Thiazolidinones: novel insights from microwave synthesis, computational studies, and potentially bioactive hybrids

• Luan A. Martinho,
• Victor H. J. G. Praciano,
• Guilherme D. R. Matos,
• Claudia C. Gatto and
• Carlos Kleber Z. Andrade

Beilstein J. Org. Chem. 2025, 21, 2618–2636, doi:10.3762/bjoc.21.203

• . Therefore, a study of the properties of both compounds was carried out. The spectroscopic data are summarized in Table 4. We first investigated their fluorescence properties through the quantum yield Φf by a comparative method with quinine sulfate, a standard of known quantum yield in 0.5 M H2SO4 (Φst

• = 0.546), with an excitation wavelength of 366 nm [83][84][85]. Nevertheless, no measurable quantum yield was observed for the fluorescence process. A solvatochromic study was conducted by measuring the UV–vis absorption and fluorescence spectra of compounds 3n (Figure 7) and 4n (Supporting Information

C2 to C6 biobased carbonyl platforms for fine chemistry

• Jingjing Jiang,
• Muhammad Noman Haider Tariq,
• Florence Popowycz,
• Yanlong Gu and
• Yves Queneau

Beilstein J. Org. Chem. 2025, 21, 2103–2172, doi:10.3762/bjoc.21.165

• ). Partial γ-acyloxy-Cy7 possesses a high fluorescence quantum yield and high photothermal conversion efficiency in PBS, two pivotal parameters in fluorescence imaging and image-guided photothermal therapy [196]. A dimerization of furfural has been found to occur at the early stage of formation of humins

Understanding the origin of stereoselectivity in the photochemical denitrogenation of 2,3-diazabicyclo[2.2.1]heptene and its derivatives with non-adiabatic molecular dynamics

• Leticia A. Gomes and
• Steven A. Lopez

Beilstein J. Org. Chem. 2025, 21, 2007–2020, doi:10.3762/bjoc.21.156

• products were the same those obtained by thermolysis, nitrogen and bicyclo[2.1.0]pentane with quantum yield approaching unity [64]. Engel and co-workers explored further the reaction using transient spectroscopic methods and discovered that the rate of N2 formation is significantly slower than that the S1

• static MEP calculation, the experimental quantum yield (Φ = 0.97–1.00) is inconsistent with this static analysis, since it suggests a non-productive and fluorescence pathway. We hypothesize that these S1 minima are shallow excited-state minima that can be escaped towards a productive region of the

• . Nevertheless, due to the challenges in consistently achieving 1.5 ps extensions while maintaining energy conservation, these trajectories were excluded from the statistical analysis of the housane quantum yield. The inverted housane exhibited the highest quantum yields, ranging from 0.69 to 0.79, consistent

Synthesis of N-doped chiral macrocycles by regioselective palladium-catalyzed arylation

• Shuhai Qiu and
• Junzhi Liu

Beilstein J. Org. Chem. 2025, 21, 1917–1923, doi:10.3762/bjoc.21.149

• , respectively. Correspondingly, 3a exhibits a deep blue emission at 453 nm with a quantum yield (ΦF) of 0.79, while a hypsochromic shift of the signal for 3b to 424 nm is observed and the ΦF value is decreased to 0.22 due to the electron-deficient character of the 3,5-bis(trifluoromethyl)phenyl groups. The

Photoswitches beyond azobenzene: a beginner’s guide

• Michela Marcon,
• Christoph Haag and
• Burkhard König

Beilstein J. Org. Chem. 2025, 21, 1808–1853, doi:10.3762/bjoc.21.143

• be easily calculated. According to the thermal half-life, photoswitches are usually classified in P-type (thermally stable, with long half-life) and T-type (thermally unstable) [3]. The quantum yield Φ measures the efficiency of the switching, and it relates the number of photons absorbed nx to the

• photoswitch can be switched before it is degraded by side reactions. It is typically reported as cyclability Z50, which “is the number of cycles required to reduce the initial absorbance at a specific wavelength by 50%” [3]. The quantum yield ΦS of these side reactions determines the resistance to fatigue of

• of the nπ* bands, which are used in the photoswitching process, are increased, leading to higher PSSs and higher excitation wavelengths, alongside with an excellent quantum yield in both directions. The bridge is also accountable for the much faster response to irradiation with respect to azobenzene

Thermodynamic equilibrium between locally excited and charge transfer states in perylene–phenothiazine dyads

• Issei Fukunaga,
• Shunsuke Kobashi,
• Yuki Nagai,
• Hiroki Horita,
• Hiromitsu Maeda and
• Yoichi Kobayashi

Beilstein J. Org. Chem. 2025, 21, 1577–1586, doi:10.3762/bjoc.21.121

• LE band of the Pe moiety. This result suggests that a stronger CT character leads to a lower overall fluorescence quantum yield. The Φf in other solvents are shown in Table S1 (Supporting Information File 1). In addition, a gradual increase in the emission intensity around 500–520 nm is observed with

Synthesis of an aza[5]helicene-incorporated macrocyclic heteroarene via oxidation of an o-phenylene-pyrrole-thiophene icosamer

• Yusuke Matsuo,
• Aoi Nakagawa,
• Shu Seki and
• Takayuki Tanaka

Beilstein J. Org. Chem. 2025, 21, 1561–1567, doi:10.3762/bjoc.21.119

• structural relaxation in the excited state. The fluorescence quantum yield (ΦF) was determined as 0.078 (λex = 300 nm), and the fluorescence lifetime (τ) using biexponential decay model fitting as 1.7 and 4.4 ns. The partially fused structure of 5 exhibited a well-defined lowest-energy absorption band peaked

Wittig reaction of cyclobisbiphenylenecarbonyl

• Taito Moribe,
• Junichiro Hirano,
• Hideaki Takano,
• Hiroshi Shinokubo and
• Norihito Fukui

Beilstein J. Org. Chem. 2025, 21, 1454–1461, doi:10.3762/bjoc.21.107

• , bis-olefin 5 fluoresces at 389 nm with a quantum yield of 7.5% and a lifetime of 6.0 ns. The radiative and non-radiative decay rate constants are calculated to be 1.3 × 107 s−1 and 1.5 × 108 s−1, respectively. The CD spectra and the dissymmetry factors (g) of enantiomers of CBBC 1, mono-olefin 3, and

• exist as an equilibrium mixture, in which the bathtub conformation is rather preferable at low temperature. Mono-olefin 3 and bis-olefin 5 exhibit enhanced configurational persistency compared to CBBC 1. Bis-olefin 5 fluoresces with a quantum yield of 7.5%, while CBBC 1 is non-emissive under ambient

Advances in nitrogen-containing helicenes: synthesis, chiroptical properties, and optoelectronic applications

• Meng Qiu,
• Jing Du,
• Nai-Te Yao,
• Xin-Yue Wang and
• Han-Yuan Gong

Beilstein J. Org. Chem. 2025, 21, 1422–1453, doi:10.3762/bjoc.21.106

• absorption and emission maxima (λabs = 399 nm, λem = 405 nm), a fluorescence quantum yield (ΦF) of 0.13, and high dissymmetry factors (|gabs| = 1.9 × 10−2, |gabs| = 9.5 × 10−3 at 403 nm) [18] (Table 2). Miura and co-workers employed Pd(II)/Ag(I)-catalyzed cyclizations to construct azahelicenes, with compound

• in solution and structurally confirmed via single-crystal X-ray diffraction. It demonstrated the highest CPL performance among the series, with a |glum| value of 3.5 × 10−3 and a photoluminescence quantum yield (PLQY) of 0.31, indicating its potential as a chiral emissive material. Building upon this

• substituent on the azahelicene core, the resulting boryl-functionalized compound 42c exhibited an emission maximum at 563 nm in CH2Cl2, with a quantum yield of 15%, representing the highest emission efficiency observed among the boron-containing quasi-circulenes. In 2022, Lu and co-workers developed a series

Recent advances in oxidative radical difunctionalization of N-arylacrylamides enabled by carbon radical reagents

• Jiangfei Chen,
• Yi-Lin Qu,
• Ming Yuan,
• Xiang-Mei Wu,
• Heng-Pei Jiang,
• Ying Fu and
• Shengrong Guo

Beilstein J. Org. Chem. 2025, 21, 1207–1271, doi:10.3762/bjoc.21.98

Biobased carbon dots as photoreductants – an investigation by using triarylsulfonium salts

• Valentina Benazzi,
• Arianna Bini,
• Ilaria Bertuol,
• Mariangela Novello,
• Federica Baldi,
• Matteo Hoch,
• Alvise Perosa and
• Stefano Protti

Beilstein J. Org. Chem. 2025, 21, 1024–1030, doi:10.3762/bjoc.21.84

• tail extending to the visible region. The emission properties of the synthesized CDs were also investigated and the results are summarized in Table 2. The fluorescence quantum yield strongly depends on the nature of the starting substrates, as is apparent by comparison of the value obtained for

On the photoluminescence in triarylmethyl-centered mono-, di-, and multiradicals

• Daniel Straub,
• Markus Gross,
• Mona E. Arnold,
• Julia Zolg and
• Alexander J. C. Kuehne

Beilstein J. Org. Chem. 2025, 21, 964–998, doi:10.3762/bjoc.21.80

• photoluminescence quantum yield (ϕ) combined with improved photostability. The spin-allowed transition from the excited doublet state to the ground state [7][8][9][10][11][12][13], combined with the absence of competing triplet states – which is a major pathway of efficiency loss in closed-shell emitters – promises

• mechanisms and reasons behind the fluorescence color and the fluorescence quantum yield and derive structure–optical property relationships. We will provide the reader with an overview of the perspectives and challenges of open-shell light-emitting radicals and discuss what to do to solve the remaining

Study of tribenzo[b,d,f]azepine as donor in D–A photocatalysts

• Katy Medrano-Uribe,
• Jorge Humbrías-Martín and
• Luca Dell’Amico

Beilstein J. Org. Chem. 2025, 21, 935–944, doi:10.3762/bjoc.21.76

• ), and 5c (3.7 eV). At the same time, 5a and 5b showed bigger values (3.9 eV and 4.0 eV, respectively) (Figure 2). The strength of common donors plays a crucial role in influencing quantum yield (QY) measurements. As shown in Table 1, we observe a notable decrease in QY across the PCs 5e, 5d, and 5c

Substituent effects in N-acetylated phenylazopyrazole photoswitches

• Radek Tovtik,
• Dennis Marzin,
• Pia Weigel,
• Stefano Crespi and
• Nadja A. Simeth

Beilstein J. Org. Chem. 2025, 21, 830–838, doi:10.3762/bjoc.21.66

• bathochromic shift of the n→π* absorption band further moving their UV–vis absorption spectrum towards the therapeutic window [35]. Moreover, a similar modification in stilbene-based photoswitches and molecular motors showed an increase in performance and photoisomerization quantum yield [36][37]. Consequently

• the n→π* transition is selectively addressed, with similar or markedly reduced quantum yields. A deviation from Kasha's rule with the opposite outcome (viz. the quantum yield of isomerization proceeding from the excitation of the π→π* state is lower than the one from the n→π*) is reported in various

• in CH3CN. UV–vis absorption maxima of Z-PAP derivatives in CH3CN (obtained through 365 nm irradiation to the corresponding PSS365). PSS distribution of various NAc-PAP derivatives.a Quantum yield values for the E→Z and Z→E photoisomerization of PAP derivatives with the corresponding 365 nm and 445 nm

Photochemically assisted synthesis of phenacenes fluorinated at the terminal benzene rings and their electronic spectra

• Yuuki Ishii,
• Minoru Yamaji,
• Fumito Tani,
• Kenta Goto,
• Yoshihiro Kubozono and
• Hideki Okamoto

Beilstein J. Org. Chem. 2025, 21, 670–679, doi:10.3762/bjoc.21.53

• processes contributing to the low fluorescence quantum yield of the F8-phenacenes (cf. Table 1). Because fluorescence behavior in the solid state reflects molecular alignment and intermolecular interactions in the crystals, solid-state fluorescence of the F8-phenacenes was investigated. We observed

Deep-blue emitting 9,10-bis(perfluorobenzyl)anthracene

• Long K. San,
• Sebastian Balser,
• Brian J. Reeves,
• Tyler T. Clikeman,
• Yu-Sheng Chen,
• Steven H. Strauss and
• Olga V. Boltalina

Beilstein J. Org. Chem. 2025, 21, 515–525, doi:10.3762/bjoc.21.39

• photochemical reaction. Its structure was elucidated by NMR spectroscopy and single crystal X-ray diffractometry. The latter revealed no π–π interaction between neighboring ANTH cores. A combination of high photoluminescence quantum yield (PLQY) of 0.85 for 9,10-ANTH(BnF)2, its significantly improved

• -emitting device. The photophysical data of ANTH and 9,10-disubstituted anthracene derivatives are summarized in Table 1. The measured photoluminescence quantum yield, PLQY (Φf) of ANTH in cyclohexane is in agreement with the literature values of 0.28–0.36 [32][33][34][35]. An increase in Φf was previously

Unprecedented visible light-initiated topochemical [2 + 2] cycloaddition in a functionalized bimane dye

• Metodej Dvoracek,
• Brendan Twamley,
• Mathias O. Senge and
• Mikhail A. Filatov

Beilstein J. Org. Chem. 2025, 21, 500–509, doi:10.3762/bjoc.21.37

• suggest potential triplet-state formation, which is involved in the proposed mechanism for the cycloaddition reaction. Although Me4B could theoretically form triplet states, given its fluorescence quantum yield of 51.7–67.3%, its crystallographic structure is not conducive to this reaction, regardless of

• fluorescence spectra are presented in Supporting Information File 1 (Figures S12–S14). For the fluorescence quantum yield measurements, solutions of each bimane were prepared, and the concentration was adjusted so that the absorbance at the right shoulder of the band at 360 nm falls within the range of 0.03

• reference (Φfl = 33%) [19]. Quantum yields were calculated using the following formula (Equation 1): where Φs is the fluorescence quantum yield of the analyte and Φref is the fluorescence quantum yield of the reference, Abs is the absorbance at the excitation wavelength, Area is the area under the

Synthesis of N-acetyl diazocine derivatives via cross-coupling reaction

• Thomas Brandt,
• Pascal Lentes,
• Jeremy Rudtke,
• Michael Hösgen,
• Christian Näther and
• Rainer Herges

Beilstein J. Org. Chem. 2025, 21, 490–499, doi:10.3762/bjoc.21.36

• Abstract Diazocines are photoswitches derived from azobenzenes by bridging the two phenyl rings in ortho position with a CH2CH2 group forming an eight membered (diazocine) ring. Diazocine is superior to most azobenzenes in almost all photophysical properties (switching efficiency, quantum yield

Red light excitation: illuminating photocatalysis in a new spectrum

• Lucas Fortier,
• Corentin Lefebvre and
• Norbert Hoffmann

Beilstein J. Org. Chem. 2025, 21, 296–326, doi:10.3762/bjoc.21.22

• transition-metal-based photosensitizers acting by triplet energy transfer for which high singlet oxygen quantum yields are crucial, the silicon phthalocyanins in this study have exhibited relatively low singlet oxygen quantum yield values (around 0.27 for the silicon-based photocatalysts used in this work

Synthesis and characterizations of highly luminescent 5-isopropoxybenzo[rst]pentaphene

• Islam S. Marae,
• Jingyun Tan,
• Rengo Yoshioka,
• Zakaria Ziadi,
• Eugene Khaskin,
• Serhii Vasylevskyi,
• Ryota Kabe,
• Xiushang Xu and
• Akimitsu Narita

Beilstein J. Org. Chem. 2025, 21, 270–276, doi:10.3762/bjoc.21.19

• properties were investigated by UV–vis absorption and fluorescence spectroscopy in compassion to pristine BPP and its oxidation product, benzo[rst]pentaphene-5,8-dione (BPP-dione). BPP-OiPr exhibited a significantly enhanced photoluminescence quantum yield (PLQY), reaching 73% in comparison to pristine BPP

• ], perylene [18][19], and coronene [20]. Besides their limited accessibility in the past, the lack of attention to BPP can presumably be ascribed to its low photoluminescence quantum yield (PLQY). We recently reported a PLQY of 13% for pristine BPP and revealed a symmetry-forbidden nature of its first excited

Streamlined modular synthesis of saframycin substructure via copper-catalyzed three-component assembly and gold-promoted 6-endo cyclization

• Asahi Kanno,
• Ryo Tanifuji,
• Satoshi Yoshida,
• Sota Sato,
• Saori Maki-Yonekura,
• Kiyofumi Takaba,
• Jungmin Kang,
• Kensuke Tono,
• Koji Yonekura and
• Hiroki Oguri

Beilstein J. Org. Chem. 2025, 21, 226–233, doi:10.3762/bjoc.21.14

• displayed a relatively broad peak with a maximum around 490 nm (blue solid line). The excitation spectra of 18 (blue dashed line), corresponding to an emission at 490 nm, was also recorded (Figure S3, Supporting Information File 1 for details). Despite the modest emission quantum yield (Φfl = 0.07, excited

Synthesis, structure and π-expansion of tris(4,5-dehydro-2,3:6,7-dibenzotropone)

• Yongming Xiong,
• Xue Lin Ma,
• Shilong Su and
• Qian Miao

Beilstein J. Org. Chem. 2025, 21, 1–7, doi:10.3762/bjoc.21.1

• orange solution in common organic solvents, and its solution in cyclohexane exhibits very weak orange photoluminescence with a quantum yield as low as 3.9 × 10−4 upon excitation at 400 nm. Such a low photoluminescence quantum yield may be attributed to the conformational motions of the helicene moieties

Efficient synthesis of fluorinated triphenylenes with enhanced arene–perfluoroarene interactions in columnar mesophases

• Yang Chen,
• Jiao He,
• Hang Lin,
• Hai-Feng Wang,
• Ping Hu,
• Bi-Qin Wang,
• Ke-Qing Zhao and
• Bertrand Donnio

Beilstein J. Org. Chem. 2024, 20, 3263–3273, doi:10.3762/bjoc.20.270

• been studied in various solutions and thin film: G66 emitted green light in solution with an absolute photoluminescent quantum yield of ca. 33%. Results and Discussion Synthesis and characterization We have recently generalized a very efficient “palladium-free” synthesis for the preparation of a

Advances in the use of metal-free tetrapyrrolic macrocycles as catalysts

• Mandeep K. Chahal

Beilstein J. Org. Chem. 2024, 20, 3085–3112, doi:10.3762/bjoc.20.257

• splitting, high quantum yield for intersystem crossing, and long triplet state lifetime, act as robust electron mediators. This section highlights the use of metal-free porphyrins in organic photoredox catalysis. So far, mainly planar metal-free porphyrins have been explored as photoredox catalysts, paving

Extension of the π-system of monoaryl-substituted norbornadienes with acetylene bridges: influence on the photochemical conversion and storage of light energy

• Robin Schulte,
• Dustin Schade,
• Thomas Paululat,
• Till J. B. Zähringer,
• Christoph Kerzig and
• Heiko Ihmels

Beilstein J. Org. Chem. 2024, 20, 3061–3068, doi:10.3762/bjoc.20.254

• , such as absorption in the range of the solar spectrum, a high quantum yield of the photoreaction, long half-lives of the photoproducts, and a high energy storage density [7][8][12][13][14]. In this context, several different MOST systems have been explored, including, for example, anthracenes [15

• sunlight. Furthermore, the photoisomerization quantum yield is very low and therefore not suitable for an application [7][8][14]. One promising way to overcome these disadvantages is the introduction of a donor–acceptor system at the norbornadiene double bonds, which has resulted in the development of new

• and the analogues 1c and 1e without an alkyne linker [29][30][34]. As the only exception, the m-substituted derivative 1k has a higher quantum yield than its analog 1b, which is, however, still lower than the one of the cyano-substituted norbornadiene 1c [30][34]. In addition, substitution at the 2