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Scintag XDS 2000 PTS Diffractometer

The phenomenon of diffraction occurs when penetrating radiation, such as X-rays, enters a crystalline substance and is scattered. The direction and intensity of the scattered (diffracted) beams depends on the orientation of the crystal lattice with respect to the incident beam. Any face of a crystal lattice consists of parallel rows of atoms separated by a unique distance (d-spacing), which are capable of diffracting X-rays. In order for a beam to be 100% diffracted, the distance it travels between rows of atoms at the angle of incidence must be equal to an integral multiple of the wavelength of the incident beam. D-spacings which are greater or lesser than the wavelength of the directed X-ray beam at the angle of incidence will produce a diffracted beam of less than 100% intensity.

Our diffractometer utilizes a powdered sample, a goniometer, and a fixed-position detector to measure the diffraction patterns of unknowns. The powdered sample provides (theoretically) all possible orientations of the crystal lattice, the goniometer provides a variety of angles of incidence, and the detector measures the intensity of the diffracted beam. The resulting analysis is described graphically as a set of peaks with % intensity on the Y-axis and goniometer angle on the X-axis. The exact angle and intensity of a set of peaks is unique to the crystal structure being examined. In a multi-component mixture, confusion can arise when two or more components have a peak in the same, or nearby, location on the X-axis. It is for sorting out these mixtures that a good search/match engine or a search method becomes most important.

The X-Ray diffraction method is most useful for qualitative, rather than quantitative, analysis (although it can be used for both).


Specifications:
  • Identify and, in some cases, quantify phases in solids and powders and thin films.
  • Measure crystal lattice parameters, residual stress, texture, crystallite size.
  • X-ray reflectivity studies.
  • Seifert ID3000 computer controlled solid state x-ray generator with a 2000 W 1x10 mm normal focus Cu target x-ray tube.
  • Liquid N2 detector.
  • Pentium II 350 MHz PC (Windows NT) running Scintag DMSNT Diffraction Management System Software v 1.35a
  • ICDD Powder Diffraction Database Library
  • Crystallographic analysis software package
  • Quantitative Analysis Package
  • Scan range from 2 - 165 degrees 2Q
  • Microstepping stepper motors with a minimum step size of 0.0003125 degrees.
  • Continuous digital two theta scan rates from 0.1 - 120 deg./min.
  • Continuously variable goniometer radius from 170 to 300 mm.
    Maximum sample size for texture measurement is 2.5 cm long, 1.5 cm wide, and 1.23 cm deep.

Contact information
Phil Anderson
4715 E. Ft Lowell Rd
Tucson, AZ 85712
(520)322-2308
pla@u.arizona.edu


University of Arizona
/ College of Engineering and Mines / Materials Science and Engineering
Mines Building, Room 135
P.O. Box 210012
The University of Arizona
Tucson, AZ 85721-0021