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Plasma processing for MEMS: deep etching, release and the stiction problem

By Vvon Engineering Team | Published | Updated

MEMS devices fail at the last step more often than the first. A practical walk through deep silicon etching, the release step, why released structures stick down, and a full process sequence for a simple cantilever.

Nanotechnology RFQ checklist (TXT)

A MEMS device can pass lithography and etch inspection yet fail to move after release. Capillary forces during drying, residue and later surface adhesion can cause stiction. Plan release, drying, storage and functional verification alongside the etch process.

This is a walk through the plasma steps that build a MEMS device and the wet and dry steps that decide whether it moves, written for groups setting up microfabrication in a Bangladeshi university.

Why MEMS breaks the habits of planar processing

Integrated circuit processing works with thin films and shallow features, and everything stays attached to the substrate for life. MEMS turns both assumptions over. Structures are tens of microns deep with aspect ratios in the tens to one. More importantly, part of the device has to be freed from the substrate so it can bend, resonate or rotate. That release step, and the drying that follows it, has no equivalent in IC work, and it is where the process sequence has to be designed rather than copied.

The practical consequence: you cannot judge a MEMS process by looking at the wafer halfway through. A batch that looks perfect under an optical microscope after etching can be entirely dead after release.

Deep etching: the Bosch process and its alternatives

Deep reactive ion etching gets vertical walls in silicon by alternating two steps in an inductively coupled plasma. An etch step, usually SF6, removes silicon almost isotropically for a few seconds. A passivation step, usually C4F8, deposits a thin fluorocarbon polymer over every surface. On the next etch step, directional ions strip that polymer from the trench floor while the sidewalls stay coated, so the etch advances downward and not sideways. Repeat several hundred times.

The signature of this process is scalloping: a ripple on the sidewall with a period set by the cycle time. Shorten the cycles and the scallops get smaller at the cost of etch rate. That trade matters if the sidewall is an optical surface or a capacitor plate, and matters much less if it is a structural wall.

The release step

Release means removing the sacrificial material underneath the moving structure. The two routes commonly used in a university lab:

Sacrificial layerRelease chemistryNatureWatch out for
Silicon dioxideHydrofluoric acid, liquidWet, isotropicTiming, anchor undercut, and the drying step that follows
Silicon dioxideAnhydrous vapour HFDry, isotropicWater management, condensation, needs dedicated equipment
SiliconXenon difluoride vapourDry, isotropic, very selective to oxide, nitride and aluminiumRoughening of the etched silicon surface, pulsed dosing

Release is timed, and the timing is unforgiving in both directions. Too short and the structure is still tethered. Too long and the same isotropic etch that freed the beam eats into the anchor that was supposed to hold it. Put release test structures of graduated width on every mask so you can read the completed undercut optically before committing the real devices.

Stiction, and the ways out of it

When a wet released device is pulled out of a rinse and left to dry, the liquid between the structure and the substrate forms a meniscus. Surface tension in that meniscus pulls the beam down with a force that easily exceeds its restoring stiffness. The beam touches the substrate, and once in contact it is held by van der Waals forces, hydrogen bonding and any residue in the gap. In most cases it never comes back up. That is release stiction, and it is a physics problem, not a workmanship problem: careful handling does not avoid it.

There are four ways out, and a good process uses more than one.

  1. Remove the liquid to vapour interface. Critical point drying is the standard answer: exchange water for isopropyl alcohol, exchange alcohol for liquid carbon dioxide in a pressure vessel, then take the carbon dioxide around its critical point so it leaves as a gas without ever forming a meniscus. A critical point dryer is an inexpensive item beside an etcher and it is the difference between working devices and a drawer of stuck ones.
  2. Sublimation drying. Exchange into a solvent that freezes and sublimes, then let it leave the solid phase directly. Cheaper than critical point drying, slower, and workable for teaching devices with generous gaps.
  3. Avoid the liquid entirely. Vapour HF or xenon difluoride release never puts liquid in the gap. This is the cleanest solution where the material stack allows it.
  4. Change the surface and the design. A self-assembled monolayer or a thin fluorocarbon film deposited from a C4F8 plasma makes both surfaces water repellent, which reduces both release stiction and later in-use sticking. On the layout side: dimples or standoff bumps under the beam to cut contact area, release holes through wide plates so the etchant reaches the middle and the plate does not act as a squeeze film, and beams stiff enough that the restoring force wins.

In-use stiction is a separate and very local problem. Water adsorbed from humid air condenses in the narrow gap between a released structure and its substrate and pulls the two together long after fabrication. In Dhaka, that is not a rare failure mode, it is a risk to assess for an unpackaged device in humid storage. Store released dies in a nitrogen purged dry cabinet from the moment they leave the dryer, and treat that cabinet as process equipment rather than furniture.

A working sequence for a simple cantilever

For an initial silicon-on-insulator project, agree these milestones with the facility's process and safety teams. They describe the capability required, not a recipe for operating an etcher or handling release chemicals.

Inspection deserves a note. A variable pressure SEM such as the Hitachi SU3800/SU3900 lets you image insulating and lightly charging samples without sputtering a conductive coating on them. For released MEMS that matters, because a gold coating adds stress to a thin beam and changes the very thing you were trying to measure.

Where university MEMS projects usually stall

Technical references

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