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Thermal, electric and spin transport in superconductor/ferromagnetic-insulator structures
2019
A ferromagnetic insulator (FI) attached to a conventional superconductor (S) changes drastically the properties of the latter. Specifically, the exchange field at the FI/S interface leads to a splitting of the superconducting density of states. If S is a superconducting film, thinner than the superconducting coherence length, the modification of the density of states occurs over the whole sample. The co-existence of the exchange splitting and superconducting correlations in S/FI structures leads to striking transport phenomena that are of interest for applications in thermoelectricity, superconducting spintronics and radiation sensors. Here we review the most recent progress in understandin…
Potential for the introduction of soybean into crop rotations in the Normandy region
2022
Europe is looking for alternatives for soybean importations and needs more local production of protein crops to meet the growing demand for proteins both for feed and food. One strategy to meet this demand could be to expand the soybean production areas (Karges et al, 2022). However, some preliminary information is required before starting producing a new crop. Firstly, farmers lack technical and economic references such as adapted technical management or potential yield but also the impact on gross margin of crop rotation. Then advisors, also needs similar information when working with farmers. Finally, collectors may need the potential total volume potentially produced in a given area to …
"Table 110" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2019
$|{\cos{\theta}^{\star}}|$ normalized differential cross-section at parton level. The parton level phase-space is limited to the region $p_T^{t,1} > 500~$GeV, $p_T^{t,2} > 350~$GeV.
"Table 170" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2018
${cos{\theta}^{\star}}$ correlation matrix for relative differential cross-section in parton level
"Table 168" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2018
${cos{\theta}^{\star}}$ correlation matrix for absolute differential cross-section in parton level
"Table 169" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2018
${cos{\theta}^{\star}}$ covariance matrix for relative differential cross-section in parton level
"Table 167" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2018
${cos{\theta}^{\star}}$ covariance matrix for absolute differential cross-section in parton level
"Table 95" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ coll…
2018
${cos{\theta}^{\star}}$ absolute differential cross-section in parton level
"Table 168" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2019
$|{\cos{\theta}^{\star}}|$ correlation matrix for the absolute differential cross-section at parton level
"Table 167" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2019
$|{\cos{\theta}^{\star}}|$ covariance matrix for the absolute differential cross-section at parton level