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The ~3[ndσ~*(n+1)pσ] Emissions of Linear Silver(I) and Gold(I) Chains withBridging Phosphine Ligands

机译:桥联膦配体的线性银(I)和金(I)链的〜3 [ndσ〜*(n + 1)pσ]发射

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The complexes [Au_3(dcmp)_2][X]_3{dcmp =bis(dicyclohexylphosphi-nomethyl)cyclohexylphosphine; X=Cl (1), ClO)_4~- (2), OTf~- (3), PF_6~-(4),SCN~-(5)}, [Ag_3(dcmp)_2][ClO_4]_6), and[Ag_3(dcmp)_2Cl_2][ClO_4](7) were pre-pared and their structures were deter-mined by X-ray crystallography. Com-plexes 2-4 display a high-energy emis-sion band with λ_(max)at 442-452 nm,whereas 1 and 5 display a low-energyemission with λ_(max)at 558-634 nm inboth solid state and in dichlorome-thane at 298 K. The former is assignedto the ~3[5dσ~*6pσ] excited state of [Au_3-(dcmp)_2]~(3+), whereas the latter is attrib-uted to an exciplex formed betweenthe ~3[5dσ~*6pσ] excited state of [Au_3-(dcmp)_2[~(3+)and the counterions. Insolid state, complex [Ag_3(dcmp)_2]-[ClO_4]_3 (6) displays an intense emissionband at 375 nm with a Stokes shift of 7200 cm~(-1) from the ~1[4dσ~*?ú5pσ] ab-sorption band at 295 nm. The 375 nmemission band is assigned to the emis-sion directly from the ~3[4dσ~*5pσ] excit-ed state of 6. Density functional theory(DFT) calculations revealed that theabsorption and emission energies areinversely proportional to the numberof metal ions (n) in polynuclear Auand Ag~I linear chain complexes withoutclose metal???anion contacts. The emis-sion energies are extrapolated to be715 and 446 nm for the infinite linearAu~I and Ag~I chains, respectively, atmetal???metal distances of about 2.93-3.02 A. A QM/MM calculation on themodel [Au_3(dcmp)_2Cl_2]~+system, withAu???Cl contacts of 2.90-3.10 A, gaveoptimized Au???Au distances of 2.99-3.11 A in its lowest triplet excited stateand the emission energies were calcu-lated to be at approximately 600-690 nm, which are assigned to a three-coordinate Au~I site with its spectro-scopic properties affected by Au~I???Au~Iinteractions.
机译:配合物[Au_3(dcmp)_2] [X] _3 {dcmp =双(二环己基膦基-无甲基)环己基膦; X = Cl(1),ClO)_4〜-(2),OTf〜-(3),PF_6〜-(4),SCN〜-(5)},[Ag_3(dcmp)_2] [ClO_4] _6)制备了[Ag_3(dcmp)_2Cl_2] [ClO_4](7),并通过X射线晶体学测定了它们的结构。复合物2-4在442-452 nm处具有λ_(max)的高能发射带,而1和5在固态和固态下均在558-634 nm处具有λ_(max)的低能发射。二氯甲烷在298 K时。前者归属于[Au_3-(dcmp)_2]〜(3+)的〜3 [5dσ〜*6pσ]激发态,而后者归属于〜之间形成的激基复合物。 [Au_3-(dcmp)_2 [〜(3+)]和抗衡离子的3 [5dσ〜*6pσ]激发态。在固态下,复杂的[Ag_3(dcmp)_2]-[ClO_4] _3(6)在375 nm处显示出很强的发射带,从〜1 [4dσ〜*?ú5pσ] ab处的斯托克斯位移为7200 cm〜(-1)。在295nm处的吸收带。从〜3 [4dσ〜*5pσ]激发态直接将375 nm发射带分配给发射。密度泛函理论(DFT)计算表明,吸收和发射能与金属离子的数量成反比( n)在没有紧密的金属阴离子接触的多核Auand Ag-1线性链络合物中。对于无限大的线性Au〜I和Ag〜I链,在金属???金属距离约为2.93-3.02 A时,发射能分别推断为715 nm和446 nm。在模型[Au_3(dcmp )_2Cl_2]〜+系统,其Au的Cl接触为2.90-3.10 A,在其最低三重激发态下,Au的最佳Au距离为2.99-3.11 A,计算出的发射能约为600- 690nm,它被分配到一个三坐标的Au-I位点,其光谱特性受Au-I-Au-Iu-相互作用的影响。

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