Recent advances in in silico design and characterization of superalkali-based materials and their potential applications: A review

In the advancement of novel materials, chemistry plays a vital role in developing the realm where we survive. Superalkalis are a group of clusters/molecules having lower ionization potentials (IPs) than that of the cesium atom (3.89 eV) and thus, show excellent reducing properties. However, the chemical industry and material science both heavily rely on such reducing substances; an in silico approach-based design and characterization of superalkalis have been the focus of ongoing studies in this area along with their potential applications. However, although superalkalis have been substantially sophisticated materials over the past couple of decades, there is still room for enumeration of the recent progress going on in various interesting species using computational experiments. In this review, the recent developments in designing/modeling and characterization (theoretically) of a variety of superalkali-based materials have been summarized along with their potential applications. Theoretically acquired properties of some novel superalkali cations (Li₃⁺) and C₆Li₆ species, etc. for capturing and storing CO₂/N₂ molecules have been unveiled in this report. Additionally, this report unravels the first-order polarizability-based nonlinear optical (NLO) response features of numerous computationally designed novel superalkali-based materials, for instance, fullerene-like mixed-superalkali-doped B₁₂N₁₂ and B₁₂P₁₂ nanoclusters with good UV transparency and mixed-valent superalkali-based CaN₃Ca (a high-sensitivity alkali-earth-based aromatic multi-state NLO molecular switch, and lead-founded halide perovskites designed by incorporating superalkalis, supersalts, and so on) which can indeed be used as a new kind of electronic nanodevice used in designing hi-tech NLO materials. Understanding the mere interactions of alkalides in the gas and liquid phases and the potential to influence how such systems can be extended and applied in the future are also highlighted in this survey. In addition to offering an overview of this research area, it is expected that this review will also provide new insights into the possibility of expanding both the experimental synthesis and the practical use of superalkalis and their related species. Superalkalis present the intriguing possibility of acting as cutting-edge construction blocks of nanomaterials with highly modifiable features that may be utilized for a wide-ranging prospective application.

Introduction

Superalkalis are one distinct class of superatoms that consist of characteristics similar to those of alkali metals but have a substantially lower ionization potential (IP) than them (Wang et al., 1999). As a result, due to their low IPs, superalkalis quickly lose their valence electrons (Gutsev and Boldyrev, 1982; Khanna and Jena, 1995, Khanna and Jena, 2011). Gutsev and Boldyrev were the first to make use of the term “superalkali” in 1982 to refer to the distinct electronic structures of numerous radical forms of lithium and sodium-related species (Gutsev and Boldyrev, 1981). Recent research has proven that superalkalis are the superior supplier of extra electrons for creating novel materials with high initial hyperpolarizabilities than other materials that drop electrons rapidly from their outermost shell (Wang et al., 2012; Sun et al., 2014b, Sun et al., 2014a, Sun et al., 2016a). These species can give one electron to other molecules and survive as cations due to their IPs being lower than those of the alkali metal atoms (5.39–3.89 eV) in the periodic table of all elements (Lias et al., 1988) which means that they are more reactive even though they do not always resemble other elements (Wang et al., 2007). Researchers are constantly executing appropriate research work on the designing and characterization (experimentally or theoretically) of the superalkalis along with their potential applications. Nowadays, scientists have put significant effort into creating and describing diverse comical superalkali-based species.

The standard formula for superalkalis is M_k+1L, where k is 1 for L (F, Cl, Br, and I) and 2 for L (O) atoms; Li_nX (Velickovic et al., 2006; Velickovic et al., 2007; Velickovic et al., 2012) extended to K₂X (X = F, Cl, Br, and I) (Velickovic et al., 2011) and Li₃O (Zintl and Morawietz, 1938; Kudo et al., 1978; Wu et al., 1979) are two instances that come up frequently in this series. Li₂F has been the subject of extensive theoretical (Gutsev and Boldyrev, 1982; Honea et al., 1989, Honea et al., 1993; Rehm et al., 1992; Koput, 2008; Wright et al., 2009) and experimental (Yokoyama et al., 2000; Neskovic et al., 2003; Fernandez-Lima et al., 2009) research. Well-known superalkalis, M₃O (M = Li, Na, and K), have a greater propensity than their equivalent alkali atoms to lose an outer electron (Gutsev and Boldyrev, 1987; Rehm et al., 1992). Comprehensive experiments on the superalkalis having one nonmetal acting as the central atom (B, N, and O) connected by the alkali metal atoms can be seen in the literature, for instance, OM₃ (M = Li, Na, and K) (Wang et al., 2011; Zein and Ortiz, 2011), NLi₄ (Rehm et al., 1992), CLi₅, SiLi_n (n = 1–5), CLi₆ (Schleyer et al., 1983; Otten and Meloni, 2018), and BLi₆ (Li et al., 2007). Next, a comprehensive work based on the in silico approach for binuclear superalkali cations having the formula M₂Li_2k+1 (M = F, O, N, C, and B for k = 1, 2, 3, 4, and 5, correspondingly) was reported by Tong et al. (2009). Furthermore, using the ab initio-based inspections, a series of binuclear superalkali cations M₂Li_2k+1⁺ (F₂Li₃⁺, O₂Li₅⁺, N₂Li₇⁺, and C₂Li₉⁺) was proposed by the same group (Tong et al., 2011). Then, focusing on the expansion from mono to binuclear superalkali cations, attempts have been made by Tong et al. (2012) in describing polynuclear superalkali cations YLi₃⁺ (Y = CO₃, SO₃, SO₄, O₄, and O₅) (Tong et al., 2013). The aforementioned remarkable cations/compounds offer a great deal of potential for use in the production of novel charge-transfer (CT) salts and cluster-assembled nanomaterials with customized characteristics, the reduction of carbon dioxide (CO₂), and activation of very stable nitrogen molecules (N₂), nitrogen oxides (NO), or as hydrogen (energy) storage materials as well as noble-gas trapping agents, ferroelectrics, catalysts, and nonlinear optical (NLO) response, among other things (Zhang et al., 2021b; Zhang et al., 2021a). These molecular species have the capability to reduce substances and can be employed to produce various cutting-edge building blocks of nanoscale materials having highly tunable features, particularly the CT salts. The superalkali cations can produce the CT salts such as a crystal salt Li₃O⁺NO₂⁻ consisting of a single singly charged superalkali cation (Li₃O⁺) (introduced by Zintl and Morawietz, 1938) that alkali elements cannot because of the unfavorable energetics, the metal atom’s relatively high IP, or steric hindrance (Li et al., 2008; Tong et al., 2009). Subsequently, the real nature of sodium nitrate (NaNO₃) was revealed to be sodium oxide nitrite, Na₃O⁺(NO₂)⁻ (Jansen, 1977). They can be utilized to create uncommon CT salts whose counterparts have a low electron affinity (EA). In silico design and characterization of superalkalis based on Zintl ions and the superatom compounds with an NLO response have been reported by some research groups along with Zintl clusters as a new class of superhalogens which can be seen in the literature (Reddy et al., 2018b, Reddy et al., 2018a; Sun et al., 2018; Sinha et al., 2022).

Design, synthesis, and potential applications of new materials consisting of large second-order NLO responses (involving optical data storage, optical computing, telecommunications, optical information processing, etc.) have gained increasing attention (Chemla and Zyss, 1987; Prasad and Williams, 1991; Bredas et al., 1994; Geskin et al., 2003). Several reports on organic molecules consisting of donor–acceptor- (D-A) or donor–π-conjugated bridge-acceptor (D-π-A) skeletons can be seen in the literature which demonstrate considerably large first hyperpolarizabilities and show high photovoltaic performance in developing new non-fullerene small-molecule acceptors (Marder, 2006; Wei et al., 2022). Such frameworks found with larger CT in the systems can establish substantial differences between the dipole moments of the ground state and the excited state as well as low-energy CT transitions (Xu et al., 2007). For example, a sequence of formal D-A chromophores is expected to show a significant NLO response and high stability when M₃O (electron donor) interacts with its counterpart, BC₅₉ (electron acceptor), and creates the CT dyads as M₃O-BC₅₉ (Tu et al., 2014).

Moreover, superalkali cations may interact with superhalogen anions, just like alkali metal cations, and this interaction is predicted to be stronger than the former due to the even lower IPs of the superalkalis. The ability of the superalkali clusters to replicate the chemical behavior of alkali metals makes them potentially useful as building blocks in the construction of innovative nanostructured materials, which is one of their most intriguing discoveries. In some situations, they can combine to form assemblies or super-atom compounds while retaining their identity, much like regular atoms, and thus can demonstrate unique chemical or tunable electronic characteristics. Examples include BF₄-M (M = Li, FLi₂, OLi₃, and NLi₄) (Yang et al., 2012), BLi₆-X (X = F, LiF₂, BeF₃, and BF₄) (Li et al., 2008), Na₂XY (X = SCN, OCN, and CN; Y = MgCl₃, Cl, and NO₂) (Anusiewicz, 2010), and Al₁₃(K₃O) as well as Al₁₃(Na₃O) (Reber et al., 2007). As a result, it makes sense to study the characterization and prediction of the superalkali-based clusters. Recent investigations have attempted to suggest various unique superalkali species (Sun et al., 2016b, Sun et al., 2019; Tkachenko et al., 2019; Ye et al., 2022; Sun et al., 2022), including organic heterocyclic superalkalis [C₃N₂(CH₃)₅ acquired from a familiar aromatic heterocycle, pyrrole] (Reddy and Giri, 2016), organo-Zintl superalkalis (P7R4) (Giri et al., 2016), non-metallic superalkali cations [F₂H₃⁺, O₂H₅⁺, N₂H₇⁺, and C₂H₉⁺] (Hou et al., 2013), and aromatic superalkali species [MLi_n+1⁺ aromatic superatom cations and Au₃ core connected with pyridine (Py) and imidazole (IMD) ligands] (Sun et al., 2013; Parida et al., 2018) (33a, 33b).

As was earlier mentioned, the superalkali clusters are a common type of super-atoms that can function as alkali metal atoms, so they can construct an extended nanostructure when put together (Reber et al., 2007; Reber and Khanna, 2017). Additionally, it has been suggested that superalkali cations could act as hydrogen storage materials (Barbatti et al., 2002; Giri et al., 2011; Pan et al., 2012) and noble gas-trapping agents (Chakraborty et al., 2010; Pan et al., 2013a; Pan et al., 2013b). For instance, Giri et al. (2011) investigated the potential of the cationic superalkalis Li₃⁺ and Na₃⁺ for H₂-binding. Additionally, it has been noted that the superalkali cation O₂Li₅⁺ can bind up to seven noble gas (Ng) atoms (Ng = He, Ne, Ar, and Kr) (Pan et al., 2013a) and up to 12 Xe atoms (Pan et al., 2013b).

The trinuclear Au₃(IMD)₃ [IMD = imidazole] combination turns aromatic, according to a recent work on the construction of a novel family of organometallic superalkali compounds (Gutsev and Boldyrev, 1982; Gutsev and Boldyrev, 1985; Parida et al., 2018; Tkachenko et al., 2019). Examining large systems such as fullerenes, the prediction of superalkali@C60 endofullerenes, their enhanced stability, and interesting properties have been reported comprehensively by Misra et al. in 2016 along with an understanding of the nanoconfinement effect on halogen bonding in (CH₃Br···NH₃)@C₆₀ (Srivastava et al., 2016b; Srivastava et al., 2016a).

Even though superalkalis have advanced significantly over the past several decades, an overview of the recent advances in a variety of remarkable species appears to be missing in the literature (Sun and Wu, 2019; Pal et al., 2021). The most advanced developments in recent years, design/modeling, characterization in the framework of in silico approaches, and first-time use of superalkali-based novel materials are outlined in this review along with their potential applications. We attempted to share the predictions for their future growth in the hopes of pointing designers in the right direction as they continue to create and use such special species. We believe that this report can open new directions in the organized interpretation of the superalkali-based materials.

Results and discussion

In this section, the authors have attempted to provide snippets on the structure, stability, and electronic features of various superalkali-based species such as NM₄ (M = Li, Na, and K) superalkalis; ab initio exploration of the polynuclear K- and Na-based superalkali hydroxides as superbases; theoretical studies on the hydration effect on the superalkali cations, Li₃⁺; and the role of the size and composition on the design of superalkalis. Moreover, in terms of the applications of a range of superalkali-based materials (i.e., high-performance NLO material/molecular switch), design and characterization (theoretically) of a novel series of D-A frameworks through superalkali–superhalogen assemblage, superalkalis doped with B₁₂N₁₂ nanocages, boron phosphide nanocages doped with superalkalis as novel electrides, and innovative inorganic aromatic mixed-valent superalkali electride, CaN₃Ca, have been highlighted in this report. This report unravels a brief overview of the capturing of nitrogen by unveiling the potential of superalkali cation Li₃⁺ and the reduction/activation of carbon dioxide with a superalkali. A short description of the modeling of aromatic organometallic superalkali complexes and superalkali ligands as the building blocks for aromatic trinuclear Cu(I)-NHC complexes, the nature of the aluminum trimer combined with different superatom clusters, superalkali–alkalide interactions, ion pairing in low-polarity solvents, and lead-based halide perovskites associated with superalkali species have been reported.

Structural and electronic features of superalkali-based species

Superalkalis are known as super-atoms which can imitate the chemistry of atoms and can be used in the synthesis of novel materials with diverse interesting features. Using high theoretical-level Gaussian 3 (G3) calculations, Zhang and Chen proposed models of a small series of superalkali NM₄ (where M = Li, Na, and K) (see Figure 1A) clusters consisting of homo- and hetero-alkalis, and studied their stability and electronic structures (Zhang and Chen, 2019). The calculated vertical IPs (3.22–3.74 eV) have been found to be smaller than that of the Cs atom having an IP value of 3.89 eV, and binding energies (BEs) and positive energies of the dissociation channel such as (NM₃ + M’) confirmed the stabilities (thermodynamically) of all probed species where NLi₄ was found to be the most stable among all the homo- and hetero-superalkalis. The order of the calculated BEs for the NM₄ clusters was found to be NLi₄ (−9.25 eV) > NNa₄ (−5.88 eV) > NK₄ (−1.92 eV), separately, where the size of the alkaline atoms has a substantial impact on the overall stability of the clusters when such atoms are combined, followed by ionic bond formation. Encouraged by the reports highlighted in this study, novel materials can be constructed by the previously designed and characterized (theoretically) species having high stability along with tetrahedral geometry. It is important to note that the structures of the NM₄ species with homogeneous alkali atoms (like NLi₄, NNa₄, and NK₄) have Jahn–Teller distortion-resistant T_d symmetry, while the clusters constructed from the heterogeneous alkali atoms have C_3v symmetry. Furthermore, the Frontier molecular orbital (FMO) approach appeared to show that the highest occupied molecular orbitals (HOMOs) of all such species are mainly spread over the complete clusters shown to diminish the repulsion among the electrons repelling each other. Their ab initio modeling approaches (MP2/MP4) described the highly symmetric structural parameters and the low IP values of the NM₄ clusters from the electronic origin point of view.

FIGURE 1

FIGURE 1. (A) Geometric structures of NM₄ (M = Li, Na, and K) clusters reproduced from Zhang and Chen (2019); (B) charge density difference in (A) Li₃B₆H₆, (B) Li₃B₆F₆, and (C) Li₃B₆(CN)₆ clusters reproduced from Banjade et al. (2021). (C) Charge density difference in (A) Li₃B₁₂H₁₂, (B) Li₃B₁₂F₁₂, and (C) Li₃B₁₂(CN)₁₂ clusters (Banjade et al., 2021); (D) superalkali cation Li₃⁺ with water molecules, Li₃⁺(H₂O)_n (n = 1–5), reproduced from Hou et al. (2018) with permission from the Royal Society of Chemistry; (E) a small series of hydroxides (XM_n+1OH) where (XM_n+1): superalkali; M (K and Na): alkali metal atom; n, maximal formal valence of the central atom X (F, O, and N), and n ≥ 1.

It is to be noted that although significant signs of progress have been made in designing, synthesis, and characterization of superhalogens, there is still room for related studies on superalkalis. With the combination of superalkalis having low IPs and superhalogens having high EA, super-ions may be used as construction blocks of a novel series of supersalts having uses in multiferroic materials, metal-ion batteries, solar cells, and so on. Jena et al. thoroughly described the role of size and composition in the design of supersalts consisting of two dissimilar classes of clusters belonging to the closo-borane family, Li_mB_nX_n (m = 1–3; n = 6, 12; X = H, F, and CN) and Zintl ion family, Li_mBe@Ge₉, in the framework of the density functional theory (DFT) with hybrid exchange-correlation functional (ωB97xd) as well as Gaussian basis sets [6-311+G (d, p)] (Banjade et al., 2021). In this work, the stabilities of such a composition of clusters were regulated by the Wade–Mingos polyhedral skeleton electron pair theory (i.e., shell closure rule), and additionally, the jellium shell closure rule was deployed to understand the stability of the Be@Ge₉ cluster. The analyzed IP values were well-connected to the EAs of the X ligands (the higher the EA, the larger the IP). They found that like the lowest IP value (2.84 eV) for Li₃B₆H₆ among Li₃B_nX_n clusters, both the closo-borane family and Zintl ion-related clusters followed the same IP patterns; however, conversely and beyond the hope, the IP values were not reduced (n = 6–12) with enhancing the cluster volume followed by being weakly bounded. It should be noted that EAs of the B_nX_n enhanced proceeding from n = 6 to n = 12, since the association of the Li atoms with the B₁₂X₁₂ cluster is stronger than that with the B₆X₆ cluster. Likewise, as the substitution of the X travels from the H atom to the F atom to the CN group in the Li₃B₁₂X₁₂ clusters (X = H, F, and CN), the IP values are enhanced. The charge density difference (CDD) plots were visualized for all six species (three closo-borane and three Zyntl ion families). For example, in the case of Li₃B₆H₆, the CDD showed that the electrons have been amassed in the area sandwiched between the three successive Li–B bonds and uniform diffusion of the electron near the Li–B bonding region (see Figure 1B), whereas a much larger charge accumulation between the Li and F atoms can be seen for the Li₃B₆F₆ cluster. These findings were consistent with the structural features. Furthermore, electron accumulation along the Li–C bonds for the Li₃B₁₂X₁₂ clusters demonstrated that the Li atoms were bonded to mostly the X atoms (see Figure 1C) which agreed with their geometries. Very importantly, however, there was an increment in the cluster volume and the F atom, as well as the CN group consisting of more electronegativity than the H atom, and stronger interactions between the cluster and the Li atoms have been observed. The IPs of the Zintl-ion family clusters were found to be higher than those in the closo-borane-family clusters since these behave like superalkalis. Very interestingly, it is noteworthy to mention that despite having the same electron count in both the Li₅Ge₉ and Li₃Be@Ge₉ clusters, the IP of the former is found to be smaller than that of the latter, implying that, indeed, composition matters therein.

Using the ab initio modeling approach, Li et al. reported an extensive study on the influence of hydration on the structure, stability (through energy decomposition analyses), and electronic features of the superalkali cation Li₃⁺ in the framework of the MP2/6-311++(d, p) level of theory (Hou et al., 2018). Assuming all possible arrangements of H₂O molecules around the Li₃⁺ cation, a series of Li₃⁺(H₂O)_n (n = 1–5) structures (see Figure 1D) have been obtained where the Li₃⁺ cation is observed to have a maximum of four coordination numbers. Interacting with five molecules of water, the CT of the Li₃⁺ cation appeared to be critically irregular which was shown by natural population analysis (NPA), and as a result, the Li₃⁺ cation lacks the ring conjugation and comes apart into the isomer of Li₃⁺(H₂O)₅ having the lowest energy. Using the NPA tool, water ligands appeared to have a dominant role in the charge distribution of Li₃⁺ along with the CT from the H₂O ligand to the Li₃⁺ skeleton. With the deployment of the polarization continuum model (PCM) tool in calculating the Gibbs free energies (∆G_r²⁹⁸) at 298.15 K, the lowest-energy isomers of Li₃⁺(H₂O)_n (n = 1–5) are not appropriate for detaching spontaneously. It is important to mention that a coordination number of 12 has been vaticinated for the Li₃⁺ cation associated with hydrogen clusters. The outcomes of the in silico approach revealed that structural and electronic integrity was maintained by the Li₃⁺ cation followed by low-lying isomers of the Li₃⁺(H₂O)_1–4 complexes, while in the lowest-energy structure of Li₃⁺(H₂O)₅, it destroyed and left its superalkali individuality. Based on such findings, like Li⁺ in water clusters, the superalkali Li₃⁺ cation contributes to the same maximum coordination number. Like the case of the lithium-ion hydrates, the localized molecular orbital energy decomposition approach showed that the electrostatic interactions play a prime role in the binding of the water molecules with the Li₃⁺ cation. A sharp increase in the contribution of the exchange-repulsion energy can be seen when the number of water ligands arrives at five and even this exchange-repulsion energy surpasses that of the electrostatic term.

Very recently, computational designing and characterization of Na- and K-based superalkali hydroxides acting as superbases have been reported by S. K. Pandey for the first time (Pandey, 2021b). A new kind of hydroxide of the superalkalis (XM_n+1OH) [where the fragment XM_n+1 refers to the superalkali moieties, X (F, O, and N), and n ≥ 1] has been modeled, and inclusive computational experiments on such fascinating species have been performed using the framework of the ab initio method (see Figure 1E). To inspect the relative basic nature of such polynuclear superalkali hydroxides (SAHs) against the representative alkali metal hydroxide (KOH, NaOH, and LiOH) along with the Li-related SAHs, the ab initio findings demonstrated that both the Na- and K-based SAHs are stronger bases than the LiOH and Li-related SAHs which is due to the larger gas-phase proton affinity (PA) and gas-phase basicity (GB) values of the Na- and K-related SAHs. Noticeably, the highest PA (1168.4 kJ/mol) and GB (1146.9 kJ/mol) of the OK₃OH base revealed its strongest basicity nature among all the existing strong bases and superbases along with the proposed K- and Na-based SAHs. The values adequately surpassed the ΔPA (142.1 kJ/mol) and ΔGB (146.9 kJ/mol) values of the threshold values (PA: 1026.3 kJ/mol and GB: 1000 kJ/mol) of a very popular IUPAC-defined superbase (DMAN).

To probe the structure, stability (bonding features), and electronic properties of the SAHs, the popular noncovalent interaction (NCI)-plot and quantum theory of atoms in molecules (QTAIM) tools were used for a variety of chemical to biochemical species to materials along with exploration of the computational studies on the HAP biomaterials including the first-principle DFT, ab initio modeling, and molecular dynamics simulations (Awasthi et al., 2021a; Awasthi et al., 2021b; Pandey, 2021a; Pandey and Arunan, 2021). In this report, new insights into the basicity features were facilitated by an ab initio modeling approach. Design, fabrication, and synthesis of the theoretically explored SAHs may lead to providing an alternative pathway for the experimentally availing applications.

High-performance NLO response material/molecular switch

Very recently, Bano et al. presented theoretical work where they showed that the mixed superalkalis (Li₂NaO, Li₂KO, Na₂LiO, Na₂KO, K₂LiO, K₂NaO, and LiNaKO) could be a better alternative than the pure superalkalis for B₁₂N₁₂ nanocages in designing hi-tech NLO materials (Bano et al., 2022). The optimized structures of the mixed-superalkali-doped B₁₂N₁₂ complexes can be seen in Figure 2A. Throughout the computational experiments, the structure, stability, electronic, and NLO response features of superalkali cluster-mixed B₁₂N₁₂ nanocages were examined. They have chosen a total of seven (A–G) thermodynamically stable designed complexes consisting of very high interaction energies ranging from −98.02 kcal/mol to −123.13 kcal/mol, which were compared with the previously reported Li₃O@B₁₂N₁₂ having an interaction energy (E_int) as −92.71 kcal/mol along with the narrow variation of the HOMO-LUMO energy gaps (from 3.36 eV to 4.27 eV) compared against the pristine B₁₂N₁₂ (11.13 eV) species. This group confirmed the CT phenomenon occurring in such probed complexes which were acquired from the NPA technique, non-bonding interactions between the doped superalkalis and nanocages followed by the QTAIM, as well as NCI-plot tools. The maximum absorbance was found in the near-infrared (IR) region ranging from 1,076–1,486 nm which appeared to be transparent in the ultraviolet (UV) region. The computed first hyperpolarizability (β_tot) of complex C was analyzed as 1.7 × 10⁴ au which was much greater than that of the pure Li₃O superalkali-doped B₁₂N₁₂ complex (3.7 × 10⁴ au) perceived from the same theoretical level of approach (by Sun et al. in 2016). As in nanoelectronics, designing and synthesizing stable and high-performance NLO materials is the foremost precedence for the scientists and researchers; an increased NLO response was detected in this work by a large second hyperpolarizability. To gain more insights into such complexes, they also computed hyper-Rayleigh scattering (6.71 × 10¹⁰ au), second harmonic generation (1.17 × 10¹⁰ au), and electro-optical Pockels (3.29 × 10¹⁰ au) effect along with the maximum obtained values of the electric field-induced second harmonic generation (3.46 × 10¹⁰ au) and electro-optic-dc-Kerr effect (3.96 × 10¹¹ au) at 1,064 nm wavelength. At the same wavelength for all A-G complexes, significant increments in quadratic nonlinear refractive index (n₂) values were seen along with the largest value of 3.35 × 10^–8 cm²·W⁻¹. The theoretical findings based on the ωB97XD/6-31G (d, p) level of approach indicated that such mixed superalkali-doped nanoclusters could have broad applications in designing, fabrication, and characterization of hi-tech optoelectronics (i.e., high-performance NLO materials).

FIGURE 2

FIGURE 2. (A) Optimized geometries of the most stable complexes of mixed-superalkali-doped B₁₂N₁₂ adapted from Bano et al. (2022) with permission from the Royal Society of Chemistry; (B) optimized structures of C₆Li₆-nCO₂ complexes (front and side views) for n = 1–6 adopted from Srivastava (2019b) with the permission of Wiley.

However, various procedures can be seen in the literature in designing high-performance NLO materials; the NLO response of three series (a total of 10 isomers, I–X) of theoretically designed compounds Li₂F@B₁₂P₁₂, Li₃O@B₁₂P₁₂, and Li₄N@B₁₂P₁₂ having three (I–III), four (IV–VII), and three (VIII–X) isomers, correspondingly, was inspected thoroughly using the DFT approach (see Figure 2B) (Ullah et al., 2019). This research work explored the effects of superalkali (Li₂F, Li₃O, and Li₄N) when these were doped on the B₁₂P₁₂ nanocage. The computational outcomes showed that most of the complexes [all isomers of the Li₂F@B₁₂P₁₂ and Li₃O@B₁₂P₁₂ model compounds (I–III and IV–VII) along with one isomer of the Li₄N@B₁₂P₁₂ complex (IX)] possessed excess electrons, whereas only two isomers of the Li₄N@B₁₂P₁₂ (VIII and X) compound were found to be inorganic electrides. It was computationally inspected that the superalkalis were chemisorbed on the boron phosphide nanocage and all such formed nanocage complexes were found to be quite stable which was confirmed by their calculated BEs. There was substantial enrichment in the first hyperpolarizability values of the system when doping a B₁₂P₁₂ nanocage with the superalkali. Isomer III of the Li₂F@B₁₂P₁₂ system showed the largest first hyperpolarizability (3.48 ×10⁵ au) and lowest the HOMO-LUMO gap (1.46 eV) among the three isomers (I–III) along with good transparency in the UV region, showing that the superalkali Li₂F provided better hyperpolarizability increment than the Li₃O and Li₄N superalkalis when associated with the B₁₂P₁₂ nanocage. In addition, the influences of several superalkalis and various doping locations on the NLO response were comprehensively examined for all three variants of model systems in the framework of the quantum chemical calculations using the DFT approach. This work will promote prospective uses of the C₆₀-like B₁₂P₁₂-based nanostructures doped with the superalkali and novel electronic nanodevices, and hi-tech NLO materials consisting of good UV transparency could be designed by the employment of new excess electron systems and electrides (VIII and X).

As several research groups have focused on designing novel superatoms with high NLO responses, A. Omidvar reported a range of representative D-A model skeleton species having elevated NLO responses through bonding the superalkali-like M₃O (K₃O, Na₃O, Li₃O, Li₂KO, Li₂NaO, Na₂KO, Na₂LiO, K₂LiO, K₂NaO, and LiNaKO) blended with the superhalogens (Al₁₃ cluster) (see Figure 3A) (Omidvar, 2018). These superalkalis consist of a low IP to the superhalogen Al₁₃ having a larger EA. Additionally, the electric field gradient tensors of the ¹⁷O nuclei and the natural bond orbital (NBO) analysis-based charges of the M₃O superalkalis were also computed. In this study, he represented the theoretical signatures for the feasibility of employing the super-atoms Al₁₃ and M₃O as construction blocks to construct nanomaterials with strong NLO responses. He observed that the IP and ¹⁷O nuclear quadrupole resonance parameters of the M₃O superalkalis have been efficiently affected by the M ligands. The electron transfer phenomenon in such types of super-atoms in the bonding superalkalis is responsible for the competent narrow HOMO-LUMO gap as well as increasing the first hyperpolarizability remarkably in the pristine Al₁₃ cluster. Significant CT takes place from the M₃O component to the Al₁₃ assembly. It was observed that the data based on the η_Q parameters of the ¹⁷O nuclei significantly increase when the pure ligands were substituted with the doped ligands in the M₃O superalkali species. The Q value (an asymmetry parameter) provides evidence of the chemical bonds taking part therein. Importantly, according to the findings of this investigation, the electropositivity of the alkali ligands was shown to play an important role in the determination of the IPs of the superalkalis. Moreover, a comprehensive exploration of the NLO response of the super-atoms M₃O-Al₁₃ can be seen that is altered by the oriented external electric fields. When the imposed oriented external electric field is enhanced along the CT direction (M₃O → Al₁₃) ranging from zero to a critical external electric field, a gradual increment in the first hyperpolarizability can be seen for the superatom compounds which appears to be used as an effective approach based on the theoretical findings.

FIGURE 3

FIGURE 3. (A) Structures of superalkalis, M₃O (where M = Li, Na, and K) associated with the Al₁₃ nanocluster reproduced with permission from Omidvar (2018); (B) different configurations (1, 2, and 3) of the CaN₃Ca molecule adopted from Wang et al. (2020) with permission from the Royal Society of Chemistry.

Using quantum mechanical approaches, a total of three configurations [two C_3v point groups (1 and 3) and one D_3h point group (2)] of trigonal bipyramidal (TBP) CaN₃Ca structures were chosen as models, and the role of the NLO response was analyzed by aiming at pioneering hi-tech single-pole double-throw (SPDT) NLO molecular switches (Wang et al., 2020). One marginally longer and one shorter vertical Ca-N₃³⁻ length was found in the case of both C_3v configurations (1 and 3), whereas there were two identical bond lengths of Ca-N₃³⁻ in configuration 2. The ab initio (MP2/6-311+G (3df) method-based equilibrium structures of the chosen CaN₃Ca species can be seen in Figure 3B where the Ca atoms are located over and under the usual triangular N₃ ring. It should be noted that energy configurations 1 and 3 are 3.99 kcal/mol smaller than that of configuration 2 at the CCSD(T)/6-311+G (3df) level of theory which illustrates that the former two configurations (1 and 3) have a larger thermal stability than configuration 2. Moreover, in the case of the configuration 2, the excess electrons equally occupied the two hemispherical orbital lobes (HOMOs) positioned over the two extremes of the CaN₃Ca molecule, while in the case of the other two configurations (1 and 3), the excess electrons mainly occupied one hemispherical orbital lobe (HOMO) (located on the left side for 1 and right side for 2) of the CaN₃Ca species. Importantly, Figure 3B also confirms that a uniform external electric field (EEF) triggered a reversible configuration conversion between 1 (L1 > L2) and 3 (L1 < L2). Hence, by deploying an appropriate external homogeneous electric field, interconversion between 1, 2, and 3 can be realized easily. All these species belonged to the novel alkaline-earth-based aromatic mixed-valent superalkalis along with acting as fascinating electrides. Very importantly, the electronic structure of the salt-like species containing configuration 2 showed a delocalized structure in the form of e^0.5−···Ca²⁺N₃³⁻Ca²⁺···e^0.5− demonstrating class III-type mixed-valent superalkali electrides, whereas the other two configurations 1 and 3 were confirmed as the rare inorganic Robin–Day class II-type structure consisting of localized redox centers. Moreover, comparison outcomes of remarkable static and dynamic first hyperpolarizabilities of all three configurations have been reported since all three were excellent candidates for SPDT NLO molecular switches.

Finally, using the ab initio modeling approach, Zhang et al. showed that the phenalenyl radical and M₃ ring (M₃–PHY, M = Li, Na, and K) stacked with parallel and vertical geometries are potential applicants for molecular switches which can exist in both superalkali electrides and superalkalides (Yi et al., 2022). A range of similar kinds of interesting research studies can be seen in the aforementioned literature. In this work, they have shown that M^δ−-M₂^(1−δ)+-PHY^- acts as a superalkalide, whereas the e⁻⋅⋅⋅M₃⁺-PHY acts as a superalkali electride where the former may isomerize to the latter using suitable long-wavelength irradiation and the latter may isomerize to the former with appropriate short-wavelength irradiation. In this report, the researchers have combined both electride and alkalide characteristics in one molecular switch and concluded that both forms demonstrated an excellent functioning NLO response.

Capturing carbon dioxide/nitrogen/hydrogen

Reduction (via electron transfer i.e. CT phenomenon) of carbon dioxide (CO₂) by the capability of the superalkali Li₃F₂ has been shown by Park and Meloni (2017). The equilibrium structure of neutral planar and non-planar clusters trapping the CO₂ and N₂ molecules can be seen in Figure 4A. To attain trustworthy outcomes on the structural and energetics/stability of the species, a composite CBS-QB3 model was deployed. The association of CO₂ with the Li₃F₂ superalkali was examined by scanning the potential energy surface (PES) which led to the formation of their transition states (TSs) and minima. Structural alterations were exposed in the terms of spin density and charge flow. The large BE (ionic interactions between the Li₃F₂ and CO₂ having the largest BE (163 kJ/mol) among the three optimized structural isomers), CT phenomenon, and the HOMO-LUMO gap explained the energetics and stability of the Li₃F₂/CO₂-associated species. It is worth mentioning that the largest determined BE (163 kJ/mol) was found to be significantly larger than that of the superhalogen cluster Sb₃F₁₆/CO₂ reported by Czapla and Skurski (2017). The choice of the Li₃F₂ toward the CO₂ has been taken using the same level of approach by which computational experiments on the association of the most copious atmospheric N₂ gaseous molecule have been conducted (a very small chemical affinity of the Li₃F₂ for N₂). In the case of the N₂ association with the superalkali Li₃F₂, the calculated BE value was only 51 kJ/mol, which reveals that the capability of the superalkali Li₃F₂ for CO₂ reduction has high selectivity over the N₂ molecule. CO₂ is actively reduced by the superalkali Li₃F₂ followed by transferring an electron as well as geometric change which brings up the CO₂ molecule in a bent shape, and it can be probably used in transforming CO₂ into fuel.

FIGURE 4

FIGURE 4. (A) Optimized geometries of neutral planar clusters (top) and neutral non-planar clusters (bottom) adapted from Park and Meloni (2017) with permission from the Royal Society of Chemistry; (B) (a) optimized structure of the Li₃⁺(N₂)₁₂ complex and (b) its HOMO 3D isosurface map adapted from Yu et al. (2020) with permission from the Royal Society of Chemistry; (C) optimized structures of C₆Li₆–nCO₂ complexes (front and side views) for n = 1–6 adopted from Srivastava (2019b) with the permission of Wiley.

With the deployment of the MP2/6-311+G(d) level of approach, an investigation was conducted by Yu et al. (2020) to obtain new insights into the capability of the superalkali cation Li₃⁺ for capturing N₂ gas as well as its behavior in gaseous nitrogen. To reduce inter-ligand Coulombic repulsion, the N₂ molecules (i.e., a maximum coordination number of 12 was envisaged for the trinuclear Li₃⁺ because every vertex Li can capture four N₂ molecules) approached to attach at various apexes of the trinuclear Li₃⁺ core of the Li₃⁺(N₂)_n (n = 1–7) complexes which were confirmed by the structure, stability, and electronic feature analyses. It is worth to mention that only in the case of the lowest-lying series of the Li₃⁺(N₂)_n complexes (where the number “n” ranges from 1 to 4) complexes, the trinuclear Li₃⁺ core retains its superatom dignity using the NPA and FMO approaches. Importantly, the interaction between the Li₃⁺ with N₂ [for example, it reached up to −24.5 kcal/mol for the Li₃⁺(N₂)₄ complex] is stronger than that with H₂ but weaker than that with H₂O molecules. The difference in the Gibbs free energies for the same series of model complexes (through possible fragmentation channels) specified the thermodynamic stability of the Li₃⁺ in the (N₂)_n clusters. As electrostatic interaction plays a dominant role over the polarization component in the case of the Li₃⁺(H₂O)_n complexes, a different case was found in the construction of the Li₃⁺(N₂)_n complex having a non-covalent nature where the electrostatic and polarization components contributed almost equally. Furthermore, they concluded that the superalkali trinuclear Li₃⁺ cation is a much better candidate than its other heavy alkali metal cations (Na₃⁺ and K₃⁺) in terms of capturing N₂ molecules which is due to a larger BE and favorable structural features for the Li₃⁺(N₂)_n complexes as compared to the N₂ associated with the Na⁺ and K⁺ cations. Moreover, by resemblance, the Li₃⁺ superalkali cation (along with retaining its identity) has been predicted to have 12 maximum coordination numbers in the nitrogen clusters whose structure (see Figure 4Ba) was assured by the ab initio molecular modeling approach with the deployment of the MP2/6-311+G(d) level of theory and the local minima was confirmed by the frequency calculations. Analogous to the isolated Li₃⁺ alkali metal cation, a delocalized s-type bonding HOMO was detected in the case of Li₃⁺(N₂)₁₂ which can be seen in Figure 4Bb. The computed NMR parameters (chemical shifts ranging from −95.5 to −94.1 ppm and −66.8 to −64.0 ppm for the ¹⁵N1 and ¹⁵N1′ nuclei, correspondingly) can indeed provide significant information for the experimental classification of the complexes. Of course, this work provided an in-depth understanding of the mechanism of binding interactions in the Li₃⁺(N₂)_n complexes and explored the superalkali-based nitrogen-gas-trapping agents by spurring more computational and experimental attempts.

As CO₂, with the property of trapping greenhouse gases, has a crucial role in the global carbon balance purpose along with its conversion into fuel, a very recent in silico-based report by H. Srivastava and A. K. Srivastava on the activation of CO₂ by various types of superalkalis can be seen in the literature where they showed comprehensive and interesting theoretical outcomes (see Figure 4C) (Srivastava and Srivastava, 2022). Some studies on the superbases which were designed with the help of superalkalis can be seen in the literature (Srivastava and Misra, 2015, Srivastava and Misra, 2016). Because of the superalkalis, for example, typical superalkalis (FLi₂, OLi₃, and NLi₄), special superalkalis [Al₃, Mn(B₃N₃H₆)₂, B₉C₃H₁₂, and C₅NH₆], binuclear superalkalis (Li₃F₂), non-metallic superalkalis (O₂H₅ and N₂H₇), and polynuclear superalkalis (Al₁₂P, N₄Mg₆M) having lower IP than those of the alkali atoms and can easily transfer an electron (due to its hypervalent nature) to the CO₂ molecule, these species possess strong reducing power and play an imperative role in altering the geometry of CO₂ (bent shape) from its linear structure by donating an electron to it, which have been reported based on the quantum chemical methods. Examining different theory-based reports, it was observed that the extent of the CT (electron transfer) is mainly dependent on the size, geometrical, and electronic features as well as the (IPs) of the superalkali species. In silico-based investigations and discussions on the activation of CO₂ by a small Li₃F₂ cluster inside the Buckminsterfullerene can also be seen in the literature. It was also found that the CO₂ molecule is not only activated by the C₆Li₆ molecule but also a total of six CO₂ molecules can be trapped by the same species. From this report, Srivastava et al. came up with concluding remarks that the reported theoretical findings imply that superalkalis could be utilized as an economical catalyst for the activation of a CO₂ molecule, and since the fuel can be formed by the activated CO₂ ion like methanol (CH₃OH) followed by the hydrogenation reaction. Moreover, Srivastava et al. (2022) have reported various computational experiments using the DFT as well as ab initio modeling approaches on the superalkali cations (X = F, O, and N) with methyl ligands, superalkali behavior of ammonium and hydronium cations, and many more studies (Srivastava, 2019b). Moreover, introducing the superalkalis, an ab initio study on single- and double-electron reductions of CO₂ was reported in 2018 (Srivastava, 2018).

Complex formations and interactions involved therein

To begin with the idea of superalkalis, complexes are superalkalis with a lower IP than the corresponding alkali and alkaline earth metals; Parida et al. reported work on the computational designing of aromatic organometallic superalkali complexes using the first principle calculations (see Figure 5A) (Parida et al., 2018). A trigonal all-metal core coupled with imidazole (IMD) and pyridine (Py) has been proposed which facilitate the probable existence of a superalkali complex. Low IEs (as compared to the Cesium atom) were found for the organometallic complexes, Au₃(IMD)₃ and Au₃(Py)₃, which imitated the general features of a superalkali very well. All the superalkali clusters revealed sp² hybridization, and therefore, a planar geometry all along with the Au₃⁺ ring showed a “doubly aromatic” character. The HOMO-LUMO gap value of the Au₃(Py)⁺ species (4.11 eV) was found to be greater than that of the Au₃(IMD)⁺ (3.84 eV). As some of the organometallic complexes were capable of showing good NLO features using the static first-order hyper-polarizability calculations, it also appeared that the characteristics of such Au-based complexes are like the features of a superalkali. Such outcomes concluded that various coinage metal-based superalkali complexes having broad applications can be synthesized in the laboratory.

FIGURE 5

FIGURE 5. (A) Optimized geometries of the ligands and the Au₃-coupled complexes reproduced with permission from Parida et al. (2018); (B) representative Al₃-M and Al₃-X superatom compounds where M is a (super)alkali (M = Li, FLi₂, OLi₃, and NLi₄) and X is a superhalogen (X = F, LiF₂, BeF₃, and BF₄) reproduced from Yang et al. (2018) with permission from the Royal Society of Chemistry; (C) computed SOMO/HOMO 3D isosurfaces of the superalkali K-15-crown-5₂ model (a) and superalkali−alkalide (K-15-crown-5₂)^δ+(Na)^δ− with the alkalide in the axial reproduced from Riedel et al. (2021) (c) and equatorial (d) positions with respect to the sandwich complex [as illustrated in the form of a cartoon (b)]; (D) optimized geometries for (a) Li₃O and (b) Li₃S (top); cubic ABX₃ perovskite structures with superalkali clusters occupying the A sites, Pb atoms occupying the B sites, and I atoms occupying the X sites (bottom) adapted from Paduani and Rappe (2017) with permission from the Royal Society of Chemistry.

Combinations of aluminum trimer and two distinct forms of the representative superatom clusters [(super) alkalis: M = F, FLi₂, OLi₃, and NLi₄; and (super) halogens: X = LiF₂, BeF₃, and BF₄)] were chosen, and the diverse structural, stability (interactions involved in the Al₃-M and Al₃-X superatom compounds), and electronic features were theoretically explored by Yang et al. (2018) at the MP2/6-311+(3df) level of theory. The Al₃-M and Al₃-X compounds (see Figure 5B) showed different structures where point-to-side interactions were seen between the Al₃ and X components of the Al₃-X compound, providing the most favorable bonding pattern while the least preferable was face-to-face. In the case of Al₃-M systems, Al₃ favored interacting with the FLi₂ and Li (super) alkalis via its ring plane, whereas it favored binding with NLi₄ and OLi₃ superalkalis over the Al–Al edge. Interestingly, the Al₃ moiety of the Al₃-X species acts as the cation (electron donor), whereas it acts as an anion (electron acceptor) in the Al₃-M compound assured by the NPA approach. Enhanced CT was detected between the Al₃ component and the super-atoms (M and X) in both polar and nonpolar solvents. The HOMO-LUMO gap values, BEs, and bond energies were calculated to be large which confirmed the stability of such blended species (Al₃-M and Al₃-X compounds) supported by strong interactions taking part between the Al₃ and super-atoms (M/X). Importantly, the solvent effect has an important role in the case of the Al₃-M (especially, the Al₃-NLi₄) compounds where it was found that such species were better stabilized in the presence of the solvent molecules, whereas the outcomes were not significant for the stability of the Al₃-X compounds. Moreover, the Al₃⁺ ring exhibited different aromatic characters (σ and π aromaticity) when associated with diverse superhalogen anions either in the gas or in liquid phases.

As it has been conventionally considered that the anionic alkali metals in the solution possess a gas-like and unperturbed nature recently, Barrett et al. reported experimental and theoretical findings on superalkali–akalide interaction-related studies which assisted ion pairing in alkalide solutions in solvents having low polarity (Riedel et al., 2021). The experimental evidence (based on coherent neutron scattering, dielectric spectroscopy, and concentration-dependent macroscopic ionic conductivity) of the observation and influence of ion pairing of alkalides in the solution agreed with each other. Furthermore, to understand the structural, stability, and electronic features, the DFT studies for a range of possible superalkali–alkalide complexes chosen as models were carried out in the framework of ab initio simulations, including the superalkalis and superalkali dimers where such species were revealed to play the dominant role in the solution. The visualized singly occupied molecular orbital (SOMO)/HOMO 3D isosurface maps of the superalkali K-15-crown-5₂ model (a), superalkali−alkalide (K-15-crown-5₂)^δ+(Na)^δ− associated with the alkalide in the axial (c), and equatorial (d) sites concerning the sandwich complex are exemplified in the form of a cartoon (b) as shown in Figure 5C. The conformational flexibility of the alkalide systems measured by the temperature-dependent alkali metal NMR spectra appeared to show both reversible perturbation and thermally triggered demonstrating a complex replacement mechanism for the ion-paired moieties. The outcomes of their research work facilitated a picture of alkalide moieties acting as a gas-like ion in the solution and attached a great significance to the interactions of the alkalide with its complex counteraction (superalkali) which could be chemically regulated and established by contemplating the interactions between the superalkali and alkalides.

Recently (in 2021), to synthesize aromatic trinuclear Cu(I)-NHC complexes constructed from superalkali ligands as a building block, a variety of NHC (N-heterocyclic carbene) ligands based on imidazole and benz-imidazole have been computationally designed by Giri et al. Six different ligands were chosen based on the pyridazine, pyrimidine, and pyrazine acting as the skeletons (Parida et al., 2019). According to the outcomes of the calculated vertical electron affinity, all of the ligands chosen in this work seem to be of the superalkali kind of molecule which has excellent NLO properties. The Cu(I)@NHC complexes were formed by the NHC ligands consisting of trinuclear Cu₃ as the central moiety. From the contribution of canonical molecular orbitals toward the computed nucleus independent chemical shift (NICS) values, the trinuclear Cu₃ ring appeared to show high σ- and low π-aromaticity. Depending on the various ligand environments, the aromatic features were altered along with other reactivity parameters such as electrophilicity and hardness. According to their theoretical findings, a more reactive and less aromatic complex can be produced by the pyrazine-based NHC ligand as opposed to pyridazine and pyrimidine-based NHCs. Like the BH₃ molecule, the inspected super-atomic clusters exhibit sp² hybridization based on the natural localized molecular orbitals (LMOs). Very interestingly, the UV-Vis spectrum calculations using the first principle study in the acetonitrile solvent showed a blue shift. It is believed that such modeled and theoretically explored complexes can be simply synthesized and utilized as catalysts in advanced synthetic chemistry.

The influence of variations in the ionicity of CT and bonding mechanism on the geometrical and electronic features of novel lead-based halide perovskites formed by introducing the superalkali species was reported by Paduani and Rappe in 2017 with the employment of the scalar relativistic DFT approach (Paduani and Rappe, 2017). In this work, the authors used two superalkalis such as Li₃O [see Figure 5Da] and Li₃S [see Figure 5Db] which were replaced by the Cs atoms in the CsPbI₃ having a cubic structure which were detected to be slightly tetragonally distorted, and the band gap values of both superalkali-based species were much lower than that of the cubic CsPbI₃. The in silico-based outcomes facilitated encouraging performance which can have applications in optoelectronics, for instance, as long-wave infrared (IR) sensors and thermoelectrics. They found that the incorporation of suitable superalkali species at the cationic A-positions in the ABX₃-type (CsPbI₃) structure can have the capability to tune the band gap of such species. Smaller band gaps (mainly occurring from the effective hybridization between the Pb and Li s-states at the top of the valence band) for the minimum-energy (i.e., equilibrium) crystal structures of both the [Li₃S]PbI₃ and [Li₃O]PbI₃ compounds were analyzed as 0.41 eV (indirect) and 0.36 eV (direct), correspondingly, where the latter is slightly larger than the former. The [Li₃O]PbI₃ compound was hoped to be more resistant to water exposure which was confirmed by the cluster calculations. In comparison to the CsPbI3 species, harsh alterations can be seen in the shape of both valance and conduction bands when the chemical environment was changed in the case of the Pb-halide perovskite structure. Because of the construction of the delocalized energy states, additional electronic states near the Fermi level were formed by introducing the superalkali cations. Such studies have the capability to crease the excitation diffusion length at a longer wavelength and promote hole mobility. Berry-phase simulations demonstrate considerable spontaneous polarization in both novel materials [Li₃O]PbI₃ and [Li₃S]PbI₃ having non-centrosymmetric structures (lacking inversion symmetry) and thus, allow this material to be used in communications, ferroelectrics, and remote sensing in a prolonged spectrum region.

Taking a quick glimpse at a different type of superalkali cation, a series of interesting computational experiments on the structural, stability/energetics, and electronic feature analyses of some new series of interesting non-metallic superalkali cations such as chain-shaped F_nH_n+1⁺ species, O_xH_2x+1⁺ clusters, and N_nH_3n+1⁺ species were reported by Srivastava (2019a), Srivastava (2019d), and Srivastava (2019c).

Concluding remarks and future perspectives

The recent advances in the theoretical development, characterization, and first-time use of superalkalis are outlined in this review. In this report, we have made an effort to provide a general overview of modeling/design and characterization (theoretically) of superalkalis and their applications including sharing predictions for their future growth in the hopes of pointing designers in the right direction as they continue to create and use these special species. Efforts have been made to unveil the potential of some novel superalkali cations (Li₃⁺) and C₆Li₆ type species for capturing and storing CO₂/N₂ molecules. The first-order hyperpolarizability-based NLO response properties of many new computationally designed superalkali-based materials (for example, fullerenes such as mixed-superalkali-doped B₁₂N₁₂ and B₁₂P₁₂ nanoclusters having good UV transparency and novel inorganic aromatic mixed-valent superalkali CaN₃Ca as an alkali-earth-based high sensitivity multi-state NLO molecular switch, and novel lead-based halide perovskites formed by introducing the superalkali species) which can, indeed, be used as a new kind of electronic nanodevice for designing hi-tech NLO materials have been unraveled in this review. Understanding the mere interactions of alkalides in a solution, as well as in the gas phase where the potential to influence how such systems can be extended and applied in the future, is also highlighted in this survey. Understanding earned from this report will, indeed, assist in the discovery of novel superalkalis and will enrich the library’s arsenal of supersalts.

Although, based on this review, we can predict the forthcoming directions at the industrial level, there are still tasks to better understand the fascinating features of superalkalis and their characteristics to be measured precisely in the fields of inorganic, organic, and material chemistry. We are hopeful that further experiments, as well as theoretical investigations, will be capable of developing the present strategies and contributing to our future sights in better understanding the attention-grabbing features of a variety of already synthesized and designed/modeled novel superalkalis or related species. Moreover, the reported model complexes (as building new materials) in this report will be advantageous, and these may pave alternative pathways for experimentally rewarding applications and can have potential uses in advanced synthetic chemistry as catalysts.

Author contributions

SP contributed mainly to this report (selection of the topic, its conception, and design). Material preparation, data collection, and figure implementation were mainly performed by SP. All version of the drafts of the manuscript were written and edited by SP, and all other co-authors commented on all drafts of the manuscript. All the authors read and approved the final manuscript.

Acknowledgments

SKP is thankful to the University Grant Commission (UGC), New Delhi, India, for providing D. S. Kothari - Postdoctoral Fellowship (CH/19-20/0028).

Conflict of interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s note

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