scholarly journals Silver Nanowires Inks for Flexible Circuit on Photographic Paper Substrate

Micromachines ◽  
2018 ◽  
Vol 10 (1) ◽  
pp. 22
Author(s):  
Xing Yang ◽  
Dexi Du ◽  
Yuehui Wang ◽  
Yuzhen Zhao

Silver nanowires (AgNWs) have inspired many research interests due to their better properties in optical, electric, and flexible applications. One such exploitable use is as the electrical conductive fillers for print electronics. In this paper, AgNWs with mean a diameter of 80 nm and mean length of 13.49 μm were synthesized using the polyol solvothermal method. A sonication-induced scission process was used to obtain AgNWs with a length range of 7.64–11.21 μm. Further AgNWs inks were prepared with the as-synthesized AgNWs as conductive fillers in anhydrous ethanol. The conductive inks were coated on resin coated photographic paper substrate using the knife coating process and dried at room temperature. The effects of the number of layers of AgNWs coating, the concentration of AgNWs, and the length of AgNWs on the microstructure and electrical properties of samples were investigated by scanning electron microscopy and using the four-point probe method. The results show that the conductivity of the AgNWs coating increases with the increase in the number of layers in the AgNWs coating, concentration and length of the AgNWs.

2020 ◽  
Vol 71 (8) ◽  
pp. 136-147
Author(s):  
Junaidi ◽  
Nur Asriyani ◽  
Simon Sembiring ◽  
Posman Manurung ◽  
Sutopo Hadi

In this research, a thin film of silver nanowires (AgNWs) is made by varying the number of layers onto a polycarbonate substrate using a spray coating process. AgNWs were obtained via the polyol method using silver nitrate (AgNO3) as rare materials, Polyvinyl pyrrolidone (PVP) as a reducing agent and ethylene glycol (EG) as a solvent. The coating material used is AgNWs solution with a concentration of 10% in ethanol, which has a diameter and length of 176.13 nm and 28.58 �m, respectively. The optical conductivity for third layers were 1.80 � 105 S.m−1,1.98 � 105 S.m−1, and 2.32 � 105 S.m−1 by the gap energy of 3.84 eV, 3.81 eV, and 3.79 eV at a wavelength of 550 nm. The greater the number of layers, the higher the optical conductivity. The smaller energy gap indicates that the material absorbs more energy, so the absorbance value is higher. The sheet resistance of AgNWs thin films in variations of each layer was 119.2 Ω.sq−1, 20.6 Ω.sq−1 and 4.98 Ω.sq−1. The lower the layer resistance, the higher the density of AgNWs and the thicker the layer. Based on the SEM images by cross-section technique, the thickness of AgNWs thin films obtained by 44.244 μm, 69.126 μm, and 100.028 μm for each layer. AgNWs thin films could be used as transparent conductive electrodes for optoelectronic applications.


Author(s):  
D. S. Marotkar ◽  
P. L Zade

<span>In this paper a compact, flexible, Multiband antenna is designed. It is having flexible Substrate of photographic paper which makes the antenna conformal. The antenna with two U slots cut in radiating patch is offset fed by microstrip lines gives the multiple bands of WLAN /WIMAX Application and two parasitic Elements improves the bandwidth of a typical microstrip antenna. The Measured results shows that the antenna resonates between Frequency band 2.10-2.95 GHz, 3.35-3.54 GHz and 5.04-6.0Hz.which are used for application such as Bluetooth, Wi-Fi, Zigbee, ISM 2.4GHz,WLAN WiMAX, and WLAN 5.2GHz.</span>


Author(s):  
Kamal Sarkar

Nanochips® cartridges (Fig 1) are disposable panels with 400 micro arrays (Fig 2) that can be independently used as test sites for various assays like genetic marker. Each site (Fig 3) is a permeation layer coated electrode with 80 μ diameter and 120 μ pitch. Permeation or “perm” layer is a thin film of a proprietary hydrogel material over the proprietary chip design. Perm layers were deposited on the electrodes using spin coating process with a proprietary solution. Performance of the cartridge depended on the quality and thickness of the permeation layer over these 400 electrodes. In this process one millimeter deep tear shaped well was constructed from the ceramic base to which 20×20 array of silicon chip were attached. These wells filled with 180 μl proprietary solution and spun at fixed 1200 RPM for 20 seconds. Process was repeated three times at room temperature in a clean room. Post process treatment included 30 minutes in dry incubator, wash in Milli Q water, and finally, dry at room temperature. Quality of the 1,500 nm thick permeation layer was so demanding that more than half of the cartridges were rejected due to poor quality of the perm layer. Major causes of rejection were bubbles, high SD (Standard Deviation), and thickness (too thick or too thin) of the layer. To understand the problem focus was given to both solution making and spin coating process. Basic hypothesis was that the film thickness was based on viscosity of solution and subsequent evaporation process. Figs 4–6 showed the details of spin coating process for developing a heuristic model. Since viscosity depended strongly on the temperature and time during a chemical reaction, a viscosity profile was developed for the solution during the reaction. From the viscosity curve (Fig. 7) it was established that 75 minute at 50° C was not enough to complete the reaction as was initially thought. The time-Viscosity curve reached the plateau after 150 minutes! So, it was necessary to continue the reaction for 75 more minutes to complete the reaction. This explained a major reason (bubble forming) in the present process. Viscosity of the solution depended on a number of other factors like dispensed volume, temperature of the spinneret, time to dispense and/or in the spinneret, etc. A systematic study on these variables led to an empirical equation of the following form: Hf=Hf0+A*(τe/Vd)*ηf*(Tc−T0)n Where Hf = Predicted Average Thickness in nm. Hf0 is minimum average thickness in nm. T, V, and τ are various temperature, dispensed volume, and time parameters. A and n are curve fitting constants for experimental set-ups. The best of part of this modeling was its ability not only to predict the thickness of the film, rather its ability to control the thickness of the film in real time for a given solution. Above equation allowed appropriate dispensing volume and time to be kept in the well of the chip before spinning for a given solution with a specific viscosity. A tabular form was given to the operator who matched the information to get a specific film thickness. This model helped dropped the rejection rate to less than 10% from more than 50%. Operators were able to control the thickness of the film within 1500 nm +/− 300 nm, as demanded by the Spec. The model further allowed to target, rather control, the film thickness. We were also able to make films as thin as 800 nm or as thick as 1,500 nm with +/− 200 nm variation from the Table developed from the empirical equation. Using the assumption that viscosity plays the most important role in our spin coating process and constructing a corresponding evaporative model, we were able to identify a major shortcoming of an existing process to develop submicron thick permeation layer. Existing process was resulting in more than 50% rejection of an expensive critical component. An empirical model of spin coating process was developed to predict the film thickness within hundreds of nanometers. This dramatically improved the yield to more than 90% from less than 50%. The model allowed to correct the process in real time and allowed targeting the film thickness anywhere around one micron with few hundred nanometer accuracy.


The Analyst ◽  
2000 ◽  
Vol 125 (7) ◽  
pp. 1327-1330 ◽  
Author(s):  
Dong Chuan ◽  
Yang Pin ◽  
Yuan Wen ◽  
Shuang Shaomin

2014 ◽  
Vol 1035 ◽  
pp. 488-491
Author(s):  
Jing Jing Li ◽  
Yun Zhao ◽  
Han Sheng Li ◽  
Qin Wu ◽  
Qing Ze Jiao

Hollow nickel ferrite microspheres with a diameter of about 1.5 to 2.5 μm were synthesized using an emulsion-based solvothermal method in combination with calcination at 550°C. The structures and morphologies of the nickel ferrite microspheres were characterized using an X-ray diffractometer, a transmission electron microscopy and a field emission scanning electron microscopy. Magnetization measurement was carried out using a vibrating sample magnetometer at room temperature. The saturation magnetization and coercivity of nickel ferrite microspheres could reach 19.41 emu/g and 202.28 Oe, respectively. Hollow nickel ferrite microspheres might be used as catalysts, magnetic materials and microwave absorbers.


2010 ◽  
Vol 114 (11) ◽  
pp. 4790-4796 ◽  
Author(s):  
Xiaofang Liu ◽  
Javed Iqbal ◽  
Zhangben Wu ◽  
Bo He ◽  
Ronghai Yu

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