Open Access Article
Giacomo Salvadori
a,
Piermarco Saraceno
b,
Alisia Santomierib,
Chris John
b and
Laura Pedraza-González
*b
aInstitute for Computational Biomedicine (INM-9), Forschungszentrum Jülich, 52428 Jülich, Germany
bDipartimento di Chimica e Chimica Industriale, Università di Pisa, Via G. Moruzzi 13, 56124 Pisa, Italy. E-mail: laura.pedraza@unipi.it
First published on 25th February 2026
Correction for “Structural and spectroscopic basis of excitation energy transfer in microbial rhodopsins binding xanthophylls” by Giacomo Salvadori et al., Chem. Sci., 2025, 16, 18423–18437, https://doi.org/10.1039/D5SC04961J.
The corrected absorption and CD spectra, previously reported in Fig. 5 in the main text, are shown in the updated Fig. 5 herein.
The revised absorption spectra display modest but systematic differences relative to those originally published. In the Kin4B8-lutein complex, the relative intensity of the two carotenoid absorption peaks in the 450–500 nm region is altered: whereas the original spectra displayed peaks of comparable height, the corrected spectra exhibit a slightly enhanced intensity for the longer-wavelength peak. In addition, the carotenoid absorption maxima are blue-shifted by approximately 5 nm. A similar trend is observed for the Kin4B8-zeaxanthin complex, where the narrower peaks lead to slightly more pronounced differences. Despite these changes, the overall agreement between simulated and experimental absorption spectra remains good, and all conclusions regarding the reliability of our exciton model are preserved.
The CD spectra are affected in an analogous manner. For Kin4B8-lutein, the carotenoid CD features exhibit a 4–5 nm blue-shift, and the central positive lutein band near 480 nm becomes slightly more intense. The negative CD band at ∼525 nm becomes marginally deeper; however, its characteristic blue-shift relative to the rPSB absorption maximum, one of the key spectroscopic signatures of the Kin4B8-xanthophyll complexes, remains essentially unchanged. For Kin4B8-zeaxanthin, the corrections are even less pronounced, and the blue-shift slightly improves the peak positions.
Importantly, correcting the spectral density has a negligible impact on the computed EET times (τEET) and efficiencies (θEET). For Kin4B8-ZEA, the updated values are τEET = 60.1 ± 1.6 and θEET = 70.1 ± 0.5% (previously 59.1 ± 1.7 and 70.5 ± 0.6%, respectively). For Kin4B8-LUT, the revised values are τEET = 60.7 ± 3.5 and θEET = 70.4 ± 1.2% (previously 60.3 ± 3.5 and 70.5 ± 1.2%, respectively). The updated data are reported in Table S5 in the SI.
Overall, although the corrected spectral densities lead to minor quantitative changes in the simulated optical spectra, all qualitative trends and mechanistic conclusions reported in the original publication remain valid. In particular, the excitonic model continues to reproduce the key experimental observables, including the characteristic shift between the rPSB absorption maximum and the negative CD band, as well as the high EET efficiencies observed for both lutein and zeaxanthin.
In addition, in the original versions of Fig. S6b, S7b, S8b, and S9b, a factor of 2 was inadvertently omitted in the excitonic contribution to the CD spectra due to a plotting error. This issue affected only the graphical representation of the data; the underlying calculations were performed correctly. This can be verified by reconstructing the total CD spectrum as the sum of the individual chromophore contributions and the excitonic contribution, which reproduces the reported total spectrum.
The affected figures in the SI have been updated accordingly (Fig. S3 and S6–S10).
The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
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