Nova Cygni Nova T Pyxidis -...

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Technische Universität München Measuring Nuclear Reaction Rates One Step at a Time Shawn Bishop, TUM Erice School, 2010 1 Novae Reaction Rates and Measurements Nova Cygni Nova T Pyxidis

Transcript of Nova Cygni Nova T Pyxidis -...

Technische Universität München

Measuring Nuclear Reaction Rates One Step at a Time

Shawn Bishop, TUM

Erice School, 2010 1

Novae Reaction Rates and

Measurements

Nova Cygni Nova T Pyxidis

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Talk Outline

• Astrophysics Primer– Experimental nuclear astrophysics

– The novae phenomenon

– Reaction Rates & Measurements

• Facilities at MLL– Mapping Explosive Rates: Q3D Spectrometer

– Doppler Lifetime Station

• Search for Supernova Signal in the Fossil Record– Intersection of astrophysics, nuclear physics techniques,

geophysics & microbiology

• Summary

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ASTROPHYSICS PRIMER

We are star-stuff. -- Carl Sagan

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Red Giant Companion

Transfer of H+He-rich (or solar-like) material

WD

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24Mg

ONe-Nova Burning Cycles

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20Ne 21Ne 22Ne

21Na 22Na 23Na

22Mg 23Mg32S 33S 34S

33Cl 34Cl 35Cl

34Ar 35Ar 36Ar

25Al

Y

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Main Sequence Companion or AGB

Transfer of H+He-rich (or solar-like) material

WD

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COMPTEL Observation

A. Iyudin et al.

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A Recent Surprise from Nova Cas. 1995

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Directionality Temporal

Spectral

2.5s

Q = 78 keV

4.14s

1.18s

845ms

298ms

2.6s All Roads lead to Romeat 32S

2.5min

What happens here?

94.44%5.56%

34Ar

34ClT1/2=1.5s

T1/2=32min

Isomeric Bypass

Qp

34ClT1/2=1.5s

T1/2=32min

Isomeric Feeding

Qp

, 42%

= 2.128 MeV

S34

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A Thermonuclear Thermometer….

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34mCl: A Thermonuclear Thermometer

• 3+ isomeric state gives rise to 2.12 MeV -line ¼ 42% per decay

• Connected directly to ground by

M3 transition (45.6% of the time)

• Radiation field can also connect

isomeric state to ground state by

induced transitions into higher

states

– If this is large enough, lifetime will

be reduced from 32 min.

• System of coupled differential

equations has been solved

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Whoa…huge lifetime

reduction!

34S

34S*

55.4%0

146

461

666

1230

0+

3+

1+

2+

1+

Exp’t

S.M.

32 min

2.2 s

5.2 ps

9.1 ps

13.7 ps

Coc et al., PRC61 (1999)

34Cl

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Some Key Nuclear Reactions

• 34mCl is a “last chance” -emitter for novae

nucleosynthesis– Bypassed: 33Cl(p,)34Ar

– Produced: 33S(p,)34mCl

– Destroyed: 34mCl(p,)35Ar

• Excited states need to be “mapped out”– Energy, width, branching ratio, spin

• Equipment and Instruments– Q3D spectrometer

– 95% hpGe detector (Canberra)

– Si-detector charged particle telescopes (Micron UK)

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X(p,)Y

Y

ExJp

Q-value

What Needs to be Measured to Determine the Rates

• Rates in explosive h-burning dominated

by resonant proton-capture into excited

states

• Properties of these states uniquely

determine explosive X(p,)Y reaction

rates

• Nuclear properties required:

– Spin

– Excitation energy

– Lifetime

– Proton and/or partial decay-widths

• Goal: Build facilities at MLL to

accomplish these

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Ga

mo

w

Win

do

w

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X(p,)Y Resonant Reaction Rate

µ - reduced mass

Ji,Jp,JX – Spins of: resonance state/

projectile/ target

T – temperature

Ei – energy of state relative to Q

Γp, Γγ – partial width of p- / γ- decay

Bp = Γp/ Γ – branching ratioresonance strength

Key

quantity

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X(p,)Y

-value

Y

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FACILITIES

Measuring Astrophysical Rates one Step at a Time

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• 14 MV Terminal voltage

• Pulsed beam

– 200 ns between pulses

– Pulse width ~ 1 ns

• Cesium sputtering ion source

– Negative ion beams

– No Nobel gas ion beams

(except 3,4He)

• Isobaric separation at

bending magnet

MLL Overview

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Accelerator Laboratory: Overview

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Doppler Shift

Lifetime Station

AMS

Q3D

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MAPPING EXPLOSIVE

REACTION RATES: THE Q3D

Extracting exp(-Ei/kT)

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Q3D High Resolution Spectrograph at TUM

X(p,)Y

Y

ExJp

Q-value

Used to search for, and study, excited states of nuclei by populating those states using one-step transfer reactions: X(3He,t)Y, as an example

Position of triton along Focal Plane is a measure of the excitation energy.

Momentum resolution:

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2.5s

4.14s

1.18s

845ms

298ms

2.6s

2.5min

A Relevant Example: to the 34Cl -ray

Emitter: 33S(p,)34Cl

34Cl excited states populated by33S(p,) can -decay into 34mCl

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34S(3He,t)34Cl, EHe = 25 MeV, q = 15˚

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Ex(34Cl)

5576

5143

Parikh et al. PRC (2009)

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MAPPING EXPLOSIVE

REACTION RATES: THE Q3D

Extracting Bp

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Q3DBeam Y*

Y +

Si Detector

X(p,)Y

Y

ExJp

Q-value

Transfer reaction

in inverse kinematics

X + p

• Transfer reaction populates astrophysical state

• Product Y* will either:

• gamma-decay

• proton-decay

• Decay cone for -decay is small

• Detection of Y with Q3D, reconstruct kinematics,

determine fraction of -decays

• Decay cone for proton decay large

• Detect X and p together with Si, determine

proton decay fraction

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DOPPLER LIFETIME STATION

Extracting the ℏ/t term

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Target Foil

hpGe

Detector

Si Detectors

Y

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Measurement of the Doppler shifted gamma yields velocity distribution of nucleus at instant

of decay.

Decay probability in :

Fraction of N total nuclei that decay with velocity in [(t) cos f, (t + dt) cos f]:

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Velocity distribution formed by an ensemble of N decaying particles:

E.K

.Warb

urte

ne

t al.

Ph

ys. R

ev. 1

60

, 93

8 -

96

3 (1

96

7)

30Turbo Pump

Target ladderStepper Motor

Silicon DE-E telescope

Slider assembly

Target ladder/Target

Copper cold trap

CollimatorLN2 Feedthrough

R = 7 cm

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Target Ladder

DE-E Si Telescope

Collimator Holder

Target Chamber Innards Installation on MLL Beamline

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Doppler Shift Station: Target Chamber

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14 cm

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Commissioning (two weeks ago)

• Chose the 32S(3He,a)31S reaction– 1st and 2nd excited states previously observed

– Lifetimes known

• Energy spacing large– Gammas easily distinguishable

– Alpha particles well-separated kinematically

• 32S beam energy: 80 MeV

• Target:– Au foil, 15 micron thick

– 1st 0.5 micron implanted with 3He at FZD

• Analysis presently underway

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Particle ID Plot (Uncalibrated)

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E

DE

p

D

t

Elastic 3He

a

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Si-Detector (x,y) Hit Pattern (Raw and Uncalibrated)

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Y

X

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ACCELERATOR MASS

SPECTROMETRY

Looking into the Past

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magnetic rigidity

in a gas-filled magnet

Accelerator Mass Spectroscopy at TUM

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BIOGENIC RECORD OF A

SUPERNOVA?

The dead don’t talk, but perhaps they have left us a message

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150 My BP

• Miocene extinction event ~2-3 My ago

• Characterized by drop in molluscs and

gastropods in Florida, Western Atlantic

ocean, Antarctica

• Possible reasons:

– Glacation & Climate cooling

– Rising of Panama isthmus

– Cosmic event – partial marine food chain failure

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T ~ 2.8 Myr ago

C. Fitoussi et al, PRL 101 (2008)

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1 2

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Ocean Drill Core Samples

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Fe Concentration in Drill Core

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w = sample mass (~ 5 g)

ms = <sample magnetic moment>(~ 6 Am2)

mrs = saturation magnetization (92 Am2/kg)

Fe concentration:

Primary Fe minerals:

Dispersed magnetite:

Intact M-somes:

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Atom flux of iron from bacteria growth and sedimentation rate:

Atom flux of 60Fe: ; f60 = 3.8 x 108 atom/cm2 [Knie et al.,

PRL (2004) ]

Ratio of fluxes gives atom ratios:

Amount of drill core: 100 – 200 grams;

approx. 2 – 4 mg magnetite

Estimate of 60Fe in the Magnetofossils

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t ~ 500 kyr

• Particle Flux of isotope “i” at radius D without decay:

• Cross sectional area of Earth intercepting SN debris:

• This debris deposited on Earth uniformly, over an area of:

Earth: A SN Yield Detector

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D

Number of atoms “i” deposited in uniform layer on Earth’s surface (now include decay) after a time T since SN occurred:

Ratio of any two radio-nuclides:

Independent of unknown distance D!

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The Problem of AMS Detection Beyond Iron

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Iron-group abundance peak

4.5 – 5 order drop in

abundance from Fe-group

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Could These be the Result of Microbial Activity?

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External ferrihydrite (rust)

Distinct internal

Fe-rich minerals

Banded Iron

Formation

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Summary

• Astrophysics program at TUM underway

• Objective: Properties of nuclear states for nova

• Status of program– Q3D spectrograph for measuring/searching out excited states

– Doppler lifetime station commissioning underway

– Arrival of neutron detector in July to extend Doppler station to

transfer reaction channels with neutron ejectiles

• Try to utilize pulsed-beam feature of MLL Tandem

• Another PhD student required (know any candidates?)

• Supernova search in microfossils– Initial phases of project underway (another PhD project)

– Manuscript presently under peer review: Icarus

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EXTRA SLIDES

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Bacteria and Archean Nuclear Reactors

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• Connected to when bacterial life evolved to cope

with increasingly richer O2 atmosphere

– Ca. 3 Gyr before present

• Erosion carries UO2 to into shallow basins

• Photosynthesis of newly evolving bacteria

produces O2 in shallow water, bringing U6+

into purely dissolved form in water column

• Water motion/currents carry U6+ out of O2-

rich water

– Redox boundary changes U6+ U4+

– U4+ is precipitated out of solution at the oxic-

anoxic boundary

– Highly concentrated in small zone

• Possible source of natural nuclear reactor

– Look for depletions in 235U

35

Cl

S

Ar

36S is s-process: not nova

AGB Star: 36Cl(n,p)36S

34S in nova from 34Cl decay

Sulfur measurements should be target of grains

If Companion is AGB

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