Pub Date : 2025-10-10DOI: 10.1007/s11224-025-02631-2
Mikhail I. Smolkov, Ekaterina O. Bukhteeva, Ekaterina D. Barabanova, Alexander F. Krutov, Vladislav A. Blatov
With our previously developed method, we generated triply periodic surfaces (TPSs) including 131 minimal surfaces (TPMSs) using crystal structures of 923 metal-organic frameworks (MOFs) as templates. Our approach is based on the topological representation of a MOF structure as a periodic net with the subsequent construction of the natural tiling for the net and generation of TPSs/TPMSs from the faces of the tiles. The TPMSs were classified into nine topological types, three of which were previously unreported. The surfaces were optimized through smoothing and finite-thickness procedures and deposited in a database together with their topological descriptors. Being designed for practical applications, the surfaces are provided in formats compatible with additive manufacturing and standard software tools. Based on some TPMSs, we fabricated periodic porous samples and experimentally showed that they can possess better mechanical properties than the corresponding bulky material. This work expands the repertoire of known minimal surfaces and bridges the gap between micro- and macrostructures in materials design and fabrication. The relations between atomic crystalline architectures and materials with regular structure including metamaterials support the ideas of generalized crystallography disseminated by Alan Mackay long ago (Struct Chem 13:215–220, 2022).
{"title":"Triply periodic surfaces based on metal-organic frameworks","authors":"Mikhail I. Smolkov, Ekaterina O. Bukhteeva, Ekaterina D. Barabanova, Alexander F. Krutov, Vladislav A. Blatov","doi":"10.1007/s11224-025-02631-2","DOIUrl":"10.1007/s11224-025-02631-2","url":null,"abstract":"<div><p>With our previously developed method, we generated triply periodic surfaces (TPSs) including 131 minimal surfaces (TPMSs) using crystal structures of 923 metal-organic frameworks (MOFs) as templates. Our approach is based on the topological representation of a MOF structure as a periodic net with the subsequent construction of the natural tiling for the net and generation of TPSs/TPMSs from the faces of the tiles. The TPMSs were classified into nine topological types, three of which were previously unreported. The surfaces were optimized through smoothing and finite-thickness procedures and deposited in a database together with their topological descriptors. Being designed for practical applications, the surfaces are provided in formats compatible with additive manufacturing and standard software tools. Based on some TPMSs, we fabricated periodic porous samples and experimentally showed that they can possess better mechanical properties than the corresponding bulky material. This work expands the repertoire of known minimal surfaces and bridges the gap between micro- and macrostructures in materials design and fabrication. The relations between atomic crystalline architectures and materials with regular structure including metamaterials support the ideas of generalized crystallography disseminated by Alan Mackay long ago (Struct Chem 13:215–220, 2022).</p></div>","PeriodicalId":780,"journal":{"name":"Structural Chemistry","volume":"36 6","pages":"1993 - 2006"},"PeriodicalIF":2.2,"publicationDate":"2025-10-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145665986","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-10-08DOI: 10.1007/s11224-025-02632-1
Rémy Mosseri, Jean-François Sadoc
This paper investigates several distinct attempts to generalize in higher dimension the standard 2-dimensional phyllotaxy set construction. We first recall known constructions for these sets on 2D manifolds of constant curvature (the Euclidean plane (mathbb {R}^2), the sphere (mathbb {S}^2) and the hyperbolic plane (mathbb {H}^2)). We then propose a first attempt to get a 3D phyllotactic set by piling up suitably shifted Euclidean 2D phyllotactic sets. A different, radially triggered, solution is then analyzed. An interesting phyllotactic set on the hypersphere (mathbb {S}^3) is then generated using a Hopf fibration approach. Finally, a simple 4-dimensional example is presented, generated as a simple product of two 2-dimensional planar sets. A 3D phyllotaxy candidate is then derived by applying a “Cut and Project” algorithm.
{"title":"Some attempts toward 3-dimensional phyllotaxy","authors":"Rémy Mosseri, Jean-François Sadoc","doi":"10.1007/s11224-025-02632-1","DOIUrl":"10.1007/s11224-025-02632-1","url":null,"abstract":"<div><p>This paper investigates several distinct attempts to generalize in higher dimension the standard 2-dimensional phyllotaxy set construction. We first recall known constructions for these sets on 2<i>D</i> manifolds of constant curvature (the Euclidean plane <span>(mathbb {R}^2)</span>, the sphere <span>(mathbb {S}^2)</span> and the hyperbolic plane <span>(mathbb {H}^2)</span>). We then propose a first attempt to get a 3<i>D</i> phyllotactic set by piling up suitably shifted Euclidean 2<i>D</i> phyllotactic sets. A different, radially triggered, solution is then analyzed. An interesting phyllotactic set on the hypersphere <span>(mathbb {S}^3)</span> is then generated using a Hopf fibration approach. Finally, a simple 4-dimensional example is presented, generated as a simple product of two 2-dimensional planar sets. A 3<i>D</i> phyllotaxy candidate is then derived by applying a “Cut and Project” algorithm.</p></div>","PeriodicalId":780,"journal":{"name":"Structural Chemistry","volume":"36 6","pages":"1963 - 1972"},"PeriodicalIF":2.2,"publicationDate":"2025-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145666011","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-10-01DOI: 10.1007/s11224-025-02629-w
Farag M. A. Altalbawy, Ali Fawzi Al-Hussainy, Suhas Ballal, Mekha Monsi, Chakshu Walia, G. V. Siva Prasad, Masar Almuttairi, Karar R. Al-Shami, Marwa Akram Nafea, Ahmed Mohsin Alsayah
{"title":"Retraction Note: Theoretical investigation of the adsorption performance of Au-functionalized MoTe2 nanosheets for sensing S containing hydroxymethanesulfonate and thiophenol molecules","authors":"Farag M. A. Altalbawy, Ali Fawzi Al-Hussainy, Suhas Ballal, Mekha Monsi, Chakshu Walia, G. V. Siva Prasad, Masar Almuttairi, Karar R. Al-Shami, Marwa Akram Nafea, Ahmed Mohsin Alsayah","doi":"10.1007/s11224-025-02629-w","DOIUrl":"10.1007/s11224-025-02629-w","url":null,"abstract":"","PeriodicalId":780,"journal":{"name":"Structural Chemistry","volume":"36 6","pages":"2379 - 2379"},"PeriodicalIF":2.2,"publicationDate":"2025-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145666035","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-09-27DOI: 10.1007/s11224-025-02628-x
Sapajan Ibragimov, Leonard Komando
<div><p>The electronic structures and redox properties of the [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+/3+}}})</span> and [Co(phen)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+/3+}}})</span> redox couple were investigated using the two different exchange–correlation functional, namely CAM-B3LYP and TPSSh, with the def2-SVP and def2-TZVP basis sets. Our results indicate that [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+}}})</span> and [Co(phen)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+}}})</span> complexes exhibit a high-spin ground state, whereas [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{3+}}})</span> [Co(phen)<span>(_{varvec{3}})</span>]<span>(^{{varvec{3+}}})</span> complexes adopt a low-spin ground state. Both basis sets and exchange–correlation functionals consistently predict the same ground-state spin configurations for these complexes. For <span>([ text {Co(bpy)}_{varvec{3}} ]^{{varvec{2+}}})</span>, the energy gap between the doublet and quartet spin states is relatively small when using the TPSSh functional, amounting to 2.21 kcal/mol with the Def2-SVP basis set and 0.09 kcal/mol with the Def2-TZVP basis set. In contrast, when the CAM-B3LYP functional is employed, the energy splitting becomes significantly larger, with values of 7.91 kcal/mol and 6.12 kcal/mol for the Def2-SVP and Def2-TZVP basis sets, respectively. We also observed similar trends for <span>([ text {Co(phen)}_{varvec{3}} ]^{{varvec{2+}}})</span>. In contrast, <span>([ text {Co(bpy)}_{varvec{3}} ]^{{varvec{3+}}})</span> exhibits a significantly larger energy separation between spin states. Using the CAM-B3LYP functional, the energy difference between the singlet ground state and the quintet excited state is calculated to be 41.42 kcal/mol and 42.07 kcal/mol with the Def2-SVP and Def2-TZVP basis sets, respectively. When the TPSSh functional is employed, this singlet-quintet energy gap becomes slightly larger, further reinforcing the strong preference for the low-spin singlet configuration in the oxidized complex. Additionally, we have observed that adiabatic ionization potentials are less affected by the choice of basis when the CAM-B3LYP functional is used. In contrast, vertical ionization potential exhibits a more pronounced basis set dependence. However, ionization potentials calculated with the TPSSh functional exhibit significantly reduced sensitivity to basis set choice. The calculated oxidation potentials (<span>({varvec{E}}^{varvec{circ }})</span>) using CAM-B3LYP functional for the [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+/3+}}})</span> couple are 5.32 V and 5.26 V employing the def2-SVP and def2-TZVP basis sets, respectively, whereas (<span>({varvec{E}}^{varvec{circ }})</span>) calculated at the TPSSh functional is 4.62 V and 4.55 V. We also have observed that the standard oxidation potential of <span>([ text {Co(phen)}_{varvec{3}} ]^{{varvec{2+/3+}}})</span> is relatively higher than the values of [Co(bpy)<
{"title":"Standard redox potential of [Co(bpy)(_3)](^{2+/3+}) and [Co(phen)(_3)](^{2+/3+}) redox couples using a density functional theory protocol","authors":"Sapajan Ibragimov, Leonard Komando","doi":"10.1007/s11224-025-02628-x","DOIUrl":"10.1007/s11224-025-02628-x","url":null,"abstract":"<div><p>The electronic structures and redox properties of the [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+/3+}}})</span> and [Co(phen)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+/3+}}})</span> redox couple were investigated using the two different exchange–correlation functional, namely CAM-B3LYP and TPSSh, with the def2-SVP and def2-TZVP basis sets. Our results indicate that [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+}}})</span> and [Co(phen)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+}}})</span> complexes exhibit a high-spin ground state, whereas [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{3+}}})</span> [Co(phen)<span>(_{varvec{3}})</span>]<span>(^{{varvec{3+}}})</span> complexes adopt a low-spin ground state. Both basis sets and exchange–correlation functionals consistently predict the same ground-state spin configurations for these complexes. For <span>([ text {Co(bpy)}_{varvec{3}} ]^{{varvec{2+}}})</span>, the energy gap between the doublet and quartet spin states is relatively small when using the TPSSh functional, amounting to 2.21 kcal/mol with the Def2-SVP basis set and 0.09 kcal/mol with the Def2-TZVP basis set. In contrast, when the CAM-B3LYP functional is employed, the energy splitting becomes significantly larger, with values of 7.91 kcal/mol and 6.12 kcal/mol for the Def2-SVP and Def2-TZVP basis sets, respectively. We also observed similar trends for <span>([ text {Co(phen)}_{varvec{3}} ]^{{varvec{2+}}})</span>. In contrast, <span>([ text {Co(bpy)}_{varvec{3}} ]^{{varvec{3+}}})</span> exhibits a significantly larger energy separation between spin states. Using the CAM-B3LYP functional, the energy difference between the singlet ground state and the quintet excited state is calculated to be 41.42 kcal/mol and 42.07 kcal/mol with the Def2-SVP and Def2-TZVP basis sets, respectively. When the TPSSh functional is employed, this singlet-quintet energy gap becomes slightly larger, further reinforcing the strong preference for the low-spin singlet configuration in the oxidized complex. Additionally, we have observed that adiabatic ionization potentials are less affected by the choice of basis when the CAM-B3LYP functional is used. In contrast, vertical ionization potential exhibits a more pronounced basis set dependence. However, ionization potentials calculated with the TPSSh functional exhibit significantly reduced sensitivity to basis set choice. The calculated oxidation potentials (<span>({varvec{E}}^{varvec{circ }})</span>) using CAM-B3LYP functional for the [Co(bpy)<span>(_{varvec{3}})</span>]<span>(^{{varvec{2+/3+}}})</span> couple are 5.32 V and 5.26 V employing the def2-SVP and def2-TZVP basis sets, respectively, whereas (<span>({varvec{E}}^{varvec{circ }})</span>) calculated at the TPSSh functional is 4.62 V and 4.55 V. We also have observed that the standard oxidation potential of <span>([ text {Co(phen)}_{varvec{3}} ]^{{varvec{2+/3+}}})</span> is relatively higher than the values of [Co(bpy)<","PeriodicalId":780,"journal":{"name":"Structural Chemistry","volume":"37 1","pages":"481 - 494"},"PeriodicalIF":2.2,"publicationDate":"2025-09-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s11224-025-02628-x.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146043423","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-09-08DOI: 10.1007/s11224-025-02586-4
Sergey M. Aksenov
Selenites and hydroselenites exhibit a wide structural diversity and are considered as functional materials with a broad spectrum of potential physical properties. The complex crystal chemistry of these compounds is predominantly determined by the peculiarities of chemical bonds between SeO3 triangles and other polyhedra, as well as the stereochemical activity of the lone electron pair, which makes this family similar in structure to sulfates and sulfites, as well as tellurites. The presence of stable modules in the structures of rare-earth selenites allows for the identification of modular series of crystal structures. This fact enables the classification of known structural types as well as the prediction of new ones using the formalism of modular crystal chemistry. This review highlights the breadth of research on the crystal structures of rare-earth selenites and aims to provide new insights for their more detailed analysis.
{"title":"The crystal chemistry and topology of modular structures. I. Selenites of rare-earth elements","authors":"Sergey M. Aksenov","doi":"10.1007/s11224-025-02586-4","DOIUrl":"10.1007/s11224-025-02586-4","url":null,"abstract":"<div><p>Selenites and hydroselenites exhibit a wide structural diversity and are considered as functional materials with a broad spectrum of potential physical properties. The complex crystal chemistry of these compounds is predominantly determined by the peculiarities of chemical bonds between SeO<sub>3</sub> triangles and other polyhedra, as well as the stereochemical activity of the lone electron pair, which makes this family similar in structure to sulfates and sulfites, as well as tellurites. The presence of stable modules in the structures of rare-earth selenites allows for the identification of modular series of crystal structures. This fact enables the classification of known structural types as well as the prediction of new ones using the formalism of modular crystal chemistry. This review highlights the breadth of research on the crystal structures of rare-earth selenites and aims to provide new insights for their more detailed analysis.</p></div>","PeriodicalId":780,"journal":{"name":"Structural Chemistry","volume":"37 1","pages":"47 - 80"},"PeriodicalIF":2.2,"publicationDate":"2025-09-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146043454","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-09-03DOI: 10.1007/s11224-025-02606-3
Ekaterina A. Zheligovskaya
The structural mechanisms of the transitions VI–VII(VIII), IV → VIII, IV → VI, XII → VIII, XII → VI, and XII → Ic are studied. It is shown that the transitions between more dense crystal ices IV, VI, VII(VIII), and XII usually proceed by small shifts of molecules with rearrangement of more than a half of the initial hydrogen bonds. In this case, only finite fragments of the initial phase are retained, which consist of a few molecules. At the same time, as was shown previously, the transitions between less dense crystal ices can proceed by retaining all hydrogen bonds in large (i.e., infinite at least in one dimension) fragments of the initial structure, with a possible change of the bond lengths and angles inside these fragments and rearrangement of hydrogen bonds only between these fragments. In this case, a large fraction (more than a half) of the initial bonds is retained. The difference in the structural mechanisms of transitions between more dense ices or between less dense ices is related to the degree of space filling in the ice structures. The structural mechanisms of the transitions IV → Ic and XII → Ic are very close to those of the transitions IV → VIII and XII → VIII, respectively, because the structures of ices IV and XII are intermediate between those of ices Ic and VII(VIII).
研究了过渡态VI - vii (VIII)、IV→VIII、IV→VI、XII→VIII、XII→VI和XII→Ic的结构机理。结果表明,密度较大的晶体冰IV、VI、VII(VIII)和XII之间的跃迁通常是由分子的小位移和超过一半的初始氢键重排进行的。在这种情况下,只有有限的初始相片段被保留下来,这些片段由几个分子组成。与此同时,如前所述,低密度冰晶之间的转变可以通过保留初始结构的大片段(即至少在一维上无限)中的所有氢键来进行,这些片段内的键长和角度可能会发生变化,并且只有这些片段之间的氢键才会重新排列。在这种情况下,初始键的很大一部分(超过一半)被保留下来。密度较大的冰与密度较小的冰之间过渡结构机制的差异与冰结构中空间填充的程度有关。IV→Ic和XII→Ic的结构机制与IV→VIII和XII→VIII的结构机制非常接近,因为IV和XII的结构介于Ic和VII(VIII)的结构之间。
{"title":"Structural mechanisms of some transitions between Ices IV, XII, VI, VII(VIII) and Ic","authors":"Ekaterina A. Zheligovskaya","doi":"10.1007/s11224-025-02606-3","DOIUrl":"10.1007/s11224-025-02606-3","url":null,"abstract":"<div><p>The structural mechanisms of the transitions VI–VII(VIII), IV → VIII, IV → VI, XII → VIII, XII → VI, and XII → Ic are studied. It is shown that the transitions between more dense crystal ices IV, VI, VII(VIII), and XII usually proceed by small shifts of molecules with rearrangement of more than a half of the initial hydrogen bonds. In this case, only finite fragments of the initial phase are retained, which consist of a few molecules. At the same time, as was shown previously, the transitions between less dense crystal ices can proceed by retaining all hydrogen bonds in large (i.e., infinite at least in one dimension) fragments of the initial structure, with a possible change of the bond lengths and angles inside these fragments and rearrangement of hydrogen bonds only between these fragments. In this case, a large fraction (more than a half) of the initial bonds is retained. The difference in the structural mechanisms of transitions between more dense ices or between less dense ices is related to the degree of space filling in the ice structures. The structural mechanisms of the transitions IV → Ic and XII → Ic are very close to those of the transitions IV → VIII and XII → VIII, respectively, because the structures of ices IV and XII are intermediate between those of ices Ic and VII(VIII).\u0000</p></div>","PeriodicalId":780,"journal":{"name":"Structural Chemistry","volume":"36 6","pages":"2037 - 2048"},"PeriodicalIF":2.2,"publicationDate":"2025-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145665989","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-09-01DOI: 10.1007/s11224-025-02573-9
Abiodun A. Ajibola, Néstor Cubillán, Faith J. Olaitan, Agnieszka Wojciechowska, Lesław Sieroń, Waldemar Maniukiewicz
A novel Cu(II) co-crystal compound, [Cu2(μ-acetate-κ1:κ1-O,O’)4(Isn)2][Cu(acetate-κ1-O)2(Isn)2(H2O)]⋅5H2O (1), (where Isn = isonicotinamide), was synthesized in ethanolic solution at room temperature. The compound was characterized by single-crystal X-ray diffraction, which revealed that it crystallizes in the monoclinic space group P2₁/c. The complex features two centrosymmetric paddle-wheel dicopper(II) moieties, a mononuclear unit, and five hydrogen-bonded water molecules. Both the lattice water molecules and the uncoordinated carboxylate oxygen atoms in the mononuclear moiety form a strong O–H⋯O hydrogen bonding network. Compound 1 represents a cocrystal structure formed by the incorporation of two chemically distinct copper complexes, one mononuclear and one dinuclear, into a single, ordered crystal lattice. Further analysis using FT − IR/FIR/Raman, NIR-Vis-UV spectroscopy, and computational methods, including Quantum Theory of Atoms in Molecules (QTAIM) and Natural Bond Orbital (NBO) theory, was conducted to investigate intra- and intermolecular interactions. Two distinct complexes were identified in the unit cell: the mononuclear copper complex (M) and the dinuclear copper complex (D). Key intra-cell interactions were analyzed by examining two representative pairwise configurations: DD, consisting of two M units, and MD, formed by one M and one D unit. The interaction energies for DD and MD were − 27.3 kcal/mol and − 34.0 kcal/mol, respectively, after correcting for non-basis set superposition error (BSSE). The DD is stabilized by N–H···O hydrogen bonds, while the MD exhibits both π-π and hydrogen bond interactions, promoting enhanced stability and stacking along the b-axis. A frontier orbital gap of 2.6 eV suggests its potential for electronic, photonic, and sensing applications. Biological assays highlighted compound M’s significant antimicrobial activity, outperforming reference compounds like Cu(OAc)₂·H₂O and isonicotinamide against Candida albicans, MRSA, E. coli, and S. typhi. Molecular docking confirmed strong binding to C. albicans, with a binding energy of − 6.89 kcal/mol, whereas compound D showed moderate activity.