We report the realization of a transparent display using glass covered by a nanopatterned quantum dot (QD) film with good transmittance. The film was fabricated by nanoimprint lithography (NIL) and spin coating of colloidal QDs with specificexcitation maxima. The produced nanopatterned QD film was attached to transparent glass, enabling active image generation using a laser light source of a specific wavelength. Selective light emission was induced by strongly exciting the laser-exposed film surface, creating desired images, with color modulationenabled by controlling the QD layer (dozens of nanometers in size) via nanopatterning. The nanopatterned QD film used for image generation exhibits excellent transmittance (>80%), and can be used for transparent displays, with image realization in both bright and dark spaces. The fabricated displays have wide viewing anglesowing to their good light emission characteristics, and the fabrication through spin coating renders the fabrication process simple and applicable to large areas.
The recently developed transparent displays find numerous applicationssuch as flexible displays that can be bent like paper, wearable displays1,2, and mirror displays3 that function as both mirror and screen at the same time. In these displays, the information is presented on a light-transmitting panel, creating an impression of images created on transparent glass4,5. Such displays can be divided into projection3 and transparent displays6. The former utilizes light projection on a transparent screen where an image needs to be displayed and includes head-up displays (HUDs)7,8 that project light on a screen, e.g., airplane or automobile windows, and head-mounted displays (HMDs)3 that project light directly on the human eye. In the past, HUDs were used for displaying various warplane informationnowadays, they are routinely used in automobile systems implementing augmented reality9,10. HMDs11,12 utilized in devices such as glasses or goggles project light directly on the human eye, making both the real-world image (viewed through the lenses) and the display image visible at the same time. Transparent displays function by changing the transmittance of the light-emitting display materials, and utilize either liquid crystals (LCDs)13 or organic light-emitting diodes (OLEDs)14,15. LCDs can hardly provide clear image quality outdoors, owing to their poor transmittance (~20%), which is caused by loss of light as it passes through the polarizing plate, color filter, and back light16. The development of light-emitting diodes (LED) technology inspired the realization of transparent OLED displays featuring incorporated organic semiconductors17, which are self-emissive and do not require a polarizing plate, color filter18, and back light, providing transmittances as high as 40%19. In particular, display characteristics of OLEDs, which are highly applicable in transparent displays, are still being studied. Heterostructured OLEDs based on glass substrates coated with transparent Indium Tin Oxide (ITO), which present a transparency of 70% in the visible light region, can be applied to high-resolution full-color displays or HUD display applications because the top electrode and electron injection layer are thin and transparent20,21.
The latest augmented reality displays utilize the transparent display technology to modify the front windows of airplanes, cars, and other means of transportation to display information such as the velocity and current location22,23. Three-dimensional augmented reality can be realized by complementing the real-world picture with informative images, which is currently achievedvia HUDs that simultaneously display the outside view and the corresponding driving-related information. However, it is worth noting that the transparency of such displays is still far from satisfactory. LCDs and OLEDs feature transmissions of ~20% and ~40–50%, respectively, but objects behind the substrate are not seen clearly and distinctly. Moreover, because these devices are mostly used under bright outdoor illumination, a very bright light source is needed to offset the low (4%) reflectivity of glass used in projection displays, hindering practical applications.
In this study, a nanopatterned QD film24,25 was fabricated by nanoimprint lithography (NIL) and spin coating for use in transparent displays (e.g., HUDs)26,27. The fabricated film not only allows QD emission wavelength tuning by the choice of QD dimensions, but also modulates the emission intensity via nanopatterning. The existing QD thin films neither provide adjustable coating thickness nor exhibit good QD layer uniformity28. On the contrary, our nanopatterned QD film employs a nanoscale line pattern, with the QD layer coating thickness being effectively adjusted by varying the nanopattern depth29,30. Moreover, the nanopattern surface quality could be improved by the deposition of SiO2 layers and O2 plasma treatment31. Becausethe fabricated nanopatterned QD film has a negatively charged surface,uniform QD layer deposition could be achieved by spin coating32. Moreover, single-layer deposition enabled easy and effective color modulation. When exposed to red, green, and blue lasers in the visible light range, selective light emission due to QD excitation enabled custom image generation on the nanopatterned QD film surface, and clear images were realized under bright open-air conditions. The fabricated film exhibits 80% transmittance in the entire visible light range. Thus, when it was used in transparent displays, objects on the back side of the display screen were clearly visible, and distinct images could be projected on the screen33. As for fabrication, the simple NIL and spin coating processes are cost-effective, and the wide viewing angle realized by QD excitation enables the construction of large-area displays.
Results and Discussion
As shown in Fig. 1, the nanopatterned QD film was fabricated by NIL using a QD suspension. To prepare the film, a nanoimprinting resin was dropped two or three times on the master with a pre-formed line pattern of nanosize width. Subsequently, the master was covered by a polyethylene terephthalate (PET) film, and the dropped resin was uniformly flattened using a roller. The resulting assembly was UV-cured for 90 s. The PET film was separated from the master and post-cured for 90 s, affording the nanopatterned film.
The master width pattern featured lines with a line width of 200 nm, pitch of 800 nm, and depth of 100 nm. When the nanopatterned film fabricated thus is duplicated, the resulting film exhibits a line width of 600 nm and pitch of 800 nm. In order to improve the adhesion between QDs and the film surface, a 10 nm buffering SiO2 layer was deposited at 1.0 Å/s using an E-beam evaporator. To fill the nanopattern with QDs, atmospheric plasma treatment was performed for 30 s. As the produced nanopatterned film was covered with hydroxyl groups, its surface was hydrophilic. Subsequently, green QDs were spin-coated from a toluene suspension for 1 min at 4000 rpm (see in Supplementary Figure S1). In the next step, the deposition of the 10 nm SiO2 layer and atmospheric plasma treatment were repeated to improve surface adhesion, followed by spin coating red QDs. The fabricated nanopatterned QD film consisted of sequential layers of green QDs, SiO2, and red QDs, counting from the bottom. Apart from this, to further enhance the efficiency, further QD and SiO2 layers were added to fabricate a double green/red QD layer structure used for characteristic analysis and application.
To examine the properties of the fabricated nanopatterned QD film, afocused ion beam (FIB; Helios NanoLab,FEI, Netherlands) technique was used for surface analysis. Figure 2 shows the Focus Ion Beam (FIB) analysis results for a layer section of the fabricated nanopatterned QD film. Figure 2a–d show the untreated nanopatterned QD film layer, and Fig. 2e–h show the nanopatterned QD film layer subjected to O2 plasma treatment. The analyzed pattern features a line width of 200 nm, pitch of 800 nm, and depth of 100 nm (Fig. 2b,f). When this pattern was duplicated to create another pattern in the reverse direction, a line width of 600 nm, pitch of 800 nm, and depth of 100 nm were obtained. For the duplicated nanopatterned film (Fig. 2c,g) with these dimensions, the double coating layer was fabricated as in Fig. 1j (Fig. 2d,h). As a result, similar to the film with an untreated QD layer surface (Fig. 2a–d), the filmfabricated by spin coating exhibited serious QD aggregation (Fig. 2b–d), with the QD layer coating being non-uniform because QDs were not filled in the pattern.
However, the nanopatterned film treated with O2 plasma to improve the QD filmdeposition was negatively charged, providing a hydrophilic surface.
In addition, during the plasma treatment, –OH groups are formed on the surface,which increasesthe particle adherence. In addition,XPS data shown in supplementary Figure S2 also reveals the higher intensity of the binding energy of the SiO2 layer34. Therefore, the deposition parameters were improved, resulting in better surface adhesion during spin coating and thereby enabling the pattern to be easily filled by the QD suspension.
As a result, a uniform QD layer was formed on the atmospheric plasma–treated patterned surface covered by SiO2 (Fig. 2e–h). In addition, a uniform 10 nm SiO2 layer was formed between the nanopatterned QD film surface and green and red QD layers, reducing QD aggregation, as manifested by the uniform coating observed in Fig. 2e–h.
The characteristics of the fabricated nanopatterned QD films vary according to the nanopattern size and number of spin coating cycles, as evidenced by the photoluminescence (PL) spectra of these films. Figure 3a shows a Flatted single and double layer nanopatterned QD film subjected to FIB analysis (Fig. 2a,e), revealing that the highest intensities of the green and red peaks were obtained at 513 and 625 nm, respectively. The maximum PL intensity was observed in a Flatted double layer nanopatterned QD film with a large pattern size (Fig. 2e), and a relatively low PL intensity was observed in the film shown in single layer nanopatterned QD film (Fig. 2a). Fig. 3b is the result of PL properties of line width of 600 nm, pitch of 800 nm and depth of 100 nm (Fig. 2g) and PL properties of line width of 200 nm, pitch of 800 nm and depth of 100 nm (Fig. 2f). This can be rationalized by the fact that more QDs fill a larger nanopattern space, resulting in a two times higher PL intensity of the film (Fig. 2g), compared to Fig. 2f, for the pattern with a line width of 600 nm, pitch of 800 nm and depth of 100 nm in Fig. 3b.
Thus, the PL intensity of each QD layer could be adjusted, because the thickness and width of these layers can be tuned by varying the size and depth of the nanopattern. Thus, the color of red and green QDs used in this experiment can also be adjusted. To confirm the improvement in the nanopatterned QD film intensity, we attempted to characterize the multiple-deposited layer by measuring the PL propertiesof green and red QD films deposited as single layers and as a double layer on a nanopatterned QD film, where each QD layer was deposited twice. PL measurements (Fig. 3c) were conducted for nanopatterned QD films examined by FIB (Fig. 2g,h). Therefore, we deposited a larger number of QD layers on the fabricated nanopatterned film to improve its characteristics, achieving higher intensity and uniform coating. The double-layered nanopatterned QD film shows a 75% increase in the PL intensity for both green and red QDs, indicating considerable improvement. According to the size and depth of the nanopattern, the QD layer thickness could be adjusted in the range of dozens to hundreds of nm, and QD films with higher PL intensity could be fabricated by sequential deposition of additional layers over the double layer. If several QD layers are added, various colors could be realized, enabling full-color tuning and hologram applications, subject to blue color implementation.
The viewing angle is one of the important aspects, now being implemented in large-area displays, although it was not implementedbefore in transparent displays or is not found in existing displays. In addition to the display, many applications are required to provide accurate images from various angles to the observer. The developed nanopatterned QDs film can be used for both indoor and outdoor light interference using a laser light source. This is owing to the strong excitation of the QDsat certain wavelengths, and this property is very favorable in terms of the viewing angle (Supplementary Figure S5). However, since the laser source is a very intense light source, power control of the intensity is required (Tables S1, S2) and the location of the laser source needs to be altered such that it is not projected directly onto the eyes of the viewer (Supplementary Figure S6(d–f)). Therefore, in this study, the intensity was identified by controlling the viewing angle of the laser source on the nanopatterned QD film.
Figure 4a shows the measured intensity of the nanopatterned QD film according to the angle of incidence of the laser, using the most efficient PL emission from Fig. 3b–c. In order to measure a wide range of incident angles, the nanopatterned QD film was placed in front a back plate capable of measuring 25 to 85°, and a multi-wavelength xenon lamp was set at a wavelength of 405 nm for excitation. The xenon lamp and PL detector were fixed at 90° with respect to each other and the angle of the back plate was adjusted. Subsequently, the light from the incident xenon lamp was directed on the nanopatterned film, and the QD PL was measured by the PL detector. The angle of incidence of the xenon light on the film shown in Fig. 4b is 25° to85°. When the θ value was 45°, the PL intensity of the double nanopatterned QD film was the highest. The PL intensitydecreased upon increasing or decreasing the θ value, and the same tendency was also observed for the single nanopatterned QD film shown in Fig. 4c. These results were obtained by fitting the peak values of the PL intensities measured according to the incident angles and their distributions are shown in Fig. 4d.
Thus, multiple QD layers were spin-coated on the nanopatterned film fabricated by NIL to produce the nanopatterned QD film, whose transmittance was measured to verify its utility in transparent displays. Figure 5a displays the transmittance of each nanopatterned QD film fabricated by spin coating, with the transmittance of the PET film taken as the reference. Figure 5a(i–v) show the nanopatterned PET films with the pattern size and structure corresponding to those in Fig. 5b. Figure 5a(i) depicts a nanopatterned PET film with no deposited QDs, Fig. 5a(ii) shows a single green QD layer film, Fig. 5a(iii) displays a single red QD layer film, and Fig. 5a(iv–v) exhibit the single and double QD films characterized in Fig. 5b, respectively. Five types of films were examined in total. As a result, transmittances of 88 and >92% were observed at 400 and >500 nm, respectively (Fig. 5a(i)), with the corresponding values for Fig. 5a(ii),(iii) being equal to 80 and 95%. In Fig. 5a(iv), transmittances of 83 and >90% at 400 and >500 nm were observed, respectively. Finally, transmittances of 85 and >94% at 400 and >500 nm, respectively were observed in Fig. 5a(v). Thus, all the QD filmsshowed transmittances exceeding those of the existing transparent displays (40%) by more than a factor of two at all visible light wavelengths. Figure 5b shows a transmitted image of the measured film, and Fig. 5b(i–v) show the background image of the transmitted film. Figures 5b(i–1) to 5b(v–1) show films excited by UV light at 365 nm, revealing that the color as well as the background images could be observedin these films.
We used a blue LED with a wavelength of 450 nm and a blue laser source with a wavelength of 405 nm to generate the image on the fabricated nanopatterned QD film. However, the blue LED driven by the low current had a very low power output and its wavelength (450 nm) is higher than that of the laser (405 nm). Therefore, the excitation efficiency of the QD was low. It was also unsuitable as a source for creatingimages on the nanopatterned QD films because the LED light spreads widely (see in Supplementary Figure S3, Table S1). On the contrary, the laser source could create images on the nanopatterned QD film, but the power of the projected laser was very high, causing damage to the skin or eyes. Therefore, in this study, a module using a 1k ohm potentiometer was fabricated and a power output test was performed for the405 nm blue laser source (see in Supplementary Figure S3). Finally, to minimize damage to the human body, the experiment was performed using 225 mW laser power with 90 mA applied at 2.5 V (see in Supplementary Table S2).
As shown in Fig. 6a(i), a “KIMM KU” image was projected onto the surface of a nanopatterned QD film attached to transparent glass using a laser module to examine the applicability of this film to transparent displays. Three 12 × 12 cm2 nanopatterned QD filmpieces were used for this experiment. As shown in Fig. 6a(ii), a shadow mask was used to create an image in front of the laser source, and an excited image was obtained on the nanopatterned QD film attached to transparent glass (see in Supplementary Figure S5). As for Fig. 6a(iii,iv,v) “KIMM KU”R (iii), G (iv), B (v) image presented respectively on transparent glass using a 405 nm laser source and shadow mask. And Fig. 6a(vi) which is 36 cm × 12 cm2 showed a large area image. As shown in Fig. 6b, exposure of the nanopatterned QD film to laser radiation resulted in QD excitation and projection of the KIMM KU image (Fig. 6b(i)). Figure 6b(i) is an experiment using laser module. Focusing the camera on the background situated 5 m behind produced a clear projection of the KIMM KU image in outdoor on the nanopatterned QD film (Fig. 6b(ii)). However, the laser light simply passed throughthe transparent glass with no nanopatterned QD film attached, and no image was projected (Fig. 6b(iii,iv)). Moreover, the experimental result shown in Fig. 6b reveals that the image is projected on the nanopatterned QD film attached on the transparent glass (Fig. 6b(iii–1, iv–1)), with the same result obtained by focusing the camera on the background situated 5 m behind (Fig. 6b(iii–2, iv–2)). Further, KIMM KU image on transparent glass inside a car using a laser module is also presented (see in Supplementary Figure S5). The experimental setup and related processes are described in detail in the Supplementary Information.
In summary, a nanopatterned QD film for transparent displays was fabricated by spincoating QDs on a nanopatterned film. Additionally, two nanopattern types were formed on the QD film to improve its characteristics, corresponding to line widths of 200 and 600 nm with the pitch and depth being same at 800 and 100 nm. The QD coating thickness could be effectively increased by varying the line width and depth of the used pattern. Moreover, the QD filmcolor could be adjusted by repeated coating of the QD layers, and the problem associated with QD aggregation was overcome by depositing SiO2 layers between each QD layer and the nanopattern. The fabricated nanopatterned QD film showed an average transmittance of >80%, exceeding the transmittances of existing transparent displays (40%) more than two-fold. Tests in indoor and outdoor spaces revealed that any image could be realized, irrespective of the location and background light, even in places where interference of lightexisted. The produced film minimizes light loss, which is the main limitation of transparent displays, and can be implemented in various applications, representing a next-generation display technology that can enable the realization of any image, even in spaces exposed to visible light.
Core/shellCdSe/ZnS quantum dots manufactured by Uniam. Co., Ltd. were utilized in the form of a toluene suspension (10 mg/mL). The red-emitting CdSe inner core has a thickness of 4 nm, and the total diameter (including ZnS in the outer core) equals 10 ± 1 nm. The green-emitting CdSe inner core is 3 nm thick, with the total outer diameter being 10 ± 1 nm. PLmaxima for red and green QDs were observed at 513 and 625 nm, respectively. The nanopattern duplicated by the nanoline master was produced on a polyurethane series UV resin fabricated by combining OH and NCO monomers. For this, a UV resin, MINS-311RM (Minuta Co., Ltd.) was used. A 0.1 T PET film was used as a substrate owing to its good flexibility and transmittance.
The line master with several nanosizedline patterns used to fabricate the nanopatterned film was ultrasonicated in a Nano-Strip solution for 30 min and sequentially washed with acetone, ethanol, and isopropyl alcohol, followed by blow-drying with a nitrogen gun. The dried line master was subjected to 30 min anti-adhesion treatment in a furnace at 80 °C to obtain self-assembled monolayers for reducing the surface temperature during imprinting. The nanopatterned film fabricated by NIL was UV-cured for 90 s. After separating the duplicated nanopatterned film from the master, it was post-cured for 90 s. To prevent the aggregation of green and red QDs, a buffering 100 Å SiO2 layer was deposited using an E-beam evaporator. O2 plasma treatment was performed for 30 s to improve the surface energy of the quantum dots layer during spin coating, rendering the SiO2 layer negatively charged and hydrophilic.
PL spectra of the nanopatterned QD films were recorded using a UV-Vis Fourier transform near infrared fluorescence spectrometer (FS-2, Scinco Co., Ltd.). A 5 × 5 mm2 area of the nanopatterned QD film was used for measurements, and QD emission was monitored every second. A Photo Multiplier Tube voltage of 450 V and an integration time of 20 ms were used. The values of the emission filter and excitation filter were setup by air condition, with the emission start and end measured at 450 and 720 nm, respectively. In addition, an analyzer-type UV-Vis spectrophotometer (S-3100, Scinco Co., Ltd.) was used to measure the transmittance. Transmittance of the 0.1-T PET film was first recorded as a reference, and then the transmittance of each sample film was analyzed. To realize images on the fabricated nanopatterned QD film, two types of lasers were used in addition to a laser module (wavelengths: red, 638 nm; green, 532 nm; blue, 445 nm and laserpower: red, 300 mW; green, 150 mW; blue, 600 mW), which can be applied for red, green, and blue colors, and a 405-nm laser source power (max: 500 mW, min: 130.5 mW)35,36,37,38,39.
Hu, L., Kim, H. S., Lee, J. Y., Peumans, P. & Cui, Y. Scalable Coating and Properties of Transparent, Flexible, Silver Nanowire Electrodes. ACSNano 4(5), 2955–2963 (2010).
Di, J. et al. Carbon-Nanotube Fibers for Wearable Devices and Smart Textiles. Adv. Materials 28, 10529–10538 (2016).
Sharples, S., Cobb, S., Moody, A. & Wilson, J. R. Virtual Reality Induced Symptoms and Effects (VRISE): Comparison of Head Mounted Display (HMD), Desktop and Projection Display Systems. Displays 29, 58–69 (2008).
Ko, Y. C. et al. Eye-Type Scanning Mirror With Dual Vertical Combs for Laser Display. Sens. Actuators A: Phys 126, 218–226 (2006).
Hsu, C. W. et al. Transparent Displays Enabled by Resonant Nanoparticle Scattering.Lasers and Electro-Optics (CLEO), 2014 Conference on. IEEE, (2014).
Park, S. H. et al. Transparent and Photo‐stable ZnO Thin‐film Transistors to Drive an Active Matrix Organic‐Light‐Emitting‐Diode Display Panel. Advanced Materials 21(6), 678–682 (2009).
Lee, J. Y., Kim, H. J. & Kim, Y.-J. Design and Fabrication of Semi-Transparent Screen Based on Micropatterns for Direct-View Type Head-Up Display in Automobiles. OpticalReview 23, 133–140 (2016).
Fan, C. & He, S. Micromirror based virtual image automotive head-up display. Microsystem Technologies 23(6), 1671–1676 (2017).
Chi, Y. Improvement of the blue-color quenching and optical efficiency of laser for the head-up display. Journal of Information Display 18(1), 41–47 (2017).
Soomro, S. R. & Urey, H. Light-efficient augmented reality 3D display using highly transparent retro-reflective screen. Applied Optics 56(22), 6108–6113 (2017).
Rolland, J. P., Hong, H. Head-mounted display systems. Encyclopedia of optical engineering, 1–13 (2005).
Laramee, R. S. & Ware, C. Rivalry and interference with a head-mounted display. ACM Transactions on Computer-Human Interaction 9(3), 238–251 (2002).
Fan, C. S. & Li, K. C. Production of Insulating Glass Ceramics From Thin Film Transistor-Liquid-Crystal Display (TFT-LCD) Waste Glass and Calcium Fluoride Sludge. J. Cleaner Prod 57, 335–341 (2013).
Tagaya, A., Nagai, M., Koike, Y. & Yokoyama, K. Thin Liquid-Crystal Display Backlight System With Highly Scattering Optical TransmissionPolymers. Appl. Optics 40, 6274–6280 (2001).
Sun, J. W. et al. A Fluorescent Organic Light-Emitting Diode With 30% External Quantum Efficiency. AdvancedMaterials 26, 5684–5688 (2014).
Su, C. W., Liao, C. C. & Chen, M. Y. Color Transparent Display Using Polymer-Dispersed Liquid Crystal. Journal of Display Technology 12, 31–34 (2016).
Greiner, M. T. & Lu, Z. H. Thin-Film Metal Oxides in Organic Semiconductor Devices: Their Electronic Structures, Work Functions and Interfaces. NPG Asia Materials 5, e55 (2013).
Mazulquim, D. et al. In Frontiers in Optics, Optical Society of America, FTh3D-7 (2014).
Lee, J. et al. Deep Blue Phosphorescent Organic Light-Emitting Diodes With Very High Brightness and Efficiency. NatureMaterials 15, 92–98 (2015).
Zulkifli, Z. et al. Highly. Transparent and Conducting C:ZnO Thin Film for Field EmissionDisplays. RSC Advances 4(110), 64763–64770 (2014).
Gu, G., Bulović, V., Burrows, P. E., Forrest, S. R. & Thompson, M. E. Transparent Organic Light-Emitting Devices. Applied Physics Letters 68, 2606–2608 (1996).
Sánchez, J. A. et al. In corporation of Head-Up Display Devices in Real-Vehicular Environments to Improve Efficiency in Driving. In Proceedings of the XVII International Conference on Human Computer Interaction 10 (2016).
Bulovic, V., Gu, G., Burrows, P. E., Forrest, S. R. & Thompson, M. E. Transparent light-emitting devices. Nature 380(6569), 29 (1996).
Kim, H. J. et al. Enhancement of Optical Efficiency in White OLED Display Using the Patterned Photoresist Film Dispersed With Quantum Dot Nanocrystals. Journal of Display Technology 12, 526–531 (2016).
Park, J. S. et al. Alternative Patterning Process for Realization of Large-Area, Full-Color, Active Quantum Dot Display. Nano Letters 16, 6946–6953 (2016).
Munshi, A. M. et al. Position-Controlled Uniform GaAs Nanowires on Silicon Using Nanoimprint Lithography. Nano Letters 14, 960–966 (2014).
Kim, L. et al. Contact Printing of Quantum Dot Light-Emitting Devices. Nano Letters 8, 4513–4517 (2008).
Song, J. H., Atay, T., Shi, S., Urabe, H. & Nurmikko, A. V. Large Enhancement of Fluorescence Efficiency from CdSe/ZnS Quantum Dots Induced by Resonant Coupling to Spatially Controlled Surface Plasmons. Nano Letters 5(8), 1557–1561 (2005).
Kim, T. H. et al. Full-Color Quantum Dot Displays Fabricated by Transfer Printing. Nature photonics 5, 176–182 (2011).
Biswas, S., Brinkmann, F., Hirtz, M. & Fuchs, H. Patterning of quantum dots by dip-pen and polymer pen nanolithography. Nanofabrication 2, 19–26 (2015).
Fu, G. et al. Optical Excitation and Emission Processes of Si-QD/SiO Multilayer Films With Different SiO Layer Thicknesses. Applied Physics A 114, 861–866 (2014).
Bao, J. & Bawendi, M. G. A Colloidal Quantum Dot Spectrometer. Nature 523(7558), 67 (2015).
Oh, Y. S. et al. Direct Micro/Nano Patterning of Multiple Colored Quantum Dots by Large Area and Multilayer Imprinting. The Journal of Physical Chemistry C 116(21), 11728–11733 (2012).
Nagashio, K., Yamashita, T., Nishimura, T., Kita, K. & Toriumi, A. Electrical Transport Properties of Graphene on SiO2 with Specific Surface Structures. Journal of Applied Physics 110(2), 024513 (2011).
Jang, E. et al. White-Light-Emitting Diodes With Quantum Dot Color Converters for Display Backlights. Advanced Materials 22, 3076–3080 (2010).
Uoyama, H., Goushi, K., Shizu, K., Nomura, H. & Adachi, C. Highly Efficient Organic Light-Emitting Diodes From Delayed Fluorescence. Nature 492(7428), 234 (2012).
Gong, X. et al. Highly Efficient Quantum Dot Near-Infrared Light-Emitting Diodes. Nature Photonics 10(4), 253–257 (2016).
Otnes, G. et al. Strategies to Obtain Pattern Fidelity in Nanowire Growth From Large-Area Surfaces Patterned Using Nanoimprint Lithography. Nano Research 9, 2852–2861 (2016).
Choi, H. J., Choo, S., Shin, J. H., Kim, K. I. & Lee, H. Fabrication of Superhydrophobic and Oleophobic Surfaces with Overhang Structure by Reverse Nanoimprint Lithography. Journal of Physical ChemistryC 117, 24354–24359 (2013).
This work was supported by the Center for Advanced Meta-Materials (CAMM) funded by the Ministry of Science, ICT and Future Planning as Global Frontier Project (CAMM- No. 2014M3A6B3063707) and by the Industrial Strategic technology development program (10052641) funded by the Ministry of Trade, Industry & Energy (MI, Korea).and by the Industrial Strategic Technology Development Program [10045269, Development of Soluble TFT and Pixel Formation Materials/Process Technologies for AMOLED TV] funded by MOTIE/KEIT.
The authors declare that they have no competing interests.
Publisher's note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Electronic supplementary material
About this article
Cite this article
Shin, Sh., Hwang, B., Zhao, ZJ. et al. Transparent Displays Utilizing Nanopatterned Quantum Dot Films. Sci Rep 8, 2463 (2018). https://doi.org/10.1038/s41598-018-20869-1
Science Advances (2020)
Development of tuneable green-to-red emitting transparent film based on Nafion with TbIII/EuIII β-diketonate complexes modulated by pH and proton flow
Materials Advances (2020)
Science China Materials (2020)
The Journal of Physical Chemistry C (2020)
Controlling fluorescence of a nano-Al2O3 film enabled by CdSe quantum dots on CdSe/Al2O3 heterojunctions
Journal of Luminescence (2019)