Change SingleSiteOperator with MultiSiteOperator

CHANGELOG.md

@@ -7,6 +7,8 @@ and this project adheres to [Semantic Versioning](https://semver.org/spec/v2.0.0
 
 ## Unreleased
 
+- Change `SingleSiteOperator` with the more general `MultiSiteOperator`. ([#324])
+
 ## [v0.22.0] (2024-11-20)
 
 - Change the parameters structure of `sesolve`, `mesolve` and `mcsolve` functions to possibly support automatic differentiation. ([#311])
@@ -33,3 +35,4 @@ and this project adheres to [Semantic Versioning](https://semver.org/spec/v2.0.0
 [#311]: https://github.com/qutip/QuantumToolbox.jl/issues/311
 [#315]: https://github.com/qutip/QuantumToolbox.jl/issues/315
 [#318]: https://github.com/qutip/QuantumToolbox.jl/issues/318
+[#324]: https://github.com/qutip/QuantumToolbox.jl/issues/324

docs/src/resources/api.md

@@ -248,7 +248,7 @@ fidelity
 
 ```@docs
 Lattice
-SingleSiteOperator
+MultiSiteOperator
 DissipativeIsing
 ```
 

docs/src/tutorials/cluster.md

@@ -11,7 +11,7 @@ We will consider two examples:
 
 ### Monte Carlo Quantum Trajectories
 
-Let's consider a 2-dimensional transferse field Ising model with 4x3 spins. The Hamiltonian is given by
+Let's consider a 2-dimensional transverse field Ising model with 4x3 spins. The Hamiltonian is given by
 
 ```math
 \hat{H} = \frac{J_z}{2} \sum_{\langle i,j \rangle} \hat{\sigma}_i^z \hat{\sigma}_j^z + h_x \sum_i \hat{\sigma}_i^x \, ,
@@ -91,9 +91,9 @@ hy = 0.0
 hz = 0.0
 γ = 1
 
-Sx = mapreduce(i->SingleSiteOperator(sigmax(), i, latt), +, 1:latt.N)
-Sy = mapreduce(i->SingleSiteOperator(sigmay(), i, latt), +, 1:latt.N)
-Sz = mapreduce(i->SingleSiteOperator(sigmaz(), i, latt), +, 1:latt.N)
+Sx = mapreduce(i -> MultiSiteOperator(latt, i=>sigmax()), +, 1:latt.N)
+Sy = mapreduce(i -> MultiSiteOperator(latt, i=>sigmay()), +, 1:latt.N)
+Sz = mapreduce(i -> MultiSiteOperator(latt, i=>sigmaz()), +, 1:latt.N)
 
 H, c_ops = DissipativeIsing(Jx, Jy, Jz, hx, hy, hz, γ, latt; boundary_condition = Val(:periodic_bc), order = 1)
 e_ops = [Sx, Sy, Sz]

docs/src/tutorials/lowrank.md

@@ -47,12 +47,12 @@ Define lr states. Take as initial state all spins up. All other N states are tak
 i = 1
 for j in 1:N_modes
     global i += 1
-    i <= M && (ϕ[i] = SingleSiteOperator(sigmap(), j, latt) * ϕ[1])
+    i <= M && (ϕ[i] = MultiSiteOperator(latt, j=>sigmap()) * ϕ[1])
 end
 for k in 1:N_modes-1
     for l in k+1:N_modes
         global i += 1
-        i <= M && (ϕ[i] = SingleSiteOperator(sigmap(), k, latt) * SingleSiteOperator(sigmap(), l, latt) * ϕ[1])
+        i <= M && (ϕ[i] = MultiSiteOperator(latt, k=>sigmap(), l=>sigmap()) * ϕ[1])
     end
 end
 for i in i+1:M
@@ -85,9 +85,9 @@ hy = 0.0
 hz = 0.0
 γ = 1
 
-Sx = mapreduce(i->SingleSiteOperator(sigmax(), i, latt), +, 1:latt.N)
-Sy = mapreduce(i->SingleSiteOperator(sigmay(), i, latt), +, 1:latt.N)
-Sz = mapreduce(i->SingleSiteOperator(sigmaz(), i, latt), +, 1:latt.N)
+Sx = mapreduce(i->MultiSiteOperator(latt, i=>sigmax()), +, 1:latt.N)
+Sy = mapreduce(i->MultiSiteOperator(latt, i=>sigmay()), +, 1:latt.N)
+Sz = mapreduce(i->MultiSiteOperator(latt, i=>sigmaz()), +, 1:latt.N)
 
 H, c_ops = DissipativeIsing(Jx, Jy, Jz, hx, hy, hz, γ, latt; boundary_condition = Val(:periodic_bc), order = 1)
 e_ops = (Sx, Sy, Sz)

src/spin_lattice.jl

@@ -1,4 +1,4 @@
-export Lattice, SingleSiteOperator, DissipativeIsing
+export Lattice, MultiSiteOperator, DissipativeIsing
 
 @doc raw"""
     Lattice
@@ -15,20 +15,60 @@ end
 
 #Definition of many-body operators
 @doc raw"""
-    SingleSiteOperator(O::QuantumObject, i::Integer, N::Integer)
+    MultiSiteOperator(dims::Union{AbstractVector, Tuple}, pairs::Pair{<:Integer,<:QuantumObject}...)
 
-A Julia constructor for a single-site operator. `s` is the operator acting on the site. `i` is the site index, and `N` is the total number of sites. The function returns a `QuantumObject` given by ``\\mathbb{1}^{\\otimes (i - 1)} \\otimes \hat{O} \\otimes \\mathbb{1}^{\\otimes (N - i)}``.
+A Julia function for generating a multi-site operator ``\\hat{O} = \\hat{O}_i \\hat{O}_j \\cdots \\hat{O}_k``. The function takes a vector of dimensions `dims` and a list of pairs `pairs` where the first element of the pair is the site index and the second element is the operator acting on that site.
+
+# Arguments
+- `dims::Union{AbstractVector, Tuple}`: A vector of dimensions of the lattice.
+- `pairs::Pair{<:Integer,<:QuantumObject}...`: A list of pairs where the first element of the pair is the site index and the second element is the operator acting on that site.
+
+# Returns
+`QuantumObject`: A `QuantumObject` representing the multi-site operator.
+
+# Example
+```jldoctest
+julia> op = MultiSiteOperator(Val(8), 5=>sigmax(), 7=>sigmaz());
+
+julia> op.dims
+8-element SVector{8, Int64} with indices SOneTo(8):
+ 2
+ 2
+ 2
+ 2
+ 2
+ 2
+ 2
+ 2
+```
 """
-function SingleSiteOperator(O::QuantumObject{DT,OperatorQuantumObject}, i::Integer, N::Integer) where {DT}
-    T = O.dims[1]
-    return QuantumObject(kron(eye(T^(i - 1)), O, eye(T^(N - i))); dims = ntuple(j -> 2, Val(N)))
+function MultiSiteOperator(dims::Union{AbstractVector,Tuple}, pairs::Pair{<:Integer,<:QuantumObject}...)
+    sites_unsorted = collect(first.(pairs))
+    idxs = sortperm(sites_unsorted)
+    _sites = sites_unsorted[idxs]
+    _ops = collect(last.(pairs))[idxs]
+    _dims = collect(dims) # Use this instead of a Tuple, to avoid type instability when indexing on a slice
+
+    sites, ops = _get_unique_sites_ops(_sites, _ops)
+
+    collect(dims)[sites] == [op.dims[1] for op in ops] || throw(ArgumentError("The dimensions of the operators do not match the dimensions of the lattice."))
+
+    data = kron(I(prod(_dims[1:sites[1]-1])), ops[1].data)
+    for i in 2:length(sites)
+        data = kron(data, I(prod(_dims[sites[i-1]+1:sites[i]-1])), ops[i].data)
+    end
+    data = kron(data, I(prod(_dims[sites[end]+1:end])))
+
+    return QuantumObject(data; type = Operator, dims = dims)
+end
+function MultiSiteOperator(N::Union{Integer,Val}, pairs::Pair{<:Integer,<:QuantumObject}...)
+    dims = ntuple(j -> 2, makeVal(N))
+
+    return MultiSiteOperator(dims, pairs...)
+end
+function MultiSiteOperator(latt::Lattice, pairs::Pair{<:Integer,<:QuantumObject}...)
+    return MultiSiteOperator(makeVal(latt.N), pairs...)
 end
-SingleSiteOperator(O::QuantumObject{DT,OperatorQuantumObject}, i::Integer, latt::Lattice) where {DT} =
-    SingleSiteOperator(O, i, latt.N)
-SingleSiteOperator(O::QuantumObject{DT,OperatorQuantumObject}, row::Integer, col::Integer, latt::Lattice) where {DT} =
-    SingleSiteOperator(O, latt.idx[row, col], latt.N)
-SingleSiteOperator(O::QuantumObject{DT,OperatorQuantumObject}, x::CartesianIndex, latt::Lattice) where {DT} =
-    SingleSiteOperator(O, latt.idx[x], latt.N)
 
 #Definition of nearest-neighbour sites on lattice
 periodic_boundary_conditions(i::Integer, N::Integer) = 1 + (i - 1 + N) % N
@@ -87,27 +127,34 @@ function DissipativeIsing(
     boundary_condition::Union{Symbol,Val} = Val(:periodic_bc),
     order::Integer = 1,
 )
-    S = [SingleSiteOperator(sigmam(), i, latt) for i in 1:latt.N]
+    S = [MultiSiteOperator(latt, i => sigmam()) for i in 1:latt.N]
     c_ops = sqrt(γ) .* S
 
     op_sum(S, i::CartesianIndex) =
         S[latt.lin_idx[i]] * sum(S[latt.lin_idx[nearest_neighbor(i, latt, makeVal(boundary_condition); order = order)]])
 
     H = 0
     if (Jx != 0 || hx != 0)
-        S = [SingleSiteOperator(sigmax(), i, latt) for i in 1:latt.N]
+        S = [MultiSiteOperator(latt, i => sigmax()) for i in 1:latt.N]
         H += Jx / 2 * mapreduce(i -> op_sum(S, i), +, latt.car_idx) #/2 because we are double counting
         H += hx * sum(S)
     end
     if (Jy != 0 || hy != 0)
-        S = [SingleSiteOperator(sigmay(), i, latt) for i in 1:latt.N]
+        S = [MultiSiteOperator(latt, i => sigmay()) for i in 1:latt.N]
         H += Jy / 2 * mapreduce(i -> op_sum(S, i), +, latt.car_idx)
         H += hy * sum(S)
     end
     if (Jz != 0 || hz != 0)
-        S = [SingleSiteOperator(sigmaz(), i, latt) for i in 1:latt.N]
+        S = [MultiSiteOperator(latt, i => sigmaz()) for i in 1:latt.N]
         H += Jz / 2 * mapreduce(i -> op_sum(S, i), +, latt.car_idx)
         H += hz * sum(S)
     end
     return H, c_ops
 end
+
+function _get_unique_sites_ops(sites, ops)
+    unique_sites = unique(sites)
+    unique_ops = map(i -> prod(ops[findall(==(i), sites)]), unique_sites)
+
+    return unique_sites, unique_ops
+end

test/core-test/low_rank_dynamics.jl

@@ -15,12 +15,12 @@
     i = 1
     for j in 1:N_modes
         i += 1
-        i <= M && (ϕ[i] = SingleSiteOperator(sigmap(), j, latt) * ϕ[1])
+        i <= M && (ϕ[i] = MultiSiteOperator(latt, j => sigmap()) * ϕ[1])
     end
     for k in 1:N_modes-1
         for l in k+1:N_modes
             i += 1
-            i <= M && (ϕ[i] = SingleSiteOperator(sigmap(), k, latt) * SingleSiteOperator(sigmap(), l, latt) * ϕ[1])
+            i <= M && (ϕ[i] = MultiSiteOperator(latt, k => sigmap(), l => sigmap()) * ϕ[1])
         end
     end
     for i in i+1:M
@@ -43,11 +43,11 @@
     hz = 0.0
     γ = 1
 
-    Sx = mapreduce(i -> SingleSiteOperator(sigmax(), i, latt), +, 1:latt.N)
-    Sy = mapreduce(i -> SingleSiteOperator(sigmay(), i, latt), +, 1:latt.N)
-    Sz = mapreduce(i -> SingleSiteOperator(sigmaz(), i, latt), +, 1:latt.N)
+    Sx = mapreduce(i -> MultiSiteOperator(latt, i => sigmax()), +, 1:latt.N)
+    Sy = mapreduce(i -> MultiSiteOperator(latt, i => sigmay()), +, 1:latt.N)
+    Sz = mapreduce(i -> MultiSiteOperator(latt, i => sigmaz()), +, 1:latt.N)
     SFxx = mapreduce(
-        x -> SingleSiteOperator(sigmax(), x[1], latt) * SingleSiteOperator(sigmax(), x[2], latt),
+        x -> MultiSiteOperator(latt, x[1] => sigmax(), x[2] => sigmax()),
         +,
         Iterators.product(1:latt.N, 1:latt.N),
     )