2023
DOI: 10.1007/s10118-023-2975-6
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Polymer Translocation

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Cited by 6 publications
(7 citation statements)
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“…This phenomenon is caused by the competition between topology and chain length effects. In Figure 4, we show the orientational order parameter P, the relative shape anisotropy κ 2 , the dihedral potential energy U φ , the Coulomb potential energy U c , the nonbonded interaction potential (U lj + U c ), and the first derivative of nonbonded interaction potential d(U lj + U c )/dT of single linear and cyclic PE chains with different lengths of N c at T = 100 K. Here, the selection length intervals of N c for linear and cyclic PE chains are [25,100] and [50,200], respectively. From Figure 4, oscillations of these conformational potential components at crystalline state with chain length N c for cyclic chains are more obvious than that for their linear counterparts, which is caused by the competition between cyclic topology and chain length effects.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
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“…This phenomenon is caused by the competition between topology and chain length effects. In Figure 4, we show the orientational order parameter P, the relative shape anisotropy κ 2 , the dihedral potential energy U φ , the Coulomb potential energy U c , the nonbonded interaction potential (U lj + U c ), and the first derivative of nonbonded interaction potential d(U lj + U c )/dT of single linear and cyclic PE chains with different lengths of N c at T = 100 K. Here, the selection length intervals of N c for linear and cyclic PE chains are [25,100] and [50,200], respectively. From Figure 4, oscillations of these conformational potential components at crystalline state with chain length N c for cyclic chains are more obvious than that for their linear counterparts, which is caused by the competition between cyclic topology and chain length effects.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…As analyzed above, the topological effect dominates the conformation of a short chain, while the chain length effect dominates that of a long chain. In the intermediate region of chain length N c ∈ [50,200], this competition results in the so-called odd−even effect.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
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“…2D semiconductors with pristine surfaces can keep high mobility and low leakage current at one atomic‐scale thickness and thus will be one of the most promising candidates for further ultrascaling. [ 17–25 ]…”
Section: Introductionmentioning
confidence: 99%
“…2D semiconductors with pristine surfaces can keep high mobility and low leakage current at one atomic-scale thickness and thus will be one of the most promising candidates for further ultrascaling. [17][18][19][20][21][22][23][24][25] In this article, we demonstrate a 2D NS vertical-stacked CFET based on chemical vapor deposition (CVD) 1L MoS 2 NS FET and WSe 2 NS FET. Through extensive design and optimization of the…”
mentioning
confidence: 99%