Ternary zero-dimensional hybrid metal halides with dual emission

Bulk assemblies of zero-dimensional (0D) metal halides with ‘host-guest’ system provide a promising platform for rationally structural tunability and photoluminescence modulation. In this work, we first report a series of ternary 0D metal halides, (bmpy)₉[Pb₃Cl₁₁](MnCl₄)_2-2x(SbCl₅)_2x (bmpy⁺ = 1-buty-1-methylpyrrolidinium⁺, C₉NH₂₀⁺), where the organic cation bmpy⁺ cocrystallizes with [Pb₃Cl₁₁]^5- trimer clusters, [MnCl₄]^2? tetrahedra, and [SbCl₅]^2? pyramids. The emission color of (bmpy)₉[Pb₃Cl₁₁](MnCl₄)_2-2x(SbCl₅)_2x can be easily tuned from green to warm white and finally to orange-red by controlling the excitation wavelength or the [SbCl₅]^2?/[MnCl₄]^2? molar ratio, promising its potential for application in multicolor light-emitting devices or even in encrypting multilevel optical codes. This work presents a novel structural modulation strategy to fabricate superior ordered single-crystalline multicomponent materials with multifunctionalities of 0D luminescent metal halides.     

Air‐Stable,Lead‐Free Zero‐Dimensional Mixed Bismuth‐Antimony Perovskite Single Crystals with Ultra‐broadband Emission

Lead‐free zero‐dimensional (0D) organic‐inorganic metal halide perovskites have recently attracted increasing attention for their excellent photoluminescence properties and chemical stability. Here, we report the synthesis and characterization of an air‐stable 0D mixed metal halide perovskite (C₈NH₁₂)₄Bi_0.57Sb_0.43Br₇?H₂O, in which individual [BiBr₆]^3? and [SbBr₆]^3? octahedral units are completely isolated and surrounded by the large organic cation C₈H₁₂N⁺. Upon photoexcitation, the bulk crystals exhibit ultra‐broadband emission ranging from 400 to 850 nm, which originates from both free excitons and self‐trapped excitons. This is the first example of 0D perovskites with broadband emission spanning the entire visible spectrum. In addition, (C₈NH₁₂)₄Bi_0.57Sb_0.43Br₇?H₂O exhibits excellent humidity and light stability. These findings present a new direction towards the design of environmentally‐friendly, high‐performance 0D perovskite light emitters.     

Air‐Stable,Lead‐Free Zero‐Dimensional Mixed Bismuth‐Antimony Perovskite Single Crystals with Ultra‐broadband Emission

Lead‐free zero‐dimensional (0D) organic‐inorganic metal halide perovskites have recently attracted increasing attention for their excellent photoluminescence properties and chemical stability. Here, we report the synthesis and characterization of an air‐stable 0D mixed metal halide perovskite (C₈NH₁₂)₄Bi_0.57Sb_0.43Br₇?H₂O, in which individual [BiBr₆]^3? and [SbBr₆]^3? octahedral units are completely isolated and surrounded by the large organic cation C₈H₁₂N⁺. Upon photoexcitation, the bulk crystals exhibit ultra‐broadband emission ranging from 400 to 850 nm, which originates from both free excitons and self‐trapped excitons. This is the first example of 0D perovskites with broadband emission spanning the entire visible spectrum. In addition, (C₈NH₁₂)₄Bi_0.57Sb_0.43Br₇?H₂O exhibits excellent humidity and light stability. These findings present a new direction towards the design of environmentally‐friendly, high‐performance 0D perovskite light emitters.     

Bromoplumbate mit kettenförmigen und isolierten Anionen: (Bzl4P)2[Pb3Br8], (Bzl4P)2[Pb3Br8(dmf)2], (Bzl4P)[PbBr3], (Bzl4P)2[PbBr4] und (Bzl4P)4[Pb2Br6][PbBr4]

Bromoplumbates with One‐dimensional Polymeric and Isolated Anions: (Bzl₄P)₂[Pb₃Br₈], (Bzl₄P)₂[Pb₃Br₈(dmf)₂], (Bzl₄P)[PbBr₃], (Bzl₄P)₂[PbBr₄], and (Bzl₄P)₄[Pb₂Br₆][PbBr₄] PbBr₂ reacts with LiBr and (Bzl₄P)(PF₆) (Bzl = CH₂C₆H₅) in acetone to form a series of bromoplumbate complexes with compositions and structures depending on the conditions of reaction and crystallization. While the anions in (Bzl₄P)₂[Pb₃Br₈] ( 1 ) and (Bzl₄P)[PbBr₃] ( 2 ) are one‐dimensional polymers with penta‐ and hexacoordinated Pb atoms, the metal atoms in the mono‐ and dinuclear complex anions of (Bzl₄P)₂[PbBr₄] · 2acetone ( 3 · 2acetone) and (Bzl₄P)₄[Pb₂Br₆][PbBr₄] ( 4 ) bind to four bromo ligands. From DMF as a solvent (Bzl₄P)₂[Pb₃Br₈(dmf)₂] ( 1 b ) crystallizes with the same bromoplumbate structure as in 1 a , but with dmf ligands occupying the coordination sites vacant in 1 a . Upon radiation of compound 3 with ultraviolet light greenish yellow photoluminescence (emssion maximum at 547 nm) is observed. Crystallographic details see “Inhaltsübersicht”.     

Ein oktaedrischer Niobcluster mit sechs terminalen Azidgruppen: Die Struktur von Rb4[Nb6Br12(N3)6](H2O)2

An Octahedral Niobium Cluster containing Six Terminal Azide Groups: The Structure of Rb₄[Nb₆Br₁₂(N₃)₆](H₂O)₂ Six terminal halide ligands of [Nb₆Br₁₂Br₆]^4? can be substituted in solution by azide ions. Single-crystals of Rb₄[Nb₆Br₁₂(N₃)₆](H₂O)₂ were obtained during the evaporation of the water/methanol solvent, and structurally characterized by X-ray methods: Space group P2₁/c, Z = 2, a = 970.8(5) pm, b = 1525.4(7) pm, c = 1280.0(7) pm, β = 97.15(6)°. The [Nb₆Br₁₂(N₃)₆]^4? ions contain six terminal azide groups at the corners of the octahedral niobium cluster (d _Nb–N = 227 pm). The [Nb₆Br₁₂(N₃)₆]^4? ions are interconnected by Rb⁺ and H₂O. Crystals of Rb₄[Nb₆Br₁₂(N₃)₆](H₂O)₂ are explosive towards heat or mechanic pressure.     

Synthese und Kristallstruktur von Blei(II)‐oxidhalogenid‐Alkoholaten mit unterschiedlichen Verknüpfungsvarianten von Pb4O4‐Heterokubaneinheiten

Synthesis and Crystal Structure Determination of Lead(II) Oxide Halide Alcoholates with Different Connectivity of Pb₄O₄ Heterocubane‐like Subunits The reaction of red lead(II) oxide (Litharge) and lead(II) halide (Cl^? and Br^?) with diethylene glycole at a temperature of 180 °C leads to the isotypic compounds [Pb₆(C₄H₈O₃)O₂Cl₆] (1) and [Pb₆(C₄H₈O₃)O₂Br₆] (2) . In a similar synthesis with PbI₂ as educt at temperature of 160 °C the two modifications β‐[Pb₆(C₄H₈O₃)O₂I₆] (3) and α‐[Pb₆(C₄H₈O₃)O₂I₆] (4) were found, whereas at a reaction temperature of 180 °C [Pb₉(C₂H₄O₂)(C₄H₈O₃)O₃I₈] (5) was surprisingly obtained as product. The X‐ray diffraction data show that at a temperature of 180 °C a splitting of the ether took place. The cited compounds show cubane like subunits built by lead and oxygen atoms. These fragments are connected by alkoholate molecules. In 5 additionally an I₆ octahedra centered by lead is observed.     

Synthese,Struktur und Thermolyse von NH4[Re3Br10]

Synthesis, Structure and Thermolysis of NH₄[Re₃Br₁₀] NH₄[Re₃Br₁₀] crystallizes as dark brown single crystals upon slow cooling of a hot, saturated hydrobromic-acid solution of [Re₃Br₉(H₂O)₂] after the addition of NH₄Br. The crystal structure (monoclinic, C2/m (Nr. 12); Z = 4; a = 1461.6(7), b = 1 085.6(4), c = 1030.3(7) pm, β = 92.63(4)°, V_m = 245.9(4)cm³/mol; R = 0.097, R_w = 0.043) contains [Re₃Br₁₂]^? units that share two common edges. These chains run along [010] and are held together by NH₄⁺ ions. Each NH₄⁺ is surrounded by eight Br^? from four different chains. The first step of the thermal decomposition at 290°C is the disproportionation to ReBr₃ (ReCl₃ type), rhenium metal and (NH₄)₂[ReBr₆]. Secondly, the internal reduction of (NH₄)₂[ReBr₆] at 390°C to rhenium metal takes place.     

Three‐Dimensional Cuprous Lead Bromide Framework with Highly Efficient and Stable Blue Photoluminescence Emission

Considering the instability and low photoluminescence quantum yield (PLQY) of blue‐emitting perovskites, it is still challenging and attractive to construct single crystalline hybrid lead halides with highly stable and efficient blue light emission. Herein, by rationally introducing d¹⁰ transition metal into single lead halide as new structural building unit and optical emitting center, we prepared a bimetallic halide of [(NH₄)₂]CuPbBr₅ with new type of three‐dimensional (3D) anionic framework. [(NH₄)₂]CuPbBr₅ exhibits strong band‐edge blue emission (441 nm) with a high PLQY of 32 % upon excitation with UV light. Detailed photophysical studies indicate [(NH₄)₂]CuPbBr₅ also displays broadband red light emissions derived from self‐trapped states. Furthermore, the 3D framework features high structural and optical stabilities at extreme environments during at least three years. To our best knowledge, this work represents the first 3D non‐perovskite bimetallic halide with highly efficient and stable blue light emission.     

Synthesis, crystal structure and optical limiting properties of some W---Se---Cu clusters

A nest-shaped cluster [(C₄H₉)₄N]₂[WOSe₃Cu₃Br_1.67Cl_1.33] (1) and a cage-shaped cluster [(C₄H₉)₄N]₃[WSe₄Cu₃Br₂Cl₂] (2) were synthesized and their structures were determined by single-crystal X-ray diffraction. It was found that cluster 1 showed better optical limiting properties under an 8 ns pulsed laser at 532 nm but poorer optical limiting properties under a 35 ps pulsed laser compared with its analogue [(C₄H₉)₄N]₂[MoOS₃Cu₃BrCl₂]. The influence of the peripheral ligands of the cluster to the optical limiting properties was also discussed.     

Ionic‐Liquid‐Based Synthesis of the Bromine‐Rich Bromidoplatinates [NBu3Me]2[Pt2Br10](Br2)2 and [NBu3Me]2[Pt2Br10](Br2)3

The bromine‐rich bromidoplatinates(IV) [NBu₃Me]₂[Pt₂Br₁₀](Br₂)₂ ( 1 ) and [NBu₃Me]₂[Pt₂Br₁₀](Br₂)₃ ( 2 ) were prepared by reaction of PtBr₄ and elemental bromine in the ionic liquid [MeBu₃N][N(Tf)₂] [N(Tf)₂ = bis(trifluoromethylsulfonyl)amide]. Both bromine‐rich bromidoplatinates(IV) contain [Pt₂Br₁₀]^2– anions and [NBu₃Me]⁺ cations as voluminous building units with an almost identical structural arrangement and very similar unit cells. The difference of the title compounds is related to the specific number of Br₂ molecules that link the [Pt₂Br₁₀]^2– anions to three‐dimensional networks. Whereas 1 is relatively stable under inert conditions, 2 releases bromine even at ambient pressure. The title compounds are characterized by single‐crystal structure analysis and Raman spectroscopy.     

Reactivity of Ammonium Halides: Action of Ammonium Chloride and Bromide on Iron and Iron(III) Chloride and Bromide

Ammonium chloride and bromide, (NH₄)Cl and (NH₄)Br, act on elemental iron producing divalent iron in [Fe(NH₃)₂]Cl₂ and [Fe(NH₃)₂]Br₂, respectively, as single crystals at temperatures around 450 °C. Iron(III) chloride and bromide, FeCl₃ and FeBr₃, react with (NH₄)Cl and (NH₄)Br producing the erythrosiderites (NH₄)₂[Fe(NH₃)Cl₅] and (NH₄)₂[Fe(NH₃)Br₅], respectively, at fairly low temperatures (350 °C). At higher temperatures, 400 °C, iron(III) in (NH₄)₂[Fe(NH₃)Cl₅] is reduced to iron(II) forming (NH₄)FeCl₃ and, further, [Fe(NH₃)₂]Cl₂ in an ammonia atmosphere. The reaction (NH₄)Br + Fe (4:1) leads at 500 °C to the unexpected hitherto unknown [Fe(NH₃)₆]₃[Fe₈Br₁₄], a mixed‐valent Fe^II/Fe^I compound. Thermal analysis under ammonia and the conditions of DTA/TG and powder X‐ray diffractometry shows that, for example, FeCl₂ reacts with ammonia yielding in a strongly exothermic reaction [Fe(NH₃)₆]Cl₂ that at higher temperatures produces [Fe(NH₃)]Cl₂, FeCl₂ and, finally, Fe₃N.     

Darstellung und Kristallstruktur der ersten Vertreter des neuen Verbindungstyps Pb4[SiO4]X4 mit X = Cl,Br

Inhaltsübersicht. Die beiden silicathaltigen Blei(II)-oxidhalogenide Pb₄[SiO₄]Cl₄ und Pb₄[SiO₄]Br₄ wurden erstmals dargestellt und ihre Kristallstruktur an Einkristallen mit Röntgen-beugungsmethoden ermittelt. Die Verbindungen kristallisieren in der monoklinen Raumgruppe P2₁/c (No. 14) mit den Gitterparametern: Pb₄[SiO₄]Cl₄: A = 8,73(1) Å, b = 15,68(1) Å, c = 8,265(6) Å, β = 92,4(1)°, Z = 4 Pb₄[SiO₄]Br₄: A = 9,00(1) Å, b = 16,217(8) Å, c = 8,404(4) Å, β = 92,4(1)°, Z = 4 Im Gegensatz zu der “nichtstöchiometrischen” Verbindungsgruppe um Pb₈O₇Br₂ · SiO₂ konnten hier alle Atomlagen ermittelt werden. Es liegen einzelne SiO₄-Gruppen vor, die über Pb²⁺ zu leicht gewellten Netzen verbunden sind. Zwischenräume und Löcher der Netze werden von Halogenidionen aufgefüllt. Preparation and Crystal Structures of the First Two Members of a New Type of Lead (II) Oxyhalides, Pb₄[SiO₄]X₄ (X = Cl, Br) Both silicate-bearing lead(II) oxyhalides Pb₄[SiO₄]Cl₄ and Pb₄[SiO₄]Br₄ were prepared and studied for their crystal structure with X-ray single crystal methods for the first time. The compounds crystallize in the monoclinic space group P2₁/c (No. 14) with following lattice parameters: Pb₄[SiO₄]Cl₄: A = 8.73(1) Å, b = 15.68(1) Å, c = 8.205(6) Å, β = 92.4(1)°, Z = 4 Pb₄[SiO₄]Br₄: A = 9.00(1) Å, b = 16.217(8) Å, c = 8.404(4) Å, β = 92.4(1)°, Z = 4. In contrast with further works about the group of nonstoichiometric lead oxyhalides Pb₈O₇Br₂ · SiO₂ in the present work all atomic positions were determined. The crystal structure shows single SiO₄ groups linked only by Pb²⁺ ions to form slightly undulated nets. Holes and interspaces of these nets are stuffed with halide ions.     

Reactivity of Liquid Ammonia Solutions of the Zintl Phase K12Sn17 towards Mesitylcopper(I) and Phosphinegold(I) Chloride

To gain more insight into the reactivity of intermetalloid clusters, the reactivity of the Zintl phase K₁₂Sn₁₇, which contains [Sn₄]^4? and [Sn₉]^4? cluster anions, was investigated. The reaction of K₁₂Sn₁₇ with gold(I) phosphine chloride yielded K₇[(η²‐Sn₄)Au(η²‐Sn₄)](NH₃)₁₆ ( 1 ) and K₁₇[(η²‐Sn₄)Au(η²‐Sn₄)]₂(NH₂)₃(NH₃)₅₂ ( 2 ), which both contain the anion [(Sn₄)Au(Sn₄)]^7? ( 1 a ) that consists of two [Sn₄]^4? tetrahedra linked through a central gold atom. Anion 1 a represents the first binary Au?Sn polyanion. From this reaction, the solvate structure [K([2.2.2]crypt)]₃K[Sn₉](NH₃)₁₈ ( 3 ; [2.2.2]crypt=4,7,13,16,21,24‐hexaoxa‐1,10‐diazabicyclo[8.8.8]hexacosane) was also obtained. In the analogous reaction of mesitylcopper with K₁₂Sn₁₇ in the presence of [18]crown‐6 in liquid ammonia, crystals of the composition [K([18]crown‐6)]₂[K([18]crown‐6)(MesH)(NH₃)][Cu@Sn₉](thf) ( 4 ) were isolated ([18]crown‐6=1,4,7,10,13,16‐hexaoxacyclooctadiene, MesH=mesitylene, thf=tetrahydrofuran) and featured a [Cu@Sn₉]^3? cluster. A similar reaction with [2.2.2]crypt as a sequestering agent led to the formation of crystals of [K[2.2.2]crypt][MesCuMes] ( 5 ). The cocrystallization of mesitylene in 4 and the presence of [MesCuMes]^? ( 5 a ) in 5 provides strong evidence that the migration of a bare Cu atom into an Sn₉ anion takes place through the release of a Mes^? anion from mesitylcopper, which either migrates to another mesitylcopper to form 5 a or is subsequently protonated to give MesH.     

X‐ray Investigation and Coordination Behaviour of the 1,3‐Diallylbenzimidazolium Cation in [C13H15N2]+2 [CuCl2.58Br1.42]2– and [C13H15N2]+[Cu2Cl0.67Br2.33]– Complexes

By means of alternating current electrochemical synthesis crystals of [C₁₃H₁₅N₂]⁺₂[CuCl_2.58Br_1.42]^– ( I ) and [C₁₃H₁₅N₂]⁺[Cu₂Cl_0.67Br_2.33]^– ( II ) have been obtained and structurally characterized. Compound I crystallizes in the orthorhombic system, space group Fddd, a = 7.828(1) Å, b = 26.402(2) Å, c = 28.595(3) Å, D_c = 1.4995(5) g/cm³, Z = 8, R = 0.067 for 2157 reflections. The CuX₄^2– tetrahedra are connected with the organic cations through an electrostatic interaction. Crystals of II are monoclinic, space group P2₁/c, a = 9.2293(8) Å, b = 22.1332(9) Å, c = 9.2939(9) Å, β = 118.021(4)°, D_c = 2.1251(5) g/cm³, Z = 4, R = 0.042 for 2858 reflections. A tetrahedral environment of the Cu1 atom involves four halide atoms, whereas Cu2 possesses a trigonal‐pyramidal coordination with the C=C‐bond and three halide atoms.     

Bis(tetramethylammonium) hexaaquadodeca‐μ‐bromo‐octahedro‐hexatantalum tetrabromide dihydrate

The novel title compound, [(CH₃)₄N]₂[Ta₆Br₁₂(H₂O)₆]Br₄·2H₂O, with a [Ta₆Br₁₂]²⁺ cluster unit, has been prepared and structurally characterized. The compound crystallizes in space group C2/c, with a twofold axis passing through the cluster and the centre of symmetry located between the clusters. The nearest neighbouring cluster units are aligned along the crystallographic c axis, forming a one‐dimensional chain pattern.     

First Characterization of an Extended Ammonium‐Ammonia Complex [{NH4(NH3)4}+(μ‐NH3)2] in the Crystal Structure of [NH4(NH3)4][Co(C2B9H11)2] · 2 NH3

The compound [NH₄(NH₃)₄][Co(C₂B₉H₁₁)₂] · 2 NH₃ ( 1 ) was prepared by the reaction of Na[Co(C₂B₉H₁₁)₂] with a proton‐charged ion‐exchange resin in liquid ammonia. The ammoniate 1 was characterized by low temperature single‐crystal X‐ray structure analysis. The anionic part of the structure consists of [Co(C₂B₉H₁₁)₂]^‐ complexes, which are connected via C‐H···H‐B dihydrogen bonds. Furthermore, 1 contains an infinite equation/tex2gif-stack-2.gif[{NH₄(NH₃)₄}⁺(μ‐NH₃)₂] cationic chain, which is formed by [NH₄(NH₃)₄]⁺ ions linked by two ammonia molecules. The N‐H···N hydrogen bonds range from 1.92 to 2.71Å (DHA = Donor···Acceptor angles: 136‐176°). Additional N‐H···H‐B dihydrogen bonds are observed (H···H: 2.3‐2.4Å).     

Multicomponent Organic Metal Halide Hybrid with White Emissions

Zero‐dimensional (0D) organic metal halide hybrids, in which organic and metal halide ions cocrystallize to form neutral species, are a promising platform for the development of multifunctional crystalline materials. Herein we report the design, synthesis, and characterization of a ternary 0D organic metal halide hybrid, (HMTA)₄PbMn_0.69Sn_0.31Br₈, in which the organic cation N‐benzylhexamethylenetetrammonium (HMTA⁺, C₁₃H₁₉N₄⁺) cocrystallizes with PbBr₄^2?, MnBr₄^2?, and SnBr₄^2?. The wide band gap of the organic cation and distinct optical characteristics of the three metal bromide anions enabled the single‐crystalline “host–guest” system to exhibit emissions from multiple “guest” metal halide species simultaneously. The combination of these emissions led to near‐perfect white emission with a photoluminescence quantum efficiency of around 73 %. Owing to distinct excitations of the three metal halide species, warm‐ to cool‐white emissions could be generated by controlling the excitation wavelength.     

Synthesis and Crystal Structure of a Novel Mixed Nido-like and Half-open Cubane-like Cluster [(n-Bu)_4N]_3[MoS_4Cu_5Br_6]

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Kristallstruktur von (NMe4)2[Re3Br11(H2O)] [Re3Br9(H2O)3](H2O)2

Crystal Structure of (NMe₄)₂[Re₃Br₁₁(H₂O)] [Re₃Br₉(H₂O)₃](H₂O)₂ . (NMe₄)₂[Re₃Br₁₁(H₂O)] [Re₃Br₉(H₂O)₃](H₂O)₂ crystallizes from hydrobromic acid solution of Re₃Br₉ · 2 H₂O and NMe₄Br at 0 – 5°C. The crystal structure (monoclinic; P2₁/m (Nr. 11); a = 967.9(3); b = 1 529.7(4); c = 1 710.9(4) pm; β = 91.66(2)°; Z = 2; R = 0.113; R_w = 0.068) has been determined from four-circle diffractometer data. The structure contains two different cluster units of trivalent rhenium, isolated anionic [Re₃Br₁₁(H₂O)]^2? units and neutral cluster units that are connected through crystal water molecules to chains{[Re₃Br₉(H₂O)₃](H₂O)₂}.     

The closo-Cluster Triad: B9X9, [B9X9]· –, and [B9X9]2– with Tricapped Trigonal Prisms (X = Cl,Br, I). Syntheses,Crystal and Electronic Structures

Halogenation of nido-B₁₀H₁₄ with C₂H₂Cl₄, C₂Cl₆, Br₂, or I₂, produces by cluster degradation the (2 n)-closo-clusters B₉X₉ (X = Cl, Br, I). The synthesis of salts of the perhalogenated radical anions of the type (2 n + 1)-closo-[B₉X₉]^{· –} and of the corresponding dianions (2 n + 2)-closo-[B₉X₉]^2– from neutral B₉X₉ is described [n is the number of cluster atoms; (2 n), (2 n + 1), and (2 n + 2) is the number of cluster electrons]. Molecular and crystal structures of B₉Cl₉, B₉Br₉, [(C₆H₅)₄P][B₉Br₉] · CH₂Cl₂, and [(C₄H₉)₄N]₂[B₉Br₉] · CH₂Cl₂ have been determined via X-ray diffraction. All three oxidation states of the cluster retain the tricapped trigonal prism. The reduction of the clusters B₉X₉ was shown by cyclic voltammetry in CH₂Cl₂ to proceed via two successive one-electron reversible steps, separated by at least 0.4 V. The paramagnetic radical anions [B₉X₉]^{· –} (X = Cl, Br) were further characterized by magnetic susceptibility measurements of [Cp₂Fe][B₉X₉] and [Cp₂Co][B₉X₉], respectively. The EPR spectra of [B₉X₉]^{· –} (X = Cl, Br, I) in glassy frozen CH₂Cl₂ solutions showed increasing g anisotropy for the heavier halogen derivatives, illustrating significant halogen participation at the singly occupied MO. The ¹¹B NMR spectra of CD₂Cl₂ solutions of the neutral clusters B₉X₉ exhibit only one sharp resonance, indicating that the boron atoms are highly fluxional in solution. In contrast, two different boron resonances as expected for a rigid tricapped trigonal prism are clearly observed for the [B₉X₉]^2– dianions in solutions and for solid B₉Br₉ in the ¹¹B MAS NMR spectra. Temperature dependent ¹¹B MAS NMR experiments on B₉Br₉ and [B₉Br₉]^2– in the solid state show a reversible coalescence of the two resonances at higher temperature. ¹¹B MAS NMR spectra and DTA measurements of [B₉Br₉]^2– showed a phase transition.