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24 results for “Neutron scattering”
simulation of Li diffusion in neutron scattering experiment
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Vibrational Neutron Scattering Spectra for Undoped and Doped P3HT
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Neutron Scattering data
<p> Background corrected radially averaged intermediate angle neutron scattering (Barotron) for <strong>a)</strong> supersaturated saturated Tb(NO<sub>3</sub>)<sub>3</sub> /D<sub>2</sub>O solutions using the electromagnet; <strong>b)</strong> supersaturated Tb(NO<sub>3</sub>)<sub>3</sub> using the permanent magnet solution; <strong>c)</strong> and <strong>d)</strong> are the 2D patterns of a) without and with 100 mT (Barotron detector l=2.85Å, d=0.1m); <strong>e)</strong> ultra-wide angle scattering (7C2) without and with a parallel magnetic field; <strong>f)</strong> very small angle neutron scattering (PA20, l=6Å, d=18m) for concentrated Tb(NO<sub>3</sub>)<sub>3</sub> /D2O solutions. Blue open squares show the empty beam path, open circles are Tb(NO<sub>3</sub>)<sub>3</sub>without an applied magnetic field, red filled squares are with 0.6 T applied magnetic field perpendicular to the beam.Background corrected radially averaged intermediate angle neutron scattering (Barotron) for <strong>a)</strong> supersaturated saturated Tb(NO<sub>3</sub>)<sub>3</sub> /D<sub>2</sub>O solutions using the electromagnet; <strong>b)</strong> supersaturated Tb(NO<sub>3</sub>)<sub>3</sub> using the permanent magnet solution; <strong>c)</strong> and <strong>d)</strong> are the 2D patterns of a) without and with 100 mT (Barotron detector l=2.85Å, d=0.1m); <strong>e)</strong> ultra-wide angle scattering (7C2) without and with a parallel magnetic field; <strong>f)</strong> very small angle neutron scattering (PA20, l=6Å, d=18m) for concentrated Tb(NO<sub>3</sub>)<sub>3</sub> /D2O solutions. Blue open squares show the empty beam path, open circles are Tb(NO<sub>3</sub>)<sub>3</sub>without an applied magnetic field, red filled squares are with 0.6 T applied magnetic field perpendicular to the beam.</p>
Neutron Scattering data
<p>Background corrected radially averaged intermediate angle neutron scattering (Barotron) for <strong>a)</strong> supersaturated saturated Tb(NO<sub>3</sub>)<sub>3</sub> /D<sub>2</sub>O solutions using the electromagnet; <strong>b)</strong> supersaturated Tb(NO<sub>3</sub>)<sub>3</sub> using the permanent magnet solution; <strong>c)</strong> and <strong>d)</strong> are the 2D patterns of a) without and with 100 mT (Barotron detector l=2.85Å, d=0.1m); <strong>e)</strong> ultra-wide angle scattering (7C2) without and with a parallel magnetic field; <strong>f)</strong> very small angle neutron scattering (PA20, l=6Å, d=18m) for concentrated Tb(NO<sub>3</sub>)<sub>3</sub> /D2O solutions. Blue open squares show the empty beam path, open circles are Tb(NO<sub>3</sub>)<sub>3</sub>without an applied magnetic field, red filled squares are with 0.6 T applied magnetic field perpendicular to the beam.</p>
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