$Re(A_0)$, $Re(A_2)$ and RG evolution for $N_f=3$

Details $Re(A_0)$, $Re(A_2)$ and RG evolution for $N_f=3$ $Re(A_0)$, $Re(A_2)$ and RG evolution for $N_f=3$

2004-09-06

arxiv.org/abs/hep-lat/0409020v2

Nucl.Phys.Proc.Suppl.140:384-386,2005

Physics

High Energy Physics

High Energy Physics - Lattice

3 pages, 4 figures, contribution to Lattice 2004 International Symposium

Scientific paper

10.1016/j.nuclphysbps.2004.11.18

We present results of $Re (A_0)$ and $Re (A_2)$ calculated using HYP staggered fermions on the lattice of $16^3 \times 64$ at $\beta=6.0$. These results are obtained using leading order chiral perturbation in quenched QCD. Buras's original RG evolution matrix develops a removable singularity for $N_f=3$. This subtlety is resolved by finding a finite solution to RG equation and the results are presented.

Affiliated with

Also associated with

No associations

Rating

$Re(A_0)$, $Re(A_2)$ and RG evolution for $N_f=3$ does not yet have a rating. At this time, there are no reviews or comments for this scientific paper.

If you have personal experience with $Re(A_0)$, $Re(A_2)$ and RG evolution for $N_f=3$, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and $Re(A_0)$, $Re(A_2)$ and RG evolution for $N_f=3$ will most certainly appreciate the feedback.

Rate now

Comments { 0 }

Profile ID: LFWR-SCP-O-374922