Emergent Spin Frustration in Neutral Mixed-Valence 2D Conjugated Polymers: A Potential Quantum Materials Platform [Dataset]

12 pages. -- Fig. S1. Electronic band structures (top) and periodic atomic structures (bottom). -- Fig. S2. Atomically-resolved spin population maps (spin-up: blue; spin-down: red) for B-mv-2DCP. -- Fig. S3. Electronic density of states (DOS) plots for in the FM (left) and AFM (right) configurations...

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Detalles Bibliográficos
Autores: Alcón, Isaac, Ribas-Ariño, Jordi, Moreira, Ibério de P. R., Bromley, Stefan T.
Tipo de recurso: conjunto de datos
Fecha de publicación:2023
País:España
Institución:Consejo Superior de Investigaciones Científicas (CSIC)
Repositorio:DIGITAL.CSIC. Repositorio Institucional del CSIC
OAI Identifier:oai:digital.csic.es:10261/336829
Acceso en línea:http://hdl.handle.net/10261/336829
Access Level:acceso abierto
Palabra clave:Organic quantum materials
Materials thus provides
Employ accurate first
Dimensional conjugated polymers
Conjugated linkers
2d spin frustration
2
Valence molecular systems
Highly attractive platform
Emergent spin frustration
Diamagnetic insulating states
Analogous neutral mixed
Neutral mixed
Magnetic states
Highly promising
Emergent superexchange
Extended mixed
Valence 2dcps
Triangular sublaticce
Surprisingly strong
Robust basis
Principles calculations
Potential applications
Parent compounds
Nodal center
New class
Mediated antiferromagnetic
Magnetic properties
Interest stems
Future bottom
Extensively studied
Device technologies
Cuprate superconductors
Carbon sp
Boron results
Descripción
Sumario:12 pages. -- Fig. S1. Electronic band structures (top) and periodic atomic structures (bottom). -- Fig. S2. Atomically-resolved spin population maps (spin-up: blue; spin-down: red) for B-mv-2DCP. -- Fig. S3. Electronic density of states (DOS) plots for in the FM (left) and AFM (right) configurations for N-mv-2DCP. -- Fig. S4. Atomically-resolved spin population maps. -- Fig. S5. Atomically-resolved spin population maps for cyclo-para-phenylmethine (analog molecular cycle of C-2DCP). -- Fig. S6. Singly occupied natural orbitals (SONO) for the singlet ground state of the CB- model with two magnetic centres. -- Fig. S7. Average of the absolute atomically-partitioned αC spin population, 〈||〉, during 3 ps of an ab initio molecular dynamics (AIMD) simulation of N-mv-2DCP at 300 K using the PBE0 functional. -- Fig. S8. Z-view (top) and y-view (bottom) of the fully optimized atomic structures (both atomic coordinates and cell parameters) for the ox-N-mv-2DCP, N-mv-2DCP and Cl-N-mv-2DCP. -- Fig. S9. Species-projected electronic density of states (PDOS) plots for: ox-N-mv-2DCP (left), N-mv-2DCP (middle) and Cl-N-mv-2DCP (right) per unit cell for the FM solution. -- Fig. S10. Estimated variance of U/t in ox-N-mv-2DCP, N-mv-2DCP and Cl-N-mv-2DCP assuming a single band Hubbard model on a 2D triangular lattice (i.e. the emergent lattice of αC centres). -- Magnetic coupling constant calculations. -- Fig. S11. Magnetic solutions used to extract the magnetic coupling constants described in the text. -- Rationalizing of CN- and CB- differences via molecular orbital diagrams.