Volume 45 Number 27 21 July 2016 Pages 10853–11200 Dalton Transactions An international journal of inorganic chemistry www.rsc.org/dalton ISSN 1477-9226 PAPER Lisa McElwee-White et al. Synthesis and evaluation of 2--diketonate and -ketoesterate tungsten(VI) oxo-alkoxide complexes as precursors for chemical vapor deposition of WOx thin films Dalton Transactions View Article Online Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. PAPER Cite this: Dalton Trans., 2016, 45, 10897 View Journal | View Issue Synthesis and evaluation of κ2-β-diketonate and β-ketoesterate tungsten(VI) oxo-alkoxide complexes as precursors for chemical vapor deposition of WOx thin films† Richard O. Bonsu,‡a Duane C. Bock,‡a Hankook Kim,‡b Roman Y. Korotkov,c Khalil A. Abboud,a Timothy J. Andersonb and Lisa McElwee-White*a Reactions of [WO(OR)4]x (x = 1, 2) complexes with bidentate ligands (LH = acacH, tbacH, dpmH, tbpaH) afforded complexes 1–13: [WO(OCH3)3(acac) (1); WO(OCH2CH3)3(acac) (2); WO(OCH(CH3)2)3(acac) (3); WO(OCH3)3(tbac) (4); WO(OCH2CH3)3(tbac) (5); WO(OCH(CH3)2)3(tbac) (6); WO(OCH2CH3)3(dpm) (7); WO(OCH(CH3)2)3(dpm) (8); WO(OCH2C(CH3)3)3(acac) (9); WO(OCH2C(CH3)3)3(tbac) (10); WO(OCH2C(CH3)3)3(dpm) (11); WO(OCH2C(CH3)3)3(tbpa) (12); WO(OC(CH3)3)3(tbac) (13)]. The synthesis is facilitated by the lability of the bridging ligands of the [WO(OR)4]2 complexes in solution, which provides a pathway for exchange of L with an alkoxide ligand. Thermogravimetric analysis and the conditions for sublimation or distillation of 1–13 demonstrate that they have sufficient vapor pressure and thermal stability for Received 19th March 2016, Accepted 29th April 2016 DOI: 10.1039/c6dt01078d www.rsc.org/dalton volatilization in a conventional Chemical Vapor Deposition (CVD) reactor. High solubility in hydrocarbon and ether solvents establishes that the complexes are also potential candidates for Aerosol-Assisted Chemical Vapor Deposition (AACVD). AACVD from 10 on ITO or bare glass resulted in growth of continuous, dense and amorphous thin films of substoichiometric WOx between 250–350 °C and nanorods of W18O49 above 350 °C. Introduction Thin films of tungsten oxide are attractive materials for applications in organic and hybrid electronic devices. Notable are anodic and cathodic charge extraction layers in Organic Light Emitting Diodes (OLEDs),1,2 anodic layers in near-infrared absorbing dye-based photovoltaics,3–6 electrochromic layers in smart windows,7–9 energy storage compartments in photovoltaics, 10 photoanodes for photoelectrocatalysis, 11 and a Department of Chemistry, University of Florida, Gainesville, FL, 32611-7200 USA. E-mail: [email protected] b Department of Chemical Engineering, University of Florida, Gainesville, FL, 32611-6005 USA c Arkema Inc., 900 First Ave., King of Prussia, PA, 19406 USA † Electronic supplementary information (ESI) available: Synthesis of 11a. Crystallographic structure determination of 11a. 1H NMR and 13C NMR spectra of complexes 1–13 and 19. Molecular geometries of 11 and 11a. Table of bond distances, bond angles, atomic coordinates, and equivalent isotropic displacement parameters for 1, 10, 11, and 11a. Thermal behaviours of 1, 2, and 5–13 based on TG measurements. Relative abundances for positive ion DIPCI mass spectra of complexes 1, 2, and 10–13. Deconvoluted XPS spectra of films grown from 10 at 200 °C and 500 °C. Selected properties of 1–13. CCDC 1454825–1454828. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c6dt01078d ‡ These authors made equal contributions to the work. This journal is © The Royal Society of Chemistry 2016 components in chemical and biological sensing devices.12,13 The versatility of WOx for applications is derived from its high work function, visible light transparency, electrical and mechanical robustness, large surface area-to-volume ratio of vapor phase deposits and electrochromism. Although WO3 itself contains a d0 transition metal in its fully oxidized W6+ state, the capability of chemical vapor deposition (CVD) to produce substoichiometric WOx material with partial occupation of W in lower oxidation states (W5+ and W4+) offers the possibility of controlling the electrical properties of the material.14,15 Deposition by CVD can provide access to conformal, highly uniform and robust layers of WOx thin films for application in a variety of organic and inorganic devices.16–21 Precursors possessing high volatility are required for CVD processes that volatilize the precursors through evaporation or sublimation.22–24 However, in aerosol-assisted chemical vapor deposition (AACVD), solutions of the precursors are aerosolized, replacing the need for volatility in the precursor itself with a requirement for solubility and stability in a suitably volatile organic solvent.16,25–28 Injection of the precursor aerosol mist into the reactor chamber not only promotes higher mass transport of the precursor leading to high material growth rate but can allow the deposition reaction to run at moderate temperatures that are cost effective.25,28,29 Dalton Trans., 2016, 45, 10897–10908 | 10897 View Article Online Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Paper Although the oxo-alkoxide complexes [WO(OR)4]n have been used as precursors for CVD growth of WOx materials, they are air- and water-sensitive.30,31 In our hands, NMR samples of WO(OtBu)4 were observed to decompose in solution after 2 hours of exposure to air. Fluorinated derivatives of WO(OR)4, such as WO(OCH2CF3)4,32 WO[OC(CH3)2CF3]4 and WO[OC(CF3)2CH3]4 33,34 have been reported to serve as precursors for growth of WOx films and nanostructures but there is still incentive to prepare and test additional precursors with greater air- and water-stability and whose syntheses do not require fluorinated starting materials. Compounds of the type [WO(OR)3L] (R = tBu, iPr, L = acac, hfac) have been previously synthesized and used for growth of electrochromic WOx materials by LPCVD.31 The thermal behavior and vapor pressure of two closely related WO(OtBu)3L precursors possessing β-ketoesterate ligands (L = methyl acetoacetate and ethyl acetoacetate) were examined in 2008.35 In both instances, the WO(OR)3L complexes were readily obtained from the corresponding monomeric oxo alkoxide complex [WO(OtBu)4]. Precursors of the type [WO(OR)3L] (L = acac, dpm, tbac) with R groups that are less sterically bulky than isopropyl have not been reported. Due to the interest in continued development of precursors for deposition of high quality WOx thin films for electronic and optoelectronic device applications, we have synthesized a series of [WO(OR)3L] complexes with less bulky alkoxide ligands (R = Me, Et, iPr, Np, L = acac, dpm, tbac, tbpa) and prescreened them as potential precursors for deposition of WOx materials. CVD experiments with WO(OCH2C(CH3)3)3(tbac) (10) resulted in growth of WOx films and nanostructures, with the morphology of the deposited material depending on the growth temperature. Experimental details General procedures All reactions were carried out under an atmosphere of dry nitrogen using either glovebox or standard Schlenk techniques. All chemicals used were of reagent grade. Methylene chloride and toluene (Fisher Scientific) were purified using an MBraun MB-SP solvent purification system and stored over activated 3 Å molecular sieves for at least 48 h prior to experiments. Diethylether and tetrahydrofuran were dried using sodium/benzophenone, distilled, and stored over activated 3 Å molecular sieves for at least 48 h prior to experiments. Hexamethyldisiloxane, acetylacetone (Hacac), tert-butylacetylacetonate (Htbac), methanol, ethanol, isopropanol, neopentanol (Sigma-Aldrich), dipivaloylmethane (Hdpm, Matrix Scientific) and benzene-d6 (Cambridge Isotopes) were stored over 4 Å molecular sieves for at least 48 h before use. tert-Butylpivaloylacetate (Htbpa) was synthesized and characterized as reported in the literature.36 WCl6, anhydrous diethylamine (SigmaAldrich) and anhydrous ammonia (AirGas) were used as received. WOCl4 37 (14), WO[OC(CH3)3]4 37 (15), [WO(OCH3)4]2 (16), [WO(OCH2CH3)4]2 (17) and [WO(OCH(CH3)2)4]2 38 (18) were synthesized and characterized according to literature 10898 | Dalton Trans., 2016, 45, 10897–10908 Dalton Transactions procedures. Compound 19 was prepared following the same route as compounds 16–18. NMR spectra were recorded on a Varian Mercury 300BB (300 MHz) spectrometer using residual protons from deuterated solvents for reference. Elemental analyses were performed at the University of Florida or by Complete Analysis Laboratory Inc. (Parsippany, NJ). The mass spectrometry was conducted on a Thermo Scientific Trace GC DSQ equipped with 70 eV electron ionization (EI), direct insertion probe (DIP) using chemical ionization (CI) with methane as the reagent gas or an Agilent 6200 ESI-TOF mass spectrometer using DART-TOF mode of operation. WO(OCH3)3(acac) (1). In the glovebox, [WO(OCH3)4]2 (16, 1.54 mmol, 1.00 g) was transferred into a 50 mL Schlenk flask containing a stir bar. THF (30 mL) was added and stirred to produce a clear yellow solution. Acetylacetone (3.09 mmol, 0.320 mL, 0.312 g) was added dropwise to the stirring solution of 16 in THF. A reflux condenser was fitted to the Schlenk flask and the entire reaction set-up was moved to the Schlenk line and refluxed for 3 h. The solution became clear and brighter, approaching a yellowish-orange color. Volatiles were removed under dynamic vacuum and the yellowish-orange solid residue was kept under vacuum for about 3 h to dry. The product was sublimed at 60–65 °C (100–150 mTorr) to afford the product as yellowish-white crystals in 77% yield (0.86 g). 1 H NMR (C6D6, 25 °C): δ 5.03 (s, 1H, COCHCO), 4.68 (s, 3H, OCH3), 4.45 (s, 6H, OCH3), 1.66 (s, 3H CH3), 1.60 (s, 3H, CH3). 13 C{1H} NMR (C6D6, 25 °C): δ 194.60 (OC(CH3)CH), 186.80 (OC(CH3)CH), 104.68 (CHC(CH3)O), 65.80 (OCH3), 63.65 (OCH3), 27.65 (CH3), 26.43 (CH3). Anal. Calcd for WO6C8H16: C, 24.51; H, 4.11. Found: C, 24.63; H, 3.96%. Crystals for single crystal X-ray crystallographic determination were obtained from the sublimate. WO(OCH2CH3)3(acac) (2). Compound 2 was synthesized following the same procedure as used for 1. Starting with [WO(OCH2CH3)4]2 (17, 1.32 mmol, 1.00 g) and Hacac (2.63 mmol, 0.27 mL, 0.263 g), a yellowish-orange moist semi-solid was obtained after removal of the volatiles under vacuum. This residue was sublimed at 60–65 °C (150–200 mTorr) to afford an orange semi-solid product in 63% yield (0.72 g). 1H NMR (C6D6, 25 °C): δ 5.15 (s, 1H, COCHCO), 5.00 (q, 2H, OCH2CH3, J = 7.0 Hz), 4.73 (dq, 2H, OCH2CH3, J = 10.8, 7.0 Hz), 4.68 (dq, 2H, OCH2CH3, J = 10.8, 7.0 Hz), 1.73 (s, 3H, CH3), 1.66 (s, 3H, CH3), 1.28 (t, 3H, CH3CH2O, J = 7.0 Hz), 1.19 (t, 6H, CH3CH2O, J = 7.0 Hz). 13C{1H} NMR (C6D6, 25 °C): δ 193.27 (OC(CH3)CH), 186.22 (OC(CH3)CH), 103.78 (CHC(CH3)O), 74.25 (OCH2CH3), 71.55 (OCH2CH3), 27.02 (CH3), 25.92 (CH3), 18.61 (CH3CH2O), 17.60 (CH3CH2O). Anal. Calcd for WO6C11H22: C, 30.43; H, 5.11. Found: C, 27.64; H, 4.67%. WO[OCH(CH3)2]3(acac) (3). Compound 3 was synthesized following the same procedure as used for 1. Starting with [WO(OCH(CH3)2)4]2 (18, 1.15 mmol, 1.00 g) and Hacac (2.29 mmol, 0.25 mL, 0.23 g) a yellow liquid residue was obtained after removal of the volatiles. This residue was vacuum distilled at 60–65 °C (150–200 mTorr) to afford a yellowish-orange liquid in 53% yield (0.58 g). 1H NMR (C6D6, 25 °C): δ 5.35 (sp, 1H, OCH(CH3)2, J = 6.2 Hz), 5.16 (s, 1H, COCHCO), 5.15 (sp, 2H, This journal is © The Royal Society of Chemistry 2016 View Article Online Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Dalton Transactions OCH(CH3)2, J = 6.2 Hz), 1.74 (s, 3H, CH3), 1.69 (s, 3H, CH3), 1.37 (d, 6H, (CH3)2CHO, J = 6.6 Hz), 1.30 (d, 6H, (CH3)2CHO, J = 6.2 Hz), 1.20 (d, 6H, (CH3)2CHO, J = 6.2 Hz). 13C{1H} NMR (C6D6, 25 °C): δ 192.84 (OC(CH3)CH), 186.40 (OC(CH3)CH), 103.82 (CHC(CH3)O), 81.47 (OCH(CH3)2), 78.59 (OCH(CH3)2), 27.34 (CH3), 26.39 (CH3), 25.70 ((CH3)2CHO), 25.50 ((CH3)2CHO), 24.50 ((CH3)2CHO). Anal. Calcd for WO6C14H28: C, 35.31; H, 5.93. Found: C, 35.19; H, 6.01%. WO(OCH3)3(tbac) (4). Complex 4 was synthesized following the same procedure as used for 1. Starting with [WO(OCH3)4]2 (16, 1.54 mmol, 1.00 g) and Htbac (3.08 mmol, 0.52 mL, 0.50 g) a yellowish-orange liquid residue was obtained after removal of the volatiles under vacuum. The crude product was vacuum distilled at 70–75 °C (200–250 mTorr) to afford a yellowish-orange oil in 68% (0.95 g) yield. 1H NMR (C6D6, 25 °C): 4.90 (s, 1H, CHC(CH3)O), 4.80 (s, 3H, OCH3), 4.39 (s, 3H, OCH3), 1.72 (s, 3H, CH3), 1.32 (s, 9H, C(CH3)3). 13 C{1H} NMR (C6D6, 25 °C): δ 181.81 (C(CH3)CH), 173.40 (COC(CH3)3CH), 92.82 (CHCOC(CH3)), 82.74 ((CCH3)3), 65.79 (OCH3), 63.21 (OCH3), 28.69 ((CH3)3C), 25.46 (CH3). Anal. Calcd for WO7C11H22: C, 29.35; H, 4.93. Found: C, 30.09; H, 5.03%. WO(OCH2CH3)3(tbac) (5). Complex 5 was synthesized following the same procedure as used for 1. Starting with [WO(OCH2CH3)4]2 (17, 1.32 mmol, 1.00 g) and Htbac (2.63 mmol, 0.45 mL, 0.43 g) a yellowish-orange liquid residue was obtained after removal of the volatiles under vacuum. The crude liquid was vacuum distilled from 60 to 65 °C (150–200 mTorr) to afford a yellowish-orange oil in 51% yield (0.66 g). 1H NMR (C6D6, 25 °C): δ 4.94 (s, 1H, CHC(CH3)O), 4.93 (q, 2H, OCH2CH3, J = 7.0 Hz), 4.92 (dq, 2H, OCH2CH3, J = 10.8, 7.0 Hz), 4.87 (dq, 2H, OCH2CH3, J = 10.8, 7.0 Hz), 1.73 (s, 3H, CH3), 1.35 (s, 9H, C(CH3)3), 1.27 (t, 3H, CH3CH2O, J = 7.0 Hz), 1.18 (t, 6H, CH3CH2O, J = 7.0 Hz). 13C{1H} NMR (C6D6, 25 °C): δ 182.40 (C(CH3)CH), 173.81 (CO(CH3)3CH), 92.76 (CHCO(CH3)), 82.69 (C(CH3)3), 74.74 (OCH2), 71.77 (OCH2), 29.12 ((CH3)3C), 25.93 (CH3), 19.17 (CH3CH2O), 18.49 (CH3CH2O). Anal. Calcd for WO7C14H28: C, 34.16; H, 5.73. Found: C, 34.12; H, 5.73%. WO[OCH(CH3)2]3(tbac) (6). Complex 6 was synthesized following the same procedure as used for 1. Starting with [WO(OCH(CH3)2)4]2 (18, 1.32 mmol, 1.00 g) and Htbac (2.29 mmol, 0.40 mL, 0.37 g) a yellowish-orange liquid residue was obtained after removal of the volatiles under vacuum. The crude liquid was vacuum distilled at 60–65 °C (150–200 mTorr) to afford a yellowish-orange oil in a yield of 0.68 g (55%). 1H NMR (C6D6, 25 °C): δ 5.24 (sp, 1H, OCH(CH3)2, J = 6.2 Hz), 5.10 (sp, 2H, OCH(CH3)2, J = 6.2 Hz), 4.97 (s, 1H, CHCO(CH3)), 1.73 (s, 3H, CH3), 1.39 (s, 9H, C(CH3)3), 1.39 (d, 6H, (CH3)2CHO, J = 5.7 Hz), 1.33 (d, 6H, (CH3)2CHO, J = 5.9 Hz), 1.22 (d, 6H, (CH3)2CHO, J = 6.2 Hz). 13C{1H} NMR (C6D6, 25 °C): δ 182.24 (C(CH3)CH), 173.46 (CO(CH3)3CH), 91.95 (CHCO(CH3)), 82.02 (C(CH3)3), 80.98 (OCH(CH3)2), 77.78 (OCH(CH3)2), 28.91 ((CH3)3C), 25.81 (CH3), 25.72 ((CH3)2CHO), 25.17 ((CH3)2CHO), 24.54 ((CH3)2CHO). Anal. Calcd for WO7C17H34: C, 38.22; H, 6.41. Found: C, 38.09; H, 6.54%. This journal is © The Royal Society of Chemistry 2016 Paper WO(OCH2CH3)3(dpm) (7). Complex 7 was synthesized following the same procedure as used for 1. Starting with [WO(OCH2CH3)4]2 (17, 1.32 mmol, 1.00 g) and Hdpm (2.63 mmol, 0.58 mL, 0.51 g), an orange liquid was obtained after removal of volatiles under vacuum. The crude liquid was vacuum distilled at 70–80 °C (300–350 mTorr) to afford a clear orange liquid in a yield of 0.8 g (60%). 1H NMR (C6D6, 25 °C): δ 5.83 (s, 1H, CHC(CH3)O), 4.98 (q, 2H, OCH2CH3, J = 7.0 Hz), 4.72 (dq, 2H, OCH2CH3, J = 10.8, 7.0 Hz), 4.68 (dq, 2H, OCH2CH3, J = 10.8, 7.0 Hz), 1.28 (t, 3H, CH3CH2O, J = 7.0 Hz), 1.16 (t, 6H, CH3CH2O, J = 7.0 Hz), 1.13 (s, 9H, C(CH3)3), 1.07 (s, 9H, C(CH3)3). 13C{1H} NMR (C6D6, 25 °C): δ 203.22 (OCC(CH3)3CH), 196.40 (OCC(CH3)3CH), 94.30 (CHCOC(CH3)3), 73.19 (OCH2CH3), 71.02 (OCH2CH3), 41.25 (C(CH3)3), 40.78 (C(CH3)3), 28.39 (C(CH3)3), 27.97 (C(CH3)3), 18.87 (CH3CH2O), 17.72 (CH3CH2O). Anal. Calcd for WO6C17H34: C, 39.40; H, 6.61. Found: C, 39.18; H, 6.66%. WO[OCH(CH3)2]3(dpm) (8). Complex 8 was synthesized following the same procedure as used for 1. Starting with [WO(OCH(CH3)2)4]2 (18, 1.15 mmol, 1.00 g) and Hdpm (2.29 mmol, 0.50 mL, 0.44 g), an orange liquid was obtained after removal of volatiles under vacuum. The crude liquid was vacuum distilled at 70–80 °C (250–300 mTorr) to afford a clear orange liquid in a yield of 0.72 g (55%). 1H NMR (C6D6, 25 °C): δ 5.83 (s, 1H, CHC(CH3)O), 5.35 (sp, 1H, OCH(CH3)2 J = 6.2 Hz), 5.04 (sp, 2H, OCH(CH3)2, J = 6.2 Hz), 1.38 (d, 6H, (CH3)2CHO, J = 6.6 Hz), 1.32 (d, 6H, (CH3)2CHO, J = 6.2 Hz), 1.18 (d, 6H, (CH3)2CHO, J = 6.2 Hz), 1.15 (s, 9H, C(CH3)3), 1.09 (s, 9H, C(CH3)3). 13C{1H} NMR (C6D6, 25 °C): δ 202.70 (OCC(CH3)3CH), 196.64 (OCC(CH3)3CH), 94.36 (CHCOC(CH3)3), 80.25 (OCH(CH3)2), 77.27 (OCH(CH3)2), 41.40 (C(CH3)3), 41.04 (C(CH3)3), 28.72 (C(CH3)3), 28.11 (C(CH3)3), 25.98 ((CH3)2CHO), 25.44 ((CH3)2CHO), 24.62 ((CH3)2CHO). Anal. Calcd for WO5C21H42: C, 42.87; H, 7.20. Found: C, 42.78; H, 7.28%. WO[OCH2C(CH3)3]3(acac) (9). Complex 9 was synthesized following the same procedure as used for 1. Starting with [WO(OCH2C(CH3)3)4]2 (19, 0.910 mmol, 1.00 g) and Hacac (0.910 mmol, 0.10 mL, 0.09 g), a bright yellow-orange liquid was obtained after removal of volatiles under vacuum. The liquid residue was vacuum distilled at 60–65 °C (200–250 mTorr) to afford a yellow-orange oil in 52% (0.53 g) yield. 1H NMR (C6D6, 25 °C): δ 5.11 (s, 1H, CHC(CH3)O), 4.78 (s, 2H, OCH2), 4.47 (d, 2H, OCH2, J = 10.5 Hz), 4.43 (d, 2H, OCH2, J = 10.6 Hz), 1.74 (s, 3H, CH3), 1.68 (s, 3H, CH3), 1.06 (s, 9H, C(CH3)3), 0.97 (s, 18H, C(CH3)3). 13C{1H} NMR (C6D6, 25 °C): δ 193.89 (OC(CH3)CH), 186.34 (OC(CH3)CH), 104.36 (CHC(CH3)O), 89.06 (OCH2), 87.09 (OCH2), 35.47 (C(CH3)3), 35.21 (C(CH3)3), 26.43, 26.41 (CH3)3C). Anal. Calcd for WO6C21H42: C, 42.87; H, 7.20. Found: C, 42.88; H, 7.16%. WO[OCH2C(CH3)3]3(tbac) (10). Complex 10 was synthesized following the same procedure as used for 1. Starting with [WO(OCH2C(CH3)3)4]2 (19, 0.910 mmol, 1.00 g) and Htbac (0.910 mmol, 0.20 mL, 0.18 g), a yellow-orange moist semisolid was obtained upon removal of volatiles under vacuum. The residue was sublimed at 55–60 °C (150–200 mTorr) to yield a pale orange waxy crystalline solid in a yield of 0.62 g Dalton Trans., 2016, 45, 10897–10908 | 10899 View Article Online Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Paper (55%). 1H NMR (C6D6, 25 °C): δ 4.95 (s, 1H, CHC(CH3)O), 4.75 (s, 2H, OCH2), 4.47 (d, 2H, OCH2, J = 10.6 Hz), 4.43 (d, 2H, OCH2, J = 10.6 Hz), 1.75 (s, 3H, CH3), 1.42 (s, 9H, OC(CH3)3), 1.06 (s, 9H, C(CH3)3), 0.98 (s, 18H, C(CH3)3). 13C {1H} NMR (C6D6, 25 °C): δ 182.36 (C(CH3)CH), 173.79 (COC(CH3)3CH), 92.80 (CHCO(CH3)3), 89.78 (OCH2), 86.80 (OCH2), 82.59 (OC(CH3)3), 35.23 (C(CH3)3), 29.20 (C(CH3)3), 27.39 ((CH3)3C), 27.33 (CH3). Anal. Calcd for WO7C24H48: C, 44.67; H, 7.50. Found: C, 44.49; H, 7.32%. Crystals for single crystal X-ray crystallographic determination were obtained from the sublimate. WO[OCH2C(CH3)3]3(dpm) (11). Complex 11 was synthesized following the same procedure as used for 1. Starting with [WO(OCH2C(CH3)3)4]2 (19, 0.910 mmol, 1.00 g) and Hdpm (0.910 mmol, 0.20 mL, 0.18 g), the yellow-cream dense residue obtained after removal of volatiles was sublimed at 90–100 °C (300–350 mTorr) to yield a cream solid in a yield of 0.62 g (55%). 1H NMR (C6D6, 25 °C): δ 5.83 (s, 1H, CHC(CH3)O), 4.67 (s, 2H, OCH2), 4.38 (d, 2H, OCH2, J = 10.6 Hz), 4.35 (d, 2H, OCH2, J = 10.6 Hz), 1.12 (s, 9H, (CH3)3), 1.08 (s, 9H, (CH3)3), 1.00 (s, 9H, C(CH3)3, 0.89 (s, 18H, C(CH3)3. 13C{1H} NMR (C6D6, 25 °C): δ 203.23 (OCC(CH3)3CH), 196.58 (OCC(CH3)3CH), 94.73 (CHCOC(CH3)3), 87.79 (OCH2), 86.34 (OCH2), 41.62 (C(CH3)3), 41.14 (C(CH3)3), 34.99 (C(CH3)3CH2O), 34.87 (C(CH3)3CH2O), 28.89 ((CH3)3C), 28.36 ((CH3)3C), 27.11 (CH3)3CCH2O), 27.01 (CH3)3CCH2O). Anal. Calcd for WO6C26H52: C, 48.45; H, 8.13. Found: C, 48.14; H, 8.40%. Crystals for X-ray crystallographic study were grown by cooling a toluene solution of 11 to −3 °C. WO[OCH2C(CH3)3]3(tbpa) (12). Complex 12 was synthesized following the same procedure as used for 1. Starting with WO(OCH2C(CH3)3)4 (19, 1.79 mmol, 0.984 g) and Htbpa (1.80 mmol, 0.360 g), the yellow-white solid obtained after removal of volatiles was sublimed at 90–100 °C (200–250 mTorr) to yield a white solid in a yield of 0.456 g (39%). 1H NMR (C6D6, 25 °C): δ 5.27 (s, 1H, CHC(CH3)O), 4.79 (s, 2H, OCH2), 4.55 (d, 2H, OCH2, J = 10.5 Hz), 4.44 (d, 2H, OCH2, J = 10.5 Hz), 1.45 (s, 9H, COOC(CH3)3), 1.16 (s, 9H, COC(CH3)3), 1.10 (s, 9H, C(CH3)3), 1.03 (s, 18H, C(CH3)3). 13 C{1H} NMR (C6D6, 25 °C): δ 191.90 (OCC(CH3)3CH), 174.68 (OCC(CH3)3CH), 89.64 (CHCOC(CH3)3), 88.96 (OCH2), 86.67 (OCH2), 82.60 (OC(CH3)3), 40.45 (C(CH3)3), 35.61 (C(CH3)3CH2O), 35.27 (C(CH3)3CH2O), 29.17 ((CH3)3C), 29.11 ((CH3)3C), 27.43 ((CH3)3CH2O), 27.33 ((CH3)3CH2O). Anal. Calcd for WO7C26H52: C, 47.28; H, 7.94. Found: C, 47.28; H, 8.10%. WO[OC(CH3)3]3(tbac) (13). In the glovebox, WO[OC(CH3)3]4 (15, 2.03 mmol, 1.00 g) was dissolved in THF (40 mL) inside a 100 mL Schlenk flask and tbacH, (2.03 mmol, 0.337 mL) dissolved in THF (20 mL), was placed inside an addition funnel fitted to the Schlenk flask. The Schlenk flask was placed in an ice bath for 30 min. The THF solution of Htbac was added dropwise to the stirring solution of 15 in the Schlenk flask. After the addition, the yellowish mixture was kept in the ice bath for additional 30 min, after which the mixture was allowed to warm to room temperature and stirred for the next 12 h. Volatiles were removed under vacuum to obtain a pale yellow waxy solid which was sublimed overnight between 10900 | Dalton Trans., 2016, 45, 10897–10908 Dalton Transactions 55–70 °C (350 mTorr) to afford white needles in a yield of 0.46 g (39%). 1H NMR (C6D6, 25 °C): δ 5.03 (s, 1H, CHC(CH3) O), 1.74 (s, 3H, CH3), 1.54 (s, 9H, COC(CH3)3), 1.47 (s, 18H, OC(CH3)3), 1.43 (s, 9H, OC(CH3)3). 13C{1H} NMR (C6D6, 25 °C): δ 181.53 (C(CH3)CH), 174.07 (C(CH3)CH), 90.45 (CHCOC(CH3)), 81.44 ((CCH3)3), 80.98 ((CCH3)3), 30.98 ((CH3)3C), 30.32 ((CH3)3C)), 28.62 ((CH3)3C)), 25.78 (CH3). Anal. Calcd for WO7C19H38: C, 41.68; H, 7.00. Found: C, 41.49; H, 7.21%. WO(OCH2C(CH3)3)4 (19). In the glovebox, WOCl4 (14, 8.77 mmol, 3.00 g) was transferred into a 500 mL Schlenk flask charged with a stir bar. THF (60 mL) was slowly added and stirred into an orange solution. Neopentyl alcohol (35.1 mmol, 3.10 g) was dissolved in a total of 20 mL THF and added dropwise to the solution of 14 in THF. An immediate change in color from orange to pale green was observed. A dry ice condenser was fitted to the Schlenk flask and the entire setup was transferred to a Schlenk line in a fume hood. The apparatus was purged with argon, after which the condenser was filled with dry ice and acetone and allowed to sit for 20 min. To the stirring mixture of 14 and neopentyl alcohol in THF, anhydrous diethylamine (10.0 mL, 4.5 equiv.) was added dropwise from a syringe. A vigorous reaction ensued and was accompanied by formation of a white precipitate, which caused the reaction medium to become viscous. The mixture was stirred for 30 min after addition of the diethylamine. The volatiles were removed under vacuum to obtain a whitish residue, which was transferred into the glovebox. The residue was dissolved in toluene, stirred and filtered under Celite to yield a pale yellow filtrate. The filtrate was transferred to the Schlenk line and the solvent was removed under vacuum. The product was kept under vacuum overnight to obtain 19 as a whitish-cream solid. Yield 3.82 g, 79%. 1H NMR (C6D6, 25 °C): 4.40 (s, 8H, CH2), 0.98 (s, 36H, CH3). 13C{1H} NMR (C6D6, 25 °C): δ 86.29 (OCH2), 34.34 (C(CH3)3), 26.29 (C(CH3)3). MS (DART-TOF) m/z calcd for [WO5C20H45]+ 549.2776, Found 549.2780. Crystallographic structure determination of 1, 10 and 11 X-Ray intensity data for 1, 10 and 11 were collected at 100 K on a Bruker DUO diffractometer using Mo Kα radiation (λ = 0.71073 Å) and an APEXII CCD area detector. Raw data frames were read by program SAINT39,40 and integrated using 3D profiling algorithms. The resulting data were reduced to produce hkl reflections and their intensities and estimated standard deviations. The data were corrected for Lorentz and polarization effects and numerical absorptions corrections were applied based on indexed and measured faces. The structure of 1 was solved and refined in SHELXTL6.1,39 using full-matrix least-squares refinement. The non-H atoms were refined with anisotropic thermal parameters and all of the H atoms were calculated in idealized positions and refined riding on their parent atoms. In the final cycle of refinement of 1, 2692 reflections (of which 2128 are observed with I > 2σ(I)) were used to refine 141 parameters and the resulting R1, wR2 and S (goodness of fit) were 1.15%, 2.39% and 1.088, respectively. The refinement was carried out by minimizing This journal is © The Royal Society of Chemistry 2016 View Article Online Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Dalton Transactions the wR2 function using F2 rather than F values. R1 is calculated to provide a reference to the conventional R value but its function is not minimized. The structure of 10 was solved and refined in SHELXTL6.1,39 using full-matrix least-squares refinement. The non-H atoms were refined with anisotropic thermal parameters and all of the H atoms were calculated in idealized positions and refined riding on their parent atoms. The W complex has two disordered regions. The alkyl group on O2 is completely disordered and refined in two parts. Atoms C1–C5 are refined against atoms C1′–C5′ along with their protons. In the second disorder, atoms C21–C25 and C21′–C25′, except C22 which is common to both parts, make up the disordered parts. In the final cycle of refinement of 10, 6565 reflections (of which 5004 are observed with I > 2σ(I)) were used to refine 292 parameters and the resulting R1, wR2 and S (goodness of fit) were 2.50%, 4.98% and 1.005, respectively. The refinement was carried out by minimizing the wR2 function using F2 rather than F values. R1 is calculated to provide a reference to the conventional R value but its function is not minimized. The structure of 11 was solved and refined in SHELXTL2013,40 using full-matrix least-squares refinement. The non-H atoms were refined with anisotropic thermal parameters and all of the H atoms were calculated in idealized positions and refined riding on their parent atoms. The asymmetric unit consists of two chemically equivalent but crystallographically independent molecules. For molecule A, four t-butyl groups on C2a, C7a, C11a and C23a are disordered. For molecule B, C2b, C11b, C15b and C23b are also disordered. All disordered regions were refined in two parts with their site occupation factors adding up to one, for each one respectively. A handful of residual electron density peaks were observed in the final refinement cycles but are attributed to ghost peaks after checking into the correctness of absorption corrections applied. In the final cycle of refinement of 11, 14 158 reflections (of which 10 570 are observed with I > 2σ(I)) were used to refine 567 parameters and the resulting R1, wR2 and S (goodness of fit) were 4.27%, 9.10% and 1.075, respectively. The refinement was carried out by minimizing the wR2 function using F2 rather than F values. R1 is calculated to provide a reference to the conventional R value but its function is not minimized. Thermolysis of 10 In the glove box, complex 10 (0.124 g, 0.201 mmol) was placed in a Schlenk tube. This tube was attached via Tygon tubing to a U tube. This apparatus was placed on a Schlenk line. A flow of nitrogen gas was introduced to the Schlenk tube through a needle. The gas flow rate was monitored by a bubbler attached to the opposing outlet of the U tube. The U tube was placed in a liquid nitrogen bath. A sand bath was used to heat the Schlenk tube to 250 °C for 30 minutes. Complex 10 formed a black product within the Schlenk tube. A white product was collected in the U tube. The U tube was removed from the liquid nitrogen bath and allowed to warm for a minute. CDCl3 (2 mL) was added to the U tube to dissolve the thermolysis products. This solution was used for 1H NMR and GC-MS analysis. This journal is © The Royal Society of Chemistry 2016 Paper WOx materials growth and characterization Solutions of complex 10 (0.034 M in diglyme) were prepared in a nitrogen filled glovebox. The aerosol of the solution was generated by using a nebulizer with a quartz plate vibrating at 1.44 MHz, and delivered to the deposition system with nitrogen (99.999% purity, Airgas) carrier gas at a flow rate of 1000 sccm. ITO covered borosilicate glass substrates sitting on a SiC coated graphite susceptor were heated to 200–550 °C by coupling the susceptor to a radio frequency power supply. During the tungsten oxide growth, the chamber pressure was maintained at 350 Torr for a total deposition time of 150 min. The elemental compositions of tungsten oxide samples were determined by X-ray photoelectron spectroscopy (XPS, Perkin-Elmer PHI 5100) after 10 min Ar+ sputtering to clean the surface. The crystallinities and morphologies were measured by X-ray diffraction (XRD, Panalytical X’pert Pro) and field emission scanning electron microscope (FESEM, FEI Nova NanoSEM 430). Atomic force microscopy (AFM, Veeco Dimension 3100) was used to measure the surface roughness. The details of the growth conditions and characterizations are reported elsewhere.33,34 Results and discussion Precursor design Design of single-source precursors for AACVD of metal oxide thin films has emphasized complexes bearing terminal oxo, alkoxide, β-diketonate and related ligands because these ligands could be varied to impart the high volatility or solubility needed for use in CVD. Additionally, decomposition of alkoxide ligands can provide mechanistic pathways for incorporation of oxygen into the deposited films via cleavage to oxo moieties.41 Terminal oxo ligands in the precursor itself provide this source of oxygen for materials growth with fewer bond cleavage steps required. The chelating ligands acetylacetonate, dipivaloylmethanate, tert-butylacetylacetonate and tert-butylpivaloylacetate ensure that no empty coordination site is available for intermolecular interactions that can give rise to oligomer formation, and provide improved stability to oxygen and water.16,42 The use of chelating ligands has proven to be effective for isolating monomeric compounds bearing alkoxide groups less bulky than tert-butoxide, which would oligomerize in the absence of the chelator.38 Moreover, the presence of sterically bulky chelates (acac, tbac, dpm and tbpa) in the coordination sphere of the metal could induce volatility43 or facile reactivity and ligand lability.44 Reactivity of the β-diketonate and β-ketoesterate ligands with the polymeric tungsten(VI) alkoxide molecule [WO(OR)4]n is engineered to break symmetry in the resulting monomeric molecule WO(OR)3L. The highly unsymmetrical WO(OR)3L target precursors could thus possess sufficient solubility and volatility to achieve acceptable materials growth under moderate reaction conditions in an AACVD reactor. Dalton Trans., 2016, 45, 10897–10908 | 10901 View Article Online Paper Dalton Transactions Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Synthesis The alkoxide-bridged dimers [WO(OR)4]2 (16–18) and the monomeric complexes WO(OtBu)4 (15) and WO(ONp)4 (19) react with β-diketones and β-ketoesters (Hacac, Htbac, Hdpm and Htbpa) under reflux for 3 h to form the mononuclear complexes WO(OR)3L (1–13; R = methyl, ethyl, isopropyl, neopentyl, L = acac, dpm, tbac, tbpa) as shown in Schemes 1 and 2. Complex 13 could also be synthesized from 15 and Htbac under much milder conditions by addition at 0 °C and then stirring at room temperature for 12 h. Syntheses of 1–8 were facilitated by the dynamic behavior of dimers 16–18 in solution, which can be observed at room temperature.38 The fluxionality of the bridging alkoxides allows facile ligand exchange with the bidentate β-diketonate and β-diketoesterate ligands under reflux. This preparatory route offers a simple workup that affords clean products in high yields. The only byproducts are alcohols that are sufficiently volatile to be removed under vacuum with the reaction solvent. The pure products were obtained by either sublimation or vacuum distillation depending on the nature of the crude product. Compounds 1, 10, 11, 12 and 13 were isolated as solids with yellow-orange, pale orange, light brown and whitish colors, respectively. Compound 2 was a moist orange semi-solid that solidifies upon freezing (−3 °C). The rest of the complexes were yellow-orange liquids of low viscosity, with exception of 9 that was slightly viscous. Reaction of 19 with 4.5 equiv. of Hdpm under conditions similar those used for synthesis of 11 resulted in formation of a mixture of 11 and the dioxo tungsten(VI) complex WO2(dpm)2 (11a). The presence of 11a as a side product suggests scission of an alkoxide C–O bond to form the second dioxo ligand in Scheme 1 Synthesis of 1–8. Scheme 2 Synthesis of 9–13. 10902 | Dalton Trans., 2016, 45, 10897–10908 11a, which was identified by X-ray crystallography (ESI, Fig. S26 and S28†). The cleavage process could be facilitated by steric repulsions among the ligands. The proportion of 11a in the product mixture was observed to generally increase with increasing amounts of Hdpm in the reaction mixture (to 8 equiv.) and increasing the reaction time to 2 days under reflux (Fig. S26†), although complete conversion to 11a could not be achieved by further extension of the reaction time to 4 days. NMR spectroscopy of 1–13 The 1H NMR and 13C NMR spectra of 1–13 contained resonances with splitting patterns and intensities consistent with the structural assignments. In the 1H NMR spectrum of each compound, there are two sets of symmetrically inequivalent alkoxide signals in a 2 : 1 intensity ratio. The integrations of all of the 1H NMR spectra confirm that only one β-diketonate/ β-ketoesterate ligand is coordinated to the tungsten. Further, all the spectra displayed symmetry inequivalence between the substituents on the chelating β-diketonate/β-ketoesterate ligands, which is consistent with their assignment as the mer isomers. X-Ray crystallographic structure determination of 1, 10 and 11 The crystalline samples obtained by sublimation of 1 and 10 contained single crystals that were suitable for crystallographic data collection. The single crystals of 11 were grown from toluene solution by cooling. Fig. 1–3 contain the molecular structures of 1, 10 and 11, respectively, and selected bond length and angles can be found in Table 1. The crystal structure of 11 contained two independent molecules, one of which is shown in Fig. 3 (see Fig. S27, ESI† for the geometry of the second independent molecule of 11). The crystal and structure refinement data are in Table 2. The coordination geometries of 1, 10 and 11 in the solid state adopt the anticipated monomeric structures. The three structures show distorted octahedral geometry about the W(VI) center. In the context of the distorted octahedral structure of 1, 10 and 11, the terminal oxo, an alkoxide and the chelating β-diketonate ligands are defined to occupy equatorial positions, which are almost in plane with the W. The two symmetrically equivalent alkoxide ligands occupy the two axial Fig. 1 Displacement ellipsoids diagram of the molecular geometry of 1 drawn at 40% probability. This journal is © The Royal Society of Chemistry 2016 View Article Online Paper Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Dalton Transactions diketonate ligands were determined to be 80.68(6)°, 80.78(8)° and 80.35(16)° for 1, 10 and 11 respectively (Table 1), and are typical of β-diketonate moieties coordinated to a d0 transition metal in a pseudo-octahedral environment.46 The trans influence exerted by the oxo moiety on the β-diketonate or β-ketoesterate ligand is quite pronounced. As a result, the W–O bonds trans to the oxo ligands are lengthened to 2.2087(16) Å, 2.2454(19) Å and 2.217(4) Å for 1, 10 and 11, respectively (Table 1), and are each an average of 0.2 Å longer than other the W–O bond to the β-diketonate or β-ketoesterate ligand. Fig. 2 Displacement ellipsoids diagram of the molecular geometry of 10 drawn at 40% probability. Fig. 3 Displacement ellipsoids diagram of the molecular geometry of 11 drawn at 40% probability. positions but are not quite linear with O–W–O bond angles of 161.78(7)°, 159.90(8)° and 161.8(8)° in 1, 10 and 11, respectively (Table 1). The alkoxide ligands are bent away from the oxo but towards the β-diketonate/β-diketonate ligand. A similar distortion has been observed in other d0 transition metal oxo complexes. Angular distortion of the axial H–Mo–H bonds away from the oxo ligands in cis-[MoO2H4]2− has been studied by EHT and attributed to strong interaction of the metal orbitals in the x–y plane with the p-orbitals of oxygen, which optimizes W–O(oxo) π-bonding.45 Strengthening of the W–O(oxo) π-bonding is also facilitated by the small bite angles of the β-diketonate ligands. The bite angles of the beta- Table 1 Mass spectrometry Table 3 highlights the abundant ions observed in the positive ion chemical ionization mass spectra of 1, 2 and 9–13. The low abundances of the molecular ions (2–7%) are consistent with extensive fragmentation in the gas phase following ionization (see Table S2, ESI†). Fragmentation tendencies during mass spectrometry have been used to model the gas phase portions of precursor decomposition during CVD, although care must be taken in interpretation.47,48 Complexes 1, 2 and 11 exhibit similar fragmentation pathways, in which net loss of alkoxide generates the [M − OR]+ species as the base peak. For the less sterically crowded 1 and 2, these [M − OR]+ ions undergo subsequent reaction with molecular ions to generate the dinuclear species [M + (M − OR)]+. The analogous [M + (M − OR)]+ ion is formed in small quantities from the more hindered neopentoxide complex 9. For complexes 10–13, the [M − OR]+ ions are evident in the spectra but the [M + (M − OR)]+ ions could not be detected because their m/z values fall outside the range of the instrument. An alternative pathway evident in Table 3 involves initial loss of β-diketonate/β-ketoesterate fragments to yield the ion [M − L]+, which can be observed for 1, 2 and 9–13. For 1, 2 and 9, the [M − L]+ ion proceeds to react with starting material, resulting in small amounts of M + [M − L]+, as shown in Table S2 (ESI†). For 10–12, the m/z value of the M + [M − L]+ ion falls outside the instrument range and thus could not be detected. However, the M + [M − L]+ ion is not present for the tert-butoxide compound 13, although its m/z value would lie within the range of the instrument. Comparison of the behavior of acac complexes 1, 2 and 9 provides information on the preferred sites for gas phase protonation and ligand loss as the steric demand of the alkoxides Selected bond distances (°) and angles (°) for compounds 1, 10 and 11 Bond parameter 1 Bond parameter 10 Bond parameter 11 W1–O1 W1–O2 W1–O3 W1–O4 W1–O5 W1–O6 O5–W1–O6 O2–W1–O3 O1–W1–O2 O2–W1–O4 1.7175(16) 2.0450(16) 2.2087(16) 1.8723(16) 1.8793(15) 1.8807(15) 161.78(7) 80.68(6) 95.54(7) 164.55(7) W1–O1 W1–O4 W1–O6 W1–O2 W1–O3 W1–O5 O3–W1–O5 O4–W1–O6 O1–W1–O4 O2–W1–O4 1.699(2) 2.021(2) 2.2454(19) 1.860(2) 1.897(2) 1.882(2) 159.90(9) 80.78(8) 93.91(9) 165.9(9) W1A–O1A W1A–O4A W1A–O6A W1A–O2A W1A–O3A W1A–O5A O3A–W1A–O5A O4A–W1A–O6A O1A–W1A–O4A O2A–W1A–O4A 1.702(5) 2.008(4) 2.217(4) 1.866(4) 1.877(5) 1.877(5) 161.8(3) 80.35(16) 94.2(2) 164.58(18) This journal is © The Royal Society of Chemistry 2016 Dalton Trans., 2016, 45, 10897–10908 | 10903 View Article Online Paper Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Table 2 Dalton Transactions Crystal data and structure refinements for 1, 10 and 11 Identification code 1 10 11 Formula Formula weight Temperature Crystal system Space group a(Å) b(Å) c(Å) α/β/γ(°) Z Volume Density (calculated) Crystal size (mm3) Absorption coefficient F(000) Index range C8H16O6W 392.06 100(2) K Monoclinic P21/n 7.3458(5) 12.0008(8) 13.3320(9) 90/97.5390(10)/90 4 2108.0(2) Å3 2.235 mg m−3 0.09 × 0.09 × 0.03 9.921 mm−1 744 −9 ≤ h ≤ 9, −14 ≤ k ≤ 15, −17 ≤ l ≤ 17 2.29 to 27.50°. 2692 [R(int) = 0.0205] 100.0%(theta = 25.50) 1.088 2692/0/141 Analytical R1 = 0.0115, wR2 = 0.0239 [2128] R1 = 0.0180, wR2 = 0.0267 0.496 and −0.579 e Å−3 C23H46O6W 618.45 100(2) K Monoclinic P21/n 9.7653(5) 17.3223(9) 17.2212(9) 90/101.5039(10)/90 4 2854.6(3) Å3 1.439 mg m−3 0.180 × 0.079 × 0.047 4.081 mm−1 1256 −12 ≤ h ≤ 12, −22 ≤ k ≤ 21, −22 ≤ l ≤ 18 1.685 to 27.499°. 6565 [R(int) = 0.0490] 100.0%(theta = 25.242) 1.005 6565/0/292 Integration R1 = 0.0250, wR2 = 0.0498 R1 = 0.0447, wR2 = 0.0547 1.184 and −0.729 e Å−3 C26H52O6W 644.52 100(2) K Monoclinic P21/c 19.3583(14) 19.5078(14) 16.7970(12) 90/103.5832(14)/90 8 6165.8(8) Å3 1.389 mg m−3 0.368 × 0.232 × 0.102 3.779 mm−1 2640 −25 ≤ h ≤ 25, −25 ≤ k ≤ 25, −21 ≤ l ≤ 21 1.082 to 27.499°. 14 158 [R(int) = 0.0398] 100.0% (theta = 25.242) 1.075 14 158/0/567 Analytical R1 = 0.0427, wR2 = 0.0910 [10 570] R1 = 0.0679, wR2 = 0.1158 3.333 and −2.696 e Å−3 Theta range for data coll. Independent reflections Completeness to theta GOF on F2 Data/restraints/param. Abs. corr. Final R indices [I > 2σ(I)] R indices (all data) Largest diff peak and hole R1 = ∑(||Fo| − |Fc||)/∑|Fo|. wR2 = [∑[w(Fo2 − Fc2)2]/∑(w(Fo2)2)]1/2. S = [∑[w(Fo2)2 − Fc2)2]/(n − p)]1/2. w = 1/[σ2(Fo2) + (m × p)2 + n × p], p = [max(Fo2,0) + 2 × Fc2]/3, m & n are constants. Table 3 Selected relative abundances (m/z) of ions in the positive ion DIPCI mass spectra of 1, 2, 9, 10, 11, 12, and 13 WO(OR)3(L) [M − OR]+ m/z (%) [M + (M − OR)]+ m/z (%) [M − L]+ m/z (%) [HOR + H]+ m/z (%) [R]+ m/z (%) [HL + H]+ m/z (%) WO(OMe)3(acac) (1) WO(OEt)3(acac) (2) WO(ONp)3(acac) (9) WO(ONp)3(tbac) (10)a WO(ONp)3(dpm) (11) WO(ONp)3(tbpa) (12)b WO(OtBu)3(tbac) (13) 361 (100) 389 (100) 473 (14) 351 (31) 557 (100) 573 (55) 502 (14) 753 (23) 823 (28) 1033 (4) n. o. n. o. n. o. n. o. 293 (31) 335 (39) 461 (2) 461 (46) 461 (9) 461 (20) 419 (13) n. o.b n. o. 89 (28) 89 (58) 89 (34) n. o. n. o. n. o. n. o. 71 (3) 71 (100) 71 (17) 71 (100) 57 (100) 101 (5) 101 (3) 101 (100) 159 (18) 185 (10) n. o. n. o. a Complex 10 also yields a large peak for a ligand fragment at m/z 57 (72%). See ESI for detailed data. b n. o. = not observed. increases. The base peak for complexes 1 and 2 is [M − OR]+, which suggests protonation at an alkoxide oxygen followed by loss of the alcohol to generate [M − OR]+. However, due to increased bulk of the neopentoxide ligands in compound 9, the diketonate ligand is preferentially protonated over the alkoxide by the chemical ionization and the dominant pathway is loss of the acac ligand to produce [HL + H]+ as the base peak. In compound 11, where the acac ligand is the sterically hindered dpm, protonation of the acac ligand is also less accessible and therefore the loss of the neopentoxide ligand becomes predominant. Complexes bearing ketoesterate ligands (10, 12 and 13) show significant alkoxide fragmentation to afford the alkyl cation as their base peaks. This suggests a facile pathway for conversion of an alkoxide ligand to a second oxo moiety, a process we have previously noted in the mass spectra of the 10904 | Dalton Trans., 2016, 45, 10897–10908 related oxo alkoxide complexes WO[OC(CH3 )2 CF 3] 4 and WO[OC(CF3 )2 CH 3 ] 4 .33,49 Thermolysis of 10 Volatile decomposition fragments of compound 10 were isolated and analyzed using 1H NMR and GC-MS following thermolysis. Neopentanol and the free β-ketoester ligand were identified as the major components in the 1H NMR spectrum of the trapped volatile products by comparison to authentic samples. The identification of neopentanol was confirmed by detection of mass spectral fragmentation patterns that match authentic spectra in the NIST database.50 A proposed mechanism for the formation of neopentanol by thermolysis of 10 (Scheme 3) follows a pathway similar to that reported for thermal decomposition of Ti(ONp)4.51 This journal is © The Royal Society of Chemistry 2016 View Article Online Dalton Transactions Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Scheme 3 Paper Proposed decomposition mechanism for 10. Mass spectra of the thermolysis products also contained tert-butyl acetoacetate, as identified by comparison to the NIST database.50 Loss of β-ketoesterate ligands and formation of acetylketene have been observed in the thermolysis of the related compound Ti(OiPr)2(tbac)2.52 Mass spectra of thermolysis products from 10 are consistent with the decomposition chemistry of Ti(OiPr)2(tbac)2, as the molecular ion for acetylketene was detected along with fragment ions from the β-ketoesterate ligand. Grown WOx material properties The tungsten oxide materials grown at 200, 300, 400, and 500 °C from complex 10 appear to be blue in color, as expected for substoichiometic WO3−x.53 These samples are shown in plan-view and cross-sectional SEM images in Fig. 4. Films were grown at low deposition temperatures (200–500 °C), with a transition in growth habit from dense polycrystalline layers to nanorod bundles as the growth temperature was raised to 500 °C. The film thicknesses are 80 (±6) and 538 (±9) nm for film samples grown at 200 and 300 °C, respectively. The textured samples grown at 400 and 500 °C have vertical heights of 522 (±26) nm and 2.23 (±0.4) μm, each. The surface roughness measured by AFM showed the dense polycrystalline films have smooth surfaces with RMS roughness values of 7.8 (±0.2) and 6.0 (±0.6) nm. However, the textured sample grown at 400 °C exhibited a higher roughness of 37.0 (±5.6) nm, and the roughness could not be measured for the nanorod sample grown at 500 °C. XRD patterns were acquired for each of the films to better understand the growth habit variations (Fig. 5). The scans for Fig. 4 Plan-view (upper) and cross-sectional (lower) SEM images of films grown on ITO/glass at (a) 200, (b) 300, (c) 400, and (d) 500 °C from precursor 10 dissolved in diglyme in N2 carrier gas. Note not all images are the same scale. This journal is © The Royal Society of Chemistry 2016 Fig. 5 XRD patterns for samples grown from precursor 10 solution under N2 at 4 temperatures. the continuous films grown at the two lowest temperatures reveal only a single sharp reflection assigned to ITO. A broad hump at lower values of 2Θ is also evident, consistent with the growth of amorphous WOx film. The samples grown at 400 and 500 °C, however, show two additional diffraction peaks corresponding to the W18O49 monoclinic phase.54 The diffraction peak at 23.5 2Θ° matches a d-spacing of 3.78 Å, and matches well the lattice parameter in the [010] direction. The growth of highly textured films at high temperature is often associated with increased surface mobility of adsorbed reactants, leading to increased crystallinity. A previous study reports that W18O49 grown by CVD at high temperatures afforded nanorod structures.33 To better understand the stoichiometry of the grown films, XPS measurements were performed and the results are shown in Fig. 6. The O 1s peaks have consistent binding energy (BE) values in the small range 530.7–530.8 eV regardless of growth temperature. These peaks correspond to oxygen bound to tungsten of mixed oxidation state, likely W4+ and W6+.55,56 The W 4f5/2 and 4f7/2 peak intensities decrease at low binding energies as deposition temperature increases. The XPS peaks of samples grown at 200 and 500 °C were deconvoluted and compared after Shirley baseline subtraction (Fig. S30†). The W peaks of sample grown at 200 °C show low BE peaks at 31.4 and 33.4 eV, which correspond to tungsten carbide,57–59 and Fig. 6 XPS O 1s, C 1s, and W 4f5/2 & 4f7/2 doublet peaks for materials grown from precursor 10 at different temperatures. Dalton Trans., 2016, 45, 10897–10908 | 10905 View Article Online Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Paper high BE peaks at 34.8 and 37.3 eV, which may match to W6+.60–62 Meanwhile, the W peaks of sample grown at 500 °C were deconvoluted to minor peaks at BEs of 32.4 and 33.7 eV, which suggest W4+,63–65 and major peaks at BEs of 35.6 or 37.7 eV, which correspond to W6+,61,66,67 thus suggesting increasing tungsten oxidation state as deposition temperature increases. The XPS results were used to estimate overall film composition (Fig. 7). The results show that the tungsten level decreases as deposition temperature increases. The oxygen atom fraction initially increases with temperature increase (200–350 °C); however it decreases slightly at higher temperatures (400–550 °C) along with increased carbon content. The stoichiometric value (O : W atomic ratio) of tungsten oxide (WOx) increases as deposition temperature increases, and this may correlate to the change in material crystallinity from amorphous to W18O49 monoclinic nanorods (O : W = 2.72). Carbon was detected in samples grown both at the lowest growth temperature (200 °C) and ≥400 °C. The carbon contamination at high temperatures is primarily attributed to the larger surface area provided by the nanorod structures. Precursor and solvent decomposition to afford carbon contamination has previously been detected in samples grown from other tungsten oxo alkoxide precursors using the same solvent.33,34 Previously reported XPS measurements on deposited films, however, showed the samples were essentially carbon-free with maximum carbon contamination (≤3 at%) detected for just a few samples. The C 1s peaks in Fig. 7 also show different BE depending on the growth temperature. The sample grown at 200 °C has its C 1s peak at 283.0 eV, while the samples grown Dalton Transactions at 400 and 500 °C have their main peaks at 283.9 and 384.1 eV. The peak at low BE of 283.0 eV corresponds to carbon in tungsten carbide,63,68 and peaks at BE of 284.0 eV are close to free carbon.63,69 Thus, the carbon contamination in samples grown at 200 °C is bound to tungsten, and carbon impurities on samples grown at high temperatures mostly exist on the surface. The formation of tungsten carbide under certain growth conditions is consistent with the low carbon content that is occasionally observed in the combustion analyses of these compounds. Conclusion Reaction of the dinuclear species [WO(OR)4]2 with β-diketonate/β-ketoesterate ligands L generated mononuclear complexes of the type WO(OR)3L, that display sufficient solubility and stability in volatile organic solvents to permit rapid growth of WOx materials by AACVD. The facile synthesis of the complexes is facilitated by the fluxional motion of [WO(OR)4]2 in solution, which provides a pathway for exchange of alkoxide with L. Additionally, the low molecular symmetry of WO(OR)3L resulted in several liquid precursors (3–9) that possess sufficient vapor pressure for facile gas phase mass transport. Growth of WOx by AACVD was demonstrated for precursor 10. Characterization of materials deposited in the temperature range 200 to 550 °C by XRD indicates growth of an amorphous film at lower temperature transitioning to bundled nanorods of monoclinic W18O49 as temperature was elevated. The amorphous substoichiometric WOx grown at 200 °C contained a small amount of C (∼5 atomic%) as evidenced by observation of an XPS peak with binding energy consistent with W–C. Growth between 200 and 300 °C resulted in continuous, dense, pure and amorphous thin films of substoichiometric WOx. Increase in oxidation of the films upon growth above 400 °C coincides with crystallization of W18O49 nanorods, a phenomenon that increased surface area and adsorbed C. Acknowledgements The authors thank the National Science Foundation for support under the GOALI grant CHE-1213965. KAA wishes to acknowledge the National Science Foundation and the University of Florida for funding of the purchase of the X-ray equipment. Notes and references Fig. 7 (a) Film composition from XPS measurements and (b) O : W atomic ratio variation with deposition temperature from complex 10 dissolved in diglyme. 10906 | Dalton Trans., 2016, 45, 10897–10908 1 M. Vasilopoulou, L. C. Palilis, D. G. Georgiadou, P. Argitis, S. Kennou, I. Kostis, G. Papadimitropoulos, N. A. Stathopoulos, A. A. Iliadis, N. Konofaos, D. Davazoglou and L. Sygellou, Thin Solid Films, 2011, 519, 5748–5753. 2 M. Vasilopoulou, G. Papadimitropoulos, L. C. Palilis, D. G. Georgiadou, P. Argitis, S. Kennou, I. Kostis, This journal is © The Royal Society of Chemistry 2016 View Article Online Dalton Transactions 3 4 Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 N. Vourdas, N. A. Stathopoulos and D. Davazoglou, Org. Electron., 2012, 13, 796–806. K. Hara, Z.-G. Zhao, Y. Cui, M. Miyauchi, M. Miyashita and S. Mori, Langmuir, 2011, 27, 12730–12736. G. Grancini, R. S. S. Kumar, A. Abrusci, H. L. Yip, C. Z. Li, A. K. Y. Jen, G. Lanzani and H. J. Snaith, Adv. Funct. Mater., 2012, 22, 2160–2166. H. D. Zheng, Y. Tachibana and K. Kalantar-zadeh, Langmuir, 2010, 26, 19148–19152. H. Choi, B. Kim, M. J. Ko, D. K. Lee, H. Kim, S. H. Kim and K. Kim, Org. Electron., 2012, 13, 959–968. B. P. Jelle, G. Hagen and S. Nodland, Electrochim. Acta, 1993, 38, 1497–1500. K. S. Deb, S.-H. Lee, E. C. Tracy, R. J. Pitts, A. B. Gregg and M. H. Branz, Electrochim. Acta, 2001, 46, 2125–2130. G. Leftheriotis, G. Syrrokostas and P. Yianoulis, Sol. Energy Mater. Sol. Cells, 2010, 94, 2304–2313. Y. Saito, S. Uchida, T. Kubo and H. Segawa, Thin Solid Films, 2010, 518, 3033–3036. W. J. Lee, P. S. Shinde, G. H. Go and E. Ramasamy, Int. J. Hydrogen Energy, 2011, 36, 5262–5270. K. S. Gullapalli, S. R. Vemuri, S. F. Manciu, L. J. Enriquez and V. C. Ramana, J. Vac. Sci. Technol., A, 2010, 28, 825– 828. G. E. Buono-Core, A. H. Klahn, G. Cabello, E. Munoz, M. J. Bustamante, C. Castillo and B. Chornik, Polyhedron, 2012, 41, 134–139. L. Meda, G. Tozzola, A. Tacca, G. Marra, S. Caramori, V. Cristino and C. A. Bignozzi, Sol. Energy Mater. Sol. Cells, 2010, 94, 788–796. S. K. Deb, Sol. Energy Mater. Sol. Cells, 2008, 92, 245–258. A. C. Jones, H. C. Aspinall and P. R. Chalker, Surf. Coat. Technol., 2007, 201, 9046–9054. J. M. Hampden-Smith and T. Kodas, Chem. Vap. Deposition, 1995, 1, 9–14. I. P. Parkin and R. G. Palgrave, in Chemical Vapour Deposition, ed. A. C. Jones and M. L. Hitchman, RSC Publishing, Cambridge, 2009, pp. 451–476. J. H. Youn, S. J. Baek, H. P. Kim, D. H. Nam, Y. Lee, J. G. Lee and J. Jang, J. Mater. Chem. C, 2013, 1, 3250–3254. S.-H. Kim, H. Otsuka, H.-W. Shin, K. Tanaka, R. C. Advincula and H. Usui, Jpn. J. Appl. Phys., 2011, 50, 01BB01. H.-M. Kim, J. Kim, J. Lee and J. Jang, ACS Appl. Mater. Interfaces, 2015, 7, 24592–24600. R. G. Palgrave and I. P. Parkin, New J. Chem., 2006, 30, 505– 561. M. J. Hampden-Smith and T. T. Kodas, Chem. Vap. Deposition, 1995, 1, 8–23. J. O. Carlsson, Acta Chem. Scand., 1991, 45, 864–869. P. Marchand, I. A. Hassan, I. P. Parkin and C. J. Carmalt, Dalton Trans., 2013, 42, 9406–9422. S. Shi, X. Xue, P. Feng, Y. Liu, H. Zhao and T. Wang, J. Cryst. Growth, 2008, 310, 462–466. X. Hou and K. L. Choy, Chem. Vap. Deposition, 2006, 12, 583–596. This journal is © The Royal Society of Chemistry 2016 Paper 28 C. Roger, T. Corbitt, C. Xu, D. Zeng, Q. Powell, C. D. Chandler, M. Nyman, M. J. Hampden-Smith and T. T. Kodas, Nanostruct. Mater., 1994, 4, 529–535. 29 K. L. Choy, Prog. Mater. Sci., 2003, 48, 57–170. 30 C. K. Molloy and A. P. Williams, Appl. Organomet. Chem., 2008, 22, 676–683. 31 D. Baxter, M. H. Chisholm, S. Doherty and N. E. Gruhn, Chem. Commun., 1996, 1129–1130. 32 K. C. Molloy and P. A. Williams, Appl. Organomet. Chem., 2008, 22, 560–564. 33 R. O. Bonsu, H. Kim, C. O’Donohue, R. Y. Korotkov, K. R. McClain, K. A. Abboud, A. A. Ellsworth, A. V. Walker, T. J. Anderson and L. McElwee-White, Dalton Trans., 2014, 43, 9226–9233. 34 H. Kim, R. O. Bonsu, C. O’Donohue, R. Y. Korotkov, L. McElwee-White and T. J. Anderson, ACS Appl. Mater. Interfaces, 2015, 7, 2660–2667. 35 G. V. Kunte, S. A. Shivashankar and A. M. Umarji, Thermochim. Acta, 2008, 474, 12–15. 36 S. D. Evans and R. P. Houghton, J. Mol. Catal. A: Chem., 2000, 164, 157–164. 37 H. J. Wengrovius and R. R. Schrock, Organometallics, 1982, 1, 148–155. 38 W. Clegg, J. R. Errington, P. Kraxner and C. Redshaw, J. Chem. Soc., Dalton Trans., 1992, 1431–1438. 39 SHELXTL6, Madison, Wisconsin, 2008. 40 SHELXTL2013, Madison, Wisconsin, 2013. 41 J. M. Mayer, Polyhedron, 1995, 14, 3273–3292. 42 A. C. Jones, J. Mater. Chem., 2002, 12, 2576–2590. 43 E. W. Berg and J. T. Truemper, J. Phys. Chem., 1960, 64, 487–490. 44 Y. Jiang, H. Song, L. Li, W. Bao and G. Meng, J. Cryst. Growth, 2004, 267, 256–262. 45 D. C. Brower, J. L. Templeton and D. M. P. Mingos, J. Am. Chem. Soc., 1987, 109, 5203–5208. 46 H. O. Davies, T. J. Leedham, A. C. Jones, P. O’Brien, A. J. P. White and D. J. Williams, Polyhedron, 1999, 18, 3165–3172. 47 Y. S. Won, Y. S. Kim, T. J. Anderson and L. McElwee-White, Chem. Mater., 2008, 20, 7246–7251. 48 Y. S. Won, Y. S. Kim, T. J. Anderson, L. L. Reitfort, I. Ghiviriga and L. McElwee-White, J. Am. Chem. Soc., 2006, 128, 13781–13788. 49 R. O. Bonsu, H. Kim, C. O’Donohue, R. Y. Korotkov, K. A. Abboud, T. J. Anderson and L. McElwee-White, Inorg. Chem., 2015, 54, 7536–7547. 50 NIST, NIST Mass Spectral Search Program Version 2.0 g, Gaithersburg, MD, 2011. 51 M. Nandi, D. Rhubright and A. Sen, Inorg. Chem., 1990, 29, 3065–3066. 52 R. Bhakta, R. Thomas, F. Hipler, H. F. Bettinger, J. Muller, P. Ehrhart and A. Devi, J. Mater. Chem., 2004, 14, 3231– 3238. 53 A. Braun, F. Aksoy Akgul, Q. Chen, S. Erat, T.-W. Huang, N. Jabeen, Z. Liu, B. S. Mun, S. S. Mao and X. Zhang, Chem. Mater., 2012, 24, 3473–3480. Dalton Trans., 2016, 45, 10897–10908 | 10907 View Article Online Published on 03 May 2016. Downloaded by University of Florida Libraries on 14/10/2016 07:04:53. Paper 54 J. Booth, T. Ekstrom, E. Iguchi and R. J. D. Tilley, J. Solid State Chem., 1982, 41, 293–307. 55 D. Gogova, K. Gesheva, A. Szekeres and M. Sendova-Vassileva, Phys. Status Solidi A, 1999, 176, 969–984. 56 D.-H. Kim, Appl. Phys. A, 2012, 108, 981–986. 57 K. Masahiro and T. Yohei, Jpn. J. Appl. Phys., 2004, 43, 7292. 58 A. Katrib, F. Hemming, P. Wehrer, L. Hilaire and G. Maire, Catal. Lett., 1994, 29, 397–408. 59 J. Chu, Y. Hsieh, C. Lin and T. Mahalingam, J. Mater. Res., 2005, 20, 1379–1384. 60 E. A. Kneer, C. Raghunath, S. Raghavan and J. S. Jeon, J. Electrochem. Soc., 1996, 143, 4095–4100. 61 Y. Zhang, J. Yuan, J. Le, L. Song and X. Hu, Sol. Energy Mater. Sol. Cells, 2009, 93, 1338–1344. 62 Y.-S. Lin, H.-T. Chen and S.-S. Wu, J. Solid State Electrochem., 2010, 14, 1885–1895. 10908 | Dalton Trans., 2016, 45, 10897–10908 Dalton Transactions 63 A. Katrib, F. Hemming, P. Wehrer, L. Hilaire and G. Maire, Top. Catal., 1994, 1, 75–85. 64 M. Ranjbar and S. M. Mahdavi, Appl. Phys. A, 2008, 92, 627–634. 65 H. L. Zhang, D. Z. Wang and N. K. Huang, Appl. Surf. Sci., 1999, 150, 34–38. 66 G. Wang, Y. Ling, H. Wang, X. Yang, C. Wang, J. Z. Zhang and Y. Li, Energy Environ. Sci., 2012, 5, 6180–6187. 67 J. Yu, K. H. Choo, L. Niu and D. H. C. Chua, Electrochem. Solid-State Lett., 2011, 14, K58. 68 G. Leclercq, M. Kamal, J. M. Giraudon, P. Devassine, L. Feigenbaum, L. Leclercq, A. Frennet, J. M. Bastin, A. Lofberg, S. Decker and M. Dufour, J. Catal., 1996, 158, 142–169. 69 Y.-S. Lin, Y.-C. Chen and P.-S. Shie, Sol. Energy Mater. Sol. Cells, 2014, 122, 59–69. This journal is © The Royal Society of Chemistry 2016
© Copyright 2026 Paperzz