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Dive into the research topics where G. E. Granroth is active.

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Featured researches published by G. E. Granroth.


Scientific Reports | 2015

An NCN-pincer ligand dysprosium single-ion magnet showing magnetic relaxation via the second excited state

Yun-Nan Guo; Liviu Ungur; G. E. Granroth; Annie K. Powell; Chunji Wu; Stephen E Nagler; Jinkui Tang; Liviu F. Chibotaru; Dongmei Cui

Single-molecule magnets are compounds that exhibit magnetic bistability purely of molecular origin. The control of anisotropy and suppression of quantum tunneling to obtain a comprehensive picture of the relaxation pathway manifold, is of utmost importance with the ultimate goal of slowing the relaxation dynamics within single-molecule magnets to facilitate their potential applications. Combined ab initio calculations and detailed magnetization dynamics studies reveal the unprecedented relaxation mediated via the second excited state within a new DyNCN system comprising a valence-localized carbon coordinated to a single dysprosium(III) ion. The essentially C2v symmetry of the DyIII ion results in a new relaxation mechanism, hitherto unknown for mononuclear DyIII complexes, opening new perspectives for means of enhancing the anisotropy contribution to the spin-relaxation barrier.


Physical Review Letters | 2001

Magnetic Spin Ladder (C5H12N)2CuBr4: High Field Magnetization and Scaling Near Quantum Criticality

Brian C. Watson; V. N. Kotov; Mark W. Meisel; D. W. Hall; G. E. Granroth; Wouter Montfrooij; Stephen E Nagler; D. A. Jensen; Rénal Backov; Melissa A. Petruska; Gail E. Fanucci; Daniel R. Talham

The magnetization, M(H< or =30 T,0.7< or =T< or =300 K), of (C5H12N)2CuBr4 has been used to identify this system as an S = 1/2 Heisenberg two-leg ladder in the strong-coupling limit, J( perpendicular) = 13.3 K and J( parallel) = 3.8 K, with H(c1) = 6.6 T and H(c2) = 14.6 T. An inflection point in M(H,T = 0.7 K) at half saturation, M(s)/2, is described by an effective XXZ chain. The data exhibit universal scaling behavior in the vicinity of H(c1) and H(c2), indicating that the system is near a quantum critical point.


Journal of Physics: Conference Series | 2010

SEQUOIA: A Newly Operating Chopper Spectrometer at the SNS

G. E. Granroth; Alexander I. Kolesnikov; Todd E Sherline; J. P. Clancy; K. A. Ross; Jacob Ruff; B. D. Gaulin; S E Nagler

A fine resolution chopper spectrometer (SEQUOIA) recently received first neutrons at the SNS. The commissioning phase of the instrument is underway. SEQUOIA is designed to utilize neutrons of an incident energy (Ei) between 10-2000 meV. A monochromatic beam is provided on a sample, 20 m from the decoupled ambient temperature H2O moderator, by filtering the white beam with a Fermi chopper located 18 m from the source. After interacting with the sample, neutrons are detected by an array of 3He linear position sensitive tubes located on a vertical cylinder with a radius of 5.5 m. This contribution presents current results from the commissioning experiments and compares SEQUOIAs actual and predicted performance. These commissioning experiments include characterization of the beam by monitors, determination of the chopper phase offsets, and runs with V and C4H2I2S. The predicted performance is provided by analytical calculations and Monte Carlo simulations.


Physical Review Letters | 2015

Interaction Driven Subgap Spin Exciton in the Kondo Insulator SmB6

Wesley Fuhrman; Jonathan C. Leiner; G. E. Granroth; Matthew Stone; M. D. Lumsden; L. DeBeer-Schmitt; J.-M. Mignot

Using inelastic neutron scattering, we map a 14 meV coherent resonant mode in the topological Kondo insulator SmB6 and describe its relation to the low energy insulating band structure. The resonant intensity is confined to the X and R high symmetry points, repeating outside the first Brillouin zone and dispersing less than 2 meV, with a 5d-like magnetic form factor. We present a slave-boson treatment of the Anderson Hamiltonian with a third neighbor dominated hybridized band structure. This approach produces a spin exciton below the charge gap with features that are consistent with the observed neutron scattering. We find that maxima in the wave vector dependence of the inelastic neutron scattering indicate band inversion.


Physical Review B | 2015

The frustrated fcc antiferromagnet Ba2 YOsO6: Structural characterization, magnetic properties and neutron scattering studies

Edwin Kermarrec; Casey Marjerrison; Corey M. Thompson; Dalini D. Maharaj; K. Levin; Scott Kroeker; G. E. Granroth; R. Flacau; Z. Yamani; J.E. Greedan; Bruce D. Gaulin

Here we report the crystal structure, magnetization, and neutron scattering measurements on the double perovskite Ba2 YOsO6. The Fm


Physical Review B | 2011

Magnetic Excitations from the Exotic Ground State of the Quantum FCC Antiferromagnet Ba2YMoO6

Jeremy P Carlo; J. P. Clancy; Tomoko Aharen; Z. Yamani; Jacob Ruff; J.J. Wagman; G. J. Van Gastel; H.M.L. Noad; G. E. Granroth; J.E. Greedan; H. A. Dabkowska; Bruce D. Gaulin


Physical Review Letters | 2007

Quantum spin correlations in an organometallic alternating-sign chain

Matthew Stone; Wei Tian; M. D. Lumsden; G. E. Granroth; David Mandrus; Jae Ho Chung; N. Harrison; Stephen E Nagler

\bar{3}


Physical Review B | 2003

Neutron scattering study of two-magnon states in the quantum magnet copper nitrate

D. A. Tennant; C. Broholm; Daniel H. Reich; Stephen E Nagler; G. E. Granroth; T. Barnes; Kedar Damle; Guangyong Xu; Y. Chen; Brian C. Sales


Physical Review B | 1998

MAGNETIC STUDIES OF END-CHAIN SPIN EFFECTS IN THE HALDANE-GAP MATERIAL NI(C3H10N2)2N3(CLO4)

G. E. Granroth; S. Maegawa; Mark W. Meisel; J. Krzystek; Louis-Claude Brunel; N. S. Bell; J. H. Adair; B. H. Ward; G. E. Fanucci; L.-K. Chou; Daniel R. Talham

m space group is found both at 290 K and 3.5 K with cell constants a0=8.3541(4) A and 8.3435(4) A, respectively. Os5+ (5d3) ions occupy a nondistorted, geometrically frustrated face-centered-cubic (fcc) lattice. A Curie-Weiss temperature θ ~₋700 K suggests the presence of a large antiferromagnetic interaction and a high degree of magnetic frustration. A magnetic transition to long-range antiferromagnetic order, consistent with a type-I fcc state below TN~69 K, is revealed by magnetization, Fisher heat capacity, and elastic neutron scattering, with an ordered moment of 1.65(6) μB on Os5+. The ordered moment is much reduced from either the expected spin-only value of ~3 μB or the value appropriate to 4d3 Ru5+ in isostructural Ba2 YRuO6 of 2.2(1) μB, suggesting a role for spin-orbit coupling (SOC). Triple-axis neutron scattering measurements of the order parameter suggest an additional first-order transition at T=67.45 K, and the existence of a second-ordered state. We find time-of-flight inelastic neutron results reveal a large spin gap Δ~17 meV, unexpected for an orbitally quenched, d3 electronic configuration. In conclusion, we discuss this in the context of the ~5 meV spin gap observed in the related Ru5+,4d3 cubic double perovskite Ba2YRuO6, and attribute the ~3 times larger gap to stronger SOC present in this heavier, 5d, osmate system.


Physical Review B | 2013

Spin Gap and the Nature of the 4d3 Magnetic Ground State in the Frustrated FCC Antiferromagnet Ba2YRuO6

Jeremy P Carlo; J. P. Clancy; Katharina Fritsch; Casey Marjerrison; G. E. Granroth; J.E. Greedan; H. A. Dabkowska; Bruce D. Gaulin

J. P. Carlo, 2 J. P. Clancy, T. Aharen, Z. Yamani, J. P. C. Ruff, J. Wagman, G. J. Van Gastel, H. M. L. Noad, G. E. Granroth, J. E. Greedan, 5 H. A. Dabkowska, and B. D. Gaulin 5, 6 Department of Physics and Astronomy, McMaster University, Hamilton, ON L8S 4M1 Canada Canadian Neutron Beam Centre, National Research Council, Chalk River, ON K0J 1J0 Canada Department of Chemistry, McMaster University, Hamilton, ON L8S 4M1 Canada Spallation Neutron Source, Oak Ridge National Laboratory, Oak Ridge, TN 37831 USA Brockhouse Institute for Materials Research, McMaster University, Hamilton, ON L8S 4M1 Canada Canadian Institute for Advanced Research, Toronto, ON M5G 1Z8 Canada (Dated: January 21, 2013)

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Stephen E Nagler

Oak Ridge National Laboratory

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M. D. Lumsden

Oak Ridge National Laboratory

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Andrei Savici

Oak Ridge National Laboratory

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Matthew Stone

Oak Ridge National Laboratory

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A. A. Aczel

Oak Ridge National Laboratory

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