cdhnew | R Documentation |
finite size corrections a la Colangelo, Duerr, Haefeli, but re-expanded as series in the quark mass
cdhnew(parm = rep(0, times = 6), rev = -1, aLamb1 = 0.055, aLamb2 = 0.58, aLamb3, aLamb4, ampiV, afpiV, aF0, a2B0mu, L, printit = FALSE, use.cimpl = TRUE)
parm |
m parameters |
rev |
rev=-1 corrects from L to L = infinity, rev=+1 the other way around |
aLamb1 |
The four low energy Lambda1-Lambda4constants in lattice units. |
aLamb2 |
see |
aLamb3 |
see |
aLamb4 |
see |
ampiV |
pseudo scalar mass values to be corrected |
afpiV |
pseudo scalar decay constant values to be corrected |
aF0 |
af0 in lattice units |
a2B0mu |
2 B0 mu in lattice units, where mu is the quark mass and B0 a low energy constant |
L |
the lattice spatial extent |
printit |
if set to TRUE the corrections are printed |
use.cimpl |
use the four times faster direct c Implementation of the correction routine |
see reference for details. We use the simplyfied formulae for the S quantities, see eq. (59) in first reference.
a list with the corrected values for mpi and fpi
Carsten Urbach curbach@gmx.de
Gilberto Colangelo, Stephan Durr, Christoph Haefeli, Nucl.Phys.B721:136-174,2005. hep-lat/0503014
and
R. Frezzotti, V. Lubicz, S. Simula, arXiv:0812.4042 hep-lat
mu <- c(0.004, 0.006, 0.008, 0.010, 0.004) L <- c(24, 24, 24, 24, 32) mps <- c(0.14448, 0.17261, 0.19858, 0.22276, 0.14320) fps <- c(0.06577, 0.07169, 0.07623, 0.07924, 0.06730) aLamb1 <- 0.05 aLamb2 <- 0.5 aLamb3 <- 0.38 aLamb4 <- 0.66 aF0 <- 0.051 a2B <- 5.64 cdhres <- cdhnew(rev=+1, aLamb1=aLamb1, aLamb2=aLamb2, aLamb3=aLamb3, aLamb4=aLamb4, ampiV=mps, afpiV=fps, aF0=aF0, a2B0mu=a2B*mu, L=L, printit=TRUE) cdhres$mpiFV cdhres$fpiFV
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