发明名称 |
Organic electroluminescence element, and light emitting apparatus, image forming apparatus, light emitting element array, display apparatus, and imaging apparatus each using the element |
摘要 |
Provided are organic electroluminescence elements that suppress SP loss even in a strong cavity satisfying a λ/4 interference condition, thereby being improved in luminous efficiency. The organic electroluminescence elements emit light having a peak wavelength of 440 nm or more to 470 nm or less, in which a wavenumber difference δk (Re) between surface plasmons generated at respective reflecting electrode and transparent electrode falls within a specific range. |
申请公布号 |
US8779656(B2) |
申请公布日期 |
2014.07.15 |
申请号 |
US201213564500 |
申请日期 |
2012.08.01 |
申请人 |
Canon Kabushiki Kaisha |
发明人 |
Kajimoto Norifumi |
分类号 |
H01L51/52 |
主分类号 |
H01L51/52 |
代理机构 |
Fitzpatrick, Cella, Harper & Scinto |
代理人 |
Fitzpatrick, Cella, Harper & Scinto |
主权项 |
1. An organic electroluminescence element, comprising a first electrode formed of a metal layer, a first charge transport layer, an emission layer, a second charge transport layer, a second electrode formed of a metal layer, and an out-coupling layer in the stated order, the element causing light emitted by the emission layer to exit from a side of the second electrode, and the element emitting light having a maximum peak wavelength in an emission spectrum of 440 nm or more to 470 nm or less, wherein:
the first charge transport layer is in contact with the first electrode; the second charge transport layer and the out-coupling layer are each in contact with the second electrode; an optical path length L between a first interface between the first electrode and the first charge transport layer, and a second interface between the second electrode and the second charge transport layer satisfies the following relationship:
(−1−φ/π)×(λ/4)<L<(1−φ/π)×(λ/4)where λ represents the maximum peak wavelength, and φ represents a sum [rad] of phase shifts upon reflection of the light having the maximum peak wavelength λ at the first interface and the second interface; and
when a real part of a wavenumber of a surface plasmon generated at the first interface is represented by kr [rad/m] and a real part of a wavenumber of a surface plasmon generated at the second interface is represented by ks [rad/m], the following relationship is satisfied:
−4.5×106≦kr−ks≦2.1×106. |
地址 |
Tokyo JP |