arxiv: 2604.07376 · v1 · submitted 2026-04-07 · ❄️ cond-mat.str-el · cond-mat.mtrl-sci

K₂Co₂(TeO₃)₃ cdot 2.5 H₂O : A mineral-inspired pseudo-honeycomb cobalt dimer antiferromagnet

Austin M. Ferrenti , Maxime A. Siegler , Yiqing Hao , Chris Lygouras , Tong Chen , Tiffany A. Soetojo , Megan R. Rutherford , Kenji M. Kojima

show 4 more authors

Huibo Cao Natalia Drichko Alannah M. Hallas Tyrel M. McQueen

This is my paper

Pith reviewed 2026-05-10 18:00 UTC · model grok-4.3

classification ❄️ cond-mat.str-el cond-mat.mtrl-sci

keywords cobalt telluriteantiferromagnetpseudo-honeycomb latticemuon spin relaxationhydroflux synthesisdimer antiferromagnetlong-range ordertellurite bridge

0 comments p. Extension

The pith

A cobalt tellurite orders antiferromagnetically below 7.6 K with moments confined to the pseudo-honeycomb plane.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper describes the hydroflux synthesis of K2Co2(TeO3)3 · 2.5 H2O, a zemannite-type compound that mixes triangular dimer and pseudo-honeycomb structural elements. Magnetometry and specific heat measurements establish long-range antiferromagnetic order below 7.6 K, while neutron diffraction and muon spin relaxation show that the ordered moments lie mostly within the pseudo-honeycomb planes. The authors attribute this planar motif to net antiferromagnetic couplings transmitted through bridging tellurite groups, which differ from the negligible or ferromagnetic inter-dimer interactions found in most dimer chain systems. Three distinct zero-field μSR frequencies further indicate unusually low structural disorder in the as-grown crystals.

Core claim

Bulk magnetometry and specific heat data support the onset of long-range AFM order below T_N = 7.6(1) K, with neutron diffraction and μSR measurements placing the majority of the ordered moment within the pseudo-honeycomb plane. The largely planar ordering motif observed in KCoTOH is instead stabilized by net antiferromagnetic interactions through bridging tellurite groups. This work highlights the potential of hydroflux synthesis methods in the stabilization of magnetic materials possessing novel and potentially more frustrated lattice geometries.

What carries the argument

Bridging tellurite groups that transmit net antiferromagnetic interactions between cobalt dimers, producing a planar ordering motif in the pseudo-honeycomb lattice.

If this is right

Long-range antiferromagnetic order sets in below 7.6 K with the majority of the moment lying in the pseudo-honeycomb plane.
Net antiferromagnetic coupling via tellurite bridges overrides the ferromagnetic or negligible inter-dimer interactions typical of cobalt dimer chains.
Three unique zero-field μSR frequencies indicate a remarkably low level of structural disorder in as-grown crystals.
Hydroflux synthesis provides access to hybrid lattice geometries that combine dimer and honeycomb motifs.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

The low-disorder pseudo-honeycomb motif may serve as a platform for tuning frustration through chemical substitution or pressure.
Comparison with other zemannite-type phases could isolate the role of hydration in stabilizing the observed magnetic structure.
Extension of hydroflux methods to related tellurites might yield additional low-disorder cobaltates for studying dimer-based magnetism.

Load-bearing premise

The planar ordering motif is caused by net antiferromagnetic interactions through the bridging tellurite groups rather than other exchange paths or disorder effects.

What would settle it

Detection of substantial out-of-plane ordered moments by neutron diffraction or more than three μSR frequencies indicating significant disorder would undermine the proposed ordering mechanism and low-disorder interpretation.

read the original abstract

In recent years, magnetically-frustrated triangular and honeycomb lattice cobaltates have seen extensive study in the pursuit of a quantum spin liquid (QSL) state in a real material. In this work, we describe the hydroflux synthesis of K$_2$Co$_2$(TeO$_{3}$)$_{3}$ $\cdot$ 2.5 H$_2$O (KCoTOH), a novel zemannite-type antiferromagnet (AFM) possessing structural elements of both triangular dimer and honeycomb structural motifs. Bulk magnetometry and specific heat data support the onset of long-range AFM order below $T_\text{N}$ = 7.6(1) K, with neutron diffraction and muon spin relaxation ($\mu$SR) measurements placing the majority of the ordered moment within the pseudo-honeycomb plane. We resolve three unique oscillation frequencies from the zero-field $\mu$SR spectra, additionally suggesting a remarkably low level of structural disorder in as-grown KCoTOH crystals. Whereas interactions between dimerized chains of Co$^{2+}$ cations are typically observed to be negligible or ferromagnetic in nature, the largely planar ordering motif observed in KCoTOH is instead stabilized by net antiferromagnetic interactions through bridging tellurite groups. This work highlights the potential of hydroflux synthesis methods in the stabilization of magnetic materials possessing novel and potentially more frustrated lattice geometries.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Desk Editor's Note private letter to a colleague

Solid experimental report on a new zemannite cobalt tellurite with AFM order at 7.6 K and planar moments, but the tellurite-bridge stabilization claim rests on structure and consistency rather than measured or calculated exchanges.

read the letter

This paper gives the synthesis and basic magnetic characterization of K2Co2(TeO3)3·2.5H2O, a zemannite-type material that mixes cobalt dimer chains with a pseudo-honeycomb motif. Hydroflux growth produces crystals that order antiferromagnetically below 7.6 K. Neutron diffraction and zero-field muSR place most of the ordered moment in the plane, and the muSR spectra resolve three frequencies that point to low structural disorder in the as-grown material. Specific heat and magnetometry line up with the transition temperature. Those measurements are the concrete contribution here, and the low-disorder muSR result is particularly clean for this class of compounds. The authors note that planar order is unusual because dimer-chain couplings are often weak or ferromagnetic, so they attribute the stabilization to net antiferromagnetic superexchange through the bridging tellurite groups. The structure and the observed moment direction are consistent with that picture, but the manuscript does not include DFT-derived J values, mean-field fits that isolate the tellurite path, or comparisons to isostructural phases lacking those bridges. The causal assignment therefore stays inferential. The work is aimed at groups searching for new frustrated cobaltates or mineral-inspired lattices. It supplies one additional well-characterized example with usable data, but it does not claim a spin liquid or test a specific theoretical prediction. I would send it for peer review because the experimental results are real and the material is new; the discussion section would benefit from tighter quantitative support on the exchange paths, but that is a normal revision point rather than a fatal gap.

Referee Report

2 major / 3 minor

Summary. This manuscript reports the hydroflux synthesis of the novel zemannite-type compound K₂Co₂(TeO₃)₃ · 2.5 H₂O (KCoTOH), which combines triangular dimer and pseudo-honeycomb structural motifs. Bulk magnetometry and specific-heat measurements establish long-range antiferromagnetic order below T_N = 7.6(1) K. Neutron diffraction and zero-field μSR data indicate that the ordered Co²⁺ moments lie predominantly within the pseudo-honeycomb plane, with three distinct μSR precession frequencies interpreted as evidence of low structural disorder. The authors conclude that this planar ordering motif is stabilized by net antiferromagnetic superexchange through bridging tellurite groups rather than the more common intra-dimer or chain pathways.

Significance. If the central observations hold, the work adds a new, mineral-inspired cobaltate to the catalog of frustrated magnets and demonstrates the utility of hydroflux methods for accessing hybrid dimer-honeycomb lattices. The multi-technique characterization (magnetometry, heat capacity, neutron diffraction, μSR) and the reported low disorder are clear strengths that could enable future inelastic neutron or NMR studies. The interpretive claim linking the planar order specifically to tellurite-mediated AFM interactions, however, remains an inference without quantitative exchange-path support, limiting the immediate impact on models of frustrated magnetism.

major comments (2)

[Discussion] Discussion section (final paragraph): the claim that 'the largely planar ordering motif observed in KCoTOH is instead stabilized by net antiferromagnetic interactions through bridging tellurite groups' is not supported by any DFT-derived J values, mean-field or susceptibility fitting that isolates the tellurite superexchange, or comparison to isostructural compounds lacking those bridges. Neutron diffraction confirms moment direction and μSR resolves three frequencies, but neither directly measures the sign or magnitude of the inter-dimer coupling; the causal assignment therefore remains an untested inference that is load-bearing for the paper's magnetic-structure interpretation.
[Results] Results (μSR and neutron sections): while three oscillation frequencies are reported, the manuscript supplies no tabulated values, temperature dependence, or fitting details (e.g., amplitudes, relaxation rates, or error bars on the ordered moment from neutron refinement). Without these quantitative data the assertion of 'remarkably low level of structural disorder' cannot be rigorously assessed and weakens the claim that the observed frequencies are intrinsic.

minor comments (3)

Figure captions and legends should explicitly label the three μSR frequencies and indicate which data sets correspond to which temperature or field.
[Introduction] Add a brief comparison table or text reference to the magnetic ordering motifs and T_N values of related cobalt tellurites or zemannite-type compounds to place the new results in context.
Ensure all error bars on T_N, ordered-moment size, and susceptibility fits are reported consistently in the text and figures.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their thorough review and constructive feedback on our manuscript. We address each major comment below, providing clarifications and revisions where appropriate to strengthen the presentation without overstating the available data.

read point-by-point responses

Referee: Discussion section (final paragraph): the claim that 'the largely planar ordering motif observed in KCoTOH is instead stabilized by net antiferromagnetic interactions through bridging tellurite groups' is not supported by any DFT-derived J values, mean-field or susceptibility fitting that isolates the tellurite superexchange, or comparison to isostructural compounds lacking those bridges. Neutron diffraction confirms moment direction and μSR resolves three frequencies, but neither directly measures the sign or magnitude of the inter-dimer coupling; the causal assignment therefore remains an untested inference that is load-bearing for the paper's magnetic-structure interpretation.

Authors: We agree that the assignment of the planar ordering to tellurite-mediated AFM superexchange is an inference rather than a direct measurement. The manuscript bases this on the observed in-plane moment orientation from neutron diffraction, the three distinct μSR frequencies indicating a well-defined magnetic structure, and the structural topology where tellurite bridges provide the primary inter-dimer connectivity—contrasting with other Co^{2+} dimer systems where such couplings are typically FM or negligible. No DFT calculations or explicit J-value fitting are presented, as these were outside the scope of the current multi-technique experimental study. In the revised manuscript, we have softened the language in the final discussion paragraph to describe this as a 'plausible stabilization mechanism consistent with the structural motifs and observed ordering,' and we explicitly note the need for future theoretical work or inelastic neutron scattering to quantify the exchanges. revision: partial
Referee: Results (μSR and neutron sections): while three oscillation frequencies are reported, the manuscript supplies no tabulated values, temperature dependence, or fitting details (e.g., amplitudes, relaxation rates, or error bars on the ordered moment from neutron refinement). Without these quantitative data the assertion of 'remarkably low level of structural disorder' cannot be rigorously assessed and weakens the claim that the observed frequencies are intrinsic.

Authors: We accept this point and have revised the Results sections to include the requested quantitative details. A new table has been added listing the three μSR precession frequencies, their relative amplitudes, and relaxation rates at base temperature, along with the temperature dependence of the frequencies up to T_N. For the neutron diffraction, we now report the refined ordered moment magnitude with error bars and the temperature evolution of the magnetic Bragg peak intensity. These additions support the low-disorder assessment through the sharpness of the transitions and consistency of the frequencies, and we have updated the text to reference the new table and figures explicitly. revision: yes

Circularity Check

0 steps flagged

No circularity: purely experimental report with no derivations or self-referential predictions

full rationale

This is an experimental materials characterization paper reporting synthesis, crystal structure, bulk magnetometry, specific heat, neutron diffraction, and μSR data on KCoTOH. The central claims (T_N = 7.6 K, planar AFM order, low disorder from three μSR frequencies, and inference that tellurite bridges stabilize the motif) rest on direct measurements and structural observations rather than any equations, fitted parameters renamed as predictions, or load-bearing self-citations. No derivation chain exists that reduces to its own inputs by construction; interpretations are inferences from data, not self-definitional or statistically forced results.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claims rest on standard experimental interpretation of magnetic and diffraction data for a newly synthesized material; no free parameters are introduced, no new entities are postulated, and the axioms are conventional assumptions of condensed-matter physics.

axioms (2)

domain assumption Magnetic susceptibility and specific heat anomalies indicate the onset of long-range antiferromagnetic order.
Standard interpretation used throughout the field for identifying magnetic phase transitions.
standard math Neutron diffraction and zero-field μSR can determine the direction of the ordered moment and the number of distinct local magnetic environments.
Established techniques whose capabilities are assumed without re-derivation.

pith-pipeline@v0.9.0 · 5634 in / 1588 out tokens · 72191 ms · 2026-05-10T18:00:46.214894+00:00 · methodology

discussion (0)

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

IndisputableMonolith/Cost/FunctionalEquation.lean washburn_uniqueness_aczel unclear

?

unclear
Relation between the paper passage and the cited Recognition theorem.

the largely planar ordering motif observed in KCoTOH is instead stabilized by net antiferromagnetic interactions through bridging tellurite groups
IndisputableMonolith/Foundation/DimensionForcing.lean alexander_duality_circle_linking unclear

?

unclear
Relation between the paper passage and the cited Recognition theorem.

critical exponent of the order parameter ... β = 0.14(2), consistent with ... 2D-Ising system

What do these tags mean?

matches: The paper's claim is directly supported by a theorem in the formal canon.
supports: The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends: The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses: The paper appears to rely on the theorem as machinery.
contradicts: The paper's claim conflicts with a theorem or certificate in the canon.
unclear: Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

39 extracted references · 39 canonical work pages

[1]

Balents, Spin liquids in frustrated magnets.Nature464(7286), 199–208 (2010)

L. Balents, Spin liquids in frustrated magnets.Nature464(7286), 199–208 (2010)

work page 2010
[2]

Broholm,et al., Quantum spin liquids.Science367(6475), eaay0668 (2020)

C. Broholm,et al., Quantum spin liquids.Science367(6475), eaay0668 (2020)

work page 2020
[3]

J. A. Paddison,et al., Continuous excitations of the triangular-lattice quantum spin liquid YbMgGaO4.Nature Physics13(2), 117–122 (2017)

work page 2017
[4]

Zhong, S

R. Zhong, S. Guo, L. T. Nguyen, R. J. Cava, Frustrated spin-1/2 dimer compound K2Co2(SeO3)3 with easy-axis anisotropy.Physical Review B102(22), 224430 (2020)

work page 2020
[5]

Banerjee,et al., Neutron scattering in the proximate quantum spin liquid𝛼-RuCl 3.Science 356(6342), 1055–1059 (2017)

A. Banerjee,et al., Neutron scattering in the proximate quantum spin liquid𝛼-RuCl 3.Science 356(6342), 1055–1059 (2017)

work page 2017
[6]

Halloran,et al., Continuum of magnetic excitations in the Kitaev honeycomb iridate D3LiIr2O6.npj Quantum Materials10(1), 1–7 (2025)

T. Halloran,et al., Continuum of magnetic excitations in the Kitaev honeycomb iridate D3LiIr2O6.npj Quantum Materials10(1), 1–7 (2025)

work page 2025
[7]

Miao,et al., Persistent spin dynamics in magnetically ordered honeycomb-lattice cobalt oxides.Physical Review B109(13), 134431 (2024)

P. Miao,et al., Persistent spin dynamics in magnetically ordered honeycomb-lattice cobalt oxides.Physical Review B109(13), 134431 (2024)

work page 2024
[8]

J. R. Chamorro, T. M. McQueen, T. T. Tran, Chemistry of quantum spin liquids.Chemical Reviews121(5), 2898–2934 (2020)

work page 2020
[9]

Halloran,et al., Geometrical frustration versus Kitaev interactions in BaCo 2(AsO4)2.Pro- ceedings of the National Academy of Sciences120(2), e2215509119 (2023)

T. Halloran,et al., Geometrical frustration versus Kitaev interactions in BaCo 2(AsO4)2.Pro- ceedings of the National Academy of Sciences120(2), e2215509119 (2023)

work page 2023
[10]

Kitaev, Anyons in an exactly solved model and beyond.Annals of Physics321(1), 2–111 (2006)

A. Kitaev, Anyons in an exactly solved model and beyond.Annals of Physics321(1), 2–111 (2006)

work page 2006
[11]

P. A. Maksimov,et al., Ab initio guided minimal model for the “Kitaev” material BaCo2(AsO4)2: Importance of direct hopping, third-neighbor exchange, and quantum fluc- tuations.Physical Review B106(16), 165131 (2022)

work page 2022
[12]

O. P. Missen, S. J. Mills, J. Spratt, Crystal chemistry of zemannite-type structures: II. Synthetic sodium zemannite.European Journal of Mineralogy31(3), 529–536 (2019). 17

work page 2019
[13]

Huang, Z

X. Huang, Z. Zhao, M. Zhang, Z. He, Crystal-to-crystal transformation of a new selenite compound CaNi 2(SeO3)3 ·2 H 2O induced by dehydration.CrystEngComm23(17), 3126– 3132 (2021)

work page 2021
[14]

F. Eder, A. Marsollier, M. Weil, Structural studies on synthetic A2−𝑥[M2(TeO3)3]·n H 2O phases (A= Na, K, Rb, Cs; M= Mn, Co, Ni, Cu, Zn) with zemannite-type structures.Mineralogy and Petrology117(2), 145–163 (2023)

work page 2023
[15]

Liu,et al., Magnetism and ESR of the𝑆 eff = 1/2 antiferromagnet BaCo 2(SeO3)3 ·3 H 2O with dimer-chain structure.Physical Review B105(13), 134417 (2022)

X. Liu,et al., Magnetism and ESR of the𝑆 eff = 1/2 antiferromagnet BaCo 2(SeO3)3 ·3 H 2O with dimer-chain structure.Physical Review B105(13), 134417 (2022)

work page 2022
[16]

Armbruster, M

T. Armbruster, M. E. Gunter, Crystal structures of natural zeolites.Reviews in Mineralogy and Geochemistry45(1), 1–67 (2001)

work page 2001
[17]

Furukawa, K

H. Furukawa, K. E. Cordova, M. O’Keeffe, O. M. Yaghi, The chemistry and applications of metal-organic frameworks.Science341(6149), 1230444 (2013)

work page 2013
[18]

Wildner, Zemannite-type selenites: crystal structures of K 2[Co2(SeO3)3]·2 H 2O and K2[Ni2(SeO3)3]·2 H 2O.Mineralogy and Petrology48(2), 215–225 (1993)

M. Wildner, Zemannite-type selenites: crystal structures of K 2[Co2(SeO3)3]·2 H 2O and K2[Ni2(SeO3)3]·2 H 2O.Mineralogy and Petrology48(2), 215–225 (1993)

work page 1993
[19]

H. S. Effenberger, M. Ende, R. Miletich, New insights into the crystal chemistry of zemannite: Trigonal rather than hexagonal symmetry due to ordering within the host-guest structure. Mineralogy and Petrology117(2), 117–131 (2023)

work page 2023
[20]

M. G. Johnston, W. T. Harrison, New BaM 2(SeO3)3 ·n H 2O (M = Co, Ni, Mn, Mg; n≈3) Zemannite-Type Frameworks: Single-Crystal Structures of BaCo 2(SeO3)3 ·3 H 2O, BaMn2(SeO3)3 ·3 H 2O and BaMg 2(SeO3)3 ·3 H 2O.European Journal of Inorganic Chem- istry2011(19), 2967–2974 (2011)

work page 2011
[21]

S. Y. Istomin, V. Koutcenko, E. Antipov, F. Lindberg, G. Svensson, Synthesis and characteri- zation of novel 6-H perovskites Ba2Co2−𝑥Sb𝑥O6−𝑦, 0.6≤x≤0.8 and x = 1.33 (Ba 3CoSb2O9). Materials Research Bulletin39(7-8), 1013–1022 (2004)

work page 2004
[22]

Miyazaki, X

Y. Miyazaki, X. Huang, T. Kajitani, Compounds and subsolidus phase relations in the CaO– Co3O4–CuO system.Journal of Solid State Chemistry178(10), 2973–2979 (2005). 18

work page 2005
[23]

Wildner, Isotypism of a selenite with a carbonate: structure of the buetschliite-type com- pound K2Co(SeO3)2.Crystal Structure Communications48(3), 410–412 (1992)

M. Wildner, Isotypism of a selenite with a carbonate: structure of the buetschliite-type com- pound K2Co(SeO3)2.Crystal Structure Communications48(3), 410–412 (1992)

work page 1992
[24]

Zhong, S

R. Zhong, S. Guo, G. Xu, Z. Xu, R. J. Cava, Strong quantum fluctuations in a quantum spin liquid candidate with a Co-based triangular lattice.Proceedings of the National Academy of Sciences116(29), 14505–14510 (2019)

work page 2019
[25]

Zhong, S

R. Zhong, S. Guo, R. Cava, Frustrated magnetism in the layered triangular lattice materials K2Co(SeO3)2 and Rb2Co(SeO3)2.Physical Review Materials4(8), 084406 (2020)

work page 2020
[26]

Xu,et al., Frustrated Magnetism in a Potential Quantum Material Based on Spin-1/2 Co 2+ Dimers.Chemistry of Materials36(9), 4157–4163 (2024)

X. Xu,et al., Frustrated Magnetism in a Potential Quantum Material Based on Spin-1/2 Co 2+ Dimers.Chemistry of Materials36(9), 4157–4163 (2024)

work page 2024
[27]

H. S. Nair,et al., Short-range order in the quantum XXZ honeycomb lattice material BaCo2(PO4)2.Physical Review B97(13), 134409 (2018)

work page 2018
[28]

Zhong, T

R. Zhong, T. Gao, N. P. Ong, R. J. Cava, Weak-field induced nonmagnetic state in a Co-based honeycomb.Science Advances6(4), eaay6953 (2020)

work page 2020
[29]

Viciu,et al., Structure and basic magnetic properties of the honeycomb lattice compounds Na2Co2TeO6 and Na3Co2SbO6.Journal of Solid State Chemistry180(3), 1060–1067 (2007)

L. Viciu,et al., Structure and basic magnetic properties of the honeycomb lattice compounds Na2Co2TeO6 and Na3Co2SbO6.Journal of Solid State Chemistry180(3), 1060–1067 (2007)

work page 2007
[30]

Kanamori, Superexchange interaction and symmetry properties of electron orbitals.Journal of Physics and Chemistry of Solids10(2-3), 87–98 (1959)

J. Kanamori, Superexchange interaction and symmetry properties of electron orbitals.Journal of Physics and Chemistry of Solids10(2-3), 87–98 (1959)

work page 1959
[31]

Zhong,et al., Field-induced spin-liquid-like state in a magnetic honeycomb lattice.Physical Review B98(22), 220407 (2018)

R. Zhong,et al., Field-induced spin-liquid-like state in a magnetic honeycomb lattice.Physical Review B98(22), 220407 (2018)

work page 2018
[32]

T. D. Schultz, D. C. Mattis, E. H. Lieb, Two-dimensional Ising model as a soluble problem of many fermions.Reviews of Modern Physics36(3), 856 (1964)

work page 1964
[33]

Bishop, P

R. Bishop, P. Li, C. Campbell, Valence-bond crystalline order in theS= 1/2 J 1–J2 model on the honeycomb lattice.Journal of Physics: Condensed Matter25(30), 306002 (2013)

work page 2013
[34]

Dordevi ´c, BaCo2(AsO4)2.Structure Reports64(9), i58–i59 (2008)

T. Dordevi ´c, BaCo2(AsO4)2.Structure Reports64(9), i58–i59 (2008). 19

work page 2008
[35]

Wildner, Structure of K 2Co2(SeO3)3.Crystal Structure Communications50(3), 336–338 (1994)

M. Wildner, Structure of K 2Co2(SeO3)3.Crystal Structure Communications50(3), 336–338 (1994)

work page 1994
[36]

Cao,et al., DEMAND, a dimensional extreme magnetic neutron diffractometer at the high flux isotope reactor.Crystals9(1), 5 (2018)

H. Cao,et al., DEMAND, a dimensional extreme magnetic neutron diffractometer at the high flux isotope reactor.Crystals9(1), 5 (2018)

work page 2018
[37]

Hao,et al., Machine-learning-assisted automation of single-crystal neutron diffraction

Y. Hao,et al., Machine-learning-assisted automation of single-crystal neutron diffraction. Applied Crystallography56(2), 519–525 (2023)

work page 2023
[38]

J. Rodriguez-Carvajal, FULLPROF: a program for Rietveld refinement and pattern matching analysis, inSatellite meeting on powder diffraction of the XV congress of the IUCr(Toulouse, France), vol. 127 (1990), p. 127

work page 1990
[39]

M. I. Aroyo, A. Kirov, C. Capillas, J. Perez-Mato, H. Wondratschek, Bilbao Crystallographic Server. II. Representations of crystallographic point groups and space groups.Foundations of Crystallography62(2), 115–128 (2006). Acknowledgments Funding:Work at JHU was supported by the Institute for Quantum Matter, an Energy Frontier Research Center funded by th...

work page doi:10.34863/3kpq-r364 2006