Ioannis G. Tigelis
National and Kapodistrian University of Athens
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Featured researches published by Ioannis G. Tigelis.
IEEE Transactions on Plasma Science | 2010
Gerd Gantenbein; Günter Dammertz; J. Flamm; S. Illy; Stefan Kern; George P. Latsas; Bernhard Piosczyk; T. Rzesnicki; A. Samartsev; A. Schlaich; M. Thumm; Ioannis G. Tigelis
Megawatt gyrotrons are found to suffer from various parasitic oscillations, in particular, RF oscillations in the beam tunnel prior to the desired interaction zone (the cavity). This paper describes the experimental results from a gyrotron experiment which was dedicated to investigate parasitic oscillations in the beam tunnel and to verify improved beam-tunnel structures. A system for improved spectral measurements and a new analysis method are presented. The results verify theoretical predictions on the parasitic oscillations, and in effect validate the corresponding improved beam-tunnel structure. In addition, other types of parasitic oscillations were observed and explained.
IEEE Transactions on Plasma Science | 2006
Zisis C. Ioannidis; O. Dumbrajs; Ioannis G. Tigelis
The authors present the mathematical analysis for the calculation of the dispersion relation, the field distributions, and the ohmic losses for TEm,p modes in an infinite coaxial waveguide with a longitudinally corrugated insert. The method employed is based on an appropriate eigenfunction expansion, and its main advantage is the very fast convergence with a few spatial harmonics. The analysis is properly extended to include tapered cavities with varying, in respect to the z-coordinate, outer and/or inner radius. Numerical results are presented for several tapered cavity geometries and compared with already published methods
IEEE Transactions on Plasma Science | 2014
John Jelonnek; F. Albajar; S. Alberti; Konstantinos A. Avramidis; P. Benin; T. Bonicelli; F. Cismondi; Volker Erckmann; Gerd Gantenbein; Klaus Hesch; Jean-Philippe Hogge; S. Illy; Zisis C. Ioannidis; J. Jin; Heinrich Laqua; George P. Latsas; F. Legrand; G. Michel; Ioannis Gr. Pagonakis; Bernhard Piosczyk; Y. Rozier; T. Rzesnicki; Ioannis G. Tigelis; M. Thumm; M. Q. Tran; John L. Vomvoridis
Europe is devoting significant joint efforts to develop and to manufacture MW-level gyrotrons for electron cyclotron heating and current drive of future plasma experiments. The two most important ones are the stellarator Wendelstein W7-X at Greifswald and the Tokamak ITER at Cadarache. While the series production of the 140 GHz, 1 MW, CW gyrotrons for the 10-MW electron cyclotron resonance heating system of stellarator W7-X is proceeding, the European GYrotron Consortium is presently developing the EU-1 MW, 170 GHz, CW gyrotron for ITER. The initial design had already been initiated in 2007, as a risk mitigation measure during the development of the advanced ITER EU-2-MW coaxial-cavity gyrotron. The target of the ITER EU-1-MW conventional-cavity design is to benefit as much as possible from the experiences made during the development and series production of the W7-X gyrotron and of the experiences gained from the earlier EU-2-MW coaxial-cavity gyrotron design. Hence, the similarity of the construction will be made visible in this paper. During 2012, the scientific design of the ITER EU-1-MW gyrotron components has been finalized. In collaboration with the industrial partner Thales electron devices, Vélizy, France, the industrial design of the technological parts of the gyrotron is being completed. A short-pulse prototype is under development to support the design of the CW prototype tube. The technological path toward the EU ITER-1 MW gyrotron and the final design will be presented.
IEEE Transactions on Plasma Science | 2004
George P. Anastasiou; George P. Latsas; Ioannis G. Tigelis; Micha Dehler; Patrick Queffelec; Nikolaos F. Dasyras
We present the mathematical analysis, based on an eigenfunction expansion, and the main steps of the corresponding numerical code developed to calculate the dispersion relation and the field distributions for all kind of waves, which can propagate in a nonperiodic circumferentially corrugated circular waveguide with losses. The code offers fast computations with accuracy, which can be chosen by the user. Numerical results are given for several geometries and comparison with already established codes is made.
IEEE Transactions on Plasma Science | 2011
Zisis C. Ioannidis; Konstantinos A. Avramides; George P. Latsas; Ioannis G. Tigelis
Coaxial resonant cavities with longitudinal corrugations on the inner conductor are used in high-frequency high-power gyrotrons as means to reduce the number of possible competing modes. For a sufficiently large number of corrugations, the analytical approach usually treats the surface corrugation as a homogeneous surface impedance to obtain simple formulas for the characteristic equation and field components. These formulas can be introduced to interaction codes in a quite straightforward way. Full-wave approaches that account for the azimuthal periodicity of the structure and consider azimuthal spatial harmonics to describe the field distributions have been also employed, increasing though the complexity of the solution and the effort given in numerical calculations. In this paper, a full-wave code is used in an attempt to identify the way that the azimuthal spatial terms contribute to the reformation of the eigenvalue spectrum and propose a criterion for the selection of the spatial terms that should be taken into account for accurate enough calculations.
IEEE Transactions on Plasma Science | 2003
A.A. Maragos; Zisis C. Ioannidis; Ioannis G. Tigelis
We study the dispersion characteristics of a rectangular waveguide grating for microwave amplifier applications. The Floquet theorem and an appropriate standing waves expansion is employed to express the fields in the vacuum region and inside the grooves, respectively. The application of the boundary conditions leads to an infinite system of equations, which is solved numerically by truncation. The main advantage of the procedure employed is that it gives directly and with a few spatial harmonics the dispersion relation. Furthermore, an adequate procedure (simulation tool) has been introduced in order to distinguish the real roots from spurious solutions and it has been found to work effectively for all cases presented in this work. Numerical results are presented for both shallow and deep grooves and comparison with previously published works is made.
IEEE Transactions on Plasma Science | 2009
George P. Latsas; J.L. Vomvoridis; Konstantinos A. Avramides; Ioannis G. Tigelis
A method based on an eigenfunction expansion and the linearized Vlasov equation to study the beam-wave interaction in cylindrical surface corrugated waveguides with losses is presented. The mathematical formulation is described in detail, and numerical results are given in comparison with the literature.
Journal of The Optical Society of America A-optics Image Science and Vision | 2004
Nikolaos F. Dasyras; Ioannis G. Tigelis; Andreas D. Tsigopoulos; Alexander B. Manenkov
For construction of the TE radiation modes of planar waveguides several methods are employed that are based on collocation techniques. The field representation in the core is based on the Lanczos-Fourier sinusoidal series. The numerical codes are very simple and give accurate results. The validity of these methods is checked for constant refractive-index profiles, while numerical results are also given for parabolic profiles. Furthermore, the validity of the orthogonality condition between the guided and the radiation modes is checked. These methods are demonstrated to be effective and can also be employed to study the TM case and waveguides of lossy media, as well as anisotropic and chiral structures.
Physics of Plasmas | 2015
Konstantinos A. Avramidis; Zisis C. Ioannidis; S. Kern; A. Samartsev; I. Gr. Pagonakis; Ioannis G. Tigelis; John Jelonnek
There are cases where gyrotron interaction simulations predict dynamic After-Cavity Interaction (ACI). In dynamic ACI, a mode is excited by the electron beam at a dominant frequency in the gyrotron cavity and, at the same time, this mode is also interacting with the beam at a different frequency in the non-linear uptaper after the cavity. In favor of dynamic ACI being a real physical effect, there are some experimental findings that could be attributed to it, as well as some physical rationale indicating the possibility of a mode being resonant with the beam at different frequencies in different regions. However, the interaction codes used in dynamic ACI prediction up to now are based on simplifications that put questions on their capability of correctly simulating this effect. In this work, the shortcomings of the usual simplifications with respect to dynamic ACI modeling, namely, the trajectory approach and the single-frequency boundary condition, are identified. Extensive simulations of dynamic ACI cases are presented, using several “in-house” as well as commercial codes. We report on the comparison and the assessment of different modeling approaches and their results and we discuss whether, in some cases, dynamic ACI can be a numerical artifact or not. Although the possibility of existence of dynamic ACI in gyrotrons is not disputed, it is concluded that the widely used trajectory approach for gyrotron interaction modeling is questionable for simulating dynamic ACI and can lead to misleading results.
international vacuum electronics conference | 2013
I. Gr. Pagonakis; Gerd Gantenbein; John Jelonnek; J. Jin; S. Illy; Stefan Kern; Bernhard Piosczyk; T. Rzesnicki; M. Thumm; S. Alberti; J.-P. Hogge; C. Schlatter; M. Q. Tran; Konstantinos A. Avramides; J.L. Vomvoridis; A. Bruschi; M. Lontano; O. Dumbrajs; Zisis C. Ioannidis; George P. Latsas; Ioannis G. Tigelis; P. Benin; Y. Rozier; F. Albajar; T. Bonicelli; F. Cismondi
EU is developing a 1 MW cylindrical cavity gyrotron. In the last year the design of the components of the new gyrotron has been finalized while the technological design of the new tube has been defined. In the present paper, the main characteristics of the new EU gyrotron for ITER are presented.