2022
DOI: 10.1002/anie.202201138
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Light‐Powered Ion Pumping in a Cation‐Selective Conducting Polymer Membrane

Abstract: The simulation of the ion pumping against a proton gradient energized by light in photosynthesis is of significant importance for the energy conversion in a non‐biological environment. Herein, we report light‐powered ion pumping in a polystyrene sulfonate anion (PSS) doped polypyrrole (PPy) conducting polymer membrane (PSS‐PPy) with a symmetric geometry. This PSS‐PPy conducting polymer membrane exhibits a cationic selectivity and a light‐responsive surface‐charge‐governed ion transport attributed to the negati… Show more

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Cited by 27 publications
(35 citation statements)
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“…Theoretical Calculation: The ion transport properties were quantitatively investigated using "Electrostatics" and "Transport of Diluted Species" modules in COMSOL Multiphysics 5.6. [33,38] To simplify the calculation, the TiO 2 /AAO membrane was theoretically modeled as a double-layer cylindrical nanochannel with a length of 600 nm, in which the segment of TiO 2 layer had a pore width of 4 nm (d 1 ) and a length of 200 nm (L 1 ), and the segment of AAO had a pore width of 17 nm (d 2 ) and a length of 400 nm (L 2 ) (Figure S7, Supporting Information). The surface charge density of TiO 2 (σ 1 ) and AAO (σ 2 ) was set to be −0.003 C m −2 and +0.002 C m −2 , respectively.…”
Section: Methodsmentioning
confidence: 99%
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“…Theoretical Calculation: The ion transport properties were quantitatively investigated using "Electrostatics" and "Transport of Diluted Species" modules in COMSOL Multiphysics 5.6. [33,38] To simplify the calculation, the TiO 2 /AAO membrane was theoretically modeled as a double-layer cylindrical nanochannel with a length of 600 nm, in which the segment of TiO 2 layer had a pore width of 4 nm (d 1 ) and a length of 200 nm (L 1 ), and the segment of AAO had a pore width of 17 nm (d 2 ) and a length of 400 nm (L 2 ) (Figure S7, Supporting Information). The surface charge density of TiO 2 (σ 1 ) and AAO (σ 2 ) was set to be −0.003 C m −2 and +0.002 C m −2 , respectively.…”
Section: Methodsmentioning
confidence: 99%
“…Generally, either the unidirectional or light-powered antigradient ion transport mimicking that in purple bacteria can be achieved in artificial membranes by introducing asymmetric factors. [18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33] For example, to obtain the unidirectional ion transport (i.e. ion rectification), membranes composed of polymers, [34][35][36][37][38] metal oxides, [39][40][41][42][43] nanoporous carbon, [44][45][46] or metal-organic frameworks [47,48] with asymmetric pore size, chemical composition, or charge polarity have been developed as artificial ion channels.…”
Section: Doi: 101002/smll202202910mentioning
confidence: 99%
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“…In the last few years, with the rapid development of smart photo-responsive materials, such as GO and MXene, new advances are directed into the field of nanofluidic systems and, as a result, sparking the explorations of bioinspired smart devices with functions of "uphill" transport. [140,[161][162][163] Antonietti's group developed many facile methods to synthesis graphitic carbon nitride materials with abundant micro-/nano-structures and morphologies. [84] The carbon nitride materials possess [121] (B) Ionic gating property based on the interactions between GO and AZO-DNA modified PAA membrane.…”
Section: Self-responsive Materials Fabricated For the Nanochannelsmentioning
confidence: 99%