Two-dimensional electronic spectroscopy (2DES) is an ultrafast laser spectroscopy technique that allows the study of ultrafast phenomena inside systems in condensed phase. The term electronic refers to the fact that the optical frequencies in the visible spectral range are used to excite electronic energy states of the system; however, such a technique is also used in the IR optical range (excitation of vibrational states) and in this case the method is called two-dimensional infrared spectroscopy (2DIR). It is also possible to combine multiple frequency ranges to study phenomena involving different energy scales. For example, by combining infrared (IR) frequency, which probe electronic excitations and THz (far-IR), which probe the vibrational excitations of solids, it is possible to study the interaction between electrons and vibrational excitations. This technique, typically, records the signal which is emitted from a system after an interaction with a sequence of 3 laser pulses. Such pulses usually have a time duration of few hundred femtosecond (10−15 s) and this high time resolution allows capturing of dynamics inside the system that evolves with the same time scale. The main result of this technique is a two-dimensional absorption spectrum that shows the correlation between excitation and detection frequencies. The first 2DES spectra were recorded in 1998. 2DES has been combined with photoelectrochemical recordings (PEC2DES) to study charge separation in the photosynthetic complex photosystem I, which is the physiological output signal in contrast to fluorescence. This method provides experimental access to the action spectra of the complexes.
Basic concepts about 2DES
Pulse sequence The pulse sequence in this experiment is the same as 2DIR in which the delay between the first and second pulse is called the coherence time and is usually labeled as t 1 {\displaystyle t_{1}} . The delay between the second and the third pulse is called the population time and it is labeled as t 2 {\displaystyle t_{2}} . The time after the third pulse corresponds to the detection time t 3 {\displaystyle t_{3}} which is usually Fourier transformed by a spectrometer. The interaction with the pulses creates a third-order nonlinear response function S ( t 1 , t 2 , t 3 ) {\displaystyle S(t_{1},t_{2},t_{3})} of the system from which it is possible to extract two-dimensional spectra as a function of excitation and detection frequencies. Although third-order two-dimensional spectroscopy is historically first and most popular, high-order two-dimensional spectroscopy approaches have also been developed.
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