A compact flat-crystal x-ray spectrometer for external beam pixe measurements

Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms

Volumn 108, Issue 1-2, 1996, Pages 197-204

  Tesauro, P ^a   Mando P A ^a   Parrini, G ^a   Pecchioli, A ^a   Sona, P ^a  

^a NONE

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EID: 0039769012     PISSN: 0168583X     EISSN: None     Source Type: Journal    
DOI: 10.1016/0168-583X(95)00787-3     Document Type: Article

References (25)

1. E. Bovet et al., Nucl. Instr. and Meth. 190 (1981) 613.
2. A. Hitachi et al., Nucl. Instr. and Meth. 195 (1982) 631.
3. H. Hamanaka et al., Nucl. Instr. and Meth. B 35 (1988) 75.
4. J. Iihara et al., Nucl. Instr. and Meth. A 299 (1990) 394.
5. F. Folkmann and F. Frederiksen, Nucl. Instr. and Meth. B 49 (1990) 126.
6. A. Badertscher et al., Nucl. Instr. and Meth. A 335 (1993) 470.
7. F. Folkmann, Z. Phys. D 21 (1991) 263.
8. P. Tesauro, thesis in Physics, University of Florence, 1992, unpublished.
9. S.I. Salem and P.L. Lee, At. Data Nucl. Data Tables 18 (1976) 234.
10. Manufactured by GEC (U.K.).
11. M. Bocciolini et al., Nucl. Instr. and Meth. A 240 (1985) 36.
12. Choog-Ki Kim, Charge-coupled Devices and Systems, eds. M.J. Howes and D.V. Morgan (Wiley, New York).
13. D.J. Burt, Nucl. Instr. and Meth. A 305 (1991) 564.
14. G.R. Hopkinson, Nucl. Instr. and Meth. 216 (1983) 423.
15. D.H. Lumb and G.R. Hopkinson, Nucl. Instr. and Meth. 216 (1983) 431.
16. L. Barsantini, thesis in Physics, University of Florence, 1987, unpublished.
17. G. Bushhorn et al., Nucl. Instr. and Meth. A 346 (1994) 578.
18. P. Del Carmine et al., Nucl. Instr. and Meth. B 75 (1993) 480.
19. F. Fujimoto et al., Phys. Lett. 57A (1976) 263.
20. K. Kawatsura et al., Phys. Lett. 60A (1977) 327.
21. M. Uda et al., Nucl. Instr. and Meth. B 22 (1987) 5.
22. D.F. Anagnostopoulos et al., Z. Phys. D 18 (1991) 139.
23. K. Yoshihara and J. Iihara, Int. J. PIXE 2 (1992) 93.
24. In the latter case, to make the use of alpha particles possible, the geometry of the end of the beam line was slightly modified. The target was in vacuum while a thin window allowed the particle-induced X-rays to be transmitted into the atmosphere, to the diffracting crystal and hence to the CCD as usual.
25. M. Deutsch et al., Phys. Rev. A 51 (1995) 283.