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Quantum state mixing in photobiology: New insight from ultrafast terahertz Stark spectroscopy

Quantum state mixing in photobiology – new insight from ultrafast terahertz Stark spectroscopy
(a) Molecular structure of the protonated retinal Schiff base in bacteriorhodopsin (black molecular structure) and its binding pocket in the protein, consisting of amino acids and an embedded water molecule. The blue arrow indicates the electric dipole moment of retinal. (b) Molecular structure of the trans and 13-cis isomers of the protonated retinal Schiff base and schematic of the electronic potential energy surfaces of the ground state S0 and the excited states S1 and S2 along the reaction coordinate for isomerization. The mixing of the S1 and S2 states leads to the shallow potential minima in the excited states with a strong impact on the initial photoinduced dynamics. The isomerization reaction occurs upon crossing the conical intersection (CI) of the excited- and ground-state potentials. (c) Schematic of the THz Stark experiment with a strong THz pump pulse and optical probe pulse. The THz field acting on the sample is enhanced with the help of a metallic antenna structure (yellow structure on top of the gray sample layer) and reaches a value of several megavolts/cm. The THz-induced absorption change of the sample is measured with the probe pulse transmitted through the antenna gap. (d) Time-dependent electric field of the THz pulse (1 ps = 10-12 s). Credit: MBI/T. Elsaesser

The membrane protein bacteriorhodopsin is a proton pump, in which proton transport is initiated by the light-induced isomerization of the chromophore retinal. The molecular quantum states involved in this ultrafast reaction have now been characterized by measuring their electric dipole moment.

The novel method of terahertz Stark spectroscopy reveals a mixing of electronically excited states with a direct impact on pathway and dynamics of the photoreaction.

The protonated retinal Schiff base, the chromophore of bacteriorhodopsin, undergoes an ultrafast change of its molecular structure upon absorption of light. Photoexcitation promotes the chromophore to a particular range of its excited-state potential energy surface, from which the excited molecule evolves along a reaction coordinate to the intersection point of the excited and ground-state potential surfaces. After this early propagation in the excited state, isomerization occurs upon passing this crossing point within some 500 fs=5×10-13 s after excitation.

So far, the character of the excited-state potential governing reaction dynamics has remained controversial. Theoretical models have invoked either the first excited state S1 only or a mixed quantum state with a contribution from the second excited state S2.

This issue calls for new experimental insight into the excited-state character. A promising quantity to probe is the of retinal, which is markedly different in the ground state S0 and the first and second excited states S1 and S2. Thus, a measurement of dipole change upon photoexcitation should allow for clarifying the character of the excited state relevant for the early dynamics of bacteriorhodopsin.

Quantum state mixing in photobiology – new insight from ultrafast terahertz Stark spectroscopy
(a) Schematic of the THz Stark effect. The local THz field Eloc in the sample induces an energy shift of the electronic ground state S0 and the excited state Sex. As a result, the frequency of the optical transition from S0 to Sex (vertical arrows) is changed. Sign and amount of the frequency shift depend on the projection of the molecular dipole moments µ0 and µex in the S0 and Sex states on the direction of Eloc. The frequency shift is proportional to the product of the projected dipole difference Δµ=µex0 and the local field Eloc. For the sample with retinal dipoles randomly oriented in space, the experiment averages over all dipole directions, resulting in a THz-induced broadening of the absorption spectrum. (b) Absorption change (symbols) induced at the maximum of the THz electric field (time t=0) as a function of optical frequency, and absorption spectrum A0 in absence of the THz pulse (blue line). The THz pulse induces a transient spectral broadening with an absorption decrease in the center of A0 and an absorption increase in its wings. The black solid line originates from a numerical analysis of the data, giving a spectral broadening by ±12 THz and a dipole change Δµ=5 Debye between S0 and Sex. Credit: MBI/T. Elsaesser

Applying the novel method of terahertz (THz) Stark spectroscopy, researchers from the Max-Born-Institut and Humboldt Universität in Berlin and the Ludwig Maximilians Universität in Munich have now determined the retinal electric dipole changes in bacteriorhodopsin (1 THz = 1012 Hz = 1012 oscillations per second).

As they report in the Proceedings of the National Academy of Sciences, photoexcitation results in a moderate change of the retinal dipole by some 5 Debye (1.67×10-29 CoulombMeter), much smaller than predicted for a neat S1 character of the excited state.

In contrast, their data and theoretical analysis show that admixture of the S2 state and temporal averaging over the first 120 fs of the ultrafast excited state dynamics account for the measured dipole change. Such results support a picture of pronounced quantum state mixing in the early electronic and nuclear dynamics of bacteriorhodopsin.

THz Stark spectroscopy employs a pump-probe approach, in which a THz pump pulse of a 1-ps duration (1 ps = 10-12 s) provides a strong external electric field, which induces a spectral (Stark) shift of the optical transitions from the retinal ground to the excited state.

This shift is proportional to the dipole difference ∆µ between the ground and . The resulting absorption change of the sample is measured by a femtosecond probe pulse, which is short compared to the THz pulse and, thus, probes the momentary impact of the THz field. For a sample with a random spatial orientation of retinal chromophores, one observes a spectral broadening of the electronic absorption band, from which the dipole change ∆µ is derived.

In time, the broadening follows the intensity of the ultrashort THz pulse. On this ultrashort time scale, the protein environment of the chromophore is practically frozen, with a negligible impact of protein dynamics on the experimental observables.

In this way, THz Stark spectroscopy allows for the accurate measurement of dipole moments in molecular systems relevant to chemistry and biology.

More information: Jia Zhang et al, Ultrafast terahertz Stark spectroscopy reveals the excited-state dipole moments of retinal in bacteriorhodopsin, Proceedings of the National Academy of Sciences (2024). DOI: 10.1073/pnas.2319676121

Provided by Max Born Institute for Nonlinear Optics and Short Pulse Spectroscopy (MBI)

Citation: Quantum state mixing in photobiology: New insight from ultrafast terahertz Stark spectroscopy (2024, June 25) retrieved 19 July 2024 from https://phys.org/news/2024-06-quantum-state-photobiology-insight-ultrafast.html
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