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Experiment‐Driven Modeling of Crystalline Phosphorus Nitride P 3 N 5 : Wide‐Ranging Implications from a Unique Structure
Author(s) -
Tolhurst Thomas M.,
Braun Cordula,
Boyko Teak D.,
Schnick Wolfgang,
Moewes Alexander
Publication year - 2016
Publication title -
chemistry – a european journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.687
H-Index - 242
eISSN - 1521-3765
pISSN - 0947-6539
DOI - 10.1002/chem.201601149
Subject(s) - band gap , nanoelectronics , materials science , density functional theory , tetrahedron , graphene , extended x ray absorption fine structure , crystallography , electronic structure , spectroscopy , ranging , ternary operation , nitride , absorption (acoustics) , chemical physics , condensed matter physics , absorption spectroscopy , nanotechnology , computational chemistry , optoelectronics , chemistry , physics , computer science , telecommunications , optics , quantum mechanics , layer (electronics) , programming language , composite material
Nitridophosphates have emerged as advanced materials due to their structural variability and broad technical applicability. Their binary parent compound P 3 N 5 , a polymeric network of corner‐ and edge‐sharing PN 4 tetrahedra with N[2][S. Horstmann, 1998] and N[3][S. Horstmann, 1997] sites, is a particularly interesting example. We present a study of the band gap and electronic structure of α‐P 3 N 5 by using soft X‐ray spectroscopy measurements and DFT calculations. The band gap, which is crucial for all applications, is measured to be 5.87±0.20 eV. This agrees well with the calculated, indirect band gap of 5.21 eV. The density of states are found to show dramatic variation between the nonequivalent N sites and a high degree of covalency. Coupled to these results is what is, to our knowledge, the largest core hole shift reported to date for a soft X‐ray absorption spectrum. We propose an intuitive bonding scheme for α‐P 3 N 5 that explains the observed band gap and unique density of states, while providing a framework for predicting these properties in known and yet to be discovered PN compounds. We briefly consider the implications of these results for new low‐dimensional P and PN materials, which alongside graphene, could become important materials for nanoelectronics.

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