Ultrafast dissociation of ammonia: Auger Doppler effect and redistribution of the internal energy




Travnikova Oksana, Kukk Edwin, Hosseini Farzad, Granroth Sari, Itälä Eero, Marchenko Tatiana, Guillemin Renaud, Ismail Iyas, Moussaoui Roba, Journel Loïc, Bozek John, Püttner Ralph, Krasnov Pavel, Kimberg Victor, Gel'mukhanov Faris, Piancastelli Maria Novella, Simon Marc

PublisherRoyal Society of Chemistry

2022

Physical Chemistry Chemical Physics

PHYSICAL CHEMISTRY CHEMICAL PHYSICS

PHYS CHEM CHEM PHYS

24

10

5842

5854

13

1463-9076

1463-9084

DOIhttps://doi.org/10.1039/d1cp05499f

https://pubs.rsc.org/en/content/articlelanding/2022/cp/d1cp05499f

https://hal.sorbonne-universite.fr/hal-03598117/file/NH3_Doppler_PCCP_resubmission%20copy.pdf



We study vibrationally-resolved resonant Auger (RAS) spectra of ammonia recorded in coincidence with the NH2+ fragment, which is produced in the course of dissociation either in the core-excited 1s(-1)4a1(1) intermediate state or the first spectator 3a(-2)4a1(1) final state. Correlation of the NH2+ ion flight times with electron kinetic energies allows directly observing the Auger-Doppler dispersion for each vibrational state of the fragment. The median distribution of the kinetic energy release E-KER, derived from the coincidence data, shows three distinct branches as a function of Auger electron kinetic energy E-e: E-e + 1.75E(KER) = const for the molecular band; E-KER = const for the fragment band; and E-e + E-KER = const for the region preceding the fragment band. The deviation of the molecular band dispersion from E-e + E-KER = const is attributed to the redistribution of the available energy to the dissociation energy and excitation of the internal degrees of freedom in the molecular fragment. We found that for each vibrational line the dispersive behavior of E(KER)vs. E-e is very sensitive to the instrumental uncertainty in the determination of E-KER causing the competition between the Raman (E-KER + E-e = const) and Auger (E-e = const) dispersions: increase in the broadening of the finite kinetic energy release resolution leads to a change of the dispersion from the Raman to the Auger one.



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