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Open Access
Abstract: Ferromagnetic resonance (FMR) and x-ray detected FMR (XFMR) results for Permalloy (Py) and [Co/Pt]10/Py films, with and without thin Pt spacers between the [Co/Pt]10 and Py layers, are presented and discussed. The first layer [Co/Pt]10 was chosen due its characteristic perpendicular anisotropy, with the potential to pin neighboring Py spins. However, in practice, the FMR results were found to be dominated by the 50-nm-thick Py films, especially when the thickness of the Pt spacer exceeds 1.5 nm. Nonetheless, out-of-plane FMR measurements reveal interesting behavior. In particular, the uniform k=0 mode is extremely sensitive to the alignment of the magnetic field normal to the film. Misalignment by just 3° shifts the cusp, at Bappz ~ μ0M in the plot of resonance frequency against applied field, upwards to ~ 6 GHz. In addition, out-of-plane VNA-FMR maps reveal the presence of additional modes. For example, a perpendicular standing spin-wave (PSSW)-state, above the cusp at Bappz ≥ μ0M, is clearly identified. However, as the magnetic field is reduced below the cusp, the PSSW state morphs, continuously, through a series of canted spin-wave states (CSSW) into a horizontal standing spin-wave (HSSW) state, increasing in frequency to ~ 9.5 GHz. Finally, the PSSW, CSSW and HSSW states, are accurately interpreted, using a multi-layer model of the Py film.
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Jan 2021
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I10-Beamline for Advanced Dichroism
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Kook Tae
Kim
,
Margaret R.
Mccarter
,
Vladimir A.
Stoica
,
Sujit
Das
,
Christoph
Klewe
,
Elizabeth P.
Donoway
,
David M.
Burn
,
Padraic
Shafer
,
Fanny
Rodolakis
,
Mauro A. P.
Gonçalves
,
Fernando
Gómez-Ortiz
,
Jorge
Íñiguez
,
Pablo
García-Fernández
,
Javier
Junquera
,
Sandhya
Susarla
,
Stephen W.
Lovesey
,
Gerrit
Van Der Laan
,
Se Young
Park
,
Lane W.
Martin
,
John W.
Freeland
,
Ramamoorthy
Ramesh
,
Dong Ryeol
Lee
Diamond Proposal Number(s):
[24797]
Open Access
Abstract: Resonant elastic X-ray scattering (REXS) offers a unique tool to investigate solid-state systems providing spatial knowledge from diffraction combined with electronic information through the enhanced absorption process, allowing the probing of magnetic, charge, spin, and orbital degrees of spatial order together with electronic structure. A new promising application of REXS is to elucidate the chiral structure of electrical polarization emergent in a ferroelectric oxide superlattice in which the polarization vectors in the REXS amplitude are implicitly described through an anisotropic tensor corresponding to the quadrupole moment. Here, we present a detailed theoretical framework and analysis to quantitatively analyze the experimental results of Ti L-edge REXS of a polar vortex array formed in a PbTiO3/SrTiO3 superlattice. Based on this theoretical framework, REXS for polar chiral structures can become a useful tool similar to x-ray resonant magnetic scattering (XRMS), enabling a comprehensive study of both electric and magnetic REXS on the chiral structures.
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Apr 2022
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I10-Beamline for Advanced Dichroism
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Maciej
Dabrowski
,
Takafumi
Nakano
,
David
Burn
,
Andreas
Frisk
,
David G.
Newman
,
Christoph
Klewe
,
Qian
Li
,
Mengmeng
Yang
,
Padraic
Shafer
,
Elke
Arenholz
,
Thorsten
Hesjedal
,
Gerrit
Van Der Laan
,
Zi Q.
Qiu
,
Robert J.
Hicken
Diamond Proposal Number(s):
[17745, 19116, 20760]
Abstract: Insulating antiferromagnets have recently emerged as efficient and robust conductors of spin current. Element-specific and phase-resolved x-ray ferromagnetic resonance has been used to probe the injection and transmission of ac spin current through thin epitaxial NiO(001) layers. The spin current is found to be mediated by coherent evanescent spin waves of GHz frequency, rather than propagating magnons of THz frequency, paving the way towards coherent control of the phase and amplitude of spin currents within an antiferromagnetic insulator at room temperature.
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May 2020
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I06-Nanoscience
I10-Beamline for Advanced Dichroism
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C. J.
Durrant
,
L. R.
Shelford
,
R. A. J.
Valkass
,
R. J.
Hicken
,
A. I.
Figueroa
,
A. A.
Baker
,
G.
Van Der Laan
,
L. B.
Duffy
,
P.
Shafer
,
C.
Klewe
,
E.
Arenholz
,
S. A.
Cavill
,
J. R.
Childress
,
J. A.
Katine
Diamond Proposal Number(s):
[8782, 11585]
Abstract: Spin pumping has been studied within Ta / Ag / Ni81Fe19 (0–5 nm) / Ag (6 nm) / Co2MnGe (5 nm) / Ag / Ta large-area spin-valve structures, and the transverse spin current absorption of Ni81Fe19 sink layers of different thicknesses has been explored. In some circumstances, the spin current absorption can be inferred from the modification of the Co2MnGe source layer damping in vector network analyzer ferromagnetic resonance (VNAFMR)
experiments. However, the spin current absorption is more accurately determined from element-specific phase-resolved x-ray ferromagnetic resonance (XFMR) measurements that directly probe the spin transfer torque (STT) acting on the sink layer at the source layer resonance. Comparison with a macrospin model allows the real part of the effective spin mixing conductance to be extracted. We find that spin current absorption in the outer Ta layers has a significant impact, while sink layers with thicknesses of less than 0.6 nm are found to be discontinuous and super-paramagnetic at room temperature, and lead to a noticeable increase of the source layer damping. For the thickest 5-nm sink layer, increased spin current absorption is found to coincide with a reduction of the zero frequency FMR line width that we attribute to improved interface quality. This study shows that the transverse spin current absorption does not follow a universal dependence upon sink layer thickness but instead the structural quality of the sink layer plays a crucial role.
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Oct 2017
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J.
Li
,
L. R.
Shelford
,
P.
Shafer
,
A.
Tan
,
J. X.
Deng
,
P. S.
Keatley
,
C.
Hwang
,
E.
Arenholz
,
G.
Van Der Laan
,
R. J.
Hicken
,
Z. q.
Qiu
Abstract: Despite recent progress in spin-current research, the detection of spin current has mostly remained indirect. By synchronizing a microwave waveform with synchrotron x-ray pulses, we use the ferromagnetic resonance of the Py (Ni 81 Fe 19 ) layer in a Py/Cu/Cu 75 Mn 25 /Cu/Co multilayer to pump a pure ac spin current into the Cu 75 Mn 25 and Co layers, and then directly probe the spin current within the Cu 75 Mn 25 layer and the spin dynamics of the Co layer by x-ray magnetic circular dichroism. This element-resolved pump-probe measurement unambiguously identifies the ac spin current in the Cu 75 Mn 25 layer.
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Aug 2016
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I06-Nanoscience
I10-Beamline for Advanced Dichroism
|
Robert Alexander James
Valkass
,
Leigh R.
Shelford
,
Chris J.
Durrant
,
Adriana
Figueroa
,
Alex A.
Baker
,
Padraic
Shafer
,
Elke
Arenholz
,
Jeffrey R.
Childress
,
Jordan A.
Katine
,
Gerrit
Van Der Laan
,
Robert
Hicken
Diamond Proposal Number(s):
[8782, 11585, 13063]
Open Access
Abstract: In spin valve structures the damping of a ferromagnetic layer driven at resonance can be modified by the transfer of spin angular momentum into a ‘sink’ ferromagnetic layer. This effect, known as spin pumping, is interface dominated and expected to increase with increasing sink layer thickness up to a saturation absorption depth, previously reported to be 1.2 nm regardless of the sink layer’s composition [1]. Using vector network analyser ferromagnetic resonance (VNA-FMR), we have studied the variation in damping as a function of sink layer thickness in a series of CoMnGe (5 nm) / Ag (6 nm) / NiFe (x nm) spin valves. These measurements show only small variations in the CoMnGe Gilbert damping parameter for x ≤ 1.8 nm, although damping is observed to increase at x = 0.3 and 0.6 nm. Element-resolved x-ray detected ferromagnetic resonance (XFMR) [2] measurements confirm spin transfer torque due to spin pumping as the origin of the damping for x = 1.5 and 1.8 nm, with both thicknesses having the same effective spin mixing conductance, supporting the findings of Ghosh et al [1]. For thicker sink layers the source and sink FMR fields are seen to coincide, hampering the identification of spin pumping. [1] A Ghosh, et al. Physical Review Letters 109, 127202 (2012) [2] M Marcham, et al. Physical Review B 87, 180403 (2013)
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Apr 2016
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I09-Surface and Interface Structural Analysis
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Paul C.
Rogge
,
Ravini U.
Chandrasena
,
Antonio
Cammarata
,
Robert J.
Green
,
Padraic
Shafer
,
Benjamin M.
Lefler
,
Amanda
Huon
,
Arian
Arab
,
Elke
Arenholz
,
Ho Nyung
Lee
,
Tien-Lin
Lee
,
Slavomir
Nemsak
,
James M.
Rondinelli
,
Alexander
Gray
,
Steven J.
May
Diamond Proposal Number(s):
[17824]
Abstract: We investigated the metal-insulator transition for epitaxial thin films of the perovskite CaFeO3, a material with a significant oxygen ligand hole contribution to its electronic structure. We find that biaxial tensile and compressive strain suppress the metal-insulator transition temperature. By combining hard x-ray photoelectron spectroscopy, soft x-ray absorption spectroscopy, and density functional calculations, we resolve the element-specific changes to the electronic structure across the metal-insulator transition. We demonstrate that the Fe sites undergo no observable spectroscopic change between the metallic and insulating states, whereas the O electronic configuration undergoes significant changes. This strongly supports the bond-disproportionation model of the metal-insulator transition for CaFeO3 and highlights the importance of ligand holes in its electronic structure. By sensitively measuring the ligand hole density, however, we find that it increases by ∼5–10% in the insulating state, which we ascribe to a further localization of electron charge on the Fe sites. These results provide detailed insight into the metal-insulator transition of negative charge transfer compounds and should prove instructive for understanding metal-insulator transitions in other late transition metal compounds such as the nickelates.
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Jan 2018
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I10-Beamline for Advanced Dichroism
|
Christoph
Klewe
,
Qian
Li
,
Mengmeng
Yang
,
Alpha T.
N’diaye
,
David M.
Burn
,
Thorsten
Hesjedal
,
Adriana
Figueroa
,
Chanyong
Hwang
,
Jia
Li
,
Robert J.
Hicken
,
Padraic
Shafer
,
Elke
Arenholz
,
Gerrit
Van Der Laan
,
Ziqiang
Qiu
Diamond Proposal Number(s):
[18542, 19116, 20483, 20493, 21616]
|
Apr 2020
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NONE-No attached Diamond beamline
|
Abstract: In this work, we present a study about the chemical and magnetic properties of thin magnetite/cobalt ferrite bilayers deposited on MgO(001). Two series of samples with different CoxFe3–xO4 stoichiometries (x = 1 and x = 0.5) in combination with Fe3O4 layers of varying thickness were prepared by reactive molecular beam epitaxy. The quality of the respective films were controlled by means of in situ X-ray photelectron spectroscopy and low energy electron diffraction. Stoichiometry and electronic structure were carried out by hard X-ray photoelectron spectroscopy. To determine the cationic distribution and magnetic moments, X-ray magnetic circular dichroism measurements were performed and charge transfer multiplet and sum rule calculations were applied. Here we find an enhanced interface magnetization for the bilayers. Additionally, superconducting quantum interference device measurements showed characteristic exchange-spring behavior.
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Oct 2021
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I06-Nanoscience
|
M.
Marcham
,
W.
Yu
,
P.
Keatley
,
L.
Shelford
,
P.
Shafer
,
S.
Cavill
,
H.
Qing
,
A.
Neudert
,
J. R.
Childress
,
J. A.
Katine
,
E.
Arenholz
,
N. D.
Telling
,
G.
Van Der Laan
,
R.
Hicken
Abstract: Precessional dynamics of a Co50Fe50(0.7)/Ni90Fe10(5)/Dy(1)/Ru(3) (thicknesses in nm) thin film have been explored by low temperature time-resolved magneto-optical Kerr effect and phase-resolved x-ray ferromagnetic resonance measurements. As the temperature was decreased from 300 to 140?K, the magnetic damping was found to increase rapidly while the resonance field was strongly reduced. Static x-ray magnetic circular dichroism measurements revealed increasing ferromagnetic order of the Dy moment antiparallel to that of Co50Fe50/Ni90Fe10. Increased coupling of the Dy orbital moment to the precessing spin magnetization leads to significantly increased damping and gyromagnetic ratio of the film while leaving its magnetic anisotropy effectively unchanged.
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Feb 2013
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