Single Crystal Diffractometry
Diffraction pattern from a microcrystal of an olygomeric organic compound
The advent of synchrotron radiation sources (SR) has provided sufficient flux and beam qualities for crystal structure determinations from micrometer-sized crystals (or “microcrystals”) [1]. With the development of third generation synchrotron radiation sources, very intense hard X-ray beams in the µm-range have become available with an acceptable divergence for single crystal experiments [2]. This allows for the probing of very small crystals of less than 250 µm3[3,4] and in exceptional cases sub-µm3 volumes[5]. One can therefore select crystals from powder grains (even from heterogeneous samples) for data collection and structure determination. This is particularly interesting for cases where structure determination from powder data was previously unsuccessful or where Rietveld analysis does not provide the required structural information.
Microgoniometer
The microgoniometer has been developed within the context of an EMBL/ESRF collaboration for protein crystallography. Its main features are:
The microgoniometer was initially designed for protein crystals of less than about 50 µm size. It is able to accept frozen samples or on-site sample freezing (sample cooling with a standard cold stream). The beam size can be defined by either 4, 10 or 30 µm diameter apertures. The crystal size requirements (e.g. needle) are :
A suite of software is provided for microgoniometer control (Microdiff GUI) and data collection (ProDC). The Microdiff GUI allows for perfect centering of the crystal either semi-automatically or manually through motor controlled PHI axis xyz translation stages.
Although the microgoniometer was designed initially for protein crystallography it is of course possible to use it for more general chemical crystallography. Typically, the resolution at the edge of the detector is 0.75 Å at l = 0.721 Å (when the detector is not tilted and PHI axis-detector distance is about 45 mm). Data collections are usually carried out at 100 K. Standard exposure times range from 0.5 s to 30 s per image, with a rotation from 1 to 6 degrees. The time taken for a full data set to be recorded is typically between 20 mn to 2 hours, following crystal quality, exposure time and rotation angle.
Sample Preparation
For protein crystals or fragile samples
Fig.1 Sample geometry for microgoniometer
As there is an integrated motorized sample centering system, it is not possible to use your own goniometer heads. All samples should be mounted on magnetic bases fitting onto a magnet diameter of 9.5 mm (HAMPTON magnet).
Cryo-loops for sensitive microcrystals (e.g. protein crystals):
HAMPTON loops with thin pins work fine. The thick (copper) pins are likely to cause problems because they provoke icing with the cryo-geometry (therefore please use thin pins!).
Geometry:
Capillaries for sensitive microcrystals (no cooling required):
Capillaries should also be mounted on magnetic bases. As there is no cooling, very sensitive samples like protein crystals will be destroyed after a few, or even just one exposure due to radiation damage.
Geometry:
For small molecule crystals or fibers:
The best sample mounting solution currently in use is to paste them with a minimal amount of epoxy glue at the end of a very thin glass tip. This operation can be done on-site using a micromanipulator attached to a Nikon optical microscope (possible magnifications: x400 and x1000). Such glass tips are usually made from borosilicate glass with a micropipette puller. This technique allows a reduction of scattering from the sample support and ensures a low background.
Combination of cryoloops and cryoprotectant (like Paratone-N from Hampton Research or glycerol) is also possible, as for protein crystals. However, with this method problems tend to occur caused by scattering. Even with very small loops, the scattering of the nylon loop and of the cryoprotectant increases the background. If necessary, it is also possible to collect data from crystals mounted inside a capillary (see above for the technical requirements).
An example of crystal structure determination from a small molecular moiety
Aromatic poly(ether ketone)s are at the base of high performance thermoplastic materials. These polymers show high thermostability and chemical resistance. They can be considered as linear polymers of intermediate chain rigidity since the polymer chains consist of bulky phenylene rings linked by ether and ketone groups. This example comes from a family of molecular compounds containing an odd number of phenylene rings (from 5 up to 11), which are all 1,4 substituted except the middle ring, which is 1,3 substituted. A diffraction pattern from this compound is shown at the top of the page.
Picture of the microcrystal used for the data collection. The picture was taken with the microgoniometer microscope before the data collection.
Crystal size: ~ 30x10x1 µm3
Space group: Pnma (62)
Lattice parameters: a = 11.450(4), b = 71.576(2) Å c = 3.947(2) Å
ORTEP drawing (50 % probability) of the molecule.
REFERENCES [1] M.M. Harding; J. Synchrotron Rad. (1996). , 250-259.
[2] C. Riekel; Rep. Progr. in Phys. (2000). , 233-262.
[3] R.W. Broach, R.L. Bedard, S.G. Song, J.J. Pluth, A.Bram, C.Riekel, H.-P.Weber; Chem. Mater. (1999) 11 (8): 2076-2080.
[4] D. Madsen, M. Burghammer, S. Fiedler, H. Müller; Acta Cryst. (1999). B55, 601-606.
[5] R. Neder, M. Burghammer, T. Grasl, H. Schulz, A. Bram, S. Fiedler, C. Riekel Z. f. Kristallographie(1996) 211 (11): 763-765 ;
R. Neder, M. Burghammer, T. Grasl, H. Schulz, A. Bram, S. Fiedler Clays and Clay Minerals(1999) 47 (4): 487-494;
[6] A. Perrakis, F. Cipriani, JC. Castagna, L. Claustre, M. Burghammer, C. Riekel, S. Cusack Acta Cryst. D55, 1765-1770, (1999).