"The data at hand indicate that the electrically excited laser dye-doped organic semiconductor yields a highly directional, spatially coherent, nearly diffraction-limited beam with characteristics normally associated with narrow-linewidth dye lasers. The estimated linewidth of the emission is comparable with the linewidth reported for broadband laser emission in pulsed dye lasers." [Opt. Lett. 31, 412-414 (2007).]
"Examination of available results indicates that there is sufficient evidence to classify the reported emission as being equivalent to broadband dye laser radiation... In the spectral domain the high visibility of the interferograms, V ~ 0.9, is a macroscopic manifestation that the measured radiation exhibits much higher coherence than the coherence associated with ASE. Also, the visibility of the observed interferograms is nicely within range of the visibility previously measured, using two-slit interferometry, for soft X-ray laser emission and approaches the visibility (V ~ 0.95) for the 3s2-3p10 transition of a He-Ne laser." [Appl. Phys. B 90, 101-108 (2008).]
These papers report on the first successful observation of coherent emission from organic gain media using direct electric excitation. This mode of excitation is also known as electrical excitation, or, electrical pumping.
The interferogram to the left corresponds to the emission of a high-power optically-pumped coumarin 545 tetramethyl dye laser. Under identical geometrical conditions the interferogram to the right corresponds to the emission from the electrically-pumped sub-micrometer-cavity organic semiconductor using coumarin 545 tetramethyl dye as gain medium. The emission wavelength is ~ 540 nm. These interferograms were recorded on silver-halide film (from Duarte et al., Opt. Lett. 30, 3072-3074 (2005)).
Note: the organic semiconductors used in these experiments are tandem organic light-emitting diodes also known as tandem oleds.
"Therefore the occurrence of fringes must be caused by the spatial coherence present during maser action." (D. F. Nelson and R. J. Collins, Spatial coherence in the output of an optical maser, J. Appl. Phys. 32, 739-740 (1961)).
"A conventional source is spatially almost completely incoherent... such a source gives rise to an intensity distribution in the far zone that changes slowly with direction, i.e. the field exhibits little dependence on direction. On the other hand a source with a high degree of spatial coherence, such as a laser, generates light that is highly directional." (E. Wolf and W. H. Carter, Opt. Commun. 13, 205-209 (1975)).
Note: coherent emission from an electrically pumped organic semiconductor device, also doped with a tetramethyl dye, has been subsequently reported by X. Liu et al., Opt. Lett. 34, 503-505 (2009). Using a similar experimental arrangement these authors report on visibilities of V = 0.89, at ~ 622 nm. A critical commentary to the paper of Liu et al. has been published by I. D. W. Samuel et al., Nat. Photon. 3, 546-549 (2009), and more recently by Duarte (2010).
Key words: coherent OLED, coherent tandem OLED, coherent OLED emission, coherent organic semiconductor, electrical excitation, electric organic laser, electric organic lasers, electrical organic laser, electrical organic lasers, electrical pumping, electrically excited organic laser, electrically pumped organic laser, electrically pumped dye laser, laser OLED emission, microcavity, organic laser, organic laser emission, sub microcavity
Page published on the 7th of March, 2009.
Updated on the 20th of January, 2016.