The difference between evaporation coating and sputtering coating is decided by the physics of atom delivery. Both are physical vapor deposition (PVD) processes run inside vacuum chambers, yet evaporation pushes fast, line-of-sight vapor while sputtering throws energetic atoms that pack into dense, hard films. Three numbers tell the story: arriving atom energy, finished film density, and deposition rate.
Content
In one sentence: evaporation coating builds films by heating source material until it vaporizes and condenses on the workpiece, while sputtering coating builds films by bombarding a solid target with ions until atoms are ejected and land hard enough to pack densely.
Everything else follows from that start: evaporation runs in deeper vacuum with no process gas and favors pure metals and simple optical stacks, while sputtering runs in an argon plasma and handles alloys, nitrides, oxides, and hard carbon. The table condenses the parameters.
| Parameter | Evaporation Coating | Sputtering Coating |
| Driving force | Resistive or e-beam heat vaporizes the source | Argon ion bombardment ejects target atoms |
| Process pressure | 10^-5 to 10^-6 mbar, no process gas | 0.3 to 1 Pa in an argon plasma |
| Typical rate on aluminum | 10-100 nm per second | 1-10 nm per second |
| Arriving atom energy | 0.1-0.5 eV | 1-10 eV |
| Film density | 85-95% of bulk | 95-100% of bulk |
| Best-fit materials | Al, Ag, Au, MgF2, organics | TiN, TiAlN, CrN, ITO, DLC, Ta-C |
Both processes start with a pumped-down chamber and end with a condensing film; the separation happens in the middle, where heat and plasma push atoms in fundamentally different ways.
Once the chamber reaches roughly 10^-5 mbar, a resistive boat, crucible, or electron beam lifts the source above its vapor point. Atoms leave the melt, cross the vacuum without striking gas molecules, and stick where they first land. That line-of-sight flight means shadowed areas stay bare unless fixtures rotate, so evaporated films cover flat panels far better than threads or deep pockets. Alloy sources also fractionate: nickel and chromium leave the melt at different rates, so film composition drifts from source composition.
A sputtering system backfills the chamber with argon at 0.3 to 1 Pa and strikes a plasma. A magnetron cathode behind the target traps electrons, holding the discharge stable at moderate voltage. Argon ions cross the sheath, strike the target, and eject roughly one atom per incident ion. Those atoms leave with 1 to 10 eV, enough to migrate and rearrange on the surface. Add nitrogen or oxygen and the same machine becomes a reactive line for TiN, TiAlN, CrN, or ITO; switch to RF power and even insulating targets deposit cleanly.
Sputtered films are denser, stick harder, and follow complex shapes better because sputtered atoms arrive with 10 to 30 times the kinetic energy of evaporated atoms.
Evaporated atoms land at 0.1 to 0.5 eV, barely enough to migrate across a surface, so at low substrate temperature they form columnar, porous films at 85 to 95 percent of bulk density. Such films pass mirror inspections but can fail humidity and abrasion tests. Sputtered atoms arrive at 1 to 10 eV, migrate, refill voids, and consolidate above 95 percent density, which is why scratch-test critical loads on sputtered nitrides run markedly higher.
Step coverage follows the same logic: line-of-sight vapor shadows reentrant corners, while scattered plasma flux with part rotation wraps edges. Hard carbon films such as DLC and Ta-C sit at the extreme of this logic and only form under energetic flux, which is why no thermal evaporation source produces them.
Evaporation deposits material roughly ten times faster and costs less to buy, while sputtering wastes less consumable per good part and cuts rework on demanding products.
An electron-beam source lays aluminum at 10 to 100 nm per second against 1 to 10 for a production magnetron, so reflective metallization on lighting reflectors, plastic trim, and packaging webs still belongs to evaporation. The trade sits in consumables and capital: planar targets surrender 25 to 35 percent of their mass before replacement, e-beam skulls lock away part of each melt, and sputtering machines carry plasma supplies, cooling, and matching networks that raise purchase price. Maintenance splits the same way: boats, liners, and filaments versus target changes and shield cleaning.
Choose evaporation for fast, bright metal and optical layers on flat parts; choose sputtering for hard, functional, large-area films that must survive wear, humidity, or heat.
| Product Family | Best-Fit Process | Reason |
| Reflective aluminum on lighting and trim | Evaporation | Fastest metallization, lowest cost per cycle |
| Optical lens stacks | Evaporation with ion assist | Dense layers at high rate |
| Cutting tools and forming dies | Reactive sputtering | TiAlN and CrN need plasma chemistry |
| Watch cases, faucets, hardware | Sputtering | Wear-proof decorative color |
| Low-E glass and display ITO | Sputtering | Large-area uniformity, stable stoichiometry |
| DLC and Ta-C on automotive parts | Sputtering or arc | Energetic carbon flux required |
A short feasibility sequence prevents the most expensive purchasing mistake, which is buying hardware around the wrong film property.
Sputtering. Atoms arrive at 1 to 10 eV rather than 0.1 to 0.5 eV, so films densify and bond far more aggressively, which shows up as higher critical loads in scratch testing and better survival in humidity cycling.
Hybrid chambers exist and suit mixed portfolios such as optical plus decorative work, but they cost more and compromise pumping and source geometry. Plants with a clear product family usually buy dedicated tools.
Momentum transfer ejects roughly one target atom per incident ion at typical energies, so rate is bounded by discharge current and material yield. Throughput recovers through multiple cathodes, planetary rotation, pulsed power, and higher-yield targets.
No. Purchase price and source material are cheaper, but for wear parts the rework and field failures erase the savings. Compare cost per good part over three years, including consumables and service.

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