Schwinger model figures
-
b5_Nf2_ResMpi_WilsonFermions.pdf → Residual pion mass as a function of
$L$ for the two flavors case. Results obtained with Wilson fermions.Parameters:
$\beta$ = 5,$L_t$ = 64,$N_f$ = 2, Fermions = Wilson, Nmeas = 10 000, sigma = 3. -
b5_Mpi_vs_m2g_WilsonFermions_AllL.pdf → Pion mass as a function of
$(m²g)^{1/3}$ for several values of$L$ . Two flavors case.Parameters:
$\beta$ = 5,$L_t$ = 64,$L$ = 6, 7, 8, 9, 10, 11, 12,$N_f$ = 2, Fermions = Wilson, NMeas = 10 000, sigma = 3. -
b5_24x24_GMOR.pdf →
$F_\pi$ obtained through the Gell-Mann--Oakes--Renner relation.Parameters:
$\beta$ = 5,$L_t$ = 24,$L$ = 24,$N_f$ = 2, 3, 4, 5, 6, Fermions = Overlap, Nmeas = 30 000. -
b4_Nf2_ResMpi_overlap.pdf → Residual pion mass as a function of
$L$ for the two flavors case.Parameters:
$\beta$ = 4,$L_t$ = 32,$L$ = 4, 5, 6, 7, 8, 10, 12,$N_f$ = 2, Fermions = Overlap, Nmeas = 10 000. We fit the full range of points. -
b4_Mpi_vs_m2g_Overlap_AllL.pdf → Pion mass as a function of
$(m²g)^{1/3}$ for several values of$L$ . Two flavors case.Parameters:
$\beta$ = 4,$L_t$ = 32,$L$ = 4, 6, 8, 10, 12,$N_f$ = 2, Fermions = Overlap, Nmeas = 10 000. -
b4_AllNf_ResMpi_overlap.pdf → Residual pion mass as a function of
$L$ for several flavors. Results obtained with overlap fermions.For
$N_f>2$ the fit is up to$L$ = 7, for$N_f=2$ we fit the full range.$F_\pi$ is computed with the "magic formula".Parameters:
$\beta$ = 4,$L_t$ = 32,$L$ = 4, 5, 6, 7, 8, 10, 12,$N_f$ = 2, 3, 4, 5, 6, Fermions = Overlap, Nmeas = 10 000. -
b5_24x24_MpiBreakingPoint.pdf → Breaking point of the pion mass with
$\sigma$ = 1 and$\sigma$ = 2 on a square lattice.Parameters:
$\beta$ = 5,$L_t$ = 24,$L$ = 24,$N_f$ = 2 Fermions = Overlap, Nmeas = 30 000.- b5_24x24_Nf2_ChiralCondensate.pdf → Chiral condensate obtained with lattice simulations compared with Hosotani's prediction.
Parameters:
$\beta$ = 5,$L_t$ = 24,$L$ = 24,$N_f$ = 2 Fermions = Overlap, Nmeas = 30 000.