The roles of apex dipoles and field penetration in the physics of charged, field emitting, single-walled carbon nanotubes

TL;DR

This study uses quantum-mechanical simulations to explore how apex dipoles and field penetration influence the field emission properties of single-walled carbon nanotubes, revealing complex behaviors and new insights into emission mechanisms.

Contribution

The paper introduces a detailed quantum-mechanical analysis of field emission in SWCNTs, highlighting the roles of apex dipoles, field penetration, and a new FEF definition, advancing understanding beyond classical models.

Findings

Field penetration and band-bending affect emission.

Hydrogen adsorption induces charge-density oscillations.

Predicted FEFs are lower than classical estimates.

Abstract

A 1 $\mu$m long, field emitting, (5,5) single-walled, carbon nanotube (SWCNT) closed with a fullerene cap, and a similar open nanotube with hydrogen-atom termination, have been simulated using the MNDO (Modified Neglect of Diatomic Overlap) quantum-mechanical method. Both contain about 80 000 atoms. It is found that field penetration and band-bending, and various forms of chemically and electrically induced apex dipole, play roles. Field penetration may help to explain electroluminescence associated with field emitting carbon nanotubes. Charge-density oscillations, induced by the hydrogen adsorption, are also found. Many of the effects can be related to known effects that occur with metallic or semiconductor field emitters; this helps both to explain the effects and to unify our knowledge about field electron emitters. However, it is currently unclear how best to treat correlation-and-exchange effects when defining the CNT emission barrier. A new form of definition for the field enhancement factor (FEF) is used. Predicted FEF values for these SWCNTs are significantly less than values predicted by simple classical formulae. The FEF for the closed SWCNT decreases with applied field; the FEF for the H-terminated open SWCNT is less than the FEF for the closed SWCNT, but increases with applied field. Physical explanations for this behavior are proposed. Curved Fowler-Nordheim plots are predicted. Overall, the predicted field emission performance of the H-terminated open SWCNT is slightly better than that of the closed SWCNT, essentially because a C-H dipole is formed that reduces the height of the tunnelling barrier. In general, the physics of a charged SWCNT seems more complex than hitherto realised.