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signatures in two-dimensional cone beam interferometrySarenac, D.*; Gorbet, G.*; Clark, C. W.*; Cory, D. G.*; Ekinci, H.*; Henderson, M. E.*; Huber, M. G.*; Hussey, D. S.*; Kapahi, C.*; Kienzle, P. A.*; et al.
Physical Review Research (Internet), 6(3), p.L032054_1 - L032054_8, 2024/09
Neutron interferometry has played a distinctive role in fundamental science and characterization of materials. Moir neutron interferometers are candidate next-generation instruments: they offer microscopy-like magnification of the signal, enabling direct camera recording of interference patterns across the full neutron wavelength spectrum. Here we demonstrate the extension of phase-grating moir interferometry to two-dimensional geometries. Our measurements of phase topologies and gravitationally induced phase shifts are in good agreement with theory.
Sarenac, D.*; Gorbet, G.*; Kapahi, C.*; Clark, C. W.*; Cory, D. G.*; Ekinci, H.*; Garrad, D. V.*; Henderson, M. E.*; Huber, M. G.*; Hussey, D.*; et al.
Physical Review Research (Internet), 6(2), p.023260_1 - 023260_15, 2024/06
Phase-grating moire interferometers (PGMIs) have emerged as promising candidates for the next generation of neutron interferometry, enabling the use of a polychromatic beam and manifesting interference patterns that can be directly imaged by existing neutron cameras. However, the modeling of the various PGMI configurations is limited to cumbersome numerical calculations and backward propagation models which often do not enable one to explore the setup parameters. Here we generalize the Fresnel scaling theorem to introduce a k-space model for PGMI setups illuminated by a cone beam, thus enabling an intuitive forward propagation model for a wide range of parameters and experimental setups.
Ca + 
Cm collisions 10% above the Coulomb barrierG
tz, M.*; Gtz, S.*; Kratz, J. V.*; D
llmann, Ch. E.*; Mokry, Ch.*; Runke, J.*; Thrle-Pospiech, P.*; Wiehl, N.*; Sch
del, M.; Ballof, J.*; et al.
Nuclear Physics A, 961, p.1 - 21, 2017/05
被引用回数：9 パーセンタイル：53.88(Physics, Nuclear)Ca + Cmの多核子移行反応の運動学を多層捕集箔法と放射化学分離法を用いて調べた。過去の研究で、生成核の同位体分布の幅が、標的よりも重い同位体より軽い同位体の方が広いことが知られており、標的よりも軽い同位体の方がエネルギーロスの大きな衝突の成分が多いためと解釈されてきた。しかし、本研究で両者の平均的な全運動エネルギー損失、すなわち平均励起エネルギーの大きさが測定され、両者に大きな違いがないことが明らかになった。このことは過去の解釈と矛盾するため、本研究では、高い励起エネルギーを持って生成される標的よりも重い同位体は核分裂によって失われる、という新しい解釈を提案した。
