frank labortory of neutron physics ion beam analysis

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FRANK LABORTORY OF NEUTRON PHYSICS ION BEAM ANALYSIS 1. Diale Boitshoko Phenyo (UWC) 2. Sefage Amanda (UZ) 3. Nkosi Steven (CSIR) Republic of South Africa Supervisor: A.P. Kobzev (JINR, Dubna) JINR Summer Practice 2009

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1. Diale Boitshoko Phenyo (UWC) 2. Sefage Amanda (UZ) 3. Nkosi Steven (CSIR) Republic of South Africa Supervisor: A.P. Kobzev (JINR, Dubna ). FRANK LABORTORY OF NEUTRON PHYSICS ION BEAM ANALYSIS. VAN DE GRAAFF ACCELERATOR EG-5. Main Characteristics - PowerPoint PPT Presentation

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Page 1: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

FRANK LABORTORY OF NEUTRON PHYSICS

ION BEAM ANALYSIS

1. Diale Boitshoko Phenyo (UWC)

2. Sefage Amanda (UZ)

3. Nkosi Steven (CSIR)

Republic of South Africa

Supervisor: A.P. Kobzev (JINR, Dubna)JINR Summer Practice 2009

Page 2: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

VAN DE GRAAFF ACCELERATOR EG-5

Main Characteristics

•Energy region 0.9-3.5 MeV

•Energy spread less than 500eV

•Beam intensity 10µA for He and

30µA for H.

Types of ions used

•4He+ and H+

JINR Summer Practice 2009

Page 3: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

ACCELERATOR EG-5

JINR Summer Practice 2009

Page 4: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

ANALYTICAL METHODS

• Rutherford Backscattering Spectrometry (RBS)

• Elastic Recoil Detection Analysis (ERDA)

• Particle Induced X-ray Emission (PIXE)

JINR Summer Practice 2009

Page 5: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

2

12

121

21

22

0

12

cos)sin(

MM

MMMEE

m

PRINCIPLE OF RBSKINEMATIC FACTOR

Atomic mass of target. ZJINR Summer Practice 2009

Page 6: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

2122

12

24

2

22

2122

12

222

21

)sin(sin

)]cos)sin[(4)4

(),(

MMM

MMME

eZZER

SCATTERING CROSS SECTION

Z1 - Atomic number of incident particle

Z2 - atomic number of target

M1 – Atomic mass of incident particle

M2 – Atomic mass of target

Ѳ - Scattering angle

JINR Summer Practice 2009

Page 7: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

PRINCIPLE OF RBS

1

x+

θ1ΔX

θθ2

ΩDetector

outinm EEEKE )( 021

E0, Z1, M1

E1, Z2, M2

21 смэВdxdE

N

Stopping cross section

N-Number of particles in the layer

dxdE -Energy loss per unit length

JINR Summer Practice 2009

Page 8: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

RBS EXPERIMENTAL RESULTS

A = σΩ .Q . Nt

A – total number of detected particlesQ – total no. of inc. ParticlesNt – no. of target atoms per unit area

Layer Element Conc. (at.%)

1 Niobium 100

2

Titanium 79Oxygen 21

3 Silicon 100

JINR Summer Practice 2009

Channel number

Page 9: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

Layer Element Thickness (nm)

1 Titanium 418

2 Niobium 254

3 Silicon 2 mm

RBS EXPERIMENTAL RESULTS

Channel number

JINR Summer Practice 2009

Page 10: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

RBS EXPERIMENTAL RESULTS

JINR Summer Practice 2009

200 400 600 800 1000 12000

500

1000

1500

2000

2500

3000

3500

4000

Yie

ld S

c.

Channel number

CO

TiSi

Si-Substrate

Energy = 2.01 MeV, H+ Detector Layer Element Conc.at% Thickness (nm)

1 Titanium 80Carbon 10 180Oxygen 10

2 Titanium 4042.3Silicon 50

Oxygen 103 Silicon 100 2 mm

Page 11: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

PRINCIPLE OF ELASTIC RECOIL DETECTION ANALYSIS

JINR Summer Practice 2009

Page 12: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

ERDA-RESULTS

200 400 600 800 1000 12000

500

1000

1500

2000

2500

3000

3500

4000

Bac

kSca

tterin

g In

ters

ity

Channel number

experimental simulated

Silicon

Carbon

Energy = 2.297 MeV, 4He+

Detector = 135

Thickness = 2600E+15 at./cm2

Element Conc. (%)

H ydrogen 35

C arbon 35

Silicon 30

Cou

nts

JINR Summer Practice 2009

Page 13: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

ERDA – RESULTS cont,d

Element Conc. (%)

H ydrogen 26

C arbon 60

O xygen 14

Channel number

Channel number

Thickness = 1570E+15 at./cm2

JINR Summer Practice 2009

Page 14: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

PRINCIPLE OF PIXE

Characteristics X-rays

JINR Summer Practice 2009

Page 15: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

PRINCIPLE OF PIXE

Characteristics X-rays

JINR Summer Practice 2009

Page 16: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

PRINCIPLE OF PIXE

Moseley law

• Rc – Rydberg’s constant• Z – atomic number• Sn – screening constant• n – main quantum number• ν - frequency of X-ray

quantum

JINR Summer Practice 2009

Page 17: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

200 400 600 800 1000 1200 1400 16000

10

20

30

40

50

60

70

80

90

26.35

16.8420.12

17.7513.94

11.893.35

Inte

nsity

Channel number

CALIBRATION

JINR Summer Practice 2009

Page 18: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

AEROSOL ANALYSIS BY PIXE & RBS

JINR Summer Practice 2009

Page 19: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

550 600 650 700 750 8000

500

1000

1500

2000

2500

3000

3500

4000B

acks

catte

ring

yiel

d

Channel number

Aerosol E

p=2.005 MeV

=1350

S

Na AlSi

Ca Fe

F

O

NC

AEROSOL ANALYSIS BY PIXE & RBS

JINR Summer Practice 2009

Page 20: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

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

AEROSOL ANALYSIS BY PIXE & RBS

JINR Summer Practice 2009

Page 21: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

CONCLUSION

• Non-destructive methods ( Different fields i.e. Electronic devices , Multi layer-structures,

geologist, archaelogist etc)

• Determine structure and composition of materials

• Elemental analysis

• Elemental concentration, depth profile in thin films ( < 1 at.%)

JINR Summer Practice 2009

Page 22: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

ELEMENT Ti Nb

MINIMUM THICKNESS, nm

30 10

MAXIMUM THICKNESS, nm

1800 1500

REAL THICKNESS, nm

264 169,5

SENSITIVITY, at/cm2 2x10xx16 1x10xx16

CONCLUSION cont.d

JINR Summer Practice 2009

Page 23: FRANK LABORTORY OF NEUTRON PHYSICS  ION BEAM ANALYSIS

Siyabonga

JINR Summer Practice 2009