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|a 10.1002/adma.202405294
|2 doi
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|a pubmed24n1516.xml
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|a (DE-627)NLM374722587
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|a (NLM)38984494
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|a DE-627
|b ger
|c DE-627
|e rakwb
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|a eng
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|a Zajac, Marc
|e verfasserin
|4 aut
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|a Optical Control of Adaptive Nanoscale Domain Networks
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|c 2024
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|a Text
|b txt
|2 rdacontent
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|a ƒaComputermedien
|b c
|2 rdamedia
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|a ƒa Online-Ressource
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|2 rdacarrier
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|a Date Revised 28.08.2024
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|a published: Print-Electronic
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|a Citation Status PubMed-not-MEDLINE
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|a © 2024 The Author(s). Advanced Materials published by Wiley‐VCH GmbH.
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|a Adaptive networks can sense and adjust to dynamic environments to optimize their performance. Understanding their nanoscale responses to external stimuli is essential for applications in nanodevices and neuromorphic computing. However, it is challenging to image such responses on the nanoscale with crystallographic sensitivity. Here, the evolution of nanodomain networks in (PbTiO3)n/(SrTiO3)n superlattices (SLs) is directly visualized in real space as the system adapts to ultrafast repetitive optical excitations that emulate controlled neural inputs. The adaptive response allows the system to explore a wealth of metastable states that are previously inaccessible. Their reconfiguration and competition are quantitatively measured by scanning x-ray nanodiffraction as a function of the number of applied pulses, in which crystallographic characteristics are quantitatively assessed by assorted diffraction patterns using unsupervised machine-learning methods. The corresponding domain boundaries and their connectivity are drastically altered by light, holding promise for light-programable nanocircuits in analogy to neuroplasticity. Phase-field simulations elucidate that the reconfiguration of the domain networks is a result of the interplay between photocarriers and transient lattice temperature. The demonstrated optical control scheme and the uncovered nanoscopic insights open opportunities for the remote control of adaptive nanoscale domain networks
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|a Journal Article
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|a domains and networks
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|a ferroelectrics
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|a light‐induced phases
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|a polar nanostructures
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|a x‐ray nanoimaging
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|a Zhou, Tao
|e verfasserin
|4 aut
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|a Yang, Tiannan
|e verfasserin
|4 aut
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|a Das, Sujit
|e verfasserin
|4 aut
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|a Cao, Yue
|e verfasserin
|4 aut
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|a Guzelturk, Burak
|e verfasserin
|4 aut
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|a Stoica, Vladimir
|e verfasserin
|4 aut
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|a Cherukara, Mathew J
|e verfasserin
|4 aut
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1 |
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|a Freeland, John W
|e verfasserin
|4 aut
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|a Gopalan, Venkatraman
|e verfasserin
|4 aut
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|a Ramesh, Ramamoorthy
|e verfasserin
|4 aut
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|a Martin, Lane W
|e verfasserin
|4 aut
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|a Chen, Long-Qing
|e verfasserin
|4 aut
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|a Holt, Martin V
|e verfasserin
|4 aut
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|a Hruszkewycz, Stephan O
|e verfasserin
|4 aut
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|a Wen, Haidan
|e verfasserin
|4 aut
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|i Enthalten in
|t Advanced materials (Deerfield Beach, Fla.)
|d 1998
|g 36(2024), 35 vom: 04. Aug., Seite e2405294
|w (DE-627)NLM098206397
|x 1521-4095
|7 nnns
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|g volume:36
|g year:2024
|g number:35
|g day:04
|g month:08
|g pages:e2405294
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|u http://dx.doi.org/10.1002/adma.202405294
|3 Volltext
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