Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where Gregory R. Hanson is active.

Publication


Featured researches published by Gregory R. Hanson.


Nuclear Fusion | 1998

Analysis of RF sheath interactions in TFTR

D.A. D'Ippolito; J.R. Myra; J. H. Rogers; K. W. Hill; J. C. Hosea; R. Majeski; G. Schilling; J. R. Wilson; Gregory R. Hanson; A.C. England; J. B. Wilgen

New theoretical and experimental tools are applied to the analysis of ICRF antenna-edge plasma interactions in the TFTR tokamak. A new numerical method for computing the three dimensional (3-D) rf sheath voltage distribution is used, and the quantitative predictions of rf sheath theory are compared with measurements of the edge density profile obtained by microwave reflectometry and with titanium impurity concentration data. It is shown that the local density depletion at the antenna is consistent with density pump-out by strong E × B convection into the Faraday screen (FS). Modelling of the FS impurity influx shows that the calculated titanium impurity concentration based on this direct influx agrees with the measured concentration for π phasing. It is also shown that screening of impurity neutrals by ionization in the SOL is a large effect and increases with rf power. At high power over many shots, a fraction of the metal impurities migrates around the machine and is deposited on the limiters, providing a secondary source of titanium. The data show that the central titanium concentration is strongly dependent on antenna phasing. Possible explanations for this phasing dependence are discussed.


Review of Scientific Instruments | 1990

ATF two-frequency correlation reflectometer

Gregory R. Hanson; J. B. Wilgen; E. Anabitarte; J. D. Bell; J. H. Harris; J.L. Dunlap; C.E. Thomas

The Advanced Toroidal Facility (ATF) density fluctuation reflectometer system consists of two individual reflectometers operating in the 30- to 40-GHz band. Each reflectometer consists of a tunable microwave source and a quadrature phase detector connected to the same antenna system. This arrangement allows two-frequency operation along the same radial chord for radial coherence measurements. The technique used in making radial coherence measurements is discussed and the results of such experiments are given. Initial experiments have shown high coherence when the frequencies of the two reflectometers are tuned close together and a clear loss of coherence as the radial separation of the cutoff layers is increased by increasing the frequency separation of the two reflectometers. Recent results have shown that local measurements of density fluctuations in plasmas with electron cyclotron heating (ECH) are possible and that detailed structure can be seen in the fluctuation spectra. In addition, radial correlation lengths have been found to be from 0.5 to 1.0 cm in ECH plasmas, with some frequency structures having correlation lengths up to 3 cm. In plasmas with neutral beam injection (NBI), the radial correlation lengths in the edge region have been found to be approximately 0.1--0.2 cm. 4 figs.


Design, process integration, and characterization for microelectronics. Conference | 2002

Direct to digital holography for semiconductor wafer defect detection and review

C. E. Thomas; Tracy M. Bahm; L. R. Baylor; Philip R. Bingham; Steven W. Burns; Matt Chidley; Long Dai; Robert J. Delahanty; Christopher J. Doti; Ayman El-Khashab; Robert L. Fisher; Judd M. Gilbert; James S. Goddard; Gregory R. Hanson; Joel D. Hickson; Martin A. Hunt; Kathy W. Hylton; George C. John; Michael L. Jones; Kenneth R. Macdonald; Michael W. Mayo; Ian M. Mcmackin; Dave R. Patek; John H. Price; D.A. Rasmussen; Louis J. Schaefer; Thomas R. Scheidt; Mark A. Schulze; Philip Schumaker; Bichuan Shen

A method for recording true holograms directly to a digital video medium in a single image has been invented. This technology makes the amplitude and phase for every pixel of the target object wave available. Since phase is proportional wavelength, this makes high-resolution metrology an implicit part of the holographic recording. Measurements of phase can be made to one hundredth or even one thousandth of a wavelength, so the technology is attractive for dining defects on semiconductor wafers, where feature sizes are now smaller than the wavelength of even deep UV light.


Review of Scientific Instruments | 1992

A swept two‐frequency microwave reflectometer for edge density profile measurements on TFTR

Gregory R. Hanson; J. B. Wilgen; T. S. Bigelow; I. Collazo; Clarence E. Thomas

The edge density profile can play a significant role in determining the plasma confinement and the coupling of the ion cyclotron resonance frequency (ICRF) heating power to the plasma. To experimentally measure the edge density profile in the Tokamak Fusion Test Facility (TFTR), a two‐frequency microwave reflectometer is being built. This reflectometer will operate in a swept two‐frequency configuration between 91 and 118 GHz using the extraordinary mode. The frequency separation between the two microwave signals will be held constant while the signals are swept across the frequency band. By measuring the differential phase delay between these two signals, the density profile can be reconstructed. Two‐frequency profile reflectometry is discussed and results of modeling of this type of reflectometer measurement for TFTR are shown. Finally, the design of the TFTR edge profile reflectometer microwave system is described.


CHARACTERIZATION AND METROLOGY FOR ULSI TECHNOLOGY: 2003 International Conference on Characterization and Metrology for ULSI Technology | 2003

Direct To Digital Holography For High Aspect Ratio Inspection of Semiconductor Wafers

C. E. Thomas; Martin A. Hunt; Tracy M. Bahm; L. R. Baylor; Philip R. Bingham; Matthew D. Chidley; Xiaolong Dai; Robert J. Delahanty; Ayman El-Khashab; Judd M. Gilbert; James S. Goddard; Gregory R. Hanson; Joel D. Hickson; Kathy W. Hylton; George C. John; Michael L. Jones; Michael W. Mayo; Christopher Marek; John H. Price; D.A. Rasmussen; Louis J. Schaefer; Mark A. Schulze; Bichuan Shen; Randall G. Smith; Allen N. Su; Kenneth W. Tobin; William R. Usry; Edgar Voelkl; Karsten S. Weber; Robert W. Owen

Direct to Digital Holography (DDH) has been developed as a semiconductor wafer inspection tool and in particular as a tool for seeing defects in high aspect ratio (HAR) structures on semiconductor wafers and also for seeing partial‐height defects. While the tool works very well for general wafer inspection, it has unusual capabilities for high aspect ratio inspection (HARI) and for detecting thin residual film defects (partial height defects). Inspection of HAR structures is rated as one of the highest unmet priorities of the member companies of International SEMATECH, and finding residual thin film defects (in some cases called “stringers”) is also a very difficult challenge. The capabilities that make DDH unusually sensitive include: 1) the capture of the whole wave—both the classical amplitude captured by traditional optical systems, and the phase of the wave, with phase potentially measured to ∼1/1000’th of a wavelength or ∼2 to 3 Angstroms for a deep ultra‐violet (DUV) laser; 2) heterodyne detection—...


Nuclear Fusion | 1996

Three dimensional modelling of ICRF launchers for fusion devices

Mark Dwain Carter; D.A. Rasmussen; P. M. Ryan; Gregory R. Hanson; D. C. Stallings; D. B. Batchelor; T. S. Bigelow; A.C. England; D. J. Hoffman; M. Murakami; C.Y. Wang; J. B. Wilgen; J.H. Rogers; J.R. Wilson; R. Majeski; G. Schilling

The three dimensional (3-D) nature of antennas for fusion applications in the ion cyclotron range of frequencies (ICRF) requires accurate modelling to design and analyse new antennas. In this article, analysis and design tools for radiofrequency (RF) antennas are successfully benchmarked with experiment, and the 3-D physics of the launched waves is explored. The systematic analysis combines measured density profiles from a reflectometer system, transmission line circuit modelling, detailed 3-D magnetostatics modelling and a new 3-D electromagnetic antenna model including plasma. This analysis gives very good agreement with measured loading data from the Tokamak Fusion Test Reactor (TFTR) Bay-M antenna, thus demonstrating the validity of the analysis for the design of new RF antennas. The 3-D modelling is contrasted with 2-D models, and significant deficiencies are found in the latter. The 2-D models are in error by as much as a factor of 2 in real and reactive loading, even after they are corrected for the most obvious 3-D effects. Three dimensional effects play the most significant role at low parallel wavenumbers, where the launched power spectrum can be quite different from the predictions of 2-D models. Three dimensional effects should not be ignored for many RF designs, especially those intended for fast wave current drive.


Review of Scientific Instruments | 2006

Reflectometer sensing of rf waves in front of the high harmonic fast wave antenna on NSTX

J. B. Wilgen; P. M. Ryan; Gregory R. Hanson; David W. Swain; S. Bernabei; N. Greenough; S. DePasquale; C. K. Phillips; J. C. Hosea; J. R. Wilson

The ability to measure rf driven waves in the edge of the plasma can help to elucidate the role that surface waves and parametric decay instabilities (PDIs) play in rf power losses on NSTX. A microwave reflectometer has recently been modified to monitor rf plasma waves in the scrape-off layer in front of the 30MHz high harmonic fast wave antenna array on NSTX. In rf heated plasmas, the plasma-reflected microwave signal exhibits 30MHz sidebands, due primarily to the modulation of the cutoff layer by the electrostatic component of the heating wave. Similarly, electrostatic parametric decay waves (when present) are detected at frequencies below the heating frequency, near 28, 26,…MHz, separated from the heating frequency by harmonics of the local ion cyclotron frequency of about 2MHz. In addition, a corresponding frequency matched set of decay waves is also detected near the ion cyclotron harmonics at 2, 4,…MHz. The rf plasma-wave sensing capability is useful for determination of the PDI power threshold as a...


Review of Scientific Instruments | 1995

Differential‐phase reflectometry for edge profile measurements on Tokamak fusion test reactor

Gregory R. Hanson; J. B. Wilgen; T. S. Bigelow; I. Collazo; A.C. England; M. Murakami; D.A. Rasmussen; J. R. Wilson

Edge electron density profile measurements, including the scrape‐off layer, have been made during ion cyclotron range of frequency (ICRF) heating with the two‐frequency differential‐phase reflectometer installed on an ICRF antenna on the Tokamak fusion test reactor (TFTR). This system probes the plasma using the extraordinary mode with two signals swept from 90 to 118 GHz, while maintaining a fixed‐difference frequency of 125 MHz. The extraordinary mode is used to obtain density profiles in the range of 1×1011–3×1013 cm−3 in high‐field (4.5–4.9 T) full‐size (R0=2.62 m, a=0.96 m) TFTR plasmas. The reflectometer launcher is located in an ICRF antenna and views the plasma through a small penetration in the center of the Faraday shield. A 26‐m‐long overmoded waveguide run connects the launcher to the reflectometer microwave electronics. Profile measurements made with this reflectometer system will be presented along with a discussion of the characteristics of this differential phase reflectometer and data ana...


Plasma Physics and Controlled Fusion | 2013

Effects of LH power on SOL density profiles and LH coupling on Alcator C-Mod

C. Lau; Gregory R. Hanson; B. LaBombard; Y. Lin; O. Meneghini; R. Ochoukov; R.R. Parker; S. Shiraiwa; J. L. Terry; G. Wallace; J. B. Wilgen; S.J. Wukitch

A swept-frequency X-mode reflectometer has been used to measure the scrape-off-layer (SOL) density profiles with and without lower hybrid (LH) power at three poloidal locations adjacent to the LH launcher for various plasma parameters in order to understand the coupling of LH waves on Alcator C-Mod. LH power has been observed to create significant poloidal SOL density profile asymmetries that are correlated with visible video camera images of emissivity patterns in front of the LH launcher. The observed density profile asymmetries depend on LH power, , magnetic geometry and magnetic field direction. A 2D diffusive?convective model has been used to show that these density profile modifications are consistent with a LH vortex, where LH power drives E???B drifts that then modify the SOL density profile. In particular, the simulations show that the density profile can possibly create a net poloidally averaged density depletion in front of the waveguide rows. A LH slab coupling model is then used to show that the simulated reflection coefficients strongly depend on the poloidal density profile asymmetries. The simulated LH power reflection coefficients agree with the experimental reflection coefficients only after the observed density depletion is included in the model.


Drying Technology | 2008

Microwave Moisture Measurement System for Hardwood Lumber Drying

William W. Moschler; Gregory R. Hanson

The goal of this project was to develop a prototype microwave-based moisture sensor system suitable for the kiln drying of hardwood lumber. The moisture sensors developed are battery powered and are capable of communicating with a host kiln control system via spread spectrum wireless communications. We have developed two designs of the sensors working at 4.5 to 6 GHz with linear response to moisture content (MC) over a range of 6–100%. These sensors allow us to make a swept frequency microwave transmission measurement through a small area of a board. Using the prototype electronics and sensors, we have obtained measurements of MC over the above MC range for red oak and yellow poplar with standard deviations of less than 1.5% MC. We have developed data for board thickness corrections and for temperature corrections for the MC measurement system.

Collaboration


Dive into the Gregory R. Hanson's collaboration.

Top Co-Authors

Avatar

J. B. Wilgen

Oak Ridge National Laboratory

View shared research outputs
Top Co-Authors

Avatar

D.A. Rasmussen

Oak Ridge National Laboratory

View shared research outputs
Top Co-Authors

Avatar

J. R. Wilson

Princeton Plasma Physics Laboratory

View shared research outputs
Top Co-Authors

Avatar

Clarence E. Thomas

Oak Ridge National Laboratory

View shared research outputs
Top Co-Authors

Avatar

J. C. Hosea

Princeton Plasma Physics Laboratory

View shared research outputs
Top Co-Authors

Avatar

G. Schilling

Princeton Plasma Physics Laboratory

View shared research outputs
Top Co-Authors

Avatar

J. H. Rogers

Princeton Plasma Physics Laboratory

View shared research outputs
Top Co-Authors

Avatar

R. Majeski

Princeton Plasma Physics Laboratory

View shared research outputs
Top Co-Authors

Avatar

Philip R. Bingham

Oak Ridge National Laboratory

View shared research outputs
Top Co-Authors

Avatar

T. S. Bigelow

Oak Ridge National Laboratory

View shared research outputs
Researchain Logo
Decentralizing Knowledge