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Mass spectrometry in radionuclide analyses P E Warwick, I W Croudace & T Warneke Southampton Oceanography Centre

P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

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Page 1: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Mass spectrometry inradionuclide analyses

P E Warwick, I W Croudace & T Warneke

Southampton Oceanography Centre

Page 2: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Range of mass spectrometric techniques

• TIMS• SIMS• RIMS• AMS• ICPMS

- quadrupole ICPMS- HR-ICPMS- MC-ICPMS

Page 3: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Advantages of mass spectrometry

• Often rapid analyses• Improved data quality

(e.g. 238U:235U ratios)• Permits analyses that are not possible

radiometrically (e.g. 239Pu and 240Pu separately)

• Improved sensitivity for long lived nuclides

Page 4: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Comparison of mass spectrometric techniques

Method Urequiredfordetection

U requiredfor isotoperatios

Isotopes reported Typicalaccuracy

Typicalprecision(2σ)

HRGS 10 µg 1 mg 235U, 238U 10% 10%

Alpha spec 10 ng 10 µg 234U, 238U 10% 5%

Quad ICPMS 5 pg 1 µ g 235U, 236U, 238U 2% 5%

HRICPMS 50 fg 5 µ g 234U, 235U, 236U, 238U 1 – 8% 0.1 – 1%

TIMS 1 fg 1 ng 234U, 235U, 236U, 238U 0.1 – 2% 0.1 – 0.2%

SIMS 5 pg 5 ng 235U, 238U 1 – 5% 10%

MCICPMS 5-50 fg 1 pg 234U, 235U, 236U, 238U 0.1 – 0.2% 0.1 – 0.2%

Modified from Toole et al, 1997

Page 5: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Sensitivity of ICPMS versus alpha spectrometry

0.00000010.0000010.000010.00010.0010.010.1

110

1001000

10000

1E-01 1E+01 1E+03 1E+05 1E+07 1E+09 1E+11

Half life (years)

Min

imum

act

ivity

(Bq)

2 x 106 years 232Th238U

235U

236U

237Np

242Pu234U

233U

230Th

239Pu

243Am/240Pu

226Ra

241Am

210Po228Th 208Po

238Pu

232U209Po

Assuming 10ppt limit5ml solution

Page 6: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Sensitivity of MC-ICPMS versus alpha spectrometry

1E-111E-101E-091E-081E-071E-061E-05

0.00010.0010.010.1

1

1E-01 1E+01 1E+03 1E+05 1E+07 1E+09 1E+11

Half life (years)

Min

imum

act

ivity

(Bq)

ca . 300 years 232Th238U

235U

236U

237Np

242Pu234U

233U

230Th

239Pu

243Am/240Pu

226Ra

241Am

210Po228Th 208Po

238Pu

232U209Po

Assuming 5ppq limit1ml solution

Page 7: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Challenges• Isobaric interferences (e.g. 99Ru on 99Tc)• Polyatomic interferences (e.g. 197Au40Ar on 237Np)• Peak tailing• Isotopic fractionation• Beam instability• Matrix effects• Method blanks

Page 8: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

High Precision Pu Isotope Ratio Measurements

Ian W. CroudaceThorsten Warneke

Phillip E. Warwick

Rex N. Taylor

J. Andy Milton

Geosciences Advisory Unit

Southampton Oceanography Centre

University of Southampton, UK.

www. gau.org.uk

Page 9: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Analytical techniques used for 240Pu/239PuAnalytical techniques used for 240Pu/239Pu

METHOD ADVANTAGE DISADVANTAGE NOMINALPRECISION

2 sigma~50 fg

AlphaSpectrometry

Not suitable because alpha energies interfere

AMS Can measure ~50fg High potential cost ~ 18%

ICPMS Quad High ionisationefficiency

Ion beam instability > 30%

ICPMS Sector High ionisationefficiency

Better stability thanICPMS Quad

~ 3%

TIMS Stable ion beam • Low ionisationefficiency

• No internalinterelementfractionationcorrection

~ 10%

MC-ICPMS • Unstable ion beambut multicollectionnegates this effect

• Interelement massfractionationcorrectioncapability

• Can measure 5 fg

High ionisationefficiency

~ 1%

Page 10: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Some applications for 240Pu/239Pu ratios

Source characterisation

Datingusing impulse and continuous events

Analogous to using 238Pu/239,240Pu but is a clearer discriminator

e.g. the 240Pu/239Pu in weapon’s testing depend on the parameters of each individual test . Therefore the 240Pu/239Pu in the fallout varies with time.

Similar to using 239,240Pu, 241Am or 137Cs

The 240Pu/239Pu versus time has significant features that can be attributed to certain years.

Page 11: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Range of Pu isotope ratiosRange of Pu isotope ratios

0 0.2 0.4 0.6 0.8

Weapon (pre-1960 Los Alamos National Laboratories)

Weapon (modern - Los Alamos National Laboratories)

Weapon grade

Average weapon testChernobyl accident

Power reactors

240Pu/239Pu

GasCooledReactor

BoilingWater

Reactor

PresurisedWater

Reactor

AdvancedGas Cooled

reactor

Pressure Tube BoilingWater

Reactor

Sellafield discharge

1950s Recent

Page 12: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

6 x 0.7 cm i.d.Eichrom 1-X8 ANION RESIN

2 x 0.7 cm i.d.Eichrom UTEVA resin

U

Pu

Stage 1 piggy-back columns

1. Load sample in 10 ml 8M HNO3 with 1drop of concentrated HCl

2. Elute 20 ml 8M HNO3 followed by 30ml of 3M HNO3

Page 13: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Anion UTEVA

Pu eluted with 50 ml offresh 1.2M HCl/H2O2

(50:1)

Pu U

PuU

30ml 3M HNO325ml 9M HCl to remove Th

U eluted with 10ml 0.02M HCl

Plus use a small 2nd anion clean-up column

Removal of any U remaining because 238Uhydride interferes with 239Pu measurement.

STAGE 2Separate the columns

Page 14: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Plutonium isotope ratio measurementPlutonium isotope ratio measurement

Objective: To measure 240Pu/239Pu with a reproducibility and

accuracy <5% 2sd on samples containing <50fg Pu(<150 µBq), to enable the analysis of low-level environmental samples.

Method:Multicollector ICP-MS (Micromass IsoProbe) using :

Peak jump ion counting through a Daly detector with inter-peak normalisation to 236U.

Page 15: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement
Page 16: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

239.0

239Pu

238UH+

Acidblank

238Utail

238.5 239.5

100

200

300

0

counts.sec-1

m/z 239 composition using:

25 ppq Pu

30 ppb U

no 233+236U

Corrections required:

1. On-peak blank subtraction including detector zero

2. Tail from 238U at +1 a.m.u. (200 ppb)

3. 238UH+ interference at m/z 239 (5.5 ppm)

4. Pu addition from 236+233U spike (2 ppm)

5. Mass bias of U-Pu (0.6% amu-1)

Page 17: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Axial Daly

Low 3 Faraday

Low 2 Faraday

239

Sequence1

238

Sequence2

242

236 (235)

Sequence3

240

233(234)

Detector and peak-jump array for Pu isotope ratios using U-double spike

Low 1 Faraday 236 (239)(237)

236

Taylor R.N., Warneke T., Milton J.A., Croudace I.W., Warwick P.E. and Nesbitt R.W. (2001) Plutonium isotope ratio analysis at fg to ng levels by multicollector ICP-MS. J. Anal. At. Spectrom., 16, 279-284.

Page 18: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

-0.7%

-0.6%

-0.5%

-0.4%

-0.3%

-0.2%

-0.7% -0.6% -0.5% -0.4% -0.3% -0.2%236U/233U mass bias amu-1

242Pu/239Pumass bias

amu-1

236U-233U (1:1) added to separated Pu solutions to correct for mass bias and instrument drift between Daly peak jumps

Page 19: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

MC-ICP-MS Site 1120.215

0.220

0.225

0.230

0.235

0.00001 0.0001 0.001 0.01 0.1239Pu Volts

240 Pu

/239 Pu

100fg ml-1

I

1pg ml-1

I

10pg ml-1

I

100pg ml-1

I

1ng 239Pu = 2.3 Bq Therefore only ~1g of a typical UK soil with fallout Pu of 0.3 Bq/Kg is neededfor a precise analysis of the Pu isotope ratio

Rothamstedgrass 1 gram

UK soil

Page 20: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

ICP AMS

TIMSTIMS

RIMS

ICP

this study MC-ICP PJD

0.14

0.16

0.18

0.20

0.22

0.24

0.26

1 10 100 1000 10000

femtograms (g.10-15) of Pu analysed

240Pu239Pu

Page 21: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Accuracy for 240Pu/239Pu atom ratios

Measured 240Pu/239PuCertified 240Pu/239Pu

Atom ratio 0.5 ng/ml 5 ng/ml

NBL122 0.13200.1318 ± 0.001

(n=4)

0.1321 ± 0.0001

(n=3)

NBL 126 0.02090.0211

(n=1)

0.0204

(n=1)

NBL 128 0.0007 -0.0007

(n=1)

UK-Pu-5 0.9662 ± 0.0011 -0.9645 ± 0.0013

(n=7)

NBL –US New Brunswick National Laboratory; UK-Pu-5 - AEA Technology

Page 22: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

An application of the developed method

Establishing a northern latitude fallout record

1 Unique collection of herbage and soil since 1843. Samples collected and stored annually or bi-annually

Given permission to take 50 grams of dried grass from 1945 until 1990

Rothamsted Grass Archive (IACR Rothamsted, Harpenden)

2 Alpine ice core 116 m ice core, Mont Blanc

Page 23: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Warneke et al. Warneke et al.Literature data

NTS June 1952Mike + NTS

US & USSR

France & PRC

ITB Treaty

Warneke, Croudace, Warwick & Taylor (2002) Earth Planetary Science Letters, 203, 1047-57

Page 24: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Warneke, Croudace, Warwick & Taylor (2002) EPSL, 203, 1047-57

Uranium isotope - 238U/235U fallout record - Europe

2sd error 2sd error

-117-112-107-102-97-92-87-82-77-72-67-62-57-52

125 130 135 140238U/235U

dept

h (m

)

Alpine Ice Core

1945

1950

1955

1960

1965

1970

1975

1980

1985

1990

137 137.5 138 138.5238U/235U

year

RothamstedGrass (UK)

Page 25: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Summary

MC-ICP-MS is a highly effective method to measure 240Pu/239Pu in environmental and other samples.

Precise measurements are possible at <10 fg Pu (<30 µBq).

Used to investigate fallout history, global and local nuclear events, sediment ages in estuarine environments, source of plutonium contamination.

Page 26: P E Warwick, I W Croudace & T Warneke Southampton ...resource.npl.co.uk/docs/science_technology/ionising... · TIMS Stable ion beam • Low ionisation efficiency • No internal interelement

Other Possible Future Application

Has great potential in plutonium and uranium bioassay

Precise U isotopic analysis using only 50ml of sample

Typically 1-2 litres urine (bulked monthly) are analysed using alpha spectrometry

Clearly MC-ICPMS can greatly enhance these data quality