Probing autoionization decay lifetimes of the 4 <i>d</i> −16 <i>ℓ</i> core-excited states in xenon using attosecond noncollinear four-wave-mixing spectroscopy

N Nicolette G. Puskar (Department of Chemistry, University of California 1 , Berkeley, California 94720,) P Patrick Rupprecht (Department of Chemistry, University of California 1 , Berkeley, California 94720,) J Jan Dvorak Y Yen-Cheng Lin (Department of Chemistry, University of California 1 , Berkeley, California 94720,) A Avery E. Greene (Department of Chemistry, University of California 1 , Berkeley, California 94720,) R Robert R. Lucchese (Chemical Sciences Division, Lawrence Berkeley National Laboratory 2 , Berkeley, California 94720,) C C. William McCurdy (Chemical Sciences Division, Lawrence Berkeley National Laboratory 2 , Berkeley, California 94720,) S Stephen R. Leone (Department of Chemistry, University of California 1 , Berkeley, California 94720,) D Daniel M. Neumark (Department of Chemistry, University of California 1 , Berkeley, California 94720,)

Abstract

The decay of core-excited states is a sensitive probe of autoionization dynamics and correlation effects in many-electron systems, occurring on ultrafast timescales. Xenon, with its dense manifold of autoionizing resonances that can be coupled with near-infrared light, provides a platform to investigate these processes. In this work, the autoionization decay lifetimes of 4d−16ℓ (ℓ = s, p, d, …) core-excited states in xenon atoms are probed with extreme ultraviolet (XUV) attosecond noncollinear four-wave-mixing (FWM) spectroscopy. The 4d{5/2,3/2}−16p XUV-bright states (optically dipole-allowed) exhibit decay lifetimes of ∼6 fs, which is consistent with spectator-type decay. In contrast, the 4d{5/2,3/2}−16s and 4d{5/2,3/2}−16d XUV-dark states (optically dipole forbidden) show longer decay lifetimes of ∼20 fs. Photoionization calculations confirm that all core-hole states with 4d character should decay via spectator channels in ≤6 fs, suggesting that the apparently longer dark-state decay times arise from an alternative mechanism. A few-level simulation of the FWM process shows that the inclusion of a nearby, longer-lived dark state can mimic the experimental FWM signal, suggesting population cycling with a second electronic state with non-4d character. Ab initio calculations support the presence of such multielectron excited states in the 60–70 eV range. These results demonstrate that FWM signals can encode coupled-state dynamics when probing complex systems, highlighting the importance of combining theoretical and experimental approaches to disentangle accurate core-level decay pathways and lifetimes.

Article Details

Volume / Issue Vol. 163, Issue 18
Published November 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 (9)

N

Nicolette G. Puskar

Department of Chemistry, University of California 1 , Berkeley, California 94720,

P

Patrick Rupprecht

Department of Chemistry, University of California 1 , Berkeley, California 94720,

J

Jan Dvorak

Y

Yen-Cheng Lin

Department of Chemistry, University of California 1 , Berkeley, California 94720,

A

Avery E. Greene

Department of Chemistry, University of California 1 , Berkeley, California 94720,

R

Robert R. Lucchese

Chemical Sciences Division, Lawrence Berkeley National Laboratory 2 , Berkeley, California 94720,

C

C. William McCurdy

Chemical Sciences Division, Lawrence Berkeley National Laboratory 2 , Berkeley, California 94720,

S

Stephen R. Leone

Department of Chemistry, University of California 1 , Berkeley, California 94720,

D

Daniel M. Neumark

Department of Chemistry, University of California 1 , Berkeley, California 94720,