Supervisor: Dr. Alexander Kobzev Students: Given Madiba Sithenkosi - - PowerPoint PPT Presentation

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Supervisor: Dr. Alexander Kobzev Students: Given Madiba Sithenkosi - - PowerPoint PPT Presentation

Supervisor: Dr. Alexander Kobzev Students: Given Madiba Sithenkosi Mlala Phuti Ngoepe Frank Laboratory of Neutron Physics (FLNP) 11 October 2012 To investigate the element content and depth distribution of different elements in various


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Supervisor: Dr. Alexander Kobzev Students: Given Madiba Sithenkosi Mlala Phuti Ngoepe

Frank Laboratory of Neutron Physics (FLNP)

11 October 2012

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To investigate the element content and depth distribution of different elements in various samples using the following methods:

} Rutherford Backscattering Spectroscopy (RBS) } Elastic Recoil Detection (ERD) } Nuclear Reaction Analysis (NRA) } Particle Induced X- ray Spectroscopy (PIXE)

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SLIDE 3

} Accelerator principles

  • Van de Graaff (parameters)

} Theoretical background } Results

  • Rutherford backscattering spectroscopy (RBS)
  • Elastic recoil detection (ERD)
  • Nuclear reaction analysis (NRA)
  • Particle induced X- ray emission (PIXE)

} Conclusion

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Van de Graaff accelerator schematic Van de Graaff accelerator schematic

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EG EG-

  • 5 accelerator

5 accelerator

  • Helium ion and proton energy:

0.9 – 3.5 M eV

  • Accelerator belt velocity:

20 m/ s

  • Beam at target: 1.5 mm
  • Tank pressure: 10 atm
  • EG-5 has six beam lines

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SLIDE 6

Inside experimental chamber Inside experimental chamber

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Experimental setup Experimental setup

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Kinematic factor Kinematic factor

K – Kinematic factor E1 – Energy after scattering E0 – Initial energy M1 – Mass of accelerated particle M2 – Mass of target atoms θ – Scattering angle

1

2 1 2 2 2 2 1 1 2 1

( sin ) cos M M M E K E M M θ θ   − +   = =   +    

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Kinematic factor at 170 Kinematic factor at 170o

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Rutherford formula Rutherford formula

σ1 – Scattering cross section Z1 – Atomic number (beam) Zi – Atomic number (target) E – Energy of accelerated particle θ – Scattering angle

2 1 2 2 2 1 2 2 1 1 1 2 2 2 2 1

cos 1 sin 2 sin 1 sin

i i i

M M Z Z e E M M θ θ σ θ θ           + −                 =           −       

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SLIDE 11

Rutherford Backscattering Spectroscopy Rutherford Backscattering Spectroscopy

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Channel

200 400 600 800

Counts

500 1000 1500 2000 2500 3000

Experimental Simulated

Ti Mo Si substrate

E = 2.035 M eV

α = 15o β = 5o θ = 170o

Experimental Simulated

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SLIDE 12

RBS RBS

Layers Thickness Element Concentrations (%) (1015 atoms/ cm2) (nm) Ti M o Si 1 2450 140.5 1.0 2 909 80.3 1.0 3 90000 1.0

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SLIDE 13

RBS RBS

Channel

200 300 400 500 600 700 800

Counts

200 400 600 800 1000 1200 1400 1600 1800

Experimental Simulated

Si Ge Si substrate

E = 1.0 M eV

α = 30o β = 20o θ = 170o

Experimental Simulated

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SLIDE 14

RBS RBS

Layers Thickness Element Concentrations (%) (1015 atoms/ cm2) (nm) Si Ge 1 170 37.3 1.0 2 150 30.1 1.0 3 160 38.4 1.0 4 150 28.1 1.0 5 165 38.4 1.0 6 140 28.1 1.0 7 175 39.6 1.0 8 135 27.1 1.0 9 60 18.1 1.0 10 150 26.4 0.2 0.8 11 3500 1.0

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SLIDE 15

Elastic Recoil Detection Elastic Recoil Detection

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Channel

200 400 600 800

Counts

50 100 150 200 250 300

Experimental Simulated

Proton Deuterium E = 2.297 M eV

α = 75o β = 75o θ = 30o

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SLIDE 16

ERD ERD

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Layers Thickness Element Concentrations (%) (1015 atoms/ cm2) (nm) H D C Ni 1 200 26 0.46 0.04 0.44 0.06 2 300 38.1 0.41 0.03 0.4 0.16 3 300 37.6 0.37 0.02 0.33 0.28 4 300 35.7 0.23 0.05 0.19 0.575 5 300 35.1 0.16 0.005 0.1 0.735 6 300 33.8 0.05 0.004 0.946 7 1000 0.03 0.002 0.968

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NRA and RBS NRA and RBS

Nuclear Reaction Analysis H+ RBS 4He+

Channel

200 400 600 800 1000

Counts

500 1000 1500 2000 2500 3000

Experimental Simulated

Nb Si

E = 2.012 M eV

α = 10o β = 0o θ = 170o

Channel

400 600 800 1000

Counts

500 1000 1500 2000

Experimental Simulated

Si Nb O Li

E = 2.012 M eV

α = 10o β = 0o θ = 170o

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SLIDE 18

NRA (H NRA (H+

+) and RBS (4He

) and RBS (4He+

+)

)

Layers Thickness Element Concentrations (%) (1015 atoms/ cm2) (nm) Li O Nb Si 1 8000 777.5 0.25 0.55 0.2 2 600 85.9 0.2 0.4 0.2 0.2 3 350 104.7 0.3 0.5 0.1 0.1 4 700 122.5 0.2 0.2 0.05 0.55 5 90000 1.0

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Particle Induced X Particle Induced X-

  • ray Emission

ray Emission

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M oseley M oseley’ ’s law s law

  • ν – frequency of X-ray quantum
  • Rc – Rydberg constant
  • Z – atomic element
  • Sn – Screening constant
  • n – main quantum number

n c

Z S R n − ν =

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Calibration: PIXE Calibration: PIXE

200 400 600 800 1000 1200 1400 1600 10 20 30 40 50 60 70 80 90

26.35 16.84 20.12 17.75 13.94 11.89 3.35 Intensity Channel number

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Aerosol: PIXE Aerosol: PIXE

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Aerosol: RBS Aerosol: RBS

600 650 700 750 800 1000 2000 3000 4000

Aerosol Ep= 2.005 MeV

Θ = 135

Si Al Na F O N C Ca S Fe Backscattering yield Channel number

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Table of concentrations Table of concentrations

Element

  • Concen. At.

% Method Element Concen. At. % Method C 41 RBS K 0.1 PIXE N 20.5 RBS Ca 0.53 RBS O 28 RBS Mn 0.007 PIXE F 2.6 RBS Fe 0.14 RBS Na 2.5 RBS Cu 0.002 PIXE Mg 1.3 RBS Zn 0.01 PIXE Al 1.3 RBS As 0.001 PIXE Si 1.8 PIXE Sr 0.0006 PIXE S 0.2 RBS Zr 0.005 PIXE Cl 0.01 PIXE Ba 0.01 PIXE

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Conclusion Conclusion

  • Depth distribution
  • M ethods are non-destructive
  • Investigate depth resolution near 10 nm

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Acknowledgements Acknowledgements

  • Dr. Jacobs
  • Prof. Lekala
  • M r. M alaza
  • National Research Foundation
  • Department of Science and Technology
  • Joint Institute for Nuclear Research

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THANK YOU!

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