L. Giudicotti
European Atomic Energy Community
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Featured researches published by L. Giudicotti.
Nuclear Fusion | 2009
P. Martin; L. Apolloni; M. E. Puiatti; J. Adamek; M. Agostini; A. Alfier; Silvia Valeria Annibaldi; V. Antoni; F. Auriemma; O. Barana; M. Baruzzo; P. Bettini; T. Bolzonella; D. Bonfiglio; M. Brombin; J. Brotankova; A. Buffa; Paolo Buratti; A. Canton; S. Cappello; L. Carraro; R. Cavazzana; M. Cavinato; B.E. Chapman; G. Chitarin; S. Dal Bello; A. De Lorenzi; G. De Masi; D. F. Escande; A. Fassina
With the exploration of the MA plasma current regime in up to 0.5 s long discharges, RFX-mod has opened new and very promising perspectives for the reversed field pinch (RFP) magnetic configuration, and has made significant progress in understanding and improving confinement and in controlling plasma stability. A big leap with respect to previous knowledge and expectations on RFP physics and performance has been made by RFX-mod since the last 2006 IAEA Fusion Energy Conference. A new self-organized helical equilibrium has been experimentally achieved (the Single Helical Axis—SHAx—state), which is the preferred state at high current. Strong core electron transport barriers characterize this regime, with electron temperature gradients comparable to those achieved in tokamaks, and by a factor of 4 improvement in confinement time with respect to the standard RFP. RFX-mod is also providing leading edge results on real-time feedback control of MHD instabilities, of general interest for the fusion community.
Plasma Physics and Controlled Fusion | 2007
L. Marrelli; P. Zanca; M. Valisa; G. Marchiori; A. Alfier; M. Gobbin; P. Piovesan; D. Terranova; M. Agostini; C. Alessi; V. Antoni; L. Apolloni; Finizia Auriemma; O. Barana; P. Bettini; T. Bolzonella; D. Bonfiglio; M Brombin; A. Buffa; A. Canton; S. Cappello; L. Carraro; R. Cavazzana; M Cavinato; G. Chitarin; S. Dal Bello; A. De Lorenzi; D. F. Escande; A. Fassina; P. Franz
RFX-mod is a reversed field pinch (RFP) experiment equipped with a system that actively controls the magnetic boundary. In this paper we describe the results of a new control algorithm, the clean mode control (CMC), in which the aliasing of the sideband harmonics generated by the discrete saddle coils is corrected in real time. CMC operation leads to a smoother (i.e. more axisymmetric) boundary. Tearing modes rotate (up to 100 Hz) and partially unlock. Plasma–wall interaction diminishes due to a decrease of the non-axisymmetric shift of the plasma column. With the ameliorated boundary control, plasma current has been successfully increased to 1.5 MA, the highest for an RFP. In such regimes, the magnetic dynamics is dominated by the innermost resonant mode, the internal magnetic field gets close to a pure helix and confinement improves.
Plasma Physics and Controlled Fusion | 2009
M. E. Puiatti; A. Alfier; Finizia Auriemma; S. Cappello; L. Carraro; R. Cavazzana; S. Dal Bello; A. Fassina; D. F. Escande; P. Franz; M. Gobbin; P. Innocente; R. Lorenzini; L. Marrelli; P. Martin; P. Piovesan; I. Predebon; F. Sattin; G. Spizzo; D. Terranova; M. Valisa; B. Zaniol; L. Zanotto; Matteo Zuin; M. Agostini; V. Antoni; L. Apolloni; M. Baruzzo; T. Bolzonella; D. Bonfiglio
The reversed field pinch configuration is characterized by the presence of magnetic structures both in the core and at the edge: in the core, at high plasma current the spontaneous development of a helical structure is accompanied by the appearance of internal electron transport barriers; at the edge strong pressure gradients, identifying an edge transport barrier, are observed too, related to the position of the field reversal surface.The aim of this paper is the experimental characterization of both the internal and edge transport barriers in relation to the magnetic topology, discussing possible analogies and differences with other confinement schemes.
Plasma Physics and Controlled Fusion | 2008
M. Valisa; T. Bolzonella; P. Buratti; L. Carraro; R. Cavazzana; S. Dal Bello; P. Martin; R. Pasqualotto; J.S. Sarff; M. Spolaore; P. Zanca; L. Zanotto; M. Agostini; A. Alfier; V. Antoni; L. Apolloni; F. Auriemma; O. Barana; M. Baruzzo; P. Bettini; D. Bonfiglio; M. Brombin; A. Buffa; A. Canton; S. Cappello; M. Cavinato; G. Chitarin; A. De Lorenzi; G. De Masi; D. F. Escande
Optimization of machine operation, including plasma position control, density control and especially feedback control on multiple magnetohydrodynamic modes, has led RFX-mod to operate reliably at 1.5?MA, the highest current ever achieved on a reversed field pinch (RFP). At high current and low density the magnetic topology spontaneously self-organizes in an Ohmical helical symmetry, with the new magnetic axis helically twisting around the geometrical axis of the torus. The separatrix of the island disappears leaving a wide and symmetric thermal structure with large gradients in the electron temperature profile. The new topology still displays an intermittent nature but its overall presence has reached 85% of the current flat-top period. The large gradients in the electron temperature profile appear to be marginal for the destabilization of ion temperature gradient modes on the assumption that ions and electrons have the same gradients. There are indications that higher currents could provide the conditions under which to prove the existence of a true helical equilibrium as the standard RFP configuration.
Review of Scientific Instruments | 2001
R. Pasqualotto; P. Nielsen; L. Giudicotti
The present Thomson scattering system at the reversed field experiment routinely determines electron temperature and density profiles in various modes of operation but only provides a single profile of each discharge. The new system will use a Nd:YLF laser providing measurements every 20 ms. At the same time we wish to improve the accuracy of the measurement: to this end a new detection system based on filter spectrometers and avalanche photodiodes has been built. The higher throughput of the spectrometers and the higher quantum efficiency of the detectors give an improvement of signal to noise levels of almost two orders. To improve dynamic range the output is ac coupled. Noise figure of detectors has been investigated in detail. The system is novel in the way data are recorded using transient recorders with multiplexing of two channels on each input. The effective accuracy and dynamic range of this system is compared to charge integrating systems. With a look to the future we have also investigated the ...
Nuclear Fusion | 2003
M. E. Puiatti; S. Cappello; R. Lorenzini; S. Martini; S. Ortolani; R. Paccagnella; F. Sattin; D. Terranova; T. Bolzonella; A. Buffa; A. Canton; L. Carraro; D. F. Escande; L. Garzotti; P. Innocente; L. Marrelli; E. Martines; P. Scarin; G. Spizzo; M. Valisa; P. Zanca; V. Antoni; L. Apolloni; M. Bagatin; W. Baker; O. Barana; D. Bettella; P. Bettini; R. Cavazzana; M. Cavinato
In this paper, we analyse the main features of the pulsed poloidal current drive (PPCD) technique, used in the reversed field pinch configuration to achieve improved confinement conditions. In the RFX experiment, PPCD corresponds to a decrease of the magnetic fluctuations, to a peaking of the temperature profile, and to a reduced transport and plasma–wall interaction. A three-dimensional MHD nonlinear code and one-dimensional time-dependent transport models have been applied to study the effect of PPCD on the magnetic and plasma profiles. The three-dimensional MHD simulations show that the external inductive drive pinches and peaks the current profile driving the configuration through a transient phase, where the spontaneous turbulent dynamo action is quenched. The one-dimensional transport codes indicate that the experimental profile modifications associated with PPCD are consistent with a reduction of the stochastic transport.
Review of Scientific Instruments | 2008
M. Kempenaars; J.C. Flanagan; L. Giudicotti; M. J. Walsh; M. Beurskens; I. Balboa; Jet-Efda Contributors
The edge light detection and ranging (LIDAR) Thomson scattering diagnostic at the Joint European Torus fusion experiment uses a 3 J ruby laser to measure the electron density and temperature profile at the plasma edge. The original system used a 1 GHz digitizer and detectors with response times of approximately 650 ps and effective quantum efficiencies <7%. This system has recently been enhanced with the installation of a new 8 GHz digitizer and four new ultrafast GaAsP microchannel plate photomultiplier tube detectors with response times of <300 ps and effective quantum efficiencies in the range of approximately 13%-20% (averaged over lambda=500-700 nm). This upgrade has enabled the spatial resolution to be reduced to approximately 6.3 cm along the laser line of sight for a laser pulse of 300 ps full width at half maximum, which is close to the requirements for the ITER core LIDAR. Performance analysis shows that the new system will have an effective spatial resolution of up to 1 cm in the magnetic midplane via magnetic flux surface mapping.
Review of Scientific Instruments | 2008
M. N. A. Beurskens; L. Giudicotti; M. Kempenaars; R. Scannell; M. J. Walsh
The core LIDAR Thomson scattering for ITER is specified for core profile measurements with a spatial resolution of 7 cm (a/30) for the range of 500 eV3x10(19) m(-3) at an accuracy of <10% for T(e). These specifications are verified using a full profile Monte Carlo simulation code. In the simulations it is assumed that the input transmission is 50% and the collection transmission is 10% for lambda=300-1200 nm and F/#=6-17. A crucial design decision lies on the choice of laser and detector combination. It is evaluated that the system can meet its spatial and accuracy specifications for higher temperatures of T(e)>5 keV with a combination of a neodymium-doped yttrium aluminum garnet (Nd:YAG) laser (lambda(0)=1064 nm, Delta lambda<1 nm, 5 J, and Delta t(FWHM)=250 ps, 5-10 Hz) and S20, GaAs, and GaAsP microchannel plate photomultipliers (Delta t(FWHM)<300 ps, effective quantum efficiency, EQE=3%-4%, and D=18 mm). In order to reach the required T(e) of 500 eV with Nd:YAG first harmonic, this choice requires a development of fast near infrared detectors.
Nuclear Fusion | 1999
R. Bartiromo; A. Buffa; V. Antoni; L. Apolloni; M. Bagatin; W. Baker; F. Bellina; P. Bettini; R. Bilato; T. Bolzonella; A. Canton; S. Cappello; L. Carraro; R. Cavazzana; G. Chitarin; S. Costa; F. D'Angelo; A. De Lorenzi; G. De Pol; D. Desideri; D. F. Escande; P. Fiorentin; P. Franz; E. Gaio; L. Garzotti; L. Giudicotti; F. Gnesotto; D. Gregoratto; S. C. Guo; P. Innocente
The article presents an overview of recent experimental results obtained on the RFX device. The authors obtained and studied a reversed field pinch plasma with a plasma current of up to 1 MA, negligible radiation losses and low effective charge. The local power and particle balance shows that in standard operation the plasma core is dominated by magnetic turbulence and that the global confinement is mainly provided by the edge region, where a strongly sheared radial electric field is present. With poloidal current drive the amplitude of magnetic fluctuations and the thermal conductivity of the plasma core are reduced, leading to improved confinement. Reduced heat transport is also observed when the width of the n spectrum of magnetic fluctuations is reduced.
Plasma Physics and Controlled Fusion | 1993
V. Antoni; L. Apolloni; M. Bagatin; W. Baker; M. Bassan; F. Bellina; L. Benfatto; H. Bergsaker; A. Buffa; P. Campostrini; S. Cappello; L. Carraro; E. Casarotto; G. Chitarin; P. Collarin; S. Costa; A. De Lorenzi; D. Desideri; M. Fauri; C. Ferrer; P. Fiorentin; E. Gaio; L. Giudicotti; F. Gnesotto; Massimo Guarnieri; R. Guatieri; O.N. Hemming; P. Innocente; P. Kusstatscher; A. Luchetta
The results of the first year of operation of the experiment RFX are reported. Profiles of electron density, electron and ion temperature and impurity emission have been measured at plasma current I<0.7 MA. The energy confinement parameters at different density are reported, the best values ( tau E approximately 1ms, beta theta approximately 8%) being obtained operating at higher density. The role of the impurity content in determining the present performance of the experiment is discussed.