Post on 03-Feb-2016
description
On the Perturbative Nuclear Physics
Jiunn-Wei Chen (陳俊瑋 )
National Taiwan U.
• Introduction to the nuclear effective field theory by Beane, Kaplan, Vuorinen (BKV, ‘08).
• Chiral extrapolations of two nucleon observables using the BKV approach
NP P
Beane, Kaplan, Vuorinen (BKV) ’08:Using a Pauli-Villars (PV) field to cancel the short distance part of the potential
BKV = KSW in
BKV = KSW+PV in
BKV = KSW+PV in
BKV = KSW+PV in
NN NPLQCD ‘06
NN NPLQCD’06
50 100 150 200 250 300 350
60 40 20
204060
Quark mass dependence ofScattering length in BKV
A hint for multiverse?
50 100 150 200 250 300 350
60 40 20
204060
Scattering length
100 150 200 250 300 350
2
4
6
8
10
Effective Range
Quark Mass Dependence in BKV (JWC work in progress)
Only need NN scattering length at different quark masses from LQCD to study the quark mass dependence of all the observables in NN systems
in JWC, Savage(99),Rupak(00)
10 20 30 40
2
4
6
8
10
12
for different pion masses
120 MeV
140 MeV150 MeV
Outlooks
• Is BKV correct?
• Only need NN scattering length at different quark masses from LQCD to study the quark mass dependence of all the observables in NN systems. (Always true, even BKV is not correct.) Lower quark mass computations are important.
50 100 150 200
10
5
5
10
15
20
25