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Lattice QCD and Nuclear Physics

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Lattice QCD and Nuclear Physics. Martin Savage. University of Washington ... V(R) between Hadrons with one Q : DD (Michael, Cook Fiebig,...) Yp Yp , YN YN , YY YY ... – PowerPoint PPT presentation

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Title: Lattice QCD and Nuclear Physics


1
Lattice QCD and Nuclear Physics
Martin Savage University of Washington
Lattice 2005, Dublin, July 2005
2
Emergence of Nuclear Physics from QCD
  • Consistent and rigorous pathway from QCD
  • Lattice QCD EFT
    Many-Body

Mq - explicit
3
Calculations where experiments are not possible
  • Supernova Remnant ?
  • neutron stars
  • b b - decay

or
black holes , .. kaon condensation ? ..
S , K
S , K
n
n
4
How does nature depend upon the fundamental
constants?
  • Quark mass dependence of element production
  • Dependence upon a

5
Understand the fine-tunings of nature
  • Deuteron Binding energy is 2.2 MeV
  • a(1s0) -24 fm
  • Infrared fixed-point of QCD
  • 3 a 12C

6
NN-Scattering (s-wave)
1S0
3S1
Quenched Data (Fukugita et al, 1995) , Latt 204
A Lattice Measurement at this mp would fix
counterterms D2
  • Mqdependence of nuclear properties Little is
    known..this is all !!!

7
Nuclear Physics with lattice QCD
  • University of New Hampshire
  • Lawrence Berkeley Laboratory
  • College of William and Mary
  • University of Groningen
  • University of Barcelona
  • University of Washington

8
Maiani-Testa End of the Innocence
d (s) ?
Away from Kinematic Thresholds at infinite volume
One Hoped that
GNN (s)Euclidean GNN
(s)Minkowski
9
Two-Particle Energy Levels (Luscher)
Below Inelastic Thresholds
UV regulator
10
NN on the Lattice
E L2
E L2
1st continuum
2nd continuum
Deuteron
1st continuum
Dont Need Huge Lattices !!!!
  • Calc. in Pionless EFT 5 fm lattices or larger
    for Mp 140 MeV
  • Need Pionful theory calc. for smaller lattices
  • Mp 350 MeV 2.5 fm lattices....
    MILC lattices

11
np dg
(William Detmold and MJS)
N
N
k1
N
N
l1
MECs
Asymmetric Lattice
N
N
g
g
12
ElectroWeak Matrix Elements
L X L/10 X L/10 X T lattice
13
Hyperon Weak Interactions
S-wave
P-wave
Lattice
surface term
( Orginos )
14
LQ LQ Potential
15
NPLQCD Current Resources SciDAC
  • JLab Clusters 8 resources 40 Gflop-yrs
  • Chroma / QDP
  • MILC staggered Lattices
  • DWF Propagators of LHPC
  • Approved Exploratory
  • NN , LL, LN , SS , SN
  • MN - s-term , strong-isospin-breaking (PQ)

16
I2 pp-scattering
  • LHPCs DWF valence propagators on 203 X 64 MILC
    staggered sea
  • Mp 480 , 350 and 290 MeV

17
Chiral-Extrapolation


  • Mp a2 -0.0426 0.0006 0.0003 0.0018

-
-
-
( c-PT for pp by Bijnens, Colangelo, Gasser,
Leutwyler, )
18
L L - Prelim.
  • Coupled Channels ?
  • a

19
Conclusion
  • Lattice QCD studies of Nuclei and Multi-Hadron
    Systems are an important part of the future of
    Nuclear Physics.

20
Topics that are or can or should be tackled today
  • Nucleon Properties (LHPC)
  • MN , mN , gA , qm..n , as functions of mq , a , V
  • The NN Systems
  • d(s) , LA1, ..
  • Hyperon Properties and Systems
  • ML , L Np , L N L N , L L
    L L ..
  • V(R) between Hadrons with one Q DD
    (Michael, CookFiebig,)
  • Yp Yp , YN YN , YY
    YY
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