Paper
25 September 2007 Interfacial physics in organic light emitting devices
Author Affiliations +
Abstract
In this paper, we will present some studies of physics at the interfaces in the organic light emitting devices. The paper can be separated into two parts. First part is the manipulation of interfacial energy structures and electron transport properties of organic semiconductors. The second part is substitution and dopant dependence of electronic structures in organic thin films I will present an investigation of the energy structures and electrical doping mechanisms of the organic semiconductor surface through current-voltage (I-V) characteristics and photoemission spectroscopies. We found that both surface energy structures and transport properties can be manipulated with mix of LiF or Cs2CO3. The I-V characteristics show that the current efficiency is significantly improved with Cs2CO3 doped either at the surface or in the bulk Alq3. As Cs2CO3 doping works efficiently with Al as well as other cathode metals, the interfacial chemistry and carrier injection mechanisms of such cathode structures are compared to that of the conventional LiF thin layers. To understand the mechanisms of the improvement on electron injection, the surface energy levels of metal and organic materials were measured with ultraviolet photoemission spectroscopy (UPS) and the interfacial chemistry was studied with X-ray photoemission spectroscopy (XPS). From UPS spectra, we found that a thin layer of Cs2CO3, as thin as 0.5 A, at the metal and organic ETL interface can bring the Fermi level of Alq3 from mid-gap to less than 0.2 eV below the lowest unoccupied molecular orbital (LUMO), indicating that the Alq3 film at the interface is heavily n-type doped with Cs2CO3 . The smaller gap between the Fermi level and LUMO with Cs2CO3 reduces the electron injection barrier. Strong dipole fields are also found at the surface, which also affects the electron injection considerably. The XPS data further show that Cs ions are dissociated at the interface as soon as Cs2CO3 is deposited on Alq3. The result is different from the case of LiF, in which Al metal is needed for releasing Li ions. With co-evaporation of Cs2CO3 with Alq3 in the bulk as n-doping ETL, the current efficiency can be further improved, which is presumably attributed to the enhancement of the electron transport in the Alq3 films.
© (2007) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). Downloading of the abstract is permitted for personal use only.
Chih-I Wu "Interfacial physics in organic light emitting devices", Proc. SPIE 6766, Optoelectronic Devices: Physics, Fabrication, and Application IV, 67660A (25 September 2007); https://doi.org/10.1117/12.730625
Advertisement
Advertisement
RIGHTS & PERMISSIONS
Get copyright permission  Get copyright permission on Copyright Marketplace
KEYWORDS
Cesium

Carbon monoxide

Interfaces

Metals

Doping

Photoemission spectroscopy

Ions

Back to Top