4.8 Article

Direct Detection of Circularly Polarized Light Using Chiral Copper Chloride-Carbon Nanotube Heterostructures

期刊

ACS NANO
卷 15, 期 4, 页码 7608-7617

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acsnano.1c01134

关键词

chiral organic-inorganic hybrid materials; chiral copper chloride; carbon nanotube; circularly polarized light detection; heterojunction; optoelectronics

资金

  1. Center for Hybrid Organic Inorganic Semiconductors for Energy (CHOISE) an Energy Frontier Research Center - Office of Basic Energy Sciences, Office of Science within the U.S. Department of Energy
  2. U.S. DOE [DE-AC36-08G028308]
  3. U.S. Department of Energy, Office of Science, Basic Energy Sciences [SC0012541]

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The study demonstrates high-performance circularly polarized light detectors by synthesizing 0D chiral copper chloride hybrids, showing superior optoelectronic properties. Results show that through the design of chiral heterostructures, high responsivity, competitive anisotropy factor, and low working voltage can be achieved for CPL detection.
The emergent properties of chiral organicinorganic hybrid materials offer opportunities in spin-dependent optoelectronic devices. One of the most promising applications where spin, charge, and light are strongly coupled is circularly polarized light (CPL) detection. However, the performance of state-of-the-art CPL detectors using chiral hybrid metal halide semiconductors is still limited by the low anisotropy factor, poor conductivity, and limited photo-responsivity. Here, we synthesize 0D chiral copper chloride hybrids, templated by chiral methylbenzylammonium (R/SMBA), i.e., (R-/S-MBA)(2)CuCl4, that display circular dichroism for the ligand-to-metal charge transfer transition with an absorption anisotropy factor (gCD) among the largest reported for chiral metal halide semiconductor hybrids. To circumvent the poor conductivity of the unpercolated inorganic framework of this chiral absorber, we develop a direct CPL detector that utilizes a heterojunction between the chiral (MBA)(2)CuCl4 absorber layer and a semiconducting single-walled carbon nanotube (s-SWCNT) transport channel. Our chiral heterostructure shows high photoresponsivity of 452 A/W, a competitive anisotropy factor (g(res)) of up to 0.21, a current response in microamperes, and low working voltage down to 0.01 V. Our results clearly demonstrate a useful strategy toward high-performance chiral optoelectronic devices, where a nanoscale heterostructure enables direct CPL detection even for highly insulating chiral materials.

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