. Pokol, O. Asztalos, P. Balazs, Y. Wu, C.C. Jia, L. Liu, J.G. Wang
Publikováno v:
Nuclear Fusion, Vol 63, Iss 12, p 125001 (2023)
The injection of energetic neutral particles into the plasma of magnetic confinement fusion reactors is a widely-accepted method for heating such plasmas; various types of neutral beam are also used for diagnostic purposes. Accurate atomic data are r
Externí odkaz:
https://doaj.org/article/3e26b4bdfde6491fa20aa81a22d5c3d3
Autor:
I. Ziaeian, K. Tőkési
Publikováno v:
Atoms, Vol 8, Iss 2, p 27 (2020)
The interaction between Be4+ and hydrogen atom is studied using the three-body classical trajectory Monte Carlo method (CTMC) and the quasiclassical trajectory Monte Carlo method of Kirschbaum and Wilets (QTMC-KW). We present total cross sections for
Externí odkaz:
https://doaj.org/article/beee14ae29824a248b0e24f207ee655e
Autor:
S. Soheyli, I. Ziaeian
Publikováno v:
Iranian Journal of Physics Research, Vol 6, Iss 2, Pp 111-121 (2006)
We have calculated the fission fragment angular anisotropy for 16O + 232Th,12C + 236U , 11B + 237 Np , 14 N + 232 Th , 11B + 235U , 12C + 232Th systems with the saddle point statistical model and compared the fission fragment angular anisotropy for t
Externí odkaz:
https://doaj.org/article/4ad5d69ae0ae4a84a3c495edbdd45a40
Publikováno v:
مجله علوم و فنون هستهای, Vol 37, Iss 4, Pp 12-17 (2017)
With the change of an ion trap geometrical shape, ring and end-cap electrodes, and also damping force effects, the first and second stability regions are studied in a stretched Paul ion trap. In this article, according to a new idea, we changed the t
Externí odkaz:
https://doaj.org/article/5c67edbc175546f9a01a1c0ecc75d86e
Publikováno v:
Iranian Journal of Physics Research, Vol 10, Iss 1, Pp 35-40 (2010)
Dynamical behavior of particles in a Paul trap has been investigated by solving the set of differential equations considering the effect of damping force. Positions of the trapped ions as a function of time, ion trajectories and the phase space curve
Externí odkaz:
https://doaj.org/article/bbf6acc97f554d08b404d97b151ee690
Autor:
K. Tőkési, I. Ziaeian
Publikováno v:
Atoms
Volume 8
Issue 2
Atoms, Vol 8, Iss 27, p 27 (2020)
Volume 8
Issue 2
Atoms, Vol 8, Iss 27, p 27 (2020)
The interaction between Be4+ and hydrogen atom is studied using the three-body classical trajectory Monte Carlo method (CTMC) and the quasiclassical trajectory Monte Carlo method of Kirschbaum and Wilets (QTMC-KW). We present total cross sections for
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::32872006ff8811177067d769992eb76a
Publikováno v:
Journal of Mass Spectrometry. 47:484-489
The homotopy analysis method (HAM) is applied to study the behavior of a hyperbolic rods of quadrupole mass filter and a sinusoidal potential form V(ac) cos(Ωt). Numerical computation method of a 20th-order HAM is employed to compare the physical pr
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::0bc7d2ffd58d46c1687730576af3419d
https://doi.org/10.1002/jms.2041
https://doi.org/10.1002/jms.2041
Publikováno v:
International Journal of Mass Spectrometry. 309:63-69
The dynamical behavior of an ion confined in a Paul ion trap supplied with a new periodic impulsional potential in the form as f(t) = V((cos Ωt ⌊ 1 + k cos 2Ωt ⌋)/(1 − k)); 0 ≤ k
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::cffce6adbcd701ab1c51027254dae02d
https://doi.org/10.1016/j.ijms.2011.08.027
https://doi.org/10.1016/j.ijms.2011.08.027
Publikováno v:
International Journal of Mass Spectrometry. 304:25-28
The influence of the ion trap geometrical shape, ring and end-cap electrodes, on the dynamical behavior of the confined ions is studied. At first by considering the geometrical parameter z 0 = ( 1 / n ) r 0 , where n is a real number, in the quadrupo
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::820e068be28622988df9063036b83f24
https://doi.org/10.1016/j.ijms.2011.03.004
https://doi.org/10.1016/j.ijms.2011.03.004
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