Fix incorrect times in time evolution solutions

src/time_evolution/lr_mesolve.jl

@@ -147,19 +147,19 @@
     return u_modified!(integrator, false)
 end
 
-_save_control_lr_mesolve(u, t, integrator) = t in integrator.p.t_l
+_save_control_lr_mesolve(u, t, integrator) = t in integrator.p.times
 
 function _save_affect_lr_mesolve!(integrator)
     ip = integrator.p
     N, M = ip.N, ip.M
-    idx = select(integrator.t, ip.t_l)
+    idx = select(integrator.t, ip.times)
 
     @views z = reshape(integrator.u[1:N*M], N, M)
     @views B = reshape(integrator.u[N*M+1:end], M, M)
     _calculate_expectation!(ip, z, B, idx)
 
     if integrator.p.opt.progress
-        print("\rProgress: $(round(Int, 100*idx/length(ip.t_l)))%")
+        print("\rProgress: $(round(Int, 100*idx/length(ip.times)))%")
         flush(stdout)
     end
     return u_modified!(integrator, false)
@@ -365,7 +365,7 @@
 #=======================================================#
 
 @doc raw"""
-    lr_mesolveProblem(H, z, B, t_l, c_ops; e_ops=(), f_ops=(), opt=LRMesolveOptions(), kwargs...) where T
+    lr_mesolveProblem(H, z, B, tlist, c_ops; e_ops=(), f_ops=(), opt=LRMesolveOptions(), kwargs...) where T
     Formulates the ODEproblem for the low-rank time evolution of the system. The function is called by lr_mesolve.
 
     Parameters
@@ -376,7 +376,7 @@
         The initial z matrix.
     B : AbstractMatrix{T}
         The initial B matrix.
-    t_l : AbstractVector{T}
+    tlist : AbstractVector{T}
         The time steps at which the expectation values and function values are calculated.
     c_ops : AbstractVector{QuantumObject}
         The jump operators of the system.
@@ -393,7 +393,7 @@
     H::QuantumObject{<:AbstractArray{T1},OperatorQuantumObject},
     z::AbstractArray{T2,2},
     B::AbstractArray{T2,2},
-    t_l::AbstractVector,
+    tlist::AbstractVector,
     c_ops::AbstractVector = [];
     e_ops::Tuple = (),
     f_ops::Tuple = (),
@@ -407,6 +407,8 @@
     c_ops = get_data.(c_ops)
     e_ops = get_data.(e_ops)
 
+    t_l = convert(Vector{_FType(H)}, tlist)
+
     # Initialization of Arrays
     expvals = Array{ComplexF64}(undef, length(e_ops), length(t_l))
     funvals = Array{ComplexF64}(undef, length(f_ops), length(t_l))
@@ -421,7 +423,7 @@
         e_ops = e_ops,
         f_ops = f_ops,
         opt = opt,
-        t_l = t_l,
+        times = t_l,
         expvals = expvals,
         funvals = funvals,
         Ml = Ml,
@@ -489,14 +491,14 @@
     H::QuantumObject{<:AbstractArray{T1},OperatorQuantumObject},
     z::AbstractArray{T2,2},
     B::AbstractArray{T2,2},
-    t_l::AbstractVector,
+    tlist::AbstractVector,
     c_ops::AbstractVector = [];
     e_ops::Tuple = (),
     f_ops::Tuple = (),
     opt::LRMesolveOptions{AlgType} = LRMesolveOptions(),
     kwargs...,
 ) where {T1,T2,AlgType<:OrdinaryDiffEqAlgorithm}
-    prob = lr_mesolveProblem(H, z, B, t_l, c_ops; e_ops = e_ops, f_ops = f_ops, opt = opt, kwargs...)
+    prob = lr_mesolveProblem(H, z, B, tlist, c_ops; e_ops = e_ops, f_ops = f_ops, opt = opt, kwargs...)
     return lr_mesolve(prob; kwargs...)
 end
 
@@ -520,7 +522,7 @@
         Additional keyword arguments for the ODEProblem.
 """
 function lr_mesolve(prob::ODEProblem; kwargs...)
-    sol = solve(prob, prob.p.opt.alg, tstops = prob.p.t_l)
+    sol = solve(prob, prob.p.opt.alg, tstops = prob.p.times)
     prob.p.opt.progress && print("\n")
 
     N = prob.p.N
@@ -535,5 +537,5 @@
         zt = get_z(sol.u, N, Ml)
     end
 
-    return LRTimeEvolutionSol(sol.t, zt, Bt, prob.p.expvals, prob.p.funvals, prob.p.Ml)
+    return LRTimeEvolutionSol(sol.prob.p.times, zt, Bt, prob.p.expvals, prob.p.funvals, prob.p.Ml)
 end

src/time_evolution/mcsolve.jl

@@ -86,13 +86,12 @@ function _mcsolve_output_func(sol, i)
     return (sol, false)
 end
 
-function _mcsolve_generate_statistics(sol, i, times, states, expvals_all, jump_times, jump_which)
+function _mcsolve_generate_statistics(sol, i, states, expvals_all, jump_times, jump_which)
     sol_i = sol[:, i]
     !isempty(sol_i.prob.kwargs[:saveat]) ?
     states[i] = [QuantumObject(normalize!(sol_i.u[i]), dims = sol_i.prob.p.Hdims) for i in 1:length(sol_i.u)] : nothing
 
     copyto!(view(expvals_all, i, :, :), sol_i.prob.p.expvals)
-    times[i] = sol_i.t
     jump_times[i] = sol_i.prob.p.jump_times
     return jump_which[i] = sol_i.prob.p.jump_which
 end
@@ -522,22 +521,18 @@ function mcsolve(
     _sol_1 = sol[:, 1]
 
     expvals_all = Array{ComplexF64}(undef, length(sol), size(_sol_1.prob.p.expvals)...)
-    times = Vector{Vector{Float64}}(undef, length(sol))
     states =
         isempty(_sol_1.prob.kwargs[:saveat]) ? fill(QuantumObject[], length(sol)) :
         Vector{Vector{QuantumObject}}(undef, length(sol))
     jump_times = Vector{Vector{Float64}}(undef, length(sol))
     jump_which = Vector{Vector{Int16}}(undef, length(sol))
 
-    foreach(
-        i -> _mcsolve_generate_statistics(sol, i, times, states, expvals_all, jump_times, jump_which),
-        eachindex(sol),
-    )
+    foreach(i -> _mcsolve_generate_statistics(sol, i, states, expvals_all, jump_times, jump_which), eachindex(sol))
     expvals = dropdims(sum(expvals_all, dims = 1), dims = 1) ./ length(sol)
 
     return TimeEvolutionMCSol(
         ntraj,
-        times,
+        _sol_1.prob.p.times,
         states,
         expvals,
         expvals_all,

src/time_evolution/mesolve.jl

@@ -150,6 +150,7 @@ function mesolveProblem(
         e_ops = e_ops2,
         expvals = expvals,
         H_t = H_t,
+        times = t_l,
         is_empty_e_ops = is_empty_e_ops,
         params...,
     )
@@ -253,7 +254,7 @@ function mesolve(prob::ODEProblem, alg::OrdinaryDiffEqAlgorithm = Tsit5())
     ρt = map(ϕ -> QuantumObject(vec2mat(ϕ), type = Operator, dims = sol.prob.p.Hdims), sol.u)
 
     return TimeEvolutionSol(
-        sol.t,
+        sol.prob.p.times,
         ρt,
         sol.prob.p.expvals,
         sol.retcode,

src/time_evolution/sesolve.jl

@@ -127,6 +127,7 @@ function sesolveProblem(
         progr = progr,
         Hdims = H.dims,
         H_t = H_t,
+        times = t_l,
         is_empty_e_ops = is_empty_e_ops,
         params...,
     )
@@ -215,7 +216,7 @@ function sesolve(prob::ODEProblem, alg::OrdinaryDiffEqAlgorithm = Tsit5())
     ψt = map(ϕ -> QuantumObject(ϕ, type = Ket, dims = sol.prob.p.Hdims), sol.u)
 
     return TimeEvolutionSol(
-        sol.t,
+        sol.prob.p.times,
         ψt,
         sol.prob.p.expvals,
         sol.retcode,

src/time_evolution/ssesolve.jl

@@ -180,6 +180,7 @@ function ssesolveProblem(
         progr = progr,
         Hdims = H.dims,
         H_t = H_t,
+        times = t_l,
         is_empty_e_ops = is_empty_e_ops,
         params...,
     )
@@ -404,7 +405,7 @@ function ssesolve(
 
     return TimeEvolutionSSESol(
         ntraj,
-        _sol_1.t,
+        _sol_1.prob.p.times,
         states,
         expvals,
         expvals_all,

src/time_evolution/time_evolution.jl

@@ -51,7 +51,7 @@ A structure storing the results and some information from solving quantum trajec
 # Fields (Attributes)
 
 - `ntraj::Int`: Number of trajectories
-- `times::AbstractVector`: The time list of the evolution in each trajectory.
+- `times::AbstractVector`: The time list of the evolution.
 - `states::Vector{Vector{QuantumObject}}`: The list of result states in each trajectory.
 - `expect::Matrix`: The expectation values (averaging all trajectories) corresponding to each time point in `times`.
 - `expect_all::Array`: The expectation values corresponding to each trajectory and each time point in `times`
@@ -63,7 +63,7 @@ A structure storing the results and some information from solving quantum trajec
 - `reltol::Real`: The relative tolerance which is used during the solving process.
 """
 struct TimeEvolutionMCSol{
-    TT<:Vector{<:Vector{<:Real}},
+    TT<:Vector{<:Real},
     TS<:AbstractVector,
     TE<:Matrix{ComplexF64},
     TEA<:Array{ComplexF64,3},
@@ -97,19 +97,22 @@ function Base.show(io::IO, sol::TimeEvolutionMCSol)
 end
 
 @doc raw"""
-     struct TimeEvolutionSSESol
- A structure storing the results and some information from solving trajectories of the Stochastic Shrodinger equation time evolution.
- # Fields (Attributes)
- - `ntraj::Int`: Number of trajectories
- - `times::AbstractVector`: The time list of the evolution in each trajectory.
- - `states::Vector{Vector{QuantumObject}}`: The list of result states in each trajectory.
- - `expect::Matrix`: The expectation values (averaging all trajectories) corresponding to each time point in `times`.
- - `expect_all::Array`: The expectation values corresponding to each trajectory and each time point in `times`
- - `converged::Bool`: Whether the solution is converged or not.
- - `alg`: The algorithm which is used during the solving process.
- - `abstol::Real`: The absolute tolerance which is used during the solving process.
- - `reltol::Real`: The relative tolerance which is used during the solving process.
- """
+    struct TimeEvolutionSSESol
+
+A structure storing the results and some information from solving trajectories of the Stochastic Shrodinger equation time evolution.
+
+# Fields (Attributes)
+
+- `ntraj::Int`: Number of trajectories
+- `times::AbstractVector`: The time list of the evolution.
+- `states::Vector{Vector{QuantumObject}}`: The list of result states in each trajectory.
+- `expect::Matrix`: The expectation values (averaging all trajectories) corresponding to each time point in `times`.
+- `expect_all::Array`: The expectation values corresponding to each trajectory and each time point in `times`
+- `converged::Bool`: Whether the solution is converged or not.
+- `alg`: The algorithm which is used during the solving process.
+- `abstol::Real`: The absolute tolerance which is used during the solving process.
+- `reltol::Real`: The relative tolerance which is used during the solving process.
+"""
 struct TimeEvolutionSSESol{
     TT<:Vector{<:Real},
     TS<:AbstractVector,

src/time_evolution/time_evolution_dynamical.jl

@@ -248,7 +248,7 @@ function dfd_mesolve(
     )
 
     return TimeEvolutionSol(
-        sol.t,
+        sol.prob.p.times,
         ρt,
         sol.prob.p.expvals,
         sol.retcode,

test/core-test/time_evolution.jl

@@ -16,10 +16,13 @@
         sol3 = sesolve(H, psi0, t_l, e_ops = e_ops, saveat = t_l, progress_bar = Val(false))
         sol_string = sprint((t, s) -> show(t, "text/plain", s), sol)
         @test sum(abs.(sol.expect[1, :] .- sin.(η * t_l) .^ 2)) / length(t_l) < 0.1
+        @test length(sol.times) == length(t_l)
         @test length(sol.states) == 1
         @test size(sol.expect) == (length(e_ops), length(t_l))
+        @test length(sol2.times) == length(t_l)
         @test length(sol2.states) == length(t_l)
         @test size(sol2.expect) == (0, length(t_l))
+        @test length(sol3.times) == length(t_l)
         @test length(sol3.states) == length(t_l)
         @test size(sol3.expect) == (length(e_ops), length(t_l))
         @test sol_string ==
@@ -68,12 +71,21 @@
         @test sum(abs.(sol_mc.expect .- sol_me.expect)) / length(t_l) < 0.1
         @test sum(abs.(vec(expect_mc_states_mean) .- vec(sol_me.expect))) / length(t_l) < 0.1
         @test sum(abs.(sol_sse.expect .- sol_me.expect)) / length(t_l) < 0.1
+        @test length(sol_me.times) == length(t_l)
         @test length(sol_me.states) == 1
         @test size(sol_me.expect) == (length(e_ops), length(t_l))
+        @test length(sol_me2.times) == length(t_l)
         @test length(sol_me2.states) == length(t_l)
         @test size(sol_me2.expect) == (0, length(t_l))
+        @test length(sol_me3.times) == length(t_l)
         @test length(sol_me3.states) == length(t_l)
         @test size(sol_me3.expect) == (length(e_ops), length(t_l))
+        @test length(sol_mc.times) == length(t_l)
+        @test size(sol_mc.expect) == (length(e_ops), length(t_l))
+        @test length(sol_mc_states.times) == length(t_l)
+        @test size(sol_mc_states.expect) == (0, length(t_l))
+        @test length(sol_sse.times) == length(t_l)
+        @test size(sol_sse.expect) == (length(e_ops), length(t_l))
         @test sol_me_string ==
               "Solution of time evolution\n" *
               "(return code: $(sol_me.retcode))\n" *