
Juan Du
Articles
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3 weeks ago |
pubs.rsc.org | Yixi Wu |Xingzhen Huang |Jing Li |Juan Du
Long-lasting time-dependent tunable afterglow in Zn2SiO4:Mn2+ glass ceramics for dynamic anti-counterfeiting Dynamic time-dependent afterglow materials have shown good application potential in the field of anti-counterfeiting. However, their short decay time (<10 s) causes poor concealment and limits their application expansion.
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Jan 24, 2025 |
biorxiv.org | Juan Du |Wei Lu |Sushant Kumar |Fei Jin
AbstractDetecting noxious heat is vital for survival, triggering pain responses that protect against harm. The TRPM3 channel is a key nociceptor for sensing noxious heat and a promising therapeutic target for pain treatment and neurological disorders such as epilepsy. Here, we functionally and structurally characterized TRPM3 in response to diverse stimuli: the synthetic superagonist CIM0216, the anticonvulsant antagonist primidone, and heat.
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Jan 16, 2025 |
mdpi.com | Juan Du |Yuan Wang |Shaohui Su |Wenwen Wang
All articles published by MDPI are made immediately available worldwide under an open access license. No special permission is required to reuse all or part of the article published by MDPI, including figures and tables. For articles published under an open access Creative Common CC BY license, any part of the article may be reused without permission provided that the original article is clearly cited. For more information, please refer to https://www.mdpi.com/openaccess.
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Oct 22, 2024 |
mdpi.com | Miao-Miao Tian |Gang Liu |Juan Du |Yue Liu
All articles published by MDPI are made immediately available worldwide under an open access license. No special permission is required to reuse all or part of the article published by MDPI, including figures and tables. For articles published under an open access Creative Common CC BY license, any part of the article may be reused without permission provided that the original article is clearly cited. For more information, please refer to https://www.mdpi.com/openaccess.
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Sep 30, 2024 |
mdpi.com | Juan Du |Fan Wu
1. Introduction ∂ t u + u · ∇ u − Δ u + ∇ π = 0 , x ∈ R 3 , t > 0 ∇ · u = 0 , x ∈ R 3 , t > 0 u t = 0 = u 0 ( x ) , x ∈ R 3 , (1) where The Navier–Stokes equation (NSE for short) is one of the fundamental equations of fluid dynamics. The three-dimensional viscous incompressible NSE reads as u = ( u 1 , u 2 , u 3 ) —the velocity field—and π—the pressure—are the unknowns, and u 0 is the initial velocity field.
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