コード例 #1
0
ファイル: hfb.py プロジェクト: ndricke/embed
    def __init__(s, h, V, m, rho=None, Delta=None, tol=10**-7):
        s.h = h
        s.V = V
        s.m = m
        s.n = h.shape[0]
        s.tol = tol
        s.app_pot = 0.
        s.mu = 0.  #each time we re-calc applied potentials, we'll keep track of the total with mu

        if rho is None:  #generate HF density matrix instead
            hart = hf.HF(h, V, m, scf='diis')
            s.rho = hart.get_rho()
            s.E_hf = hart.e / s.n
            print "HF energy: ", s.E_hf
        else:
            s.rho = rho
        if Delta is None:  #just set to 0's, as it would be for HF solution
            s.Delta = np.zeros((s.n, s.n))
        else:
            s.Delta = Delta
        s.F = hf.HF.genFock(s.rho, s.h, s.V)
        s.H = np.zeros((2 * s.n, 2 * s.n))
        s.H[:s.n, :s.n] = s.F
        s.H[s.n:, s.n:] = -s.F
        s.H[:s.n, s.n:] = s.Delta
        s.H[s.n:, :s.n] = -s.Delta
        s.G = s.genG(s.H)
コード例 #2
0
ファイル: hfb_try.py プロジェクト: ndricke/embed
    def __init__(s, h, V, m, rho=None, Delta=None):
        s.h = h
        s.V = V
        s.m = m
        s.n = h.shape[0]

        if rho is None:  #generate HF density matrix instead
            hart = hf.HF(h, V, m)
            s.rho = hart.get_rho()
            print hart.e / s.n
        else:
            s.rho = rho
        if Delta is None:  #just set to 0's, as it would be for HF solution
            s.Delta = np.zeros((s.n, s.n))
        else:
            s.Delta = Delta
        s.F = hf.HF.genFock(s.rho, s.h, s.V)
        s.H = s.genH(s.F, s.Delta)
        s.G = s.genG(s.H)
コード例 #3
0
def C2():
    
    return C2

if __name__ == "__main__":
    n = 12
    m = 4
    U = 2.
    nf = 2

#    h,V = randHV(n,U=U,scale=0.0)
    h,V = coulV(n,U=U,cutoff=2)

    print "Beginning HF"
    hart = hf.HF(h,V,m)
    psi = hart.get_Cocc()
    rho = hart.get_rho()
    F = hart.F
    print np.trace(np.dot(rho,h+F))/n

    print "HF energy:"
    print hart.get_energy()/n

    #make a list of range(nf) that tile n
    fraglist = []
    for i in range(n//nf): #assumes n divisible by nf
        fraglist.append(range(nf*i,nf*(1+i)))

    e_list1 = []; e_list2 = []; e_list3 = []
    for frag_sites in fraglist:
コード例 #4
0
ファイル: hfschm.py プロジェクト: ndricke/embed
        V[i, i, i, i] = U
    return V


n = 12
m = 6
U = 0.
nf = 2
V = V_hubbard(n, U)

h = np.diag(np.ones(n - 1), 1)
h[0, -1] = -1
h += h.T
h *= -1

hart = hf.HF(h, V, m)
psi = hart.get_Cocc()
rho = hart.get_rho()
print hart.get_energy() / n
print hf_energy(h, V, rho) / n

M = psi[:nf, :]
S_M = np.dot(M.T, M)

u, s, v = np.linalg.svd(M)

C = psi.dot(v.T)
T = np.zeros((n, 2 * nf))
T[:nf, :nf] = C[:nf, :nf]
T[nf:, nf:] = C[nf:, :nf]
Tc = C[:, nf:]