Here you find information on ID22's

 

X-ray Source

ID22 is located at a "high-ß" section of the storage ring. The X-rays are produced by an U23 in-vacuum undulator (2 m long, 6 mm minimum gap) and a revolver, which offers the choice of a U35 or a U19 undulator (1.6 m long, 11 mm minimum gap). We can cover the entire energy range from 6 keV to 80 keV (2.07 Å. to 0.15 Å in wavelength) with very high photon flux on both the soft- and hard-energy sides.

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Optics Hutch

Powder diffraction is a technique that requires a relatively large beam to illuminate a sufficient volume of sample so as to give a good powder average. Thus there is no focussing; the highly collimated beam from the source is simply monochromated and passes unperturbed to the sample.

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Figure 1: The outline of the ID22 optics hutch.

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Monochromator

The beam is monochromated by a channel cut Si 111 monochromator, with an overall length of 300 mm and a distance of 4 mm between the two diffracting surfaces. The second surface can be tuned to compensate for changes in the Bragg angle caused by changes in the heat load. The first block of the monochromator crystal, which has the highest heat load, is side cooled to about 105 K by copper blocks through which liquid nitrogen flows. Water-cooled slits define the size of the beam incident on the monochromator, and of the monochromatic beam transmitted to the sample, typically in the range 0.5 – 1.6 mm (horizontal) by 0.1 – 1.5 mm (vertical).

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Figure 2: Drawing of the channel cut crystal installed on ID22, showing the beampath at 6 keV and 90 keV.

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Transfocator

The new transfocator, using parabolic cylindrical Al lenses produced by the ESRF, has been installed.

For strain-mapping experiments, the beam will be focussed to 50 µm to improve spatial resolution and efficiency, instead of cutting down the beam with slits. Strain scanning will also benefit from the enhanced hard-energy performance, permitting the investigation of thicker components and those made of highly absorbing materials such as steel and nickel. It will also be possible to combine a focussed beam of energy 80 keV with an area detector to allow the use of the "fast-PDF" technique, complementing the "quality-PDF" obtained by (slow) scanning of the nine analyser crystals.

[Figure: Drawing of the transfocator vessel]

Figure 3: Drawing of the tranfocator to be installed on ID22.

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Experimental Hutch

Diffractometer

Currently, the ID22 diffractometer (manufactured by Rotary Precision Instruments, UK) is the original machine from BM16. It is a heavy-duty construction and is mechanically stable, accurate (nominally ±1 arcsec) and precise (sensitive to displacements of 5x10-5°). It can accept spinning capillary or flat plate specimens. In routine operation, a bank of nine detectors is scanned vertically to measure the diffracted intensity as a function of 2θ. Each detector is preceded by a Si 111 analyser crystal and the detector channels are nominally 2° apart. Multiple crystals operating in parallel increase the efficiency of detecting the diffracted radiation, and for dynamic measurements means that on ID22 the detector arm needs to be scanned by no more than about 2.3° to measure an angular range of 18° in 2θ.

For crystallographic studies, the use of a spinning capillary mounted on the axis of the diffractometer greatly reduces preferred-orientation effects for all but needle-like samples that can align with the capillary axis. With the energy range available, the energy and capillary diameter can be selected to minimise absorption even for samples containing heavy elements. Hence the diffracted intensities can also be very accurate. Indeed, even in cases where a highly absorbing sample is unavoidable, such as when working at the absorption edge of an element in the sample, we would usually prefer to stick a fine layer of sample to the outside of a 1-mm-diameter glass capillary with silicone grease, rather than use a flat plate.

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Figure 4: The ID22 powder diffractometer (right), with the sample changing robot (middle) and the cryostream (left).

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Strain-Scanning Diffractometer (planned)

This diffractometer is the original machine from the first high-resolution powder diffraction line at the ESRF. It has been in operation on BM16, ID31 and ID22 in its vertical scanning configuration for more than 17 years. With the move to ID22, the diffractometer will be refurbished (late 2015) and transformed to a horizontal strain-scanning diffractometer. It will be possible to mount large components and to map their residual strain, exploiting the focussed beam (→ transfocator) at hard-energies.

[Figure: Photo of the Strain scanning Diffractometer]

Figure 5: The ID22 strain-scanning diffractometer.

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Multianalyser stage

The nine analyser crystals are mounted on a single rotation stage, so only a single adjustment of the Bragg angle is needed when changing the wavelength. This multianalyser stage, shown in figure 6 [1] was conceived by the Laboratoire de Cristallographie at the CNRS, Grenoble, and produced as part of the collaboration that supported the construction of BM16. Several powder diffractometers at new national synchrotrons have now adopted this approach and pushed the concept further, e.g. with the diffractometer on beamline 11-BM at APS having 12 detectors; beamline Crystal at Soleil, 21 detectors; and beamline I11 at Diamond, 45 detectors in 5 banks of 9.

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Figure 6: Schematic drawing of the multianalyser stage [1].

A diffracted X-ray must strike the analyser crystal at the correct angle to be diffracted into the detector. Since the acceptance of a Si 111 crystal is very small (a few arcsec, depending on energy), an analyser crystal stringently defines the 2θ angle of diffraction. Since the analyser determines a true angle of diffraction, (rather than inferring the angle from the position of a slit or a pixel on a position-sensitive detector), the use of an analyser crystal renders the positions of diffraction peaks immune to aberrations, such as specimen transparency and modest misalignment of the sample with respect to the axis of the diffractometer, that affect conventional arrangements with a scanning slit or a PSD.

Mechanically and optically having the exact nominal offset between channels is not critical. However, to combine the data from different channels, the offsets need to be known accurately and are obtained by comparing those parts of the diffraction pattern measured by all of the channels. The offsets and channel efficiencies are then computed so that the signals superimpose as closely as possible [2]. A sample such as Si standard NIST 640c is usually used for this calibration step which is performed regularly, and whenever the wavelength is changed.

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Figure 7: Peak from LaB6 NIST 660a, lambda= 0.8  Å, measured on ID31.

With the excellent mechanical integrity of the diffractometer and the high collimation of the beam, the peaks are very narrow, with an instrumental contribution to the FWHM of around 0.003° 2θ, and their positions are accurate and reproducible to a few tenths of a millidegree. Narrow peaks (see figure 7) and accuracy in the peak positions are essential for high quality powder diffraction measurements. Since for flat-plate samples there is no need to be in the θ/2θ condition for narrow peaks, (there being no parafocussing condition to fulfill), the analyser crystals also offer advantages for diffraction at grazing- incidence, and for reflectivity.

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2D detector

The flat panel Perkin Elmer XRD 1611CP3 is now available as a complementary detector for total scattering measurements at high energies.

The XRD 1611 consists of a 41 × 41 cm2 CsI scintillator bonded to an amorphous silicon substrate. The detector has a pixel size of 100 × 100 µm2 and potentially a maximum readout speed of 3.75 frames per second (fps) at maximum resolution. Installed on a motorized linear translation stage (Figure 8) that allows variation of the sample-detector distance between 2500 and 380 mm, it can be used to attain a maximum momentum transfer in one shot (Qmax) of up to 25 Å-1 at 80 keV).

The acquisition workstation is based on the "LIMA" software library developed by ESRF for 2D detector control and data acquisition. On-the-fly dark-current image subtraction is possible to correct for the heterogeneity in the pixel response to photons and afterglow. 2D powder diffraction data reduction software is available for calibration and data integration.

Figure 8: The XRD 1611 detector mounted on a motorized translation stage

 

 

Laboratory Space

The ID22 sample preparation laboratory is located in front of the beamline (room 21.0.04a), towards the outside of the ring. It provides the ID22 users with space, tools and supplies to prepare and mount sample capillaries.

You will also find:

  • standard laboratory items (tweezers, spatulas, scalpels, gloves, goggles, pipettes, syringes, needles, ...)
  • a balance
  • a drying oven and a fridge for chemicals
  • a centrifuge for capillaries (e.g. sedimentation of precipitates)
  • an optical microscope

 

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Figure 9: The sample preparation laboratory at ID22.

If you want to use the ESRF support laboratories, you have to book them in advance via the A-Form. For access to the chemistry laboratory, fill in the user declaration form (.doc)(.pdf) and return it to the user office at least 15 days before the starting date of the experiment.

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References:

[1] Nine crystal multi-analyser stage for high-resolution powder diffraction between 6 and 40 keV. J.-L. Hodeau, P. Bordet, M. Anne, A. Prat, A. N. Fitch, E. Dooryhee, G. Vaughan, and A. Freund, Proc. SPIE, 3448, 353 (1998).

[2] Merging data from a multi-detector continuous scanning powder diffraction system. J. P. Wright, G. B. M. Vaughan, and A. N. Fitch, IUCr Computing Commission Newsletter, 1, 92 (2003).