Potential energy surfaces of bound and metastable electron-attached states of N2O characterized by a joint experimental and theoretical study

M Madhubani Mukherjee (Department of Chemistry, University of Southern California 1 , Los Angeles, California 90089,) C Carson Baker (Department of Chemistry, University of Southern California 1 , Los Angeles, California 90089,) M Miloš Ranković (J. Heyrovský Institute of Physical Chemistry, Czech Academy of Sciences 2 , Dolejškova 3, 18223 Prague 8,) P Pamir Nag (J. Heyrovský Institute of Physical Chemistry, Czech Academy of Sciences 2 , Dolejškova 3, 18223 Prague 8,) J Juraj Fedor (J. Heyrovský Institute of Physical Chemistry, Czech Academy of Sciences 2 , Dolejškova 3, 18223 Prague 8,) A Anna I. Krylov (Department of Chemistry, University of Southern California 1 , Los Angeles, California 90089,)

Abstract

We report a combined experimental and theoretical investigation of electron scattering from nitrous oxide (N2O). Experimental two-dimensional electron energy loss spectra (EELS) provide information about vibrational states of a molecule and about potential energy surfaces of anionic resonances. This study reports the EELS measured at 2.5–2.6 eV incident energy. The calculations using complex-valued extensions of equation-of-motion coupled-cluster theory (based on the non-Hermitian quantum mechanics) facilitate the assignment of all major EELS features. Our simulations identified two broad and partially overlapping resonances—one of π* and another of σ* character—located at ∼2.8 and 2.3 eV vertically at the equilibrium geometry of the neutral. Due to the Renner–Teller effect, the π* resonance splits upon bending. The upper state, 2Π, remains linear. The lower state mixes with the σ* configuration, giving rise to the 2A′ resonance, which becomes strongly stabilized at bent geometries (αNNO = 134°), resulting in very low adiabatic electron attachment energy. The calculations estimate the electron affinity of N2O to be −0.140 eV. The 2A′ state is predissociative, with the barrier for the N–O bond dissociation of 0.183 eV. The measured EELS feature sharp vibrational structures at low energy losses, followed by a linear (in logarithmic scale) tail extending to the maximum energy loss. The simulations attribute the sharp features at the low energy loss to the non-resonant excitations and contributions from the cold 2Π resonance. The tail is attributed to the vibrationally hot 2A′ state, and its slope is determined by the excess energy available in this state.

Article Details

Volume / Issue Vol. 163, Issue 2
Published July 14, 2025
ISSN 0021-9606
Publisher American Institute of Physics

Journal Info

The Journal of Chemical Physics

American Institute of Physics

ISSN: 0021-9606 Physical Sciences

Authors (6)

M

Madhubani Mukherjee

Department of Chemistry, University of Southern California 1 , Los Angeles, California 90089,

C

Carson Baker

Department of Chemistry, University of Southern California 1 , Los Angeles, California 90089,

M

Miloš Ranković

J. Heyrovský Institute of Physical Chemistry, Czech Academy of Sciences 2 , Dolejškova 3, 18223 Prague 8,

P

Pamir Nag

J. Heyrovský Institute of Physical Chemistry, Czech Academy of Sciences 2 , Dolejškova 3, 18223 Prague 8,

J

Juraj Fedor

J. Heyrovský Institute of Physical Chemistry, Czech Academy of Sciences 2 , Dolejškova 3, 18223 Prague 8,

A

Anna I. Krylov

Department of Chemistry, University of Southern California 1 , Los Angeles, California 90089,