REVIEW 4 major objections 4 minor 72 references
This paper claims that a regularized Born series solves coupled-channel quantum scattering in O(N²) operations with guaranteed convergence.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · deepseek-v4-flash
2026-08-03 12:53 UTC pith:YVJBTTKW
load-bearing objection A credible O(N^2) single-column coupled-channel method with genuinely useful closed-channel handling and a convincing He+CO benchmark; the 'guaranteed convergence' label currently outruns the spectral verification in the paper. the 4 major comments →
A quadratic-scaling algorithm with guaranteed convergence for quantum coupled-channel calculations
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The paper's central claim is that the multichannel Lippmann-Schchinger equation for one column of the S-matrix can be solved in O(N²) operations with guaranteed convergence, regardless of interaction strength or anisotropy. The divergence of the naive Born series is traced to the presence of Weinberg eigenvalues with magnitude at least one. The WISE algorithm splits the kernel into a divergent part built from those eigenvectors and a regularized remainder with spectral radius strictly below one, solves the divergent part exactly through a small linear system, and iterates the convergent series for the rest. Closed channels are incorporated through a stable ratio-propagation construction of t
What carries the argument
The load-bearing object is the spectrum of the discretized multichannel Lippmann-Schwinger kernel K = G U_off, and in particular its Weinberg eigenvalues η_k, defined as eigenvalues of that kernel. The WISE decomposition K = K_R + K_D splits off eigenvectors with |η_k| ≥ 1 into a separable divergent operator K_D, leaving a regularized remainder K_R whose spectral radius is less than one. The full solution is then the convergent Born series for K_R plus a finite correction involving the divergent eigenvectors, with coefficients fixed by a small linear system. A stable ratio-propagation method constructs the Green's function without explicit evaluation of exponentially growing closed-channel w
Load-bearing premise
The guarantee stands only if the eigensolver finds every Weinberg eigenvalue with magnitude at least one and the kernel is diagonalizable on that divergent subspace; if an eigenvalue is missed or defective, the regularized kernel may still have spectral radius at least one and the series can diverge, and the numerical agreement additionally assumes the uniform radial grid is fine enough to represent the Green's operator faithfully.
What would settle it
For a system with a closed channel, compute the full spectrum of the regularized kernel K_R after regularization: if any eigenvalue has magnitude at least one, the claimed guaranteed convergence fails. On the numerical side, rerun the CO+N₂ benchmark with a halved radial step, e.g., Δr = 0.05 a₀, and check that the WISE cross-sections move onto the reference coupled-channel curve; if they do not, the discretized kernel, not the regularization, is controlling the error.
If this is right
- State-to-state scattering for molecules prepared in a specific incoming quantum state can be computed in O(N²) time, a quadratic reduction from the O(N³) cost of standard propagation methods.
- Closed channels can be included robustly, so Feshbach resonances and threshold effects are captured rather than lost in open-channel-only approximations.
- Highly anisotropic molecule-molecule systems such as CO+N₂ become feasible for systematic energy-resolved calculations, including the scans needed for atmospheric line-shape modeling.
- The regularization supplies a formal convergence guarantee for the iterative series, removing the need for ad-hoc acceleration schemes in a broad class of coupled-channel problems.
- Weinberg eigenvalue spectra provide a quantitative diagnostic of how strongly perturbative an interaction potential is, which can guide basis-set and method choices.
Where Pith is reading between the lines
- A cheap, auditable robustness check is left implicit: after forming K_R, one could directly verify that its spectral radius is below one by testing K_R v_k ≈ 0 for each removed eigenvector; adding this residual check would turn the guarantee from an assumption into a numerical fact.
- Because the benchmarks show the eigenvalue search dominating total cost, future gains for very large channel counts likely depend on improving the eigensolver step more than on the Born iterations themselves.
- The residual differences visible in the CO+N₂ results could plausibly be removed by adaptive radial grids at no extra asymptotic cost, which the paper notes but does not implement.
- The Weinberg spectrum could be repurposed as a principled channel-selection tool: channels that push eigenvalues outside the unit circle are precisely the ones responsible for strong coupling, so they indicate which closed channels matter most.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces the Weinberg-regularized Iterative Series Expansion (WISE) algorithm for quantum coupled-channel scattering. The method recasts the coupled-channel equations as a multichannel Lippmann-Schwinger equation for a single column of the S-matrix, discretizes the radial coordinate, and solves the resulting linear system by Born iteration. To cure divergence of the Born series, the kernel is decomposed into a divergent part K_D built from Weinberg eigenvalues with |η|≥1 and a regularized part K_R claimed to have spectral radius <1; the divergent part is treated by a small linear system. Closed channels are included through a ratio-propagation construction of the Green's function. The algorithm is validated against standard CC results for He+CO and CO+N2 collisions, and timing benchmarks are reported for channel counts up to 343.
Significance. If the central claims hold, this is a substantial methodological advance: quadratic scaling for a single S-matrix column, explicit inclusion of closed channels, and removal of the Born-series divergence would extend rigorous CC calculations to systems currently considered intractable. The He+CO benchmark is strong and clean: it reproduces independent CC reference results, including Feshbach resonances, without fitted parameters. The CO+N2 application to a molecule-molecule system with strong anisotropy is also a meaningful stress test. The matrix-free implementation and the stable ratio-propagation construction of the Green's function are well-designed engineering. However, the paper's main guarantee is asserted rather than proved, and several numerical details are under-specified; the work is promising but needs revision before the central claims are fully supported.
major comments (4)
- [Spectral Regularization and Guaranteed Convergence, Eq. (16)] The statement after Eq. (16) that ρ(K_R)<1 'by construction' is the load-bearing step for the guaranteed-convergence claim. The construction using right and left eigenvectors of K is valid only if the discretized kernel is diagonalizable on the subspace spanned by all eigenvalues with |η|≥1 and if the Arnoldi/ARPACK run returns every such eigenvalue. For a non-symmetric matrix, a defective Jordan block or a missed eigenvalue leaves ρ(K_R)≥1; then the Born series for u0^(R) and v_k^(R) in Eqs. (17)-(18) need not converge, and Eq. (19) need not represent the solution of Eq. (4). Please provide a theorem with explicit assumptions, or add numerical verification: residuals ||K v_k - η_k v_k|| and ||K† w_k - η_k* w_k||, a completeness check for the selected divergent set, and an estimate of ρ(K_R).
- [Application, Fig. 3(b), and Methods (grid)] The abstract and text describe the CO+N2 results as 'exact quantum results,' but Fig. 3(b) shows visible residual differences between WISE and CC. The Methods state that Δr=0.1 'ensures strict convergence (<1%) of benchmark CC calculations' and then attribute the WISE residuals to the uniform radial discretization. This conflates two sources of error: the trapezoid quadrature in Eq. (10) is not identical to the propagator used in the benchmark, and the same grid step can give different quadrature errors in the two formulations. Please quantify the residuals and report a convergence study in Δr, or an adaptive quadrature, before using the word 'exact'.
- [Methods, Numerical Implementation of the Iterative Algorithm] The fixed-point iteration is stopped when the L2 norm of the update ||u^(n)-u^(n-1)||_2 falls below 0.1. This is an absolute tolerance, not a relative one; for wavefunction components of order unity it is a very loose stopping criterion. Since the paper claims numerically exact agreement with CC, please justify this tolerance or perform a convergence test with ε decreased by factors of 10 and report the effect on the S-matrix elements.
- [Scaling and Summary/Outlook] The quadratic-scaling claim is supported by timing data only up to N=343 and by visual fits in Fig. 4. The total time includes an Arnoldi eigensolver whose iteration count is not bounded as N grows, and the Outlook estimates n_D ∝ N (up to 10^5), in which case a dense solve of the n_D×n_D M-matrix would be O(n_D^3). To support 'quadratic scaling guaranteed,' please give a complexity argument for the eigensolver and regularization steps, or report scaling of each stage with N over a wider range.
minor comments (4)
- [Abstract] The abstract as supplied mentions a 'contour-integral construction' that does not appear anywhere in the body; the convergence guarantee is instead based on spectral regularization. Please reconcile the abstract with the actual method.
- [Summary of the Algorithm] The statement that K_R v_k ≈0 should be an equality if K_D is constructed from the complete divergent eigenspace; the approximate equality signals an unquantified Arnoldi error. Please explain or remove the approximation.
- [Methods, Numerical Implementation] The M-matrix in Eq. (21) is described as sparse, but the implementation uses the dense LAPACK driver ZGESV. Clarify when a sparse solver would be needed and how the sparse structure would be exploited.
- [Methods, ARPACK] Please report ARPACK restart parameters, the number of eigenvalues requested, and residual tolerances so that the calculation is reproducible and the claimed convergence of the divergent subspace can be assessed.
Circularity Check
No significant circularity: the central derivation is benchmarked against independent CC results, and the self-citations are context, not load-bearing premises.
full rationale
The paper's derivation chain is not circular. The WISE algorithm solves the multichannel Lippmann-Schrödinger equation by Born iteration after spectrally removing the Weinberg subspace with |η_k| ≥ 1; the statement that ρ(K_R) < 1 'by construction' is a legitimate definitional construction (the divergent modes are removed), not a fitted parameter renamed as a prediction. The benchmark S-matrix elements and cross-sections are compared with independent standard CC calculations on published ab initio PESs, and no parameter is tuned to force agreement with the target observables. The authors' self-citations (refs. 14, 16, 28, 43, 62, 63) supply potential energy surfaces, line-shape context, and an estimate of conventional CC capabilities; none is invoked as the unverified basis for the convergence guarantee. The main weakness—that the 'guaranteed convergence' claim assumes the Arnoldi iterations find every eigenvalue with |η| ≥ 1 and that K is diagonalizable on that subspace—is an unproven mathematical/computational premise and therefore a correctness risk, not circularity, because the premise is not equivalent to the conclusions it is used to support.
Axiom & Free-Parameter Ledger
free parameters (4)
- Born-series convergence tolerance ε =
0.1
- Radial grid step Δr and grid size =
0.05 a0 / Ng=933 (He+CO); 0.1 a0 / Ng=458 (CO+N2)
- Basis truncation for CO+N2 =
jCO=0-14, jN2=4,6,8
- Arnoldi subspace/restart parameters =
not specified
axioms (6)
- standard math The multichannel LS equation (4) with Green's function (9) is equivalent to the CC equations (3) with the proper boundary conditions.
- domain assumption The non-symmetric kernel K has a complete set of left and right eigenvectors for its divergent subspace.
- ad hoc to paper After removing all eigenvalues with |η|≥1, the regularized kernel K_R has spectral radius <1, and Arnoldi iteration finds every such eigenvalue.
- domain assumption The closed-channel Green's function can be constructed stably from solution ratios via Eqs. (13)-(15).
- domain assumption The ab initio PESs from refs. [71] and [54] are accurate enough for benchmark comparisons.
- domain assumption The rigid-rotor approximation with frozen bond lengths for CO and N2.
read the original abstract
Rigorous quantum dynamics calculations provide essential insights into complex scattering phenomena across atomic and molecular physics, chemical reaction dynamics, and astrochemistry. However, the application of the gold-standard quantum coupled-channel (CC) method has been fundamentally constrained by a steep cubic scaling of computational cost $[{O}(N^3)]$. Here, we develop a general, rigorous, and robust method for solving the time-independent Schr\"odinger equation for a single column of the scattering S-matrix with quadratic scaling $[{O}(N^2)]$ in the number of channels. The Weinberg-regularized Iterative Series Expansion (WISE) algorithm resolves the divergence issues affecting iterative techniques by applying a regularization procedure to the kernel of the multichannel Lippmann-Schwinger integral equation. The method also explicitly incorporates closed-channel effects, including those responsible for multichannel Feshbach resonances. We demonstrate the power of this approach by performing rigorous calculations on He + CO and CO + N$_2$ collisions, achieving exact quantum results with quadratic scaling guaranteed by a contour-integral construction. Our results establish a highly scalable computational paradigm, enabling state-to-state quantum scattering computations for complex molecular systems.
Reference graph
Works this paper leans on
-
[1]
C.Chin,R.Grimm,P.Julienne,E.Tiesinga,Feshbachresonancesinultracoldgases.Rev.Mod. Phys.82, 1225–1286 (2010), doi:10.1103/RevModPhys.82.1225,https://link.aps.org/ doi/10.1103/RevModPhys.82.1225
-
[2]
C.H.Greene,P.Giannakeas,J.Pérez-Ríos,Universalfew-bodyphysicsandclusterformation. Rev. Mod. Phys.89, 035006 (2017), doi:10.1103/RevModPhys.89.035006,https://link. aps.org/doi/10.1103/RevModPhys.89.035006
-
[3]
R.Krems,MoleculesinElectromagneticFields:FromUltracoldPhysicstoControlledChem- istry(Wiley-VCH) (2019)
2019
-
[4]
S. C. Althorpe, D. C. Clary, Quantum Scattering Calculations on Chemical Reactions.Annu. Rev. Phys. Chem.54(1), 493–529 (2003), doi:10.1146/annurev.physchem.54.011002.103750, http://dx.doi.org/10.1146/annurev.physchem.54.011002.103750
arXiv 2003
-
[5]
D. C. Clary, Quantum Dynamics of Chemical Reactions.Science321(5890), 789 (2008), doi:10.1126/science.1157718
-
[6]
R. V. Krems, Cold Controlled Chemistry.Phys. Chem. Chem. Phys.10, 4079–4092 (2008)
2008
-
[7]
Balakrishnan, Perspective: Ultracold molecules and the dawn of cold controlled chemistry
N. Balakrishnan, Perspective: Ultracold molecules and the dawn of cold controlled chemistry. J. Chem. Phys.145(15), 150901 (2016), doi:10.1063/1.4964096
-
[8]
E. Roueff, F. Lique, Molecular Excitation in the Interstellar Medium: Recent Advances in Collisional, Radiative, and Chemical Processes.Chem. Rev.113(12), 8906–8938 (2013), doi:10.1021/cr400145a,http://dx.doi.org/10.1021/cr400145a
-
[9]
E. F. van Dishoeck, E. Herbst, D. A. Neufeld, Interstellar Water Chemistry: From Laboratory to Observations.Chem. Rev.113(12), 9043–9085 (2013), doi:10.1021/cr4003177,https: //doi.org/10.1021/cr4003177
-
[10]
K. Hagino, K. Ogata, A. M. Moro, Coupled-channels calculations for nuclear reac- tions: From exotic nuclei to superheavy elements.Prog. Part. Nucl. Phys.125, 103951 24 (2022), doi:https://doi.org/10.1016/j.ppnp.2022.103951,https://www.sciencedirect. com/science/article/pii/S0146641022000126
arXiv 2022
-
[11]
J.Hartmann,C.Boulet,D.Robert,CollisionalEffectsonMolecularSpectra(Elsevier)(2008), doi:10.1016/b978-0-444-52017-3.x0001-5
-
[12]
J.-M. Hartmann,et al., Recent advances in collisional effects on spectra of molecular gases and their practical consequences.J. Quant. Spectrosc. Radiat. Transf.213, 178 – 227 (2018), doi:https://doi.org/10.1016/j.jqsrt.2018.03.016
-
[13]
P. J. Rayer,Pressure Broadening of Spectral Lines: The Theory of Line Shape in Atmospheric Physics(Cambridge University Press) (2020)
2020
-
[14]
H.Jóźwiak,F.Thibault,H.Cybulski,P.Wcisło,AbinitioinvestigationoftheCO–N 2 quantum scattering: The collisional perturbation of the pure rotational R(0) line in CO.J. Chem. Phys. 154(5) (2021), doi:10.1063/5.0040438,http://dx.doi.org/10.1063/5.0040438
-
[15]
A. Olejnik,et al., Ab initio quantum scattering calculations and a new potential energy sur- face for the HCl(𝑋1Σ+)-O2(𝑋 3Σ− 𝑔) system: Collision-induced line shape parameters for O2- perturbed R(0) 0–0 line in H35Cl.J. Chem. Phys.159(13) (2023), doi:10.1063/5.0169968, http://dx.doi.org/10.1063/5.0169968
-
[16]
H.Jóźwiak,etal.,AccuratereferencespectraofHDinanH 2–Hebathforplanetaryapplications. Astron.Astrophys.687,A69(2024),doi:10.1051/0004-6361/202449889,https://doi.org/ 10.1051/0004-6361/202449889
-
[17]
J. Tennyson, S. N. Yurchenko, Laboratory spectra of hot molecules: Data needs for hot super- Earth exoplanets.Mol. Astrophys.8, 1–18 (2017), doi:10.1016/j.molap.2017.05.002,http: //dx.doi.org/10.1016/j.molap.2017.05.002
-
[18]
Niraula,et al., The impending opacity challenge in exoplanet atmospheric characterization
P. Niraula,et al., The impending opacity challenge in exoplanet atmospheric characterization. Nat. Astron.6(11), 1287–1295 (2022), doi:10.1038/s41550-022-01773-1,http://dx.doi. org/10.1038/s41550-022-01773-1. 25
-
[19]
K. L. Chubb,et al., Data availability and requirements relevant for the Ariel space mission and other exoplanet atmosphere applications.RAS Techniques and Instruments3(1), 636–690 (2024), doi:10.1093/rasti/rzae039,http://dx.doi.org/10.1093/rasti/rzae039
-
[20]
L. Wiesenfeld,et al., Ab Initio Quantum Dynamics as a Scalable Solution to the Exoplanet Opacity Challenge: A Case Study of CO2 in a Hydrogen Atmosphere.Astrophys. J.981(2), 148 (2025), doi:10.3847/1538-4357/adb02e,http://dx.doi.org/10.3847/1538-4357/ adb02e
-
[21]
J. L. Bohn, A. M. Rey, J. Ye, Cold molecules: Progress in quantum engineering of chemistry and quantum matter.Science357, 1002–1010 (2017)
2017
-
[22]
S. N. Vogels,et al., Imaging resonances in low-energy NO-He inelastic collisions.Science 350(6262), 787 (2015)
2015
-
[23]
R. Bause, A. Christianen, A. Schindewolf, I. Bloch, X.-Y. Luo, Ultracold Sticky Collisions: TheoreticalandExperimentalStatus.J.Phys.Chem.A127(3),729–741(2023),doi:10.1021/ acs.jpca.2c08095,http://dx.doi.org/10.1021/acs.jpca.2c08095
-
[24]
B. Margulis,et al., Tomography of Feshbach resonance states.Science380(6640), 77–81 (2023), doi:10.1126/science.adf9888,https://doi.org/10.1126/science.adf9888
-
[25]
K.P.Horn,etal.,FeshbachResonancesinColdCollisions:BenchmarkingState-of-the-ArtAb Initio Potential Energy Surfaces.J. Phys. Chem. Lett.16, 7862–7867 (2025), doi:10.1021/acs. jpclett.5c01581,https://pubs.acs.org/doi/abs/10.1021/acs.jpclett.5c01581
doi:10.1021/acs 2025
-
[26]
G. Tang,et al., Quantum state–resolved molecular dipolar collisions over four decades of energy.Science379(6636),1031–1036(2023),doi:10.1126/science.adf9836,https://doi. org/10.1126/science.adf9836
-
[27]
J. J. Park,et al., Spectrum of Feshbach Resonances inNaLi+NaCollisions.Phys. Rev. X 13, 031018 (2023), doi:10.1103/PhysRevX.13.031018,https://link.aps.org/doi/10. 1103/PhysRevX.13.031018. 26
-
[28]
M. Morita, M. B. Kosicki, P. S. Żuchowski, P. Brumer, T. V. Tscherbul, Magnetic Fesh- bach resonances in ultracold atom-molecule collisions.Phys. Rev. A110, L021301 (2024), doi:10.1103/PhysRevA.110.L021301,https://link.aps.org/doi/10.1103/PhysRevA. 110.L021301
-
[29]
Y.-X.Liu,etal.,Hyperfine-to-rotationalenergytransferinultracoldatom–moleculecollisions ofRbandKRb.Nat.Chem.17(5),688–694(2025),doi:10.1038/s41557-025-01778-z,https: //doi.org/10.1038/s41557-025-01778-z
-
[30]
M. B. Soley, E. J. Heller, Ultracold Molecular Collisions: Quasiclassical, Semiclassical, and Classical Approaches in the Quantum Regime.Chem. Rev.125(14), 6609–6652 (2025), doi: 10.1021/acs.chemrev.4c01014,https://doi.org/10.1021/acs.chemrev.4c01014
-
[31]
J. P. D’Incao, Few-body physics in resonantly interacting ultracold quantum gases.J. Phys. B51(4), 043001 (2018), doi:10.1088/1361-6455/aaa116,http://dx.doi.org/10.1088/ 1361-6455/aaa116
-
[32]
Haze,et al., Controlling few-body reaction pathways using a Feshbach resonance.Nat
S. Haze,et al., Controlling few-body reaction pathways using a Feshbach resonance.Nat. Phys.21(2), 228–232 (2025), doi:10.1038/s41567-024-02726-3,https://doi.org/10. 1038/s41567-024-02726-3
-
[33]
M. D. Higgins, C. H. Greene, Five-body recombination of identical bosons.Proc. Natl. Acad. Sci.USA122(18),e2503390122(2025),doi:10.1073/pnas.2503390122,https://doi.org/ 10.1073/pnas.2503390122
-
[34]
D. Skouteris, J. Castillo, D. Manolopoulos, ABC: a quantum reactive scattering program. Comput. Phys. Commun.133(1), 128–135 (2000), doi:10.1016/s0010-4655(00)00167-3, http://dx.doi.org/10.1016/s0010-4655(00)00167-3
-
[35]
D. Bostan, B. Mandal, D. Babikov, Mixed quantum/classical theory for rotationally inelastic scattering of identical collision partners revised.Phys. Chem. Chem. Phys.26(43), 27567– 27582 (2024), doi:10.1039/D4CP02806F,http://dx.doi.org/10.1039/D4CP02806F. 27
-
[36]
L. D. Thomas, Solution of the coupled equations of inelastic atom–molecule scattering for a single initial state.J. Chem. Phys.70(6), 2979–2985 (1979), doi:10.1063/1.437836,https: //doi.org/10.1063/1.437836
-
[37]
L. D. Thomas, Solution of the coupled equations of inelastic atom–molecule scattering for a single initial state. II. Use of nondiagonal matrix Green functions.J. Chem. Phys.76(10), 4925–4931 (1982), doi:10.1063/1.442838,https://doi.org/10.1063/1.442838
-
[38]
M. Rhoades-Brown, M. H. Macfarlane, S. C. Pieper, Techniques for heavy-ion coupled- channels calculations. II. Iterative solution of the coupled radial equations.Phys. Rev. C 21, 2436–2446 (1980), doi:10.1103/PhysRevC.21.2436,https://link.aps.org/doi/10. 1103/PhysRevC.21.2436
-
[39]
A. M. Arthurs, A. Dalgarno, The theory of scattering by a rigid rotator.Proc. R. Soc. Lond. Ser. A256(1287), 540–551 (1960), doi:10.1098/rspa.1960.0125,http://dx.doi.org/10. 1098/rspa.1960.0125
arXiv 1960
-
[40]
Johnson, The multichannel log-derivative method for scattering calculations.J
B. Johnson, The multichannel log-derivative method for scattering calculations.J. Comput. Phys.13(3), 445–449 (1973), doi:10.1016/0021-9991(73)90049-1,http://dx.doi.org/ 10.1016/0021-9991(73)90049-1
-
[41]
B. R. Johnson, The renormalized Numerov method applied to calculating bound states of the coupled-channel Schroedinger equation.J. Chem. Phys.69(10), 4678–4688 (1978), doi: 10.1063/1.436421,http://dx.doi.org/10.1063/1.436421
doi:10.1063/1.436421 1978
-
[42]
D. E. Manolopoulos, An improved log derivative method for inelastic scattering.J. Chem. Phys.85(11), 6425–6429 (1986), doi:10.1063/1.451472,http://dx.doi.org/10.1063/ 1.451472
-
[43]
Y. V. Suleimanov, T. V. Tscherbul, R. V. Krems, Efficient method for quantum calculations of molecule-molecule scattering properties in a magnetic field.J. Chem. Phys.137(2) (2012), doi:10.1063/1.4733288,http://dx.doi.org/10.1063/1.4733288
-
[44]
R. G. Newton,Scattering theory of waves and particles(Springer Science & Business Media) (2013). 28
2013
-
[45]
Child,Molecular Collision Theory(Wiley) (1974)
M. Child,Molecular Collision Theory(Wiley) (1974)
1974
-
[46]
R.T.Pack,G.A.Parker,Quantumreactivescatteringinthreedimensionsusinghyperspherical (APH) coordinates. Theory.J. Chem. Phys.87(7), 3888–3921 (1987), doi:10.1063/1.452944, https://doi.org/10.1063/1.452944
-
[47]
D. E. Manolopoulos, R. E. Wyatt, D. C. Clary, Iterative solution in quantum scattering theory. The log derivative Kohn approach.J. Chem. Soc., Faraday Trans.86(10), 1641–1648 (1990), doi:10.1039/FT9908601641,http://dx.doi.org/10.1039/FT9908601641
-
[48]
Weinberg, Quasiparticles and the Born Series.Phys
S. Weinberg, Quasiparticles and the Born Series.Phys. Rev.131, 440–460 (1963), doi:10. 1103/PhysRev.131.440,https://link.aps.org/doi/10.1103/PhysRev.131.440
-
[49]
J. Hoppe, C. Drischler, R. J. Furnstahl, K. Hebeler, A. Schwenk, Weinberg eigenvalues for chiral nucleon-nucleon interactions.Phys. Rev. C96, 054002 (2017), doi:10.1103/PhysRevC. 96.054002,https://link.aps.org/doi/10.1103/PhysRevC.96.054002
doi:10.1103/physrevc 2017
-
[50]
N. Balakrishnan, A. Dalgarno, R. C. Forrey, Vibrational relaxation of CO by collisions with 4Heatultracoldtemperatures.J.Chem.Phys.113(2),621–627(2000),doi:10.1063/1.481838, https://doi.org/10.1063/1.481838
-
[51]
C. Cecchi-Pestellini, E. Bodo, N. Balakrishnan, A. Dalgarno, Rotational and Vibrational Ex- citation of CO Molecules by Collisions with4He Atoms.Astrophys. J.571(2), 1015 (2002), doi:10.1086/340020,https://doi.org/10.1086/340020
-
[52]
P. M. Florian, M. Hoster, R. C. Forrey, Rotational relaxation in ultracoldCO+Hecollisions. Phys. Rev. A70, 032709 (2004), doi:10.1103/PhysRevA.70.032709,https://link.aps. org/doi/10.1103/PhysRevA.70.032709
-
[53]
Chem.7(4), 349–353 (2015), doi: 10.1038/nchem.2204,https://doi.org/10.1038/nchem.2204
A.Bergeat,J.Onvlee,C.Naulin,A.vanderAvoird,M.Costes,Quantumdynamicalresonances in low-energy CO(𝑗=0) + He inelastic collisions.Nat. Chem.7(4), 349–353 (2015), doi: 10.1038/nchem.2204,https://doi.org/10.1038/nchem.2204
-
[54]
H. Cybulski,et al., Ab initio study of the CO–N2 complex: a new highly accurate inter- molecular potential energy surface and rovibrational spectrum.Phys. Chem. Chem. Phys. 29 20(18), 12624–12636 (2018), doi:10.1039/c8cp01373j,http://dx.doi.org/10.1039/ c8cp01373j
-
[55]
R. D. Stephens, S. H. Cadle, Remote Sensing Measurements of Carbon Monoxide Emissions from On-Road Vehicles.J. Air Waste Manag. Assoc.41(1), 39–46 (1991), doi:10.1080/ 10473289.1991.10466823
arXiv 1991
-
[56]
W. W. McMillan,et al., An observational and modeling strategy to investigate the impact of remote sources on local air quality: A Houston, Texas, case study from the Second Texas Air Quality Study (TexAQS II).J. Geophys. Res.115(D1) (2010), doi:10.1029/2009jd011973
-
[57]
C. Shan,et al., Regional CO emission estimated from ground-based remote sensing at Hefei site, China.Atmos. Res.222, 25–35 (2019), doi:10.1016/j.atmosres.2019.02.005
-
[58]
J. C. W. W. W. Carole, N. Beale,Global climate change linkages: acid rain, air quality, and stratospheric ozone(Springer Science & Business Media) (1989)
1989
-
[59]
J. S. Daniel, S. Solomon, On the climate forcing of carbon monoxide.J. Geophys. Res.: Atmospheres103(D11), 13249–13260 (1998), doi:10.1029/98jd00822
-
[60]
A. Nishiyama,et al., Line-shape study of CO perturbed by N 2 with mid- infrared frequency comb-based Fourier-transform spectroscopy.Measurement227, 114273 (2024), doi:10.1016/j.measurement.2024.114273,http://dx.doi.org/10.1016/ j.measurement.2024.114273
arXiv 2024
-
[61]
D. J. Jacob,Introduction to atmospheric chemistry(Princeton University Press) (1999)
1999
-
[62]
D. Paredes-Roibás, R. Z. Martínez, H. Jóźwiak, F. Thibault, Collisional line broadening and mixing in the Raman spectrum of CO perturbed by N2: Experimental measurements and theoreticalcalculations.J.Quant.Spectrosc.Radiat.Transf.275,107868(2021),doi:10.1016/ j.jqsrt.2021.107868,http://dx.doi.org/10.1016/j.jqsrt.2021.107868
arXiv 2021
-
[63]
A.Zadrożny,H.Jóźwiak,E.Quintas-Sánchez,R.Dawes,P.Wcisło,Abinitioquantumscatter- ing calculations for the CO–O2 system and a new CO–O2 potential energy surface: O2 and air 30 broadening of the R(0) line in CO.J. Chem. Phys.157(17) (2022), doi:10.1063/5.0115654, http://dx.doi.org/10.1063/5.0115654
-
[64]
R. B. Lehoucq, D. C. Sorensen, C. Yang,ARPACK users’ guide: solution of large-scale eigenvalue problems with implicitly restarted Arnoldi methods(SIAM) (1998)
1998
-
[65]
F. Lique, A. Faure, eds.,Gas-Phase Chemistry in Space, 2514-3433 (IOP Publishing) (2019), doi:10.1088/2514-3433/aae1b5,https://doi.org/10.1088/2514-3433/aae1b5
-
[66]
𝑗𝑧 -conserving coupled states approximation.J
P.McGuire,D.J.Kouri,Quantummechanicalclosecouplingapproachtomolecularcollisions. 𝑗𝑧 -conserving coupled states approximation.J. Chem. Phys.60(6), 2488–2499 (1974), doi: 10.1063/1.1681388,https://doi.org/10.1063/1.1681388
-
[67]
C. Joy, B. Mandal, D. Bostan, M.-L. Dubernet, D. Babikov, Mixed quantum/classical theory (MQCT) approach to the dynamics of molecule–molecule collisions in complex systems. FaradayDiscuss.251,225–248(2024),doi:10.1039/d3fd00166k,http://dx.doi.org/10. 1039/d3fd00166k
-
[68]
D. G. Truhlar, Long-standing themes in computational chemical dynamics.Comput. Phys. Commun.84(1–3), 78–90 (1994), doi:10.1016/0010-4655(94)90204-6,http://dx.doi. org/10.1016/0010-4655(94)90204-6
-
[69]
C. Leforestier, K. Szalewicz, A. van der Avoird, Spectra of water dimer from a newab initio potential with flexible monomers.J. Chem. Phys.137(1), 014305 (2012), doi:10.1063/1. 4722338,https://doi.org/10.1063/1.4722338
doi:10.1063/1 2012
-
[70]
X.-G. Wang, S. Yang, J. Carrington, Tucker, D. H. Zhang, A numerically exact calculation of vibration–rotation–tunnelinglevelsofwaterdimeronanewaccuratepotentialenergysurface: Achieving sub-cm−1 accuracy from the terahertz to the infrared.J. Chem. Phys.163(14), 144308 (2025), doi:10.1063/5.0294206,https://doi.org/10.1063/5.0294206
-
[71]
K. A. Peterson, G. C. McBane, A hierarchical family of three-dimensional potential energy surfacesforHe-CO.J.Chem.Phys.123(8)(2005),doi:10.1063/1.1947194,http://dx.doi. org/10.1063/1.1947194. 31
-
[72]
K. P. Huber, G. Herzberg,Constants of diatomic molecules(Springer US, Boston, MA), pp. 8–689 (1979), doi:10.1007/978-1-4757-0961-2_2,https://doi.org/10.1007/ 978-1-4757-0961-2_2. Acknowledgments We thank George McBane and Jeremy Hutson for stimulating discussions in the early stages of this work and Nathan Prins for valuable comments. H. J. J. was support...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.