# Electrothermally tunable cholesteric liquid crystal laser achieving 130 nm range with high circular polarization purity (|g| ≥ 1.4)

**Authors:** Mi-Yun Jeong, Keumcheol Kwak

PMC · DOI: 10.1038/s41598-025-34461-x · 2026-01-06

## TL;DR

This paper introduces a tunable laser using cholesteric liquid crystals that can emit circularly polarized light across a 130 nm range with high purity.

## Contribution

The study presents a novel electrothermally tunable cholesteric laser with a 130 nm tuning range and high circular polarization purity.

## Key findings

- Wedge-shaped SCLC cells enable continuous spectral tuning across 100–126 nm.
- The laser maintains a dissymmetry factor g ≥ 1.4 across the full tuning range.
- Phase transitions were analyzed to guide optimal voltage-sweep strategies.

## Abstract

Circularly polarized light lasers are attracting growing attention for quantum optics, spin-optoelectronics, and next-generation display technologies. However, despite many demonstrations of cholesteric liquid crystal (CLC) lasers, two challenges remain: achieving broadband and continuous wavelength tunability and quantitatively determining the dissymmetry factor (g) under realistic conditions. Here, we present an actively tunable cholesteric laser based on supersaturated CLC (SCLC) cells driven by electrothermal control. In parallel SCLC cells, lasing wavelengths can be tuned about 130 nm (553–682 nm), but the spectral shift occurs discontinuously due to boundary constraints. In contrast, wedge-shaped SCLC cells form an electrothermally induced pitch gradient that enables rapid and continuous spectral tuning across ~ 100–126 nm. To rigorously quantify the polarization state, we employed the Stokes–Mueller analysis with three circular analyzers, correcting for non-ideal transmission and leakage. Across the full 130-nm tuning range, the generated laser maintained a consistently high degree of circular polarization purity, with the dissymmetry factor g quantified as 1.633 at 600–620 nm and 1.40 at 630–650 nm ranges. These results verify that the circular polarization performance of the SCLC-based tunable laser remains robust throughout the entire visible lasing spectrum. Differential scanning calorimetry further revealed second-order SmA–CLC–isotropic phase transitions, clarifying dynamic asymmetries between heating and cooling and guiding optimal voltage-sweep strategies. Together, these findings demonstrate a reliable pathway toward broadband, color-tunable, and spin-selective CLC lasers, bridging photonic bandgap engineering with practical applications in nanophotonics, spin-optoelectronics, and advanced display technologies.

The online version contains supplementary material available at 10.1038/s41598-025-34461-x.

## Full-text entities

- **Diseases:** SCLC (MESH:D000070657)
- **Chemicals:** PBG (-), toluene (MESH:D014050), silica (MESH:D012822), LDS698 (MESH:C582868), PI (MESH:D010716), 4-dicyanomethylene-2-methyl-6-p-dimethylaminostyryl-4Hpyran (MESH:C082825), perovskite (MESH:C059910), polymer (MESH:D011108)
- **Cell lines:** W — Drosophila melanogaster (Fruit fly), Spontaneously immortalized cell line (CVCL_Z791), F — Mesocricetus auratus (Golden hamster), Transformed cell line (CVCL_XK46), S2 — Drosophila melanogaster (Fruit fly), Spontaneously immortalized cell line (CVCL_Z232), LCLC648 — Homo sapiens (Human), Induced pluripotent stem cell (CVCL_DQ30), -SCLC2,-3 — Homo sapiens (Human), Lung small cell carcinoma, Cancer cell line (CVCL_7005), -SCLC1 — Homo sapiens (Human), Lung small cell carcinoma, Cancer cell line (CVCL_WH07), W-SCLC2 — Homo sapiens (Human), Lung small cell carcinoma, Cancer cell line (CVCL_7016), LCLC — Homo sapiens (Human), Lung large cell carcinoma, Cancer cell line (CVCL_1375), F-LCLC613 — Homo sapiens (Human), Finite cell line (CVCL_4D18)

## Figures

7 figures with captions in the complete paper: https://tomesphere.com/paper/PMC12859137/full.md

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Source: https://tomesphere.com/paper/PMC12859137