1999
DOI: 10.1088/1367-2630/1/1/309
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The electron analogue to the Faraday rotation

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Cited by 14 publications
(6 citation statements)
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“…In principle, four different effects may explain the experimental facts at least qualitatively: (i) electric dipole forces; (ii) current-induced magnetic torque [29]; (iii) coherent spin-rotation at the interface [154]; and (iv) intra-atomic NCM [153]. As already sketched in section 3.2.1 and figure 10 the apex of the tip is probably formed by a small cluster of magnetic material that protrudes from the spherical end of the tip.…”
Section: Spatial Resolutionmentioning
confidence: 99%
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“…In principle, four different effects may explain the experimental facts at least qualitatively: (i) electric dipole forces; (ii) current-induced magnetic torque [29]; (iii) coherent spin-rotation at the interface [154]; and (iv) intra-atomic NCM [153]. As already sketched in section 3.2.1 and figure 10 the apex of the tip is probably formed by a small cluster of magnetic material that protrudes from the spherical end of the tip.…”
Section: Spatial Resolutionmentioning
confidence: 99%
“…Another possibility, i.e. coherent spin-rotation, may be caused by the precession of the electron spin around the magnetic field [154]. In an SP-STM experiment it may occur in the vacuum gap between the sample and the tip where the magnetic field can be substantial.…”
Section: Spatial Resolutionmentioning
confidence: 99%
“…Another successful method is transmission of spin-polarized electrons (usually produced with a GaAs source) through freestanding ferromagnetic films [6]. This way, the spin motion which shows up as precession of the electron spin-polarization (ESP) P around the magnetization direction and as relaxation of P towards the magnetization M was investigated [7,8].…”
mentioning
confidence: 99%
“…21 The origin of the motion of the electron-spin polarization in ferromagnetic films is the spin-dependent scattering of electrons within the film and at its surface. 22,23 Supposing a completely spin-polarized electron beam with its initial spin polarization P 0 perpendicular to the magnetization M of the film, the spin part of the incident electron wave function is described by a coherent superposition of a majority-spin ↑ and a minority-spin ↓ wave function ͑with their moments parallel and antiparallel to M, respectively͒ with equal amplitudes. Because of spin-dependent scattering, the spin wave function of the beam after reflection from the film reads: ϰ ͉r ↑ ͉exp͑i ↑ ͒ ↑ + ͉r ↓ ͉exp͑i ↓ ͒ ↓ with ͉r ↑,↓ ͉ and ↑,↓ are, respectively, the moduli and the phases of the spin-dependent reflection amplitudes.…”
mentioning
confidence: 99%
“…To observe a maximum spin motion P 0 has to be oriented perpendicularly with respect to M of the film. 22,23 It is only in a noncollinear geometry that M can exert a torque on the spinpolarization vector. Upon reflection from the sample, the specular beam passes through a retarding field energy analyzer.…”
mentioning
confidence: 99%