Ale Self Limited Kinetics
Atomic Layer Etching is the leading-edge subtractive nanofabrication technology that utilizes sequential, self-limiting surface modification and volatile desorption half-reactions to remove material layer-by-layer with cycle-by-cycle depth control and chemistry-dependent selectivity. As semiconductor scaling advances into sub-2nm Gate-All-Around nanosheets and 3D memory architectures, conventional continuous reactive ion etching causes unacceptable atomic lattice damage, microloading, profile bowing, and severe aspect-ratio-dependent etching lag. ALE resolves these challenges by decoupling chemical reactant adsorption from reaction product removal, enabling fine depth control, low roughness, and reduced-damage etching across both directional plasma and isotropic thermal regimes.
The two saturation tests answer different questions. A modification-dose sweep shows whether reactive sites have filled; an activation sweep shows whether modified material is removed without crossing into appreciable attack of the underlying surface. Both tests must be repeated on representative patterned structures because a blanket-wafer plateau can coexist with under-dose, incomplete purge, charging, redeposition, or slow product evacuation at the bottom of a high-aspect-ratio feature.
The useful window is process-specific. Modification lowers the removal threshold of the reacted surface; ALE behavior exists only where that layer leaves while unmodified material remains comparatively stable. Ion-energy spread, incomplete saturation, spontaneous chemical etching and redeposition blur both boundaries, so an experimentally measured plateau and synergy—not a nominal energy setting—establish the window.
Self-limiting half-reactions govern layer-by-layer digital removal in atomic layer etching. In classic reactive ion etching (RIE), chemical etching radicals and energetic ions strike the wafer surface simultaneously, creating continuous, uncontrollable etching profiles susceptible to microloading and micro-trenching. ALE replaces this continuous regime with two distinct, self-limiting steps comprising surface modification (where reactive halogens like $\text{Cl}_2$ or $\text{NF}_3$ chemisorb and alter the topmost 1 to 2 atomic layers) followed by product desorption (where low-energy $\text{Ar}^+$ ions or thermal ligand-exchange vapors selectively desorb the modified layer and abruptly halt).
ALE synergy defines the degree of self-limiting ideality and process controllability. The performance of an atomic layer etching process is quantified by the dimensionless ALE Synergy metric ($S$):
Here, $\text{EPC}_{\text{mod}}$ is the spontaneous chemical etch rate during the modification pulse alone, and $\text{EPC}_{\text{des}}$ is the physical sputtering rate during the desorption pulse alone. An idealized ALE process approaches $S=1$ because neither half-step removes appreciable material alone. Real processes report measured synergy with uncertainty and test it across dose, purge, energy, pattern density, and feature depth; no universal percentage defines ALE.
Directional plasma ALE exploits the ion energy window between desorption and sputtering. In directional plasma ALE, anisotropic feature profiles are achieved by directing low-energy $\text{Ar}^+$ ions perpendicular to the wafer substrate. Process engineers seek an ALE energy window bounded below by the modified-layer removal threshold and above by appreciable sputtering or damage of the unmodified surface. Those thresholds are distributions and depend on material, surface state, ion species, angle, and reactor conditions; they must be measured for the actual stack. Operating below the sputtering threshold reduces physical damage and mask erosion relative to operation above the sputtering threshold; selectivity remains material- and recipe-dependent.
Thermal isotropic ALE uses sequential fluorination and ligand-exchange coordination chemistry. For complex 3D nanostructures requiring uniform isotropic lateral recess, thermal ALE operates entirely without energetic plasma ions. In the thermal ALE of aluminum oxide ($\text{Al}_2\text{O}_3$), hydrogen fluoride ($\text{HF}$) fluorinates the oxide surface into an aluminum fluoride ($\text{AlF}_3$) layer. In the subsequent step, a metal-organic precursor such as Trimethylaluminum ($\text{Al(CH}_3)_3$) or Tin(II) acetylacetonate ($\text{Sn(acac)}_2$) undergoes transmetalation ligand exchange, reacting with $\text{AlF}_3$ to form volatile organometallic compounds ($\text{AlF(CH}_3)_2\uparrow$) that vaporize into the vacuum exhaust.
| ALE Process Module | Reactant Pairing | Operating Temperature | Etch Per Cycle (EPC) | Etch Selectivity | Primary Semiconductor Implementation |
|---|---|---|---|---|---|
| Directional Silicon ALE | $\text{Cl}_2\ \text{adsorption} + \text{Ar}^+\ \text{ions (30 eV)}$ | Room Temp ($20^\circ\text{C}\text{--}60^\circ\text{C}$) | $0.6\text{--}1.0\text{ \AA/cycle}$ | $> 100:1$ to $\text{SiO}_2/\text{Si}_3\text{N}_4$ | FinFET & GAA fin trimming and gate recess |
| Directional Dielectric ALE | $\text{C}_4\text{F}_8/\text{Ar}\ \text{deposition} + \text{Ar}^+\ \text{activation}$ | $20^\circ\text{C}\text{--}80^\circ\text{C}$ | $0.4\text{--}0.8\text{ \AA/cycle}$ | $> 50:1$ $\text{SiO}_2$ over $\text{Si}_3\text{N}_4$ | Self-Aligned Contact (SAC) hole opening |
| Thermal Isotropic $\text{Al}_2\text{O}_3 / \text{HfO}_2$ | $\text{HF} / \text{XeF}_2 + \text{Al(CH}_3)_3 / \text{Sn(acac)}_2$ | $150^\circ\text{C}\text{--}300^\circ\text{C}$ | $0.5\text{--}1.2\text{ \AA/cycle}$ | Near-infinite to $\text{Si} / \text{SiO}_2$ | High-k gate dielectric recess & cleanup |
| Sacrificial $\text{SiGe}$ Cavity Recess | $\text{CF}_4/\text{O}_2\ \text{radicals} + \text{organic vapor}$ | $60^\circ\text{C}\text{--}120^\circ\text{C}$ | $0.8\text{--}1.5\text{ \AA/cycle}$ | $> 150:1\ \text{SiGe}:\text{Si}$ | GAA nanosheet inner spacer cavity formation |
| Metal ALE ($\text{Cu} / \text{Ru} / \text{Co}$) | $\text{Cl}_2 / \text{O}_2\ \text{oxidation} + \text{hfac / acetylacetone}$ | $120^\circ\text{C}\text{--}250^\circ\text{C}$ | $0.3\text{--}0.6\text{ \AA/cycle}$ | $> 80:1$ to dielectrics | Dual Damascene via bottom clean & 3D packaging |
Atomic layer etching eliminates aspect-ratio-dependent etching lag across deep nanostructures. In conventional reactive ion etching of high-aspect-ratio holes and trenches ($AR > 40:1$), neutral Knudsen diffusion throttling starves deep feature floors of chemical etchants, causing narrow trenches to etch far slower than wide fields. Because ALE separates modification from removal, saturation exposure and purge time can reduce pattern-dependent etch-rate variation. Deep or narrow features can still be transport-limited, however: radicals, ions and volatile products must reach or leave the feature before each half-cycle is complete. ALE can suppress ARDE and microloading within a qualified window; it does not eliminate them by definition.
Separating modification from removal is the core control mechanism. Inside a deep feature, however, self-limiting chemistry still requires enough reactant dose, ion or ligand access, purge conductance, and product removal to reach saturation at the bottom. ALE stops after available modified sites are consumed; it does not make transport limitations disappear.
Read ALE through a saturation-and-synergy lens: modification dose must saturate every accessible surface, purge must separate the half-cycles, activation must remove the modified layer without appreciably attacking the underlying material, and products must escape. Atomic-scale average EPC is useful only when selectivity, roughness, damage, feature-depth uniformity, and defectivity remain inside the integration budget.