2021
DOI: 10.1080/23746149.2021.1871862
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Future applications of the high-flux thermal neutron spectroscopy: the ever-green case of collective excitations in liquid metals

Abstract: The European landscape of neutron sources for research applications is changing and the major European joint effort, the European Spallation Source (ESS) currently under construction in Lund (Sweden), is progressing. The high flux source ESS is designed to deliver slow neutrons with a longpulse time structure, a rather unique feature, with characteristics optimised to maximise the instrument performances and the experimental throughput. This is expected to result in unprecedented scientific capability over bro… Show more

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Cited by 4 publications
(4 citation statements)
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References 188 publications
(332 reference statements)
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“…Nowadays, liquid metals have been actively studying, because they are known as advanced functional materials for novel applications which exploit the material flexibility coupled to the high electrical conductivity such as notably transient devices, soft robotics, biomedical sensing, and health monitoring [20]. The impact of liquids Hg and Ga as adaptive sensors and Ga-based alloys as biomaterials [21] is receiving a great attention.…”
Section: Discussionmentioning
confidence: 99%
“…Nowadays, liquid metals have been actively studying, because they are known as advanced functional materials for novel applications which exploit the material flexibility coupled to the high electrical conductivity such as notably transient devices, soft robotics, biomedical sensing, and health monitoring [20]. The impact of liquids Hg and Ga as adaptive sensors and Ga-based alloys as biomaterials [21] is receiving a great attention.…”
Section: Discussionmentioning
confidence: 99%
“…Therefore the model based on more than one mode, interacting with each other, is employed [4] where the combination of two basic modes, described by the amplitude operator Q Q j , were employed by assuming the same dynamic characteristics, that is energy ( hω Q j ) and self-energy [(σ j (Q, ω)], identified by a branch index j = 1 and 2. As in other investigations the self-energy was approximated by its simplest form having the correct ω dependence, that is σ j (Q, ω) = i j (Q) ω, where j (Q) depends only on Q and, in the low damping limit, is the full width at half maximum of S j j (Q, ω).…”
Section: Modeling the Scattering Datamentioning
confidence: 99%
“…This model [4] is known to be able to provide a straightforward description of the positive dispersion and the global evolution of the measured dynamic structure factors of Fig. 3.…”
Section: Modeling the Scattering Datamentioning
confidence: 99%
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