Ewald summation in Julia

Question

I am writing a small MD (molecular dynamics) engine in Julia and I noticed that 67% of the time spent running the following Ewald summation function (to calculate coulomb energy of an infinite crystal lattice in reciprocal space) is spent in garbage collection. Besides algorithmic improvements, which can certainly be made here, what can I do to make it faster in terms of Julia tricks / good practices?

function getEwaldEnergy(top::Topology, xyz::Array{Float64})::Float64
    # cubic box only for now
    tolerance::Float64 = 1.0e-24
    tryUntil::Int64 = 4  # 5 box sizes gets it to five decimal places
    L::Float64 = top.box[1]
    rc::Float64 = L / 2.0

    α::Float64 = 3.5 / (top.box[1] / 2)
    σ::Float64 = 1 / (sqrt(2) * α)

    λ::Float64 = 1.0
    ns::Array{Int64} = getCombinations(-tryUntil, tryUntil, 3)

    # self-energy corrections
    selfEnergy::Float64 = 0.0
    for i::Int64 in 1:top.nAtoms
        selfEnergy += (1 / (sqrt(2 * pi) * σ)) * (top.charges[i] * top.charges[i])
    end

    # short-range energy
    shortRangeEnergy::Float64 = 0.0
    shortRangeEnergyBefore::Float64 = 0.0
    for l::Int64 in 1:size(ns)[1]
        shortRangeEnergyBefore = shortRangeEnergy
        for i in 1:top.nAtoms
            for j::Int64 in 1:top.nAtoms
                ci::Float64 = top.charges[i]
                cj::Float64 = top.charges[j]

                idx::Array{Array{Int64}} = top.bondIdx
                bonded::Bool = false

                # check if i/j pair is bonded
                for k::Int64 in 1:length(idx)
                    if (i == idx[k][1] && j == idx[k][2]) || (j == idx[k][1] && i == idx[k][2])
                        bonded = true
                        break
                    end
                end

                if bonded == false && !(i == j && ns[l, :] == [0.0, 0.0, 0.0])
                    r::Float64 = norm(xyz[i, :] - xyz[j, :] + L * ns[l, :])
                    if r < rc - λ
                        shortRangeEnergy += 0.5 * ((ci * cj) / r) * erfc(r / (sqrt(2) * σ))
                    elseif r < rc && r > rc - λ
                        # switching function turns on
                        shortRangeEnergy += 0.5 * ((ci * cj) * (rc - r)^2 * (-2 * rc + 2 * r + 3 * λ) * erfc(r / (sqrt(2) * σ))) / (2 * r * λ^3)
                    end
                end
            end
        end
    end


    # long-range energy
    longRangeEnergy::Float64 = 0.0
    longRangeEnergyBefore::Float64 = 0.0
    volume::Float64 = L^3
    ms = ns

    longRangeEnergyBefore = copy(longRangeEnergy)
    for l in 1:size(ms)[1]  # no k = [0, 0, 0]
        if ms[l, :] == [0.0, 0.0, 0.0]
            continue
        end

        # define reciprocal space vectors
        kVector::Array{Float64} = (2 * pi) * (ms[l, :] / L)
        k::Float64 = norm(kVector)

        # check this equal 1 good
        # println(exp(-im * dot(kVector, L * [ms[l, 1], ms[l, 2], ms[l, 3]])))
        strucFactor::ComplexF64 = 0.0
        for i in 1:top.nAtoms
            strucFactor += top.charges[i] * exp(im * dot(kVector, xyz[i, :]))
        end

        longRangeEnergy += ((4 * pi) / (volume)) * ((exp(-σ^2 * k^2 / 2) / k^2) * (abs(strucFactor)^2))
    end


    # this roughly cancels out long range energy due to bonded interactions (Tuckerman pg. 663)
    bondEnergy::Float64 = 0.0
    idx = top.bondIdx
    for b::Int64 in 1:size(idx)[1]
        for i in 1:top.nAtoms
            for j in 1:top.nAtoms
                if ((idx[b][1] == i && idx[b][2] == j) || (idx[b][1] == j && idx[b][2] == i)) # && !(i in isdone)
                    # println("firing j: ", j)
                    ci::Float64 = top.charges[i]
                    cj::Float64 = top.charges[j]
                    # rx::Float64 = xyz[i, 1] - xyz[j, 1]
                    # ry::Float64 = xyz[i, 2] - xyz[j, 2]
                    # rz::Float64 = xyz[i, 3] - xyz[j, 3]
                    rij::Float64 = norm(xyz[i, :] - xyz[j, :])
                    bondEnergy += (ci * cj * erf(rij / (sqrt(2) * σ))) / rij
                end
            end
        end
    end

    ewaldEnergy = shortRangeEnergy + longRangeEnergy - selfEnergy - bondEnergy

    return ewaldEnergy
end