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Updated: Aug 21, 2026

Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization
Published on: August 6, 2018
Site-Specific and Mode-Specific Photodissociation of OH bonds in a Pentapeptide by Laser-Driven Tunneling through a
Kendrew Au1, Isaac Ofori2, Chin Lee1
1Gas Phase Chemical Physics, Combustion Research Facility, Sandia National Laboratories, Livermore, California94550, United States.
Abstract:
The prospect of using lasers to selectively break chemical bonds in molecules is often thwarted by the intrinsic anharmonic mixing of the vibrational levels that lead to dissociation with a dense manifold of other vibrational states that do not. Using an ultraviolet-infrared (UV-IR) double resonance excitation scheme, we demonstrate both site- and mode-selective photodissociation of the O-H bond in either of the two tyrosine chromophores (Tyr, Y) in a cryogenically cooled, gas phase protonated pentapeptide ion [YGGYL+H]+ with 231 vibrational modes. The two tyrosine's have unique UV absorptions with electronic origins separated from one another by 324 cm-1, enabling site-specific electronic excitation of the 1ππ* state of the Y1 or Y4 chromophore. Isotopic substitution of 18OH on one of the two tyrosine's phenol moiety (forming Y(18O)GGYL or YGGY(18O)L) produces a shift in the infrared absorption frequency of the OH stretch fundamental of -11 cm-1. Since the OH stretch fundamental shifts by -72 cm-1 in the 1ππ* state relative to the ground state, UV-IR spectra as a function of IR-UV time delay map out the excited state IR spectra and provides a means for promoting either OH group to OH(v = 1) in their 1ππ* excited state. Using UV-IR excitation at short IR-UV delay times, we observe site-selective and mode-selective loss of the OH hydrogen atom, which is efficiently lost only when both UV and IR excitation are on the same Tyr chromophore, with a mode-selectivity of greater than 100:1. No other combination of UV and IR excitation produces any measurable H atom loss. Since the OH stretch coordinate is the reaction coordinate for H atom loss, we identify tunneling underneath the 1ππ*/1πσOH* conical intersection (CI) as responsible for the mode-selectivity of the photofragmentation, and argue that tunneling through the CI following OH(v = 1) excitation is fast enough that it competes favorably over vibrational energy scrambling, making it possible to selectively fragment either OH bond in this large molecule with high fidelity.
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