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Merge branch 'master' of igit.ific.uv.es:fernando.p.csic.es/latticegpu.jl into fix/flow_obc
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commit
349ff2405f
17 changed files with 585 additions and 165 deletions
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@ -165,7 +165,7 @@ include("YMfields.jl")
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export randomize!, zero!, norm2
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include("YMact.jl")
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export krnl_plaq!, force_gauge, force_wilson
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export krnl_plaq!, force_gauge, force_gauge_flw, force_wilson
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include("YMhmc.jl")
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export gauge_action, hamiltonian, plaquette, HMC!, MD!
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@ -320,6 +320,22 @@ function krnl_force_impr_pln!(frc1, frc2, U::AbstractArray{T}, c0, c1, Ubnd, cG,
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return nothing
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end
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function bnd_rescale_flw!(frc1, lp::SpaceParm{N,M,BC_OPEN,D}) where {N,M,D}
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@inbounds begin
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b = Int64(CUDA.threadIdx().x)
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r = Int64(CUDA.blockIdx().x)
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I = point_coord((b,r), lp)
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it = I[N]
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for id in 1:N-1
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if (((it == 1) || (it == lp.iL[4])))
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frc1[b,id,r] = 2*frc1[b,id,r]
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end
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end
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end
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return nothing
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end
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##
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## SF
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@ -874,7 +890,6 @@ function krnl_force_impr_pln!(frc1, frc2, U::AbstractArray{T}, c0, c1, Ubnd, cG,
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end
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##
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## PERIODIC
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##
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@ -1143,6 +1158,38 @@ end
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force_gauge(ymws::YMworkspace, U, c0, gp, lp) = force_gauge(ymws, U, c0, gp.cG[1], gp, lp)
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force_gauge(ymws::YMworkspace, U, gp, lp) = force_gauge(ymws, U, gp.c0, gp.cG[1], gp, lp)
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"""
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function force_gauge_flw(ymws::YMworkspace, U, c0, cG, gp::GaugeParm, lp::SpaceParm{N,M,BC_OPEN,D})
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Computes the force for the gauge flow with Open Boundaries. An aditional factor two in the boundaries
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is included, see
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M. Luescher, S. Schaefer: "Lattice QCD with open boundary conditions and twisted-mass reweighting", Comput.Phys.Commun. 184 (2013) 519,
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for more details.
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"""
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function force_gauge_flw(ymws::YMworkspace, U, c0, cG, gp::GaugeParm, lp::SpaceParm{N,M,BC_OPEN,D}) where {NI,N,M,D}
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ztw = ztwist(gp, lp)
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if abs(c0-1) < 1.0E-10
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@timeit "Wilson gauge force" begin
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force_pln!(ymws.frc1, ymws.frc2, U, gp.Ubnd, cG, ztw, lp::SpaceParm)
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end
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else
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@timeit "Improved gauge force" begin
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force_pln!(ymws.frc1, ymws.frc2, U, gp.Ubnd, cG, ztw, lp::SpaceParm, c0)
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end
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end
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CUDA.@sync begin
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CUDA.@cuda threads=lp.bsz blocks=lp.rsz bnd_rescale_flw!(ymws.frc1,lp::SpaceParm)
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end
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return nothing
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end
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"""
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function force_wilson(ymws::YMworkspace, U, gp::GaugeParm, lp::SpaceParm)
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@ -93,7 +93,7 @@ function Base.show(io::IO, int::FlowIntr{N,T}) where {N,T}
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if N == 0
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println(io, " * Euler schem3")
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elseif N == 1
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println(io, " * One stage scheme. Coefficients3")
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println(io, " * One stage scheme. Coefficients")
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println(io, " stg 1: ", int.e0[1], " ", int.e1[1])
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elseif N == 2
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println(io, " * Two stage scheme. Coefficients:")
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@ -201,6 +201,31 @@ function flw(U, int::FlowIntr{NI,T}, ns::Int64, eps, gp::GaugeParm, lp::SpacePar
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end
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flw(U, int::FlowIntr{NI,T}, ns::Int64, gp::GaugeParm, lp::SpaceParm, ymws::YMworkspace) where {NI,T} = flw(U, int, ns, int.eps, gp, lp, ymws)
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function flw(U, int::FlowIntr{NI,T}, ns::Int64, eps, gp::GaugeParm, lp::SpaceParm{N,M,BC_OPEN,D}, ymws::YMworkspace) where {NI,T,N,M,D}
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@timeit "Integrating flow equations" begin
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for i in 1:ns
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force_gauge_flw(ymws, U, int.c0, 1, gp, lp)
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if int.add_zth
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add_zth_term(ymws::YMworkspace, U, lp)
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end
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ymws.mom .= ymws.frc1
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U .= expm.(U, ymws.mom, 2*eps*int.r)
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for k in 1:NI
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force_gauge_flw(ymws, U, int.c0, 1, gp, lp)
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if int.add_zth
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add_zth_term(ymws::YMworkspace, U, lp)
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end
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ymws.mom .= int.e0[k].*ymws.mom .+ int.e1[k].*ymws.frc1
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U .= expm.(U, ymws.mom, 2*eps)
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end
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end
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end
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return nothing
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end
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flw(U, int::FlowIntr{NI,T}, ns::Int64, gp::GaugeParm, lp::SpaceParm{N,M,BC_OPEN,D}, ymws::YMworkspace) where {NI,T,N,M,D} = flw(U, int, ns, int.eps, gp, lp, ymws)
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##
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# Adaptive step size integrators
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@ -320,30 +345,30 @@ Eoft_plaq(U, gp::GaugeParm{T,G,NN}, lp::SpaceParm{N,M,B,D}, ymws::YMworkspace) w
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function krnl_plaq_pln!(plx, U::AbstractArray{T}, Ubnd, ztw, ipl, lp::SpaceParm{N,M,B,D}) where {T,N,M,B,D}
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@inbounds begin
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b = Int64(CUDA.threadIdx().x)
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r = Int64(CUDA.blockIdx().x)
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I = point_coord((b,r), lp)
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id1, id2 = lp.plidx[ipl]
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SFBC = ((B == BC_SF_AFWB) || (B == BC_SF_ORBI)) && (id1 == N)
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TWP = ((I[id1]==1)&&(I[id2]==1))
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bu1, ru1 = up((b, r), id1, lp)
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bu2, ru2 = up((b, r), id2, lp)
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if SFBC && (ru1 != r)
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if SFBC && (point_time((b,r),lp) == lp.iL[end])
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gt = Ubnd[id2]
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else
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gt = U[bu1,id2,ru1]
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end
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if TWP
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plx[I] = ztw*tr(U[b,id1,r]*gt / (U[b,id2,r]*U[bu2,id1,ru2]))
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else
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plx[I] = tr(U[b,id1,r]*gt / (U[b,id2,r]*U[bu2,id1,ru2]))
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end
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end
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end
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return nothing
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end
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@ -92,7 +92,7 @@ end
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"""
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function setbndfield(U, phi, lp::SpaceParm)
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Sets abelian boundary fields with phases `phi[1]` and `phi[2]` to the configuration `U` at time salice ``x_0=0``.
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Sets abelian boundary fields with phases `phi[1]` and `phi[2]` to the configuration `U` at time slice ``x_0=0``.
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"""
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function setbndfield(U, phi, lp::SpaceParm{N,M,B,D}) where {N,M,B,D}
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