| Literature DB >> 26734093 |
Anna Wrona-Piotrowicz1, Janusz Zakrzewski1, Anna Gajda2, Tadeusz Gajda2, Anna Makal3, Arnaud Brosseau4, Rémi Métivier4.
Abstract
Friedel-Crafts-type reaction of pyrene with diethyl 1-(isothiocyanato)alkylphosphonates promoted by trifluoromethanosulfonic acid afforded diethyl 1-(pyrene-1-carbothioamido)alkylphosphonates in 83-94% yield. These compounds were transformed, in 87-94% yield, into the corresponding diethyl 1-(pyrene-1-carboxamido)alkylphosphonates by treatment with Oxone(®). 1-(Pyrene-1-carboxamido)methylphosphonic acid was obtained in a 87% yield by treating the corresponding diethyl phosphonate with Me3Si-Br in methanol. All of the synthesized amidophosphonates were emissive in solution and in the solid state. The presence of a phosphonato group brought about an approximately two-fold increase in solution fluorescence quantum yield in comparison with that of a model N-alkyl pyrene-1-carboxamide. This effect was tentatively explained by stiffening of the amidophosphonate lateral chain which was caused by the interaction (intramolecular hydrogen bond) of phosphonate and amide groups. The synthesized phosphonic acid was soluble in a biological aqueous buffer (PBS, 0.01 M, pH 7.35) and was strongly emissive under these conditions (λem = 383, 400 nm, τ = 18.7 ns, ΦF > 0.98). Solid-state emission of diethyl 1-(pyrene-1-carboxamido)methylphosphonate (λmax = 485 nm; ΦF = 0.25) was assigned to π-π aggregates, the presence of which was revealed by single-crystal X-ray diffraction analysis.Entities:
Keywords: X-ray structure; amide; fluorescence; isothiocyanate; phosphonate; pyrene; thioamide
Year: 2015 PMID: 26734093 PMCID: PMC4685883 DOI: 10.3762/bjoc.11.266
Source DB: PubMed Journal: Beilstein J Org Chem ISSN: 1860-5397 Impact factor: 2.883
Scheme 1Synthesis of diethyl 1-(pyrene-1-carbothioamido)alkylphosphonates 2a–d, diethyl 1-(pyrene-1-carboxamido)alkylphosphonates 3a–d and (pyrene-1-carboxamido)methylphosphonic acid (4).
Figure 1Structure of amide 5.
Steady-state absorption and emission data for 3a–d, 4, 5 in CHCl3 solutions (c = 10−6 M).
| Compound | Absorption λmax/nm (εmax/M−1 cm−1) | Emissionb λmax/nm | ΦF |
| 331 (27450), 345 (50910), 380 (960) | 385, 405 | 0.68 | |
| 332 (38710), 345 (52480), 379 (4000) | 385, 404 | 0.66 | |
| 331 (37850), 345 (51610), 379 (2750) | 385, 404 | 0.63 | |
| 331 (37220), 345 (51400), 379 (4200) | 387, 406 | 0.68 | |
| 327 (36350), 341 (50410), 376 (5100) | 383, 400 | >0.98 | |
| 316 (16990), 329 (37400), 345 (52360), 377 (2030) | 385, 403 | 0.34 | |
a10–6 M solution in 0.01 M PBS (pH 7.35). bλexcit = 360 nm.
Figure 2Normalized electronic absorption (a) and emission (b) spectra of 3a in various solvents.
Figure 3Fluorescence decay curves for 3a and 5 in chloroform and for 4 in 0.01 M PBS (pH 7.35). λexcit = 360 nm; λem = 385, 390 and 383 nm, respectively.
Fluorescence lifetimes and decay rate constants for 3a and 5 in CHCl3 and for 4 in 0.01 M PBS (pH 7.35).
| Compound | τ (ns); contribution | ||
| 10.6 (1.00) | 6.4 | 3.0 | |
| 18.7 (1.00) | 5.2 | 0.1 | |
| 12.3 (1.00) | 2.8 | 5.4 | |
akr = ΦF /τ; bknr = (1−ΦF )/τ.
Figure 4Intramolecular hydrogen bond in 3a–d.
Figure 5Normalized electronic absorption (violet) and emission (pink) spectrum of 3a in CHCl3 (c = 10−6 M) and its solid-state emission spectrum (yellow). λexcit = 360 nm.
Figure 6Molecular structure of 3a (ORTEP representation). Displacement ellipsoids were drawn at a 50% probability level. Hydrogen atom labels are analogous to those of bonded non-H atoms and were omitted for clarity, apart from the H1 atom which was involved in intermolecular hydrogen bond formation.
Selected geometrical parameters for 3a.
| Bond lengths | Å |
| P1–O2 | 1.5761(11) |
| P1–O3 | 1.4751(10) |
| P1–O4 | 1.5694(11) |
| P1–C18 | 1.8000(14) |
| C1–C17 | 1.5053(18) |
| O1–C17 | 1.2315(16) |
| N1–C18 | 1.4500(17) |
| N1–C17 | 1.3463(17) |
| Torsion angles | ° |
| C12–C15–C16–C5 | −179.43(12) |
| C12–C15–C16–C9 | −0.42(19) |
| C2–C1–C17–O1 | −123.81(15) |
| C2–C1–C17–N1 | 58.89(17) |
| C17–N1–C18–P1 | 102.39(13) |
Selected hydrogen bonds in the crystal structure of 3a.
| D | H | A | D–H [Å] | D–H [Å] | D–H [Å] | D–H … A [ ° ] | Symmetry operation for A atom |
| N1 | H1 | O3 | 0.871(14) | 1.941(14) | 2.7991(15) | 168.0(16) | 1−x, −y, 1−z |
| C20 | H20C | O1 | 0.981 | 2.683 | 3.369(2) | 127.3 | 1−x, −½+y, ½−z |
| C21 | H21A | O1 | 0.990 | 2.6145 | 3.585(2) | 166.6 | 1−x, −½+y, ½−z |
| C22 | H22C | O3 | 0.980 | 2.708 | 3.664(2) | 165.2 | 1−x, ½+y, ½−z |
Figure 7(a) Dimers of π-stacked and hydrogen-bonded molecules of 3a represented in single figures; (b) network of weak C–H…O and C–H…π interactions stabilizing H-bonded dimer strings and (c) crystal packing along the crystallographic b direction. Ellipsoids are drawn at 50% probability level for all non-C and non-H atoms. The remaining atoms are represented as wires in grey or green in order to differentiate between adjacent π…π interacting chains of H-bonded atoms. The shortest intermolecular contacts are represented in cyan.