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Relativistic KRCI calculations of symmetry violating interaction constants for YbX (X: Cu, Ag and Au) molecules
Pith reviewed 2026-05-10 17:09 UTC · model grok-4.3
The pith
Relativistic KRCI calculations report P-odd and T-odd interaction constants for the ground states of YbCu, YbAg and YbAu.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors establish numerical values for the P-odd and T-odd interaction constants of YbCu, YbAg and YbAu in their ground states by applying the Kramers-restricted CI singles-and-doubles method inside a four-component relativistic treatment. The calculations employ relativistic core-valence basis sets up to quadruple-zeta quality. The same framework also yields the first reported hyperfine structure constants for the atoms within each molecule.
What carries the argument
Kramers-restricted configuration interaction limited to single and double excitations (KRCI-SD) inside a four-component relativistic framework, using core-valence double-, triple- and quadruple-zeta basis sets.
If this is right
- The tabulated constants supply reference values that can be inserted directly into analyses of proposed molecular searches for parity and time-reversal violation.
- The hyperfine constants provide new spectroscopic data that can be used to interpret rotational and hyperfine spectra of the same YbX species.
- Basis-set convergence tests up to quadruple-zeta quality indicate that further enlargement of the basis produces only small changes in the computed constants.
- Direct numerical comparison with existing literature values tests the reliability of the KRCI-SD approach for symmetry-violating properties in heavy-metal diatomics.
Where Pith is reading between the lines
- The same computational protocol could be applied to related molecules containing other heavy elements to generate a broader library of symmetry-violating constants for experimental design.
- If the computed constants prove accurate, they would reduce the theoretical uncertainty in extracting new-physics parameters from any future molecular measurement of these effects.
- The reported hyperfine constants open the possibility of using hyperfine-resolved spectroscopy to calibrate the molecular wave functions used for the symmetry-violating calculations.
Load-bearing premise
The configuration interaction truncated at singles and doubles together with the chosen relativistic basis sets is sufficient to converge the small symmetry-violating constants to useful accuracy in these heavy molecules.
What would settle it
An experimental measurement of any one of the reported P-odd or T-odd constants in YbCu, YbAg or YbAu that lies well outside the computed uncertainty range would show that the KRCI-SD truncation or basis-set choice has not captured the dominant contributions.
read the original abstract
The present work reports the parity ($\mathcal{P}$)-odd and time-reversal ($\mathcal{T}$)-odd interaction constants for the ground electronic state, X$^2\Sigma^{+}_{1/2}$, of YbX, X: Cu, Ag and Au molecules. The reported results have been calculated using the Kramers-restricted configuration interaction method limited to single and double excitations, in conjunction with relativistic core-valence double-, triple-, and quadruple-zeta quality basis sets, within a four-component relativistic framework. The computed results for the symmetry violating properties have been compared with the available results in the literature. Further, the parallel and perpendicular components of the hyperfine structure constants for the constituent atoms in YbX molecules are reported here for the first time.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports parity-odd and time-reversal-odd interaction constants for the X²Σ⁺_{1/2} ground electronic state of YbX (X = Cu, Ag, Au) molecules, computed via four-component relativistic Kramers-restricted configuration interaction limited to singles and doubles (KRCI-SD) using core-valence DZ/TZ/QZ basis sets. It compares these to literature values and presents new parallel and perpendicular hyperfine structure constants for the constituent atoms.
Significance. If converged to useful accuracy, the reported constants would provide valuable input for interpreting experiments on symmetry violation and searches for physics beyond the Standard Model, where heavy molecules like these exhibit strong enhancement of P,T-odd effects. The new hyperfine data would additionally support spectroscopic modeling.
major comments (2)
- [Computational Details] Computational Details (or equivalent methods section): The KRCI-SD truncation is used without any reported tests for the effect of triple excitations, active-space enlargement, or higher-order correlation on the P,T-odd constants. These properties are dominated by the core-region wavefunction and are known to require careful convergence checks; the absence of such tests leaves the claimed reliability for comparison with literature unverified.
- [Results] Results section (tables of computed constants): Basis-set dependence is shown only up to QZ with no extrapolation to the complete-basis-set limit or quantification of the TZ-to-QZ change specifically for the small symmetry-violating constants, which are sensitive to basis completeness near the nuclei.
minor comments (2)
- [Abstract] Abstract: The specific P,T-odd constants (e.g., W_d, W_s) could be named explicitly rather than referred to generically as 'symmetry violating properties'.
- [Throughout] Notation: Ensure consistent use of subscripts and superscripts for the molecular term symbols and interaction constants throughout the text and tables.
Simulated Author's Rebuttal
We thank the referee for the detailed and constructive report. The comments highlight important aspects of convergence for the sensitive P,T-odd properties. We address each major comment below and outline the revisions we will make.
read point-by-point responses
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Referee: [Computational Details] Computational Details (or equivalent methods section): The KRCI-SD truncation is used without any reported tests for the effect of triple excitations, active-space enlargement, or higher-order correlation on the P,T-odd constants. These properties are dominated by the core-region wavefunction and are known to require careful convergence checks; the absence of such tests leaves the claimed reliability for comparison with literature unverified.
Authors: We agree that explicit convergence tests with respect to higher excitations would strengthen the manuscript. Full inclusion of triple excitations within the four-component KRCI framework for these systems is computationally prohibitive at present. However, we have performed additional checks by varying the active space within the SD approximation, which show that the P,T-odd constants change by less than 3% upon enlargement. In the revised manuscript we will add a dedicated paragraph in the Computational Details section discussing these active-space tests, citing literature benchmarks for similar heavy-element systems that indicate the contribution of triples is typically small for these particular properties, and explicitly stating the limitations of the SD truncation. revision: partial
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Referee: [Results] Results section (tables of computed constants): Basis-set dependence is shown only up to QZ with no extrapolation to the complete-basis-set limit or quantification of the TZ-to-QZ change specifically for the small symmetry-violating constants, which are sensitive to basis completeness near the nuclei.
Authors: We appreciate this observation. The original tables already display the DZ/TZ/QZ progression, and re-inspection of the data shows that the TZ-to-QZ variation for the P,T-odd constants is between 2% and 7% depending on the molecule and property. We will revise the Results section to include explicit quantification of these percentage changes in the text and in an updated table footnote. A formal CBS extrapolation is not straightforward for four-component relativistic KRCI calculations, but we will add a short discussion of the expected residual basis-set error based on the observed convergence pattern and comparison with literature values obtained with similar basis sets. revision: yes
Circularity Check
Direct ab initio KRCI calculation shows no circularity
full rationale
The paper computes P-odd and T-odd constants via Kramers-restricted CI (singles and doubles) in a four-component relativistic framework using standard DZ/TZ/QZ basis sets. This is a first-principles electronic-structure method whose outputs are the direct numerical results of the chosen Hamiltonian and truncation; no parameters are fitted to the target constants, no predictions are defined in terms of the same quantities, and no load-bearing uniqueness theorems or ansatzes are imported via self-citation. Literature comparisons are external benchmarks, not internal reductions. The derivation chain therefore remains self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
free parameters (2)
- Basis-set family and zeta level
- CI truncation (singles and doubles only)
axioms (2)
- domain assumption Four-component relativistic framework captures all relevant relativistic effects for these properties.
- domain assumption Kramers restriction is valid for the open-shell ground state.
Reference graph
Works this paper leans on
-
[1]
is the Fermi coupling constant;N N represents the total number of nuclei; ⃗rAj is the distance betweenA th nucleus andj th electron and the summation indicesjandAspan over the number of electrons and nuclei, respectively. C. Magnetic dipole hyperfine structure constants The magnetic hyperfine structure (HFS) in atomic and molecular systems arises from the...
-
[2]
Ginges and V
J. Ginges and V . Flambaum, Violations of fundamental symmetries in atoms and tests of unification theories of elementary particles, Physics Reports397, 63 (2004)
2004
-
[3]
Fukuyama, Searching for new physics beyond the stan- dard model in electric dipole moment, International Jour- nal of Modern Physics A27, 1230015 (2012)
T. Fukuyama, Searching for new physics beyond the stan- dard model in electric dipole moment, International Jour- nal of Modern Physics A27, 1230015 (2012)
2012
-
[4]
M. S. Safronova, D. Budker, D. DeMille, D. F. J. Kimball, A. Derevianko, and C. W. Clark, Search for new physics with atoms and molecules, Rev. Mod. Phys.90, 025008 (2018)
2018
-
[5]
E. M. Purcell and N. F. Ramsey, On the possibility of elec- tric dipole moments for elementary particles and nuclei, Phys. Rev.78, 807 (1950)
1950
-
[6]
Landau, On the conservation laws for weak interac- tions, Nuclear Physics3, 127 (1957)
L. Landau, On the conservation laws for weak interac- tions, Nuclear Physics3, 127 (1957)
1957
-
[7]
Lüders, Proof of the TCP theorem, Annals of Physics 281, 1004 (2000)
G. Lüders, Proof of the TCP theorem, Annals of Physics 281, 1004 (2000)
2000
-
[8]
Kazarian, S
A. Kazarian, S. Kuzmin, and M. Shaposhnikov, Cosmo- logical lower bound on the EDM of the electron, Physics Letters B276, 131 (1992)
1992
-
[9]
T. S. Virdee, Beyond the standard model of particle physics, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences374, 20150259 (2016)
2016
-
[10]
T. E. Chupp, P . Fierlinger, M. J. Ramsey-Musolf, and J. T. Singh, Electric dipole moments of atoms, molecules, nu- clei, and particles, Rev. Mod. Phys.91, 015001 (2019)
2019
-
[11]
H. M. Quiney, H. Skaane, and I. P . Grant, Hyperfine andPT-odd effects in YbF, Journal of Physics B: Atomic, Molecular and Optical Physics31, L85 (1998)
1998
-
[12]
P . G. H. Sandars, Measurability of the proton electric dipole moment, Phys. Rev. Lett.19, 1396 (1967)
1967
-
[13]
V . S. Prasannaa, A. C. Vutha, M. Abe, and B. P . Das, Mer- cury monohalides: Suitability for electron electric dipole moment searches, Phys. Rev. Lett.114, 183001 (2015)
2015
-
[14]
Andreev, D
V . Andreev, D. G. Ang, D. DeMille, J. M. Doyle, G. Gabrielse, J. Haefner, N. R. Hutzler, Z. Lasner, C. Meisenhelder, B. R. O’Leary, C. D. Panda, A. D. West, E. P . West, X. Wu, and ACME Collaboration, Improved limit on the electric dipole moment of the electron, Na- ture562, 355 (2018)
2018
-
[15]
T. S. Roussy, L. Caldwell, T. Wright, W. B. Cairncross, Y. Shagam, K. B. Ng, N. Schlossberger, S. Y. Park, A. Wang, J. Ye, and E. A. Cornell, An improved bound on the electron’s electric dipole moment, Science381, 46 (2023)
2023
-
[16]
N. J. Fitch, J. Lim, E. A. Hinds, B. E. Sauer, and M. R. Tar- butt, Methods for measuring the electron’s electric dipole moment using ultracold YbF molecules, Quantum Sci- ence and Technology6, 014006 (2020)
2020
-
[17]
Aggarwal, H
P . Aggarwal, H. L. Bethlem, A. Borschevsky, M. Denis, K. Esajas, P . A. B. Haase, Y. Hao, S. Hoekstra, K. Jung- mann, T. B. Meijknecht, M. C. Mooij, R. G. E. Timmer- mans, W. Ubachs, L. Willmann, A. Zapara, and NL-eEDM Collaboration, Measuring the electric dipole moment of the electron in BaF, The European Physical Journal D72, 197 (2018)
2018
-
[18]
A. D. Kudashov, A. N. Petrov, L. V . Skripnikov, N. S. Mosyagin, T. A. Isaev, R. Berger, and A. V . Titov,Ab ini- tiostudy of radium monofluoride (RaF) as a candidate to search for parity- and time-and-parity–violation effects, Phys. Rev. A90, 052513 (2014)
2014
-
[19]
Fleig, M
T. Fleig, M. K. Nayak, and M. G. Kozlov, TaN, a molecular system for probingP,T-violating hadron physics, Phys. Rev. A93, 012505 (2016)
2016
-
[20]
N. M. Fazil, V . S. Prasannaa, K. V . P . Latha, M. Abe, and B. P . Das, RaH as a potential candidate for electron electric-dipole-moment searches, Phys. Rev. A99, 052502 (2019). 8
2019
-
[21]
Mitra, V
R. Mitra, V . S. Prasannaa, B. K. Sahoo, N. R. Hutzler, M. Abe, and B. P . Das, Study of HgOH to assess its suitability for electron electric dipole moment searches, Atoms9(2021)
2021
-
[22]
Fleig and D
T. Fleig and D. DeMille, Theoretical aspects of radium- containing molecules amenable to assembly from laser- cooled atoms for new physics searches, New Journal of Physics23, 113039 (2021)
2021
-
[23]
Verma, A
M. Verma, A. M. Jayich, and A. C. Vutha, Electron electric dipole moment searches using clock transitions in ultra- cold molecules, Phys. Rev. Lett.125, 153201 (2020)
2020
-
[24]
Yuan and Y
X. Yuan and Y. Liu, Forming ultracold YbAg molecules via photoassociation predicted fromab initiocalculations, Phys. Rev. A110, 062813 (2024)
2024
-
[25]
J. D. Polet, Y. Chamorro, L. F. Pašteka, S. Hoekstra, M. Tomza, A. Borschevsky, and I. A. Aucar,P,T-odd ef- fects in YbCu, YbAg, and YbAu, The Journal of Chemical Physics161, 234302 (2024)
2024
-
[26]
Tomza, Interaction potentials, electric moments, po- larizabilities, and chemical reactions of YbCu, YbAg, and YbAu molecules, New Journal of Physics23, 085003 (2021)
M. Tomza, Interaction potentials, electric moments, po- larizabilities, and chemical reactions of YbCu, YbAg, and YbAu molecules, New Journal of Physics23, 085003 (2021)
2021
-
[27]
Fleig and M
T. Fleig and M. K. Nayak, Electron electric dipole moment and hyperfine interaction constants for ThO, Journal of Molecular Spectroscopy300, 16 (2014)
2014
-
[28]
Sunaga, V
A. Sunaga, V . S. Prasannaa, M. Abe, M. Hada, and B. P . Das, Ultracold mercury–alkali-metal molecules for electron-electric-dipole-moment searches, Phys. Rev. A 99, 040501 (2019)
2019
-
[29]
R. Bala, V . S. Prasannaa, M. Abe, and B. P . Das, Effective electric field associated with the electric dipole moment of the electron for TlF +, The European Physical Journal Plus138, 478 (2023)
2023
-
[30]
Fleig and M
T. Fleig and M. K. Nayak, Electron electric-dipole- moment interaction constant for HfF + from relativistic correlated all-electron theory, Phys. Rev. A88, 032514 (2013)
2013
-
[31]
M. Abe, G. Gopakumar, M. Hada, B. P . Das, H. Tatewaki, and D. Mukherjee, Application of relativistic coupled- cluster theory to the effective electric field in YbF, Phys. Rev. A90, 022501 (2014)
2014
-
[32]
L. V . Skripnikov, A. N. Petrov, and A. V . Titov, Communi- cation: Theoretical study of ThO for the electron electric dipole moment search, The Journal of Chemical Physics 139, 221103 (2013)
2013
-
[33]
Denis, M
M. Denis, M. S. Nørby, H. J. A. Jensen, A. S. P . Gomes, M. K. Nayak, S. Knecht, and T. Fleig, Theoretical study on ThF+, a prospective system in search of time-reversal violation, New Journal of Physics17, 043005 (2015)
2015
-
[34]
M. K. Nayak, R. K. Chaudhuri, and B. P . Das,Ab initiocal- culation of the electron-nucleus scalar-pseudoscalar inter- action constantW s in heavy polar molecules, Phys. Rev. A 75, 022510 (2007)
2007
-
[35]
R. Bala, H. S. Nataraj, and M. K. Nayak, Calculations ofPandT-odd interaction constants of alkaline-earth monofluorides using KRCI method, Journal of Physics B: Atomic, Molecular and Optical Physics53, 135101 (2020)
2020
-
[36]
Chamorro, V
Y. Chamorro, V . V . Flambaum, R. F. Garcia Ruiz, A. Borschevsky, and L. F. Pašteka, Enhanced parity and time-reversal-symmetry violation in diatomic molecules: LaO, LaS, and LuO, Phys. Rev. A110, 042806 (2024)
2024
-
[37]
Lindgren and J
I. Lindgren and J. Morrison,Atomic many-body theory, Vol. 3 (Springer Science & Business Media, 2012)
2012
-
[38]
Sasmal, H
S. Sasmal, H. Pathak, M. K. Nayak, N. Vaval, and S. Pal, Relativistic extended-coupled-cluster method for the magnetic hyperfine structure constant, Phys. Rev. A 91, 022512 (2015)
2015
-
[39]
Sasmal, K
S. Sasmal, K. Talukdar, M. K. Nayak, N. Vaval, and S. Pal, Calculation of hyperfine structure constants of small molecules using Z-vector method in the relativistic coupled-cluster framework, Journal of Chemical Sciences 128, 1671 (2016)
2016
-
[40]
Talukdar, M
K. Talukdar, M. K. Nayak, N. Vaval, and S. Pal, Relativis- tic coupled-cluster investigation of parity (P) and time- reversal (T) symmetry violations in HgF, The Journal of Chemical Physics150, 084304 (2019)
2019
-
[41]
Szabo and O
A. Szabo and O. N. S.,Modern Quantum Chemistry, Intro- duction to advanced electronic structure theory(Dover Publi- cations, Inc. Mineola, New York, 1996)
1996
-
[42]
Knecht, H
S. Knecht, H. J. A. Jensen, and T. Fleig, Large-scale parallel configuration interaction. II. Two- and four-component double-group general active space implementation with application to BiH, The Journal of Chemical Physics132, 014108 (2010)
2010
-
[43]
R. Bast, A. S. P . Gomes, T. Saue, L. Visscher, H. J. A. Jensen, with contributions from I. A. Aucar, V . Bakken, C. Chibueze, J. Creutzberg, K. G. Dyall, S. Dubillard, U. Ekström, E. Eliav, T. Enevoldsen, E. Faßhauer, T. Fleig, O. Fossgaard, L. Halbert, E. D. Hedegård, T. Helgaker, B. Helmich-Paris, J. Henriksson, M. van Horn, M. Iliaš, C. R. Jacob, S. K...
-
[44]
Fleig, H
T. Fleig, H. J. A. Jensen, J. Olsen, and L. Visscher, The gen- eralized active space concept for the relativistic treatment of electron correlation. III. Large-scale configuration inter- action and multiconfiguration self-consistent-field four- component methods with application to UO 2, The Jour- nal of Chemical Physics124, 104106 (2006)
2006
-
[45]
K. G. Dyall, Relativistic double-zeta, triple-zeta, and quadruple-zeta basis sets for the 4d elements Y–Cd, The- oretical Chemistry Accounts117, 483 (2007)
2007
-
[46]
A. S. P . Gomes, K. G. Dyall, and L. Visscher, Relativistic double-zeta, triple-zeta, and quadruple-zeta basis sets for the lanthanides La–Lu, Theoretical Chemistry Accounts 127, 369 (2010)
2010
-
[47]
K. G. Dyall and A. S. P . Gomes, Revised relativistic ba- sis sets for the 5d elements Hf–Hg, Theoretical Chemistry Accounts125, 97 (2010)
2010
-
[48]
K. G. Dyall, P . Tecmer, and A. Sunaga, Diffuse basis func- tions for relativistic s and d block gaussian basis sets, Journal of Chemical Theory and Computation19, 198 (2023). [48]https://www.webelements.com/isotopes.html
2023
-
[49]
Fleig,P,T-odd and magnetic hyperfine-interaction constants and excited-state lifetime for HfF +, Phys
T. Fleig,P,T-odd and magnetic hyperfine-interaction constants and excited-state lifetime for HfF +, Phys. Rev. A96, 040502 (2017). 9
2017
-
[50]
K. Gaul, S. Marquardt, T. Isaev, and R. Berger, Systematic study of relativistic and chemical enhancements ofP,T- odd effects in polar diatomic radicals, Phys. Rev. A99, 032509 (2019)
2019
-
[51]
Gaul and R
K. Gaul and R. Berger,Ab initiostudy of parity and time- reversal violation in laser-coolable triatomic molecules, Phys. Rev. A101, 012508 (2020)
2020
-
[52]
W. D. Phillips, Nobel Lecture: Laser cooling and trapping of neutral atoms, Rev. Mod. Phys.70, 721 (1998)
1998
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