Open Access

Hybrid light-emitting diodes from anthracene-contained polymer and CdSe/ZnS core/shell quantum dots

Nanoscale Research Letters20149:611

https://doi.org/10.1186/1556-276X-9-611

Received: 6 June 2014

Accepted: 30 October 2014

Published: 12 November 2014

Abstract

In this paper, we added CdSe/ZnS core/shell quantum dots (QDs) into anthracene-contained polymer. The photoluminescent (PL) characteristic of polymer/QD composite film could identify the energy transitions of anthracene-contained polymer and QDs. Furthermore, the electroluminescent (EL) characteristic of hybrid LED also identifies emission peaks of blue polymer and QDs. The maximum luminescence of the device is 970 cd/m2 with 9.1 wt.% QD hybrid emitter. The maximum luminous efficiency is 2.08 cd/A for the same device.

Keywords

Light-emitting diode Efficiency Optical polymer

Background

Poly(p-phenyene vinylene) (PPV) for application in optoelectronic fields had attracted great interest [1]. The polymer has certain advantages, such like low-cost, easy procession, and large-area display over light-emitting diodes (LEDs) made from inorganic material, especially in flexible displays [2]. Somehow, polymer LED (PLED) has one characteristic that its electron-injection is more difficult than its hole-injection due to the high energy barrier for electron-injection and low electron mobility in organic polymers. Therefore, one of the most important challenges in PLEDs is to balance the charge carrier injection that is essential for high efficiency. One method of adding nanoparticles into emissive material of PLED could be a good solution. Some former study used ZnO nanoparticles to enhance the electroluminescent characteristics of green polymer LED [3], or used ZnO nanorods to improve violet electroluminescence of polymer LED [4]. Moreover, the stable white light electroluminescence could be obtained from flexibly polymer/ZnO nanorods hybrid heterojunction [5].

Recently, several kinds of II-VI and III-V group quantum dots (QDs) were reported for different applications, including bio-sensing, marking and security, energy saving, and light-emitting [69]. The quasi-bound theory was utilized to predict about photogeneration efficiency improvement on polymer-embedded nanoparticles [10]. A hybrid light-emitting diode which consisted of polymer as well as QDs blending as the emissive layer is proposed for possible optoelectronic device. Following the combination of easy processing and flexibility of polymers and exotic optical properties of QDs, the so-called polymer-quantum-dot light-emitting diodes (PQD-LEDs) with different polymer and inorganic QD materials could be a successful candidate for visible displays [11, 12].

We had reported blue electroluminescence from organic light-emitting diode with new anthracene-contained polymer. The polymer was synthesized through Suzuki coupling reaction. The electron-deficient oxadiazole and electron-rich carbazole derivatives were incorporated into the polymer for enhancing charge injection and transport. The good efficiency of LED based on anthracene-contained polymer was proved in the last study [13]. For researching in solid-state-lighting application, we add inorganic CdSe/ZnS quantum dots into anthracene-contained polymer for fabricating hybrid LED. The LEDs of single hybrid emissive layer have been fabricated and characterized in this study.

Methods

The CdSe/ZnS QDs used in this study, which had an estimated diameter of 5.2 nm. The picture of transmission electron microscope (TEM) for QDs is shown in Figure 1. The core/shell QDs were well-dispersed in toluene with a concentration of 10 mg/ml. The polymer powder was solved into toluene for preparing solution of 3 wt.% concentration. The polymer solution and QD solution were mixed together by the 9.1 wt.% QD ratio. We had tried other QD ratios. The luminance of higher ratios LEDs could not be measured. The LED consists of composite emissive film cast from mixed solution sandwiched between a cathode and an anode. The spin speeds of cast films were 2,000, 3,000, and 4,000 r/min, from which the composited LEDs were denoted as devices 1, 2, and 3. The thicknesses of composite films for these three devices were 573, 374, and 314 nm, respectively. The full device structure is shown in Figure 2. ITO film was used for anode. The 50-nm-thick poly(3,4-ethylenedioxythiophene)-poly(4-styrene sulfonate) (PEDOT:PSS) film was for hole transport purpose. Ca/Al was deposited as the cathode by thermal evaporation. The Ca/Al films utilized for cathode were 60/120-nm-thick.
Figure 1

Transmission electron microscope (TEM) picture of CdSe/ZnS quantum dots.

Figure 2

The structure of hybrid light-emitting diode.

Results and discussions

The photoluminescence (PL) measurement could be used to identify energy transition of optoelectronic semiconductor [14, 15]. The PL spectrum of polymer/QD composite film is shown in Figure 3.
Figure 3

The photoluminescence spectrum of anthracene-contained blue polymer and CdSe/ZnS quantum dots composite film.

There are two separate PL peaks. That is two energy transitions existing in polymer/QD composite film. The first energy transition is at 452-nm wavelength and lies in the region of pure blue emission. This energy transition is owing to blue anthracene-contained polymer. This blue PL peak has 42-nm full width half maximum (FWHM). The sharp FWHM means the polymer is a very high homogeneous structure. It is obviously that QDs have energy transition at 614 nm which lies in red emission region. The PL peak of QDs has 40-nm FWHM.

The current-voltage (I-V) and luminance-current (L-I) characteristics are shown in Figure 4.
Figure 4

The current-voltage ( I - V ) (a) and luminance-current ( L - I ) (b) characteristics of hybrid light-emitting diode.

It should be noticed that the devices were first biased under a moderate range to prevent the luminance degradation and voltage drift caused by overstress [16]. The threshold voltages are 26, 18, and 13 for devices, 1, 2, and 3, respectively. The thicknesses (TEMI) of polymer/QD films with spin speeds of 2,000, 3,000 and 4,000 r/min were as 573, 374, and 314 nm measured by α-step method, respectively. The polymer/QD film is thicker than pure polymer film in the same spin speed. It can be attributed to the contribution of QDs on viscosity. The threshold voltage is obviously decreased with TEMI decreasing. If the threshold voltage divided by TEMI, about 0.41 ~ 0.45 × 108 V/m would be derived. Such a high field could generate injecting of carriers into the quantum dots [17]. This field is often observed in PLEDs, and it suggests that the injection current may be limited by space charge effect or tunneling effect within polymer LED [18]. Moreover, the output luminance is also dramatically increased with TEMI increasing as seen in Figure 4b. The PLEDs have a feature of luminance characteristics. The maximum luminance can be obtained at some point of supplied current. Luminance is gradually extinct beyond that point of supplied current. The maximum luminances are 959, 705, and 472 cd/m2 at supplied current of 31.6, 42.5, and 44.2 mA for devices 1, 2 and 3, respectively.

The characteristics of luminous efficiency vs. current are shown in Figure 5. It is clearly that the efficiency is gradually decreasing beyond some maximum value even though the current injection is increasingly more. Because the polymer/QD layer is a semiconducting material, the excessive current injection turns to heat and damages the device. The maximum luminous efficiencies are 2.08, 1.25, and 0.3 cd/A for device 1, 2, and 3, respectively. The currents for maximum efficiency are 0.044, 0.018, and 0.099 mA for device 1, 2 and 3, respectively. As described before, the thicknesses of composite films for these three devices were 573, 374, and 314 nm, respectively. The electrical fields on maximum efficiency are 0.0293, 0.0291, and 0.031 V/nm for device 1, 2, and 3, respectively. The luminous efficiencies are changed with varied electrical field. The photo-generation efficiencies of the three LEDs exhibit a strong filed intensity dependency based upon quasi-bound state (QBS) theory [10].Figure 6 shows the electroluminescent (EL) spectrum of anthracene-contained blue polymer/QD hybrid LED.
Figure 5

The luminous efficiency-current characteristics of hybrid light-emitting diode.

Figure 6

The electroluminescent spectrum of hybrid light-emitting diode.

In the spectrum, three definite EL peaks can be distinguished. The peaks appear at wavelengths of 458.2, 479.3, and 615 nm. The major EL peaks, 458.2 and 479.3 nm, are attributed to electroluminescence of anthracene-contained polymer [13]. These both EL peaks belong to blue emission zone. Intensity ratio of the third peak, 615 nm, compared with major 458.2 nm is 0.25. And clearly, the third EL peak could be attributed to QD electroluminescence. The luminescence of hybrid LED is mixed by blue (458.2 and 479.3-nm peaks) and red (615-nm peak) light.

The band-diagram of hybrid LED is shown in Figure 7[19]. Blue chart is for polymer, and red chart is for QDs. As seen in Figure 7, the carriers are injected to polymer/QD layer. Some carriers cause luminescence of polymer and emit blue light. Some carriers cause luminescence of QDs and emit red light. The luminous efficiencies of hybrid LEDs decrease as compared with pure polymer LED. Even though, the EL of hybrid LED combines blue and red emissions and could have possibility for using solid-state-lighting application.
Figure 7

The band-diagram of hybrid light-emitting diode.

Conclusions

In summary, the efficient hybrid LED by using anthracene-contained blue polymer and QD composite emissive film has been demonstrated. The 959 cd/m2 of maximum luminance is obtained at supplied 31.6 mA. The maximum luminous efficiency is 2.08 cd/A at 0.044 mA of applied current. In the EL spectrum, three definite emissions can be distinguished. The peaks appear at wavelengths of 458.2, 479.3, and 615 nm. All these three EL peaks are attributed to emit from anthracene-contained blue polymer and QDs. The hybrid LED could have possibility for using solid-state-lighting application.

Declarations

Acknowledgements

We are grateful for the financial support from the National Science Council (NSC) of Taiwan under grant number of NSC 102-2221-E-268-002.

Authors’ Affiliations

(1)
Department of Electronic Engineering, Fortune Institute of Technology
(2)
Institute of Microelectronics and Department of Electrical Engineering, National Cheng Kung University
(3)
Department of Electro-Optical Engineering, Southern Taiwan University of Science and Technology

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Copyright

© Tu et al.; licensee Springer. 2014

This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.