Recherche

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

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

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

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

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 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 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 // 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 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 real and Pi // Oy The incident polarisation vector is chosen parallel to the Y axis, i.e. perpendicular to the scattering vec