Introduction

Ligand-protected metal nanoclusters, especially those based on gold, have attracted considerable attention due to their potential applications in catalysis and photofunctional materials1,2,3,4,5,6,7,8,9,10,11,12. Extensive research on their structural determination and electronic properties has revealed that these nanoclusters are stabilized by forming discrete electron shells that accommodate valence electrons. This behavior can be described by “Jellium model”13. Because their electron configurations resemble Bohr’s atomic model, such nanoclusters are often referred to as “superatom”14.

Most metal nanoclusters possess spherical geometries, and their electronic structures can be well explained by superatom theory. However, there also exist non-spherical, anisotropic metal nanoclusters—often called “cluster of clusters”15—whose stability cannot be accounted for by the simple Jellium model. To explain the stability of these structures, Cheng and Yang proposed the super valence bond (SVB) theory16,17,18. In this theory, the stability arises from the formation of superatomic molecular orbitals (SAMOs), and such clusters are referred to as “superatomic molecules” (Fig. 1). These molecules are formed by the linear combination of superatomic orbitals (SAOs), in a manner analogous to how natural atoms form molecular orbitals through the combination of atomic orbitals.

Fig. 1: Concept of superatomic molecules.
Fig. 1: Concept of superatomic molecules.
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a General scheme for the formation of superatomic molecules by the combination of superatoms. b Energy diagram of the formation of superatomic molecular orbitals by the combination of superatomic orbitals.

Although superatomic molecules exhibit natural atom-like bonding schemes, some of them display unique features that deviate from those observed in natural atomic systems—there are considered characteristic traits of superatomic molecules. This review introduces the concept of superatoms, presents representative examples, highlights recent advances, and discuss future perspective on the development and application of superatomic molecules.

What is superatom?

”Superatom” represents a cluster composed of several atoms that collectively behave like a single atom, particularly due to the stabilization arising from the closure of electronic shells. Early studies using ultraviolet photoelectron spectroscopy (UPS) of gas-phase clusters such as Aun, Agn, and Cun revealed that their electron affinities drop sharply at specific “magic numbers” (e.g., n = 8, 20, 34, and 58)19. According to the jellium model13, the stability of these coinage metal clusters can be explained by the closure of superatomic electron shells. In this model, valence electrons are delocalized and confined in quantized orbitals, so-called “superatomic orbitals” such as 1S, 1 P, 1D, 2S, 1 F, 2 P, 1 G, and so on, analogous to atomic orbitals. The magic numbers (n = 2, 8, 18, 20, 34, 40, 58, etc) correspond to fully filled superatomic shells, contributing to cluster stability.

This superatomic behavior is not limited to gas-phase clusters. Similar shell-closing characteristics are also observed in ligand-protected coinage metal clusters. Since the discovery of thiolate-protected gold nanoclusters1,2, a wide variety of ligand-protected gold nanoclusters have been synthesized, incorporating different numbers of gold atoms and several types of ligands, such as thiolate20,21,22, alkynyl10, amide11, phosphine, N-heterocyclic carbene (NHC)12, etc. In most cases, the gold atoms form a superatomic core. However, in thiolate- and alkynyl-protected clusters, the core is further stabilized by gold–ligand oligomers known as staples.

Several representative gold superatoms have been reported, such as [Au4]2+, [Au11]3+, [Au13]5+23, [Au78]20+, [Au107]26+, [Au114]30+, and [Au147]30+ (Fig. 2)4,24. Their valence electron counts, 2e, 8e, 8e, 58e, 81e, 84e, and 117e, respectively, mostly correspond to the magic numbers identified in gas-phase UPS studies. The electron configurations of these superatoms can be described in terms of SAOs, such as (1S)2, (1S)2(1 P)6, (1S)2(1 P)6, (1S)2….(2 P)6(1 G)18, (1S)2….(2D)10(1H)13, (1S)2….(2D)10(1H)16, and (1S)2….(3 P)6(1 l)5, with most exhibiting closed electronic shells. Owing to their closed-shell nature, [Au4]2+ and [Au11]3+/[Au13]5+ are regarded to helium- and neon-type superatoms, respectively.

Fig. 2: Examples of spherical gold superatoms.
Fig. 2: Examples of spherical gold superatoms.
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a Energy diagram and SAOs of [Au13]5+ superatom. The formula with charge state (the number of valence electrons in parenthesis), and its electron configuration in superatomic orbitals, 1S, 1 P, 1D, etc of b [Au4]2+, c [Au11]3+, d [Au13]5+, e [Au78]20+, f [Au107]26+, g [Au114]30+, and h [Au147]30+. a Reproduced with permission from Royal Society of Chemistry23.

Similar ligand-protected silver superatoms have also been identified, including [Ag13]5+ (8e)25, [Ag32]14+ (18e), [Ag28]8+ (20e)26, [Ag38]18+ (20e), and [Ag103]45+ (58e).4 Recently, a copper-based spherical superatom, [Cu13]5+ (8e), was also reported by Sun27.

All of these superatoms have the potential to act as building block for superatomic molecules by the combination with other superatoms.

Superatomic molecules with natural atom-like bonding

The concept of superatomic molecules was first introduced by Cheng and Yang in 201316,17,18, who proposed the super valence bond (SVB) theory to describe the bonding interactions between superatoms through the formation of superatomic molecular orbitals (SAMOs). Within this theoretical framework, the Au38(SR)24 nanocluster28,29, possessing a [Au23]9+ core, was identified as an F2-type superatomic molecule16. Density functional theory (DFT) calculations demonstrated the formation of SAMOs, designated as Σ, Σ*, Π, and Π*, via the linear combination of constituent SAOs. Fourteen valence electrons are accommodated within these SAMOs in the electron configuration of (Σ)2(Σ*)2px,py)4pz)2(Π*px,py)4, corresponding to a singly bonded structure analogous to that of the diatomic F2 molecule (Fig. 3a)30. The Au38(SR)24 nanoclusters are the pioneering superatomic molecule and the [Au23]9+ core exhibits inherent chirality, thus their catalytic31,32,33,34,35 and chiroptical36,37,38 properties have been extensively studied to date.

Fig. 3: Examples of superatomic molecules with natural atom-like bonding.
Fig. 3: Examples of superatomic molecules with natural atom-like bonding.
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a Superatomic molecular orbitals in the F2-type superatomic molecule with [Au23]9+ core. Singly bonded superatomic molecules: b [Au23]9+, c [Ag23]9+, d [Au8Ag15]9+, e [Au2Ag21]9+, f [Au20]4+. Multiply bonded superatomic molecules: g [Pd2Au21]9+, h [Pt2Au21]9+, i [Au30Ag2]12+, j [Pd2Au17]7+, k [Pt2Au17]7+. Color code, yellow: gold, gray: silver, green: palladium, pink: platinum, red: shared gold/silver atom. a Reproduced with permission from Royal Society of Chemistry16.

This bonding scheme suggests that two Au13 (7e, F-type) superatoms are fused through the sharing of three gold atoms and two electrons, resulting in an F2-type superatomic molecule (Fig. 3b). Analogous structural motifs have also been reported in silver and gold–silver alloy nanoclusters, including [Ag23]9+39, [Au8Ag15]9+, and [Au2Ag21]9+40, all of which have been categorized as F2-type superatomic molecules (Fig. 3c–e).

Furthermore, Cheng and Yang identified Au20(PPhPy2)10Cl4]Cl2 nanocluster bearing a [Au20]6+ core as another F2-type superatomic molecule (Fig. 3f)17. In this case, two Au11 (7e, F-type) superatoms are joined by sharing two gold atoms and two electrons. Similarly, Tsukuda proposed that Au25(SDpp)11, synthesized via thiolation of a polyvinylpyrrolidone-stabilized gold nanocluster, also adopts an F2-type superatomic molecular structure41.

All these F2-type superatomic molecules exhibit single superatomic bonding, with the electron configuration (Σ)2(Σ*)2px,py)4pz)2(Π*px,py)4. The formal bond order of these superatomic molecules can be tuned by electron oxidation and reduction to produce [F2]+ and [F2]42,43. Oxidized analogues such as [Au38(SR)24]2+ and [M2Au36(SR)24] (M = Pd, Pt)44,45, which contain 12 valence electrons, have been postulated to correspond to O2-type superatomic molecules30,46,47. Takano and Tsukuda successfully synthesized [M2Au36(SR)24] (M = Pd, Pt) nanoclusters by a newly developed fusion reaction between hydride-activated [MAu8(PPh3)8]2+ and [M’Au24(SR)18]48,49. Single crystal X-ray diffraction and DFT calculations revealed that the resulting [M2Au21]9+ cores (Fig. 3g, h) adopt an electron configuration of (1A1)2(1B2)2(2A1)2(3A1)2(1B1)2(2B2)2 in C2v symmetry, which differs from the Dh symmetry of the ideal O2 molecule. Although this configuration deviates from that of molecular O2 due to the bent geometry of the two MAu12 superatoms, the formal bond order is higher than that observed in singly bond superatomic molecules.

Shi and Cheng subsequently reported another superatomic molecule exhibiting an even higher bond order50. DFT calculations suggested the presence of a three superatomic center-two electron (3sc-2e) bond within the [Au30Ag2]12+ core of the Au36Ag2(SR)18 nanocluster (Fig. 3i)51. In this system, three Au11Ag2 superatoms are arranged in a cyclic manner, with each pair sharing one gold atom and two electrons to form Σ-type 2sc-2e bonds, while the two silver atoms collectively contribute to a central 3sc-2e bond. This bonding motif is analogous to that found in the [O3]2− ion, leading to the assignment of an [O3]2−-type superatomic molecule.

Although no doubly bonded superatomic molecules have yet been reported, triply bonded superatomic molecules were recently disclosed by Isozaki and Nakamura52. A photoinduced fusion reaction between MAu12(PR3)Cl4 (M = Pd, Pt) clusters led to the formation of N2-type superatomic molecules, M2Au17(PR3)10Cl7 featuring [M2Au17]7+ cores, the first known examples exhibiting superatomic Π-bonding (Fig. 3j, k). Notably, these species display pronounced absorption features attributed to symmetry-allowed electron transition between superatomic molecular Π-orbitals, demonstrating photophysical behavior reminiscent of conventional molecular orbitals.

In addition to the aforementioned synthetic examples, several superatomic molecules featuring natural atom-like bonding have been theoretically predicted. Recently, Cheng demonstrated that sequential or multiple 2sc-2e bonding between metal-doped M@Au12 superatoms can give rise to a variety of superatomic analogues of small molecules, including Cl2, 1O2, 3O2, N2, CO, CO2, CF4, Cl3, O3, N ≡ C–C ≡ N, and Cl–C ≡ C–Cl53,54.

Superatomic molecules with non-natural atom-like bonding

In addition to exhibiting natural atom-like bonding behavior, superatomic molecules can also display non-natural bonding characteristics, in which multiple superatoms are connected through formally non-bonding interactions in the absence of direct electron sharing. Under ambient conditions, noble gas atoms are generally inert and do not form chemical bonds. However, numerous superatomic molecules have been reported that structurally resemble non-bonded dimers, trimers, or oligomers of noble gas-type superatoms, such as [He]∙∙∙[He], or [Ne]∙∙∙[Ne]. For example, in the [Ne]∙∙∙[Ne]-type superatomic molecule based on a [Au25]9+ core, the occupied SAMOs follow the electron configuration (Σpz)2px,py)4(Π*px,py)4(Σ*pz)2 (Fig. 4a)55. Although the formal bond order in such system is regarded as zero (non-bonding), these nanoclusters are stabilized by the surrounding ligands and metal–ligand coordination frameworks.

Fig. 4: Examples of superatomic molecules with non-natural atom-like bonding.
Fig. 4: Examples of superatomic molecules with non-natural atom-like bonding.
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a Schematic image of filled superatomic molecular orbitals in non-bonding [Ne]∙∙∙[Ne]-type superatomic molecules. Non-bonding superatomic molecules: b [Au25]9+, c [Au37]13+, d [Ag49]17+, e [Au18Ag18]12+, f [Au60]20+, g [Au7]3+, h [Au8]4+, i [Au22]6+, j [Au24]8+. Color code, yellow: gold, gray: silver, red: shared gold/silver atom. a Reproduced with permission from Wiley43.

Following pioneering work by Teo, a variety of vertex-shared superatomic molecules have been reported to date (Figs. 3b–d; see in the recent review reported by Negishi56)15,55,56,57,58,59,60,61,62,63. In these systems, a single vertex atom is shared between two M13 superatoms without direct electron sharing. The formation of thiolate-protected gold nanowires has been theoretically proposed through the elongation of vertex-sharing superatomic structures, and their charge-dependent electrical conductivity has been examined61. These “clusters of clusters”57 often form cyclic structures, which may be interpreted as cyclic [Ne]364 or [Ne]565,66 analogues (Fig. 3e, f).

Beyond vertex-shared motifs, additional examples of non-bonding superatomic molecules have been reported. The [Au7]3+ cores in Au20(SR)1667 and Au22(C ≡ CR)1868, for instance, consist of two Au4 (2e) superatoms that share a single gold atom (Fig. 3g). A similar structural motif has also been proposed for Au22(SR)18 based on theoretical calculations69,70.

Another Au4-based non-bonding configuration, [Au8]4+, has been observed in the cores of Au24(ER)18 (E = S, Se) nanoclusters71,72,73,74, in which two Au4 superatoms are arranged without any shared atoms (Fig. 3h). On the basis of various Au4-containing polymorphs, Cheng and Yang proposed the formation of “superatomic networks” constructed of Au4 superatomic units75. According to this model, the [Au14]6+ cores found in [Au24(C ≡ CR)14(PPh3)4]2+76, Au28(SR)2077, and Au28(C ≡ CR)2078 may also be interpreted as assemblies of Au4-based superatoms.

More recently, novel types of non-bonding superatomic molecules have been reported involving bisphosphine and NHC ligands. The [Au22]6+ and [Au24]8+ cores in [Au22H4(dppo)6]2+ and [Au24H3(NHC)14Cl2]3+79,80,81, respectively, can be described as [Ne]∙∙∙[Ne]-type superatomic molecules (Fig. 3i and j), wherein two [Au11]3+ and [Au12]4+ superatoms are combined without formal bonding but are stabilized through the coordination of chelating hydrides.

Although these systems formally possess a bond order of zero, their overall structures are stabilized by ligand coordination and surface protection. Importantly, such non-natural bonding between noble gas-type superatoms results in the emergence of new absorption bands, arising from the formation of superatomic molecular orbitals. This distinctive behavior—absent in natural atoms—is a key feature driving the development of functional materials based on superatomic molecules.

Conclusion and outlook

Superatomic molecules are assemblies of multiple superatoms connected via natural or non-natural atom-like bonding interactions, mediated through the formation of SAMOs. This review outlined the molecular and electronic structures of both superatoms and superatomic molecules. Superatomic molecules exhibiting natural atom-like bonding include representative examples of singly and multiply bonded systems, in which superatoms are connected through the sharing of multiple metal atoms. In contrast, non-natural bonding motifs encompass not only classical vertex-shared poly-icosahedral clusters but also more recently identified species such as He-type ([Au4]-based) and Ne-type ([Au11–13]-based) superatomic molecules. Molecular orbital analyses, supported by computational studies, reveal that these systems can be stabilized by chelating and surface-protecting ligands, even in cases where antibonding SAMOs are fully occupied.

To date, research in this field has primarily focused on synthesis, structural characterization, and electronic structure analysis via DFT calculations, aiming to elucidate the correlation between molecular geometry and electron configuration within the framework of the SVB model. Based on the accumulated insights, the field is now poised to transition from structural understanding to the rational design of functional materials that harness the unique characteristics of superatomic molecules.

The following perspectives are proposed for the future development of superatomic molecular materials:

1) Superatomic molecules with natural atom-like bonding: The bonding nature of superatomic molecules closely resembles that of conventional molecules, suggesting that similar design strategies may be applicable for the development of functional materials. Notably, symmetry-dependent electron transitions between superatomic molecular Π-orbitals have been recently observed52, analogous to transitions in traditional π-conjugated systems. Such π-orbital resonance is a fundamental feature in controlling the functionality of a wide range of photonic and electronic applications, including luminescent materials, catalysts, and electron transport materials. Accordingly, the resonance of superatomic molecular Π-orbitals is considered a key element in the rational design of functional superatomic materials.

One essential feature associated with resonant π-systems is the emergence of aromaticity. In a seminal study, Zhu et al. reported the synthesis of a nanocluster, [Au60Se2(PPh3)10(SePh)15]+, containing a [Au60]20+ core composed of cyclized five icosahedral Au13 superatoms, each sharing one gold atom and two electrons with its neighbors via 2 superatom center-2 electron (2sc-2e) bonds (Figs. 4f and 5a)65. Due to the electronic shell closure within each Au13 unit, the [Au60]20+ core can be regarded as a cyclic [He]5-type superatomic molecule. DFT-based molecular orbital analysis by Lin revealed that the five superatoms are connected via weak interactions, and although these interactions resemble non-bonding, they contribute to the overall stability of the cyclic assembly66.

Fig. 5: Aromatic superatomic molecule.
Fig. 5: Aromatic superatomic molecule.
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a 1S SAO-combined occupied orbitals of the [Au60Se2(PH3)10(SeH)15]+ as a model cluster for the [Au60Se2(PPh3)10(SePh)15]+. b Comparison of the molecular orbitals for the [(Pt@Au11)5Ga2Cl2] cluster and cyclopentadienyl anion. a, b Reproduced with permission from ACS54,69.

Building on this concept, Xu and Cheng proposed the design of an aromatic superatomic molecule, analogous to the cyclopentadienyl anion, by modifying the parent [Au60Se2(PPh3)10(SePh)15]+ nanocluster82. A simplified model, [Au60Se2Cl15]+, was employed in DFT calculations. While the parent cluster, with 40 valence electrons, corresponds to a non-aromatic cyclic [He]5 system, its two-electron reduced form, [Au60Se2Cl15] (42e), as well as a modified version, [(Pt@Au11)5Ga2Cl15] (46e)—in which the central Au atoms of each icosahedral superatoms were replaced with Pt and the central-chelating Se atoms with Ga—were both predicted to exhibit aromatic character based on Hückel’s 4n + 2 rule (Fig. 5b). Furthermore, nucleus-independent chemical shift (NICS) analysis supported the aromaticity of the [Au60Se2Cl15] (42e) nanocluster.

These theoretical insights highlight the remarkable potential of superatomic molecules as candidates for super-aromatic and super-Π-delocalized materials. The ability to rationally tune aromaticity and Π-delocalization at the superatomic level opens a new avenue for the design of advanced materials with tailored optoelectronic properties.

2) Superatomic molecules with non-natural atom-like bonding: Within the framework of the SVB model, numerous examples have emerged in which superatoms with closed-shell electronic configurations are combined, despite exhibiting formally non-bonding characteristics. Although these superatomic assemblies may appear non-bonded in terms of formal bond order, they frequently exhibit new absorption bands that originate from the interaction of SAOs. This unique property of superatomic molecules with non-natural atom-like bonding offers new possibilities for designing photofunctional materials that lie beyond the capabilities of conventional molecules.

A Representative example of such weakly bonded superatomic systems is the class of [Au3]-based clusters. Tsukuda and co-workers reported the formation of a [Au6]4+ core in the Au18S2(SR)12 nanocluster, which can be interpreted as two [Au3]2+ superatoms weakly interacting via 1S SAOs, despite the apparent antibonding character of the interaction (Fig. 6a, e)83. A structurally similar [Au9]5+ core was identified in Au18(SR)1484, which consists of two [Au3]2+ and one [Au3]+ superatoms, also interacting through 1S SAOs (Fig. 6b, f).

Fig. 6: Au3-based weakly-bonding superatomic molecules.
Fig. 6: Au3-based weakly-bonding superatomic molecules.
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a The [Au6]4+ core in Au18S2(STipb)12 composed of weakly-bonding dimer of [Au3]2+. b [Au9]5+ core in Au18(SCy)14 composed of weakly-bonding trimer of [Au3]+/2+ sequences. c [Au20]10+ core in Au42(PET)32 and d [Au32]16+ core in Au60(PET)44 composed of weakly-bonding [Au3]+/2+ sequences. eh DFT-calculated Kohn–Sham orbitals of HOMO(-1) and LUMO of Au18S2(STipb)12, Au18(SCy)14, Au42(PET)32, and Au60(PET)44. e, f Reproduced with permission from Wiley70,71. g, h Reproduced from PNAS72.

More recently, Jin and colleagues reported a series of rod-shaped gold nanoclusters, including Au42(SR)32, Au60(SR)44, Au78(SR)56, Au96(SR)68, and Au112(SR)80, all of which incorporate repeating [Au3] units85,86. The cores of these nanoclusters, [Au20]10+, [Au32]16+, [Au44]22+, [Au56]28+, and [Au68]34+, respectively, can be described as a weakly bonded linear sequence of alternating [Au3]2+ and [Au3]+ superatoms, end-capped with [Au4]2+ units: [Au4]2+∙∙∙2n{[Au3]2+∙∙∙[Au3]+}∙∙∙[Au4]2+ (Fig. 6c, d, g, h). These [Au3]-based rod-shaped superatomic molecules exhibit intense absorption in the near infrared (NIR) region, which has never been observed in other known metal nanoclusters reported to date. Due to the weak yet coherent interactions between 1S SAOs across the superatomic chain, these structures may be interpreted as superatomic Σ-polymers, a bonding motif unique to superatomic systems. The development of such superatom Σ-polymeric architectures opens a new frontier in the design of superatom-based photofunctional materials, with promising applications in optoelectronics and photonics that are inaccessible to traditional molecular frameworks.