Identifiability limits and deep-learning-assisted reconstruction of rotational density matrices for symmetric-top molecules

B Bowen Dong M Ming Zhang Y Yicheng Zhuang (Department of Physics, Harvard University) S Shutao Zhang D Dongyu Liu M Mohan Xu (State Key Laboratory for Mesoscopic Physics and Collaborative Innovation Center of Quantum Matter, School of Physics, Peking University 2 , Beijing 100871,) S Sizhe Li (Department of Materials Science) A Anatoly A. Ischenko (Lomonosov Institute of Fine Chemical Technologies, RTU-MIREA – Russian Technological University 9 , Vernadskii Avenue 86, 119571 Moscow,) H Haitan Xu (School of Materials Science and Intelligent Engineering, Nanjing University 10 , Suzhou 215163,) R R. J. Dwayne Miller (Departments of Chemistry and Physics, University of Toronto, 80 St. George Street, Toronto, ON M5S3H6, Canada) Z Zheng Li

Abstract

Recovering the rotational density matrix of a molecular ensemble from time-resolved angular distributions is central to understanding ultrafast rotational dynamics, yet the inverse problem is severely underdetermined. We analyze the forward operator that maps the density matrix of laser-aligned symmetric-top molecules to the angular distribution retrieved in pump–probe experiments and demonstrate through singular value decomposition that 74%–88% of the real density matrix unknowns lie in the null space for maximum angular momentum quantum numbers Jmax = 2–5. This rank deficiency is intrinsic to the measurement geometry and imposes a linear lower bound on reconstruction error: the minimum-norm least-squares (pseudoinverse) solution sets all null-space components to zero, establishing the best achievable error for any linear, unbiased estimator. Nonlinear constraints—positive semidefiniteness, trace conservation, and block symmetries—partially recover null-space information, but the residual error grows with Jmax, reaching 15%–44% for Jmax = 5. We present a two-stage pipeline in which a convolutional neural network trained on simulated data provides a warm start for the fast iterative shrinkage-thresholding algorithm. For both CF3I and CH3Cl across Jmax = 2–6, this approach reduces the Frobenius reconstruction error by 80%–99% relative to optimization from thermal equilibrium, maintaining stable errors of 0.5%–1.1% as Jmax increases. The pipeline is robust to data noise down to a 20 dB signal-to-noise ratio and operates ten times faster than the baseline and outperforms the maximum-entropy approach by a factor of 15–39×. The classical iterative quantum tomography algorithm becomes numerically unstable for Jmax ≥ 4, whereas the proposed method converges reliably at all tested truncation levels.

Article Details

Volume / Issue Vol. 165, Issue 3
Published July 21, 2026
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 (11)

B

Bowen Dong

M

Ming Zhang

Y

Yicheng Zhuang

Department of Physics, Harvard University

S

Shutao Zhang

D

Dongyu Liu

M

Mohan Xu

State Key Laboratory for Mesoscopic Physics and Collaborative Innovation Center of Quantum Matter, School of Physics, Peking University 2 , Beijing 100871,

S

Sizhe Li

Department of Materials Science

A

Anatoly A. Ischenko

Lomonosov Institute of Fine Chemical Technologies, RTU-MIREA – Russian Technological University 9 , Vernadskii Avenue 86, 119571 Moscow,

H

Haitan Xu

School of Materials Science and Intelligent Engineering, Nanjing University 10 , Suzhou 215163,

R

R. J. Dwayne Miller

Departments of Chemistry and Physics, University of Toronto, 80 St. George Street, Toronto, ON M5S3H6, Canada

Z

Zheng Li