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Dive into the research topics where B. Farmer is active.

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Featured researches published by B. Farmer.


Journal of Applied Physics | 2014

Ferromagnetic resonance study of eightfold artificial ferromagnetic quasicrystals

Vinayak Bhat; Joseph Sklenar; B. Farmer; Justin Woods; J. B. Ketterson; J. T. Hastings; L. E. De Long

We have performed broadband (10 MHz–18 GHz) and narrowband (9.7 GHz) ferromagnetic resonance (FMR) measurements on permalloy thin films patterned with quasiperiodic Ammann tilings having eightfold rotational symmetry. We observed highly reproducible mode structures in the low-frequency, hysteretic regime in which domain walls and unsaturated magnetization textures exist. A minimum of 10 robust modes were observed in patterned samples, compared to the single uniform mode observed in unpatterned permalloy films. The field dependence and approximate eightfold rotational symmetry of the FMR spectra are in good agreement with micromagnetic simulations that confirm the importance of patterning for controlling static and dynamic magnetic response.


Journal of Applied Physics | 2015

Magnetic response of aperiodic wire networks based on Fibonacci distortions of square antidot lattices

B. Farmer; Vinayak Bhat; Joseph Sklenar; E. Teipel; Justin Woods; J. B. Ketterson; J. T. Hastings; L. E. De Long

The static and dynamic magnetic responses of patterned ferromagnetic thin films are uniquely altered in the case of aperiodic patterns that retain long-range order (e.g., quasicrystals). We have fabricated permalloy wire networks based on periodic square antidot lattices (ADLs) distorted according to an aperiodic Fibonacci sequence applied to two lattice translations, d1 = 1618 nm and d2 = 1000 nm. The wire segment thickness is fixed at t = 25 nm, and the width W varies from 80 to 510 nm. We measured the DC magnetization between room temperature and 5 K. Room-temperature, narrow-band (9.7 GHz) ferromagnetic resonance (FMR) spectra were acquired for various directions of applied magnetic field. The DC magnetization curves exhibited pronounced step anomalies and plateaus that signal flux closure states. Although the Fibonacci distortion breaks the fourfold symmetry of a finite periodic square ADL, the FMR data exhibit fourfold rotational symmetry with respect to the applied DC magnetic field direction.


Journal of Applied Physics | 2014

Nonstochastic magnetic reversal in artificial quasicrystalline spin ice

B. Farmer; Vinayak Bhat; Joseph Sklenar; Justin Woods; E. Teipel; N. Smith; J. B. Ketterson; J. T. Hastings; L. E. De Long

We have measured the isothermal DC magnetization of Penrose P2 tilings (P2T) composed of wire segments of permalloy thin film. Micromagnetic simulations reproduce the coercive fields and “knee anomalies” observed in experimental data and show magnetic shape anisotropy constrains segments to be single-domain (Ising spins) at low fields, similar to artificial spin ice (ASI). Mirror symmetry controls the initial reversal of individual segments oriented parallel to the applied field, followed by complex switching of multiple adjacent segments (“avalanches”) of various orientations such that closed magnetization loops (“vortices”) are favored. Ferromagnetic P2T differ from previously studied ASI systems due to their aperiodic translational symmetry and numerous inequivalent pattern vertices, which drive nonstochastic switching of segment polarizations.


AIP Advances | 2018

Coexistence of ferromagnetism and spin glass freezing in the site-disordered kagome ferrite SrSn2Fe4O11

Larysa Shlyk; Sabine Strobel; B. Farmer; L. E. De Long; Rainer Niewa

Single-crystal x-ray diffraction refinements indicate SrSn2Fe4O11 crystallizes in the hexagonal R-type ferrite structure with non-centrosymmetric space group P63mc and lattice parameters a = 5.9541(2) A, c = 13.5761(5) A, Z = 2 (R(F) = 0.034). Octahedrally coordinated sites are randomly occupied by Sn and Fe; whereas tetrahedrally coordinated sites are exclusively occupied by Fe, whose displacement from ideal trigonal-bipyramidal coordination causes the loss of inversion symmetry. DC magnetization data indicate SrSn2Fe4O11 single crystals undergo ferro- or ferri-magnetic order below a transition temperature TC = 630 K with very low coercive fields Hc⊥ = 0.27 Oe and Hc// = 1.5 Oe at 300 K, for applied fields perpendicular and parallel to the c-axis, respectively. The value for TC is exceptionally high, and the coercive fields exceptionally low, among the known R-type ferrites. Enhanced coercivity and thermomagnetic hysteresis suggest the onset of short-range, spin glass order occurs below Tf = 35 K. Optica...


ieee international magnetics conference | 2017

Macrospin reversals and spin wave softening in isolated nodes of Kagome-like structures: Statics and dynamics

F. Montoncello; L. Giovannini; J. B. Ketterson; Wonbae Bang; L. E. DeLong; B. Farmer

In complex networks of ferromagnetic macrospins, like artificial spin ices or artificial quasi-crystals, much interest has focused on the dynamics of Dirac strings, i.e. the apparently irregular path followed by macrospin reversals, producing a magnetic charge drift across the network.


IEEE Transactions on Magnetics | 2013

Observation of Robust FMR in Permalloy Quasiperiodic Arrays

Vinayak Bhat; Justin Woods; B. Farmer; L. E. De Long; J. T. Hastings; Joseph Sklenar; J. B. Ketterson

We have used ferromagnetic resonance (FMR) at fixed frequency 9.7 GHz to investigate permalloy thin films patterned with antidots to form a five-fold quasicrystal pattern. For DC applied fields H below 3.5 kOe, we observed robust FMR spectra exhibiting two-fold rotational symmetry instead of the five-fold symmetry expected for quasicrystals. Dynamic micromagnetic simulations of the FMR spectra performed at H = 1 kOe and 12 kOe exhibit two-fold and ten-fold rotational symmetry, respectively. The ten-fold symmetry observed in simulations is consistent with a saturated state of isolated write fields. We infer the two-fold rotational symmetry observed for H = 1 kOe is due to an unsaturated state of five-fold write fields closely spaced on a square lattice.


Physica C-superconductivity and Its Applications | 2014

Non-stochastic switching and emergence of magnetic vortices in artificial quasicrystal spin ice

Vinayak Bhat; B. Farmer; N. Smith; E. Teipel; Justin Woods; Joseph Sklenar; J. B. Ketterson; J. T. Hastings; L. E. De Long


Physical Review B | 2018

Mutual influence between macrospin reversal order and spin-wave dynamics in isolated artificial spin-ice vertices

F. Montoncello; L. Giovannini; Wonbae Bang; J. B. Ketterson; Matthias B. Jungfleisch; A. Hoffmann; B. Farmer; L. E. De Long


arXiv: Strongly Correlated Electrons | 2018

Magnetically Charged Superdomain Walls In Square Artificial Spin Ice

Jct Lee; Sk Mishra; Vinayak Bhat; R Streubel; B. Farmer; X Shi; Led Long; I McNulty; P Fischer; Sd Kevan; S. Roy


Nanoscale | 2018

Imaging the magnetic structures of artificial quasicrystal magnets using resonant coherent diffraction of circularly polarized X-rays

Daeho Sung; Chulho Jung; Byeong-Gwan Cho; Wonhyuk Jo; Hee-Sung Han; Ki-Suk Lee; Vinayak Bhat; B. Farmer; L. E. De Long; Ki Bong Lee; D. J. Keavney; Dong Ryeol Lee; Changyong Song

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E. Teipel

University of Kentucky

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