D2AM Material science Diffractometer
- Overview of the experiment.
- Description of the 7 circles goniometer.
- Sample environments.
- Detectors available.
- Filters to attenuate the direct beam.
- Description the goniometer slits system.
For question about this experiment and not covered in the following user guide, you can mail d2am.
Overview of the experiment.
The material science diffractometer is a general purpose instrument which was designed to record intensities over a wide dynamical range. It consists of 7 circles allowing users to record data in and out of the polarization plane. The whole instrument lies on a table used for its alignment.
The (x,y,z) axis are defined on Figure 1.
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| Fig 1 | Fig 2 |
- The sample can be oriented through 3 circles of the instrument :
- THETA : sample rotation around a horizontal axis perpendicular to the incident beam (y).
- CHI : sample rotation around x, it is carried by THETA. On figure 1 chi=90.
- PHI : sample rotation around the sample normal. It is carried by CHI and THETA, so that the sample lies horizontal at chi=90 (its normal is z) and vertical at chi=0 (its normal is then y). Note that at CHI=0, THETA and PHI axis are parallel and horizontal.
- The detection line uses the 4 remaining circles. 2 of them adjust the position of the detector arm in and out of the diffraction plane. The 2 last are used to set the analyser at the right energy.
- ALPHA : horizontal motion of the detector arm to allow measurement out of the polarization plane, its full use needs a special configuration of the experiment control program.
- 2THETA ( or tth ) : vertical motion of the detector arm. It is carried by ALPHA.
- THETA_A ( or omegaa ) : bragg angle for the analyser cristal, carried by detector arm.
- 2THETA_A ( or ttha ) : vertical motion of the detector after the analysing crystal.
Description of the 7 circles goniometer.
The main characteristics of the 7 axis are listed below, units and angular values are user values expressed in physical values:
| motor name in spec | angular range (deg.) | speed (deg./s) | step (deg.) | mechanical origin at user angle (deg.) |
| th | -20 +70 | 0.35 | 0.0001 | 6.2337 (6Dec95) |
| chi | -30 +110 | 0.45 | 0.0003 | -2.452 (6Dec95) |
| phi | continuous | 5 | 0.00025 | |
| alpha | -75? +40? | 2.5 | 0.0001 | 1.0488 (29Jun94) |
| tth | -8 +130 | 1 | 0.00005 | 91.8157 (20Sep95) |
| omegaa | continuous | 2.5 | 0.0001 | |
| ttha | |
0.5 | 0.00005 | 0.0955 (20Sep95) |
The spec macro get_7csettings can be used to ensure that user and dial values agree, It use the data file 7c_settings.db of your directory or the standard one (~/specadm/d2_macros/7c_settings.db).
You can get a complementary description of motor axis.
Sample environments available :
- A simple z-motorized sample holder , on which a huber goniometer head can be mounted. Its allows to keep a good confusion sphere.
- An x,y,z-motorized sample holder using the same goniometer head as previous holder. On both last holders, at room temperature, a vacuum chamber with a 80mm diameter Be hemisphere can be used to reduce the sources of diffusion, still allowing a wide access to the reciprocal space.
- A Displex cryostat (15-300K) with Be hemispheres. When it is used, the angular range available for PHI and CHI are restricted to avoid collision. PHI can only be moved from -60 to +60 and CHI from -5 to 95.
- About the cryostat used on the goniometer
- About the high temperature reaction chamber (Anton Parr XRK 900) for powder studies
- here is a pdf document describing size available around the goniometer center.

