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Volumn 80, Issue 5, 2009, Pages

Strong enhancement of the direct magnetoelectric effect in strained ferroelectric-ferromagnetic thin-film heterostructures

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EID: 70249094610     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.054102     Document Type: Article
Times cited : (31)

References (31)
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    • Liu, G.1    Nan, C.W.2    Sun, J.3
  • 21
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    • This formula follows from the relation u 33 s = λs M3 2 / Ms2 combined with the field dependence of the mean magnetization M3 described by the Langevin function f (x) =coth (x) -1/x; see 10.1063/1.1850618
    • This formula follows from the relation u 33 s = λs M3 2 / Ms2 combined with the field dependence of the mean magnetization M3 described by the Langevin function f (x) =coth (x) -1/x; see X. J. Zheng and X. E. Liu, J. Appl. Phys. 97, 053901 (2005), and references therein. 10.1063/1.1850618
    • (2005) J. Appl. Phys. , vol.97 , pp. 053901
    • Zheng, X.J.1    Liu, X.E.2
  • 22
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    • This relation provides the volume conservation in strained Terfenol-D. It holds for the macroscopic deformations resulting from magnetization reorientations in a model polycrystal, where the crystallites have a cubic lattice with the same spatial orientation and a randomly oriented magnetization with fixed magnitude.
    • This relation provides the volume conservation in strained Terfenol-D. It holds for the macroscopic deformations resulting from magnetization reorientations in a model polycrystal, where the crystallites have a cubic lattice with the same spatial orientation and a randomly oriented magnetization with fixed magnitude.
  • 23
  • 24
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    • We suppose that the single-domain state can be created in an epitaxial ferroelectric film even at small misfit strains near um =0, where the formation of ferroelastic (non- 180°) domains becomes energetically favorable [10.1103/PhysRevB.73.214103
    • We suppose that the single-domain state can be created in an epitaxial ferroelectric film even at small misfit strains near um =0, where the formation of ferroelastic (non- 180°) domains becomes energetically favorable [V. G. Kukhar, N. A. Pertsev, H. Kohlstedt, and R. Waser, Phys. Rev. B 73, 214103 (2006)]. The domain nucleation may be suppressed by rapid cooling of a thin film subjected to a strong electric field. 10.1103/PhysRevB.73.214103
    • (2006) Phys. Rev. B , vol.73 , pp. 214103
    • Kukhar, V.G.1    Pertsev, N.A.2    Kohlstedt, H.3    Waser, R.4
  • 28
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    • The strain sensitivities S1 and S2 of the in-plane polarization components are not further discussed in this paper. These sensitivities differ from zero in the monoclinic r phase and the orthorhombic aa phase and give rise to nonzero transverse ME coefficients α13 and α23.
    • The strain sensitivities S1 and S2 of the in-plane polarization components are not further discussed in this paper. These sensitivities differ from zero in the monoclinic r phase and the orthorhombic aa phase and give rise to nonzero transverse ME coefficients α13 and α23.
  • 29
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    • 10.1103/PhysRevB.78.212102
    • N. A. Pertsev, Phys. Rev. B 78, 212102 (2008). 10.1103/PhysRevB.78.212102
    • (2008) Phys. Rev. B , vol.78 , pp. 212102
    • Pertsev, N.A.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.