You are here: Home Users and Science Experimental facilities Structure of soft matter ID13 - Microfocus Beamline Single Crystal Diffractometry

Single Crystal Diffractometry

last modified 13-11-2006 16:54

Pbo
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:

  • Goniometer: single, horizontal rotation axis (PHI) with 1 µm eccentricity. Semi-automatic sample transfer and sample alignment tools are available [6].
  • Detector: MarCCD (2D CCD, ~ 130mm diameter, 2048x2048 pixels), mounted on a translation rail, which is itself mounted on a rotation arm. Rotation arm and PHI axis are aligned to be colinear.
  • Cryosystem: Oxford Cryostream 700 (temperature range: 85 K to 400 K), with possible helijet adaption upon request.
  • 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 :

  • screening experiments: > ~5 µm diameter
  • full data collection: > ~15 µm diameter (assuming sufficient crystal quality).
  • 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

    sam_prep
    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:

  • optimum mounting length 25 mm (magnet touching surface to sample distance)
  • maximum mounting length is 26 mm
  • minimum mounting length 20 mm (increasing danger of icing with short loops

    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:

  • 20 mm < mounting length 25 mm (magnet touching surface to sample distance)
  • maximum capillary length = mounting length + 3mm

    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.

    m7_2
    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

    m7_molecule
    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).


  • European Synchrotron Radiation Facility