International Journal of Photoenergy

International Journal of Photoenergy / 2014 / Article
Special Issue

Materials, Designs, Fabrications, and Applications of Organic Electronic Devices

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Research Article | Open Access

Volume 2014 |Article ID 319390 | 6 pages |

Top-Emission Organic Light Emitting Diode Fabrication Using High Dissipation Graphite Substrate

Academic Editor: K. R. Justin Thomas
Received14 Mar 2014
Revised14 May 2014
Accepted22 May 2014
Published02 Jul 2014


This study uses a synthetic graphite fiber as the heat dissipation substrate for top-emission organic light emitting diode (TEOLED) to reduce the impact from joule heat. UV glue (YCD91) was spin coated onto the substrate as the insulation layer. The TEOLED structure is (glass; copper; graphite) substrate/YCD91 glue/Al/Au/EHI608/TAPC/Alq3/LiF/Al/Ag. The proposed graphite fiber substrate presents better luminous performance compared with glass and copper substrate devices with luminance of 3055 cd/m2 and current efficiency of 6.11 cd/A at 50 mA/cm2. When lighting period of different substrates TEOLED, the substrate case back temperature was observed using different lighting periods. A glass substrate element operating from 5 to 25 seconds at 3000 cd/m2 luminance produced a temperature rate of 1.207°C/sec. Under 4000 cd/m2 luminance the copper and graphite substrate temperature rates were 0.125°C/sec and 0.088°C/sec. Graphite component lifetime was determined to be 1.875 times higher than the glass components and 1.125 times higher than that of copper.

1. Introduction

Pope used anthracene monocrystals as luminescent materials in 1963 [1]. However, the operating voltage was higher with lower energy transformation efficiency and no application value [2]. Afterwards, Tang and VanSlyke, Kodak, USA, used vacuum evaporate plating to produce a multilayered OLED using small molecular organic Alq3 as the luminescent and charge transfer material. This innovation greatly improved OLED component characteristics to less than 10 V operating voltage with a quantum efficiency and device structure close to 1%. Using non-mono-vacuum evaporate plating or close to amorphous organic semiconducting thin film technology created a device structure with heterogeneous multilayer organic film contact that greatly improved OLED device performance. This became the operating standard for current OLEDs [3, 4]. In 1990 the Cambridge research team successfully developed a yellow-green lumination LED [5] using PPV luminescent material. Because these macromolecular polymer materials possess characteristics similar to semiconductors and have a simple manufacturing process, they attracted great interest as a potential OLED polymer. The substrate selection process used for TEOLED should consider the surface eveness, resistance to bumping, light weight, and thin, waterproof, and anticorrosive properties. For example, a plastic substrate possesses light, thin, short, and small advantages with resistance to fracture and reelability. However, most of these materials are not resistant to high temperature and are easily degraded by water and oxygen, further reducing the component service life [6]. Someone also attempted to produce OLEDs, a paper base, but there is still a long way to go before this product is ready for commercialization [7]. The introduction of metal foil as the substrate seems to solve the plastic substrate shortcomings with better energy dissipation that could strengthen the component operating time. However, the required surface polishing is something that requires great attention [8]. In 2001, Paulo N. M. Dos Anjos and others used ITO/NPB/Alq3/Mg:Ag as the experimental structure and applied a buffer layer, CuPc, onto the ITO electrode. From the experimental result, we can see that the structure temperature is 70°C without applying a buffer layer, reducing the temperature to 22°C after applying the buffer layer [9]. K. Sudheendra Rao et al. raised the device with structure ITO/m-MTDATA/NPB/Alq3:C545T/Alq3/LiF/Al. As a standard procedure Alq3 is doped with C545T for optimized efficiency (12 cd/A) [10].

2. Experimental

The substrate is spin coated onto glass, copper, and graphite substrates at 1200 rpm for 15 seconds and at 2400 rpm for 20 seconds of UV glue (YCD91) (from Material and Chemical Research Laboratories, Industrial Technology Research Institute). YCD91 was exposed under UV light for 75 seconds to cure. Correct curing produces appropriate substrate material viscosity, which produces uniform spin coating. The treated substrates were placed into a metal thermal system and vacuumized to 6.65 × 10−4 Pa. Al and Au metals were then vacuum evaporized according to the sequence. The substrates were then placed in an organic evaporator and vacuumed to 6.65 × 10−4 Pa. Hole injection layer (HIL) material EHI608, hole transport layer (HTL) material TAPC, and emitting layer material (EML) or electron transport layer (ETL) Alq3 were then vacuum evaporated according to the sequence. The LiF, Al, and Ag cathode metals were then vacuum evaporated in sequence. The finished TEOLED components were tested for luminous characteristics and temperture at the substrate back using multifunctional ammeter KEITHLEY 2400, spectrophotometer PR650, and IR camera NEC TH7716.

3. Results and Discussion

3.1. Characteristics Comparison of Different TEOLED Device Substrates

The TEOLED device structure is Al (100 nm)/Au (2 nm)/EHI608 (10 nm)/TAPC (25 nm)/Alq3 (55 nm)/LiF (0.6 nm)/Al (2 nm)/Ag (17 nm) as indicated in Figure 1. The material thickness of each OLED layer is listed in Table 2. The UV glue (YCD91) material, including heat dissipation particles, was spin coated onto glass, copper, and graphite substrates and then left exposed in air for hardening. The substrate surface roughness was then analyzed using atomic force microscopy (AFM) as shown in Figure 2 and Table 1. The measurement results show that the Rms roughness of the glass, copper, and graphite substrates before spin coating was 4.37, 3.27, and 15.07 nm and 2.97, 2.85, and 0.68 nm after spin coating and drying. Because the graphite substrate is obtained from carbon fiber the surface roughness is quite high. After UV glue spin coating the material roughness was significantly reduced to Rms 0.68 nm. Table 2 shows the roughness comparison of each spin coated UV plastic substrate material.


NumberSubstratesUV glue* (YCD91)W/o UV glue
(Rms: nm)
With UV glue
(Rms: nm)

aGlass18  m4.372.97
bCopper19  m3.272.85
cGraphite21  m15.070.68

Material composition (YCD91).

Oligomer-TM621Monomer-2PEATMPTA-20EAPhoto initiator 184


NumberSubstrate (with UV glue)AlAuHILHTLEML/ETLEILAlAg


The TEOLED device with the graphite substrate exhibited that operating voltage is 14.6 V, lower than that of the glass and copper substrates at 15 V and 15.5 V at 50 mA/cm2. The luminance and current efficiency of the graphite substrate were 3054 cd/m2 and 6.11 cd/A, respectively, compared with those of the cooper substrate (2835 cd/m2 and 5.67 cd/A) and the glass substrate (2730 cd/m2 and 5.46 cd/A). Comparing the luminous characteristics of graphite, copper, and glass, we can see that materials with higher substrate thermal conductivity coefficient achieve better luminous characteristics compared with the glass substrate. The heat dissipating substrate could also elevate the device stability, allowing operation at higher voltage.

The thermal conductivity coefficients for the graphite and copper substrates are much better than that of glass, as indicated in Table 3. From Figure 2 these three substrates are relatively closer in device characteristics at low voltage. However, under high voltage the thermal conductivity of glass restrained the device from dissipating heat, leading to organic layer material crystallization, making the overall device luminous characteristics worse. The graphite and copper substrate devices could maintain higher luminance and current efficiency under higher operating voltage. The thermal conductivity of graphite fiber is better than that of copper. At a current density from 50 to 175 mA/cm2, Device III current efficiency roll-off is 18.1% while that of Device II is 21.3%, both better than Device I (roll-off is 51.3% at current density from 50 to 125 mA/cm2) (see Figure 3).

Substrate materialsThermal conductivity value (W/m*K)

Graphite fiber400~500

Using material with high thermal conductivity coefficient as the TEOLED substrate could make TEOLED devices achieve better luminous characteristics. At the same time it could also dissipate the heat, removing the negative impact on device luminous characteristics at high voltage. The heat flow reference is defined in (1), within a setting time (); the heat () flows from the plane of a higher temperature () to the plane of a lower temperature () where is the area, the length, and the material thermal conductivity. However, (1) is specifically for the rate of heat flow for a single layer material. The OLED device is composed of two electrodes and multiple organic layers. Therefore the above equation should be replaced with (2) [11]. Consider

Comparing (3) for the current TEOLED structure, the key factors affecting the heat flow rate are the thermal conductivity (), substrate thickness (), and UV glue materials. Since the thermal conductivity of graphite is about = 400~500 W/mK, copper is about = 397 W/mK, glass is about = 1.38 W/mK, and UV glue is about = 0.5 W/mK, the rate of heat flow for TEOLED with a graphite substrate is better than that of both copper and glass substrates. Figure 4 shows the measured junction temperature and surface thermal distribution image results.

3.2. Heat Dissipation Test of TEOLED Devices

Substrate temperature tests were conducted using copper, graphite, and glass substrates on the emission area and substrate back after operating from 5 to 25 seconds. When the luminance was 3000 cd/m2 (current density of 57 mA/cm2) for the glass substrate device, the device highest temperature area was the emission area about 41.33°C as indicated in Figure 4(a). With 25-second operation the temperature increased to 65.46°C, concentrated in the emission area. When the copper substrate device was operated at 4000 cd/m2 luminance (current density of 75 mA/cm2), its back temperature was at 30.07°C as indicated in Figure 4(b). The temperature increased slightly to 32.57°C after lighting for 25 seconds. The temperature at the back of the substrate was 29.12°C when the graphite substrate component was operated at 4000 cd/2 luminance (current density of 68 mA/cm2) as indicated in Figure 4(c). The temperature increased slightly to 30.88°C after lighting for 25 seconds. When the device was emitted for a certain period the device surface was cooler than that of copper and glass. The above study result shows that the high thermal conductivity characteristics of the graphite fiber substrate could effectively dissipate the heat produced from the device during high voltage operation.

Three TOLEDs with different substrates were packaged in PET for component lifetime measurements. At 500 cd/m2 of luminance, Figure 5 shows that the glass substrate had a lifetime of only 4 hours due to poor heat dissipation. The graphite substrate component lifetime was 11.5 hours due to better cooling.

4. Conclusions

The TEOLED structure is (glass; copper; graphite) substrate/YCD91 glue/Al/Au/EHI608/TAPC/Alq3/LiF/Al/Ag. From the experimental results the graphite fiber substrate produced better luminous performance compared with the glass and copper substrate devices at luminance of 3055 cd/m2 and current efficiency of 6.11 cd/A at 50 mA/cm2. At a current density from 50 to 175 mA/cm2, Device III current efficiency roll-off was 18.1%. The substrate case back temperature was observed for different TEOLED substrates operated at several lighting periods. A glass substrate element operating from 5 to 25 seconds of luminance at 3000 cd/m2 produced a temperature rate of 1.207°C/sec. Under luminance of 4000 cd/m2 the copper and graphite substrate temperature rates were 0.125°C/sec and 0.088°C/sec. Glass, copper, and graphite comparative operating lifetimes were 4, 8.5, and 11.5 hours, respectively.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.


This work is sponsored by the Ministry of Science and Technology of Taiwan, Projects NSC99-2221-E-235-005, NSC101-2221-E-235-008, and NSC102-2221-E-150-066-MY2. Special thanks are due to Shu-Ling Yeh researcher team from Material and Chemical Research Laboratories, Industrial Technology Research Institute, for the UV glue (YCD91).


  1. M. Pope, H. P. Kallmann, and P. Magnante, “Electroluminescence in organic crystals,” The Journal of Chemical Physics, vol. 38, no. 8, pp. 2042–2043, 1963. View at: Publisher Site | Google Scholar
  2. A. Kraft, A. C. Grimsdale, and A. B. Holmes, “Electroluminescent conjugated polymers—seeing polymers in a new light,” Angewandte Chemie International Edition, vol. 37, no. 4, pp. 402–428, 1998. View at: Publisher Site | Google Scholar
  3. C. W. Tang and S. S. van Slyke, “Organic electroluminescent diodes,” Applied Physics Letters, vol. 51, no. 12, pp. 913–915, 1987. View at: Publisher Site | Google Scholar
  4. C. W. Tang, S. A. van Slyke, and C. H. Chen, “Electroluminescence of doped organic thin films,” Journal of Applied Physics, vol. 65, no. 9, pp. 3610–3616, 1989. View at: Publisher Site | Google Scholar
  5. J. J. Burroughes, D. D. C. Bradley, A. R. Brown et al., “Light-emitting diodes based on conjugated polymers,” Nature, vol. 347, pp. 539–541, 1990. View at: Publisher Site | Google Scholar
  6. G. Gustafsson, Y. Cao, G. M. Treacy, F. Klavetter, N. Colaneri, and A. J. Heeger, “Flexible light-emitting diodes made from soluble conducting polymers,” Nature, vol. 357, no. 6378, pp. 477–479, 1992. View at: Publisher Site | Google Scholar
  7. C. J. Lee, D. G. Moon, and J. I. Han, “Sports over a distance, portraits with a sense of their personal space, and telephones crossed with flotation tanks,” in Proceedings of the 3rd Workshop on Social Intelligence Design (SID '04), p. 1005, Seattle , DC, USA, May 2004. View at: Google Scholar
  8. C. C. Wu, S. D. Theiss, G. Gu et al., “Integration of organic LED's and amorphous Si TFT's onto flexible and lightweight metal foil substrates,” IEEE Electron Device Letters, vol. 18, no. 12, pp. 609–612, 1997. View at: Publisher Site | Google Scholar
  9. P. N. M. dos Anjos, H. Aziz, N.-X. Hu, and Z. D. Popovic, “Temperature dependence of electroluminescence degradation in organic light emitting devices without and with a copper phthalocyanine buffer layer,” Organic Electronics, vol. 3, no. 1, pp. 9–13, 2002. View at: Publisher Site | Google Scholar
  10. K. S. Rao and Y. N. Mohapatra, “Disentangling degradation and auto-recovery of luminescence in Alq3 based organic light emitting diodes,” Journal of Luminescence, vol. 145, pp. 793–796, 2014. View at: Publisher Site | Google Scholar
  11. Y. Tsai, S. Wang, C. Chen et al., “Using copper substrate to enhance the thermal conductivity of top-emission organic light-emitting diodes for improving the luminance efficiency and lifetime,” Applied Physics Letters, vol. 95, no. 23, Article ID 233306, 2009. View at: Publisher Site | Google Scholar

Copyright © 2014 Yu-Sheng Tsai et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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