IEEE International Frequency Control Sympposium and PDA Exhibition Jointly With the 17th European Frequency and Time Forum, 200
DOI: 10.1109/freq.2003.1275210
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Magnetically tunable SAW-resonator

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Cited by 38 publications
(20 citation statements)
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“…Our definition of d f /dH is analogue to the high frequency magnetoelectric coupling coefficient defined by Srinivasan and his coauthors, 4 except that f here means the center frequency of SAW instead of the ferromagnetic resonance frequency. In addition, a similar multilayer structure like Fig.1 has been reported in an early work by Smole et al 15 and recent work by Nan et al 16 However, due to much lower ∆E effect (∼30%) of Metglas in a thin film form, 17 relatively large magnetic…”
Section: Theoretical Modelsupporting
confidence: 77%
“…Our definition of d f /dH is analogue to the high frequency magnetoelectric coupling coefficient defined by Srinivasan and his coauthors, 4 except that f here means the center frequency of SAW instead of the ferromagnetic resonance frequency. In addition, a similar multilayer structure like Fig.1 has been reported in an early work by Smole et al 15 and recent work by Nan et al 16 However, due to much lower ∆E effect (∼30%) of Metglas in a thin film form, 17 relatively large magnetic…”
Section: Theoretical Modelsupporting
confidence: 77%
“…4 respectively are attributed to the ΔE effect, which is a change in Young's modulus E under magnetic fields, and to a dynamic magnetoelastic coupling, which is the interaction between acoustic waves and magnetic moments. Indeed, as described by P. Smole et al [22], applying an external field in hard axis direction leads primarily to a decrease in the elastic modulus towards a local minimum. A further increase of the external field causes a proportional growth of the elastic modulus up to a saturation value where the E modulus is approximately the same as in the initial state.…”
Section: Figmentioning
confidence: 89%
“…SAW resonators with Ni interdigitated transducers (IDTs) were investigated by Kadota et al [24]. Kadota et al [24], Yamaguchi et al [25] and Smole et al [26] have also attempted to describe the physical phenomenon behind the sensor behaviour without any magnetic characterisation of the IDT. In our last report [27] we showed that the shape anisotropy induced in the magnetic IDT can reorient the easy axis of magnetization along the IDT length when the magnetic material is soft, limiting delta-E effects to geometries with applied fields along the acoustic wave propagation.…”
Section: Introductionmentioning
confidence: 99%