2000
DOI: 10.1016/s0921-4526(99)01334-4
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Observation of neutron standing waves at total reflection of polarized neutrons by precision gamma-spectroscopy

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Cited by 9 publications
(4 citation statements)
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“…The sample was a bilayer Gd(5 nm)/Fe(100 nm)//glass(substrate) with the sizes 100(along beam)×60(width)×5(substrate thickness) mm 3 . The initial motivation of the investigation of this sample was demonstration of neutron standing waves [36,37] using enhanced neutron absorption in the absorbing Gd layer. But during the experiment, the beam splitting in a low parallel external field was recorded on the position-sensitive detector.…”
Section: Methodsmentioning
confidence: 99%
“…The sample was a bilayer Gd(5 nm)/Fe(100 nm)//glass(substrate) with the sizes 100(along beam)×60(width)×5(substrate thickness) mm 3 . The initial motivation of the investigation of this sample was demonstration of neutron standing waves [36,37] using enhanced neutron absorption in the absorbing Gd layer. But during the experiment, the beam splitting in a low parallel external field was recorded on the position-sensitive detector.…”
Section: Methodsmentioning
confidence: 99%
“…The presence of the waveguide enhancement in systems with absorbing and ferromagnetic Gd layer can be seen either via dips on the total reflection plateau of non-spin-flip (NSF) reflectivities [10], [11] or as peaks in the spin-flip (SF) channel [7]. In the latter case the vector of magnetization should lie in the sample plane and be normal to the external magnetic field.…”
Section: Samples Designmentioning
confidence: 99%
“…In a study on a layered magnetic Fe/Gd structure deposited on a glass substrate, two polarization states of a neutron beam were used. The difference between the NSW formed with the two polarization states was quantified via the characteristic γ fluorescence after neutron capture by Gd [69]. In another study [70], neutron resonance in a 6 LiF/Ti/Cu/glass layered structure was quantified in simultaneous measurements of neutron reflectivity and the 6 Li(n, α) 3 H nuclear reaction as fluorescence signal.…”
Section: Thin Films On Solid Surfacesmentioning
confidence: 99%
“…This intensity maximum reflects the amplification of the NSW in the 6 LiF cap layer as it results from the resonance condition in the spacer layer. In another study by Aksenov and co-workers it was shown that experiments with NSW can yield specific structural information without the use of element-specific fluorescence radiation [71]. A NSW with a particular spin state was generated in a Cu/Ti/Co/ Ti multilayer structure on a glass substrate in a magnetic field.…”
Section: Thin Films On Solid Surfacesmentioning
confidence: 99%