Determination of the branching ratios of the decay of I-135 and Xe-135m

Determination of the branching ratios of the decay of I-135 and Xe-135m

INORG. NUCL. CHEM. LETTERS DETERMINATION Vol. 12, pp. 243-245, 1976. BRANCHING OF T ~ Pergamon RATIOS Press. Printed in Great Britain...

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INORG.

NUCL.

CHEM. LETTERS

DETERMINATION

Vol.

12,

pp.

243-245,

1976.

BRANCHING

OF T ~

Pergamon

RATIOS

Press.

Printed

in

Great

Britain

OF THE DECAY OF

1-135 AND X e - 1 3 5 m H . F e u e r s t e i n and J.Oschinski, Gesellschaft f~r K e r n f o r s c h u n g mbH, 75 K a r l s r u h e , G e r m a n y , W e b e r s t r a B e 5 (Received 1 August 1975; in revised form 15 October 1975)

Experiments

performed with the Fission Product Loop

and 1974 (I)(2) the behavior

showed

some unexpected

of X e - 1 3 5 m

and Xe-135.

at that time on the branching and Xe-135m, Iodine

we determined

was separated

technique sample

about

ratios experimentally.

after irradiation

in the FR2 reactor.

into the aqueous phase

available

of the decay of 1-135

from fission products

Io hours

in 1973

concerning

No data were

ratios

these

results

Afterwards

by an extraction of an uranium

it was reextracted

as I-. Two kinds of experiments

were

performed. To determine xenon

the branching

isotopes

ratio of the decay of 1-135,

just produced were

by an argon stream.

This argon

detector,

attached

analyzer.

The Y-lines

Io seconds,

of the xenon Xe-135m

which

isotopes,

the transport

of the argon

the ratio

the branching

After

charcoal

trap where

5 to Io minutes

stream was less

of the production

rates

of

directly.

ratio

of the X e - 1 3 5 m

was used as the sweep gas, passing cooled

time to and

is short compared with the half lives

and X e - 1 3 5 was measured

To determine

at 527 keV and of Xe-135

Because

the delay time at the detector than

over a Ge(Li)

Data 44oo multichannel

of X e - 1 3 5 m

at 25o keV were measured.

swept out of the solution

stream passed

to a N u c l e a r

the

through

the xenon

collection

decay,

a liquid nitrogen

isotopes were

adsorbed.

time the activities

243

helium

of

244

The Decay of I-135 and Xe-135m

Xe-135m and Xe-135 in the trap were measured.

After the

decay of Xe-135m the activity of Xe-135 was measured again. From the initial values for Xe-155m and Xe-155 and the final value of Xe-135,

the branching ratio of the Xe-135m decay

was calculated. For all calculations Xe-135m

the following decay data were used (3):

: half life 15.6 m, 527 keV T-line with 8o.o % yield,

Xe-135

: half life

9.14h,

25o keV y-line with

92.o % yield.

Results

and Discussion

The decay scheme shows the results of our measurements.

\

o5

84.5± 0.5 %/"/

\

Xe- 135 x ~ ~ Cs- 135

The Decay of 1-135 and Xe-135m

245

Because of the half life relation between Xe-135m and Xe-135 and, hence, the very low increase in the counting rate of Xe-135 due to the decay of Xe-135m, the data of the branching ratio of the Xe-135m decay were scattered over a wide range. From our measurements 65 to 88 % of the Xe-135m decays forming Xe-135, the most probable value is higher than 75 %. The results of the branching ratio of the 1-135 decay are in very good agreement with the data now published. Fukuda and Omori found, that 15.o ~ o.8 % of 1-135 decays forming Xe-135m (4), while Meek and Rider list a value of 14.7 % (5). Our experimental result is 15.5 + o.5 %.

Re ference s

I.

I.FUJII, M.OHNO, K.TA/uq~HARA, H.OKANO, T.MIYAZAWA, T.ISHIZAKA, A.YOKOZAWA, H.KA21AI, N.MITSUTSUKA, M.HADA, T.NAGAMINE, J.of the British Nuclear Energy Society 13 (1974),4o3

2.

Results to be published

3.

G.ERDTMANN and W.SOYKA, J ~ - 1 o o 3 - A C

4.

T.FUKUDA and S.OMORI, J.of the Atomic Energy Society

(1973)

of Japan 17 (1975),177 5.

M.E.MEEK and B.F.RIDER, NEDO-12154 (1974)