Typos varios

src/Solvers/Propagators.jl

@@ -155,16 +155,16 @@ Returns the boundary to boundary propagator of the Schrodinger functional given
 """
 function bndtobnd(bndpro::AbstractArray, U::AbstractArray, dpar::DiracParam, dws::DiracWorkspace, lp::SpaceParm{4,6,1,D}) where {D}
 
-    function krnl_bndtobnd!(psi::AbstractArray, bndp::AbstractArray, U::AbstractArray, lp)
+    function krnl_bndtobnd!(psi::AbstractArray, bndp::AbstractArray, U::AbstractArray, lp::SpaceParm)
         b=Int64(CUDA.threadIdx().x)
         r=Int64(CUDA.blockIdx().x)
 
         it = point_time((b, r), lp)
 
-        if it == lp.il[end]
+        if it == lp.iL[end]
             psi[b,r] = gdagpmul(Pgamma{4,1},U[b,4,r],bndpro[b,r])
         else
-            psi[b,r] = 0.0 * bndpro[b,r]
+            psi[b,r] = 0.0*bndpro[b,r]
         end
 
         return nothing
@@ -174,7 +174,7 @@ function bndtobnd(bndpro::AbstractArray, U::AbstractArray, dpar::DiracParam, dws
         CUDA.@cuda threads=lp.bsz blocks=lp.rsz krnl_bndtobnd!(dws.sp, bndpro ,U, lp)
     end
 
-    res = -dpar.ct*CUDA.mapreduce(x -> x, +, dws.sp)./(lp.iL[1]*lp.iL[2]*lp.iL[3])
+    res = -dpar.ct*CUDA.mapreduce(x -> x, +, dws.sp) / (lp.iL[1]*lp.iL[2]*lp.iL[3])
 
     return res
 end