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Published byAshlyn Walton Modified over 9 years ago
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FRANK LABORATORY OF NEUTRON PHYSICS ION BEAM ANALYSIS STANCIU-OPREAN LIGIA SUPERVISOR DR. KOBZEV ALEXANDER
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MAIN PROPERTIES OF VAN DE GRAAF ACCELERATOR Accelerated ions 1 H +, 2 H +, 3 He +, 4 He +, 12 C +, 14 N +, 16 O + Energy range 0.7 – 3.5 MeV Energy spread` < 500 eV Accuracy in energy 1 keV Beam intensities H – 30 A He – 10 A C, N, O ~ 1 A Beam lines 6 Height of the accelerating tube 6 m Diameter of the tank 2.5 m Pressure in the tank 8 at
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Rutherford Backscattering Spectrometry M1 –mass of incident particle М2 –mass of scattering atom; - scattering angle
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Backscattering crossection Backscattering crossection Z 1 – the atomic number of incident particles; Z 2 – the atomic number of scattered atom; е – the electronic charge; E 0 – the energy of the projectile immediately before scattering
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RBS SPECTRUM FOR W/La/Si – SAMPLE
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PIXE Method PIXE Method Moseley lawMoseley law frequency of X-ray; Rc –Rydberg’s constant; Z –atomic number; Sn – screening constant; n –main quantum number;
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PIXE SPECTRUM FOR ENVIRONMENT SAMPLE
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RBS PIXE C 34 N 28 О 19 F 3.4 Na 5.1 Mg 1.8 Al 3.3 Si 3.5 S 0.02 K 0.2 Ca 1.2 Mn 0.015 Fe 0.40 Cu 0.003 Zn 0.01 As 0.001 Zr 0.003 Ba 0.02 Sample N1
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Conclusion 1.RBS and PIXE are undamaging methods. 2. Any element with mass from 1 up to 200 can be identified exactly. 3. The depth resolution reaches 2-3 nm. 4. The actual accessible depth for analysis is near 2-3 mkm for He-beam and is 10-15 mkm for proton beam. 5.The sensitivity is different for the various samples, but for heavy elements it can be less, than 0.1 atomic %.
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