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

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

Pedagogical animations Six animations are shown : without phase shifter (-> no contrast) normal with absorber with spin flipper, vertical analyzer (-> no contrast) with spin flipper, horizontal analyz

Pictures The instrument Brisp2 008 The big shielding Internal Shielding BRISP at work Detector Monochromator Honeycomb collimator Sample chamber BRISP team Data reduction Standard treatment of BRISP r

Miscellaneous D19 - Introduction D19 is a diffractometer combining a high flux monochromatic neutron beam and a large area detector that covers Horizontal 120° x Vertical 30°. This provides the user c

Manual This manual is an introduction to the use of the two-axis diffractometer D20 at the ILL. It first describes the general features of the instrument and try to provide the minimum information nee