对 "用于各种柔性电子器件的超细高导电银电极的电流体动力印刷 "的更正

Jingxuan Ma, Jiayun Feng, He Zhang, Xuanyi Hu, Jiayue Wen, Shang Wang, Yanhong Tian
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The corrected Figure 2 and the associated figure caption are displayed below.</p>\n<figure><picture>\n<source media=\"(min-width: 1650px)\" srcset=\"/cms/asset/d8be67d0-361e-4f32-90d0-a6da6b3cb2e5/admt202400606-fig-0001-m.jpg\"/><img alt=\"Details are in the caption following the image\" data-lg-src=\"/cms/asset/d8be67d0-361e-4f32-90d0-a6da6b3cb2e5/admt202400606-fig-0001-m.jpg\" loading=\"lazy\" src=\"/cms/asset/5bd5c517-a1e2-4457-9102-c9a66253b4fb/admt202400606-fig-0001-m.png\" title=\"Details are in the caption following the image\"/></picture><figcaption>\n<div><strong>Figure 2<span style=\"font-weight:normal\"></span></strong><div>Open in figure viewer<i aria-hidden=\"true\"></i><span>PowerPoint</span></div>\n</div>\n<div>a) OM images of EHD-printed droplets and lines with different solvent compositions. b) The printed line width and resistance of different solvent compositions. c) Schematic illustration of the evaporation process of Ag ink droplets with different water contents.</div>\n</figcaption>\n</figure>\n<p>In Figure 4a,b of the originally published article, plots of conductivity data taken five days after printing were mistakenly used rather than the plots of the freshly printed samples from the accepted version of the article. There is a small discrepancy in the data between the two sets of plots owing to a slight decrease in conductivity over time. Further, in Figures Figure a-c, the right-hand axis was mistakenly labeled “Resistivity (µΩ cm)” and is hereby corrected to “Line resistance (Ω cm<sup>−1</sup>)”. The corrected Figure 4 and the associated figure caption are displayed below.</p>\n<figure><picture>\n<source media=\"(min-width: 1650px)\" srcset=\"/cms/asset/90f900cb-46a6-4d33-a713-9c2a38d7431a/admt202400606-fig-0002-m.jpg\"/><img alt=\"Details are in the caption following the image\" data-lg-src=\"/cms/asset/90f900cb-46a6-4d33-a713-9c2a38d7431a/admt202400606-fig-0002-m.jpg\" loading=\"lazy\" src=\"/cms/asset/2e8543d7-6627-4e1e-99ab-e173611be853/admt202400606-fig-0002-m.png\" title=\"Details are in the caption following the image\"/></picture><figcaption>\n<div><strong>Figure 4<span style=\"font-weight:normal\"></span></strong><div>Open in figure viewer<i aria-hidden=\"true\"></i><span>PowerPoint</span></div>\n</div>\n<div>a) The printed line width and resistance of different printing speeds. b) The printed line width and resistance of different voltages. c) The printed line width and resistance of different working heights. d) Four printing modes of EHD printing. e) Optimal conditions under different voltages and working heights. f) OM images of the Ag grid electrode.</div>\n</figcaption>\n</figure>\n<p>The text in paragraph 9 of Section 2 of the originally published article describing the data in Figure 4a-c refers to the freshly printed samples and is therefore accurate. Namely: “Figure 4a shows the effect of printing speed on line width and conductivity. As the printing speed increased from 0.1 to 1.6 mm s<sup>−1</sup>, the line width gradually decreased from 37.52 ± 2.66 to 8.84 ± 0.98 µm. Printing speed plays an essential role in printing uniformity and process stability. If the printing speed is too high, it is difficult for the Taylor cone to remain stable for a long time. Figure 4b illustrates the effect of voltage on printing quality. As the voltage increased from 1.0 to 2.0 kV, the line width gradually increased (from 9.91 ± 1.29 to 31.65 ± 2.40 µm) and the conductivity increased. Furthermore, with the increase of the nozzle-substrate distance, the line width gradually increases (from 11.08 ± 0.77 to 28.28 ± 2.51 µm), but the conductivity decreases, as shown in Figure 4c.”</p>\n<p>These corrections do not affect the overall conclusions of the study.</p>\n<p>We apologize for this error.</p>","PeriodicalId":7200,"journal":{"name":"Advanced Materials & Technologies","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Correction to “Electrohydrodynamic Printing of Ultrafine and Highly Conductive Ag Electrodes for Various Flexible Electronics”\",\"authors\":\"Jingxuan Ma, Jiayun Feng, He Zhang, Xuanyi Hu, Jiayue Wen, Shang Wang, Yanhong Tian\",\"doi\":\"10.1002/admt.202400606\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><i>Adv. Mater. 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引用次数: 0

摘要

Adv.Technol.2023,8,e2300080DOI: 10.1002/admt.202300080在最初发表的文章的图 2 和图 4 中发现了如下错误:在图 2b 中,右侧轴被错误地标注为 "电阻率 (Ω cm)"。现更正为 "线电阻 (Ω cm-1)"。此外,图 2a-c 的标题标注错误,顺序也不对。更正后的图 2 和相关图表说明如下。图 2在图形查看器中打开PowerPointa) 不同溶剂成分的电致发光印刷液滴和线条的 OM 图像。 b) 不同溶剂成分的印刷线条宽度和电阻。c) 不同含水量的银墨液滴蒸发过程示意图。在最初发表的文章图 4a、b 中,错误地使用了印刷五天后的电导率数据图,而不是已接受版本中的新印刷样品图。由于随着时间的推移,电导率会略有下降,因此两组图之间的数据存在微小差异。此外,在图 a-c 中,右侧坐标轴被误标为 "电阻率 (µΩ cm)",现更正为 "线电阻 (Ω cm-1)"。更正后的图 4 和相关图表说明如下。图 4在图形浏览器中打开PowerPointa)不同印刷速度下的印刷线宽和电阻。d) EHD 印刷的四种印刷模式。 e) 不同电压和工作高度下的最佳条件。 f) Ag 栅电极的 OM 图像。最初发表的文章第 2 部分第 9 段中描述图 4a-c 中数据的文字指的是新印刷的样品,因此是准确的。即"图 4a 显示了印刷速度对线宽和导电率的影响。随着印刷速度从 0.1 mm s-1 增加到 1.6 mm s-1,线宽从 37.52 ± 2.66 µm 逐渐减小到 8.84 ± 0.98 µm。印刷速度对印刷均匀性和工艺稳定性起着至关重要的作用。如果印刷速度过快,泰勒锥就很难长时间保持稳定。图 4b 显示了电压对印刷质量的影响。随着电压从 1.0 千伏增加到 2.0 千伏,线宽逐渐增加(从 9.91 ± 1.29 微米增加到 31.65 ± 2.40 微米),导电率也随之增加。此外,如图 4c 所示,随着喷嘴与基底距离的增加,线宽逐渐增加(从 11.08 ± 0.77 到 28.28 ± 2.51 µm),但导电率却降低了。"这些修正并不影响研究的总体结论,我们对此错误表示歉意。
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Correction to “Electrohydrodynamic Printing of Ultrafine and Highly Conductive Ag Electrodes for Various Flexible Electronics”

Adv. Mater. Technol. 2023, 8, e2300080

DOI: 10.1002/admt.202300080

Errors have been identified in Figures 2 and 4 of the originally published article, as follows.

In Figure 2b, the right-hand axis was mistakenly labeled “Resistivity (Ω cm).” It is hereby corrected to “Line resistance (Ω cm−1)”. Further, the captions to Figure 2a–c were labeled incorrectly and in the wrong order. The corrected Figure 2 and the associated figure caption are displayed below.

Details are in the caption following the image
Figure 2
Open in figure viewerPowerPoint
a) OM images of EHD-printed droplets and lines with different solvent compositions. b) The printed line width and resistance of different solvent compositions. c) Schematic illustration of the evaporation process of Ag ink droplets with different water contents.

In Figure 4a,b of the originally published article, plots of conductivity data taken five days after printing were mistakenly used rather than the plots of the freshly printed samples from the accepted version of the article. There is a small discrepancy in the data between the two sets of plots owing to a slight decrease in conductivity over time. Further, in Figures Figure a-c, the right-hand axis was mistakenly labeled “Resistivity (µΩ cm)” and is hereby corrected to “Line resistance (Ω cm−1)”. The corrected Figure 4 and the associated figure caption are displayed below.

Details are in the caption following the image
Figure 4
Open in figure viewerPowerPoint
a) The printed line width and resistance of different printing speeds. b) The printed line width and resistance of different voltages. c) The printed line width and resistance of different working heights. d) Four printing modes of EHD printing. e) Optimal conditions under different voltages and working heights. f) OM images of the Ag grid electrode.

The text in paragraph 9 of Section 2 of the originally published article describing the data in Figure 4a-c refers to the freshly printed samples and is therefore accurate. Namely: “Figure 4a shows the effect of printing speed on line width and conductivity. As the printing speed increased from 0.1 to 1.6 mm s−1, the line width gradually decreased from 37.52 ± 2.66 to 8.84 ± 0.98 µm. Printing speed plays an essential role in printing uniformity and process stability. If the printing speed is too high, it is difficult for the Taylor cone to remain stable for a long time. Figure 4b illustrates the effect of voltage on printing quality. As the voltage increased from 1.0 to 2.0 kV, the line width gradually increased (from 9.91 ± 1.29 to 31.65 ± 2.40 µm) and the conductivity increased. Furthermore, with the increase of the nozzle-substrate distance, the line width gradually increases (from 11.08 ± 0.77 to 28.28 ± 2.51 µm), but the conductivity decreases, as shown in Figure 4c.”

These corrections do not affect the overall conclusions of the study.

We apologize for this error.

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