Cu–Ag and Ni–Ag meshes based on cracked template as efficient transparent electromagnetic shielding coating with excellent mechanical performance

Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We developed Cu–Ag and Ni–Ag meshes on flexible PET substrate for highly efficiency transparent EMI shielding coating. Cu–Ag and Ni–Ag meshes ob...

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Published inJournal of materials science Vol. 56; no. 26; pp. 14741 - 14762
Main Authors Voronin, A. S., Fadeev, Y. V., Govorun, I. V., Podshivalov, I. V., Simunin, M. M., Tambasov, I. A., Karpova, D. V., Smolyarova, T. E., Lukyanenko, A. V., Karacharov, A. A., Nemtsev, I. V., Khartov, S. V.
Format Journal Article
LanguageEnglish
Published New York Springer US 01.09.2021
Springer
Springer Nature B.V
Subjects
Bend radius
Characterization and Evaluation of Materials
Chemistry and Materials Science
Classical Mechanics
Coatings
Copper
Crystallography and Scattering Methods
Deformation
Deposition
Efficiency
Electrical resistivity
electromagnetic interference
Electromagnetic shielding
Electromagnetism
Graphene
Materials Science
Mechanical properties
Metals & Corrosion
Nickel
Polymer Sciences
Radiation
Science
Silver
Solid Mechanics
Substrates
Sulfur
Superhigh frequencies
Theft
Thin films
Online AccessGet full text
ISSN0022-2461
1573-4803
DOI10.1007/s10853-021-06206-4

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Abstract Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We developed Cu–Ag and Ni–Ag meshes on flexible PET substrate for highly efficiency transparent EMI shielding coating. Cu–Ag and Ni–Ag meshes obtained with galvanic deposition of copper and nickel on thin Ag seed mesh which was made by cracked template method. Coefficients S 11 , S 21 and shielding efficiency ( SE ) were measured for Cu–Ag and Ni–Ag meshes in X-band (8–12 GHz) and K-band (18–26.5 GHz). 90 s copper deposition increase SE from 23.2 to 43.7 dB at 8 GHz with a transparency of 82.2% and a sheet resistance of 0.25 Ω/sq. The achieved maximum SE was 47.6 dB for Cu–Ag mesh with 67.8% transparency and 41.1 dB for Ni–Ag mesh with 77.8% transparency. Cu–Ag and Ni–Ag meshes have high bending and long-term stability. Minimum bend radius is lower than 100 µm. This effect allows to produce different forms of transparent shielding objects, for example, origami method. Our coatings are the leading among all literary solutions in three-dimensional coordinates: of sheet resistance–optical transmittance–cost of produced. Graphical abstract
AbstractList Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We developed Cu-Ag and Ni-Ag meshes on flexible PET substrate for highly efficiency transparent EMI shielding coating. Cu-Ag and Ni-Ag meshes obtained with galvanic deposition of copper and nickel on thin Ag seed mesh which was made by cracked template method. Coefficients S.sub.11, S.sub.21 and shielding efficiency (SE) were measured for Cu-Ag and Ni-Ag meshes in X-band (8-12 GHz) and K-band (18-26.5 GHz). 90 s copper deposition increase SE from 23.2 to 43.7 dB at 8 GHz with a transparency of 82.2% and a sheet resistance of 0.25 â¦/sq. The achieved maximum SE was 47.6 dB for Cu-Ag mesh with 67.8% transparency and 41.1 dB for Ni-Ag mesh with 77.8% transparency. Cu-Ag and Ni-Ag meshes have high bending and long-term stability. Minimum bend radius is lower than 100 [micro]m. This effect allows to produce different forms of transparent shielding objects, for example, origami method. Our coatings are the leading among all literary solutions in three-dimensional coordinates: of sheet resistance-optical transmittance-cost of produced.
Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We developed Cu–Ag and Ni–Ag meshes on flexible PET substrate for highly efficiency transparent EMI shielding coating. Cu–Ag and Ni–Ag meshes obtained with galvanic deposition of copper and nickel on thin Ag seed mesh which was made by cracked template method. Coefficients S₁₁, S₂₁ and shielding efficiency (SE) were measured for Cu–Ag and Ni–Ag meshes in X-band (8–12 GHz) and K-band (18–26.5 GHz). 90 s copper deposition increase SE from 23.2 to 43.7 dB at 8 GHz with a transparency of 82.2% and a sheet resistance of 0.25 Ω/sq. The achieved maximum SE was 47.6 dB for Cu–Ag mesh with 67.8% transparency and 41.1 dB for Ni–Ag mesh with 77.8% transparency. Cu–Ag and Ni–Ag meshes have high bending and long-term stability. Minimum bend radius is lower than 100 µm. This effect allows to produce different forms of transparent shielding objects, for example, origami method. Our coatings are the leading among all literary solutions in three-dimensional coordinates: of sheet resistance–optical transmittance–cost of produced.
Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We developed Cu-Ag and Ni-Ag meshes on flexible PET substrate for highly efficiency transparent EMI shielding coating. Cu-Ag and Ni-Ag meshes obtained with galvanic deposition of copper and nickel on thin Ag seed mesh which was made by cracked template method. Coefficients S.sub.11, S.sub.21 and shielding efficiency (SE) were measured for Cu-Ag and Ni-Ag meshes in X-band (8-12 GHz) and K-band (18-26.5 GHz). 90 s copper deposition increase SE from 23.2 to 43.7 dB at 8 GHz with a transparency of 82.2% and a sheet resistance of 0.25 â¦/sq. The achieved maximum SE was 47.6 dB for Cu-Ag mesh with 67.8% transparency and 41.1 dB for Ni-Ag mesh with 77.8% transparency. Cu-Ag and Ni-Ag meshes have high bending and long-term stability. Minimum bend radius is lower than 100 [micro]m. This effect allows to produce different forms of transparent shielding objects, for example, origami method. Our coatings are the leading among all literary solutions in three-dimensional coordinates: of sheet resistance-optical transmittance-cost of produced. Graphical abstract
Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We developed Cu–Ag and Ni–Ag meshes on flexible PET substrate for highly efficiency transparent EMI shielding coating. Cu–Ag and Ni–Ag meshes obtained with galvanic deposition of copper and nickel on thin Ag seed mesh which was made by cracked template method. Coefficients S11, S21 and shielding efficiency (SE) were measured for Cu–Ag and Ni–Ag meshes in X-band (8–12 GHz) and K-band (18–26.5 GHz). 90 s copper deposition increase SE from 23.2 to 43.7 dB at 8 GHz with a transparency of 82.2% and a sheet resistance of 0.25 Ω/sq. The achieved maximum SE was 47.6 dB for Cu–Ag mesh with 67.8% transparency and 41.1 dB for Ni–Ag mesh with 77.8% transparency. Cu–Ag and Ni–Ag meshes have high bending and long-term stability. Minimum bend radius is lower than 100 µm. This effect allows to produce different forms of transparent shielding objects, for example, origami method. Our coatings are the leading among all literary solutions in three-dimensional coordinates: of sheet resistance–optical transmittance–cost of produced.
Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We developed Cu–Ag and Ni–Ag meshes on flexible PET substrate for highly efficiency transparent EMI shielding coating. Cu–Ag and Ni–Ag meshes obtained with galvanic deposition of copper and nickel on thin Ag seed mesh which was made by cracked template method. Coefficients S 11 , S 21 and shielding efficiency ( SE ) were measured for Cu–Ag and Ni–Ag meshes in X-band (8–12 GHz) and K-band (18–26.5 GHz). 90 s copper deposition increase SE from 23.2 to 43.7 dB at 8 GHz with a transparency of 82.2% and a sheet resistance of 0.25 Ω/sq. The achieved maximum SE was 47.6 dB for Cu–Ag mesh with 67.8% transparency and 41.1 dB for Ni–Ag mesh with 77.8% transparency. Cu–Ag and Ni–Ag meshes have high bending and long-term stability. Minimum bend radius is lower than 100 µm. This effect allows to produce different forms of transparent shielding objects, for example, origami method. Our coatings are the leading among all literary solutions in three-dimensional coordinates: of sheet resistance–optical transmittance–cost of produced. Graphical abstract
Audience Academic
Author Nemtsev, I. V.
Podshivalov, I. V.
Karacharov, A. A.
Khartov, S. V.
Voronin, A. S.
Fadeev, Y. V.
Govorun, I. V.
Simunin, M. M.
Karpova, D. V.
Smolyarova, T. E.
Tambasov, I. A.
Lukyanenko, A. V.
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  fullname: Karpova, D. V.
  organization: Federal Research Center «Krasnoyarsk Science Center, Siberian Branch, Russian Academy of Sciences» (FRC KSC SB RAS)
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Copyright The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021
COPYRIGHT 2021 Springer
The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021.
Copyright_xml – notice: The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021
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Snippet Nowadays, the technical advances call for efficient electromagnetic interference (EMI) shielding of transparent devices which may be subject to data theft. We...
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SubjectTerms Bend radius
Characterization and Evaluation of Materials
Chemistry and Materials Science
Classical Mechanics
Coatings
Copper
Crystallography and Scattering Methods
Deformation
Deposition
Efficiency
Electrical resistivity
electromagnetic interference
Electromagnetic shielding
Electromagnetism
Graphene
Materials Science
Mechanical properties
Metals & Corrosion
Nickel
Polymer Sciences
Radiation
Science
Silver
Solid Mechanics
Substrates
Sulfur
Superhigh frequencies
Theft
Thin films
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Title Cu–Ag and Ni–Ag meshes based on cracked template as efficient transparent electromagnetic shielding coating with excellent mechanical performance
URI https://link.springer.com/article/10.1007/s10853-021-06206-4
https://www.proquest.com/docview/2545000598
https://www.proquest.com/docview/2636382290
Volume 56
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