{'fraction_non_alphanumeric': 0.018469656992084433, 'fraction_numerical': 0.0, 'mean_word_length': 5.540229885057471, 'pattern_counts': {'":': 0, '<': 0, '<?xml version=': 0, '>': 0, 'https://': 0, 'lorem ipsum': 0, 'www.': 0, 'xml': 0}, 'pii_count': 0, 'substrings_counts': 0, 'word_list_counts': {'cursed_substrings.json': 0, 'profanity_word_list.json': 0, 'sexual_word_list.json': 0, 'zh_pornsignals.json': 0}}
Covariant cubic approximation for many-body electronic systems

A charge conserving approximation scheme determining the excitations of crystalline solids is proposed. Like other such approximations, it relies on "downfolding" of the original microscopic model to a simpler electronic model on the lattice with pairwise interactions. A systematic truncation of the set of Dyson - Schwinger equations for correlators of the low energy (downfolded) model of a material, supplemented by a "covariant" calculation of correlators lead to a converging series of approximates. The covariance preserves all the Ward identities among correlators describing various condensed matter probes. It is shown that the third order approximant of this kind beyond classical and gaussian (Hartree - Fock) is precise enough and due to several fortunate features the complexity of calculation is surprisingly low so that a realistic material computation is feasible. Focus here is on the electron field correlator describing the electron (hole) excitations measured in photoemission and other probes. The scheme is tested on several solvable benchmark models