打卡11月的第一个任务,在前面的博客中提到过计算拓扑不变量的问题,利用Wilson Loop的方法可以很好的将规范选择问题避免,最近正好在看一篇高阶拓扑半金属的文章,正好学习一下如何利用Wilson loop来计算拓扑不变量.
{:.info}

前言

在这里就不阐述到底如何计算Wilson loop,它与Wannier Center的关系可以看我的这篇博客通过Wannier Center计算体系Z2拓扑不变量,我所有的内容也是从Equivalent expression of Z2 topological invariant for band insulators using the non-Abelian Berry connection中学习的,感兴趣可以参考这篇文章,你也可以将哈密顿量换成BHZ模型,遮掩过就可以计算文章中的结果.

我这里势利用了Higher-Order Weyl Semimetals中的哈密顿量,因为自己正在看这篇文章,正好也可以学习一下如何计算Wilson loop.

代码实现

using LinearAlgebra,PyPlot,DelimitedFiles
# =====================================================
function hamset(kx::Float64,ky::Float64,kz::Float64)::Matrix{ComplexF64}
    # 构造系统哈密顿量
    t1::Float64 = 0.2
    t2::Float64 = 0.24
    gam::Float64 = 0.5
    lam::Float64 = 1.0
    ham = zeros(ComplexF64,4,4)
    ham1 = zeros(ComplexF64,4,4)
    #----------------------------
    ham[1,2] = (1 + exp(-1im*kz))*(t1 + t2*exp(-1im*(kx + ky)))
    ham[1,3] = gam + lam*exp(-1im*kx)
    ham[1,4] = gam + lam*exp(-1im*ky)
    ham[2,3] = exp(1im*kz)*(gam + lam*exp(1im*ky))
    ham[2,4] = gam + lam*exp(1im*kx)
    ham[3,4] = (1 + exp(-1im*kz))*(t1 + t2*exp(-1im*(-kx + ky)))
    #-----------------------------------------------------------
    ham1 = ham + ham'
    return ham1
end
# ======================================================================
function main(kz)
    nx::Int64 = 100
    ny::Int64 = 800
    Noccu::Int64 = 2  # 占据态数目
    Kx = range(0,2,length = nx)
    Ky = range(-1,0.9999,length = ny)
    klist = []
    Wave = zeros(ComplexF64,4,4,nx)
    Wan = zeros(ComplexF64,Noccu,Noccu)
    ang = zeros(Float64,ny,Noccu)
    for iy in 1:ny
        ky = Ky[iy]*pi
        append!(klist,ky)
        for ix in 1:nx    # 在固定ky的时候，对每一个kx进行对角化
            kx = Kx[ix]*pi
            ham = hamset(kx,ky,kz)
            val,vec = eigen(ham)
            Wave[:,:,ix] = vec[:,:]  # 存储所有点上的本征矢量
        end
        Wave[:,:,nx] = Wave[:,:,1]  # 首尾相连
        F = 1
        for i1 in 1:nx-1
            for i2 in 1:Noccu
                for i3 in 1:Noccu
                    Wan[i2,i3] = Wave[:,i2,i1]'*Wave[:,i3,i1 + 1]   # 计算Berry联络
                end
            end
            F = F*Wan
        end
        val,vec = eigen(F)
        ang[iy,:] = map(angle,val)/(2*pi)
    end
    return klist,ang
end
# =================================================================
k,ang = main(0.2*pi)
plot(k,ang)