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| Hauptseite > Publikationsdatenbank > Diffraction Enhancement of the Stern—Gerlach Effect for a Neutron in a Crystal > print |
| Hauptseite > Publikationsdatenbank > Diffraction Enhancement of the Stern—Gerlach Effect for a Neutron in a Crystal > print |
| 001 | 891095 | ||
| 005 | 20230111074308.0 | ||
| 024 | 7 | _ | |a 10.1134/S0021364019210124 |2 doi |
| 024 | 7 | _ | |a 0021-3640 |2 ISSN |
| 024 | 7 | _ | |a 1090-6487 |2 ISSN |
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| 037 | _ | _ | |a FZJ-2021-01366 |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a Voronin, V. V. |0 P:(DE-HGF)0 |b 0 |
| 245 | _ | _ | |a Diffraction Enhancement of the Stern—Gerlach Effect for a Neutron in a Crystal |
| 260 | _ | _ | |a Heidelberg [u.a.] |c 2019 |b Springer |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a The spatial splitting of an unpolarized neutron beam into two spin components in an inhomogeneous magnetic field (an analog of the Stern-Gerlach experiment) with small gradients has been measured at the Laue diffraction in a crystal and Bragg angles θB = (78–82)° close to a right one. The spatial splitting of the beam at a path length of 21.8 cm has reached (4.1 ± 0.1) cm (at a maximum gradient of 1.5 G/cm and a diffraction angle of 82°). In the absence of the crystal, the splitting would be ∼ 3.8 × 10−7 cm at the same distance and gradient. The experimental enhancement coefficient is ∼ 105 tan2 θB, which is consistent with the theory. |
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| 700 | 1 | _ | |a Semenikhin, S. Yu. |0 P:(DE-HGF)0 |b 1 |e Corresponding author |
| 700 | 1 | _ | |a Shapiro, D. D. |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Braginetz, Yu. P. |0 P:(DE-HGF)0 |b 3 |
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| 773 | _ | _ | |a 10.1134/S0021364019210124 |g Vol. 110, no. 9, p. 581 - 584 |0 PERI:(DE-600)1472906-4 |n 9 |p 581 - 584 |t JETP letters |v 110 |y 2019 |x 1090-6487 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/891095/files/Voronin2019_Article_DiffractionEnhancementOfTheSte.pdf |
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