We report a large Stokes shift and broad emission band in a Mn-based organic–inorganic hybrid halide, (guanidinium)6Mn3Br12 [GuMBr], consisting of trimeric units of distorted MnBr6 octahedra representing a zero-dimensional compound with a liquid like crystalline lattice. Analysis of the photoluminescence (PL) line width and Raman spectra reveals the effects of electron–phonon coupling, suggestive of the formation of Frenkel-like bound excitons. These bound excitons, regarded as the self-trapped excitons (STEs), account for the large Stokes shift and broad emission band. The excited-state dynamics was studied using femtosecond transient absorption spectroscopy, which confirms the STE emission. Further, this compound is highly emissive with a PL quantum yield of ∼50%. With chloride ion incorporation, we observe enhancement of the emissive properties and attribute it to the effects of intrinsic quantum confinement. Localized electronic states in flat bands lining the gap and their strong coupling with phonons are confirmed with first-principles calculations.

The usefulness of a chirped broadband probe and spectral dispersion to obtain Raman spectra under nonresonant/resonant impulsive excitation is revisited. A general methodology is presented that inherently takes care of phasing the time-domain low-frequency oscillations without probe pulse compression and retrieves the absolute phase of the oscillations. As test beds, neat solvents (CCl4, CHCl3, and CH2Cl2) are used. Observation of periodic intensity modulation along detection wavelengths for particular modes is explained using a simple electric field interaction picture. This method is extended to diatomic molecule (iodine) and polyatomic molecules (Nile blue and methylene blue) to assign vibrational frequencies in ground/excited electronic state that are supported by density functional theory calculations. A comparison between frequency-domain and time-domain counterparts, i.e., stimulated Raman scattering and impulsive stimulated Raman scattering using degenerate pump–probe pairs is presented, and most importantly, it is shown how impulsive stimulated Raman scattering using chirped broadband probe retains unique advantages offered by both.

Elucidating the origin of large Stokes shift (LSS) in certain fluorescent proteins absorbing in blue/blue-green and emitting in red/far-red has been quite illusive. Using a combination of spectroscopic measurements, corroborated by theoretical calculations, the presence of four distinct forms of the chromophore of the red fluorescent protein mKeima is confirmed, two of which are found to be emissive: a feeble bluish-green fluorescence (∼520 nm), which is enhanced appreciably in a low pH or deuterated medium but significantly at cryogenic temperatures, and a strong emission in red (∼615 nm). Using femtosecond transient absorption spectroscopy, the trans-protonated form is found to isomerize within hundreds of femtoseconds to the cis-protonated form, which further yields the cis-deprotonated form within picoseconds followed by structural reorganization of the local environment of the chromophore. Thus, the mechanism of LSS is substantiated to proceed via stepwise excited-state isomerization followed by proton transfer involving three isomers, leaving the fourth one (trans-deprotonated) as a bystander. The exquisite pH sensitivity of the dual emission is further exploited in fluorescence microscopy.

Using „spectrally dispersed’ impulsive stimulated Raman spectroscopy, vibrational spectra arising from motion of nuclear wavepackets in ground and excited electronic states of iodine in carbon tetrachloride are recorded isolating from solvent modes.

We investigate ultrafast dynamics of excited-state proton transfer coupled with cis-trans isomerization in the red fluorescent protein mKeima, elucidating the mechanism of “reverse protonation” and how it is fine-tuned by pH of the local environment.