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2014
DOI: 10.1073/pnas.1410105111
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Extreme cross-peak 2D spectroscopy

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Cited by 4 publications
(3 citation statements)
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“…Two-dimensional electronic spectroscopy (2DES) is [1][2][3][4][5][6][7][8][9][10] steadily becoming a favorable tool to track photoinduced phenomena in complex systems. [1][2][3][4][5][6][7][8][9][10][11] This is due to its enhanced spatial resolution as compared to its one-dimensional pump-probe (1D-PP) counterpart, stemming from the use of an extra laser pulse in the build-up of the third-order nonlinear response signal compared to the latter: a typical experiment is performed by scanning time delays between the first and second laser pulses (t 1 ) for a given time delay between the second and third pulses (t 2 ), which can be considered as the analogue of the waiting time between pump and probe pulses in PP spectroscopy, and between a third pulse and a local oscillator (t 3 ), which heterodynes the field emitted by the sample in response to the perturbation by the three incident pulses. By Fourier transforming the signal along t 1 and t 3 , 2D frequency maps with signals S(Ω 1 ,t 2 ,Ω 3 ) can be obtained at different waiting times t 2 , where all electronic transitions involved in the three field-matter interactions are recorded [12][13][14].…”
Section: Introductionmentioning
confidence: 99%
“…Two-dimensional electronic spectroscopy (2DES) is [1][2][3][4][5][6][7][8][9][10] steadily becoming a favorable tool to track photoinduced phenomena in complex systems. [1][2][3][4][5][6][7][8][9][10][11] This is due to its enhanced spatial resolution as compared to its one-dimensional pump-probe (1D-PP) counterpart, stemming from the use of an extra laser pulse in the build-up of the third-order nonlinear response signal compared to the latter: a typical experiment is performed by scanning time delays between the first and second laser pulses (t 1 ) for a given time delay between the second and third pulses (t 2 ), which can be considered as the analogue of the waiting time between pump and probe pulses in PP spectroscopy, and between a third pulse and a local oscillator (t 3 ), which heterodynes the field emitted by the sample in response to the perturbation by the three incident pulses. By Fourier transforming the signal along t 1 and t 3 , 2D frequency maps with signals S(Ω 1 ,t 2 ,Ω 3 ) can be obtained at different waiting times t 2 , where all electronic transitions involved in the three field-matter interactions are recorded [12][13][14].…”
Section: Introductionmentioning
confidence: 99%
“…Nonlinear optical electronic spectroscopy, through a plethora of diverse experimental variations, provides an ultimate technique to track photoinduced events, 11,12 yet yielding a vast amount of signals hard to interpret and understand. It is here where theoretical chemistry comes at hand, 13 as it allows simulating the spectra and provides a route map to recognize the distinct fingerprints and assign them to specific molecular conformations and electronic excited state transitions.…”
Section: Introductionmentioning
confidence: 99%
“…vibrational or electronic), even if different central pump and probe wavelengths were used [ 91 , 118 ]. This changed with the advent of ‘extreme cross’ peak spectroscopies [ 119 ] such as 2D electronic–vibrational (2DEV) [ 120 ] and 2D vibrational–electronic (2DVE) [ 121 ] spectroscopies. These mixed electronic–vibrational spectroscopies are uniquely placed to investigate how the interplay and coupling between electronic and nuclear degrees of freedom dictates the non-radiative relaxation dynamics of molecules, especially those that involve conical intersections (CIs).…”
Section: Extreme Cross-peak Multidimensional Spectroscopymentioning
confidence: 99%