Antiprotons for Nuclear Structure Investigations

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Antiprotons for Nuclear Structure Investigations H. Lenske Institut für Theoretische Physik, U. Giessen

description

Antiprotons for Nuclear Structure Investigations. H. Lenske Institut für Theoretische Physik, U. Giessen. Measuring Neutron Skins on Isotopic Chains (Ni,Sn…): p + A Absorption@FAIR: the AIC Proposal. - PowerPoint PPT Presentation

Transcript of Antiprotons for Nuclear Structure Investigations

Page 1: Antiprotons for Nuclear Structure Investigations

Antiprotons for Nuclear Structure Investigations

H. Lenske Institut für Theoretische Physik, U. Giessen

Page 2: Antiprotons for Nuclear Structure Investigations

Measuring Neutron Skins on Isotopic Chains (Ni,Sn…):

p + A Absorption@FAIR: the AIC Proposal

P. Kienle, NMB 214 (2004) and AIC@FAIR

Proposal

H.L., P. Kienle, Phys.Lett. B647 (2007) 82-87

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Antiprotons for Nuclear Structure Investigations @FAIR

Agenda:

Antiproton-N and Antiproton-Nucleus Antiproton-N and Antiproton-Nucleus InteractionsInteractions

Nuclear Radii from Absorption Cross SectionsNuclear Radii from Absorption Cross Sections Antiprotons and Neutron-SkinsAntiprotons and Neutron-Skins Screening Effects in Neutron-rich NucleiScreening Effects in Neutron-rich Nuclei Isospin Tagging by Pion ProductionIsospin Tagging by Pion Production Strangeness ProductionStrangeness Production OutlookOutlook

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The antiproton-proton Interaction: LEAR Data

p p

p p

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Antiproton-Nucleon Interactions

KK

p p

...

- 0

0

K K

n p

...

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The History of the longterm relation…

…of antiprotons and nuclei:

• anti-protonic atoms and tails of nuclear densities

• antiproton-A elastic scattering

• annihilation and pion production

• G-parity transformation of scalar and vector self-energies deep potentials ~ -500 MeV

• dispersive self-energies from annihilation channels

• Annihilation and Quark Models

• Meson & Hadron Dynamics from pphh

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Consequences of G-Parity in Nuclear Binding

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Energy Deposition in a Nucleus

(Cascade-Calculations, Clover et al., PRC 26)

p p (at rest)

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The antiproton-Nucleus Interaction

Antiproton+A scattering:

• Free Space pN T-Matrix

• Nuclear Structure: state-of-the-art HFB p and n Densities

• optical Potential in Impulse (t) Approximation

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Antiproton+Nucleus Interactions:Elastic Scattering

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pA Scattering: Optical Potential and Absorption Cross

Section From The Continuity

Equation:

3 ( )† ( )abs s s opt s2

2m 1tr d r r, k (U ) r, k

2s 1k

s2 (z,b)2abs s opt2

2m 1tr d bdz (U (r))e

2s 1k

Eikonal Approximation:

Page 12: Antiprotons for Nuclear Structure Investigations

Antiproton Absorption on 58,78Ni: The Monopole Annihilation Kernel and the

Nuclear Density

( ) 2s

1 1ˆ(r, k) dr | (r, k) |

2s 1 4

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Antiproton+A Absorption: Limiting Cases

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Probing Nuclear Radii by Antiprotons

• scaling of abs ~ <r2>

• energy independent slope

• convergence of magnitude

• from proton to neutron skin

• increasing <r2>

• neutron skins up to 0.6 fm

• charge radii by e- scattering

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Measuring Neutron Skins on Isotopic Chains (Ni,Sn…):

p + A Absorption on protons and neutrons

H.L., P. Kienle, Phys.Lett. B647 (2007) 82-87

Page 16: Antiprotons for Nuclear Structure Investigations

Localization of the Annihilation Process

2

dP(b) (b)

bdb

bk ( 1)

Page 17: Antiprotons for Nuclear Structure Investigations

Spatial Localization of Antiproton

Annihilation on a Nucleus:

Peripheral Process

Cascade Results by Clover et al., PRC 26

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Absorption on Protons

b=4fm

Absorption on Neutrons

b=4fm

Shielding of Target Protons by the Neutron Skin

protons

neutrons

Tlab=700 MeV

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Antiproton Annihilation on Ni-Isotopes: Scaling of abs

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Antiproton+N Absorption: Isospin Symmetry

ppnp

ppnp

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Antiproton+Nucleus Interactions: Isospin Symmetry

...)()()(

)()()(~)(

2

20

rrkt

rrktrU

pnF

pnFAp

Enhanced along isotopic chains!

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p A(N,Z) C(N 1,Z) k

0p A(N,Z) B(N,Z 1) k n

Peripheral Antiproton Annihilation on a Nucleus:

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Pion Production:

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Differential Coherent Antiproton Annihilation on a Nucleus:

k kk

0

...

KK ...Np a hh

YY ...

... (N=n)

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( )*3 3 ( )pN n nM (k ,k ) d r d r (k , r ) t (x) (r ) (k , r )

i(k r k r ) 2 (r , r )3 3pN n nM (k ,k ) ~ d r d r e t (x) (r )e

Differential Antiproton Annihilation on a Nucleus:

Eikonal Approximation:

Quantum Mechanical Amplitude:

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LEAR-Data (PS185) on Strangeness Production

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DDRH Flavour Dynamics: Single Particle Energies

DDRH Theory: Density Dependent NN and N Dirac-Brueckner Vertices

Nuclear Matter S

= 28 MeV

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Phase Space Distribution for pbar+A -> anti-Y+B(Y)+pi^- Target: 40Ca

Lambda 300 200 100

Sigma^0 300 200 100

0100200300400500600700800k(anti-Y) [MeV/c] 100200300400500600700800

q(pi^-) [MeV/c]

050

100150200250300350

d^2P(k,q)/dE(k)dE(q)

Phase Space Distribution for pbar+A -> anti-Y+B(Y)+pi^- Target: 56Ca

Lambda 200 150 100 50

Sigma^0 200 150 100 50

0100200300400500600700800k(anti-Y) [MeV/c] 100200300400500600700800

q(pi^-) [MeV/c]

050

100150200250

d^2P(k,q)/dE(k)dE(q)

and Strangeness Production on Stable

and Exotic Nuclei

40Ca

56Ca

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• Antiprotons as a Probe for Nuclear Structure

• Antipoton-neutron Interactions in Neutron-rich Nuclei

• Antiproton Absorption in Neutron Skin Matter:

• Exclusive Processes: Studies of A A-1 Reactions

• Multi-Pion and YY Production

• Antiproton In-Medium Interactions:

• Test of G-parity for antiproton-N interactions,

• Study of dispersive self-energies

Summary and Outlook

Antiproton Ion Collider (AIC) Collaboration @ FAIR

Page 30: Antiprotons for Nuclear Structure Investigations

Measuring Neutron Skins on Isotopic Chains (Ni,Sn…):

p + A Absorption@FAIR: the AIC Proposal

P. Kienle, NMB 214 (2004) and AIC@FAIR

Proposal

H.L., P. Kienle, Phys.Lett. B647 (2007) 82-87