Understanding X-ray-induced isomerisation in photoswitchable surfactant assemblies

• Beatrice E. Jones,
• Camille Blayo,
• Jake L. Greenfield,
• Matthew J. Fuchter,
• Nathan Cowieson and
• Rachel C. Evans

Beilstein J. Org. Chem. 2024, 20, 2005–2015, doi:10.3762/bjoc.20.176

• (365 nm, irradiance = 6.00 mW⋅cm−2), blue (455 nm, 5.16 mW⋅cm−2) or green (525 nm, 0.06 mW⋅cm−2) light. For the SAXS studies at high concentration, samples were irradiated in a custom-build LED light box with UV (365 nm) light at an irradiance of 1.24 mW⋅cm−2 for 3.5 h. This resulted in 98 ± 2 and 71

Allostreptopyrroles A–E, β-alkylpyrrole derivatives from an actinomycete Allostreptomyces sp. RD068384

• Marwa Elsbaey,
• Naoya Oku,
• Mohamed S. A. Abdel-Mottaleb and
• Yasuhiro Igarashi

Beilstein J. Org. Chem. 2024, 20, 1981–1987, doi:10.3762/bjoc.20.174

• total 6.5 mg of 1, 3.1 mg of 2, 2.6 mg of 3, 7.2 mg of 4, and 5.6 mg of 5 from 12 L culture. Allostreptopyrrole A (1): greenish yellow amorphous solid; UV (MeOH) λmax nm (log ε) 234 (3.86), 273 sh (3.44); IR (ATR) νmax: 3275, 2964, 2928, 2855, 1658, 1554, 1418 cm−1; 1H and 13C NMR data, see Table 1

• ; HRESITOFMS (m/z): [M – H]– calcd for C15H22NO4, 280.1554; found, 280.1550. Allostreptopyrrole B (2): greenish yellow amorphous solid; +15 (c 0.10, MeOH); UV (MeOH) λmax, nm (log ε): 235 (3.87), 273 sh (3.49); IR (ATR) νmax: 3263, 2964, 2925, 2854, 1658, 1556, 1417 cm−1; 1H and 13C NMR data, see Table 2

• ; HRESITOFMS (m/z): [M – H]– calcd for C15H22NO4, 280.1554; found, 280.1554. Allostreptopyrrole C (3): greenish yellow amorphous solid; −6.1 (c 0.10, MeOH); UV (MeOH) λmax, nm (log ε): 235 (3.82), 276 sh (3.46); IR (ATR) νmax: 3265, 2925, 2856, 1657, 1555, 1417 cm−1; 1H and 13C NMR data, see Table 2

Regioselective alkylation of a versatile indazole: Electrophile scope and mechanistic insights from density functional theory calculations

• Pengcheng Lu,
• Luis Juarez,
• Paul A. Wiget,
• Weihe Zhang,
• Krishnan Raman and
• Pravin L. Kotian

Beilstein J. Org. Chem. 2024, 20, 1940–1954, doi:10.3762/bjoc.20.170

• (dd, J = 8.9, 1.9 Hz, 1H), 4.17 (s, 3H), 3.92 (s, 3H); 13C{1H} NMR (75 MHz, DMSO-d6) δ 161.8, 139.4, 132.7, 129.4, 124.1, 123.0, 116.0, 113.0, 51.8, 36.6; IR (KBr disk): 1722, 1466, 1433, 1395, 1354, 1289, 1200, 1183, 1153 cm−1; HRESIMS (m/z): [M + H]+ calcd for C10H10BrN2O2+, 268.9921; found

• (s, 3H); 13C{1H} NMR (75 MHz, DMSO-d6) δ 159.4, 144.7, 129.3, 123.6, 123.2, 122.8, 120.0, 118.0, 64.2, 52.2, 41.4, 14.4, 13.9; IR (KBr disk): 1708, 1459, 1442, 1392, 1326, 1252, 1196 cm−1; HRESIMS (m/z): [M + H]+ calcd for C10H10BrN2O2+, 268.9921; found, 268.9918. Indazole-containing bioactive

A new platform for the synthesis of diketopyrrolopyrrole derivatives via nucleophilic aromatic substitution reactions

• Vitor A. S. Almodovar and
• Augusto C. Tomé

Beilstein J. Org. Chem. 2024, 20, 1933–1939, doi:10.3762/bjoc.20.169

• chromatography (TLC) was carried out on precoated sheets with silica gel (Merck 60, 0.2 mm thick). Preparative TLC was carried out on 20 cm × 20 cm glass plates precoated with a layer of silica gel 60 (0.5 mm thick) and activated in an oven at 100 °C for 12 h. Melting points were determined with a Büchi B-540

The Groebke–Blackburn–Bienaymé reaction in its maturity: innovation and improvements since its 21st birthday (2019–2023)

• Cristina Martini,
• Muhammad Idham Darussalam Mardjan and
• Andrea Basso

Beilstein J. Org. Chem. 2024, 20, 1839–1879, doi:10.3762/bjoc.20.162

A facile three-component route to powerful 5-aryldeazaalloxazine photocatalysts

• Ivana Weisheitelová,
• Radek Cibulka,
• Marek Sikorski and
• Tetiana Pavlovska

Beilstein J. Org. Chem. 2024, 20, 1831–1838, doi:10.3762/bjoc.20.161

• characteristic band at 353 nm (ε = 24.4 × 103 M−1.cm−1), while it moved to 370 nm for 7,8-dimethoxydeazaalloxazine 2f (ε = 26.2 × 103 M−1.cm−1) and even to 387 nm (ε = 12.2 × 103 M−1.cm−1) for 7-methoxydeazaalloxazine 2j. This indicates that, besides the 7,8-dimethoxy derivatives usually studied in deazaflavin

• -aryldeazaalloxazine (2). (C) This work, which describes an efficient three-component method for the synthesis of 2. UV–vis absorption spectra of 5-arydeazaalloxazines 2f, 2j and 2n in DMF (l = 1 cm, c = 2.50 × 10−5 mol·L−1). Three-component condensation of anilines, aldehydes and N,N-dimethylbarbituric acid

Methyltransferases from RiPP pathways: shaping the landscape of natural product chemistry

• Maria-Paula Schröder,
• Isabel P.-M. Pfeiffer and
• Silja Mordhorst

Beilstein J. Org. Chem. 2024, 20, 1652–1670, doi:10.3762/bjoc.20.147

• first RiPP to be isolated from Myxobacteria. It was specifically isolated from Chondromyces crocatus Cm C5. The core peptide is composed of only three amino acids: isoleucine, tyrosine, and tryptophan. It forms a tetracyclic core system that contains a tetrahydropyrroloindoline, which is unprecedented

New triazinephosphonate dopants for Nafion proton exchange membranes (PEM)

• Fátima C. Teixeira,
• António P. S. Teixeira and
• C. M. Rangel

Beilstein J. Org. Chem. 2024, 20, 1623–1634, doi:10.3762/bjoc.20.145

• usually the best weight loading for doped Nafion membranes. The FTIR-ATR spectra of Nafion membranes (Supporting Information File 1, Figure S1) showed the characteristic very strong and broad absorption bands of Nafion near 1200 and 1145 cm−1 due to the C–F stretching vibration [59][60][61][62][63]. The

• observed in the spectra of new membranes compared to commercial Nafion [64]. Other characteristic bands of S–O group, CF2–CF and C–O–C are observed at near 1050, 980 and 960 cm−1, respectively, in the FTIR spectra [63]. The proton conductivity of the new proton exchange membrane is a key property relevant

• of the membranes was carried out on a Perkin Elmer Spectrum Two, with an attenuated total reflectance (ATR) module, with a wavenumber range from 450 to 4000 cm−1, and their band wavelengths are quoted in cm−1. Low-resolution and high-resolution (HRMS) mass spectra (MS) were performed on an APEX-Q

Supramolecular assemblies of amphiphilic donor–acceptor Stenhouse adducts as macroscopic soft scaffolds

• Ka-Lung Hung,
• Leong-Hung Cheung,
• Yikun Ren,
• Ming-Hin Chau,
• Yan-Yi Lam,
• Takashi Kajitani and
• Franco King-Chi Leung

Beilstein J. Org. Chem. 2024, 20, 1590–1603, doi:10.3762/bjoc.20.142

• heating. Flash column chromatography was performed using Macherey-Nagel silica gel 60 (230–400 mesh). Deuterated solvents were purchased from Cambridge Isotope Laboratories. UV–vis spectroscopy UV–vis measurements were performed on an Agilent Cary 60 UV–vis spectrophotometer with a quartz cuvette of 1 cm

• source (380–800 nm, 300 W) positioned at a distance of 1 cm from the sample. Preparation of aqueous samples All aqueous solutions of DAn were prepared according to the following general procedure: DAn (5.0 wt %) was mixed with 1.0 equivalent NaOH in Milli-Q water. The obtained aqueous solution was

• normalized by the concentration of the solution to yield the molar scattering intensity. Ten replications were performed, and the data was averaged to show the molar scattering intensity and the error standard deviation. WAXD WAXD of DA scaffolds was measured on a sapphire substrate (φ = 2.0 cm) using a

Electrocatalytic hydrogenation of cyanoarenes, nitroarenes, quinolines, and pyridines under mild conditions with a proton-exchange membrane reactor

• Koichi Mitsudo,
• Atsushi Osaki,
• Haruka Inoue,
• Eisuke Sato,
• Naoki Shida,
• Mahito Atobe and
• Seiji Suga

Beilstein J. Org. Chem. 2024, 20, 1560–1571, doi:10.3762/bjoc.20.139

• reduced to 25 F mol−1 when decreasing the current density to 25 mA cm−2, and 7a was obtained in 90% yield (see the Supporting Information File 1). Next, the substrate scope was examined under optimal conditions (Scheme 4). Substrates bearing a methyl group afforded the corresponding products in high

• mmol; solvent, CH2Cl2 (0.5 M); flow rate of the solution of 6a, 0.75 mL min−1; flow rate of H2 gas, 100 mL min−1; reaction temperature, room temperature; current density, 50 mA cm−2. The solution was circulated until the passage of 50 F mol−1 (10 h). The yields were determined by 1H NMR analysis using

• H2 gas, 100 mL min−1; reaction temperature, room temperature; current density, 50 mA cm−2 (10 h). The solution was circulated until the passage of 50 F mol−1. The yields were determined by 1H NMR analysis using 1,1,2,2-tetrachloroethane as an internal standard. Plausible mechanism for the reduction

Tetrabutylammonium iodide-catalyzed oxidative α-azidation of β-ketocarbonyl compounds using sodium azide

• Christopher Mairhofer,
• David Naderer and
• Mario Waser

Beilstein J. Org. Chem. 2024, 20, 1510–1517, doi:10.3762/bjoc.20.135

• = 17.2 Hz, 1H), 2.99 (d, J = 17.2 Hz, 1H), 1.45 (s, 9H); 13C NMR (75 MHz, CDCl3, 298 K, δ/ppm) 198.1, 167.4, 152.3, 136.4, 133.3, 128.4, 126.5, 125.6, 84.6, 70.6, 38.6, 28.0; IR (neat, FT-ATR, 298 K, ν̃/cm−1): 2984, 2928, 2853, 2110, 1747, 1736, 1718, 1604, 1589, 1548, 1466, 1431, 1397, 1372, 1353, 1326

• , 1H), 7.48 (t, J = 7.5 Hz, 1H), 4.11 (d, J = 17.9 Hz, 1H), 3.99 (d, J = 17.9 Hz, 1H), 1.49 (s, 9H); 13C NMR (126 MHz, CDCl3, 298 K, δ/ppm) 188.4, 162.0, 150.1, 137.0, 132.9, 129.1, 126.5, 126.2, 96.7, 86.1, 37.5, 27.8; IR (neat, FT-ATR, 298 K, ν̃/cm−1): 2984, 2930, 2878, 2854, 1748, 1719, 1656, 1604

Towards an asymmetric β-selective addition of azlactones to allenoates

• Behzad Nasiri,
• Ghaffar Pasdar,
• Paul Zebrowski,
• Katharina Röser,
• David Naderer and
• Mario Waser

Beilstein J. Org. Chem. 2024, 20, 1504–1509, doi:10.3762/bjoc.20.134

• reported in terms of frequency of absorption (cm−1). HPLC was performed using a Shimadzu Prominence system with a diode array detector with a CHIRALPAK AD-H, CHIRAL ART Amylose-SA, (250 × 4.6 mm, 5 µm) chiral stationary phase. Optical rotations were recorded on a Schmidt + Haensch Polarimeter Model UniPol

• ), 3.52–3.16 (m, 4H), 1.15 (t, J = 7.1 Hz, 3H); 13C NMR (75 MHz, CDCl3, 298.0 K) δ/ppm = 177.4, 171.0, 160.3, 139.1, 133.8, 132.6, 130.5, 128.6, 128.0, 127.8, 127.3, 125.6, 118.1, 75.9, 60.9, 44.9, 39.3, 13.9; IR (neat): 3080, 3070, 2917, 1815, 1732, 1656, 1480, 1175, 1093, 1059, 1030, 974, 893, 694 cm−1

Rapid construction of tricyclic tetrahydrocyclopenta[4,5]pyrrolo[2,3-b]pyridine via isocyanide-based multicomponent reaction

• Xiu-Yu Chen,
• Ying Han,
• Jing Sun and
• Chao-Guo Yan

Beilstein J. Org. Chem. 2024, 20, 1436–1443, doi:10.3762/bjoc.20.126

• , 58.2, 56.7, 55.2, 53.3, 52.2, 51.3, 50.4, 50.2, 32.4, 31.5, 31.2, 26.2, 25.7, 25.6, 18.2 ppm; IR (KBr) ν: 3435, 2931, 2862, 2360, 1737, 1698, 1587, 1547, 1435, 1385, 1335, 1251, 1204, 1125, 1092, 1001, 977, 895, 853, 792 cm−1; HRESIMS (m/z): [M + Na]+ calcd. for C41H46NaN2O11, 765.2994; found, 765.2993

Diameter-selective extraction of single-walled carbon nanotubes by interlocking with Cu-tethered square nanobrackets

• Guoqing Cheng and
• Naoki Komatsu

Beilstein J. Org. Chem. 2024, 20, 1298–1307, doi:10.3762/bjoc.20.113

• than that of 1a (9.74 Å), implying preference of 1b to larger diameter of SWNTs. In the Raman spectra at 488 nm excitation wavelength, 1a and 1b show the signals at similar wavenumbers in the range of 400–1200 cm−1 (Figure 2c and Figure S1 in Supporting Information File 1). The spectra are almost

• in Figure 3b, all the materials were analyzed with Raman spectroscopy in the solid phase with normalization at G-band (1570 cm−1) of SWNTs. The characteristic signals from Cu-nanobrackets 1b are observed in e- and i-SWNTs, but not in p-SWNTs, indicating the interlocking of SWNTs with 1b, because the

• breathing vibration, resulting in higher frequency shift as shown in Figure 4 [11][26]. With normalization in G-band at 1570 cm−1, the relative intensity decreases in the RBM region of e- and i-SWNTs may be due to light absorption and/or peak broadening caused by the interlocking Cu-nanobrackets 1b

Synthesis and physical properties of tunable aryl alkyl ionic liquids based on 1-aryl-4,5-dimethylimidazolium cations

• Stefan Fritsch and
• Thomas Strassner

Beilstein J. Org. Chem. 2024, 20, 1278–1285, doi:10.3762/bjoc.20.110

• than the alkyl chain length. The conductivity of the unsubstituted TAAIL 37 with 319 μS cm−1 is the highest among the investigated 4,5-dimethylimidazolium based TAAILs (Figure 2, Table 3). This is supported by the corresponding observation that TAAIL 37 also shows the lowest viscosity. As a result of

• their high viscosity, the 4-Br substituted TAAILs 46 and 47 display the lowest conductivities (96 and 62 μS cm−1, respectively). To visualize the correlation between conductivity and viscosity, the conductivity is plotted against the viscosity in Figure 3. The 4-OCF3 substituted TAAIL 52 shows a similar

• viscosity to TAAIL 37, the conductivity, however, is much lower (198 μS cm−1), demonstrating the influence of the perfluorinated 4-OCF3 group on the conductivity. Changing the position of the methyl and methoxy substituent from ortho to para leads to an increase in conductivity. Overall, longer alkyl chains

Synthesis of indano[60]fullerene thioketone and its application in organic solar cells

• Yong-Chang Zhai,
• Shimon Oiwa,
• Shinobu Aoyagi,
• Shohei Ohno,
• Tsubasa Mikie,
• Jun-Zhuo Wang,
• Hirofumi Amada,
• Koki Yamanaka,
• Kazuhira Miwa,
• Naoyuki Imai,
• Takeshi Igarashi,
• Itaru Osaka and
• Yutaka Matsuo

Beilstein J. Org. Chem. 2024, 20, 1270–1277, doi:10.3762/bjoc.20.109

• -functionalized compound (t-Bu-FIDS) was chosen for further studies in this work. To identify the formation of the thiocarbonyl group, Fourier transform infrared spectroscopy (FTIR) was conducted as shown in Figure 1a. The carbonyl stretching vibration peak of t-Bu-FIDO at 1720 cm−1 disappeared, indicating all

• the t-Bu-FIDO was completely consumed. Interestingly, the characteristic vibration peak of thiocarbonyl groups was not observed, which should be located at 1050–1300 cm−1 theoretically. Instead, numerous new low-intensity peaks were observed in this region. To gain a comprehensive understanding of the

• around 1000 cm−1 for t-Bu-FIDS. Ultraviolet–visible (UV–vis) spectroscopy of t-Bu-FIDS in o-DCB exhibited two prominent UV absorption bands with peaks at 257 nm and 320 nm (Figure 1b). The absorption at 257 nm indicated the integrity of the fullerene cage chromophore. The absorption peak at 320 nm was

Mechanistic investigations of polyaza[7]helicene in photoredox and energy transfer catalysis

• Johannes Rocker,
• Till J. B. Zähringer,
• Matthias Schmitz,
• Till Opatz and
• Christoph Kerzig

Beilstein J. Org. Chem. 2024, 20, 1236–1245, doi:10.3762/bjoc.20.106

• extinction coefficient, Δε455(Rubpy*) = −10100 M−1 cm−1 [37][79], following excitation (Figure 4B). 0.3 mM methyl viologen (MV2+) were added to Aza-H to quantitatively quench the triplet-excited photocatalyst in an electron transfer reaction yielding Aza-H•+ and MV•+, which are clearly observed in the TA

• the reliability of our procedure. Taking the literature-known extinction coefficient of the methyl viologen radical cation Δε395(MV•+) ≈ 39000 M−1 cm−1 [82] to calculate its concentration and the initial Aza-H excited-state concentration obtained through Rubpy* actinometry allows us to determine the

• (distance 6 cm) was used as the excitation light source. D) Irradiation experiments of (E)-stilbene (blue) and (Z)-stilbene (red) with 2 mol % Aza-H employing a 427 nm LED as light source. E) Schematic energy diagram of triplet sensitized E/Z isomerization of stilbene. F) Reaction scheme of the cyclization

Competing electrophilic substitution and oxidative polymerization of arylamines with selenium dioxide

• Vishnu Selladurai and
• Selvakumar Karuthapandi

Beilstein J. Org. Chem. 2024, 20, 1221–1235, doi:10.3762/bjoc.20.105

• benzenoid→quinonoid excitonic transitions, respectively, which was characteristic of polyaniline existing as emeraldine free base [41][42]. The polyaniline nature was further confirmed by FTIR spectroscopy (Figure S2, Supporting Information File 1). The broad peak observed in the range of 3300–3400 cm−1 was

• due to N–H stretching of the polymer [43][44]. The peak appearing at around 3000 cm−1 corresponded to the aryl C–H stretching. The peaks observed at 1593 and 1479 cm−1 were associated with C=C and C=N stretching, respectively. The obtained result was further supported by solid-state synthesis of

• , 1282, 1073, 820, 752 cm−1. N1,N2-Diphenyloxalamide (3): Colorless solid (2.6 mg, 0.22%); mp 231–232 °C; 1H NMR (500 MHz, CDCl3, δ) 9.36 (s, 2H), 7.70 (d, J = 7.9 Hz, 4H), 7.44 (t, J = 7.8 Hz, 4H), 7.25 (t, J = 7.5 Hz, 2H); HRESIMS (m/z): [M + CH3COOH + H]+ calcd for C16H17N2O4, 301.1183; found

Cofactor-independent C–C bond cleavage reactions catalyzed by the AlpJ family of oxygenases in atypical angucycline biosynthesis

• Jinmin Gao,
• Liyuan Li,
• Shijie Shen,
• Guomin Ai,
• Bin Wang,
• Fang Guo,
• Tongjian Yang,
• Hui Han,
• Zhengren Xu,
• Guohui Pan and
• Keqiang Fan

Beilstein J. Org. Chem. 2024, 20, 1198–1206, doi:10.3762/bjoc.20.102

• the stable CM• radical through electron paramagnetic resonance. Based on previous studies of cofactor-independent oxygenases and our results, we propose a radical-mediated catalytic mechanism for the cofactor-independent AlpJ-family oxygenases (Scheme 2). The catalytic cascade was initiated by

Synthesis of 1,4-azaphosphinine nucleosides and evaluation as inhibitors of human cytidine deaminase and APOBEC3A

• Maksim V. Kvach,
• Stefan Harjes,
• Harikrishnan M. Kurup,
• Geoffrey B. Jameson,
• Elena Harjes and
• Vyacheslav V. Filichev

Beilstein J. Org. Chem. 2024, 20, 1088–1098, doi:10.3762/bjoc.20.96

• anomers with a α/β ratio of 2:1, as determined by 1H and 13C NMR. Deprotected nucleosides Va and Vb but not Vc exhibited absorbance in the UV region with ε258 = 4230 L⋅mol−1⋅cm−1 and ε262 = 4730 L⋅mol−1⋅cm−1, respectively. This was most likely a result of the presence of a double bond next to the P=O unit

Light on the sustainable preparation of aryl-cored dibromides

• Fabrizio Roncaglia,
• Alberto Ughetti,
• Nicola Porcelli,
• Biagio Anderlini,
• Andrea Severini and
• Luca Rigamonti

Beilstein J. Org. Chem. 2024, 20, 1076–1087, doi:10.3762/bjoc.20.95

• ), solvent (either CH2Cl2 or chlorobenzene, 1.0–4.0 mL), H2O (1.5 mL), and HBr (48 wt % aqueous solution, d = 1.49 g/mL, 1.25 mL, 11 mmol, 2.2 equiv) were inserted. The mixture was kept under stirring at rt and irradiated with a LED lightbulb placed at 10 cm from the side of the reaction tube. Aqueous H2O2

• at rt, H2O (3.6 mL) and HBr (48 wt % aqueous solution, 3.00 mL, 26.5 mmol, 2.2 equiv) were inserted. The mixture was then irradiated with a LED lightbulb, placed at 10 cm from the side of the flask and aqueous H2O2 (35 wt % solution, 4.8 mL, 56 mmol, 4.7 equiv) was added over 2 h using a syringe pump

• mixture was kept under stirring at rt and irradiated with a LED lightbulb placed at 10 cm from the side of the reaction tube. Aqueous H2O2 (35 wt % solution, 3.0 mL, 23.3 mmol, 4.7 equiv) was added over 2 h using a syringe pump, through a small PTFE tube inserted through the side arm of the Schlenk. After

Structure–property relationships in dicyanopyrazinoquinoxalines and their hydrogen-bonding-capable dihydropyrazinoquinoxalinedione derivatives

• Tural N. Akhmedov,
• Ajeet Kumar,
• Daken J. Starkenburg,
• Kyle J. Chesney,
• Khalil A. Abboud,
• Novruz G. Akhmedov,
• Jiangeng Xue and
• Ronald K. Castellano

Beilstein J. Org. Chem. 2024, 20, 1037–1052, doi:10.3762/bjoc.20.92

• 40 μM solutions of the DCPQs and DPQDs on a Cary 100 Bio spectrophotometer using 1 cm quartz cells. All solvents were HPLC grade (purchased from Fisher) and stored over 4 Å molecular sieves. The absorption intensity at λmax was then plotted against the concentration in all cases to confirm, by

Spin and charge interactions between nanographene host and ferrocene

• Akira Suzuki,
• Yuya Miyake,
• Ryoga Shibata and
• Kazuyuki Takai

Beilstein J. Org. Chem. 2024, 20, 1011–1019, doi:10.3762/bjoc.20.89

• Evolution instruments (Horiba) with an excitation laser operated at 532 nm in the wavenumber range from 1000 to 2000 cm−1. FTIR spectra were obtained using an FT/IR-6600 (JASCO) in ATR method with a diamond prism. Magnetic susceptibility measurements were carried out by a superconducting quantum

• significant influences by nanographene domains. The Raman spectra for both ACFs and FeCp2–ACFs-150 shown in Figure 4 exhibit two broad peaks near 1350 and 1600 cm−1. The peak around 1600 cm−1 corresponds to the Raman-allowed E2g mode (G-band) in graphene. The D-band peak around 1350 cm−1 is forbidden in ideal

• graphene crystals but becomes Raman-active by an electron-scattering process due to impurities and edges in crystallites [29]. The G and D-bands were fitted with two Lorentzian curves, as shown in Figure 4. Although characteristic peaks of FeCp2 molecules around 1100 cm−1 are not obtained in the spectrum

Synthesis and properties of 6-alkynyl-5-aryluracils

• Ruben Manuel Figueira de Abreu,
• Till Brockmann,
• Alexander Villinger,
• Peter Ehlers and
• Peter Langer

Beilstein J. Org. Chem. 2024, 20, 898–911, doi:10.3762/bjoc.20.80

• appears to have the opposite effect, as 5m demonstrates. Although it was expected that this would result in a higher absorption intensity, a drastic reduction in the intensity was observed. The extinction coefficient of 5m (8766 M−1 cm−1) was rather low compared to 5d. Furthermore, the substitution of a π

Synthesis of new representatives of A₃B-type carboranylporphyrins based on meso-tetra(pentafluorophenyl)porphyrin transformations

• Victoria M. Alpatova,
• Evgeny G. Rys,
• Elena G. Kononova and
• Valentina A. Ol'shevskaya

Beilstein J. Org. Chem. 2024, 20, 767–776, doi:10.3762/bjoc.20.70

• spectra of porphyrins 2 and 3 exhibit the absorption band at 3321 cm−1 corresponded to NН stretching vibrations. Bands at 2127 cm−1 confirmed the presence of the N3 group in porphyrins 2 and 7. The IR spectra of porphyrins 5–7, 11, 12, 14, 18–20, 23, 24, and 26 exhibit absorption bands at 2605–2609 cm−1

• assigned to the BH-stretching vibration in neutral closo-carborane polyhedra and the bands at 3061–3069 cm−1 related to carborane CH groups. All prepared porphyrins 2, 3, 5–7, 11, 12, 14, 18–20, 23, 24, and 26 had the characteristic bands at ν = 1466–1499 cm−1 assigned to C–F stretching vibrations. Bands

• in the 1797–1641 cm−1 range in porphyrins 11, 12, and 14 correspond to the displacement of the C=O group. In the 1H NMR spectra eight β-protons of the porphyrin macrocycle for all compounds 2, 3, 5–7, 11, 12, 14, 18–20, 23, 24, and 26 were found between δ = 8.94–9.39 ppm and broadened singlets of the