Beamline Phone Number:
+44 (0) 1235 778711
Principal Beamline Scientist:
Alessandro Bombardi
Tel: +44 (0) 1235 778087
E-mail: [email protected]
Email: [email protected]
Tel: +44 (0) 1235 778056
The I16 diffractometer is a 6-circle kappa geometry diffractometer, capable of aligning a sample in any orientation relative to the incident beam.
The large sample space provides space to fit a wide range of sample environments including cryostats, fields and various detectors.
We use a eulerian geometry to drive the sample and detector positions, however these are not always the true motors, for example Chi is a composite of real motors kappa and kphi.
The Eulerian PDs used to drive the diffractometer angles are:
|
Description |
Limits (conservative) |
---|---|---|
chi | composite angle perpendicular to beam | 98-0 Deg |
eta | sample rotation || to beam, vertical | 0-110 Deg & < Delta |
delta | detector arm, verticle, depends on pos do | 0-130 Deg |
phi | sample rotation, kphi is real motor | 0-360 Deg |
gamma | detector arm, horizontal | 0-130 Deg |
mu | sample rotation, horizontal | 0-100 Deg & < gam |
sx/sy | sample translation (rotates with phi) | -2 - +2 mm |
We typically operate the diffratometer in one of two geometries - Vertical or Horizontal.
In this geometry the scattering plane is vertical in the lab frame. We rotate the detector arm (Delta) vertically as the 2theta angle, eta rotates the sample parallel to the plane (sample theta), chi rotates the sample perpendicular to the scattering plane and phi rotates the sample about the scattering plane.
An example specular reflection scan is:
pos delta c2th([0,0,12]) eta c2th([0,0,12])/2 chi 90 phi 0
In this geometry the scattering plane is horizontal in the lab frame. We rotate the detector axis (gamma) horizontally as the 2theta angle, mu rotates the sample parallel to the plane (sample theta), chi rotates the sample perpendicular to the scattering plane and phi (chi=0) or eta (chi=90) rotates the sample about the scattering plane.
An example specular reflection scan is:
pos gamma c2th([0,0,12]) mu c2th([0,0,12])/2
The software Diffcalc is used to move the diffractometer directly in reciprocal space, based on the orientation of the crystal.
The orientation of the crystal is determined by either setting Orientations manually (based on the visible surfaces of the crystal) or through finding and indexing Bragg reflections.
An example of the alignment commands is provided below:
Here the rotation matrices for the diffractometer are given, based on Euler rotation matrices.
The full sample rotation is an intrinsic rotation about the following axes:
Detectors:
The following PDF document explains the rotations matrices:
Diffractometer Rotation Matrix
Freely available python code:
If you have any comments, suggestions or corrections, please contact a member of the beamline staff.
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