🗊Презентация Optical identification using imperfections in 2D materials

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Optical identification using imperfections in 2D materials, слайд №1Optical identification using imperfections in 2D materials, слайд №2Optical identification using imperfections in 2D materials, слайд №3Optical identification using imperfections in 2D materials, слайд №4Optical identification using imperfections in 2D materials, слайд №5Optical identification using imperfections in 2D materials, слайд №6Optical identification using imperfections in 2D materials, слайд №7Optical identification using imperfections in 2D materials, слайд №8Optical identification using imperfections in 2D materials, слайд №9Optical identification using imperfections in 2D materials, слайд №10Optical identification using imperfections in 2D materials, слайд №11Optical identification using imperfections in 2D materials, слайд №12Optical identification using imperfections in 2D materials, слайд №13
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Optical identification using imperfections in 2D materials
Описание слайда:
Optical identification using imperfections in 2D materials

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Introduction The ability to uniquely identify an object or device is important for authentication. Imperfections, locked into structures during fabrication, can be used to provide a fingerprint that is challenging to reproduce.
Описание слайда:
Introduction The ability to uniquely identify an object or device is important for authentication. Imperfections, locked into structures during fabrication, can be used to provide a fingerprint that is challenging to reproduce.

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Objective To analise a proposed simple optical technique to read unique information from nanometer-scale defects in 2D materials. 
Описание слайда:
Objective To analise a proposed simple optical technique to read unique information from nanometer-scale defects in 2D materials. 

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Tasks Method Results for WS2 from mechanically exfoliation Results for WS2 from chemical vapor deposition Conclusion
Описание слайда:
Tasks Method Results for WS2 from mechanically exfoliation Results for WS2 from chemical vapor deposition Conclusion

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Method Measurement apparatus, in which the photoluminescence from a monolayer TMD is collected by an objective lens (OL), selectively transmitted through a rotatable optical bandpass filter (BPF), finally imaged on a CCD sensor. 
Описание слайда:
Method Measurement apparatus, in which the photoluminescence from a monolayer TMD is collected by an objective lens (OL), selectively transmitted through a rotatable optical bandpass filter (BPF), finally imaged on a CCD sensor. 

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Angular orientations of the BPF determines the center-wavelength of its pass band, which varies with incidence angle Angular orientations of the BPF determines the center-wavelength of its pass band, which varies with incidence angle
Описание слайда:
Angular orientations of the BPF determines the center-wavelength of its pass band, which varies with incidence angle Angular orientations of the BPF determines the center-wavelength of its pass band, which varies with incidence angle

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Concept of the angular selective transmission Changing the BPF angle lights up a random subset of pixels on the CCD; red, green and blue conceptually correspond to positions on the monolayer TMD that emits in differing energy ranges. When no filter is present, all energies are picked up.
Описание слайда:
Concept of the angular selective transmission Changing the BPF angle lights up a random subset of pixels on the CCD; red, green and blue conceptually correspond to positions on the monolayer TMD that emits in differing energy ranges. When no filter is present, all energies are picked up.

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Makeup of PUF The BPF angular orientation θ, the corresponding BPF bandwidth, and the spatially varying photoluminescence of the monolayer TMD PL makes up the physical unclonable function.
Описание слайда:
Makeup of PUF The BPF angular orientation θ, the corresponding BPF bandwidth, and the spatially varying photoluminescence of the monolayer TMD PL makes up the physical unclonable function.

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Results for WS2 from mechanically exfoliation 50× Optical image of the exfoliated  flake on PDMS. μ-PL map of this flake was recorded with 532 nm excitation and 100 μW excitation power at 300 K. The integration time for each pixel is 0.5 s. 
Описание слайда:
Results for WS2 from mechanically exfoliation 50× Optical image of the exfoliated  flake on PDMS. μ-PL map of this flake was recorded with 532 nm excitation and 100 μW excitation power at 300 K. The integration time for each pixel is 0.5 s. 

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Results for WS2 from chemical vapor deposition Angular-dependent PL images of  monolayer flake, excited by 450 nm laser, collected using 50×  (a)–(c) and 10×  (d)–(f) respectively.
Описание слайда:
Results for WS2 from chemical vapor deposition Angular-dependent PL images of  monolayer flake, excited by 450 nm laser, collected using 50×  (a)–(c) and 10×  (d)–(f) respectively.

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Angular dependent PL images of WS2 monolayer flake, excited by 450 nm laser, imaged by a 10×  objective lens Angular dependent PL images of WS2 monolayer flake, excited by 450 nm laser, imaged by a 10×  objective lens
Описание слайда:
Angular dependent PL images of WS2 monolayer flake, excited by 450 nm laser, imaged by a 10×  objective lens Angular dependent PL images of WS2 monolayer flake, excited by 450 nm laser, imaged by a 10×  objective lens

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Conclusion Spatial non-uniform photoluminescence is more pronounced for chemical vapor grown flakes than those created using mechanical exfoliation. The key to implementing a real authentication or identification system based on an optical PUF, such as the one we described, is to capture the random response or physical characteristics and generate unique fingerprints. So far we have discussed a method to capture the response from 2D materials, based on imaging the fluorescence from structural defects with a bandpass filter at different detection angles.
Описание слайда:
Conclusion Spatial non-uniform photoluminescence is more pronounced for chemical vapor grown flakes than those created using mechanical exfoliation. The key to implementing a real authentication or identification system based on an optical PUF, such as the one we described, is to capture the random response or physical characteristics and generate unique fingerprints. So far we have discussed a method to capture the response from 2D materials, based on imaging the fluorescence from structural defects with a bandpass filter at different detection angles.

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