[PDF]     https://doi.org/10.3952/physics.2026.66.3.3

Open access article / Atviros prieigos straipsnis
Lith. J. Phys. 66, 154–163 (2026)
 


DANGLING BONDS IN HYDROXYLATED AND AMINATED NANODIAMONDS: APPLICATION OF THE GLOBAL OPTIMIZATION ALGORITHM
Šarūnas Masysa, Valdas Jonauskasa, and Zilvinas Rinkeviciusb
aInstitute of Theoretical Physics and Astronomy, Faculty of Physics, Vilnius University, Saulėtekio 3, 10257 Vilnius, Lithuania
bDepartment of Theoretical Chemistry and Biology, School of Engineering Sciences in Chemistry, Biotechnology and Health, KTH Royal Institute of Technology, SE-10691 Stockholm, Sweden
Email: sarunas.masys@tfai.vu.lt

Received 10 December 2025; revised 29 April 2026; accepted 30 April 2026

The geometric configuration of dangling bonds (DBs) – one of the most abundant paramagnetic defects in nanodiamonds (NDs) – is investigated by applying the global optimization algorithm (GOAT). A total of more than five million geometry optimization runs are carried out to search for the lowest-energy conformers of DBs introduced into hydroxylated and aminated NDs. An analysis of over 3,000 electronic g-tensor calculations performed for the obtained structures shows that only three unique DB types are present in octahedrally shaped C35(OH)36 and C35(NH2)36 nanoparticles, enabling future studies on similar NDs with fully functionalized surfaces to consider a relatively small number of DBs and thereby save computational time and resources. It is also revealed that the arithmetically averaged isotropic g-shifts from the geometries of the standard optimization agree well with the GOAT results, although the behaviour of individual DBs is not properly captured.
Keywords: nanodiamonds, dangling bonds, geometry optimization, electronic g-tensor


NEKOMPENSUOTIEJI RYŠIAI HIDROKSILO IR AMINO GRUPĖMIS FUNKCIONALIZUOTUOSE NANODEIMANTUOSE: GLOBALIOSIOS OPTIMIZACIJOS ALGORITMO TAIKYMAS
  Šarūnas Masysa, Valdas Jonauskasa, Žilvinas Rinkevičiusb
aVilniaus universiteto Fizikos fakulteto Teorinės fizikos ir astronomijos institutas, Vilnius, Lietuva
bKarališkojo technologijos instituto Chemijos, biotechnologijos ir sveikatos inžinerijos mokslų mokyklos Teorinės chemijos ir biologijos departamentas, Stokholmas, Švedija
 
Nanodeimantai (ND) yra deimanto nanodalelės, kurių dydis siekia nuo apytiksliai vieno iki keliolikos dešimčių nanometrų. Jos pasižymi nanomedicinai itin tinkamomis savybėmis: išskirtiniu biosuderinamumu, didele pernašos talpa bei nepaprastai gausia paviršiaus funkcinių grupių įvairove. Tačiau vienas iš ND panaudojimo trūkumų – sudėtinga sekti jų lokalizaciją ir judėjimą in vivo, todėl tai apriboja galimybę stebėti ilgalaikio gydymo eigą. Vis dėlto tiek magnetinio rezonanso, tiek fluorescencijos pagrindo ND vizualizacija yra įmanoma, bet tam būtini paramagnetiniai defektai. Kadangi nekompensuotieji ryšiai (NR) yra vieni iš dažniausiai ND susidarančių paramagnetinių defektų, šiame darbe tiriama jų geometrinė konfigūracija hidroksilo ir amino grupėmis funkcionalizuotuose ND. Atsižvelgus į tokių ND paviršiaus geometrinį sudėtingumą, tyrimams taikytas globaliosios optimizacijos algoritmas, kuris, priešingai nei standartinė geometrijos optimizacijos procedūra, užtikrina visuotinai žemiausios sistemos būsenos paiešką. Optimizuotos NR struktūros buvo panaudotos įvertinant elektroninį g-tenzorių – vieną svarbiausių elektronų paramagnetinio rezonanso parametrų. Gauti rezultatai rodo, kad oktaedrinės formos C35(OH)36 ir C35(NH2)36 nanodalelėse egzistuota tik trys unikalūs NR, o tai suteikia vertingos informacijos ateities ND tyrimams ir leidžia reikšmingai sutaupyti skaičiavimo laiko ir išteklių.


References / Nuorodos

[1] N. Nunn, M. Torelli, G. McGuire, and O. Shenderova, Nanodiamond: A high impact nanomaterial, Curr. Opin. Solid State Mater. Sci. 21, 1 (2017),
https://doi.org/10.1016/j.cossms.2016.06.008
[2] S. Chauhan, N. Jain, and U. Nagaich, Nanodiamonds with powerful ability for drug delivery and biomedical applications: Recent updates on in vivo study and patents, J. Pharm. Anal. 10, 1 (2020),
https://doi.org/10.1016/j.jpha.2019.09.003
[3] C. Fryer, P. Murray, and H. Zhang, Modification of nanodiamonds for fluorescence bioimaging, RSC Adv. 14, 4633 (2024),
https://doi.org/10.1039/D3RA08762J
[4] N. Priyadarshni, R. Singh, and M.K. Mishra, Nanodiamonds: Next generation nano-theranostics for cancer therapy, Cancer Lett. 587, 216710 (2024),
https://doi.org/10.1016/j.canlet.2024.216710
[5] D.E.J. Waddington, M. Sarracanie, H. Zhang, N. Salameh, D.R. Glenn, E. Rej, T. Gaebel, T. Boele, R.L. Walsworth, D.J. Reilly, and M.S. Rosen, Nanodiamond-enhanced MRI via in situ hyperpolarization, Nat. Commun. 8, 15118 (2017),
https://doi.org/10.1038/ncomms15118
[6] D.E.J. Waddington, T. Boele, E. Rej, D.R. McCamey, N.J.C. King, T. Gaebel, and D.J. Reilly, Phase-encoded hyperpolarized nanodiamond for magnetic resonance imaging, Sci. Rep. 9, 5950 (2019),
https://doi.org/10.1038/s41598-019-42373-w
[7] A.I. Shames and A.M. Panich, Chapter 6 – Paramagnetic defects in nanodiamonds, in: Nanodiamonds: Advanced Material Analysis, Properties and Applications, ed. J.C. Arnault (Elsevier, Amsterdam, 2017) pp. 131–154,
https://doi.org/10.1016/B978-0-32-343029-6.00006-4
[8] M. Barzegar Amiri Olia, P.S. Donnelly, L.C.L. Hollenberg, P. Mulvaney, and D.A. Simpson, Advances in the surface functionalization of nanodiamonds for biological applications: A review, ACS Appl. Nano Mater. 4, 9985 (2021),
https://doi.org/10.1021/acsanm.1c02698
[9] Š. Masys, V. Jonauskas, and Z. Rinkevicius, Electronic g-tensors of dangling bonds in hydroxylated and aminated nanodiamonds: A computational study, Phys. Scr. 100, 015402 (2024),
https://doi.org/10.1088/1402-4896/ad9555
[10] V. Barone and P. Cimino, Validation of the B3LYP/N07D and PBE0/N07D computational models for the calculation of electronic g-tensors, J. Chem. Theory Comput. 5, 192 (2009),
https://doi.org/10.1021/ct800279g
[11] A.M. Panich, N.A. Sergeev, and S.D. Goren, Location of paramagnetic defects in detonation nanodiamond from proton spin-lattice relaxation data, Solid State Nucl. Magn. Reson. 105, 101624 (2020),
https://doi.org/10.1016/j.ssnmr.2019.101624
[12] F. Neese, Software update: The ORCA program system–version 6.0, WIREs Comput. Mol. Sci. 15, e70019 (2025),
https://doi.org/10.1002/wcms.70019
[13] B. de Souza, GOAT: A global optimization algorithm for molecules and atomic clusters, Angew. Chem. Int. Ed. 64, e202500393 (2025),
https://doi.org/10.1002/anie.202500393
[14] C. Bannwarth, S. Ehlert, and S. Grimme, GFN2-xTB – An accurate and broadly parametrized self-consistent tight-binding quantum chemical method with multipole electrostatics and density-dependent dispersion contributions, J. Chem. Theory Comput. 15, 1652 (2019),
https://doi.org/10.1021/acs.jctc.8b01176
[15] C. Bannwarth, E. Caldeweyher, S. Ehlert, A. Hansen, P. Pracht, J. Seibert, S. Spicher, and S. Grimme, Extended tight-binding quantum chemistry methods, WIREs Comput. Mol. Sci. 11, e1493 (2021),
https://doi.org/10.1002/wcms.1493
[16] F. Neese, The ORCA program system, WIREs Comput. Mol. Sci. 2, 73 (2012),
https://doi.org/10.1002/wcms.81
[17] F. Neese, F. Wennmohs, U. Becker, and C. Riplinger, The ORCA quantum chemistry program package, J. Chem. Phys. 152, 224108 (2020),
https://doi.org/10.1063/5.0004608
[18] S. Ehlert, M. Stahn, S. Spicher, and S. Grimme, Robust and efficient implicit solvation model for fast semiempirical methods, J. Chem. Theory Comput. 17, 4250 (2021),
https://doi.org/10.1021/acs.jctc.1c00471
[19] Š. Masys, Z. Rinkevicius, and J. Tamulienė, On the magnetic properties of nanodiamonds: Electronic g-tensor calculations, J. Chem. Phys. 151, 044305 (2019),
https://doi.org/10.1063/1.5111024
[20] A.D. Becke, Density-functional thermochemistry. III. The role of exact exchange, J. Chem. Phys. 98, 5648 (1993),
https://doi.org/10.1063/1.464913
[21] P.J. Stephens, F.J. Devlin, C.F. Chabalowski, and M.J. Frisch, Ab initio calculation of vibrational absorption and circular dichroism spectra using density functional force fields, J. Phys. Chem. 98, 11623 (1994),
https://doi.org/10.1021/j100096a001
[22] R. Krishnan, J.S. Binkley, R. Seeger, and J.A. Pople, Self-consistent molecular orbital methods. XX. A basis set for correlated wave functions, J. Chem. Phys. 72, 650 (1980),
https://doi.org/10.1063/1.438955
[23] M.J. Frisch, J.A. Pople, and J.S. Binkley, Self-consistent molecular orbital methods 25. Supplementary functions for Gaussian basis sets, J. Chem. Phys. 80, 3265 (1984),
https://doi.org/10.1063/1.447079
[24] S. Koseki, M.W. Schmidt, and M.S. Gordon, MCSCF/6-31G(d,p) calculations of one-electron spin–orbit coupling constants in diatomic molecules, J. Phys. Chem. 96, 10768 (1992),
https://doi.org/10.1021/j100205a033
[25] S. Koseki, M.S. Gordon, M.W. Schmidt, and N. Matsunaga, Main group effective nuclear charges for spin–orbit calculations, J. Phys. Chem. 99, 12764 (1995),
https://doi.org/10.1021/j100034a013
[26] S. Koseki, M.W. Schmidt, and M.S. Gordon, Effective nuclear charges for the first- through third-row transition metal elements in spin–orbit calculations, J. Phys. Chem. A 102, 10430 (1998),
https://doi.org/10.1021/jp983453n
[27] F. Neese, An improvement of the resolution of the identity approximation for the formation of the Coulomb matrix, J. Comput. Chem. 24, 1740 (2003),
https://doi.org/10.1002/jcc.10318
[28] F. Neese, F. Wennmohs, A. Hansen, and U. Becker, Eflcient, approximate and parallel Hartree–Fock and hybrid DFT calculations. A ‘chain-of-spheres’ algorithm for the Hartree–Fock exchange, Chem. Phys. 356, 98 (2009),
https://doi.org/10.1016/j.chemphys.2008.10.036
[29] F. Weigend, Accurate Coulomb-fitting basis sets for H to Rn, Phys. Chem. Chem. Phys. 28, 1057 (2006),
https://doi.org/10.1039/B515623h
[30] Š. Masys, Z. Rinkevicius, and J. Tamulienė, Electronic g-tensors of nanodiamonds: Dependence on the size, shape, and surface functionalization, J. Chem. Phys. 151, 144305 (2019),
https://doi.org/10.1063/1.5121849
[31] Š. Masys, Z. Rinkevicius, and J. Tamulienė, Computational study on the electronic g-tensors of hydrophilic and hydrophobic nanodiamonds interacting with water, J. Chem. Phys. 152, 144302 (2020),
https://doi.org/10.1063/5.0001485
[32] Š. Masys, V. Jonauskas, and Z. Rinkevicius, Electronic g-tensor calculations for dangling bonds in nanodiamonds, J. Phys. Chem. A 125, 8249 (2021),
https://doi.org/10.1021/acs.jpca.1c06253
[33] Š. Masys, V. Jonauskas, and Z. Rinkevicius, Geometries of defects in nanodiamonds optimized with the low-cost methods: How good are they for the electronic g-tensor calculations?, Diam. Relat. Mater. 136, 110009 (2023),
https://doi.org/10.1016/j.diamond.2023.110009
[34] K. Momma and F. Izumi, VESTA3 for three-dimensional visualization of crystal, volumetric and morphology data, J. Appl. Crystallogr. 44, 1272 (2011),
https://doi.org/10.1107/S0021889811038970
[35] S. Eldemrdash, G. Thalassinos, A. Alzahrani, Q. Sun, E. Walsh, E. Grant, H. Abe, T.L. Greaves, T. Ohshima, P. Cigler, P. Matjíek, D.A. Simpson, A.D. Greentree, G. Bryant, B.C. Gibson, and P. Reineck, Fluorescent HPHT nanodiamonds have disk- and rod-like shapes, Carbon 206, 268 (2023),
https://doi.org/10.1016/j.carbon.2023.02.018