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Featured researches published by N. Kim.


American Mineralogist | 2007

Scandium-45 NMR of pyrope-grossular garnets: Resolution of multiple scandium sites and comparison with X-ray diffraction and X-ray absorption spectroscopy

N. Kim; Jonathan F. Stebbins; Simona Quartieri; Roberta Oberti

Abstract Here we present 45Sc and 27Al NMR results on Sc-doped pyrope (Mg3Al2Si3O12), grossular (Ca3Al2Si3O12), and an 80% grossular-20% pyrope garnet (grs80) that have recently been well-studied by X-ray diffraction and X-ray spectroscopies. Clearly distinct NMR peaks are observed for Sc in the eight-coordinated X site (pyrope and grs80) and in the six-coordinated Y site (grossular and grs80). X-ray and NMR data agree that only eight-coordinated Sc is present in pyrope and that six-coordinated Sc is predominant in grossular; however, the XRD results also indicated significant X and Z site (four-coordinated) Sc in the Ca-rich garnet. Possible reasons for this apparent discrepancy are discussed. We demonstrate that 45Sc NMR is potentially a useful new method for studies of the site occupancies of Sc3+ in oxides and silicates, at least in experimental systems where its concentration is a few percent or greater.


Solid State Nuclear Magnetic Resonance | 2011

Temperature calibration for high-temperature MAS NMR to 913 K: 63Cu MAS NMR of CuBr and CuI, and 23Na MAS NMR of NaNbO3.

Jingshi Wu; N. Kim; Jonathan F. Stebbins

The solid-state phase transitions of CuBr, CuI and NaNbO(3) can be readily observed using (63)Cu and (23)Na high-temperature magic-angle spinning nuclear magnetic resonance spectroscopy. Temperature has large, linear effects on the peak maximum of (63)Cu in each solid phase of CuBr and CuI, and there is large jump in shift across each phase transition. The (23)Na MAS NMR peak intensities and the line widths in NaNbO(3) also clearly show its high-temperature transition to the cubic phase. These data can be used to calibrate high-temperature MAS NMR probes up to 913 K, which is two hundred degrees higher than the commonly-used temperature calibration based on the chemical shift of (207)Pb in Pb(NO(3))(2).


APL Materials | 2015

Order within disorder: the atomic structure of ion-beam sputtered amorphous tantala (a-Ta2O5)

R. Bassiri; Franklin Liou; M. R. Abernathy; Angie C. Lin; N. Kim; Apurva Mehta; Badri Shyam; Robert L. Byer; Eric K. Gustafson; M. J. Hart; Ian MacLaren; I. W. Martin; R. Route; S. Rowan; Jonathan F. Stebbins; Martin M. Fejer

Amorphous tantala (a-Ta2O5) is a technologically important material often used in high-performance coatings. Understanding this material at the atomic level provides a way to further improve performance. This work details extended X-ray absorption fine structure measurements of a-Ta2O5 coatings, where high-quality experimental data and theoretical fits have allowed a detailed interpretation of the nearest-neighbor distributions. It was found that the tantalum atom is surrounded by four shells of atoms in sequence; oxygen, tantalum, oxygen, and tantalum. A discussion is also included on how these models can be interpreted within the context of published crystalline Ta 2O5 and other a-T2O5 studies.


European Journal of Mineralogy | 2009

Confirmation of octahedrally coordinated phosphorus in AlPO4-containing stishovite by 31P NMR

Jonathan F. Stebbins; N. Kim; Fabrice Brunet; Tetsuo Irifune

Using 31 P and 27 Al Nuclear Magnetic Resonance (NMR) spectroscopy, we confirm the discovery of six-coordinated phosphorus ( VI P) in stishovite that contains about 1 wt% P 2 O 5 and Al 2 O 3 (synthesized at 18 GPa), as described in a recent study based on micro-X-ray Absorption Near-Edge Structure (XANES) data at the phosphorus and aluminum K -edges in a similar sample. We also confirm the presence of six-coordinated Al ( VI Al) in the stishovite. The VI P is marked by a 31 P NMR peak far below the known range for phosphate groups in solid oxide materials, at −158 ppm. A sample of pure AlPO 4 made under the same conditions contained only IV P, as well as IV Al, VI Al, and a minor amount of V Al. Observed chemical shifts and peak shapes in this material, along with X-ray powder diffraction data (XRPD), indicate a mixture of the high-pressure form of AlPO 4 ( Cmcm , CrVO 4 -structure), its low-cristobalite form, an amorphous phase, and one or more unknown crystalline phases.


Journal of Non-crystalline Solids | 2013

Influence of network bond percolation on the thermal, mechanical, electrical and optical properties of high and low-k a-SiC:H thin films

Sean W. King; Jeff Bielefeld; Guanghai Xu; W. A. Lanford; Yusuke Matsuda; Reinhold H. Dauskardt; N. Kim; Donald Hondongwa; Lauren Olasov; Brian C. Daly; Gheorghe Stan; Ming Liu; Dhanadeep Dutta; David W. Gidley


Solid State Ionics | 2008

Structure, local environment, and ionic conduction in scandia stabilized zirconia

Hong Huang; Cheng-Han Hsieh; N. Kim; Jonathan F. Stebbins; Fritz B. Prinz


Journal of the American Ceramic Society | 2009

Characterization of Phase Separation and Thermal History Effects in Magnesium Silicate Glass Fibers by Nuclear Magnetic Resonance Spectroscopy

Jonathan F. Stebbins; N. Kim; Michael J. Andrejcak; Paul M. Boymel; Bruce K. Zoitos


Solid State Ionics | 2007

High temperature 17O MAS NMR study of calcia, magnesia, scandia and yttria stabilized zirconia

N. Kim; Cheng-Han Hsieh; Hong Huang; Fritz B. Prinz; Jonathan F. Stebbins


ACS Applied Materials & Interfaces | 2013

Tunable Plasticity in Amorphous Silicon Carbide Films

Yusuke Matsuda; N. Kim; Sean W. King; Jeff Bielefeld; Jonathan F. Stebbins; Reinhold H. Dauskardt


Journal of Non-crystalline Solids | 2014

The structure of ion beam sputtered amorphous alumina films and effects of Zn doping: High-resolution 27Al NMR

N. Kim; R. Bassiri; Martin M. Fejer; Jonathan F. Stebbins

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Apurva Mehta

SLAC National Accelerator Laboratory

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Badri Shyam

SLAC National Accelerator Laboratory

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Eric K. Gustafson

California Institute of Technology

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