OLED Charge Generation Layer Structure for High-Temperature Reliability

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Solution Overview

Problem

Existing organic electroluminescent devices face challenges in maintaining high temperature reliability due to imbalanced energy levels between charge generation layers, which affects the stability and performance of light emitting devices.

Innovation Solution

A light emitting device structure is developed with an N-type charge generation layer having a host material with a lowest unoccupied molecular orbital energy level less than or equal to −2.9 and a glass transition temperature greater than 130° C, combined with a P-type charge generation layer, to improve energy level balance and high temperature reliability, comprising specific host and guest materials and layer thicknesses.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If conventional charge generation layers are used, then device structure is simple, but energy level balance is poor and high temperature reliability deteriorates

Engineering Contradiction:
Improvehigh temperature reliabilityVSAvoiddevice structure
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The charge generation layer is divided into two separate layers: an N-type charge generation layer and a P-type charge generation layer. This segmentation allows each layer to be independently optimized for its specific charge carrier type, enabling better energy level matching and improved high temperature reliability without compromising device simplicity.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent specifies precise parameter ranges for the host materials in each charge generation layer: the N-type layer uses host materials with LUMO levels of -2.0 eV to -3.5 eV and glass transition temperatures of 80°C to 150°C, while the P-type layer uses host materials with HOMO levels of 5.0 eV to 6.5 eV and glass transition temperatures of 100°C to 200°C. These parameter optimizations resolve the energy level imbalance while maintaining structural simplicity.

Inventive Principle:
Principle #35Parameter changes

2Stability of the object's composition

If charge generation layers with imbalanced energy levels are used, then device structure is simple, but performance stability deteriorates

Engineering Contradiction:
Improveperformance stabilityVSAvoidenergy level balance
Core Design Contradiction:
Stability of the object's compositionVSDevice complexity

Solution Approach 1:

Each charge generation layer is designed with locally optimized properties: the N-type layer is tailored with specific electron transport materials and electron-doping compounds for optimal electron generation, while the P-type layer uses specific hole transport materials and hole-doping compounds for optimal hole generation. This local quality optimization ensures stable performance by matching energy levels at each interface without requiring complex overall device redesign.

Inventive Principle:
Principle #3Local quality

Data Source

PatentUS11758747B2Light emitting device and manufacturing method thereof and display panel
Publication Date: 2023.09.12 BOE TECHNOLOGY GROUP CO LTD
  • US11758747B2 patent drawing
  • US11758747B2 patent drawing
  • US11758747B2 patent drawing

AI summary

The present disclosure provides a light emitting device including: a first electrode; a first light emitting layer on a side of the first electrode; an N-type charge generation layer on a side of the first light emitting layer distal to the first electrode; a P-type charge generation layer on a side of the N-type charge generation layer distal to the first light emitting layer; a second light emitting layer on a side of the P-type charge generation layer distal to the N-type charge generation layer; and a second electrode on a side of the second light emitting layer distal to the P-type charge generation layer. The N-type charge generation layer includes a host material which has a lowest unoccupied molecular orbital energy level less than or equal to −2.9 and a glass transition temperature greater than 130° C.