1995
DOI: 10.1016/0304-8853(95)90006-3
|View full text |Cite
|
Sign up to set email alerts
|

Theory of magnetostatic waves for in-plane magnetized isotropic films

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

4
65
0

Year Published

2009
2009
2024
2024

Publication Types

Select...
4
4

Relationship

0
8

Authors

Journals

citations
Cited by 93 publications
(69 citation statements)
references
References 28 publications
4
65
0
Order By: Relevance
“…Spin waves exhibit a peculiarity that differentiates them from light or sound waves: their dispersion relation is highly anisotropic 13,14 . This means that their energy significantly depends on the relative angle between their propagation direction and the magnetization orientation.…”
mentioning
confidence: 99%
“…Spin waves exhibit a peculiarity that differentiates them from light or sound waves: their dispersion relation is highly anisotropic 13,14 . This means that their energy significantly depends on the relative angle between their propagation direction and the magnetization orientation.…”
mentioning
confidence: 99%
“…The experimentally found spin-wave numbers k SW are combined in Fig. 4(c) with theoretical calculations based on the Damon-Eshbach formula for the lowest order BVMSW mode [16]. The solid line has been calculated based on the measured field value, a film thickness of 5 µm and a saturation magnetisation 4πµ 0 M s = 0.175 T. In comparison, the dashed line is the result of a fit, where the film thickness and the magnetic field were taken as fit parameters.…”
Section: Resultsmentioning
confidence: 99%
“…To a microstrip transducer on the surface of the YIG stripe a 200 ns long microwave pulse with 7.132 GHz carrier frequency was supplied with a 1 µs repetition rate. The configuration was chosen in such a way that the microwave pulse excites a packet of backward volume magnetostatic spin waves (BVMSW) which propagates in the film in the direction of the bias magnetic field [15,16]. Thus, the in-plane wave vector of the excited spin waves has a well defined, unique non-zero component.…”
Section: Setupmentioning
confidence: 99%
“…25 Indeed, a θ = π rotation of the magnetic field results in a decrease of the SWs' excitation efficiency 26,27 and in a drastic change in the SWs amplitude profile, which is confined to the opposite surface of the ferromagnetic layer. 28 In the case of θ = π/2, pure backward volume magnetostatic spin waves (BVMSW) are excited. 22,28 These modes have lower resonant frequencies (Supplementary Note 3) than the DESW and are characterized by a sinusoidal magnetization oscillation profile across the thickness of the ferromagnetic layer.…”
Section: Mw 4 Mwmentioning
confidence: 99%
“…28 In the case of θ = π/2, pure backward volume magnetostatic spin waves (BVMSW) are excited. 22,28 These modes have lower resonant frequencies (Supplementary Note 3) than the DESW and are characterized by a sinusoidal magnetization oscillation profile across the thickness of the ferromagnetic layer. In Fig.…”
Section: Mw 4 Mwmentioning
confidence: 99%