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Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy of Sciences of Czech Republic

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Page 1: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Determination of experimental cross-sections by activation

method

Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner

Nuclear Physics Institute, Academy of Sciences of Czech Republic

Page 2: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Contents

Introduction

Spectrum analysis with DEIMOS32

Cross-sections calculation

Statistical analysis (incertainty calculation)

Results

Page 3: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Introduction

My work consists:

In analysing gamma spectrums from experiment with DEIMOS32…

Experiment = measurement of radioactive sample (activated by activation method in a cyclotron) with different configurations

…To get experimental cross-sections

Page 4: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Spectrum analysis with

DEIMOS32Gamma lines peak analysis with the software DEIMOS 32

Page 5: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Spectrum analysis with

DEIMOS32We’re able to plan possible reactions and isotopes produced

Page 6: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Spectrum analysis with

DEIMOS32Comparison between the result tables from DEIMOS 32 analysis and the internet data base (decay data search) on gamma lines to identify the isotopes

Page 7: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Spectrum analysis with

DEIMOS324 isotopes found from (n,2n) to (n,4n) reactions and 1 isotope (198Au) found from (n,gamma) reaction.

Page 8: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Cross-sections calculation

Nyield calculation:

)()(

)(

11

1

)(

)( 0

irrreal tirr

t

t

foillive

real

areaP

aabspyield e

t

e

e

mt

t

CCoiEI

BECSN

Peak area Self-absorption correction

Beam correction

Dead time correction Decay during cooling and measurement

γline intensity

Detector efficiency

Correction for coincidences

Square-emitter correction

Weight normalization

Decay during irradiation

Page 9: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Cross-sections calculation

Detector efficiency (given):

Nyield approximation:

173815,0

18474,3

3295,18

6493,36

d

c

b

a

)()(

)(

11)(

0

irrreal tirr

t

t

live

real

P

pyield e

t

e

e

t

t

EI

SN

Page 10: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Cross-sections calculation

Nyield calculation:

)()(

)(

11)(

0

irrreal tirr

t

t

live

real

P

pyield e

t

e

e

t

t

EI

SN

Sp: peak areaIγ: gamma line intensity (in %)Treal & Tlive: datas from exp.λ: decay constant

Tirr: irradiation timeT0: beam end – start of measurement

2/1

)2ln(

T

Page 11: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Cross-sections calculation

Cross-section calculation:

Nn: neutrons number (depends on experiment) mfoil: foil massS: foil size (in cm2)

A: mass number (197 for Au)NA: Avogadro’s number (6,022.1023 {mol-1})

Afoiln

yield

NmN

ASN

..

..

Page 12: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Statistical analysis

N yield_average calculation for each isotope => to increase the precision:

n

i i

n

i i

i

averageyield

N

N

N

N

12

12

_ 1 ideimosi NaerrN .

Aerr: incertainty of peak area (data from DEIMOS)

So =>

n

i i

averageyield

N

N

12

_1

1

Page 13: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Statistical analysis

N yield_average calculation for each isotope => to increase the precision:

n

i i

n

i i

i

averageyield

N

N

N

N

12

12

_ 1 ideimosi NaerrN .

Aerr: incertainty of peak area (data from DEIMOS)

So =>

n

i i

averageyield

N

N

12

_1

1

Page 14: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Statistical analysis

Finally:

)1(1

2

2_

2

n

N

NN

X

n

i i

averageyieldi

averageyieldNX _2 yincertaint1

2_

2 .yincertaint1 XNX averageyield

With:

Page 15: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Results

0 2 4 6 8 10 12 1417800

18000

18200

18400

18600

18800

332,983 keV

Series1Series5Series7Series9

Measurement

Num

ber

of

nucle

i

197Au (n, 2n) 196Au

0 2 4 6 8 10 12 1418200

18400

18600

18800

19000

19200

19400

355,684 keV

Series1Series5Series7Series9

Measurement

Num

ber

of

nucle

i (1

0^

6)

Page 16: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Results197Au (n, 4n) 194Au

0 2 4 6 8 10 12 1412450

12500

12550

12600

12650

12700

12750

12800

194Au (328 keV)Series5Series7Series9

Measurement

Nu

mb

er o

f ra

dio

acti

ve

nu

clei

0 2 4 6 8 10 12 1411300

11400

11500

11600

11700

11800

11900

12000

12100

194 Au (293 keV

Series5

Series7

Series9

Measurement

nu

mb

er o

f ra

dio

nu

clid

e [1

0^6]

Page 17: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Results197Au (n, 2n) 196m2Au

0 2 4 6 8 10 12 141000

1100

1200

1300

1400

1500

1600

147,81 keV

Series1Series5Series7Series9

Measurement

Num

ber o

f nuc

lei (

10^6

)

0 2 4 6 8 10 12 14800900

100011001200130014001500

188,27 keV

Series1Series5Series7Series9

Measurement

Num

ber

of

nucle

i

Page 18: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Results

Comments:

Fluctuations are purely systematical

Nyield-average isn’t depending on the configuration

But the difference of Nyield-average (calculated for each gamma line and isotope) is bigger than the uncertainty of weighted average. It comes from the systematic uncertainty of efficiency determination.

Page 19: Determination of experimental cross-sections by activation method Pierre-Jean Viellenave Tutor: Dr. Vladimir Wagner Nuclear Physics Institute, Academy

Thank you for your attention !!!