8 research outputs found

    Ruthenium Derivatives of in Situ Generated Redox-Active 1,2-Dinitrosobenzene and 2‑Nitrosoanilido. Diverse Structural and Electronic Forms

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    The article describes one-pot synthesis and structural elucidation of <i>tc</i>-[Ru<sup>II</sup>(pap)<sub>2</sub>(L<sup>•–</sup>)]­ClO<sub>4</sub> [<b>1</b>]­ClO<sub>4</sub> and <i>tc</i>-[Ru<sup>II</sup>(pap)<sub>2</sub>(L′<sup>–</sup>)]­ClO<sub>4</sub> [<b>2</b>]­ClO<sub>4</sub>, which were obtained from <i>tc</i>-[Ru<sup>II</sup>(pap)<sub>2</sub>(EtOH)<sub>2</sub>]­(ClO<sub>4</sub>)<sub>2</sub> and benzofuroxan (L = 1,2-dinitrosobenzene, an intermediate tautomeric form of the biologically active benzofuroxan, L′<sup>–</sup> = 2-nitrosoanilido, pap = 2-phenylazopyridine, <i>tc</i> = <i>trans</i> and <i>cis</i> corresponding to pyridine and azo nitrogen donors of pap, respectively). The same reaction with the newly synthesized and structurally characterized metal precursor <i>cc</i>-Ru<sup>II</sup>(2,6-dichloropap)<sub>2</sub>Cl<sub>2</sub>, however, affords isomeric <i>ct</i>-[Ru<sup>II</sup>(2,6-dichloropap)<sub>2</sub>(L<sup>•–</sup>)]<sup>+</sup> (<b>3a</b><sup>+</sup>) and <i>tc</i>-[Ru<sup>II</sup>(2,6-dichloropap)<sub>2</sub>(L<sup>•–</sup>)]<sup><b>+</b></sup> (<b>3b</b><sup>+</sup>) (<i>cc</i>, <i>ct</i>, and <i>tc</i> with respect to pyridine and azo nitrogens of 2,6-dichloropap) with the structural authentication of elusive <i>ct</i>-isomeric form of {Ru­(pap)<sub>2</sub>} family. The impact of <i>trans</i> or <i>cis</i> orientation of the nitroso group of L/L′ with respect to the NN (azo) function of pap in the complexes was reflected in the relative lengthening or shortening of the latter distance, respectively. The redox-sensitive bond parameters of <b>1</b><sup>+</sup> and <b>3</b><sup>+</sup> reveal the intermediate radical form of L<sup>•–</sup>, while <b>2</b><sup>+</sup> involves in situ generated L′<sup>–</sup>. The multiple redox processes of the complexes in CH<sub>3</sub>CN are analyzed via experimental and density functional theory (DFT) and time-dependent DFT calculations. One-electron oxidation of the electron paramagnetic resonance-active radical species (<b>1</b><sup>+</sup> and <b>3</b><sup>+</sup>) leads to [Ru<sup>II</sup>(pap)<sub>2</sub>(L)]<sup>2+</sup> involving fully oxidized L<sup>0</sup> in <b>1</b><sup>2+</sup> and <b>3</b><sup>2+</sup>; the same in <b>2</b><sup>+</sup> results in a radical species [Ru<sup>II</sup>(pap)<sub>2</sub>(L′<sup>•</sup>)]<sup>2+</sup> (<b>2</b><sup>2+</sup>). Successive reductions in each case are either associated with pap or L/L′<sup>–</sup>-based orbitals, revealing a competitive scenario relating to their π-accepting features. The isolated or electrochemically generated radical species either by oxidation or reduction exhibits near-IR transitions in each case, attributing diverse electronic structures of the complexes in accessible redox states

    Ruthenium-Hydride Mediated Unsymmetrical Cleavage of Benzofuroxan to 2‑Nitroanilido with Varying Coordination Mode

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    The reaction of R-benzofuroxan (R = H, Me, Cl) with the metal precursor [Ru­(Cl)­(H)­(CO)­(PPh<sub>3</sub>)<sub>3</sub>] (<b>A</b>) or [Ru­(Cl)­(H)­(CH<sub>3</sub>CN)­(CO)­(PPh<sub>3</sub>)<sub>2</sub>] (<b>B</b>) in CH<sub>3</sub>CN at 298 K resulted in the intermediate complex [Ru­(Cl)­(L<sup>1</sup>)­(CH<sub>3</sub>CN)­(CO)­(PPh<sub>3</sub>)<sub>2</sub>] (L<sup>1</sup> = monodentate 2-nitroanilido) (<b>1</b>, pink), which however underwent slow transformation to the final product [Ru­(Cl)­(L<sup>2</sup>)­(CO)­(PPh<sub>3</sub>)<sub>2</sub>] (L<sup>2</sup> = bidentate 2-nitroanilido) (<b>2</b>, green). On the contrary, the same reaction in refluxing CH<sub>3</sub>CN directly yielded <b>2</b> without any tractable intermediate <b>1</b>. Structural characterization of the intermediates <b>1a</b>–<b>1c</b> and the corresponding final products <b>2a</b>–<b>2c</b> (R = H, Me, Cl) authenticated their identities, revealing ruthenium-hydride mediated unsymmetrical cleavage of benzofuroxan to hydrogen bonded monodentate 2-nitroanilido (L<sup>1</sup>) in the former and bidentate 2-nitroanilido (L<sup>2</sup>) in the latter. The spectrophotometric monitoring of the transformations of <b>B</b> → <b>1</b> as well as <b>1</b> → <b>2</b> with time and temperature established the first order rate process with associatively activated pathway for both cases. Both <b>1</b> and <b>2</b> exhibited one reversible oxidation and an irreversible reduction within ±1.5 V versus saturated calomel reference electrode in CH<sub>3</sub>CN with slight variation in potential based on substituents in the benzofuroxan framework (R = H, Me, Cl). Spectroscopic (electron paramagnetic resonance and UV–vis) and density functional theory calculations collectively suggested varying contribution of metal based orbitals along with the ligand in the singly occupied molecular orbital of <b>1</b><sup>+</sup> or <b>2</b><sup>+</sup>, ascertaining the noninnocent potential of the in situ generated (L<sup>1</sup>) or (L<sup>2</sup>)

    Revelation of Varying Coordination Modes and Noninnocence of Deprotonated 2,2′-Bipyridine-3,3′-diol in {Os(bpy)<sub>2</sub>} Frameworks

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    The reaction of 2,2′-bipyridine-3,3′-diol (H<sub>2</sub>L) and <i>cis</i>-Os<sup>II</sup>(bpy)<sub>2</sub>­Cl<sub>2</sub> (bpy = 2,2′-bipyridine) results in isomeric forms of [Os<sup>II</sup>(bpy)<sub>2</sub>(HL<sup>–</sup>)]­ClO<sub>4</sub>, [<b>1</b>]­ClO<sub>4</sub> and [<b>2</b>]­ClO<sub>4</sub>, because of the varying binding modes of partially deprotonated HL<sup>–</sup>. The identities of isomeric [<b>1</b>]­ClO<sub>4</sub> and [<b>2</b>]­ClO<sub>4</sub> have been authenticated by their single crystal X-ray structures. The ambidentate HL<sup>–</sup> in [<b>2</b>]­ClO<sub>4</sub> develops the usual N,N bonded five-membered chelate with a strong O–H···O hydrogen bonded situation (O–H···O angle: 160.78°) at its back face. The isomer [<b>1</b>]­ClO<sub>4</sub> however represents the monoanionic O<sup>–</sup>,N coordinating mode of HL<sup>–</sup>, leading to a six-membered chelate with the moderately strong O–H···N hydrogen bonding interaction (O–H···N angle: 148.87°) at its backbone. The isomeric [<b>1</b>]­ClO<sub>4</sub> and [<b>2</b>]­ClO<sub>4</sub> also exhibit distinctive spectral, electrochemical, electronic structural, and hydrogen bonding features. The p<i>K</i><sub>a</sub> values for [<b>1</b>]­ClO<sub>4</sub> and [<b>2</b>]­ClO<sub>4</sub> have been estimated to be 0.73 and <0.2, respectively, thereby revealing the varying hydrogen bonding interaction profiles of O–H···N and O–H···O involving the coordinated HL<sup>–</sup>. The O–H···O group of HL<sup>–</sup> in <b>2</b><sup>+</sup> remains invariant in the basic region (pH 7–12), while deprotonation of O–H···N group of HL<sup>–</sup> in <b>1</b><sup>+</sup> estimates the p<i>K</i><sub>b</sub> value of 11.55. This indeed has facilitated the activation of the exposed O–H···N function in [<b>1</b>]­ClO<sub>4</sub> by the second {Os<sup>II</sup>(bpy)<sub>2</sub>} unit to yield the L<sup>2–</sup> bridged [(bpy)<sub>2</sub>Os<sup>II</sup>(μ-L<sup>2–</sup>)­Os<sup>II</sup>(bpy)<sub>2</sub>]­(ClO<sub>4</sub>)<sub>2</sub> ([<b>3</b>]­(ClO<sub>4</sub>)<sub>2</sub>). However, the O–H···O function in [<b>2</b>]­ClO<sub>4</sub> fails to react with {Os<sup>II</sup>(bpy)<sub>2</sub>}. The crystal structure of [<b>3</b>]­(ClO<sub>4</sub>)<sub>2</sub> establishes the symmetric N,O<sup>–</sup>/O<sup>–</sup>,N bridging mode of L<sup>2–</sup>. On the other hand, the doubly deprotonated L′<sup>2–</sup> (H<sub>2</sub>L′ = 2,2′-biphenol) generates structurally characterized twisted seven-membered O<sup>–</sup>,O<sup>–</sup> bonded chelate (torsion angle >50°) in paramagnetic [Os<sup>III</sup>(bpy)<sub>2</sub>­(L′<sup>2–</sup>)]­ClO<sub>4</sub> ([<b>4</b>]­ClO<sub>4</sub>). The electronic structural aspects of the complexes reveal the noninnocent potential of the coordinated HL<sup>–</sup>, L<sup>2–</sup>, and L′<sup>2–</sup>. The <i>K</i><sub>c</sub> value of 49 for <b>3</b><sup>3+</sup> reveals a class I mixed-valent Os<sup>II</sup>Os<sup>III</sup> state

    Ru-Complex Framework toward Aerobic Oxidative Transformations of β‑Diketiminate and α‑Ketodiimine

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    The impact of the {Ru­(acac)<sub>2</sub>} (acac<sup>–</sup> = acetylacetonate) framework on the transformations of C–H and C–H/C–C bonds of coordinated β-diketiminate and ketodiimine scaffolds, respectively, has been addressed. It includes the following transformations involving {Ru­(acac)<sub>2</sub>} coordinated β-diketiminate in <b>1</b> and ketodiimine in <b>2</b> with the simultaneous change in metal oxidation state: (i) insertion of oxygen into the C­(sp<sup>2</sup>)–H bond of β-diketiminate in <b>1</b>, leading to the metalated ketodiimine in <b>2</b> and (ii) Bronsted acid (CH<sub>3</sub>COOH) assisted cleavage of unstrained C­(sp<sup>2</sup>)–C­(sp<sup>2</sup>)/CN bonds of chelated ketodiimine (<b>2</b>) with the concomitant formation of intramolecular C–N bond in <b>3</b>, as well as insertion of oxygen into the C­(sp<sup>3</sup>)–H bond of <b>2</b> to yield −CHO function in <b>4</b> (−CH<sub>3</sub> → −CHO). The aforesaid transformation processes have been authenticated via structural elucidation of representative complexes and spectroscopic and electrochemical investigations

    Unsymmetric (μ-oxido)/(μ-pyrazolato) and Symmetric (μ-pyrazolato)<sub>2</sub> Bridged Diosmium Frameworks: Electronic Structure and Magnetic Properties

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    The present article deals with the structurally characterized unsymmetric oxido/pyrazolato-bridged [(bpy)<sub>2</sub>Os<sup>III</sup>(μ-oxido)­(μ-pz)­Os<sup>III</sup>­(bpy)<sub>2</sub>]­(ClO<sub>4</sub>)<sub>3</sub> ([<b>1</b>]­(ClO<sub>4</sub>)<sub>3</sub>) and symmetric dipyrazolato-bridged [(bpy)<sub>2</sub>Os<sup>II</sup>(μ-pz)<sub>2</sub>­Os<sup>II</sup>(bpy)<sub>2</sub>]­(ClO<sub>4</sub>)<sub>2</sub> ([<b>2</b>]­(ClO<sub>4</sub>)<sub>2</sub>) (pz = pyrazolato, bpy = 2,2′-bipyridine) complexes with the Os···Os separations of 3.484 and 4.172 Å, respectively. The anti-ferromagnetically coupled Os<sup>III</sup> centers [<i>E</i>(<i>S</i> = 1)-<i>E</i>(BS­(1,1) <i>S</i> = 0) = 322.504 cm<sup>–1</sup>] in <b>1</b><sup>3+</sup> and diamagnetic (<i>S</i> = 0) <b>2</b><sup>2+</sup> exhibit well-resolved <sup>1</sup>H NMR resonances. [<b>1</b>]­(ClO<sub>4</sub>)<sub>3</sub> shows temperature- and magnetic field-dependent paramagnetism at low magnetic field and diamagnetism at high magnetic field. <b>1</b><sup>3+</sup> and <b>2</b><sup>2+</sup> display successive metal-based oxidation processes involving the intermediate mixed-valent states and isovalent congeners: Os<sup>IV</sup>Os<sup>IV</sup> (<b>1</b><sup>5+</sup>)→Os<sup>III</sup>Os<sup>IV</sup> (<b>1</b><sup>4+</sup>)⇌Os<sup>III</sup>Os<sup>III</sup> (<b>1</b><sup>3+</sup>)⇌Os<sup>III</sup>Os<sup>II</sup> (<b>1</b><sup>2+</sup>) and Os<sup>III</sup>Os<sup>III</sup> (<b>2</b><sup>4+</sup>)→Os<sup>II</sup>Os<sup>III</sup> (<b>2</b><sup>3+</sup>)⇌Os<sup>II</sup>Os<sup>II</sup> (<b>2</b><sup>2+</sup>) as well as bpy-centered reductions. The effect of π donor O<sup>2–</sup> and σ/π-donating pz<sup>–</sup> in <b>1</b><sup>3+</sup> and <b>2</b><sup>2+</sup>, respectively, leads to varying oxidation state of the metal ions in the isolated complexes: Os<sup>III</sup>Os<sup>III</sup> versus Os<sup>II</sup>Os<sup>II</sup>. UV–visible–near-IR–electron paramagnetic resonance spectro-electrochemistry and density functional theory (DFT)/time-dependent DFT calculations collectively reveal overlapping of the metal- and ligand (pz, O, bpy)-based frontier orbitals in the delocalized mixed-valent states in <b>1</b><sup>4+</sup> and <b>1</b><sup>2+</sup> with comproportionation constant (<i>K</i><sub>c</sub>) value > 1 × 10<sup>14</sup> as well as in isovalent <b>1</b><sup>3+</sup>, resulting in mixed metal/ligand to metal/ligand near-IR transitions in all the three states. The mixed-valent Os<sup>II</sup>Os<sup>III</sup> state in <b>2</b><sup>3+</sup> exhibits high <i>K</i><sub>c</sub> value of 1 × 10<sup>22</sup> corresponding to a strong electrochemical coupling situation. However, closeness of the bandwidth (Δν<sub>1/2</sub>, 4861 cm<sup>–1</sup>) of broad and weak intervalence charge transfer transition of <b>2</b><sup>3+</sup> at 1360 nm (ε/M<sup>–1</sup> cm<sup>–1</sup>: 490) with the calculated Δν<sub>1/2</sub> of 4121 cm<sup>–1</sup> based on the Hush formula as well as spin-density distributions of Os1: 0.811/0.799, Os2: 0.045/0042, and pz: 0.162/0.173 in <i>meso</i> and <i>rac</i> diastereomeric forms, respectively, attribute its localized class II state

    Ancillary Ligand Control of Electronic Structure in o-Benzoquinonediimine-Ruthenium Complex Redox Series: Structures, Electron Paramagnetic Resonance (EPR), and Ultraviolet−Visible−Near-Infrared (UV-vis-NIR) Spectroelectrochemistry

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    The compounds Ru­(acac)<sub>2</sub>(Q) (<b>1</b>), [Ru­(bpy)<sub>2</sub>(Q)]­(ClO<sub>4</sub>)<sub>2</sub> ([<b>2</b>]­(ClO<sub>4</sub>)<sub>2</sub>), and [Ru­(pap)<sub>2</sub>(Q)]­PF<sub>6</sub> ([<b>3</b>]­PF<sub>6</sub>), containing Q = <i>N,N</i>′-diphenyl-<i>o</i>-benzoquinonediimine and donating 2,4-pentanedionate ligands (acac<sup>–</sup>), π-accepting 2,2<sup>/</sup>-bipyridine (bpy), or strongly <i>π-</i>accepting 2-phenylazopyridine (pap) were prepared and structurally identified. The electronic structures of the complexes and several accessible oxidized and reduced forms were studied experimentally (electrochemistry, magnetic resonance, ultraviolet-visible-near-infrared (UV-vis-NIR) spectroelectrochemistry) and computationally (DFT/TD-DFT) to reveal significantly variable electron transfer behavior and charge distribution. While the redox system <b>1</b><sup>+</sup>–<b>1</b><sup>–</sup> prefers trivalent ruthenium with corresponding oxidation states Q<sup>0</sup>–Q<sup>2–</sup> of the noninnocent ligand, the series <b>2</b><sup>2+</sup>–<b>2</b><sup>0</sup> and <b>3</b><sup>2+</sup>–<b>3</b><sup>–</sup> retain Ru<sup>II</sup>. The bpy and pap co-ligands are not only spectators but can also be reduced prior to a second reduction of Q. The present study with new experimental and computational evidence on the influence of co-ligands on the metal is complementary to a report on the substituent effects in <i>o</i>-quinonediimine ligands [Kalinina et al., <i>Inorg. Chem</i>. <b>2008</b>, <i>47</i>, 10110] and to the discussion of the most appropriate oxidation state formulation Ru<sup>II</sup>(Q<sup>0</sup>) or Ru<sup>III</sup>(Q<sup>• –</sup>)

    Ancillary Ligand Control of Electronic Structure in o-Benzoquinonediimine-Ruthenium Complex Redox Series: Structures, Electron Paramagnetic Resonance (EPR), and Ultraviolet−Visible−Near-Infrared (UV-vis-NIR) Spectroelectrochemistry

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    The compounds Ru­(acac)<sub>2</sub>(Q) (<b>1</b>), [Ru­(bpy)<sub>2</sub>(Q)]­(ClO<sub>4</sub>)<sub>2</sub> ([<b>2</b>]­(ClO<sub>4</sub>)<sub>2</sub>), and [Ru­(pap)<sub>2</sub>(Q)]­PF<sub>6</sub> ([<b>3</b>]­PF<sub>6</sub>), containing Q = <i>N,N</i>′-diphenyl-<i>o</i>-benzoquinonediimine and donating 2,4-pentanedionate ligands (acac<sup>–</sup>), π-accepting 2,2<sup>/</sup>-bipyridine (bpy), or strongly <i>π-</i>accepting 2-phenylazopyridine (pap) were prepared and structurally identified. The electronic structures of the complexes and several accessible oxidized and reduced forms were studied experimentally (electrochemistry, magnetic resonance, ultraviolet-visible-near-infrared (UV-vis-NIR) spectroelectrochemistry) and computationally (DFT/TD-DFT) to reveal significantly variable electron transfer behavior and charge distribution. While the redox system <b>1</b><sup>+</sup>–<b>1</b><sup>–</sup> prefers trivalent ruthenium with corresponding oxidation states Q<sup>0</sup>–Q<sup>2–</sup> of the noninnocent ligand, the series <b>2</b><sup>2+</sup>–<b>2</b><sup>0</sup> and <b>3</b><sup>2+</sup>–<b>3</b><sup>–</sup> retain Ru<sup>II</sup>. The bpy and pap co-ligands are not only spectators but can also be reduced prior to a second reduction of Q. The present study with new experimental and computational evidence on the influence of co-ligands on the metal is complementary to a report on the substituent effects in <i>o</i>-quinonediimine ligands [Kalinina et al., <i>Inorg. Chem</i>. <b>2008</b>, <i>47</i>, 10110] and to the discussion of the most appropriate oxidation state formulation Ru<sup>II</sup>(Q<sup>0</sup>) or Ru<sup>III</sup>(Q<sup>• –</sup>)

    Significant Influence of Coligands Toward Varying Coordination Modes of 2,2′-Bipyridine-3,3′-diol in Ruthenium Complexes

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    The varying coordination modes of the ambidentate ligand 2,2′-bipyridine-3,3′-diol (H<sub>2</sub>L) in a set of ruthenium complexes were demonstrated with special reference to the electronic features of the coligands, including σ-donating acac<sup>–</sup> (= acetylacetonate) in Ru<sup>III</sup>(acac)<sub>2</sub>(HL<sup>–</sup>) (<b>1</b>), strongly π-accepting pap (= 2-phenylazopyridine) in Ru<sup>II</sup>(pap)<sub>2</sub>(L<sup>2–</sup>) (<b>2</b>)/[(pap)<sub>2</sub>Ru<sup>II</sup>(μ-L<sup>2–</sup>)­Ru<sup>II</sup>­(pap)<sub>2</sub>]­(ClO<sub>4</sub>)<sub>2</sub> ([<b>4</b>]­(ClO<sub>4</sub>)<sub>2</sub>), and reported moderately π-accepting bpy (= 2,2′-bypiridine) in [Ru<sup>II</sup>(bpy)<sub>2</sub>­(HL<sup>–</sup>)]­PF<sub>6</sub> ([<b>5</b>]­PF<sub>6</sub>)/[(bpy)<sub>2</sub>Ru­(μ-L<sup>2–</sup>)­Ru­(bpy)<sub>2</sub>]­(PF<sub>6</sub>)<sub>2</sub> ([<b>7</b>]­(PF<sub>6</sub>)<sub>2</sub>). The single-crystal X-ray structures reveal that, in paramagnetic and electron paramagnetic resonance active <b>1</b> and reported diamagnetic [<b>5</b>]­PF<sub>6</sub>, nearly planar monoanionic HL<sup>–</sup> coordinates to the metal ion via the <i>N</i>,<i>N</i> donors forming a five-membered chelate ring with hydrogen-bonded O–H···O function at the backbone of the ligand framework, as has also been reported in other metal complexes. However, structurally characterized diamagnetic <b>2</b> represents O<sup>–</sup>,O<sup>–</sup> bonded seven-membered chelate of fully deprotonated but twisted L<sup>2–</sup>. The nonplanarity of the coordinated L<sup>2–</sup> in <b>2</b> does not permit the second metal fragment {Ru­(pap)<sub>2</sub>} or {Ru­(bpy)<sub>2</sub>} or {Ru­(acac)<sub>2</sub>} to bind with the available N,N donors at the back face of L<sup>2–</sup>. Further, the deprotonated form of the model ligand 2,2′-biphenol (H<sub>2</sub>L′) yields Ru<sup>II</sup>(pap)<sub>2</sub>(L′<sup>2–</sup>) (<b>3</b>); its crystal structure establishes the expected O<sup>–</sup>,O<sup>–</sup> bonded seven-membered chelate of nonplanar L′<sup>2–</sup> as in reported Ru<sup>II</sup>(bpy)<sub>2</sub>(L′<sup>2–</sup>) (<b>6</b>), although {Ru­(acac)<sub>2</sub>} metal precursor altogether fails to react with H<sub>2</sub>L′. All attempts to make diruthenium complex from {Ru­(acac)<sub>2</sub>} and H<sub>2</sub>L failed; however, the corresponding {Ru­(pap)<sub>2</sub><sup>2+</sup>} derived dimeric [<b>4</b>]­(ClO<sub>4</sub>)<sub>2</sub> was structurally characterized. It establishes the symmetric N,O<sup>–</sup>/N,O<sup>–</sup> bridging mode of nonplanar L<sup>2–</sup> as in reported [<b>7</b>]­(PF<sub>6</sub>)<sub>2</sub>. Besides structural and spectroscopic characterization of the newly developed complexes, the ligand (HL<sup>–</sup>, L<sup>2–</sup>, L′<sup>2–</sup>, pap)-, metal-, or mixed metal–ligand-based accessible redox processes in <b>1</b><sup><i>n</i></sup> (<i>n</i> = +2, +1, 0, −1), <b>2</b><sup><i>n</i></sup>/<b>3</b><sup><i>n</i></sup> (<i>n</i> = +2, +1, 0, −1, −2), and <b>4</b><sup><i>n</i></sup> (<i>n</i> = +4, +3, +2, +1, 0, −1) were analyzed in conjunction with density functional theory calculations
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