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. 2022 Sep 19;61(38):e202205701.
doi: 10.1002/anie.202205701. Epub 2022 Aug 16.

Visible-Light-Responsive Self-Assembled Complexes: Improved Photoswitching Properties by Metal Ion Coordination

Affiliations

Visible-Light-Responsive Self-Assembled Complexes: Improved Photoswitching Properties by Metal Ion Coordination

Ray G DiNardi et al. Angew Chem Int Ed Engl. .

Abstract

A photoswitchable ligand based on azobenzene is self-assembled with palladium(II) ions to form a [Pd2 (E-L)4 ]4+ cage. Irradiation with 470 nm light results in the near-quantitative switching to a monomeric species [Pd(Z-L)2 ]2+ , which can be reversed by irradiation with 405 nm light, or heat. The photoswitching selectivity towards the metastable isomer is significantly improved upon self-assembly, and the thermal half-life is extended from 40 days to 850 days, a promising approach for tuning photoswitching properties.

Keywords: Metal-Template; Molecular Cage; Non-Equilibrium; Photoswitch; Self-Assembly.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Figure 1
Figure 1
Visible‐light responsive photoswitchable ligand 1 and self‐assembled products [Pd2(E1)4]4+ and [Pd(Z1)2]2+.
Figure 2
Figure 2
The UV/Visible absorption (DMSO, 298 K) spectra of photoswitch 1 at PSS generated using LEDs with emission centered at various wavelengths. The spectrum for Z1 was calculated using the 1H and 19F NMR data together with absorption spectra solutions at PSS when irradiated with 405, 470, 530 and 617 nm. See Supporting Information S3 for details.
Figure 3
Figure 3
a) Single crystal X‐ray structures of E1. The N=N bond length is 1.243(2) Å and CAr−N is 1.414(2) Å. The asymmetric unit contains half the molecule and the two phenyl rings are perfectly co‐planar, with C−N=N bond angles of 115.24°, and C(F)−C−N=N torsion angle of 177.6(1)°. The parent ortho‐tetrafluoroazobenzene [31n] is less planar, with C(F)−C−N=N torsion angles of 139.29 and 139.41°. b) Major positional conformer of [Pd2(E1)4]4+ in the single crystal X‐ray structure of [Pd2(E1)4](BF4)4 ⋅ 0.5H2O ⋅ 4CH3CN. The ligands adopt a range of conformations, with one ligand almost planar and others twisted with the two phenyl rings demonstrating no clear conformational preference in the solid state. c) Major positional disorder of [Pd(Z1)2]2+ in the single crystal X‐ray structure of [Pd(Z1)2](BF4)2⋅2 CH3CN⋅0.8 (MePh). For crystallography details, see Supporting Information S11.
Figure 4
Figure 4
A) Partial 1H (DMSO‐d 6, 600 MHz, 298 K) and 19F (DMSO‐d 6, 565 MHz, 298 K) NMR spectra of i) photoswitch E1 ([1]=10 mM, 2 equiv.); ii) the same sample after adding [Pd(CH3CN)4](BF4)2 (5.2 mM, 1 equiv.), iii) the same sample immediately after irradiating with 530 nm light for 15 min, and iv) the same sample after heating in the dark for 16 h at 90 °C and equilibrating at room temperature for 30 min. B) Zoom scans of select high resolution ESI‐MS peaks for a sample of i) [Pd2(E1)4](BF4)4 ([1]=16 mM), corresponding to [Pd2(1)4]4+, and ii) the same sample after irradiating with 530 nm light for 20 min, corresponding to [Pd(1)2]2+. See Supporting Information S6 for more details.
Figure 5
Figure 5
Partial 1H NMR (DMSO‐d 6, 600 MHz, 298 K) spectra of i) A 1 : 1 mixture of E1 and Z1 generated using 470 nm light ([1]=1.6 mM, 2 equiv.), ii) the same sample 2 hours after adding [Pd(CH3CN)4](BF4)2 (0.82 mM, 1 equiv.), and iii) the same sample after irradiating with 470 nm light for 20 min, see Supporting Information S8 for details. iv) a mixture of [Pd2(E1)4](BF4)4 and [Pd(Z1)2](BF4)2 ([1]=7.1 mM) after irradiating with 405 nm light for 20 min, and v) the sample after irradiating with 530 nm light for 20 min, for more details see Supporting Information S8.
Figure 6
Figure 6
Comparison of thermal isomerization of Z1 ([1]=8.7 mM) and [Pd(Z1)2](BF4)2 ([1]=7.9 mM), using 1H NMR (500 MHz, DMSO‐d 6, 363 K) integrals of photoswitch Z1 (9.14 ppm) and [Pd(Z1)2](BF4)2 (10.07 ppm) normalized to initial integrals. The barrier for the thermal isomerization of Z1 at 363 K was measured at variable temperature (see Supporting Information S3.3 for details). The apparent barrier for the relaxation of [Pd(Z1)2](BF4)2 was determined by monitoring its depletion at 363 K.

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