这项工作是部分被格兰特 - 在援助科学研究（24225003号）的支持。这项工作是由JX新日本石油和能源公司资助。

1.活动层溶液的制备<ol><li> 对于胺掺杂PFD设备的有源层解决方案 注:PFD，4,4&#39;，4&#39;&#39; -三[2-萘基（苯基）氨基]三苯基胺（2-TNATA），9,9-二甲基-N，N&#39; -二（1-萘基） - N ，N&#39;-二苯基-9H-芴-2,7-二胺（DMFL-NPB），聚（环氧乙烷）（PEO），被原样使用。钾酯（K 2 CF 3 SO 3）的混合物在200℃下真空干燥，使用前1小时。 <ol><li>对于具有PFD的设备:1胺比:0.25，溶解10毫克的PFD和在1毫升氯仿中2.5毫克的芳香族胺中，并在40℃下搅拌1小时。对于那些具有PFD:1胺:1的比例，用10毫克的芳香胺。 </li><li>另外，将溶解10毫克的PEO在1ml环己酮，并在60℃下搅拌1小时，并溶解2.5毫克的钾三氟甲烷磺酸（KCF 3 SO 3）在1毫升环己酮中并搅拌在40℃1小时。 </li><li>添加0.78毫升PEO的溶液和0.147毫升所述KCF 3 SO 3溶液，使用微量PFD的溶液。搅拌4小时，在40℃的混合溶液中。 </li><li>筛选使用旋转涂布之前的膜过滤器的混合溶液中。 </li></ol></li><li> 对于未掺杂PFD设备有源层解决方案 <ol><li>对于未掺杂的PFD装置中，溶解10毫克PFD的在1毫升氯仿中，并搅拌，在40℃1小时。随后的步骤是相同的​​那些1.1.2胺掺杂的工艺流程图先前描述 - 1.1.4。 </li></ol></li></ol> 2. LEC器件的制造注:LEC器件的制造过程总结于图1中 。 <ol><li>超声清洁图案化氧化铟锡（ITO）玻璃用稀洗涤剂基质，接着离子水，丙酮和2-丙醇用台式超声浴（38千赫）下3分钟为每一个步骤。最后，删除使用N 2鼓风机溶剂。 </li><li>治疗用UV / O 3的基片，使用的UV / O 3，根据制造商的协议处理单元3分钟。在惰性气氛下进行，在手套箱中的活性层涂覆过程。 </li><li>设置于旋涂器的头部的清洗衬底。分配大约100微升使用微量有源层溶液。旋转该衬底，如下所示:800转60秒，增加的速率1000转以上3秒，然后以1000rpm旋转10秒。有源层厚度将大约150纳米。 </li><li>干燥在手套箱过夜涂覆的基材。 </li><li>擦去过量的聚合物，以确保正确的电极连接和封装。 </li><li>放置在基板上的铝沉积的蒸发支架。装载在蒸发腔室中的保持器，并且热沉积的铝100nm的层在通过一个不锈钢蒸发掩模0.4纳米/秒的蒸镀速率，它有3毫米淀积铝反电极宽的开口。 </li><li>当沉积完成时，传送在惰性气氛下的设备的手套箱。在使用分配器的矩形的形状应用UV固化环氧树脂的珠粒。放置的盖玻璃（15毫米×12毫米×厚0.7mm）在树脂封装装置（参见图1）。 </li><li>固化用树脂的紫外辐射（累积剂量:6000毫焦/厘米2，波长:365纳米）从UV-LED光源。 </li></ol> 3.表征<ol><li> JVL测量 注意:电流密度（J） - 电压（V）的-luminance（L）使用配备有直流电压电流源监视器的光谱光检测器进行测定（JVL）特性和委员会国际歌DE L&#39;Eclairage（CIE）坐标。该测量系统是由一个控制PC与数据采集自定义的控制软件。该系统进行校准以下制造商的方案，并在一个黑色的帘在黑暗中进行的测量。 <ol><li>终端连接到设备的鳄鱼夹的联系人。放置设备上的测量载台。 </li><li>运行数据采集控制软件。该系统控制随着时间的推移所施加的电压和电流，并通过光纤收集由分光计的发射光谱。 </li></ol></li></ol>

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B., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Light-emitting+electrochemical+cells:+recent+progress+and+future+prospects.">Light-emitting electrochemical cells: recent progress and future prospects.</a> Mater. Today. 17 (5), 217-223 (2014).</li><li>Edman, L., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Single-component+light-emitting+electrochemical+cell+fabricated+from+cationic+polyfluorene:+Effect+of+film+morphology+on+device+performance.">Single-component light-emitting electrochemical cell fabricated from cationic polyfluorene: Effect of film morphology on device performance.</a> J. Appl. 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Iterfaces. 7 (46), 25955-25960 (2015).</li><li>Nishikitani, Y., Takizawa, D., Nishide, H., Uchida, S., Nishimura, S. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=White+Polymer+Light-Emitting+Electrochemical+Cells+Fabricated+Using+Energy+Donor+and+Acceptor+Fluorescent+&#960;-Conjugated+Polymers+Based+on+Concepts+of+Band-Structure+Engineering.">White Polymer Light-Emitting Electrochemical Cells Fabricated Using Energy Donor and Acceptor Fluorescent &#960;-Conjugated Polymers Based on Concepts of Band-Structure Engineering.</a> J. Phys. Chem. C. 119 (52), 28701-28710 (2015).</li><li>Sun, M., Zhong, C., Li, F., Cao, Y., Pei, Q. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+Fluorene&#8722;+Oxadiazole+Copolymer+for+White+Light-Emitting+Electrochemical+Cells.">A Fluorene&#8722; Oxadiazole Copolymer for White Light-Emitting Electrochemical Cells.</a> Macromolecules. 43 (4), 1714-1718 (2010).</li><li>Tang, S., Pan, J., Buchholz, H., Edman, L. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=White+Light-Emitting+Electrochemical+Cell.">White Light-Emitting Electrochemical Cell.</a> ACS Appl. Mater. Interfaces. 3 (9), 3384-3388 (2011).</li><li>Tang, S., Pan, J., Buchholz, H. A., Edman, L. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=White+light+from+a+single-emitter+light-emitting+electrochemical+cell.">White light from a single-emitter light-emitting electrochemical cell.</a> J. Am. Chem. Soc. 135 (9), 3647-3652 (2013).</li><li>Nishikitani, Y., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=White+polymer+light-emitting+electrochemical+cells+using+emission+from+exciplexes+with+long+intermolecular+distances+formed+between+polyfluorene+and+&#960;-conjugated+amine+molecules.">White polymer light-emitting electrochemical cells using emission from exciplexes with long intermolecular distances formed between polyfluorene and &#960;-conjugated amine molecules.</a> J. Appl. Phys. 118 (22), 225501 (2015).</li><li>Tang, S., Mindemark, J., Araujo, C. M. 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The authors have nothing to disclose.

该LEC具有包含疏水PFD和芳族胺，和亲水聚环氧乙烷和KCF 3 SO 3的有源层。因为这些材料具有非常不同的溶解度，旋涂溶液的精心准备是关键的，以避免不完全溶解。每个必须首先在有足够的溶解能力的，则该溶液被混合在一起以形成均匀的混合物的溶剂分别和完全溶解。平衡激子和激基复合物的排放量是关键，获得白光发射。因此，PFD和胺的量必须精确测量。 ...

Research and development of polymer light-emitting electrochemical cells (PLECs) have expanded in recent years.1-15 PLECs are similar to organic light-emitting diodes (OLEDs) in that both are surface emitting organic devices and are expected to find their way into future lighting applications. OLEDs are already on the market, but the cost is still high, one reason being that OLEDs need a complicated device structure with multiple layers. In contrast, PLECs have a very simple device structure which consists of a single active layer (emitting layer) between a pair of electrodes. This means that PLECs are suited to mass production processes such as roll-to-roll printing and coating. 
A PLEC has an active layer consisting of a fluorescent &#960;-conjugated polymer (FCP). The FCP can be electrochemically doped with a polymer electrolyte (a mixture of an ion conducting polymer and a salt). The FCP is p-doped on the anode side and n-doped on the cathode side during operation, and generates excitons which emit light between the p- and n-doped regions. Therefore, the emission color reflects the exciton emission (=fluorescence) wavelength of the FCP.
Stable white light emission is important for lighting applications, and color mixing techniques which employ two or more emitters have been widely used to achieve this.10-14 Recently, we presented a different approach for obtaining stable white light emission, using an active layer which contains blue-fluorescent poly(9,9-di-n-dodecylfluorenyl-2,7-diyl) (PFD) and &#960;-conjugated aromatic amines15. This white light emission comes from exciplexes formed between PFD and amine molecules in excited states. Exciplex emission has a broader spectrum compared to the exciton emission from the PDF and/or amines, which gives it a color close to that of natural light. This translates to a higher color rendering index (CRI), which is preferable for lighting applications.
In this article, the authors describe the procedure used to fabricate the exciplex based LECs and show the stability of their white light emission.

<table border="0" cellpadding="0" cellspacing="0" width="734">
	<tbody>
		<tr height="21">
			<td height="21" style="height:21px;width:332px;">Poly(9,9-di-n-dodecylfluorenyl-2,7-diyl) (PFD)</td>
			<td style="width:99px;">Aldrich</td>
			<td style="width:115px;">571660</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="63">
			<td height="63" style="height:63px;width:332px;">4,4&#8217;,4&#8217;&#8217;-Tris[2-naphthyl(phenyl)amino]triphenylamine (2-TNATA)</td>
			<td style="width:99px;">Aldrich</td>
			<td style="width:115px;">768669</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">9,9-Dimethyl-N,N&#8217;-di(1-naphthyl)-N,N&#8217;-diphenyl-9H-fluorene-2,7-diamine (DMFL-NPB)</td>
			<td style="width:99px;">Aldrich</td>
			<td style="width:115px;"></td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="21">
			<td height="21" style="height:21px;width:332px;">Poly(ethylene oxide) (PEO)</td>
			<td style="width:99px;">Aldrich</td>
			<td style="width:115px;">182028</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">Potassium tirifluoromethansulfonate (KCF3SO3)</td>
			<td style="width:99px;">Aldrich</td>
			<td style="width:115px;">422843</td>
			<td style="width:189px;">dried under vacuum at 200 &#176;C for 2 hr prior to use</td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">Chloroform</td>
			<td style="width:99px;">Kanto Chemical Co.</td>
			<td style="width:115px;">08097-25</td>
			<td style="width:189px;">dehydrated</td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">Cyclohexanone</td>
			<td style="width:99px;">Kanto Chemical Co.</td>
			<td style="width:115px;">07555-00</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">SCAT 20-X (detergent)</td>
			<td style="width:99px;">Daiichi Kogyo Seiyaku</td>
			<td style="width:115px;"></td>
			<td style="width:189px;">diluted with water</td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">Acetone</td>
			<td style="width:99px;">Kanto Chemical Co.</td>
			<td style="width:115px;">01866-25</td>
			<td style="width:189px;">Electronic grage</td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">2-propanol</td>
			<td style="width:99px;">Kanto Chemical Co.</td>
			<td style="width:115px;">32439-75</td>
			<td style="width:189px;">Electronic grage</td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">13mm GD/X Disposable Filter Device PVDF Filter Media, Polypropylene Housing</td>
			<td style="width:99px;">Whatman</td>
			<td style="width:115px;">6872-1304</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">UV/O3 Treating Unit</td>
			<td style="width:99px;">SEN Lights Co.&#160;</td>
			<td style="width:115px;">SSP16-110</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="42">
			<td height="42" style="height:42px;width:332px;">Spectral Photo Detector</td>
			<td style="width:99px;">Otsuka Electronics</td>
			<td style="width:115px;">MCPD 9800</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="21">
			<td height="21" style="height:21px;width:332px;">Voltage Current Source Monitor</td>
			<td style="width:99px;">&#160;ADCMT</td>
			<td style="width:115px;">6241A&#160;</td>
			<td style="width:189px;"></td>
		</tr>
		<tr height="168">
			<td height="168" style="height:168px;width:332px;">Evaporation Mask</td>
			<td style="width:99px;">&#160;Tokyo Process Service Co., Ltd.</td>
			<td style="width:115px;">NA</td>
			<td style="width:189px;">The evaporation mask was wet-etched to create openings for patterned deposition of aluminum. The size of the mask is 100 mm x 100 mm x 0.2 mm-thick.</td>
		</tr>
	</tbody>
</table>

fabrication of white light-emitting electrochemical cells with stable emission from exciplexes

作者提出的用于制造由高分子发光电化学电池具有其由蓝色荧光的聚（9,9-二正dodecylfluorenyl -2,7-二基）的活性层稳定的白光发射（PLECS）的方法（ PFD）和π共轭三苯基胺的分子。这种白光发射从电子激发态PFD和胺之间形成激发络合物起源。含有PFD，4,4&#39;，4&#39;&#39;装置-三[2-萘基（苯基）氨基]三苯基胺（2-TNATA），聚（环氧乙烷）和K 2 CF 3 SO 3显示白色发光用委员会国际歌DE L&#39;éclairage（CIE）坐标的（0.33，0.43）和以3.5 V恒定电压测量的施加电压为Ra = 73的显色指数（CRI）表明，在CIE的（0.27，0.37）中，Ra的坐标67，及5V的施加电压后立即观察到的发光颜色几乎不变，后稳定300秒。

电致发光（EL）光谱用来计算CIE坐标和CRI值（ 图2,4，5）。收集发射器件的拍摄图像来验证发射（ 图3）的白度。 胺掺杂PFD设备和未掺杂的PFD器件的EL光谱示于图2。未掺杂的PFD器件显示相对应的PFD激子发射的蓝色发射。同时，2-TNATA和DMFL-NPB掺杂器件表现出更长的波长发射相比，未掺杂的PFD?...

Watch this Scientific Journal Video about Fabrication of White Light-emitting Electrochemical Cells with Stable Emission from Exciplexes at JoVE.com

Fabrication of White Light-emitting Electrochemical Cells with Stable Emission from Exciplexes

The authors present a method for fabricating stable white-light-emitting electrochemical cells utilizing emission from exciplexes formed between a blue-emitting fluorene polymer and aromatic amines.

白的制造发光电化学细胞与来自激发络合物稳定的发射

The authors present an approach for fabricating stable white light emission from polymer light-emitting electrochemical cells (PLECs) having an active ...

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8.0K 次观看.  JX Nippon Oil & Energy Corporation. The authors present a method for fabricating stable white-light-emitting electrochemical cells utilizing emission from exciplexes formed between a blue-emitting fluorene polymer and aromatic amines.

视频: Fabrication of White Light-emitting Electrochemical Cells with Stable Emission from Exciplexes

Echo Particle Image Velocimetry

The transport of mass, momentum, and energy in fluid flows is ultimately determined by spatiotemporal distributions of the fluid velocity field.1 Consequently, a prerequisite for understanding, predicting, and controlling fluid flows is the capability to measure the velocity field with adequate spatial and temporal resolution.2 For velocity measurements in optically opaque fluids or through optically opaque geometries, echo particle image velocimetry (EPIV) is an attractive diagnostic technique to generate "instantaneous" two-dimensional fields of velocity.3,4,5,6 In this paper, the operating protocol for an EPIV system built by integrating a commercial medical ultrasound machine7 with a PC running commercial particle image velocimetry (PIV) software8 is described, and validation measurements in Hagen-Poiseuille (i.e., laminar pipe) flow are reported.
For the EPIV measurements, a phased array probe connected to the medical ultrasound machine is used to generate a two-dimensional ultrasound image by pulsing the piezoelectric probe elements at different times. Each probe element transmits an ultrasound pulse into the fluid, and tracer particles in the fluid (either naturally occurring or seeded) reflect ultrasound echoes back to the probe where they are recorded. The amplitude of the reflected ultrasound waves and their time delay relative to transmission are used to create what is known as B-mode (brightness mode) two-dimensional ultrasound images. Specifically, the time delay is used to determine the position of the scatterer in the fluid and the amplitude is used to assign intensity to the scatterer. The time required to obtain a single B-mode image, t, is determined by the time it take to pulse all the elements of the phased array probe. For acquiring multiple B-mode images, the frame rate of the system in frames per second (fps) = 1/&delta;t. (See 9 for a review of ultrasound imaging.)
For a typical EPIV experiment, the frame rate is between 20-60 fps, depending on flow conditions, and 100-1000 B-mode images of the spatial distribution of the tracer particles in the flow are acquired. Once acquired, the B-mode ultrasound images are transmitted via an ethernet connection to the PC running the PIV commercial software. Using the PIV software, tracer particle displacement fields, D(x,y)[pixels], (where x and y denote horizontal and vertical spatial position in the ultrasound image, respectively) are acquired by applying cross correlation algorithms to successive ultrasound B-mode images.10 The velocity fields, u(x,y)[m/s], are determined from the displacements fields, knowing the time step between image pairs, &Delta;T[s], and the image magnification, M[meter/pixel], i.e., u(x,y) = MD(x,y)/&Delta;T. The time step between images &Delta;T = 1/fps + D(x,y)/B, where B[pixels/s] is the time it takes for the ultrasound probe to sweep across the image width. In the present study, M = 77[&mu;m/pixel], fps = 49.5[1/s], and B = 25,047[pixels/s]. Once acquired, the velocity fields can be analyzed to compute flow quantities of interest.

An echo particle image velocimetry (EPIV) system capable of acquiring two-dimensional fields of velocity in optically opaque fluids or through optically opaque geometries is described, and validation measurements in pipe flow are reported.

回声粒子图像测速技术

The transport of mass, momentum, and energy in fluid flows is ultimately determined by spatiotemporal distributions of the fluid velocity field.1 ...

科研

工程学

Fabrication of VB2/Air Cells for Electrochemical Testing

A technique to investigate the properties and performance of new multi-electron metal/air battery systems is proposed and presented. A method for synthesizing nanoscopic VB2 is presented as well as step-by-step procedure for applying a zirconium oxide coating to the VB2 particles for stabilization upon discharge. The process for disassembling existing zinc/air cells is shown, in addition construction of the new working electrode to replace the conventional zinc/air cell anode with a the nanoscopic VB2 anode. Finally, discharge of the completed VB2/air battery is reported. We show that using the zinc/air cell as a test bed is useful to provide a consistent configuration to study the performance of the high-energy high capacity nanoscopic VB2 anode.

Fabrication of VB2/Air Cells for Electrochemical Testing

A protocol is presented to study multi-electron metal/air battery systems by using previous technology developed for the zinc/air cell. Electrochemical testing is then performed on fabricated batteries to evaluate performance.

VB制作<sub&gt; 2</sub&gt; /空气电池电化学测试

A technique to investigate the properties and performance of new multi-electron metal/air battery systems is proposed and presented. A method for ...

Fabrication of Low Temperature Carbon Nanotube Vertical Interconnects Compatible with Semiconductor Technology

We demonstrate a method for the low temperature growth (350 &#176;C) of vertically-aligned carbon nanotubes (CNT) bundles on electrically conductive thin-films. Due to the low growth temperature, the process allows integration with modern low-&#954; dielectrics and some flexible substrates. The process is compatible with standard semiconductor fabrication, and a method for the fabrication of electrical 4-point probe test structures for vertical interconnect test structures is presented. Using scanning electron microscopy the morphology of the CNT bundles is investigated, which demonstrates vertical alignment of the CNT and can be used to tune the CNT growth time. With Raman spectroscopy the crystallinity of the CNT is investigated. It was found that the CNT have many defects, due to the low growth temperature. The electrical current-voltage measurements of the test vertical interconnects displays a linear response, indicating good ohmic contact was achieved between the CNT bundle and the top and bottom metal electrodes. The obtained resistivities of the CNT bundle are among the average values in the literature, while a record-low CNT growth temperature was used.

A method for the growth of low temperature vertically-aligned carbon nanotubes, and the subsequent fabrication of vertical interconnect electrical test structures using semiconductor fabrication is presented.

低温碳纳米管垂直互连的制作兼容半导体技术

We demonstrate a method for the low temperature growth (350 &#176;C) of vertically-aligned carbon nanotubes (CNT) bundles on electrically conductive ...

Indirect Fabrication of Lattice Metals with Thin Sections Using Centrifugal Casting

One of the typical methods to manufacture 3D lattice metals is the direct-metal additive manufacturing (AM) process such as Selective Laser Melting (SLM) and Electron Beam Melting (EBM). In spite of its potential processing capability, the direct AM method has several disadvantages such as high cost, poor surface finish of final products, limitation in material selection, high thermal stress, and anisotropic properties of parts. We propose a cost-effective method to manufacture 3D lattice metals. The objective of this study is to provide a detailed protocol on fabrication of 3D lattice metals having a complex shape and a thin wall thickness; e.g., octet truss made of Al and Cu alloys having a unit cell length of 5 mm and a cell wall thickness of 0.5 mm. An overall experimental procedure is divided into eight sections: (a) 3D printing of sacrificial patterns (b) melt-out of support materials (c) removal of residue of support materials (d) pattern assembly (e) investment (f) burn-out of sacrificial patterns (g) centrifugal casting (h) post-processing for final products. The suggested indirect AM technique provides the potential to manufacture ultra-lightweight lattice metals; e.g., lattice structures with Al alloys. It appears that the process parameters should be properly controlled depending on materials and lattice geometry, observing the final products of octet truss metals by the indirect AM technique.

An indirect additive manufacturing method combining a 3D printing of polymers with a centrifugal casting is outlined for manufacturing 3D octet truss metals (Al and Cu alloys) having a unit cell length of 5 mm with a wall thickness of 0.5 mm.

与超薄切片格金属制造间接使用离心铸造

One of the typical methods to manufacture 3D lattice metals is the direct-metal additive manufacturing (AM) process such as Selective Laser Melting (SLM) ...

A Fabrication Method for Highly Stretchable Conductors with Silver Nanowires

Stretchable electronics are identified as a key technology for electronic applications in the next generation. One of the challenges in fabrication of stretchable electronic devices is the preparation of stretchable conductors with great mechanical stability. In this study, we developed a simple fabrication method to chemically solder the contact points between silver nanowire (AgNW) networks. AgNW nanomesh was first deposited on a glass slide via spray coating method. A reactive ink composed of silver nanoparticle (AgNPs) precursors was applied over the spray coated AgNW thin films. After heating for 40 min, AgNPs were preferentially generated over the nanowire junctions to solder the AgNW nanomesh, and reinforced the conducting network. The chemically modified AgNW thin film was then transferred to polyurethane (PU) substrates by casting method. The soldered AgNW thin films on PU exhibited no obvious change in electrical conductivity under stretching or rolling process with elongation strains up to 120%.

A simple synthesis method is used to chemically solder silver nanowire thin film to fabricate highly stretchable and conductive metal conductors.

对于高伸缩的导线与银纳米线制作方法

Stretchable electronics are identified as a key technology for electronic applications in the next generation. One of the challenges in fabrication of ...

Printing Fabrication of Bulk Heterojunction Solar Cells and In Situ Morphology Characterization

Polymer-based materials hold promise as low-cost, flexible efficient photovoltaic devices. Most laboratory efforts to achieve high performance devices have used devices prepared by spin coating, a process that is not amenable to large-scale fabrication. This mismatch in device fabrication makes it difficult to translate quantitative results obtained in the laboratory to the commercial level, making optimization difficult. Using a mini-slot die coater, this mismatch can be resolved by translating the commercial process to the laboratory and characterizing the structure formation in the active layer of the device in real time and in situ as films are coated onto a substrate. The evolution of the morphology was characterized under different conditions, allowing us to propose a mechanism by which the structures form and grow. This mini-slot die coater offers a simple, convenient, material efficient route by which the morphology in the active layer can be optimized under industrially relevant conditions. The goal of this protocol is to show experimental details of how a solar cell device is fabricated using a mini-slot die coater and technical details of running in situ structure characterization using the mini-slot die coater.

Printing Fabrication of Bulk Heterojunction Solar Cells and In Situ Morphology Characterization

Here, we present a protocol to fabricate organic thin film solar cells using a mini-slot die coater and related in-line structure characterizations using synchrotron scattering techniques.

散装异质结太阳能电池的印刷和制作<em&gt;原位</em&gt;形态特征

Polymer-based materials hold promise as low-cost, flexible efficient photovoltaic devices. Most laboratory efforts to achieve high performance devices ...

Emission Spectroscopic Boundary Layer Investigation during Ablative Material Testing in Plasmatron

Ablative Thermal Protection Systems (TPS) allowed the first humans to safely return to Earth from the moon and are still considered as the only solution for future high-speed reentry missions. But despite the advancements made since Apollo, heat flux prediction remains an imperfect science and engineers resort to safety factors to determine the TPS thickness. This goes at the expense of embarked payload, hampering, for example, sample return missions. 
Ground testing in plasma wind-tunnels is currently the only affordable possibility for both material qualification and validation of material response codes. The subsonic 1.2MW Inductively Coupled Plasmatron facility at the von Karman Institute for Fluid Dynamics is able to reproduce a wide range of reentry environments. This protocol describes a procedure for the study of the gas/surface interaction on ablative materials in high enthalpy flows and presents sample results of a non-pyrolyzing, ablating carbon fiber precursor. With this publication, the authors envisage the definition of a standard procedure, facilitating comparison with other laboratories and contributing to ongoing efforts to improve heat shield reliability and reduce design uncertainties.
The described core techniques are non-intrusive methods to track the material recession with a high-speed camera along with the chemistry in the reactive boundary layer, probed by emission spectroscopy. Although optical emission spectroscopy is limited to line-of-sight measurements and is further constrained to electronically excited atoms and molecules, its simplicity and broad applicability still make it the technique of choice for analysis of the reactive boundary layer. Recession of the ablating sample further requires that the distance of the measurement location with respect to the surface is known at all times during the experiment. Calibration of the optical system of the applied three spectrometers allowed quantitative comparison. At the fiber scale, results from a post-test microscopy analysis are presented.

Development of new ablative materials and their numerical modeling requires extensive experimental investigation. This protocol describes procedures for material response characterization in plasma flows with the core techniques being non-intrusive methods to track the material recession along with the chemistry in the reactive boundary layer by emission spectroscopy.

烧蚀材料在试验过程中等离子体发生器发射光谱边界层研究

Ablative Thermal Protection Systems (TPS) allowed the first humans to safely return to Earth from the moon and are still considered as the only solution ...

Electrochemical Etching and Characterization of Sharp Field Emission Points for Electron Impact Ionization

A new variation of the drop-off method for fabricating field emission points by electrochemically etching tungsten rods in a NaOH solution is described. The results of studies in which the etching current and the molarity of the NaOH solution used in the etching process were varied are presented. The investigation of the geometry of the tips, by imaging them with a scanning electron microscope, and by operating them in field emission mode is also described. The field emission tips produced are intended to be used as an electron beam source for ion production via electron impact ionization of background gas or vapor in Penning trap mass spectrometry applications.

A method for electrochemically etching field emission tips is presented. Etching parameters are characterized and the operation of the tips in field emission mode is investigated.

电化学腐蚀和电子碰撞电离夏普场发射点的表征

A new variation of the drop-off method for fabricating field emission points by electrochemically etching tungsten rods in a NaOH solution is described. ...

A System to Create Stable Nanoparticle Aerosols from Nanopowders

Nanoparticle aerosols released from nanopowders in workplaces are associated with human exposure and health risks. We developed a novel system, requiring minimal amounts of test materials (min. 200 mg), for studying powder aerosolization behavior and aerosol properties. The aerosolization procedure follows the concept of the fluidized-bed process, but occurs in the modified volume of a V-shaped aerosol generator. The airborne particle number concentration is adjustable by controlling the air flow rate. The system supplied stable aerosol generation rates and particle size distributions over long periods (0.5-2 hr and possibly longer), which are important, for example, to study aerosol behavior, but also for toxicological studies. Strict adherence to the operating procedures during the aerosolization experiments ensures the generation of reproducible test results. The critical steps in the standard protocol are the preparation of the material and setup, and the aerosolization operations themselves. The system can be used for experiments requiring stable aerosol concentrations and may also be an alternative method for testing dustiness. The controlled aerosolization made possible with this setup occurs using energy inputs (may be characterized by aerosolization air velocity) that are within the ranges commonly found in occupational environments where nanomaterial powders are handled. This setup and its operating protocol are thus helpful for human exposure and risk assessment.

We designed and developed an effective nanopowder aerosolization setup and operating protocol. The system generated nanoparticle aerosols with stable number concentrations and size distributions for long durations, requiring only small quantities of test material (min. 200 mg).

系统创建从纳米粉体纳米稳定气溶胶

Nanoparticle aerosols released from nanopowders in workplaces are associated with human exposure and health risks. We developed a novel system, requiring ...

Production and Characterization of Vacuum Deposited Organic Light Emitting Diodes

A method for producing simple and efficient thermally-activated delayed fluorescence organic light-emitting diodes (OLEDs) based on guest-host or exciplex donor-acceptor emitters is presented. With a step-by-step procedure, readers will be able to repeat and produce OLED devices based on simple organic emitters. A patterning procedure allowing the creation of personalized indium tin oxide (ITO) shape is shown. This is followed by the evaporation of all layers, encapsulation and characterization of each individual device. The end goal is to present a procedure that will give the opportunity to repeat the information presented in cited publication but also using different compounds and structures in order to prepare efficient OLEDs.

A protocol for the production of simple structured organic light-emitting diodes (OLEDs) is presented.

真空沉积有机发光二极管的生产与表征

A method for producing simple and efficient thermally-activated delayed fluorescence organic light-emitting diodes (OLEDs) based on guest-host or exciplex ...

白的制造发光电化学细胞与来自激发络合物稳定的发射

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