Beispiel #1
0
 def __init__(self, Hlist,dospin=False,tag=''):
    ## Check dimensionality
    LG.info('Creating Hamiltonian: %s    (spin:%s)'%(tag,dospin))
    dims = [x.mat.shape[0] for x in Hlist]
    if len(set(dims)) == 1 and not dospin:
       pass  # same dimension for every term
    elif len(set(dims)) == 2 or dospin:
       LG.info('Spin doubling')
       md, Md = min(dims), max(max(dims),2*min(dims))
       for i in range(len(Hlist)):
          x = Hlist[i]
          if x.mat.shape[0] == md:
             LG.info('spin doubling term: %s'%(x.name))
             x.mat = alg.m2spin(x.mat)
             if x.mat.shape[0] != Md:
                LG.critical('Error doubling spin in term %s'%(x.name))
    else:
       LG.critical('Different dimensions not coherent with spin')
       exit()
    ## Old stuff
    self.lista = Hlist
    try: self.dim = int(list(set([x.mat.shape[0] for x in Hlist]))[0])
    except TypeError:
       LG.critical('Different dimensions not coherent with spin')
       exit()
    self.tag = tag
Beispiel #2
0
def layer(base):
   """
     This function returns a matrix with the layer of each element in the
     diagonal
   """
   aux = [[None for _ in base] for _ in base]
   for E in base:
      N = len(E.onsite)
      aux[E.place][E.place] = E.layer * np.identity(N)
   if base.DOspin: return alg.m2spin(bmat(aux))
   else: return bmat(aux)
Beispiel #3
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def position(base,coor=2):
   """
     Returns a matrix with the given coordinate of each atom in the diagonal
   """
   aux = [[None for _ in base] for _ in base]
   for E in base:
      r = E.position
      N = len(E.onsite)
      aux[E.place][E.place] = r[coor] * np.identity(N)
   if base.DOspin: return alg.m2spin(bmat(aux))
   else: return bmat(aux)
Beispiel #4
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def dist(base,r0=np.array([0.,0.,0.])):
   """
     Returns a matrix with the distance of each atom to a given point in the
     diagonal
   """
   aux = [[None for _ in base] for _ in base]
   for E in base:
      r = np.linalg.norm( E.position - r0 )
      N = len(E.onsite)
      aux[E.place][E.place] = r * np.identity(N)
   if base.DOspin: return alg.m2spin(bmat(aux))
   else: return bmat(aux)
Beispiel #5
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def atom(base,Ats=[1]):
   """
     This function returns a matrix with identity matrices in the places of
     the provided atoms (provided by order in the basis)
   """
   if isinstance(Ats,int): Ats = [Ats]
   elif isinstance(Ats,list): pass
   else: LG.error('Wrong input in atom operator')
   aux = [[None for _ in base] for _ in base]
   for E in base:
      dim = len(E.onsite)
      if E.place in Ats: aux[E.place][E.place] = np.identity(dim,dtype=int)
      else: aux[E.place][E.place] = np.zeros((dim,dim),dtype=int)
   if base.DOspin: return alg.m2spin(bmat(aux))
   else: return bmat(aux)
Beispiel #6
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def orbital(base,Orbs=['pz']):
   """
     This function returns a matrix with 1's in the place of the provided
     orbitals
   """
   if isinstance(Orbs,str): Orbs = [Orbs]
   elif isinstance(Orbs,list): pass
   else: LG.error('Wrong input in orbital operator')
   diag_name = []
   for E in base:
      for o in E.orbitals:
         diag_name.append(o)
   diag = [0 for _ in diag_name]
   for i in range(len(diag_name)):
      if diag_name[i] in Orbs: diag[i] = 1
   if base.DOspin: return alg.m2spin(coo_matrix(np.diag(diag)))
   else: return coo_matrix(np.diag(diag))
Beispiel #7
0
def green_function(e, v, h, delta=0.01, path_selfes='.', force=False, l=1.0):
    """
     Returns the Green's function of a given hamiltonian (v) with self-energy
     (s) and broadening (delta)
   ** Note that v is a matrix (on-site) but h is a hamiltonian class
   """
    e = round(e, 8)
    LG = logging.getLogger('mygreen_tools')
    emat = np.matrix(np.identity(v.shape[0]), dtype=complex) * (e + delta * 1j)
    if l == 0.:
        LG.debug('Self-Energy coupling = 0')
        #print('Self-Energy coupling = 0')
        return (emat - v).I
    else:
        sname = path_selfes + 'self%s.npy' % (e)
        try:
            if force: raise FileNotFoundError
            s = np.load(sname)
            if v.shape != s.shape: s = alg.m2spin(s)
            LG.info('loaded from file ' + sname)
            #print('loaded from file '+sname)
        except FileNotFoundError:
            LG.debug('Calculating for E=%s' % (e))
            print('Calculating for E=%s' % (e))
            #_,s = calc_selfe(e,h,delta=delta,path=path_selfes)
            _,s = mygreen.bloch_selfenergy(h,energy=e,delta=delta,\
                                          nk=100,error=10**(-5),\
                                       #mode="full")
                                       #mode="renormalization")


                                          mode="adaptative")
            if path_selfes != None:
                sname = path_selfes + 'self%s.npy' % (e)
                np.save(sname, s)
                LG.debug('Saved: %s' % (sname))
        return (emat - v - l * s).I
Beispiel #8
0
 def dospin(self):
     LG.info('Modifying basis for spin')
     self.LAYS = alg.m2spin(self.LAYS)
     self.ORBS = alg.m2spin(self.ORBS, Delt='')
     self.SUBS = alg.m2spin(self.SUBS)
     self.ATS = alg.m2spin(self.ATS)
     self.AUX_INDS = alg.m2spin(self.AUX_INDS)
     self.INDS = alg.m2spin(self.INDS)
     self.SPIN = np.array([(-1)**i for i in range(len(self.ORBS))])
     if len(self.LAYS) != len(self.ORBS) != len(self.SUBS) !=\
        len(self.ATS) != len(self.AUX_INDS) != len(self.INDS):
         LG.critical('Problem Spin-doubling')
         print('Layers:', len(self.LAYS))
         print('Orbitals:', len(self.ORBS))
         print('Sublattice:', len(self.SUBS))
         print('Atoms:', len(self.ATS))
         print('Indices', len(self.INDS))
         print('Aux Indices:', len(self.AUX_INDS))
         exit()
     self.ndim = len(self.ATS)  # Hamiltonian dimension
     LG.info('New basis dimension: %s' % (self.ndim))