Ion Getter Pump
A pump with no moving parts, no oil, and no exhaust — it buries the gas inside itself forever.
Maintains ultra-high vacuum (UHV) in sealed chambers — from particle accelerators and surface-science instruments to satellite ion thrusters and quantum computers — by continuously removing residual gas without any mechanical moving parts, oil, or cryogen. Once switched on and handed a pressure below about 10⁻⁴ mbar, it can hold a chamber at 10⁻¹¹ mbar essentially indefinitely.
Inside the pump, an array of short cylindrical anode cells sits between two flat titanium cathode plates, all immersed in a permanent magnetic field of roughly 0.1–0.2 T. A high voltage of 3–7 kV is applied to the anodes. Stray electrons spiral into helical orbits along the magnetic field lines — a Penning discharge — and collide with residual gas molecules, ionising them. The resulting positive ions accelerate toward the grounded titanium cathodes at high energy, doing two things simultaneously: they implant themselves physically into the titanium (pumping noble gases such as argon), and they sputter fresh titanium atoms onto surrounding surfaces. That freshly deposited titanium film is highly chemically reactive, chemisorbing active gases like nitrogen, oxygen, hydrogen, carbon monoxide, and water vapour on contact. Both mechanisms permanently remove gas from the chamber with no exhaust path.
In plain terms
Imagine a vacuum cleaner that, instead of a bag, melts the dust into the walls so it can never come back out. That's what an ion getter pump does to air molecules — it zaps them, flings them at a metal plate, and the metal swallows them permanently.
Also called: sputter ion pump, SIP, VacIon pump, ion pump.
Why it matters
- Zero moving parts means zero vibration — critical in scanning-tunnelling microscopes, gravitational-wave detectors, and atom interferometers where mechanical noise destroys measurements.
- No oil or cryogen is introduced, so the vacuum stays hydrocarbon-free and the chamber never needs warming for pump maintenance.
- The pump current is directly proportional to pressure, making every ion pump a built-in pressure gauge at no extra cost.
- Operates silently inside particle accelerator beamlines — CERN's Large Hadron Collider uses thousands of distributed ion pumps to maintain its 10⁻¹⁰ mbar beam vacuum over 27 km.
- Pumping speed is available from 2 L/s (miniature appendage pumps) up to 2,500 L/s, covering almost every UHV application.
Where it lives
- CERN Large Hadron Collider beam vacuum (thousands of units over 27 km)
- LIGO gravitational-wave interferometers (custom 2,500 L/s units)
- Molecular-beam epitaxy (MBE) growth chambers
- Scanning-tunnelling and atomic-force microscopes
- Synchrotron light source storage rings
- Satellite ion-thruster test facilities
Key numbers
- Operating range: 10⁻⁴ to 10⁻¹¹ mbar (Handed off from a turbomolecular pump at the upper end)
- Pumping speed (N₂): 2 – 2,500 L/s (Commercial range; Gamma Vacuum TiTan series to 1,600 L/s)
- Anode voltage: 3 – 7 kV (Controller adjusts with pressure for efficiency)
- Magnetic field: 0.1 – 0.2 T (Permanent ferrite or Alnico magnets, external to vacuum)
- Startup pressure: ≤ 10⁻⁴ mbar (Requires prior roughing by turbo or sorption pump)
- StarCell cathode life: 80,000 h @ 10⁻⁶ mbar (Diode element: 50,000 h)
Surprising facts
- An ion getter pump operates across a pressure span of seven orders of magnitude — from 10⁻⁴ mbar (where it starts) down to 10⁻¹¹ mbar — without any adjustment other than applying high voltage.
- The pump has no exhaust. Gas pumped in 1960 is still entombed in the same titanium cathode today — the pump is literally a graveyard for molecules.
- A StarCell-element pump can run continuously for 80,000 hours (over nine years) at 10⁻⁶ mbar before the titanium cathode is consumed through.
- The pump doubles as a pressure gauge: the ion current flowing to ground is proportional to chamber pressure down to around 10⁻¹⁰ mbar, enabling pressure readout with no separate instrument.
A short history
The sputter ion pump was invented at Varian Associates in Silicon Valley. Robert Jepsen, Lewis Hall, and John Helmer filed the foundational patent in 1957, initially to maintain UHV inside microwave klystron tubes after processing. The pump leveraged the Penning discharge — a plasma confinement geometry described by Frans Penning in the 1930s — and replaced the titanium Penning gauge cathode with a thick, long-lived getter target. By 1960 Varian was selling commercial units with honeycomb anodes and pumping speeds in the thousands of litres per second. The triode geometry (W. Brubaker, Consolidated Electrodynamics, 1960) solved the argon-instability problem of diode pumps for noble-gas environments. In 1983 Varian introduced the StarCell cathode structure — titanium fins arranged radially — which achieved the longest cathode life and best noble-gas pumping of any diode geometry. Agilent Technologies acquired Varian's vacuum division in 2010 and continues to manufacture the VacIon Plus family.
Sources
- Agilent Technologies — Sputter Ion Pumps: A 60 Year History (https://www.agilent.com/cs/library/periodicals/public/Agilent-Ion-Pump-History.pdf)
- Agilent VacIon Plus product catalog (via Ideal Vacuum) (https://www.idealvac.com/files/literature/06_Ion_Pumps.pdf)
- Edwards Vacuum — Working with Ion Getter Pumps (https://www.edwardsvacuum.com/en-uk/vacuum-pumps/knowledge/applications/working-with-ion-getter-pumps)
- USPAS Fermilab — Ion Pump lecture notes (Yulin Li) (https://uspas.fnal.gov/materials/13Duke/USPASVacuumSession3_2AIonPumps.pdf)
- CERN Accelerator School — Ion Getter Pumps (Maccarrone, 2017) (https://cas.web.cern.ch/sites/default/files/lectures/glumslov-2017/maccarrone.pdf)