Abstract

Circularly polarized luminescence (CPL) spectroscopy measures the difference in luminescence intensity between left- and right-circularly polarized light, and is often used to analyze the structure of chiral molecules in their excited state. Recently, it has found an increasing range of applications in the analysis of molecules that emit circularly polarized light and can be employed in 3D displays. Thus, the number of articles focusing on CPL spectroscopy has increased dramatically. However, since the luminescence dissymmetry factor (glum) for organic compounds is generally <|0.01|, CPL spectrometers must offer high sensitivity and produce spectra that are artifact-free for chiral molecules. Until now, the principal targets of CPL measurements have been solution samples. However, for practical device applications, it is also necessary to be able to measure the CPL spectra of solid-state samples. In addition, since electronic devices often operate at high temperatures, it is important to evaluate the thermal dependence of the CPL characteristics. Moreover, in the measurement of solid-state samples, the degree of anisotropy of the samples must be evaluated, because a large degree of anisotropy can cause artifacts. Therefore, we describe methods to evaluate the degree of anisotropy of solid-state samples and their high-temperature applications.

Highlights

  • Circularly polarized luminescence (CPL) spectroscopy has attracted attention in the study of optically active substances

  • Circular dichroism (CD) spectroscopy is used for structural analysis of the ground state of such substances, while circularly polarized luminescence (CPL) spectroscopy is a complementarily method that can obtain information about the excited state

  • The CPL signal is defined as the difference in luminescence intensity between left- and right-circularly polarized light, and the luminescence dissymmetry factor is defined as: glum

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Summary

INTRODUCTION

Circularly polarized luminescence (CPL) spectroscopy has attracted attention in the study of optically active substances. Kimoto et al (2013) reported that the sign of the CPL spectrum of binaphthyl fluorophores was reversed in a KBr pellet and a PMMA film. This suggests that it is possible to control the CPL properties by changing the environment of the chiral compound without using an enantiomer. There have been some reports on solid-state CPL measurements of samples in KBr pellets (Nishiguchi et al, 2011; Taniguchi et al, 2015) and PMMA films (Kimoto et al, 2012, 2013; Nakabayashi et al, 2014), the number of studies is still quite small. We describe methods to evaluate the degree of anisotropy of solid-state samples, and high-temperature measurement techniques for such samples

ARTIFACTS IN CPL MEASUREMENTS
PRINCIPLES OF CPL SPECTROSCOPY
CALIBRATION OF CPL SPECTROMETER
CPL MEASUREMENTS USING KBR PELLET METHOD
FUTURE PROSPECTS

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