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Hybrid metal nanoparticles, consisting of a nano-crystalline metal core and a protecting shell of organic ligand molecules, have applications in diverse areas such as biolabeling, catalysis, nanomedicine, and solar energy. Despite a rapidly growing database of experimentally determined atom-precise nanoparticle structures and their properties, there has been no successful, systematic way to predict the atomistic structure of the metal-ligand interface. Here, we devise and validate a general method to predict the structure of the metal-ligand interface of ligand-stabilized gold and silver nanoparticles, based on information about local chemical environments of atoms in experimental data. In addition to predicting realistic interface structures, our method is useful for investigations on the steric effects at the metal-ligand interface, as well as for predicting isomers and intermediate structures induced by thermal dynamics or interactions with the environment. Our method is applicable to other hybrid nanomaterials once a suitable set of reference structures is available.

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We present an implementation of distance-based machine learning (ML) methods to create a realistic atomistic interaction potential to be used in Monte Carlo simulations of thermal dynamics of thiolate (SR) protected gold nanoclusters. The ML potential is trained for Au 38 (SR) 24 by using previously published, density functional theory (DFT)-based, molecular dynamics (MD) simulation data on two experimentally characterised structural isomers of the cluster, and validated against independent DFT MD simulations. This method opens a door to efficient probing of the configuration space for further investigations of thermal-dependent electronic and optical properties of Au 38 (SR) 24. Our ML implementation strategy allows for generalisation and accuracy control of distance-based ML models for complex nanostructures having several chemical elements and interactions of varying strength. ligand such as halide or thiolate) ligands. The largest such known cluster was the phosphinehalide protected Au 39 , reported in 1992. 3 Considerable steps forward were taken when Brust and coworkers 4 reported a synthesis that produced all-thiolate protected gold clusters for an average size of two nanometers. Several new chemical compositions of both organo-soluble and water-soluble clusters were reported soon after, 5-8 culminating to the breakthroughs of the first crystal structure of a large Water-soluble all-thiol protected cluster Au 102 (pMBA) 44 (pMBA = para mercapto benzoic acid) by the Kornberg group in 2007 9 as well as the organo-soluble Au 25 (PET)-18 10-12 in 2008 and Au 38 (PET) 24 (PET = phenyl ethyl thiolate) 13,14 clusters in 2008-2010. Up to date, atomic structures of at least 150 different compounds are crystallographically known, which facilitates detailed theoretical computations and dynamical simulations of the properties of MPCs and greatly helps to correlate structures to measured properties in experimental data. Density functional theory (DFT) methods are the cornerstone for all computations that need to deal with details of the electronic structure, such as studies of optical absorption, optical excitation, fluorescence, and magnetism. However, while giving the most accurate and detailed information, DFT methods are also numerically the most demanding. DFT computations of some of the largest structurally known MPCs like the thiolate protected Ag 374 15,16 have to deal with up to 13 000 valence electrons, and even a single-point DFT energy calculation can take minutes and use hundreds or even thousands of CPU cores in a supercomputer. Force fields describing gold-thiolate MPCs have been developed to be used in molecular dynamics (MD) simulations , e.g., in the context of ReaxFF 17 and AMBER-GROMACS. 18 Effective but reliable methods to simulate the atomic dynamics of MPCs are needed, for instance, to study interactions of the clusters with the environment in the solvent phase, or with biomolecules and biological materials (viruses, proteins, lipid layers etc.). 19-21

In-beam γ γ coincidence data have been collected for 186 Pb by combining the JUROGAM Ge-detector array and the GREAT spectrometer with the RITU gas-filled recoil separator for recoil-decay tagging measurements. In addition to the known prolate yrast band in 186 Pb, these data have enabled a new low-lying side band to be identified. Based on the analysis of its decay pattern and comparison with Interacting Boson Model (IBM) calculations, the new band is associated with an oblate shape.

The neutron-deficient nucleus 162 Os, produced in the 106 Cd͑ 58 Ni, 2n͒ reaction, has been studied using the JUROGAM ␥-ray spectrometer in conjunction with the RITU gas-filled separator and the GREAT focal plane spectrometer. ␥-ray transitions in 162 Os have been assigned for the first time through the application of the recoil decay tagging technique. The excitation energy of the 2 + state and the tentative energy of the 8 + state are discussed in terms of the systematic energy trends as the N = 82 shell gap is approached.