def chgsum(cll, el, site, silent = 1): """ calculate sum of Bader charges for particular atoms """ for cl in cll: # print(cl.id, end = ' ') try: cl.chgsum[(el, site)] = 0 except: pass if not hasattr(cl, 'charges') or len(cl.charges) == 0: cl.get_bader_ACF() # determine_symmetry_positions(cl.end, el, silent = 0) # print('') try: pos = determine_symmetry_positions(cll[0].end, el, silent = 1) except: printlog('chgsum() Warning!', cll[0].id, 'is broken!') return 0 for p in pos[site]: '' for cl in cll: if not hasattr(cl, 'chgsum'): cl.chgsum = {} cl.chgsum[(el, site)] = 0 cl.chgsum[(el, site)] += cl.charges[p] # print('{:5.3f}'.format(cl.charges[p]), end = ' ') # print('') if not silent: print('Sum of charges for ', el+str(site+1), ':') el_ind = cl.init.znucl.index(invert(el)) # index of element in znucl and zval and nznucl zval = cl.init.zval[el_ind] # number of electrons in chosen potential for cl in cll: cl.chgsum[(el, site)]/=len(pos[site]) chgsum = zval - cl.chgsum[(el, site)] if cl == cll[0]: chgsum_ref = chgsum if not silent: print('{:5.2f}({:4.2f})'.format(chgsum, chgsum_ref-chgsum), end = ' ') if not silent: print('\n') # print(cl.charges) return chgsum
def form_en(sources, products, norm_el = None): """ Calculate formation energy of reaction sources, products - list of tuples (x, cl), where x is multiplier and cl is calculation norm_el - which element to use for normalization 'all' - normalize by total number of atoms """ El = [] Nzl = [] for ls in [sources, products]: E = 0 Nz = {} for x, cl in ls: E += x*cl.e0 for i, z in enumerate(cl.end.znucl): if z not in Nz: Nz[z] = 0 Nz[z] += x*cl.end.nznucl[i] El.append(E) Nzl.append(Nz) for z in Nzl[0]: if abs(Nzl[0][z] - Nzl[1][z]) > 1e-5: printlog('Error! Number of', invert(z), 'atoms in source and product are different!') # norm = 1 if 'all' == norm_el: norm = sum(Nzl[0].values()) elif type(norm_el) == str: norm = Nzl[0][invert(norm_el)] elif norm_el != None: norm = norm_el else: norm = 1 # print('Normalizing by ', norm_el, norm, 'atoms') print('dE = {:4.2f} eV'.format((El[1]-El[0])/norm))
def set_potential(self,znucl, arg = ''): # print arg if not arg: arg = header.PATH2POTENTIALS+'/'+invert(znucl) printlog('Attention!, Default potentials is chosen from ',header.PATH2POTENTIALS, 'for',invert(znucl) , imp ='Y') if type(arg) not in (str,): # sys.exit("\nset_potential error\n") raise RuntimeError if znucl in self.potdir: if arg == self.potdir[znucl]: print_and_log( "Warning! You already have the same potential for "+str(znucl)+" element\n" ) # print type(self.potdir) self.potdir[znucl] = arg self.history += "Potential for "+str(znucl)+" was changed to "+arg+"\n" print_and_log( "Potential for "+str(znucl)+" was changed to "+arg+"\n" ) # self.update() return
else: cases = case_raw.keys() if vectors == 'Binary': # Take log base 2 to figure out how many bits we need for each human_size = int(ceil(log(len(human), 2))) # 2 dec_size = int(ceil(log(len(declensions), 2))) # 3 gen_size = int(ceil(log(len(genders), 2))) # 2 case_size = int(ceil(log(len(cases), 2))) # 3 if casenum_sep == True: num_size = int(ceil(log(len(numbers), 2))) # 1 # Now make two way dictionary with bit vectors human_dict = functions.binaryDict(human) dec_dict = functions.binaryDict(declensions) dec_dict.update(functions.invert(dec_dict)) gen_dict = functions.binaryDict(genders) gen_dict.update(functions.invert(gen_dict)) case_dict = functions.binaryDict(cases) case_dict.update(functions.invert(case_dict)) if casenum_sep == True: num_dict = functions.binaryDict(numbers) num_dict.update(functions.invert(num_dict)) # Identity vectors else: human_size = len(human) dec_size = len(declensions) gen_size = len(genders) case_size = len(cases) if casenum_sep == True: num_size = len(numbers)
def add_neb( starting_calc=None, st=None, st_end=None, it_new=None, ise_new=None, i_atom_to_move=None, up='up2', search_type='vacancy_creation', images=None, r_impurity=None, corenum=None, calc_method=['neb'], inherit_option=None, mag_config=None, i_void_start=None, i_void_final=None, atom_to_insert=None, atom_to_move=None, rep_moving_atom=None, end_pos_types_z=None, replicate=None, it_new_folder=None, inherit_magmom=False, x_start=None, xr_start=None, x_final=None, xr_final=None, upload_vts=False, run=False, add_loop_dic=None, old_behaviour=None, ): """ Prepare needed files for NEB Provides several regimes controlled by *search_type* flag: - existing_voids - search for voids around atom and use them as a final position - vacancy_creation - search for neighbors of the same type and make a vacancy as a start position - interstitial_insertion - search for two neighboring voids; use them as start and final positions by inserting atom *atom_to_insert* - None - just use st and st2 as initial and final ###INPUT: - starting_calc (Calculation) - Calculation object with structure - st (Structure) - structure, can be used instead of Calculation - it_new (str) - name for calculation - st_end (Structure) - final structure - i_atom_to_move (int) - number of atom for moving starting from 0; - *mag_config* (int ) - choose magnetic configuration - allows to obtain different localizations of electron - *replicate* (tuple 3*int) - replicate cell along rprimd - i_void_start, i_void_final (int) - position numbers of voids (or atoms) from the suggested lists - atom_to_insert (str) - element name of atom to insert - atom_to_move (str) - element name of atom to move - it_new_folder (str) - section folder - inherit_option (str) - passed only to add_loop - inherit_magmom (bool) - if True than magmom from starting_calc is used, else from set - end_pos_types_z (list of int) - list of Z - type of atoms, which could be considered as final positions in vacancy creation mode - calc_method (list) - 'neb' - 'only_neb' - run only footer - x_start, x_final (array) - explicit xcart coordinates of moving atom for starting and final positions, combined with atom_to_insert - xr_start, xr_final (array) - explicit xred - rep_moving_atom (str)- replace moving atom by needed atom - can be useful than completly different atom is needed. - upload_vts (bool) - if True upload Vasp.pm and nebmake.pl to server - run (bool) - run on server ###RETURN: None ###DEPENDS: ###TODO 1. Take care of manually provided i_atom_to_move in case of replicate flag using init_numbers 2. For search_type == None x_m and x_del should be determined for magnetic searching and for saving their coordinates to struct_des; now their just (0,0,0) """ if old_behaviour: naming_conventions209 = False # else: naming_conventions209 = True # set False to reproduce old behavior before 2.09.2017 # print(atom_to_insert) # sys.exit() calc = header.calc struct_des = header.struct_des varset = header.varset if not add_loop_dic: add_loop_dic = {} if not end_pos_types_z: end_pos_types_z = [] if not hasattr(calc_method, '__iter__'): calc_method = [calc_method] if starting_calc and st: printlog( 'Warning! both *starting_calc* and *st* are provided. I use *starting_calc*' ) st = copy.deepcopy(starting_calc.end) elif starting_calc: st = copy.deepcopy(starting_calc.end) printlog('I use *starting_calc*') elif st: '' printlog('I use *st*') else: printlog( 'Error! no input structure. Use either *starting_calc* or *st*') if corenum == None: if images == 3: corenum = 15 elif images == 5: corenum = 15 elif images == 7: corenum = 14 else: printlog('add_neb(): Error! number of images', images, 'is unknown to me; please provide corenum!') # print(atom_to_insert) # sys.exit() if corenum: # header.corenum = corenum '' else: corenum = header.CORENUM if corenum % images > 0: print_and_log( 'Error! Number of cores should be dividable by number of IMAGES', images, corenum) if not ise_new: ise_new = starting_calc.id[1] printlog('I use', ise_new, 'as ise_new', imp='y') name_suffix = '' st_pores = [] name_suffix += 'n' + str(images) """Replicate cell """ if replicate: print_and_log('You have chosen to replicate the structure by', replicate) st = replic(st, mul=replicate) name_suffix += str(replicate[0]) + str(replicate[1]) + str( replicate[2]) printlog('Search type is ', search_type) if search_type == None: if st_end == None: printlog( 'Error! You have provided search_type == None, st_end should be provided!' ) st1 = st st2 = st_end x_m = (0, 0, 0) x_del = (0, 0, 0) else: """1. Choose atom (or insert) for moving """ if is_list_like(xr_start): x_start = xred2xcart([xr_start], st.rprimd)[0] st1, i_m = st.add_atoms([x_start], atom_to_insert, return_ins=1) x_m = x_start # i_m = st1.find_atom_num_by_xcart(x_start) # print(st1.get_elements()[i_m]) # sys.exit() if i_atom_to_move: nn = str(i_atom_to_move + 1) else: nn = str(i_void_start) name_suffix += atom_to_insert + nn write_xyz(st1, file_name=st.name + '_manually_start') printlog('Start position is created manually by adding xr_start', xr_start, x_start) type_atom_to_move = atom_to_insert el_num_suffix = '' else: atoms_to_move = [] atoms_to_move_types = [] # print('d', i_atom_to_move) # sys.exit() if i_atom_to_move: typ = st.get_elements()[i_atom_to_move] printlog('add_neb(): atom', typ, 'will be moved', imp='y') atoms_to_move.append( [i_atom_to_move, typ, st.xcart[i_atom_to_move]]) atoms_to_move_types.append(typ) if naming_conventions209: name_suffix += typ + str(i_atom_to_move + 1) else: #try to find automatically among alkali - special case for batteries for i, typ, x in zip(range(st.natom), st.get_elements(), st.xcart): if typ in ['Li', 'Na', 'K', 'Rb', 'Mg']: atoms_to_move.append([i, typ, x]) if typ not in atoms_to_move_types: atoms_to_move_types.append(typ) if atoms_to_move: # print(atom_to_move) # sys.exit() if not atom_to_move: atom_to_move = atoms_to_move_types[ 0] # taking first found element if len(atoms_to_move_types) > 1: printlog( 'Error! More than one type of atoms available for moving detected', atoms_to_move_types, 'please specify needed atom with *atom_to_move*') type_atom_to_move = atom_to_move #atoms_to_move[0][1] # printlog('atom ', type_atom_to_move, 'will be moved', imp ='y') if i_atom_to_move: printlog('add_neb(): *i_atom_to_move* = ', i_atom_to_move, 'is used', imp='y') numbers = [[i_atom_to_move]] i_void_start = 1 else: printlog('add_neb(): determine_symmetry_positions ...', imp='y') numbers = determine_symmetry_positions(st, atom_to_move) # print(numbers) # sys.exit() if len(numbers) > 0: printlog('Please choose position using *i_void_start* :', [i + 1 for i in range(len(numbers))], imp='y') printlog('*i_void_start* = ', i_void_start) i_m = numbers[i_void_start - 1][0] printlog('Position', i_void_start, 'chosen, atom:', i_m + 1, type_atom_to_move, imp='y') else: i_m = numbers[0][0] x_m = st.xcart[i_m] el_num_suffix = type_atom_to_move + str(i_m + 1) atom_to_insert = atom_to_move st1 = st # elif atom_to_replace: # num = st.get_specific_elements(atom_to_replace) # if len(n)>0: # printlog('Please choose position using *i_void_start* :', [i+1 for i in range(len(num))],imp = 'y' ) # printlog('*i_void_start* = ', i_void_start) # i_m = num[i_void_start-1] # printlog('Position',i_void_start,'chosen, atom to replace:', i_m+1, atom_to_replace, imp = 'y' ) # sys.exit() else: print_and_log( 'No atoms to move found, you probably gave me deintercalated structure', important='y') st_pores, sums, avds = determine_voids(st, r_impurity, step_dec=0.1, fine=2) insert_positions = determine_unique_voids(st_pores, sums, avds) print_and_log( 'Please use *i_void_start* to choose the void for atom insertion from the Table above:', end='\n', imp='Y') if i_void_start == None: sys.exit() if atom_to_insert == None: printlog('Error! atom_to_insert = None') st = st.add_atoms([ insert_positions[i_void_start], ], atom_to_insert) name_suffix += 'i' + str(i_void_start) i_m = st.natom - 1 x_m = st.xcart[i_m] search_type = 'existing_voids' type_atom_to_move = atom_to_insert el_num_suffix = '' st1 = st """2. Choose final position""" if is_list_like(xr_final): x_final = xred2xcart([xr_final], st.rprimd)[0] #old #check if i_atom_to_move should be removed # st2 = st1.del_atom(i_m) # st2 = st2.add_atoms([x_final], atom_to_insert) #new st2 = st1.mov_atoms(i_m, x_final) # st1.printme() # st2.printme() # sys.exit() x_del = x_final search_type = 'manual_insertion' name_suffix += 'v' + str(i_void_final) write_xyz(st2, file_name=st.name + '_manually_final') printlog('Final position is created manually by adding xr_final', xr_final, x_del) elif search_type == 'existing_voids': #Search for voids around choosen atoms if not st_pores: st_pores, sums, avds = determine_voids(st, r_impurity) sur = determine_unique_final(st_pores, sums, avds, x_m) print_and_log('Please choose *i_void_final* from the Table above:', end='\n', imp='Y') if i_void_final == None: sys.exit() x_final = sur[0][i_void_final] # printlog('You chose:', np.array(x_final).round(2), end='\n', imp='Y') x_del = x_final #please compare with vacancy creation mode write_xyz(st.add_atoms([x_final], 'H'), replications=(2, 2, 2), file_name=st.name + '_possible_positions2_replicated') print_and_log('Choosing the closest position as end', important='n') st1 = st st2 = st.mov_atoms(i_m, x_final) name_suffix += el_num_suffix + 'e' + str( i_void_final) + atom_to_insert st1 = return_atoms_to_cell(st1) st2 = return_atoms_to_cell(st2) write_xyz(st1, file_name=st1.name + name_suffix + '_start') write_xyz(st2, file_name=st2.name + name_suffix + '_final') elif search_type == 'vacancy_creation': #Create vacancy by removing some neibouring atom of the same type print_and_log( 'You have chosen vacancy_creation mode of add_neb tool', imp='Y') print_and_log('Type of atom to move = ', type_atom_to_move, imp='y') # print 'List of left atoms = ', np.array(st.leave_only(type_atom_to_move).xcart) sur = local_surrounding(x_m, st, n_neighbours=12, control='atoms', only_elements=[invert(type_atom_to_move)] + end_pos_types_z, periodic=True) #exclude the atom itself # print(x_m) # print(sur) # st.nn() print_and_log( 'I can suggest you ' + str(len(sur[0][1:])) + ' end positions. The distances to them are : ', np.round(sur[3][1:], 2), ' A\n ', 'They are ', type_atom_to_move, [invert(z) for z in end_pos_types_z], 'atoms, use *i_void_final* to choose required: 1, 2, 3 ..', imp='y') if not i_void_final: i_void_final = 1 #since zero is itself print_and_log('Choosing position ', i_void_final, 'with distance', round(sur[3][i_void_final], 2), 'A', imp='y') name_suffix += el_num_suffix + 'v' + str(i_void_final) x_del = sur[0][i_void_final] printlog('xcart of atom to delete', x_del) i_del = st.find_atom_num_by_xcart(x_del) # print(x_del) # print(st.xcart) # for x in st.xcart: # if x[0] > 10: # print(x) print_and_log('number of atom to delete = ', i_del, imp='y') if i_del == None: printlog('add_neb(): Error! I could find atom to delete!') # print st.magmom # print st1.magmom # try: if is_list_like(xr_start): st2 = st1.mov_atoms( i_m, x_del) # i_m and sur[0][neb_config] should coincide # i_del = st1.find_atom_num_by_xcart(x_del) st1 = st1.del_atom(i_del) else: print_and_log( 'Making vacancy at end position for starting configuration', imp='y') st1 = st.del_atom(i_del) print_and_log( 'Making vacancy at start position for final configuration', important='n') st2 = st.mov_atoms( i_m, x_del) # i_m and sur[0][neb_config] should coincide # except: # st2 = st st2 = st2.del_atom(i_del) # these two steps provide the same order """Checking correctness of path""" #if start and final positions are used, collisions with existing atoms are possible if is_list_like(xr_start) and is_list_like(xr_final): printlog('Checking correctness') st1, _, _ = st1.remove_close_lying() stt = st1.add_atoms([ x_final, ], 'Pu') stt, x, _ = stt.remove_close_lying( rm_both=True ) # now the final position is empty for sure; however the order can be spoiled # print(st._removed) if stt._removed: st1 = stt # only if overlapping was found we assign new structure st2, _, _ = st2.remove_close_lying(rm_first=stt._removed) stt = st2.add_atoms([ x_start, ], 'Pu') stt, x, _ = stt.remove_close_lying( rm_both=True) # now the start position is empty for sure if stt._removed: st2 = stt print(st2.get_elements()) # sys.exit() elif is_list_like(xr_final) and not is_list_like(xr_start) or is_list_like( xr_start) and not is_list_like(xr_final): printlog( 'Attention! only start of final position is provided, please check that everything is ok with start and final states!!!' ) """ Determining magnetic moments """ vp = varset[ise_new].vasp_params if search_type != None: #for None not implemented; x_m should be determined first for this if 'ISPIN' in vp and vp['ISPIN'] == 2: print_and_log( 'Magnetic calculation detected. Preparing spin modifications ...', imp='y') cl_test = CalculationVasp(varset[ise_new]) cl_test.init = st1 # print 'asdfsdfasdfsadfsadf', st1.magmom if inherit_magmom and hasattr(st, 'magmom') and st.magmom and any( st.magmom): print_and_log( 'inherit_magmom=True: You have chosen MAGMOM from provided structure', imp='y') name_suffix += 'mp' #Magmom from Previous else: cl_test.init.magmom = None print_and_log( 'inherit_magmom=False or no magmom in input structure : MAGMOM will be determined from set', imp='y') name_suffix += 'ms' #Magmom from Set cl_test.actualize_set() #find magmom for current structure st1.magmom = copy.deepcopy(cl_test.init.magmom) st2.magmom = copy.deepcopy(cl_test.init.magmom) # sys.exit() # print_and_log('The magnetic moments from set:') # print cl_test.init.magmom #checking for closest atoms now only for Fe, Mn, Ni, Co sur = local_surrounding(x_m, st1, n_neighbours=3, control='atoms', periodic=True, only_elements=header.TRANSITION_ELEMENTS) dist = np.array(sur[3]).round(2) numb = np.array(sur[2]) a = zip(numb, dist) # a= np.array(a) # print a[1] # a = np.apply_along_axis(np.unique, 1, a) # print a def unique_by_key(elements, key=None): if key is None: # no key: the whole element must be unique key = lambda e: e return list({key(el): el for el in elements}.values()) # print a mag_atoms_dists = unique_by_key(a, key=itemgetter(1)) # print (mag_atoms_dists) # a = unique_by_key(a, key=itemgetter(1)) print_and_log( 'I change spin for the following atoms:\ni atom dist\n', np.round(mag_atoms_dists, 2), imp='y') # print 'I have found closest Fe atoms' muls = [(1.2, 0.6), (0.6, 1.2)] mag_moments_variants = [] for mm in muls: mags = copy.deepcopy(cl_test.init.magmom) # print mags for a, m in zip(mag_atoms_dists, mm): # print t[1] mags[a[0]] = mags[a[0]] * m mag_moments_variants.append(mags) print_and_log('The list of possible mag_moments:', imp='y') for i, mag in enumerate(mag_moments_variants): print_and_log(i, mag) print_and_log( 'Please use *mag_config* arg to choose desired config', imp='y') if mag_config != None: st1.magmom = copy.deepcopy(mag_moments_variants[mag_config]) st2.magmom = copy.deepcopy(mag_moments_variants[mag_config]) name_suffix += 'm' + str(mag_config) print_and_log('You have chosen mag configuration #', mag_config, imp='y') else: print_and_log('Non-magnetic calculation continue ...') """3. Add to struct_des, create geo files, check set, add_loop """ if starting_calc: it = starting_calc.id[0] it_new = it + 'v' + str(starting_calc.id[2]) + '.' + name_suffix if not it_new_folder: it_new_folder = struct_des[it].sfolder + '/neb/' obtained_from = str(starting_calc.id) if not ise_new: print_and_log('I will run add_loop() using the same set', important='Y') ise_new = cl.id[1] elif st: if not it_new: printlog( 'Error! please provide *it_new* - name for your calculation', important='Y') it = None it_new += '.' + name_suffix obtained_from = st.name if not ise_new: printlog('Error! please provide *ise_new*', important='Y') if not it_new_folder: printlog( 'Error! please provide *it_new_folder* - folder for your new calculation', important='Y') if rep_moving_atom: it_new += 'r' + rep_moving_atom if it_new not in struct_des: add_des(struct_des, it_new, it_new_folder, 'Automatically created and added from ' + obtained_from) print_and_log( 'Creating geo files for starting and final configurations (versions 1 and 2) ', important='y') # if starting_calc: # cl = copy.deepcopy(starting_calc) # else: cl = CalculationVasp() #write start position struct_des[it_new].x_m_ion_start = x_m struct_des[it_new].xr_m_ion_start = xcart2xred([x_m], st1.rprimd)[0] # st1, _, _ = st1.remove_close_lying() # st2, _, _ = st2.remove_close_lying() i1 = st1.find_atom_num_by_xcart(x_m, prec=0.3) i2 = st2.find_atom_num_by_xcart(x_del, prec=0.3) if rep_moving_atom: #replace the moving atom by required st1 = st1.replace_atoms([i1], rep_moving_atom) st2 = st2.replace_atoms([i2], rep_moving_atom) else: #allows to make correct order for nebmake.pl st1 = st1.replace_atoms([i1], type_atom_to_move) st2 = st2.replace_atoms([i2], type_atom_to_move) i1 = st1.find_atom_num_by_xcart(x_m, prec=0.3) # the positions were changed i2 = st2.find_atom_num_by_xcart(x_del, prec=0.3) cl.end = st1 ver_new = 1 cl.version = ver_new cl.path["input_geo"] = header.geo_folder + struct_des[it_new].sfolder + '/' + \ it_new+"/"+it_new+'.auto_created_starting_position_for_neb_'+str(search_type)+'.'+str(ver_new)+'.'+'geo' cl.write_siman_geo(geotype='end', description='Starting conf. for neb from ' + obtained_from, override=True) #write final position struct_des[it_new].x_m_ion_final = x_del struct_des[it_new].xr_m_ion_final = xcart2xred([x_del], st2.rprimd)[0] cl.end = st2 ver_new = 2 cl.version = ver_new cl.path["input_geo"] = header.geo_folder + struct_des[it_new].sfolder + '/' + \ it_new+"/"+it_new+'.auto_created_final_position_for_neb_'+str(search_type)+'.'+str(ver_new)+'.'+'geo' cl.write_siman_geo(geotype='end', description='Final conf. for neb from ' + obtained_from, override=True) if not rep_moving_atom: st1s = st1.replace_atoms([i1], 'Pu') st2s = st2.replace_atoms([i2], 'Pu') else: st1s = copy.deepcopy(st1) st2s = copy.deepcopy(st2) vec = st1.center_on(i1) st1s = st1s.shift_atoms(vec) st2s = st2s.shift_atoms(vec) write_xyz(st1s, file_name=it_new + '_start') write_xyz(st2s, file_name=it_new + '_end') st1s.write_poscar('xyz/POSCAR1') st2s.write_poscar('xyz/POSCAR2') # print(a) # runBash('cd xyz; mkdir '+it_new+'_all;'+"""for i in {00..04}; do cp $i/POSCAR """+ it_new+'_all/POSCAR$i; done; rm -r 00 01 02 03 04') with cd('xyz'): a = runBash(header.PATH2NEBMAKE + ' POSCAR1 POSCAR2 3') dst = it_new + '_all' makedir(dst + '/any') for f in ['00', '01', '02', '03', '04']: shutil.move(f + '/POSCAR', dst + '/POSCAR' + f) shutil.rmtree(f) #prepare calculations # sys.exit() #Check if nebmake is avail # if int(runBash('ssh '+cluster_address+' test -e '+project_path_cluster+'/tools/vts/nebmake.pl; echo $?') ): # '' # print_and_log('Please upload vtsttools to ',cluster_address, project_path_cluster+'/tools/vts/') # raise RuntimeError # copy_to_server(path_to_wrapper+'/vtstscripts/nebmake.pl', to = project_path_cluster+'/tools/', addr = cluster_address) # if int(runBash('ssh '+cluster_address+' test -e '+project_path_cluster+'/tools/Vasp.pm; echo $?') ): # copy_to_server(path_to_wrapper+'/vtstscripts/Vasp.pm', to = project_path_cluster+'/tools/', addr = cluster_address) inherit_ngkpt(it_new, it, varset[ise_new]) add_loop(it_new, ise_new, verlist=[1, 2], up=up, calc_method=calc_method, savefile='oc', inherit_option=inherit_option, n_neb_images=images, corenum=corenum, run=run, **add_loop_dic) if upload_vts: siman_dir = os.path.dirname(__file__) # print(upload_vts) push_to_server([ siman_dir + '/cluster_tools/nebmake.pl', siman_dir + '/cluster_tools/Vasp.pm' ], to=header.cluster_home + '/tools/vts', addr=header.cluster_address) else: print_and_log('Please be sure that vtsttools are at', header.cluster_address, header.cluster_home + '/tools/vts/', imp='Y') printlog('add_neb finished') return it_new
######## # Read in corpus (corpus, suffixes) = objects.readCorpus(constants.corpus_file) # Determine corpus size from this corpus_size = len(corpus) # Create suffix dictionary if constants.vectors == 'binary': suffix_size = int(ceil(log(len(suffixes), 2))) # 6 suffix_dict = functions.binaryDict(suffixes) else: suffix_size = len(suffixes) suffix_dict = dict(zip(suffixes, map(tuple, identity(suffix_size)))) suf_to_tup = functions.invert(suffix_dict) suffix_dict.update(functions.invert(suffix_dict)) ########## # OUTPUT # ########## # Output layer will be list of potential suffixes, gathered from corpus output_nodes = suffix_size # Print information print '''Training on %d Epochs Number of Input Nodes: %d Number of Hidden Nodes: %d Number of Output Nodes: %d Token Frequency taken into account: %s\n''' % (
# Determine corpus size from this corpus_size = len(corpus) root_size = int(ceil(log(corpus_size, 2))) # Create suffix dictionary suf_dict = {} for suffix in suffixes: phon_suf = functions.reworkSuffix(suffix) feat_suf = () for phoneme in ''.join(phon_suf): feat_suf += constants.phon_to_feat[phoneme] suf_dict[suffix] = feat_suf inv_suf = functions.invert(suf_dict) # TOTAL input bits # If binary and casenum separate: 9 + 2 + 3 + 2 + 3 + 1 = 20 # If binary and casenum together: 9 + 2 + 3 + 2 + 4 = 20 # If identity and casenum separate: 9 + 3 + 5 + 3 + 5 + 2 = 27 # If identity and casenum together: 9 + 3 + 5 + 3 + 10 = 30 input_nodes = sum([root_size, constants.human_size, constants.dec_size, constants.gen_size, constants.case_size]) if constants.casenum_sep == True: input_nodes += constants.num_size ########## # OUTPUT # ########## # # Output layer will be list of potential suffixes, gathered from corpus
# Determine corpus size from this corpus_size = len(corpus) root_size = int(ceil(log(corpus_size, 2))) # Create suffix dictionary suf_dict = {} for suffix in suffixes: phon_suf = functions.reworkSuffix(suffix) feat_suf = () for phoneme in ''.join(phon_suf): feat_suf += constants.phon_to_feat[phoneme] suf_dict[suffix] = feat_suf inv_suf = functions.invert(suf_dict) # TOTAL input bits # If binary and casenum separate: 9 + 2 + 3 + 2 + 3 + 1 = 20 # If binary and casenum together: 9 + 2 + 3 + 2 + 4 = 20 # If identity and casenum separate: 9 + 3 + 5 + 3 + 5 + 2 = 27 # If identity and casenum together: 9 + 3 + 5 + 3 + 10 = 30 input_nodes = sum([ root_size, constants.human_size, constants.dec_size, constants.gen_size, constants.case_size ]) if constants.casenum_sep == True: input_nodes += constants.num_size ########## # OUTPUT #
def find_polaron(st, i_alk_ion, out_prec = 1): """ #using magmom, find the transition atoms that have different magnetic moments #i_alk_ion - number of ion from 0 to calculate distances to transition metals out_prec (int) - precision of magmom output # maglist = cli.end.get_maglist() # magm = np.array(cli.end.magmom) # n_tm = len(magm[maglist]) # # print(len(maglist)) # numb, dist, chosen_ion = around_alkali(cli.end, n_tm, atom_num) # # print(magm[numb][1:]) # mtm = magm[numb][1:] # the first is alkali # m_av = sum(mtm)/len(mtm) # print(mtm-m_av) """ def zscore(s): # print(np.std(s)) return (s - np.mean(s)) / np.std(s) magmom = np.array(st.magmom) if len(magmom) == 0 : printlog('Error! magmom is empty') _, mag_numbers = st.get_maglist() pol = {} # for z in mag_numbers: # pos = determine_symmetry_positions(st, invert(z)) # sys.exit() magmom_tm = None for key in mag_numbers: printlog('Looking at polarons on transition atoms: ',invert(key) ) numbs = np.array(mag_numbers[key]) # print(numbs) # print(magmom) magmom_tm = magmom[numbs] dev = np.absolute( zscore(magmom_tm) ) # print(magmom_tm) # print(list(zip(magmom_tm, dev.round(1)))) # p = np.where(dev>2)[0] # 2 standard deviations # print(dev>2) # print (type(numbs)) nstd = 1.5 # nstd = 4 i_pols = numbs[dev>nstd] if len(i_pols) > 0: x1 = st.xcart[i_alk_ion] d_to_pols = [] for j in i_pols: x2 = st.xcart[j] d, _ = st.image_distance(x1, x2, st.rprimd) d_to_pols.append(d) print('polarons are detected on atoms', [i+1 for i in i_pols], 'with magnetic moments:', magmom[i_pols], 'and distances: '+', '.join('{:2.2f}'.format(d) for d in d_to_pols), 'A' ) print('mag moments on trans. atoms:', magmom_tm.round(out_prec)) pol[key] = i_pols else: print('no polarons is detected with nstd', nstd) print('mag moments on trans. atoms:', magmom_tm.round(out_prec)) # print(' deviations :', dev.round(1)) pol[key] = None return pol, magmom_tm
def add_to_archive_database(cl, subgroup): """ cl is Calculation which should be added to database subgroup (str) - subgroup folder """ from pymatgen.core.composition import Composition from pymatgen.io.cif import CifWriter from pymatgen.symmetry.analyzer import SpacegroupAnalyzer join = os.path.join basename = os.path.basename dirname = os.path.dirname save_format = 'azh' dbpath = header.PATH2DATABASE it = cl.id[0] # print(cl.path) sub_folder = cl.path['output'].split('/')[ 0] # usually basic chemical formula # sub_folder = header.struct_des[it].sfolder.split('/')[0] # usually basic chemical formula print('Processing ', cl.id) cl.read_results() if '4' not in cl.state: return st = cl.end # print(cl.end.typat) # sys.exit() if 1: #determine x #universal method, supports several alkali elements #requires cl.base_formula in 'Na2FePO4F' format #requires pymatgen, would be nice to remove dependency cmb = Composition(cl.base_formula) cm = st.get_pm_composition() rc = cl.end.get_reduced_composition().as_dict( ) #reduced composition dict rcb = cmb.reduced_composition.as_dict() # print(rc, rcb) alk = list(set(st.get_specific_elements( header.ALKALI_ION_ELEMENTS))) # list of unique alkali elements tra = list(set(st.get_specific_elements(header.TRANSITION_ELEMENTS))) # print(alk, tra) el_for_norm = tra[0] #first element used for normalization nnb = rcb[el_for_norm] #number of norm elements in base nn = rc[el_for_norm] #number of norm elements in interesting structure # print(nb, n) mul = nn / nnb # multiplier that garanties normalization # print(rcb) nab = sum([ rcb[invert(z)] for z in header.ALKALI_ION_ELEMENTS if invert(z) in rcb ]) na = sum([rc[el] for el in alk]) x = na / mul / nab # determine formula # cm = st.get_pm_composition() #get pymatgen composition class # print( (cm/4).formula) # print('Material detected:', formula, 'sub_folder:', sub_folder) #obtain base without alk formula = (cm.reduced_composition / mul).formula # formula = formula.replace('1 ', '').replace(' ', '') # print(formula) cl.formula = formula # print(Composition('Na0.75')) print('Material detected:', formula, 'sub_folder:', sub_folder) # sys.exit() if 0: #Old method, not robust at all! #determine x for alkali ion from structure name parsed = re.findall(r'([A-Z][a-z]*)(\d*)', formula) parsed = [(el, x if x else '1') for (el, x) in parsed] print(parsed) print('detected element is ', parsed[0][0]) if parsed[0][0] in [invert(z) for z in header.ALKALI_ION_ELEMENTS]: x = parsed[0][0] if hasattr(cl, 'max_alk_ion_content'): x = float(x) / cl.max_alk_ion_content else: x = '1' else: x = '0' sfolder = os.path.join(dbpath, sub_folder) name = [] if 'azh' in save_format: #1. Single point calculation of total energy # print(sfolder) makedir(join(sfolder, 'dummy')) if x < 1: x = int(round(100 * x, 0)) else: x = int(round(x, 0)) print('Concentration x:', x) name.append('x' + str(x)) # sys.exit() # if formula in ['LiCoO2', 'LiTiO2', 'LiFePO4', 'NaFePO4', 'LiMnPO4', # 'LiNiO2', 'LiTiS2', 'LiMn2O4', 'LiVP2O7', 'LiVPO4F', # 'NaMnAsO4', 'Na2FePO4F', 'Na2FeVF7', 'KFeSO4F', 'NaLiCoPO4F', 'KVPO4F' ]: sfolder = join(sfolder, subgroup) makedir(join(sfolder, 'dummy')) cl.set.update() # print(cl.potcar_lines) potcar1_m = cl.potcar_lines[0][0] if '_' in potcar1_m: (pot, _) = potcar1_m.split('_') else: pot = potcar1_m xc = cl.xc_inc if '-' in xc: xc = cl.xc_pot if xc == 'PE': func = 'PBE' elif xc == 'CA': func = 'LDA' elif xc == 'PS': func = 'PBEsol' else: print('uknown xc type:', xc) sys.exit() if cl.set.spin_polarized: func = 'U' + func #unrestricted u_ramping_flag = False if hasattr(cl.set, 'u_ramping_nstep') and cl.set.u_ramping_nstep: func += '-UR' u_ramping_flag = True elif cl.set.dftu: func += '-U' else: func += '-' func += pot.lower() ecut = str(round(cl.set.ecut)) func += ecut # print(func) name.append(func) name.extend([it.replace('.', '_')] + [cl.id[1]] + [str(cl.id[2])]) name_str = '_'.join(name) # print('_'.join(name) ) # sys.exit() outcar_name = name_str + '.out' shutil.copyfile(cl.path["output"], join(sfolder, outcar_name)) if u_ramping_flag: print(cl.associated_outcars) for i, u_outcar in enumerate( cl.associated_outcars[:-1] ): # except the last one, which was copied above u = u_outcar.split('.')[1] # print(u) path_to_outcar = join(dirname(cl.path["output"]), u_outcar) cl.read_results(load='o', choose_outcar=i + 1, only_load=1) shutil.copyfile(path_to_outcar, join(sfolder, name_str + '_' + u + '.out')) # sys.exit() cl.end.write_xyz(path=sfolder, filename=name_str) pickle_file = cl.serialize(os.path.join(sfolder, 'bin', name_str)) # cl #write input, problem with fitted version 100, which does not have input geometry, since they are created on cluster # makedir(sfolder+'input/dummy') # shutil.copyfile(cl.path["input_geo"], sfolder+'input/'+name_str+'.geo') st_mp = cl.end.convert2pymatgen() sg_before = st_mp.get_space_group_info() # from pymatgen.symmetry.finder import SymmetryFinder # sf = SymmetryFinder(st_mp_prim) symprec = 0.1 sf = SpacegroupAnalyzer(st_mp, symprec=symprec) st_mp_prim = sf.find_primitive() # st_mp_prim = sf.get_primitive_standard_structure() # st_mp_prim = sf.get_conventional_standard_structure() # st_mp_conv = sf.get_conventional_standard_structure() # print(st_mp_conv) # print(st_mp_conv.lattice.matrix) # print(st_mp_prim) # print(st_mp_prim.lattice) sg_after = st_mp_prim.get_space_group_info() if sg_before[0] != sg_after[0]: printlog( 'Attention! the space group was changed after primitive cell searching', sg_before, sg_after) printlog('I will save supercell in cif and reduce symprec to 0.01') st_mp_prim = st_mp symprec = 0.01 if st_mp_prim: cif = CifWriter(st_mp_prim, symprec=symprec) cif_name = name_str + '.cif' cif.write_file(join(sfolder, cif_name)) printlog('Writing cif', cif_name) if 0: #get multiplication matrix which allows to obtain the supercell from primitive cell. #however this matrix is not integer which is not convinient. print(st_mp.lattice.matrix.round(2)) print(st_mp_prim.lattice.matrix.round(2)) mul_matrix = np.dot(st_mp.lattice.matrix, np.linalg.inv(st_mp_prim.lattice.matrix)) print(mul_matrix.round(1)) rprimd = np.dot(mul_matrix, st_mp_prim.lattice.matrix) print(rprimd.round(2)) #write chg if 1: path_to_chg = cl.get_chg_file('CHGCAR') if path_to_chg: makedir(join(sfolder, 'bin', 'dummy')) printlog('path to chgcar', path_to_chg) gz = '.gz' if gz not in path_to_chg: gz = '' shutil.copyfile(path_to_chg, join(sfolder, 'bin', name_str + '.chg' + gz)) #write dos if subgroup in ['dos', 'DOS']: DOSCAR = cl.get_file('DOSCAR', nametype='asoutcar') if DOSCAR: printlog('path to DOSCAR', DOSCAR) gz = '.gz' if gz not in path_to_chg: gz = '' shutil.copyfile(DOSCAR, join(sfolder, 'bin', name_str + '.dos' + gz)) if subgroup in ['BAD']: #bader cl.get_bader_ACF() acf = cl.get_file(basename(cl.path['acf'])) # print(acf) # sys.exit() if acf: shutil.copyfile(acf, join(sfolder, 'bin', name_str + '.acf')) if subgroup in ['ph', 'PH']: #bader # cl.get_bader_ACF() xml = cl.get_file('vasprun.xml', nametype='asoutcar') # print(acf) # sys.exit() if xml: shutil.copyfile(xml, join(sfolder, 'bin', name_str + '.xml')) #make dat #incars makedir(join(sfolder, 'dat', 'dummy')) incars = glob.glob(join(cl.dir, '*INCAR*')) # print(incars) for inc in incars: dest = join(sfolder, 'dat') # inc_name = if not os.path.exists(join(dest, basename(inc))): shutil.copy(inc, dest) #kpoints if it in header.struct_des: with open(join(sfolder, 'dat', 'kpoints_for_kspacings.json'), 'w', newline='') as fp: json.dump( header.struct_des[it].ngkpt_dict_for_kspacings, fp, ) else: printlog('Warning!, it not in struct_des:', it) # print(cl.set.toJSON()) #prepare for neb # makedir(sfolder+'neb_'+name_str+'/dummy') return