中文名称 | 英文名称 | CAS号 | 化学式 | 分子量 |
---|---|---|---|---|
1-(2-叠氮乙基)萘 | 1-(2-azidoethyl)naphthalene | 406953-52-4 | C12H11N3 | 197.239 |
1-萘乙酰胺 | 1-Naphthylacetamide | 86-86-2 | C12H11NO | 185.225 |
1-(1-萘基)-2-硝基乙烷 | 1-(2-nitroethyl)naphthalene | 70360-84-8 | C12H11NO2 | 201.225 |
1-(2-溴乙基)萘 | 1-(2-bromo)ethylnaphthalene | 13686-49-2 | C12H11Br | 235.123 |
1-萘乙腈 | 1-Naphthylacetonitrile | 132-75-2 | C12H9N | 167.21 |
1-萘乙醇 | 2-naphthaleneethanol | 773-99-9 | C12H12O | 172.227 |
—— | 1-naphthylacetaldoxime | 31125-58-3 | C12H11NO | 185.225 |
—— | (2-[1]naphthyl-ethyl)-carbamic acid ethyl ester | 645393-37-9 | C15H17NO2 | 243.305 |
甲基萘 | 1-Methylnaphthalene | 90-12-0 | C11H10 | 142.2 |
萘-1-基乙酰氯 | naphthalen-1-yl-acetyl chloride | 5121-00-6 | C12H9ClO | 204.656 |
—— | 1-(naphthalen-1-yl)-2-nitroethanol | 39221-01-7 | C12H11NO3 | 217.224 |
1-萘甲醛 | 1-naphthaldehyde | 66-77-3 | C11H8O | 156.184 |
1-溴甲基萘 | 2-(bromomethyl)naphthalene | 3163-27-7 | C11H9Br | 221.096 |
中文名称 | 英文名称 | CAS号 | 化学式 | 分子量 |
---|---|---|---|---|
—— | 1-(2-formamidoylethyl)naphthalene | 23950-49-4 | C13H13NO | 199.252 |
—— | (2-[1]naphthyl-ethyl)-guanidine | 62658-35-9 | C13H15N3 | 213.282 |
—— | N-(2-(naphthalen-1-yl)ethyl)acetamide | 25055-71-4 | C14H15NO | 213.279 |
—— | (2-Naphthalen-1-yl-ethyl)-((E)-3-phenyl-allyl)-amine | 1071127-51-9 | C21H21N | 287.404 |
—— | (E)-N-methyl-N-(3-phenyl-2-propenyl)-1-naphthalene-2-ethanamine | 98977-58-3 | C22H23N | 301.431 |
—— | N-(2-(naphthalen-1-yl)ethyl)benzamide | 3185-51-1 | C19H17NO | 275.35 |
—— | 7-(2-naphthalen-1-yl-ethylcarbamoyl)-heptanoic acid methyl ester | 406726-56-5 | C21H27NO3 | 341.45 |
Chiral hybrid organic–inorganic metal halides (HOMHs) offer an ideal platform for the advancement of second‐order nonlinear optical (NLO) materials owing to their inherent noncentrosymmetric structures. The enhancement of optical nonlinearity of chiral HOMHs could be achieved by matching the free exciton and/or self‐trapped exciton energy levels with desired NLO frequencies. However, the current scarcity of resonance modes and low resonance ratio hamper the further improvements of NLO performance. Herein, we propose a new resonant channel of charge transfer (CT) excited states from metal halide polyhedra to organic ligand to boost the second‐order optical nonlinearity of chiral HOMHs. The model lead halide (C7H10N)PbBr3 (C7H10N=1‐ethylpyridinium) exhibits a drastically enhanced second harmonic generation in resonance to the deep CT exciton energy, with intensity of up to 111.0 times that of KDP and 10.9 times that of urea. The effective NLO coefficient has been determined to be as high as ~40.2 pm V−1, balanced with a large polarization ratio and high laser damage threshold. This work highlights the contribution of organic ligands in the construction of a resonant channel for enhancing second‐order NLO coefficients of metal halides, and thus provides guidelines for designing new chiral HOMHs materials for advanced nonlinear photonic applications.