fs–ps Exciton dynamics in a stretched tetraphenylsquaraine polymer

2019 ◽  
Vol 21 (28) ◽  
pp. 15346-15355 ◽  
Author(s):  
Maximilian H. Schreck ◽  
Lena Breitschwerdt ◽  
Henning Marciniak ◽  
Marco Holzapfel ◽  
David Schmidt ◽  
...  

A squaraine polymer shows surprisingly fast light induced energy transfer between two different structural sections on the ps/fs time scale.

1998 ◽  
Vol 76-77 ◽  
pp. 467-469 ◽  
Author(s):  
K.V. Bautin ◽  
S.V. Kudyakov ◽  
I.N. Ogorodnikov ◽  
A.V. Kruzhalov ◽  
V.Yu. Yakovlev

1998 ◽  
Vol 23 (1) ◽  
pp. 107-111
Author(s):  
M. Godlewski ◽  
P.O. Holz ◽  
J.P. Bergman ◽  
B. Monemar ◽  
K. Reginski ◽  
...  

1998 ◽  
Vol 102 (23) ◽  
pp. 4392-4398 ◽  
Author(s):  
Jakub Pšenčík ◽  
Tomáš Polívka ◽  
Petr Němec ◽  
Juraj Dian ◽  
Jakub Kudrna ◽  
...  

2010 ◽  
Vol 14 (01) ◽  
pp. 55-63 ◽  
Author(s):  
Pierre D. Harvey ◽  
Christine Stern ◽  
Claude P. Gros ◽  
Roger Guilard

Recent discoveries from our research groups on the photophysics of a few cofacial bisporphyrin dyads for through space singlet and triplet energy transfers raised several important investigations about the mechanism of energy transfers and energy migration in light-harvesting devices, notably LH II, in the heavily investigated purple photosynthetic bacteria. The key feature is that for face-to-face and slipped dyads with controlled structure using rigid spacers or spacers with limited flexibilities, our fastest rates for singlet energy transfer are in the 10 × 109 s -1 (i.e. 100 ps time scale) for donor-acceptor distances of ~3.5–3.6 Å. The time scale for energy transfers between different bacteriochlorophylls, notably B800*→B850, is in the ps despite the long Mg ⋯ Mg separation (~18 Å). This short rate drastically contrasts with the well-accepted Förster theory. This review focuses on the photophysical processes and dynamics in LH II and compares these parameters with our investigated model dyads build upon octa-etio-porphyrin chromophores and rigid and semi-rigid spacers. The recently discovered role of the rhodopin glucoside (carotenoid) will be analyzed as possible relay for energy transfers, including the possibility of uphill processes at room temperature. In this context the concept of energy migration may be complemented by parallel relays and uphill processes. It is also becoming more obvious that the irreversible electron transfer at the reaction center (electron transfer from the special pair to the phaeophytin) renders the rates for energy transfer and migration faster precluding all possibility of back transfers.


2018 ◽  
Vol 20 (34) ◽  
pp. 22331-22341 ◽  
Author(s):  
Sandra Doria ◽  
Andrea Lapini ◽  
Mariangela Di Donato ◽  
Roberto Righini ◽  
Nicolò Azzaroli ◽  
...  

We aim to get insight the aggregation effect on the exciton behavior in phthalocyanine systems with coherent spectroscopy.


2013 ◽  
Vol 17 (01n02) ◽  
pp. 44-55 ◽  
Author(s):  
Hai-Jun Xu ◽  
Bin Du ◽  
Claude P. Gros ◽  
Philippe Richard ◽  
Jean-Michel Barbe ◽  
...  

Four dyad systems composed of a central truxene and either one or three β-substituted zinc(II) porphyrins (ZnP: TruZnP (7) and TruTriZnP (9)) or free-bases (H2P: TruP (6) and TruTriP (8)) have been prepared. The presence of β-methyl groups minimizes π-conjugation through the quasi right angle made by the porphyrin and the truxene planes, and renders these dyads relatively rigid. The position of the absorption and emission 0–0 peaks confirms the role of the truxene and porphyrin as the energy donor and acceptor, respectively. Selective excitation of the truxene results in an efficient singlet energy transfer (S1 ET) from the truxene to the porphyrin unit. The rates for S1 ET (k ET ) are extracted from the change in the fluorescence lifetime of truxene in the presence and absence of the acceptor, and are temperature independent, (TruP (6), TruTriP (8), TruZnP (7) and TruTriZnP (9) are 5.0, 1.4, 1.0 and 1.4 at 298 K and 5.9, 1.3, 2.6, and 0.86 (ns)-1 at 77 K, respectively), consistent with their relative rigidity. These k ET 's are similar to other related but more flexible systems reported by one of us (Inorg. Chem.2011, 50, 11493–11505). The k ET 's time scale was assumed, based on modeling, to be related with hindered rotations about the truxene-porphyrin C–C bonds due to steric hexyl–hexyl interactions. This work confirms this earlier conclusion was correct.


2011 ◽  
Vol 41 (2) ◽  
pp. 378-395 ◽  
Author(s):  
Maxim Nikurashin ◽  
Sonya Legg

Abstract Fine- and micro-structure observations indicate that turbulent mixing is enhanced within O(1) km above rough topography. Enhanced mixing is associated with internal wave breaking and, in many regions of the ocean, has been linked to the breaking and dissipation of internal tides. The generation and dissipation of internal tides are explored in this study using a high-resolution two-dimensional nonhydrostatic numerical model, which explicitly resolves the instabilities leading to wave breaking, configured in an idealized domain with a realistic multiscale topography and flow characteristics. The control simulation, chosen to represent the Brazil Basin region, produces a vertical profile of energy dissipation and temporal characteristics of finescale motions that are consistent with observations. Results suggest that a significant fraction of mixing in the bottom O(1) km of the ocean is sustained by the transfer of energy from the large-scale internal tides to smaller-scale internal waves by nonlinear wave–wave interactions. The time scale of the energy transfer to the smaller scales is estimated to be on the order of a few days. A suite of sensitivity experiments is carried out to examine the dependence of the energy transfer time scale and energy dissipation on topographic roughness, tidal amplitude, and Coriolis frequency parameters. Implications for tidal mixing parameterizations are discussed.


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