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Posts Tagged ‘chamber’

Mechanistic Modeling of Silicon ALE for FinFETs

Tuesday, April 25th, 2017

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With billions of device features on the most advanced silicon CMOS ICs, the industry needs to be able to precisely etch atomic-scale features without over-etching. Atomic layer etching (ALE), can ideally remove uniform layers of material with consistent thickness in each cycle, and can improve uniformity, reduce damage, increase selectivity, and minimize aspect ratio dependent etching (ARDE) rates. Researchers Chad Huard et al. from the University of Michigan and Lam Research recently published “Atomic layer etching of 3D structures in silicon: Self-limiting and nonideal reactions” in the latest issue of the Journal of Vacuum Science & Technology A (http://dx.doi.org/10.1116/1.4979661). Proper control of sub-cycle pulse times is the key to preventing gas mixing that can degrade the fidelity of ALE.

The authors modeled non-idealities in the ALE of silicon using Ar/Cl2 plasmas:  passivation using Ar/Cl2 plasma resulting in a single layer of SiClx, followed by Ar-ion bombardment to remove the single passivated layer. Un-surprisingly, they found that ideal ALE requires self-limited processes during both steps. Decoupling passivation and etching allows for several advantages over continuous etching, including more ideal etch profiles, high selectivity, and low plasma-induced damage. Any continuous etching —when either or both process steps are not fully self-limited— can cause ARDE and surface roughness.

The gate etch in a finFET process requires that 3D corners be accurately resolved to maintain a uniform gate length along the height of the fin. In so doing, the roughness of the etch surface and the exact etch depth per cycle (EPC) are not as critical as the ability of ALE to be resistant to ARDE. The Figure shows that the geometry modeled was a periodic array of vertical crystalline silicon fins, each 10nm wide and 42nm high, set at a pitch of 42 nm. For continuous etching (a-c), simulations used a 70/30 mix of Ar/Cl gas and RF bias of 30V. Just before the etch-front touches the underlying SiO2 (a), the profile has tapered away from the trench sidewalls and the etch-front shows some micro-trenching produced by ions (or hot neutrals) specularly reflected from the tapered sidewalls. After a 25% over-etch (b), a significant amount of Si remains in the corners and on the sides of the fins. Even after an over-etch of 100% (c), Si still remains in the corners.

FIGURE CAPTION: Simulated profiles resulting from etching finFET gates with (a)–(c) a continuous etching process, or (d)–(f) an optimized ALE process. Time increases from left to right, and images represent equal over-etch (as a percentage of the time required to expose the bottom SiO2) not equal etch times. Times listed for the ALE process in (d)–(f) represent plasma-on, ignoring any purge or dwell times. (Source: J. Vac. Sci. Technol. A, Vol. 35, No. 3, May/Jun 2017)

In comparison, the ALE process (d-f) shows that after 25% over-etch (e) the bottom SiO2 surface would be almost completely cleared with minimal corner residues, and continuing to 100% over-etch results in little change to the profile. The ALE process times shown here do not include the gas purge and fill times between plasma pulses; to clear the feature using ALE required 200 pulses and assuming 5 seconds of purge time between each pulse results in a total process time of 15–20 min to clear the feature. This is a significant increase in total process time over the continuous etch (2 min).

One conclusion of this ALE modeling is that even small deviations from perfectly self-limited reactions significantly compromise the ideality of the ALE process. For example, having as little as 10 ppm Cl2 residual gas in the chamber during the ion bombardment phase produced non-idealities in the ALE. Introducing any source of continuous chemical etching into the ALE process leads to the onset of ARDE and roughening of the etch front. These trends have significant implications for both the design of specialized ALE chambers, and also for the use of ALE to control uniformity.

—E.K.

Picosun and Hitachi MECRALD Process

Friday, February 24th, 2017

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By Ed Korczynski, Sr. Technical Editor

A new microwave electron cyclotron resonance (MECR) atomic layer deposition (ALD) process technology has been co-developed by Hitachi High-Technologies Corporation and Picosun Oy to provide commercial semiconductor IC fabs with the ability to form dielectric films at lower temperatures. Silicon oxide and silicon nitride, aluminum oxide and aluminum nitride films have been deposited in the temperature range of 150-200 degrees C in the new 300-mm single-wafer plasma-enhanced ALD (PEALD) processing chamber.

With the device features within both logic and memory chips having been scaled to atomic dimensions, ALD technology has been increasingly enabling cost-effective high volume manufacturing (HVM) of the most advanced ICs. While the deposition rate will always be an important process parameter for HVM, the quality of the material deposited is far more important in ALD. The MECR plasma source provides a means of tunable energy to alter the reactivity of ALD precursors, thereby allowing for new degrees of freedom in controlling final film properties.

The Figure shows the MECRALD chamber— Hitachi High-Tech’s ECR plasma generator is integrated with Picosun’s digitally controlled ALD system—from an online video (https://youtu.be/SBmZxph-EE0) describing the process sequence:

1.  first precursor gas/vapor flows from a circumferential ring near the wafer chuck,

2.  first vacuum purge,

3.  second precursor gas/vapor is ionized as it flows down through the ECR zone above the circumferential ring, and

4.  second vacuum purge to complete one ALD cycle (which may be repeated).

Cross-sectional schematic of a new Microwave Electron Cyclotron Resonance (MECR) plasma source from Hitachi High-Technologies connected to a single-wafer Atomic Layer Deposition (ALD) processing chamber from Picosun. (Source: Picosun)

The development team claims that MECRALD films are superior to other PEALD films in terms of higher density, lower contamination of carbon and oxygen (in non-oxides), and also show excellent step-coverage as would be expected from a surface-driven ALD process. The relatively density of these films has been confirmed by lower wet etch rates. The single-wafer process non-uniformity on 300mm wafers is claimed at ~1% (1 sigma). The team is now exploring processes and precursors to be able to deposit additional films such as titanium nitride (TiN), tantalum nitride (TaN), and hafnium oxide (HfO). In an interview with Solid State Technology, a spokesperson from Hitachi High-Technologies explained that, “We are now at the development stage, and the final specifications mainly depend on future achievements.”

The MECR source has been used in Hitachi High-Tech’s plasma chamber for IC conductor etch for many years, and is able to generate a stable high-density plasma at very low pressure (< 0.1 Pa). MECR plasmas provide wide process windows through accurate plasma parameter management, such as plasma distribution or plasma position control. The same plasma technology is also used to control ions and radicals in the company’s dry cleaning chambers.

“I’m really impressed by the continuous development of ALD technology, after more than 40 years since the invention,” commented Dr. Tuomo Suntola, and the famous inventor and patentor of the Atomic Layer Deposition method in Finland in 1974, and member of the Picosun board of directors. “Now combining Hitachi and Picosun technologies means (there is) again a major breakthrough in advanced semiconductor manufacturing.”

MECRALD chambers can be clustered on a Picosun platform that features a Brooks robot handler. This technology is still under development, so it’s too soon to discuss manufacturing parameters such as tool cost and wafer throughput.

—E.K.

Applied Materials Releases Selective Etch Tool

Wednesday, June 29th, 2016

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By Ed Korczynski, Sr. Technical Editor

Applied Materials has disclosed commercial availability of new Selectra(TM) selective etch twin-chamber hardware for the company’s high-volume manufacturing (HVM) Producer® platform. Using standard fluorine and chlorine gases already used in traditional Reactive Ion Etch (RIE) chambers, this new tool provides atomic-level precision in the selective removal of materials in 3D devices structures increasingly used for the most advanced silicon ICs. The tool is already in use at three customer fabs for finFET logic HVM, and at two memory fab customers, with a total of >350 chambers planned to have been shipped to many customers by the end of 2016.

Figure 1 shows a simplified cross-sectional schematic of the Selectra chamber, where the dashed white line indicates some manner of screening functionality so that “Ions are blocked, chemistry passes through” according to the company. In an exclusive interview with Solid State Technology, company representative refused to disclose any hardware details. “We are using typical chemistries that are used in the industry,” explained Ajay Bhatnagar, managing director of Selective Removal Products for Applied Materials. “If there are specific new applications needed than we can use new chemistry. We have a lot of IP on how we filter ions and how we allow radicals to combine on the wafer to create selectivity.”

FIG 1: Simplified cross-sectional schematic of a silicon wafer being etched by the neutral radicals downstream of the plasma in the Selectra chamber. (Source: Applied Materials)

From first principles we can assume that the ion filtering is accomplished with some manner of electrically-grounded metal screen. This etch technology accomplishes similar process results to Atomic Layer Etch (ALE) systems sold by Lam, while avoiding the need for specialized self-limiting chemistries and the accompanying chamber throughput reductions associated with pulse-purge process recipes.

“What we are doing is being able to control the amount of radicals coming to the wafer surface and controlling the removal rates very uniformly across the wafer surface,” asserted Bhatnagar. “If you have this level of atomic control then you don’t need the self-limiting capability. Most of our customers are controlling process with time, so we don’t need to use self-limiting chemistry.” Applied Materials claims that this allows the Selectra tool to have higher relative productivity compared to an ALE tool.

Due to the intrinsic 2D resolutions limits of optical lithography, leading IC fabs now use multi-patterning (MP) litho flows where sacrificial thin-films must be removed to create the final desired layout. Due to litho limits and CMOS device scaling limits, 2D logic transistors are being replaced by 3D finFETs and eventually Gate-All-Around (GAA) horizontal nanowires (NW). Due to dielectric leakage at the atomic scale, 2D NAND memory is being replaced by 3D-NAND stacks. All of these advanced IC fab processes require the removal of atomic-scale materials with extreme selectivity to remaining materials, so the Selectra chamber is expected to be a future work-horse for the industry.

When the industry moves to GAA-NW transistors, alternating layers of Si and SiGe will be grown on the wafer surface, 2D patterned into fins, and then the sacrificial SiGe must be selectively etched to form 3D arrays of NW. Figure 2 shows the SiGe etched from alternating Si/SiGe stacks using a Selectra tool, with sharp Si corners after etch indicating excellent selectivity.

FIG 2: SEM cross-section showing excellent etch of SiGe within alternating Si/SiGe layers, as will be needed for Gate-All-Around (GAA) horizontal NanoWire (NW) transistor formation. (Source: Applied Materials)

“One of the fundamental differences between this system and old downstream plasma ashers, is that it was designed to provide extreme selectivity to different materials,” said Matt Cogorno, global product manager of Selective Removal Products for Applied Materials. “With this system we can provide silicon to titanium-nitride selectivity at 5000:1, or silicon to silicon-nitride selectivity at 2000:1. This is accomplished with the unique hardware architecture in the chamber combined with how we mix the chemistries. Also, there is no polymer formation in the etch process, so after etching there are no additional processing issues with the need for ashing and/or a wet-etch step to remove polymers.”

Systems can also be used to provide dry cleaning and surface-preparation due to the extreme selectivity and damage-free material removal.  “You can control the removal rates,” explained Cogorno. “You don’t have ions on the wafer, but you can modulate the number of radicals coming down.” For HVM of ICs with atomic-scale device structures, this new tool can widen process windows and reduce costs compared to both dry RIE and wet etching.

—E.K.