F4280 Technology of thin film deposition and surface treatment 5. Chemical Vaport Deposition Lenka Zajíčková Faculty of Science, Masaryk University, Brno & Central European Institute of Technology - CEITEC lenkaz@physics.muni.cz spring semester 2021 Chemical Vapor Deposition 5.1 Gaseous Sources 5.2 Chemical Vapor Deposition Scheme 5.3 Typical Chemical Reactions in CVD 5.4 Variants of CVD 5.5 CVD Precursors & Gas Supply 5.5.1 Precursor Requirements 5.5.2 Precursor Volatility 5.5.3 Gas Supply Set-up 5.5.4 Contamination 5.6 Chemical Reactors 5.7 Understanding the Overall Reaction 5.7.1 Gas-phase and surface reactions 5.8 APCVD versus LPCVD 5.9 MOCVD 5.10 Atomic Layer Deposition 5.11 Thermal Forming Processes F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition ka Zajíčková 3/23 5.1 G aseous Sources Let's use practical distinguishment of gas and vapor: gas does not condense when held above room T and below 1-atm partial pressure. Distinguishing the methods of delivery according to equilibrium vapor pressure pv: ► sources species having pv < 10-2 Pa at the wall T of the deposition chamber must by "physically" evaporated (using heat or energy beams) PVD processes (requiring low-p operation and "line-in-sight" geometry ► materials with pv > 10-2 Pa at the wall T are used in CVD (can operate at atmospheric pressure or lower - fluid flow Kn < 1) Most of elements, with exception of alkali metals and alkaline earths (group IA and 11 A) can be converted to gases or to chemical vapors by reacting them with terminating radicals, e.g. ► H ► halogens F, CI, Br, I ► carbonyl CO ► H-saturated organic radicals R such as methyl CH3 and ethyl CH2CH3 F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková ... constituents of the vapour phase react chemically on a substrate surface to form a solid product (heterogenous reactions). Some gas-phase reactions are unavoidable due to high gas temperature. Undesirable homogeneous reactions in the gas phase nucleate particles that may form powdery deposits and lead to particle contamination. Deposition Variables: temperature pressure (from low pressures, i.e., 10-1000 Pa - LPCVD, up to atmospheric pressures - APCVD) input concentration gas flow rates reactor geometry ► ► ► ► ► Kinetics of the reactions may depend on such factors like substrate material, etri ir»ti iro onrl r\riontatir\n AOurce-ga* *Uppl> I transport and homogeneous reaction forced Convection i free convection 1 ľ diffusion ~1 adsorption | deposition 1 fturfcee reactio } d r sorption film composition ] and structure F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition 5.3 Typical Chemical Reactions in CVD Lenka Zajíčková 5/23 TABLE 7 i Typical Overall Reaction? Li»d in CVD pyrfilyw-H t hernial dwflmpoHiLiiiiiJ SiH4<£) -+ Siíc} + 2ü^gi SiH.ri.j- ť ■ -ft S-., i- + J H' ..: CH4(f) -* 0(diamond or graphiLŕ) + 2Hs + -iNH^R) -ft Sialic) + 12Hj(g) JA i i '-.j1 K' + 3H20<(S) -ft Al2ü3(c) -ft 6HCKgj WFflfg) + 3Ha(g) —* Wte) + 6HFXg) GriCH^g) ♦ AiH^g) -» G*Aa(e> + SCH^gJ ZnClaig) + H^g) -ft ZuStc) + 2HCHgi 2Tin^i:B:. + 2NH3(g) + H^g) -ft T1N + BHCUg) Overall CVD reactions consist of a series of steps, some in the gas phase and some on the surface. Materials deposited at low temperatures (bellow 600 °C for silicon) are generally amorphous. Higher temperatures tend to lead to polycrystalline phases. Very high temperatures (typically 900-1100 °C in the case of silicon) are necessary for growing single-crystal films. F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Len ka Zajíčková 6/23 5.4 Variants of CVD Most CVD reactions are thermodynamically endothermic energy has to be supplied to the reacting system: ► thermal CVD - traditional method of energy input by a thermal energy input: ► direct resistance heating of the substrate or substrate holder; ► rf induction of the substrate holder or susceptor; ► thermal radiation heating; ► photoradiation heating. ► hot filament CVD (HFCVD) - electrons ► photo-assisted CVD - higher frequency radiation such as UV ► plasma enhanced CVD (PECVD) - plasma (chapter 7) Other variants of CVD: ► low pressure and atmospheric pressure CVD (LPCVD, APCVD) - traditionally used for the deposition of polycrystalline or amorphous materials like polysilicon, silicon oxide Si02, silicon nitride Si3N4. ► metal-organic chemical vapour deposition (MOCVD) - utilizes metal-organic precursors, traditionally used for lll-V compound semiconductors like AlAs, GaAs. ► atomic layer deposition (ALD) - gaseous precursors are introduced alternately to the reaction chamber, where they reach a saturated adsorption level on the substrate surface ► epitaxial methods related to CVD (chapters) - CVD epitaxy or vapour-phase epitaxy (VPE), metal-organic vapor phase epitaxy (MOVPE), chemical beam apitaxy (CBE), metal-organic molecular beam epitaxy (MOMBE), atomic layer epitaxy (ALE / ALEp) F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 7/23 5.5 CVD Precursors & Gas Supply 5.5.1 Precursor Requirements Whatever form a CVD process takes, the same precursor requirements generally apply. The characteristics of an "ideal" CVD precursor can be summarised as follows: ► Adequate volatility to achieve acceptable growth rates at moderate evaporation temperatures. ► Stability so that decomposition does not occur during evaporation. ► A sufficiently large temperature "window" between evaporation and decomposition for film deposition. ► High chemical purity. ► Clean decomposition without the incorporation of residual impurities. ► Good compatibility with co-precursors during the growth of complex materials. ► Long shelf-life with indefinite stability under ambient conditions, i.e. unaffected by air or moisture. ► Readily manufactured in high yield at low cost. ► Non-hazardous or with a low hazard risk. Although these features are common for most CVD precursors, sometimes the precise precursor requirements can depend on the specific nature of the CVD process. A. C. Jones, M. L. Hitchman, Overview of Chemical Vapour Deposition in Chemical Vapour Deposition: Precursors, Processes and Applications, Eds A, C. Jones and M. L. Hitchman, Royal Society of Chemistry 2009 F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 8/23 5.5 CVD Precursors & Gas Supply 5.5.2 Precursor Volatility Adequate volatility necessary - With precursors that occur naturally in a gaseous state (e.g. silane, diborane, ammonia, etc.) this is not a problem. However, for precursors that are liquids or solids, volatility has to be studied. 100-90-80-70--? 60-Í" 50-I 40 30 20 10-0 V. (a) \ •* \*. (£)\ \\ \*. v. \ • (by MeCp2HfMe2 (a) MeCp2Hf(OMe)Me (b) Hf (NEtMe)4 (c) 100 200 300 400 Temperature (°C) 500 600 100 o I-£ D m 0) O Q. > 10 25 30 35 40 45 50 55 60 Temperature (C) Vapour pressure data for Ta(NMe2)5 Thermogravimetric analysis of different Hf precursors F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 9/23 5.5 CVD Precursors & Gas Supply 5.5.3 Gas Supply Set-up Schematic of a typical MOCVD reactor used for the deposition of lll-V semiconductor films. H2 N2 -|MFCfc-1 Pd cell I I purifier ^5- exhaust to chamber (run) injection manifold -d I—|MPC[>-MhCT Group III precursor d- ■fj MO precursors dopant precursor 1 pump reactor ^chamber/ load \ lock / gate valve particle trap process pump MOCVD reactor system hydride dopant Precursor precursor Gas cabinet effluent system ^exhaust A commercial "bubbler" used to evaporate metal-organic compounds for MOCVD. F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 10/23 5.5 CVD Precursors & Gas Supply General gas supply set-up ensuring the safety (D. Smith, Figure 7.2) cxhaunt duct exhaust duct Luct . ,-------Cm duct Outdoor Ran cabinet KEY rwl maiiuaJ itmí valve pneunaüc »Ivo 0 -3 - way rrpJj lor niu-iH (low O ---canlri:l wiring LO fif*8 exhaust treatment F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 11/23 Flow control thermal mass-flow controller schematic •at point-1 sensor 1 lube (n control hoard K shunt Pi orifice Pa leak vita to) Determination of flow from change of pressure in the closed chamber: Q = Ap V [Ol Ař Parm =sccm for [\/]=cm3 and [Ar]=min F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 12/23 5.5 CVD Precursors & Gas Supply 5.5.4 Contamination Impurities can occur in the gas or liquid as supplied by the manufacturer. Carrier gases are available in very high purity but final purification at the reactor may still be desired ► for H2 - diffusing through hot Pd foil (blocks other gases) ► inter gases (e.g. Ar) - passing through "getters" (contain reactive surface that chemisorbs reactive impurities) ► water and 02 can be removed by bubbling through Ga-ln-AI alloy (liquid at room T) Impurities can also intrude during vapor transport ► cleaning of reactor - until outgassing stops. It is pressure dependent only if the partial pressure of the outgassing species begins to approach its pv. Either pumping to low pressure (low pressure systems) or purging with carrier gas (atmospheric pressure systems). Beware of contamination from backstreaming of pump oil (for low pressure systems). ► cross-contamination due to switching during the deposition of multilayers - gas remaining upstream from the deposition of the previous layer becomes contaminant for the next layer ->> purging (high downstream gas velocity for quick process), problem of "dead spots" F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition ka Zajíčková 13/23 emical Reactors Chemical reactors must provide several basic functions: ► transport of the reactant and diluent gases to the reaction site, ► provide activation energy to the reactants (heat, radiation, plasma), ► maintain a specific system pressure and temperature, ► allow the chemical processes for thin film deposition to proceed optimally, ► remove the by-product gases and vapours. F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 14/23 (o hatch F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 15/23 Reactor geometries in the view of gas mixing Reactor geometry affects the gas flow characteristics which, in turn affect the properties of the deposited layer. Two basic flow type reactors: ► Displacement or plug flow reactor in which the entering gas displaces the gas already present with no intermixing of successive fluid elements. Plug flow is a simplified and idealized picture of the motion of a fluid, whereby all the fluid elements move with a uniform velocity along parallel streamlines. Mass balance for reactant A involved in a single reaction is very simple: FA — (FA + dFA) = rAdV. ► Perfectly mixed flow reactor is the opposite extreme from the plug flow reactor. To approach the ideal mixing pattern, the feed has to be intimately mixed with the contents of the reactor in a time interval that is very small compared to the mean residence time of the fluid flowing through the vessel. The essential feature is the assumption of complete uniformity of concentration and temperature throughout the reactor. F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition ka Zajíčková 16/23 gthe eac Chemical equilibrium Gibbs free energies of formation for selected gaseous and solid (c) compounds at 105 Pa: 400 200 200 -WO A0Ů -1400 -1600 -IflOO 300 Calculated equilibrium CVD phase diagram for deposition of Si borides from BCI3+ SiH4 1 1 1 ' 1 1 ľ 1 I6OO L si +siea 1 p, - n o;ta ATM \ — \ 1 5la< w I50O K 4 = i r 400 u ii \\ SU* " + 1 \ sie. \ **' \ + \ \ ; 1 11 \ 1 \ J f. . 1 \l as 0* OlT Q.fl N 0.1 0,01 1000 800 600 450 - I I I I Desorptton and/or - prereacJions j i i /—-__ i A '---~~~-J / j Diffusion |\ Kinetic — / control i \ I ■ E ■ control I 0.7 0.9 1.1 1.3 1000 7s"1 (K~1) 1.5 At lower T the growth rate is controlled by the kinetics of chemical reactions occurring either in the gas-phase or on the substrate surface. This region is generally termed the region of kinetic growth control and the film growth rate increases exponentially with substrate temperature according to the Arrhenius equation. As T increases, the growth rate becomes nearly independent of temperature and is controlled by the mass transport of reagents through the boundary layer to the growth surface, and this is termed the region of mass transport or diffusion-controlled growth. F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 21 /23 5.10 Atomic Layer Deposition General sketch of metal oxide ALD qh qh qh oh qh oh 1) Lnl_3 Pulse 2) N2 Purge 3) H20 Pulse 4) N2 Purge 1 L L L L L V L v I /\ I o oh o o oh o Ľ ho oh oh ho oh V L V i A i o oh o o oh o Example of other precursors with large ligands CH, Hf(mmp)4 ° CH, H3C -CH, CH, H3C-H3c' O... I ^O- -CH, -T X- ° CH, H,C- ■CH, CH2 I 0 1 CH3 Ce(mmp)4 h,cv ch. .ch. H3C^ O / ch, h3c— H3C/ ■ o... \ / ^°- "~'Ce-. H,C / "O- -CH \ O CH3 CH, CH, https://www.youtube.com/watch?v=HUsOMnV65jk This example shows the ALD chemistry for producing Hf02 from gaseous precursors HfCI4 (Cl=green) and H20 (0=red). ALD allows a uniform coating to be applied to complex objects - such as the inside of the fibre optic cable shown here. https://www.youtube.com/watch?v=XMda8TXLiFk Deposition of Ti02 using TiCI4 and H20. F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition ka Zajíčková 22/23 Atomic Layer Deposition 0) 3 i— c o ' o Q. 0) Q A well-designed ALD precursor will demonstrate an experimental 'ALD window' in which its deposition is truly self-limiting. In Fig. a, the window is a plateau of growth over a range of temperatures: For low T the process will demonstrate either low deposition rates from the reaction lacking the thermal energy necessary for chemisorption of the precursor on the substrate surface or too high a rate owing to condensation and physisorption of semi-reacted precursor material on the surface. In the steady plateau the ALD process is demonstrating self-limiting deposition for the temperature range. Over a certain T there is the danger of precursor decomposition, the ligand structure protecting the target atom falling apart, or chemical desorption of the precursor before the second precursor has had chance to react with the resulting surface. Condensation/ physisorption \ j , Decomposition activation S energy / \J«— ALD window —\/ Chemical \ desorption b Deposition temperature Physisorption \ \J«— ALD window —\/ . Decomposition Gas phase / reactions / / \ \ Decomposition Purge time W F4280 Technologie depozice a povrchových úprav: Chemical Vapor Deposition Lenka Zajíčková 23/23 5.11 Thermal Forming Processes In the gas phase, thermal oxidation and nitridation is a chemical thin-film forming process in which the substrate itself provides the source for the metal or semiconductor constituent of the oxide and nitride, respectively. This technique is obviously much more limited than CVD. The thermal oxidation extremely important applications in Si device technology (very high purity oxide films with high quality Si/Si02 interface are required). ► Thermal oxidation of silicon surfaces produces glassy films of Si02 for protecting highly sensitive p-n junctions and for creating dielectric layers for MOS devices. ► T = 700 - 1200 oC ► dry oxygen or water vapour (steam) as the oxidant; steam oxidation proceeds at a much faster rate than dry oxidation ► The oxidation rate is a function of the oxidant partial pressure and is controlled essentially by the rate of oxidant diffusion through the growing Si02 layer interface, resulting in a decrease of the growth rate with increased oxide thickness. ► The process is frequently conducted in the presence of hydrochloric acid vapours or vapours of chlorine-containing organic compounds. The HCI vapour formed acts as an effective impurity getter, improving the Si/Si02 interface properties and stability. ► Si oxidation under elevated pressure is of technological interest where the temperature must be minimized (VLSI devices): oxidation rate of silicon is « p higher product throughput and/or decreased temperatures. Oxidant: H20, p up to 10 atm, T usually 750-950 °C. Gas-phase oxidation of other materials is of limited technical importance. Examples: metallic Ta films converted by thermal oxidation to tantalum pentoxide for use as antireflection coating in photovoltaic devices and as capacitor elements in microcircuits. Other metal oxides grown thermally: capacitor dielectrics in thin-film devices, improve the bondina with alass in alass-to metal seals, inwove corrosion resistance.