Y(hfac)3 (and for comparison Y(thd)3) was used as yttrium source for the preparation of high-k
dielectric Y2O3 layers by oxygen-plasma assisted MOCVD at 350-450°C deposition temperature; Y(hfac)3 precursor was evaporated at 140-150°C/0.3mbar. F-containing precursor Y(hfac)3 resulted in the Y2O3 layers having unacceptable large hysteresis in capacitance-voltage data (possibly due to the F incorporation) [[i]]
[i] D. Niu, R. W. Ashcraft, Z. Chen, S. Stemmer, G. N. Parsons , J. Electrochem. Soc., Vol. 150, Iss. 5, pp. F102-F109 (2003), “Chemical, Physical, and Electrical Characterizations of Oxygen Plasma Assisted Chemical Vapor Deposited Yttrium Oxide on Silicon”
Yttrium tris(2,2,6,6-tetramethyl-3,5-heptanedionate) Y(thd)3 (or Y(DPM)3 (DPM=dipivaloylmethanate) is conventional precursor for the growth of Y-containing high temperature superconductor layers by MOCVD [[i]] and electroluminescent Y2O3 [[ii]]. However, it has some disadvantages for MOCVD applications: Y(thd)3 is a solid at room temperature (not convenient to use in flash vaporization systems), also it is not very stable in a heated bubbler (leading to difficulty to obtain a reproducible concentration of its vapors).
High purity Y(thd)3was successfully synthesized from inorganic Y salts and HDPM in ethanol/aqueous solution, purified by recrystallization from toluene and characterized by elemental analysis, XRD, TGA/DTA, NMR and FTIR spectroscopy (both fresh and aged for 30 days in air), Y(thd)3was applied as precursor of MOCVD of Y-containing multi-component oxide thin films. [[iii][PS1] ]
Vapor pressure and vapor molecular weight of Y(thd)3 (Y(C11H19O2)3) were measured by a torsion-effusion/mass-loss method in the ranges (346 to 375) K and (361 to 387) K, respectively. The molecular weight data indicate that the saturated vapor of Y(thd)3 precursor is highly monomeric. Vapor pressures, estimated to be accurate within 5% was presented in equation form for reliable extrapolation to higher temperatures. [[iv]]
The TGA curve of Y(thd)3 precursor is presented in Fig. The most of the precursor is evaporating between 188 and 255°C, only a small residue (2.6%) is left non-evaporated.
[i] H. Meinem, K. Timmer, H.L. Linden, C.I.M.A. Spee, Mat. Res. Soc. Symp. Proc., 335, 193-201, 1994
[ii] G.A. Hirata, J. McKittrick, M. Avalos-Borja, J.M. Siqueros, D. Devlin, Appl. Surf. Sci, 1997, 113/114, 509-514
[iii]H. Song, Y. Jiang, Ch. Xia, G. Meng, D. Peng, https://doi.org/10.1016/S0022-0248(02)02413-2, https://www.sciencedirect.com/science/article/pii/S0022024802024132
“Synthesis and characterization of volatile metal β-diketonate chelates of M(DPM)n (M=Ce, Gd, Y, Zr, n=3,4) used as precursors for MOCVD”
[iv] C. Colominas, K. H. Lau, D. L. Hildenbrand, S. Crouch-Baker, A. Sanjurjo, J. Chem. Eng. Data, 2001, 46 (2), p.446–450, DOI: 10.1021/je0003445, “Vapor Pressures of the Copper and Yttrium β-Diketonate MOCVD Precursors”, http://pubs.acs.org/doi/abs/10.1021/je0003445
Y(thd)3 is a useful precursor for the growth of thin films of yttria Y2O3 by CECVD
for potential applications as electronic insulators, coatings, reaction barriers and superconducting materials[[i]]
[i]Y. Zhang, R. Puddephatt, Chem. Mater.11, 148, (1999)
Y(thd)3 (and for comparison Y(hfac)3) was applied as Y precursor for the growth of high-k dielectric Y2O3 layers by oxygen-plasma assisted MOCVD at 350-450°C deposition
temperature; air-exposed Y2O3 layers grown with Y(thd)3 after annealing exhibited triple layer structure having stoichiometric
Y2O3 on top and yttrium silicate/SiO2 at dielectric/Si interface, as found by TEM, XPS and EELS (electron energy loss spectroscopy) and confirmed by FTIR, XRD and AFM; the reaction with the Si substrate was impeded by prenitridation of the silicon surface,
which promoting the Y2O3 structure. [[i]]
[i] D. Niu, R. W. Ashcraft, Z. Chen, S. Stemmer, G. N. Parsons , J. Electrochem. Soc., Vol. 150, Iss. 5, pp. F102-F109 (2003), “Chemical, Physical, and Electrical Characterizations of Oxygen Plasma Assisted Chemical Vapor Deposited Yttrium Oxide on Silicon”
Y(thd)3 (vaporised at 190°C/2.7mbar) was applied as Y source for the deposition of amorphous YSiO and Y2O3 layers at 350-450°C by the liquid injection
plasma-enhanced MOCVD (the combined approach has advantages: plasma assistance enables deposition at a much lower substrate temperature, whereas pulsed-liquid precursor delivery allows an accurate control of the supplied reactive species). Yttrium silicate
YSiOx or yttrium oxide Y2O3 layers were formed depending on the deposition temperature: ultrathin Y2O3 deposition was performed at temperature <380 °C; according to the XPS the films contained carbon
contamination that was reduced by increasing the growth temperature. Plasma played a key role in the deposition mechanisms and chemical structure of the films and interface. The injection frequency (i.e., reactive species supply rate) played a significant
role in the silicate and interface formation: high injection frequency limited the formation of SiO2 interfacial layer (and therefore YSiOx silicate layer) and favored the
growth of Y2O3 (as determined by angle-resolved XPS). As-deposited at 350°C Y2O3 films had low leakage current (J<10−7 A/cm2) and high breakdown field
(∼8 MV/cm).[[i]]
[i] C.Durand, C.Dubourdieu, C.Vallée, V.Loup, M. Bonvalot, O. Joubert, H. Roussel,O. Renault, J. Appl. Phys. 2004 , 96, 1719; http://dx.doi.org/10.1063/1.1766412, “Microstructure and electrical characterizations of yttrium oxide and yttrium silicate thin films deposited by pulsed liquid-injection plasma-enhanced metal-organic chemical vapor deposition”
Yttrium tris(2,2,6,6-tetramethyl-3,5-heptanedionate) Y(thd)3 (in conjunction with barium and copper(II)
β-diketonates) was applied for the MOCVD deposition of YBa2Cu3O7−δ superconducting thin films [[i]]
[i] G. B Deacon, P. MacKinnon, R. S Dickson, G. N Pain, B. O West, “Applied Organometallic Chemistry, 1990, Vol. 4, Iss. 5, p.439–449, DOI: 10.1002/aoc.590040504 “CVD of metal organic and other rare-earth compounds”
Y(thd)3(bipy) , Y(thd)3(phen) (and for comparison Y(thd)3 ) have been applied as ALD precursors for the growth of cubic Y2O3 films on soda lime glass and Si(100) at 200-425°C temperature; ozone O3 was used as oxidant.
The precursor evaporation conditions were following: Y(thd)3 at 120°C/2-3 mbar, Y(thd)3(bipy) at 130°C/2-3 mbar, and Y(thd)3(phen) at 180°C/2-3 mbar. With all precursors, a deposition rate of 0.22–0.23 Å/cycle was obtained at 250–350
°C on both substrates, indicating a surface-controlled growth and similar surface species at the deposition temperatures used. Crystalline (100) preferentially oriented Y2O3 films were obtained within ALE deposition window (temperature range of 250–375
°C), whereas nearly amorphous films were deposited at temperatures <250 °C. At deposition temperatures slightly above the ALE window (375 °C), where a partial decomposition of Y(thd)3 probably takes place (judging on impurity levels and growth
rates), preferential orientation of Y2O3 layers changed from (100) to (111); the adducting of Y(thd)3 did not bring any advantages in the ALE growth of Y2O3.Deposited Y2O3 layers
were characterized by XRD (crystallinity), AFM (surface morphology), ion-beam analysis/ XPS (stoichiometry and impurity levels) and IR measurements (to determine the type of carbon impurity) [[i]]
[i] M. Putkonen, T. Sajavaara, L.-S. Johansson, L. Niinistö, Chem. Vap. Dep., 2001,Vol. 7, Iss.1, p.44–50; “Low-Temperature ALE Deposition of Y2O3 Thin Films from β-Diketonate Precursors”, DOI: 10.1002/1521-3862(200101)7:1<44::AID-CVDE44>3.0.CO;2-Q
Yttrium 6,6,7,7,8,8,8-heptafluoro-2,2-dimethyl-3,5-octanedionate Y(fod)3 (in conjunction with barium and copper(II)
β-diketonates) was mentioned to have been tested to deposit YBa2Cu3O7−δ as superconducting thin films by MOCVD [[i]]
[i] G. B Deacon, P. MacKinnon, R. S Dickson, G. N Pain, B. O West, “Applied Organometallic Chemistry, 1990, Vol. 4, Iss. 5, p.439–449, DOI: 10.1002/aoc.590040504 “CVD of metal organic and other rare-earth compounds”
Y(tod)3, a complex with new type of diketonate ligand, has been successfully used as Y precursor (in combination with Hf(tod)4) for the pulsed liquid injection
(PLI) MOCVD growth of Y-stabilized HfO2 (YSH) layers; the precursor Y(tod)3 was vaporised at 280°C/6.7mbar. The growth rate was significantly higher especially at lower temperatures, compared to the conventional precursor system Y(thd)3 + Hf(thd)4. The grown YSH films were characterized by XRD, XPS, EDS and AFM; highly textured
and in-plane oriented films were deposited on sapphire by liquid injection MOCVD. [[i]]
[i] Sergej V. Pasko, Liliane G. Hubert-Pfalzgraf, Adulfas Abrutis, Philippe Richard, Ausrine Bartasyte and Vida Kazlauskiene, J . M a t e r . C h e m . , 2 0 0 4 , 1 4 , 1 2 4 5 – 1 2 5 1 , « New sterically hindered Hf, Zr and Y b-diketonates as MOCVD precursors for oxide films »
Y(tmod)3 and Y(tmod)3(tetraglyme) were compared as potential yttrium MOCVD precursors, by using thermogravimetric (“TG-DTA) analysis. The adducted molecule Y(tmod)3(tetraglyme) was
a liquid and left no residue after full evaporation (which finishes at ca. 320°C), whereas the unadducted molecule Y(tmod)3 is solid. The TGA-DTA curves for Y(tmod)3(tetraglyme) are shown in Fig. [i]
[i] C Dussarrat, US Patent App. 12/536,804, 2009 , « NOVEL LANTHANIDE BETA-DIKETONATE PRECURSORS FOR LANTHANIDE THIN FILM DEPOSITION »
www.google.de/patents?id=mQ7MAAAAEBAJ&pg=PA11&zoom=4&dq=%22Gd%28TMOD%293%22&output=text#c_top
Tris(6-ethyl-2,2-dimethyl-3,5-decanedionato) yttrium Y(EDMDD)3 (M = 764.96) is pale yellow liquid at RT, slightly reacting with H2O.
Y(EDMDD)3 was proposed as potential yttrium MOCVD precursor [[i]]
[i]ADEKA 2008