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The Long and the Short of it: Measuring picosecond half-lives… Paddy Regan Dept. of Physics, University of Surrey, Guildford, GU2 7XH, UK e-mail: [email protected]

The Long and the Short of it: Measuring picosecond half-lives…

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The Long and the Short of it: Measuring picosecond half-lives…. Paddy Regan Dept. of Physics, University of Surrey, Guildford, GU2 7XH, UK e-mail: [email protected]. Electromagnetic Transition Rates. EM transition rates ( = 1 / decay mean lifetime, t ) are related to the - PowerPoint PPT Presentation

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Page 1: The Long and the Short of it: Measuring picosecond half-lives…

The Long and the Short of it:Measuring picosecond half-lives…

Paddy Regan

Dept. of Physics, University of Surrey,

Guildford, GU2 7XH, UK

e-mail: [email protected]

Page 2: The Long and the Short of it: Measuring picosecond half-lives…

Electromagnetic Transition RatesEM transition rates ( = 1 / decay mean lifetime, ) are related to the multipole order of the transition by the expression

Tif (L) = 1 / = (ang.mom. fact) x (E)2L+1 x B(L:Ii->If)

Thus e.g, for E2 transitions, B(E2:Ii->If) = k. E-5 x Tif

Thus, if B(E2) is big (lots of overlap of wavefunctions), Tif is big and is small (i.e. fast = collective);

If B(E2) is small is big (i.e. slow = isomer)Also, slower for larger L values, (classically further away)

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For lifetimes, , in units of seconds and and E in MeV,

T(E1) =1/= 1.59 x 1015 E3 B(E1)

T(E2) =1/ = 1.22 x 109 E5 B(E2)

T(E3) = 1/ = 5.70 x 102 E7 B(E3)

B(ML) in units of e2fm2L

i.e., transition rates get slower (i.e., longer lifetimes associated with) higher order multipole decays.

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Annual Review of Nuclear Science (1968) 18 p265-290

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In-beam, electronic technique (t)

eg, PHR et al. Nucl. Phys. A586 (1995) p351

Fusion-evaporation reaction with pulsed beam (~1ns), separated by fixed period (~500ns). Using coincidence gamma-rays to see across isomer

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136Xe+198PtDobon et al.,

nano to microsecond isomer tagging ?

Page 9: The Long and the Short of it: Measuring picosecond half-lives…

Identification of new ‘seniority’ isomer in 136Ba, N=80 isotone.

J.J. Valiente-Dobon, PHR, C.Wheldon et al., Phys. Rev. C69 (2004) 024316

T1/2=91(2) ns

Page 10: The Long and the Short of it: Measuring picosecond half-lives…

Structure of 8+ final state changes from 134Xe -> 136Ba ?See Valiente-Dobon, PHR, Wheldon et al., PRC69 (2004) 024313

Isomer decayalso depends on structureof final state

N=80, (h11/2)-210+ isomers

Page 11: The Long and the Short of it: Measuring picosecond half-lives…

Pair Truncated Shell Model

Calculations (by Yoshinaga,Higashiyama et al. Saitama)predict yrast 8+ in 136Ba no longer mostly (h11/2)-2

but rather, (d5/2)2(g7/2)2

Page 12: The Long and the Short of it: Measuring picosecond half-lives…

BaF2 ‘fast timing’ data from H. Mach et al. Contribution to ENAM 2001

Allows an ordering of the gammas under isomer from their (~ps) lifetimes.

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From Henryk Mach et al., 96Pd.

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Use (BaF2,BaF2) coincidences below isomers to get B(E2) values ( & order gamma-transitions)

96Pd H. Mach et al.,

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100Pd

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Fusion evaporation…good way to populate nuclei for study…put into (high spin) excited states. Fuse beam and target nucleus and boil off excess energy via neutron evaporation. e.g. 80Se beam (Z=34; N=46) + 24Mg target (Z=12; N=12) to make 104Pd* (Z=46; N=58). Boil off 4 neutrons to leave 100Pd which decays by gamma to ground state. Whole process from creation to gs takes < 1ns.

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100Pd • Z=46 4 proton holes in Z=50:

• N=54 4 neutron particles above N=50

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24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m

4+ →2+2+ →0+

6+ →4+

100Pd

Page 40: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m

tof ~ 4ps

tof~ 9ps

tof~ 12ps

tof~ 15ps

tof~ 30ps

Page 41: The Long and the Short of it: Measuring picosecond half-lives…

Es = Eo (1 +0.058cos(41.5o))Es = Eo * 1.0434

Es = Eo (1 +0.058cos(139.5o))Es = Eo * 0.9558

Eo Es (139.5o) Es (41.5o)

665 636 694

750 717 783

773 739 807

798 763 833

Time of flight = 16.8 m per ps

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24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m4+ →2+

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24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m4+ →2+

Page 44: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m4+ →2+

Page 45: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m4+ →2+

Page 46: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m

4+ →2+2+ →0+

6+ →4+

Page 47: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m

6+ →4+

Page 48: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m

6+ →4+

Page 49: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m

6+ →4+

Page 50: The Long and the Short of it: Measuring picosecond half-lives…

24Mg (80Se , 4n) 100Pd EB=268 MeV, v/c ~5.8c

75m

150m

200m

250m

500m

6+ →4+

Page 51: The Long and the Short of it: Measuring picosecond half-lives…

Some (cool) numbers?• Power: From 2 ps transition of E=800 keV

• P = E / t = (800 x 1.6 x 10-16 J) / (2 x 10 -12 s)→ 0.064 Watts per decay

Assume ~ 1000 per second measured = 64 W from per second…singles rate much larger (x 100 at least)

Beam Velocity: 280 MeV = ½ Mv2

v = sqrt ( 280 x 1.6 x 10-13 J x 2 / 80 x 1.66 x 10-27kg) v= 2.6x107 m/s = 8.6% speed of light.

Recoil velocity (measured from Es = Eo ( 1+ v/c COS ()) ~ 5.6% of c vrec ~ 1.7x 107ms-1 = 16.8 m per ps

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• Now over to Vassia to get the final (accurate numbers)….does the structure change (from ~vibrator to ~rotor) with spin ?

• To be continued…