N. Kafle
University of Tennessee
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Featured researches published by N. Kafle.
Journal of Vacuum Science and Technology | 2017
J. B. O. Caughman; R. H. Goulding; T. M. Biewer; T. S. Bigelow; Ian H. Campbell; Juan Caneses; S.J. Diem; Andy Fadnek; D. T. Fehling; R.C. Isler; E. H. Martin; Chad M. Parish; J. Rapp; Kun Wang; Clyde Beers; David Donovan; N. Kafle; H.B. Ray; G.C. Shaw; M. Showers
Plasma-facing materials in the divertor of a magnetic fusion reactor have to tolerate steady state plasma heat fluxes in the range of 10 MW/m2 for ∼107 s, in addition to fusion neutron fluences, which can damage the plasma-facing materials to high displacements per atom (dpa) of ∼50 dpa. Materials solutions needed for the plasma-facing components are yet to be developed and tested. The material plasma exposure experiment (MPEX) is a newly proposed steady state linear plasma device designed to deliver the necessary plasma heat flux to a target for testing, including the capability to expose a priori neutron-damaged material samples to those plasmas. The requirements of the plasma source needed to deliver the required heat flux are being developed on the Proto-MPEX device which is a linear high-intensity radio-frequency (RF) plasma source that combines a high-density helicon plasma generator with electron- and ion-heating sections. The device is being used to study the physics of heating overdense plasmas i...
Fusion Science and Technology | 2017
R. H. Goulding; J. B. O. Caughman; J. Rapp; T. M. Biewer; T. S. Bigelow; I. H. Campbell; Juan Caneses; D. Donovan; N. Kafle; E. H. Martin; H. B. Ray; G. C. Shaw; M. Showers
Abstract Proto-MPEX is a linear plasma device being used to study a novel RF source concept for the planned Material Plasma Exposure eXperiment (MPEX), which will address plasma-materials interaction (PMI) for nuclear fusion reactors. Plasmas are produced using a large diameter helicon source operating at a frequency of 13.56 MHz at power levels up to 120 kW. In recent experiments the helicon source has produced deuterium plasmas with densities up to ~6 × 1019 m–3 measured at a location 2 m downstream from the antenna and 0.4 m from the target. Previous plasma production experiments on Proto-MPEX have generated lower density plasmas with hollow electron temperature profiles and target power deposition peaked far off axis. The latest experiments have produced flat Te profiles with a large portion of the power deposited on the target near the axis. This and other evidence points to the excitation of a helicon mode in this case.
Physics of Plasmas | 2018
Clyde Beers; R. H. Goulding; R.C. Isler; E. H. Martin; T. M. Biewer; Juan Caneses; J. B. O. Caughman; N. Kafle; J. Rapp
The Prototype-Material Plasma Exposure eXperiment (Proto-MPEX) linear plasma device is a test bed for exploring and developing plasma source concepts to be employed in the future steady-state linear device Material Plasma Exposure eXperiment (MPEX) that will study plasma-material interactions for the nuclear fusion program. The concept foresees using a helicon plasma source supplemented with electron and ion heating systems to reach necessary plasma conditions. In this paper, we discuss ion temperature measurements obtained from Doppler broadening of spectral lines from argon ion test particles. Plasmas produced with helicon heating alone have average ion temperatures downstream of the Helicon antenna in the range of 3 ± 1 eV; ion temperature increases to 10 ± 3 eV are observed with the addition of ion cyclotron heating (ICH). The temperatures are higher at the edge than the center of the plasma either with or without ICH. This type of profile is observed with electrons as well. A one-dimensional RF anten...
Physics of Plasmas | 2018
T. M. Biewer; T. S. Bigelow; Juan Caneses; S. J. Diem; D.L. Green; N. Kafle; J. Rapp; Proto-MPEX Team
The Prototype Material Plasma Exposure Experiment at the Oak Ridge National Laboratory utilizes a variety of power systems to generate and deliver a high heat flux plasma onto the surface of material targets. In the experiments described here, a deuterium plasma is produced via a ∼100 kW, 13.56 MHz RF helicon source, to which ∼20 kW of 28 GHz microwave power is applied. The electron density and temperature profiles are measured using a Thomson scattering (TS) diagnostic, and indicate that the electron density is centrally peaked. In the core of the plasma column, the electron density is higher than the cut-off density (∼0.9 × 1019 m−3) for the launched mixture of X- and O-mode electron cyclotron heating waves to propagate. TS measurements indicate electron temperature increases from ∼5 eV to ∼20 eV during 28 GHz power application when the neutral deuterium pressure is reduced below 0.13 Pa (∼1 mTorr.).
Physics of Plasmas | 2018
N. Kafle; L.W. Owen; Juan Caneses; T. M. Biewer; J. B. O. Caughman; D. Donovan; R. H. Goulding; J. Rapp
The Prototype Material Plasma Exposure eXperiment (Proto-MPEX) at Oak Ridge National Laboratory is a linear plasma device that combines a helicon plasma source with additional microwave and radio frequency heating to deliver high plasma heat and particle fluxes to a target. Double Langmuir probes and Thomson scattering are being used to measure local electron temperature and density at various radial and axial locations. A recently constructed Mach-double probe provides the added capability of simultaneously measuring electron temperatures ( T e), electron densities ( n e), and Mach numbers (M). With this diagnostic, it is possible to infer the plasma flow, particle flux, and heat flux at different locations along the plasma column in Proto-MPEX. Preliminary results show Mach numbers of 0.5 (towards the dump plate) and 1.0 (towards the target plate) downstream from the helicon source, and a stagnation point (no flow) near the source for the case where the peak magnetic field was 1.3 T. Measurements of particle flow and ne and Te profiles are discussed. The extensive coverage provided by these diagnostics permits data-constrained B2.5-Eirene modeling of the entire plasma column, and comparison with results of modeling in the high-density helicon plasmas will be presented.
Physics of Plasmas | 2018
Juan Caneses; P. A. Piotrowicz; T. M. Biewer; J. B. O. Caughman; R. H. Goulding; N. Kafle; J. Rapp
The physics of electron and ion heating of high-density deuterium helicon plasmas (>3 × 10 19 m−3) in the Proto-Material Plasma Exposure Experiment linear device are under investigation. Theoretical estimates indicate that for efficient heating, discharges with very low neutral gas content ( ≪0.1 Pa) in the heating sections are required to minimize collisional losses and charge exchange interactions with neutrals. However, this requirement is typically not compatible with the neutral gas pressures (1–2 Pa) commonly used in high-density, light-ion helicon sources. To satisfy these competing requirements, differential pumping techniques are needed. In this paper, results are presented that demonstrate the production of high-density discharges (2–6 × 10 19 m−3) with very low neutral gas content ( 75%) in the heating sections. Results indicate that the best fueling location is upstream of the plasma source. We elaborate on the key aspects that must be considered to produce these discharges: (1) fueling location, radio-frequency pulse length, and magnetic field configuration, (2) flow rate and timing of the gas injection, and (3) use of conductance-limiting elements.The physics of electron and ion heating of high-density deuterium helicon plasmas (>3 × 10 19 m−3) in the Proto-Material Plasma Exposure Experiment linear device are under investigation. Theoretical estimates indicate that for efficient heating, discharges with very low neutral gas content ( ≪0.1 Pa) in the heating sections are required to minimize collisional losses and charge exchange interactions with neutrals. However, this requirement is typically not compatible with the neutral gas pressures (1–2 Pa) commonly used in high-density, light-ion helicon sources. To satisfy these competing requirements, differential pumping techniques are needed. In this paper, results are presented that demonstrate the production of high-density discharges (2–6 × 10 19 m−3) with very low neutral gas content ( 75%) in the heating sections. Results indicate that the best fueling location is upstream of the plasma source. We elaborate on the key aspects that must be cons...
Review of Scientific Instruments | 2018
N. Kafle; T. M. Biewer; D. Donovan
Bulletin of the American Physical Society | 2017
N. Kafle; Juan Caneses; T. M. Biewer; L.W. Owen; M. Showers; David Donovan; J. B. O. Caughman; R. H. Goulding; J. Rapp
Bulletin of the American Physical Society | 2017
J. B. O. Caughman; R. H. Goulding; T. M. Biewer; T. S. Bigelow; Juan Caneses; S.J. Diem; D.L. Green; R.C. Isler; J. Rapp; P. A. Piotrowicz; Clyde Beers; N. Kafle; Showers
Bulletin of the American Physical Society | 2017
T. M. Biewer; T. S. Bigelow; Juan Caneses; S.J. Diem; J. Rapp; M. Reinke; N. Kafle; H.B. Ray; M. Showers