2020
DOI: 10.1021/acsnano.0c02060
|View full text |Cite
|
Sign up to set email alerts
|

Designing Hybrid Chiral Photonic Films with Circularly Polarized Room-Temperature Phosphorescence

Abstract: Circular polarized luminescence (CPL) is essential to chiral sciences and photonic technologies, but the achievement of circular polarized room-temperature phosphorescence (CPRTP) remains a great challenge due to the instability of triplet state excitons. Herein, we found that dual CPL and CPRTP were demonstrated by hybrid chiral photonic films designed by the coassembly of cellulose nanocrystals (CNCs), poly(vinyl alcohol) (PVA), and carbon dots (CDs). Tunable photonic band gaps were achieved by regulating th… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

3
171
0
1

Year Published

2021
2021
2024
2024

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 175 publications
(175 citation statements)
references
References 64 publications
3
171
0
1
Order By: Relevance
“…The asymmetric factor, | g lum | of 0.61, achieved here is much higher than those reported for chiral‐induced CPL emission with CNC materials. [ 25,27,50 ] The origin of active CPL emission in our work is distinguished with passive right‐handed CPL emission with negative g lum value induced by overlapping between photonic bandgap and emission band (Figure S20, Supporting Information). [ 22,24–26 ]…”
Section: Resultsmentioning
confidence: 90%
See 2 more Smart Citations
“…The asymmetric factor, | g lum | of 0.61, achieved here is much higher than those reported for chiral‐induced CPL emission with CNC materials. [ 25,27,50 ] The origin of active CPL emission in our work is distinguished with passive right‐handed CPL emission with negative g lum value induced by overlapping between photonic bandgap and emission band (Figure S20, Supporting Information). [ 22,24–26 ]…”
Section: Resultsmentioning
confidence: 90%
“…The asymmetric factor, |g lum | of 0.61, achieved here is much higher than those reported for chiral-induced CPL emission with CNC materials. [25,27,50] The origin of active CPL emission in our work is distinguished with passive right-handed CPL emission with negative g lum value induced by overlapping between photonic bandgap and emission band (Figure S20, Supporting Information). [22,[24][25][26] To further investigate dynamic control of the light emission, we triggered the reversible isomerization of SP molecules by changing the surrounding pH environment through exposure to acid and water vapor treatments in an alternating manner (Figure 5a, top).…”
Section: Switching Handedness Of Cpl Emissionmentioning
confidence: 76%
See 1 more Smart Citation
“…When a fluorescent dye is doped into the R‐CLCs, provided that the fluorescence of the dye overlaps with the PBG band, L‐CPL emission is achieved as a result of the forbidden nature of the R‐CPL emission within the PBG under certain pumping conditions (Figure S3). [ 35 ] Similarly, R‐CPL emission is obtained in left‐handed CLCs (L‐CLCs). The well‐assembled periodic helical superstructure of CLCs gives rise to a high degree of CPL emission at a given wavelength, which is favorable to the realization of compelling 3D displays.…”
Section: Resultsmentioning
confidence: 99%
“…By designing the types and proportions of chiral molecules, luminophores, and main liquid crystals of N*LC, the |g lum | of obtained CPL can reach the order from 10 -1 to 1. 11,[17][18][19][20][21][22][23][24][25] Moreover, it is a flexible design that the units in N*LC can be either doped independently or connected by the covalent bond. In addition, substantial effort has been devoted to introducing functional groups in N*LC units so that using multiple physical stimuli, like electric field [26][27][28][29][30] , light 29 and thermal 20,31 to tune CPL activity, can be realized.…”
mentioning
confidence: 99%