Gas-phase photoelectron spectroscopy( PES) was conducted on [XAg 24 (SPhMe 2 ) 18 ] À (X = Ag, Au) and [YAg 24 -(SPhMe 2 ) 18 ] 2À (Y = Pd, Pt), which have aformal superatomic core (X@Ag 12 ) 5+ or (Y@Ag 12 ) 4+ with icosahedral symmetry. PES results show that superatomic orbitals in the (Au@Ag 12 ) 5+ core remain unshifted with respect to those in the (Ag@Ag 12 ) 5+ core,whereas the orbitals in the (Y@Ag 12 ) 4+ (Y = Pd, Pt) core shift up in energy by about 1.4 eV.T he remarkable doping effect of asingle Yatom (Y = Pd, Pt) on the electronic structure of the chemically modified (Ag@Ag 12 ) 5+ superatom was reproduced by theoretical calculations on simplified model systems and was ascribed to 1) the weaker binding of valence electrons in Y@(Ag + ) 12 compared to Ag + @(Ag + ) 12 due to the reduction in formal charge of the core potential, and 2) the upward shift of the apparent vacuum level due to the presence of ar epulsive Coulomb barrier between [YAg 24 (SPhMe 2 ) 18 ] À and electron.Thiolate (RS)-or dithiolate (RS 2 )-protected silver clusters, such as [Ag 25 (SR) 18 ] À , [1] [Ag 29 (S 2 R) 12 ] 3À , [2] and [Ag 44 -(SR) 30 ] 4À , [3][4][5] are an emerging class of nanomaterials.S inglecrystal X-ray diffraction (SCXRD) analysis showed that [Ag 25 (SR) 18 ] À and [Ag 29 (S 2 R) 12 ] 3À have an icosahedral Ag 13 core (Scheme 1), [1,2] whereas [Ag 44 (SR) 30 ] 4À has at wo-shell Keplerate Ag 32 core. [5] TheA g 13 and Ag 32 cores form the closed-shell electronic configurations (1S) 2 (1P) 6 and (1S) 2 -(1P) 6 (1D) 10 ,r espectively:1 S, 1P,a nd 1D represent superatomic orbitals with angular momenta of 0, 1, and 2, respectively. [6] Structural similarities to gold analogues indicate that the thiolate-protected Ag clusters represent another family of chemically modified superatoms. [7][8][9] Thiolate-protected Ag clusters have attracted researchers due to specific properties such as photoluminescence [10] although they are generally less stable than the gold analogues.Doping with heteroatoms is apromising approach to enhance the stability and further improve the properties of the Ag clusters.S tate-of-the-art synthesis based on coreduction [11,12] and galvanic replacement [13,14] allowed us to precisely define the number, element, and location of the heteroatom(s) introduced into the Ag clusters.F or example, as ingle Ma tom (M = Au,P d, Pt) can be integrated exclusively at the central position of an icosahedral Ag 13 core of [Ag 25 (SPhMe 2 ) 18 ] À[1] to form M@Ag 12 cores in [AuAg 24 (SPhMe 2 ) 18 ] À[13] and [MAg 24 (SPhCl 2 ) 18 ] 2À (M = Pd, Pt) [11] (Scheme 1). Both the undoped Ag 13 and doped M@Ag 12 cores form ac losed electron configuration, (1S) 2 -(1P) 6 .These atomically defined bimetallic clusters provide an ideal platform to study the effect of single-atom doping on their properties.O ptical spectroscopy (Figure 1a)a nd voltammetry [15] showed that the doping slightly modulates the HOMO-LUMO gap of [Ag 25 (SPhMe 2 ) 18 ] À .T he stability [13,15] and photoluminescence quantum yield (PLQY) [10] of [A...