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Dive into the research topics where O. Meneghini is active.

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Featured researches published by O. Meneghini.


Physics of Plasmas | 2010

Absorption of lower hybrid waves in the scrape off layer of a diverted tokamak

G.M. Wallace; R.R. Parker; P.T. Bonoli; A. Hubbard; J.W. Hughes; B. LaBombard; O. Meneghini; A.E. Schmidt; S. Shiraiwa; D.G. Whyte; John Wright; S.J. Wukitch; R. W. Harvey; A. P. Smirnov; J. R. Wilson

The goal of the Lower Hybrid Current Drive (LHCD) system on the Alcator C-Mod tokamak [Hutchinson et al., Phys. Plasmas 1, 1511 (1994)] is to investigate current profile control under plasma conditions relevant to future tokamak experiments. Experimental observations of a LHCD “density limit” for C-Mod are presented in this paper. Bremsstrahlung emission from relativistic fast electrons in the core plasma drops suddenly above line averaged densities of 1020 m−3 (ω/ωLH∼3–4), well below the density limit previously observed on other experiments (ω/ωLH∼2). Electric currents flowing through the scrape off layer (SOL) between the inner and outer divertors increase dramatically across the same density range that the core bremsstrahlung emission drops precipitously. These experimental x-ray data are compared to both conventional modeling, which gives poor agreement with experiment above the density limit and a model including collisional absorption in the SOL, which dramatically improves agreement with experimen...


Nuclear Fusion | 2011

Lower hybrid current drive at high density in Alcator C-Mod

G.M. Wallace; A. Hubbard; P.T. Bonoli; I. Faust; R. W. Harvey; J.W. Hughes; B. LaBombard; O. Meneghini; R.R. Parker; Andrea Schmidt; S. Shiraiwa; A. P. Smirnov; D.G. Whyte; J. R. Wilson; John Wright; S.J. Wukitch

Experimental observations of lower hybrid current drive (LHCD) at high density on the Alcator C-Mod tokamak are presented in this paper. Bremsstrahlung emission from relativistic fast electrons in the core plasma drops suddenly above line-averaged densities of 1020 m−3 (ω/ωLH ~ 3) in single null discharges with large (≥8 mm) inner gaps, well below the density limit previously observed on limited tokamaks (ω/ωLH ~ 2). Modelling and experimental evidence suggest that the absence of LHCD driven fast electrons at high density may be due to parasitic collisional absorption in the scrape-off layer (SOL). Experiments show that the population of fast electrons produced by LHCD at high density ( 10^{20}\,{\rm m}^{-3} SRC=http://ej.iop.org/images/0029-5515/51/8/083032/nf381190in001.gif/>) can be increased by operating with an inner gap of less than ~5 mm with the strongest non-thermal emission in inner wall limited plasmas. A change in plasma topology from single to double null produces a modest increase in non-thermal emission at high density. Increasing the electron temperature in the periphery of the plasma (0.8 > r/a > 1.0) also results in a modest increase in non-thermal electron emission above the density limit. Ray tracing/Fokker–Planck simulations of these discharges predict the observed sensitivity to plasma position when the effects of collisional absorption in the SOL are included in the model.


Physics of Plasmas | 2009

Full wave simulation of lower hybrid waves in Maxwellian plasma based on the finite element method

O. Meneghini; S. Shiraiwa; R.R. Parker

A full wave simulation of the lower-hybrid (LH) wave based on the finite element method is presented. For the LH wave, the most important terms of the dielectric tensor are the cold plasma contribution and the electron Landau damping (ELD) term, which depends only on the component of the wave vector parallel to the background magnetic field. The nonlocal hot plasma ELD effect was expressed as a convolution integral along the magnetic field lines and the resultant integro-differential Helmholtz equation was solved iteratively. The LH wave propagation in a Maxwellian tokamak plasma based on the Alcator C experiment was simulated for electron temperatures in the range of 2.5–10 keV. Comparison with ray tracing simulations showed good agreement when the single pass damping is strong. The advantages of the new approach include a significant reduction of computational requirements compared to full wave spectral methods and seamless treatment of the core, the scrape off layer and the launcher regions.


Physics of Plasmas | 2011

Full wave effects on the lower hybrid wave spectrum and driven current profile in tokamak plasmas

Syun'ichi Shiraiwa; Jinseok Ko; O. Meneghini; R.R. Parker; A.E. Schmidt; S. Scott; M. Greenwald; A. Hubbard; J.W. Hughes; Y. Ma; Y. Podpaly; J. E. Rice; G. Wallace; J. R. Wilson; S.M. Wolfe

A numerical modeling of current profile modification by lower hybrid current drive (LHCD) using a fullwave/Fokker-Planck simulation code is presented. A MHD stable LHCD discharge on Alcator C-Mod was analyzed, and the current profile from full wave simulations was found to show better agreement with the experiment than a ray-tracing code. Comparison of full wave and ray-tracing simulation shows that, although ray-tracing can reproduce the stochastic wave spectrum broadening, the full wave calculation predicts even wider spectrum broadening, and the wave spectrum fills all of the kinematically allowed domain. This is the first demonstration of LHCD current profile modeling using a full wave simulation code in a multi-pass absorption regime, showing the clear impact of full wave effects on the LHCD driven current profile.


Nuclear Fusion | 2009

Lower hybrid heating and current drive on the Alcator C-Mod tokamak

R. Wilson; R.R. Parker; M. Bitter; P.T. Bonoli; C. Fiore; R. W. Harvey; K. W. Hill; A. Hubbard; J.W. Hughes; A. Ince-Cushman; C. Kessel; Jinseok Ko; O. Meneghini; C. K. Phillips; M. Porkolab; J. E. Rice; A.E. Schmidt; S. Scott; S. Shiraiwa; Ernest J. Valeo; G. Wallace; John Wright

On the Alcator C-Mod tokamak, lower hybrid current drive (LHCD) is being used to modify the current profile with the aim of obtaining advanced tokamak (AT) performance in plasmas with parameters similar to those that would be required on ITER. To date, power levels in excess of 1 MW at a frequency of 4.6 GHz have been coupled into a variety of plasmas. Experiments have established that LHCD on C-Mod behaves globally as predicted by theory. Bulk current drive efficiencies, n20IlhR/Plh ~ 0.25, inferred from magnetics and MSE are in line with theory. Quantitative comparisons between local measurements, MSE, ECE and hard x-ray bremsstrahlung, and theory/simulation using the GENRAY, TORIC-LH CQL3D and TSC-LSC codes have been performed. These comparisons have demonstrated the off-axis localization of the current drive, its magnitude and location dependence on the launched n∥ spectrum, and the use of LHCD during the current ramp to save volt-seconds and delay the peaking of the current profile. Broadening of the x-ray emission profile during ICRF heating indicates that the current drive location can be controlled by the electron temperature, as expected. In addition, an alteration in the plasma toroidal rotation profile during LHCD has been observed with a significant rotation in the counter-current direction. Notably, the rotation is accompanied by peaking of the density and temperature profiles on a current diffusion time scale inside of the half radius where the LH absorption is taking place.


Physics of Plasmas | 2011

Investigation of lower hybrid physics through power modulation experiments on Alcator C-Mod

A.E. Schmidt; P.T. Bonoli; O. Meneghini; R.R. Parker; M. Porkolab; S. Shiraiwa; G. Wallace; John Wright; R. W. Harvey; J. R. Wilson

Lower hybrid current drive (LHCD) is an attractive tool for off-axis current profile control in magnetically confined tokamak plasmas and burning plasmas (ITER), because of its high current drive efficiency. The LHCD system on Alcator C-Mod operates at 4.6 GHz, with ~ 1 MW of coupled power, and can produce a wide range of launched parallel refractive index (n||) spectra. A 32 chord, perpendicularly viewing hard x-ray camera has been used to measure the spatial and energy distribution of fast electrons generated by lower hybrid (LH) waves. Square-wave modulation of LH power on a time scale much faster than the current relaxation time does not significantly alter the poloidal magnetic field inside the plasma and thus allows for realistic modeling and consistent plasma conditions for different n|| spectra. Inverted hard x-ray profiles show clear changes in LH-driven fast electron location with differing n||. Boxcar binning of hard x-rays during LH power modulation allows for ~ 1 ms time resolution which is s...


Nuclear Fusion | 2011

Design, and initial experiment results of a novel LH launcher on Alcator C-Mod

Syun'ichi Shiraiwa; O. Meneghini; R.R. Parker; G. Wallace; J. R. Wilson; I. Faust; C. Lau; R. Mumgaard; S. Scott; S.J. Wukitch; W. Beck; J. Doody; James H. Irby; P. MacGibbon; D. Johnson; A. Kanojia; P. Koert; D. Terry; R. Vieira

The design, construction and initial results of a new lower hybrid current drive (LHCD) launcher on Alcator C-Mod (Hutchinson et al 1994 Phys. Plasmas 1 1511) are presented. The new LHCD launcher (LH2) is based on a novel splitter concept which evenly distributes the microwave power in four ways in the poloidal direction. This design allows for simplification of the feeding structure while keeping the flexibility to vary the peak launched toroidal index of refraction, Ntoroidal, from ?3.8 to 3.8. An integrated model predicts good plasma coupling over a wide range of edge densities, while poloidal variations of the edge density are found to affect the evenness of power splitting in the poloidal direction. The measured transmission loss is about 30% lower than the previous launcher, and a clean Ntoroidal spectrum has been confirmed. Power handling capability exceeding an empirical weak conditioning limit and reliable operation up to 1.1?MW net LHCD power have been achieved. A survey of antenna?plasma coupling shows the existence of a millimetric vacuum gap in front of the launcher. Fully non-inductive, reversed shear plasma operation has been demonstrated and sustained for multiple current diffusion times. The current drive efficiency, ?LH ? neR0Ip/PLH, of these plasmas is (0.2?0.25) ? 1020?m?2A?W?1, which is in agreement with the expected efficiency on the International Thermonuclear Experimental Reactor (ITER).


Nuclear Fusion | 2011

Development of a plasma current ramp-up technique for spherical tokamaks by the lower hybrid wave

Y. Takase; A. Ejiri; Hidetoshi Kakuda; Y. Nagashima; Takuma Wakatsuki; Osamu Watanabe; P.T. Bonoli; O. Meneghini; S. Shiraiwa; John Wright; C.P. Moeller; H. Kasahara; R. Kumazawa; T. Mutoh; K. Saito

Spherical tokamaks (STs) have the advantage of high beta capability, but the realization of a compact reactor requires the elimination of the central solenoid (CS). The possibility of using the lower hybrid wave (LHW) to ramp up the plasma current (Ip) from zero to a high enough level required for fusion burn in ST is examined theoretically and experimentally. Excitation of a travelling fast wave (FW) by the combline antenna installed on TST-2 was confirmed by a finite element analysis, but efficient current drive requires excitation of the LHW, either directly by the antenna or by mode conversion from the FW. The analysis using the TORLH full-wave solver indicates that core current drive by LHW is possible in the low-density, low Ip plasma formed by electron cyclotron heating (ECH). It is important to keep the density low during Ip ramp-up, and the wavenumber must be reduced as Ip increases. Initial results from TST-2 demonstrate that RF power in the LH frequency range (200 MHz) can achieve initial Ip formation, and is more effective than ECH for further ramp-up of Ip. Ip ramp-up to over 12 kA was achieved by combining ramp-up of the externally applied vertical magnetic field and ramp-up of the RF power. The significant asymmetry observed between co-current drive and counter-current drive is attributed to the presence of RF driven current. An optimized LHW antenna with appropriate polarization and wavenumber spectrum controllability is being designed. The success of the TST-2 experiment would provide a scientific basis for quantitatively evaluating the required CS capability for a low-aspect-ratio reactor.


RADIO FREQUENCY POWER IN PLASMAS: Proceedings of the 18th Topical Conference | 2009

Plasma wave simulation based on versatile FEM solver on Alcator C‐mod

S. Shiraiwa; O. Meneghini; R.R. Parker; G. Wallace; J. R. Wilson

The finite element method (FEM) has the potential of simulating plasma waves seamlessly from the core to the vacuum and antenna regions. We explored the possibility of using a versatile FEM solver package, COMSOL, for lower hybrid (LH) wave simulation. Special care was paid to boundary conditions to satisfy toroidal symmetry. The non‐trivial issue of introducing hot plasma effects was addressed by an iterative algorithm. These techniques are verified both analytically and numerically. In the lower hybrid (LH) grill antenna coupling problem, the FEM solver successfully reproduced the solution that was obtained analytically. Propagation of LH waves on the Alcator C and Alcator C‐MOD plasmas was compared with a ray‐tracing code, showing good consistency. The approach based on the FEM is computationally less intensive compared to spectral domain solvers, and more suitable for the simulation of larger device such as ITER.


RADIO FREQUENCY POWER IN PLASMAS: 17th Topical Conference on Radio Frequency Power in Plasmas | 2007

TOPLHA: an accurate and efficient numerical tool for analysis and design of LH antennas

Daniele Milanesio; Vito Lancellotti; O. Meneghini; Riccardo Maggiora; Giuseppe Vecchi; R. Bilato

Auxiliary ICRF heating systems in tokamaks often involve large complex antennas, made up of several conducting straps hosted in distinct cavities that open towards the plasma. The same holds especially true in the LH regime, wherein the antennas are comprised of arrays of many phased waveguides. Upon observing that the various cavities or waveguides couple to each other only through the EM fields existing over the plasma‐facing apertures, we self‐consistently formulated the EM problem by a convenient set of multiple coupled integral equations. Subsequent application of the Method of Moments yields a highly sparse algebraic system; therefore formal inversion of the system matrix happens to be not so memory demanding, despite the number of unknowns may be quite large (typically 105 or so). The overall strategy has been implemented in an enhanced version of TOPICA (Torino Polytechnic Ion Cyclotron Antenna) and in a newly developed code named TOPLHA (Torino Polytechnic Lower Hybrid Antenna). Both are simulati...

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R.R. Parker

Massachusetts Institute of Technology

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S. Shiraiwa

Massachusetts Institute of Technology

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J. R. Wilson

Princeton Plasma Physics Laboratory

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P.T. Bonoli

Massachusetts Institute of Technology

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G. Wallace

Massachusetts Institute of Technology

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John Wright

Massachusetts Institute of Technology

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A.E. Schmidt

Massachusetts Institute of Technology

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A. Hubbard

Massachusetts Institute of Technology

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J.W. Hughes

Massachusetts Institute of Technology

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S. Scott

Princeton Plasma Physics Laboratory

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