Recherche

206OXHV26 (7T) Stray Magnetic Field and Siting Issues on D17 We present below the magnetic forces measured on D17 with the 7T vertical field magnet 206OXHV26 and the new spin analyser installed in the

Stray Magnetic Field and Siting Issues on IN22 We present below the magnetic forces measured on IN22 with the 12 and 15 T symmetric split-pair coil magnets CRG-CEA and 158OXHV26 . Two configurations h

Spherical Neutron Polarimetry simulations. Case of pure magnetic signal: M real and Pi // Ox The incident polarisation vector is chosen parallel to the X axis, i.e. parallel to the scattering vector Q

Spherical Neutron Polarimetry simulations. Case of pure magnetic signal: M real and Pi // Oy The incident polarisation vector is chosen parallel to the Y axis, i.e. perpendicular to the scattering vec

Spherical Neutron Polarimetry simulations. Case of pure magnetic signal: M real and Pi // Oz The incident polarisation vector is chosen parallel to the Z axis, i.e. perpendicular to the scattering vec

Spherical Neutron Polarimetry simulations. Case of pure magnetic signal: M complex and Pi // Ox The incident polarisation vector is chosen parallel to the X axis, i.e. around the scattering vector Q.

Spherical Neutron Polarimetry simulations. Case of pure magnetic signal: M complex and Pi // Oy The incident polarisation vector is chosen parallel to the Y axis, i.e. perpendicular to the scattering

Spherical Neutron Polarimetry simulations. Case of pure magnetic signal: M complex and Pi // Oz The incident polarisation vector is chosen parallel to the X axis, i.e. around the scattering vector Q.

Spherical Neutron Polarimetry simulations. Case of mixed nuclear/magnetic signal : N and M in phase, Pi // Ox The incident polarisation vector is chosen parallel to the X axis, i.e. parallel to the sc

Spherical Neutron Polarimetry simulations. Case of mixed nuclear/magnetic signal : N and M in phase, Pi // Oy The incident polarisation vector is chosen parallel to the Y axis, i.e. perpendicular to t