scholarly journals Antiferromagnetic resonance modes for theS= 1/2 kagome antiferromagnet Cs2Cu3SnF12

2011 ◽  
Vol 302 ◽  
pp. 012011
Author(s):  
S Sharmin ◽  
I Umegaki ◽  
H Tanaka ◽  
T Ono ◽  
G Tanaka ◽  
...  
2020 ◽  
Vol 101 (1) ◽  
Author(s):  
V. N. Glazkov ◽  
Yu. V. Krasnikova ◽  
I. K. Rodygina ◽  
J. Chovan ◽  
R. Tarasenko ◽  
...  

1964 ◽  
Vol 136 (5A) ◽  
pp. A1316-A1320 ◽  
Author(s):  
G. L. Witt ◽  
A. M. Portis

2021 ◽  
Vol 8 (1) ◽  
pp. 7
Author(s):  
Xing Chen ◽  
Cuixiu Zheng ◽  
Sai Zhou ◽  
Yaowen Liu ◽  
Zongzhi Zhang

Magnons (the quanta of spin waves) could be used to encode information in beyond Moore computing applications. In this study, the magnon coupling between acoustic mode and optic mode in synthetic antiferromagnets (SAFs) is investigated by micromagnetic simulations. For a symmetrical SAF system, the time-evolution magnetizations of the two ferromagnetic layers oscillate in-phase at the acoustic mode and out-of-phase at the optic mode, showing an obvious crossing point in their antiferromagnetic resonance spectra. However, the symmetry breaking in an asymmetrical SAF system by the thickness difference, can induce an anti-crossing gap between the two frequency branches of resonance modes and thereby a strong magnon-magnon coupling appears between the resonance modes. The magnon coupling induced a hybridized resonance mode and its phase difference varies with the coupling strength. The maximum coupling occurs at the bias magnetic field at which the two ferromagnetic layers oscillate with a 90° phase difference. Besides, we show how the resonance modes in SAFs change from the in-phase state to the out-of-phase state by slightly tuning the magnon-magnon coupling strength. Our work provides a clear physical picture for the understanding of magnon-magnon coupling in a SAF system and may provide an opportunity to handle the magnon interaction in synthetic antiferromagnetic spintronics.


1973 ◽  
Author(s):  
B. Enders ◽  
P. L. Richards ◽  
W. E. Tennant ◽  
E. Catalano ◽  
Hugh C. Wolfe ◽  
...  

1968 ◽  
Vol 39 (2) ◽  
pp. 816-817 ◽  
Author(s):  
I. S. Jacobs ◽  
S. Roberts ◽  
S. D. Silverstein

1971 ◽  
Vol 32 (C1) ◽  
pp. C1-1149-C1-1150
Author(s):  
V. A. SANINA ◽  
E. I. GOLOVENCHITS ◽  
T. A. FOMINA ◽  
A. G. GUREVICH

Sensors ◽  
2021 ◽  
Vol 21 (6) ◽  
pp. 2022
Author(s):  
Benjamin Spetzler ◽  
Elizaveta V. Golubeva ◽  
Ron-Marco Friedrich ◽  
Sebastian Zabel ◽  
Christine Kirchhof ◽  
...  

Magnetoelectric resonators have been studied for the detection of small amplitude and low frequency magnetic fields via the delta-E effect, mainly in fundamental bending or bulk resonance modes. Here, we present an experimental and theoretical investigation of magnetoelectric thin-film cantilevers that can be operated in bending modes (BMs) and torsion modes (TMs) as a magnetic field sensor. A magnetoelastic macrospin model is combined with an electromechanical finite element model and a general description of the delta-E effect of all stiffness tensor components Cij is derived. Simulations confirm quantitatively that the delta-E effect of the C66 component has the promising potential of significantly increasing the magnetic sensitivity and the maximum normalized frequency change ∆fr. However, the electrical excitation of TMs remains challenging and is found to significantly diminish the gain in sensitivity. Experiments reveal the dependency of the sensitivity and ∆fr of TMs on the mode number, which differs fundamentally from BMs and is well explained by our model. Because the contribution of C11 to the TMs increases with the mode number, the first-order TM yields the highest magnetic sensitivity. Overall, general insights are gained for the design of high-sensitivity delta-E effect sensors, as well as for frequency tunable devices based on the delta-E effect.


2021 ◽  
Vol 523 ◽  
pp. 167562
Author(s):  
J. Zhang ◽  
M. Białek ◽  
A. Magrez ◽  
H. Yu ◽  
J.-Ph. Ansermet

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