diff --git a/mesons.jl b/mesons.jl
index b49c457..7c7fba9 100644
--- a/mesons.jl
+++ b/mesons.jl
@@ -47,7 +47,7 @@ end
     r is the radius in fm,
     An initial guess initial_sol=(Φ0, W0, B0, A0) can be provided to speed up convergence (permuting!).
 Reference: P. Giuliani, K. Godbey, E. Bonilla, F. Viens, and J. Piekarewicz, Frontiers in Physics 10, (2023)"
-function solveMesonWfs(ρ_sp, ρ_vp, ρ_sn, ρ_vn, r_max, divs, iterations=3; initial_sol=(zeros(1 + divs) for _ in 1:4))
+function solveMesonWfs(ρ_sp, ρ_vp, ρ_sn, ρ_vn, r_max, divs, iterations=10; initial_sol=(zeros(1 + divs) for _ in 1:4))
     (Φ0, W0, B0, A0) = initial_sol
     (src_Φ0, src_W0, src_B0, src_A0) = (zeros(1 + divs) for _ in 1:4)
 
@@ -60,8 +60,8 @@ function solveMesonWfs(ρ_sp, ρ_vp, ρ_sn, ρ_vn, r_max, divs, iterations=3; in
         @. src_W0 = g2_v * ((ζ/6) * (W0/ħc)^3 + 2Λv * (2B0/ħc)^2 * (W0/ħc)) - g2_v * (ρ_vp + ρ_vn)
         @. src_B0 = (2Λv * g2_ρ * (W0/ħc)^2 * (2B0/ħc) - g2_ρ/2 * (ρ_vp - ρ_vn)) / 2
         Φ0 .= solveKG(m_s, src_Φ0, r_max)
-        W0 .= solveKG(m_ω, src_W0, r_max)
-        B0 .= solveKG(m_ρ, src_B0, r_max)
+        W0 .= (solveKG(m_ω, src_W0, r_max) .+ W0) ./ 2 # to supress oscillation
+        B0 .= (solveKG(m_ρ, src_B0, r_max) .+ B0) ./ 2 # to supress oscillation
     end
 
     return (Φ0, W0, B0, A0)
diff --git a/test/Pb208_meson_flds.jl b/test/Pb208_meson_flds.jl
index f8b11ac..e360d5f 100644
--- a/test/Pb208_meson_flds.jl
+++ b/test/Pb208_meson_flds.jl
@@ -24,7 +24,7 @@ xs = test_data[:, 1]
 r_max = maximum(xs)
 divs = length(xs) - 1
 
-(Φ0, W0, B0, A0) = solveMesonWfs(ρ_sp, ρ_vp, ρ_sn, ρ_vn, r_max, divs, 1; initial_sol=(Φ0_bench, W0_bench, B0_bench, A0_bench))
+(Φ0, W0, B0, A0) = solveMesonWfs(ρ_sp, ρ_vp, ρ_sn, ρ_vn, r_max, divs, 200) # many iterations needed without an initial solution
 
 plot!(xs, hcat(Φ0, W0, B0, A0), layout=4, label=["Φ0" "W0" "B0" "A0"])
 xlabel!("r (fm)")
\ No newline at end of file