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Dr. G. Mirjalili, Physics Dept. Yazd University Vacuum techniques Pumps

Vacuum Pump

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  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Vacuum techniques

    Pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Vacuum theory and pumping laws

    How the vacuum is created?

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    to reduce gas density in given volume to below atmospheric pressure with pump

    enclosed vessel has continuous sources which launch gas into volume and present pump with continuous gas load

    vacuum achievable at steady state is result of dynamic balance between gas load and ability of pump to remove gas form volume

    Production of vacuumProduction of vacuum

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Vacuum pumps and their characteristics

    Gas transfer pumps:(a) Positive displacement pumps that transfer

    repeated volumes of gas from inlet to outlet by compression ( e.g. rotary pump).

    (b) Kinetic pumps that continuously transfer gas from inlet to outlet by imparting momentum to gas molecules (e.g. Diffusion pump, turbomolecular pump).

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Entrapment/capture pumps,

    retain molecules by sorption or condensation on internal surfaces (e.g. sorption pump, sublimation pump, sputter ion pump, cryogenic pump).

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Low vacuum pumps (1atm-10-3)

    mbarRoughing Pumps

    1

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ultrahigh Vacuum High Vacuum Rough Vacuum

    Typical HighPressure

    Typical Low Pressure

    Vacuum (units)

    1 atm.1.3x10-31.3x10-61.3x10-9

    760 Torr1 Torr1 mTorr1x10-6 Torr

    1 Torr =1 mm-Hg

    101,333 Pa133 Pa0.133 Pa0.133x10-3 Pa

    1 Pascal =1 N/m2

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    VACUUM PUMPING METHODS

    Sliding VaneRotary Pump

    MolecularDrag Pump

    TurbomolecularPump

    Fluid EntrainmentPump

    VACUUM PUMPS(METHODS)

    ReciprocatingDisplacement Pump

    Gas TransferVacuum Pump

    DragPump

    EntrapmentVacuum Pump

    Positive DisplacementVacuum Pump

    KineticVacuum Pump

    RotaryPump

    DiaphragmPump

    PistonPump

    Liquid RingPump

    RotaryPiston Pump

    RotaryPlunger Pump

    RootsPump

    Multiple VaneRotary Pump

    DryPump

    AdsorptionPump

    Cryopump

    GetterPump

    Getter IonPump

    Sputter IonPump

    EvaporationIon Pump

    Bulk GetterPump

    Cold TrapIon TransferPump

    Gaseous Ring Pump

    TurbinePump

    Axial FlowPump

    Radial FlowPump

    EjectorPump

    Liquid JetPump

    Gas JetPump

    Vapor JetPump

    DiffusionPump

    DiffusionEjector Pump

    Self PurifyingDiffusion Pump

    FractionatingDiffusion Pump

    Condenser

    SublimationPump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Name of Pump Mechanism of PumpingMechanical (roughing)* Compression of gasSorption Physical or chemical absorption Diffusion* Intermolecular collisions Turbo Molecular collisions with surfacesIon Ionization and implantation of gasCryo(genic) Solidification of gas by liquid He *used in lab

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    PUMP OPERATING RANGES

    10-12 10-10 10-8 10-6 10-4 10-2 1 10+2P (mbar)

    Rough VacuumHigh VacuumUltra High Vacuum

    Venturi Pump

    Rotary Vane Mechanical PumpRotary Piston Mechanical Pump

    Sorption PumpDry Mechanical Pump

    Blower/Booster Pump

    High Vac. PumpsUltra-High Vac. Pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    VACUUM SYSTEM USE

    1

    2

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    5

    9

    8

    8

    7

    1233a456789

    ChamberHigh Vac. PumpRoughing PumpForeline PumpHi-Vac. ValveRoughing ValveForeline ValveVent ValveRoughing GaugeHigh Vac. Gauge

    7

    33a

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Mechanical pumps Mechanical pumps (displacement pumps) remove gas atoms

    from the vacuum system and expel them to atmosphere, either directly or indirectly

    In effect, they are compressors and one can define a compression ratio, K, given by

    K is a fixed value for any given pump for a particular gas species when measured under conditions of zero gas flow.

    out

    in

    PKP

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Rotary Vane, Oil-Sealed Mechanical Pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pump Mechanism

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Gas ballastting

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pump Down Curves

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    The Molecular Sieve/Zeolite Trap

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Rotary pump Trap

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Single &Dual Stage

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    How 2-stage rotary pump Works

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    OIL BACKSTREAMING

    2

    PRESSURE LEVELS: LESS THAN 0.2 mbar

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Other types of Mechanical pumps

    Rotary Piston

    Roots

    Rotary Vane

    Dry pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Dry Vacuum Pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Root pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    How Root Pump works

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    One Stage Roots Blower Pump Assembly

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Vacuum system use for Root pumps

    123456789

    101112

    ChamberForelineRoughing ValveRoughing GaugeRoughing PumpForelineForeline ValveForeline GaugeHigh Vacuum ValveBooster/BlowerVent ValveHigh Vacuum Gauge

    1

    9

    3

    12

    4

    11

    5

    2

    678

    10

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diaphragm pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diaphragm pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diaphragm Pump Eccentric shaft produces

    alternate expansion / compression process

    Inlet / outlet via reed valves

    Ultimate vacuum 100 - 0.1 torr - limited by external leakage past valves, internal back-streaming, dead volume

    Compression ratio typically 10 - 30

    Pumping speed: single unit 0.1-0.7 l/s, parallel units up to 5.3 l/s

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diaphragm Pump

    High resistance to chemical attack

    Oil free - used with roots blower or cryopump for completely oil-free system

    Lifetime ~ 5000 hours

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diaphragm pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Piston Type Pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Piston design

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Sorption Pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Sorption Pump Components

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    The sorption pump has no moving parts and therefore no oils or other lubricants. (5 liters of liquid nitrogen)

    Sorption pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    HIGH VACUUM PUMPS

    2

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    VACUUM PUMPING METHODS

    Sliding VaneRotary Pump

    MolecularDrag Pump

    TurbomolecularPump

    Fluid EntrainmentPump

    VACUUM PUMPS(METHODS)

    ReciprocatingDisplacement Pump

    Gas TransferVacuum Pump

    DragPump

    EntrapmentVacuum Pump

    Positive DisplacementVacuum Pump

    KineticVacuum Pump

    RotaryPump

    DiaphragmPump

    PistonPump

    Liquid RingPump

    RotaryPiston Pump

    RotaryPlunger Pump

    RootsPump

    Multiple VaneRotary Pump

    DryPump

    AdsorptionPump

    Cryopump

    GetterPump

    Getter IonPump

    Sputter IonPump

    EvaporationIon Pump

    Bulk GetterPump

    Cold TrapIon TransferPump

    Gaseous Ring Pump

    TurbinePump

    Axial FlowPump

    Radial FlowPump

    EjectorPump

    Liquid JetPump

    Gas JetPump

    Vapor JetPump

    DiffusionPump

    DiffusionEjector Pump

    Self PurifyingDiffusion Pump

    FractionatingDiffusion Pump

    Condenser

    SublimationPump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    PUMP OPERATING RANGES

    10-12 10-10 10-8 10-6 10-4 10-2 1 10+2P (Torr)

    Rough VacuumHigh VacuumUltra High Vacuum

    Roughing Pumps

    Turbo PumpDiffusion Pump

    Cryo PumpIon PumpTit. Subl. Pump

    Liquid Nitrogen Trap

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    VACUUM SYSTEM USE (high vacuum)

    1

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    8

    8 1233a456789

    ChamberHigh Vac. PumpRoughing PumpFore PumpHi-Vac. ValveRoughing ValveForeline ValveVent ValveRoughing GaugeHigh Vac. Gauge

    7

    33a

    28

    2

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diffusion pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diffusion pumps

    diffusion pump is one form of a fluid entrapment pump a fluid (usually oil) is heated and vaporized the vapor is A sent through a nozzle with supersonic speed the pump fluid vapor is condensed on a cooled surface

    Gas molecules are transported to the bottom of the pump by the pump fluid, where it is evacuated by a backing pump (usually a rotary vane pump) through the pump exhaust (the foreline)

    In order to work, the pump cannot be started until the foreline pressure

    is sufficiently low (~millitorr)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Water ejector pump (Liquid Jet pump)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pump Construction

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    How the Pump Works

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    How the Pump Works

    -A coil heater (1) raises the temperature of the oil pool (2) inside the pump body (3) with external cooling coils (4)

    -The pump body is bolted to the vacuum system by a flange (5)

    -The oil vapor rises through the housing that has 4 exit nozzles (A D).

    - The oil vapor exits the nozzles at high velocity (7) and collides with gas molecules (6), imparting a downward momentum to them.

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Release of Vapors

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    First stage vapors are separated from others

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pumping Speed

    10-10 10--3 10--1

    Pum

    ping

    Spe

    ed (A

    ir) 1 2 3 4

    Inlet Pressure (Torr)

    Critical Point

    1. Compression Ratio Limit2. Constant Speed3. Constant Q (Overload)4. Mechanical Pump Effect

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Maximum Tolerable Foreline Pressure (critical pressure)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    LN2 reservoir with baffles

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    How the LN2 Trap Works

    GasApproximate Vapor

    Pressure (mbar)

    Water (H2O)Argon (A)Carbon Dioxide (CO2)Carbon Monoxide (CO)Helium (He)Hydrogen (H2)Oxygen (O2)Neon (Ne)Nitrogen (N2)Solvents

    10-22 500 10 -7>760>760>760 350>760 760

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diffusion pump characters

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diffusion pump Fluids

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Diffusion pumps -- additional information

    The only justification for calling them diffusion pumps is due to the observation that the molecules of the pumped gas penetrate some distance into the vapor jet in a manner resembling diffusion of one gas into another. (Hablanian, High Vacuum Technology)

    Original pumping fluid (before 1928) was mercury, since it did not break down and early oils did -- over 99% today use oil

    The boiler pressure inside a nozzle is 1 to 2 torr, while at the center of the vapor stream it is about 0.1 torr

    A cold trap is often used in the high vacuum side to reduce oil backstreaming

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Low cost per unit pumping speed, very high pumping speeds Very well understood Hard to destroy Continuous operating expense (LN2) Potential for serious vacuum accidents Open system:Forbidden in certain applications

    Diffusion pumps -- additional information

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Vacuum system use for diffusion pumps

    LN2 cold trap

    Chamber

    Diffusion pump

    Rotary pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbomolecular pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbomolecular pumps (high vacuum and UHV)

    Medium to high cost per unit pumping speed Very clean, pumps rare gases Requires periodic maintenance which can be

    expensive Difficult to reach very low UHV base pressures Open system:Forbidden in certain

    applications

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pump OperationMolecule V

    Moving Wall with Speed V

    Principle of the Turbomolecular Pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbomolecular pumps Operation can be extended to higher pressure

    by adding a drag stage

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Principal of Turbomolecular pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Rotor - stator assembly

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbomolecular pump principle To maximise the compression ratio, blade tip velocities

    need to be comparable to molecular thermal velocities. For a single blade, at zero flow

    where 12 is the forward transmission probability and 21 is the reverse transmission probability It can be shown that

    where Vb is the blade velocity

    12

    21

    out

    in

    PKP

    0

    exp2

    bV MKTkN

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Compression ratio

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    high pressurestages

    fore vacuum

    high vacuum

    low pressurestages

    moving rotors impartdownward momentumto gas molecules

    fixed stators decelerate the molecule for thenext rotor hit

    without the stators,the next rotor couldnot impart additionalvelocity to the gasmolecule

    med. pressurestages

    moving rotors only:a molecular dragpump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbomolecular PumpROTOR BODY

    HIGH PUMPING SPEED

    HIGH COMPRESSION

    EXHAUST

    HIGH FREQ. MOTOR

    INLET FLANGE

    STATOR BLADES

    BEARING

    BEARING

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    A typical turbomolecular pumpA typical turbomolecular pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbomolecular Pumps Similar in design to a

    jet engine. Alternating rotor and stator blade assemblies turn at 20,000-90,000 rpm to force out molecules. Requires a region of low or medium vacuum behind and in front of pump.

    Pfeiffer Vacuum GmbH

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbomolecular pump.

    Turbo pumps cannot pump from atmosphere and cannot eject to atmosphere, so they require: 1-roughing (fore vacuum) pumps to reduce the pressure in the vacuum system before they can be started and

    2-backing pumps to handle the exhaust. There are many types of roughing and backing

    pumps. Most accelerators now use clean (dry) pumps to avoid oil contamination in the system.

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbopump (cont) contains no oil and is capable of reducing the pressure into the ultrahigh vacuum range

    operates as a molecular bat - rotor blades spinning at speeds as high as 6x104 rpm, - gives a blade velocity at a radius of 10 cm of 3.8x106 cm/s. - the mean velocity of a molecule of N2 at 300 K is 4.8x104 cm/s Because the rotor blades are slanted downward, the gas molecules are driven towards the pump outlet Blade sizes increase towards the high pressure exit port Stator (stationary) blade sets are placed between rotor blade sets

    Pumping efficiency is greatest when the spacing between blades is less than the mean free path of the molecules. (~5 cm at 10-3 Torr)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbo pumps speed

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Vacuum system use for Turbo pumps

    123456

    ChamberTurbo PumpRoughing PumpVent ValveRoughing GaugeHigh Vac. Gauge

    1

    67

    4

    3

    25

    2

    Rotary pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Turbo pump &Rotary pump

    Process chamber

    Turbomolecular Pump

    High rotation speed turbine imparts momentum to gas atoms

    Inlet pressures:

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion Pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion Getter Pump

    A getterIs a materialthat reactswith a gasmolecule toform a solid nonvaporizable material

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion pump The ion pump works by ionizing

    gas molecules and accelerating them into walls coated with freshly-evaporated titanium the gas ions strike a titanium

    cathode and cause sputtering the sputtered Ti is reactive and

    will getter reactive gases (N2, O2)

    the gas ions can be buried by self-ion implantation

    A strong magnetic field is applied to cause the electrons to move in helical paths and increase the ionization efficiency

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion pump (sputter- Ion pump, getter Ion pump)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion pumps Main components

    Array of parallel stainless tubes

    Various charged surfaces

    Titanium or tantalum coated surfaces

    Trap molecules with varying speeds via chemical reactions

    Varian Scientific Instrumentation, Inc.

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion pumps Ion pumps have several serious disadvantages

    low pumping speeds (inert gases are pumped especially poorly)

    can only be started at low pressures (~ 10-4 torr) can arc-over if pressure increases suddenly

    However, ion pumps are very clean and can produce very high vacuums (

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion pump

    Expensive per unit pumping speed Low pumping speed Generates hydrocarbons Has a memory effect Very low maintenance Moderately difficult to destroy Excellent base pressures

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Does not pump rare gases well Does not pump hydrogen Closed system: very safe against

    vacuum accidents

    A typical A typical ion-pumpion-pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion Pumps Current (per cell) and hence pumping

    speed depends on voltage, magnetic field, pressure and history.

    nI kP 1.05 < n < 1.2Pump life depends on quantity of gas pumped

    > 20 years at 10-9 mbar

    Prone to generate particulates

    Leakage current unpredictable, so pressure indication below 10-8 mbar unreliable

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion Pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion Pumps

    HighestLowHigherLowestCostHighestGoodLowLowUHV

    Highest

    Highest

    Lowest

    -5kV

    Triode

    GoodLowestLowestStarting Pressure

    HigherGoodLowestPumping Speed (Noble gases)

    GoodGoodHighestPumping Speed (Active gases)

    +2-5kV+7kV+7kVVoltage

    StarcellDifferential Diode

    Diode

  • Dr. G. Mirjalili, Physics Dept. Yazd University

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion PumpsPumping in the basic diode Penning cell

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Ion Pumps

    The Diode pump has poor pumping speed for noble gases

    Remedies Differential Ion; Noble Diode

    Heavy cathode Triode Special Anode shape e.g. Starcell

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cryopumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cryo-condensation

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cryopumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pumping by Cryocondensation

    Cold surface

    molecules

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cryopumps Similar in principle to

    the ion pump but uses a cryogenically cooled surface of activated charcoal or zeolites to condense and trap gas molecules.

    Kurt J. Lesker Vacuum Technology

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cryosorption in charcoal

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Charcoal placement

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    CryopumpsCryopumps condense gases on cold

    surfaces to produce vacuum

    Typically there are three cold surfaces:

    Inlet array condenses water and hydrocarbons (60-100 Kelvin)

    Condensing array pumps argon, nitrogen and most other gases (10-20 K)

    Adsorption is needed to trap helium, hydrogen and neon in activated carbon at 10-12 K. These gases are pumped very slowly!

    Warning: all pumped gases are trapped inside the pump, so explosive, toxicand corrosive gases are not recommended. No mech. pump is needed until regen.

    adapted from www.helixtechnology.com

    (Campbell)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cryopumps

    Expensive per unit pumping speed Very high pumping speeds are possible Pumping hydrogen (pumps everything) Requires periodic recharging Vibration can be a serious problem

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Types of Cryogenic Pumps There are two major classes of such

    pumps Liquid Pool

    Liquid helium temperature (~4K) Closed cycle

    Refrigerator (~12K) Supplemented by cryosorption

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cyro pump (Liquid Pool)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cyro pump (Closed cycle )

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Cryogenic Pump Speed

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Getter Pumps When a gas molecule impinges on a clean metal film,

    the sticking probability can be quite high. For an active gas with the film at room temperature,

    values can be between 0.1 and 0.8. These fall with coverage.

    For noble gases and hydrocarbons sticking coefficients are very low (essentially zero)

    Evaporated films, most commonly of titanium or barium, are efficient getters and act as vacuum pumps for active gases.

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Getter pumps In recent times, thin films of getter material have been

    formed on the inside of vacuum vessels by magnetron sputtering

    These have the advantage of pumping gas from the vacuum chamber by gettering and of stopping gases from diffusing out of the walls

    of the vessels

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Getter Pumps

    For vacuum use, the most common getter pump is the titanium sublimation pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Titanium sublimation pumps (HV and UHV)

    Very inexpensive and simple Requires periodic maintenance,

    which is cheap Often misused, which limits their

    performance Selective in what it pumps (good for

    oxygen, N2, air, not for rare gases)

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    A typical titanium sublimation pumpA typical titanium sublimation pump

  • Dr. G. Mirjalili, Physics Dept. Yazd University

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Others Getter Pumps An important class of getter pumps are the Non

    Evaporable Getters (NEGs) These are alloys of elements like Ti, Zr, V, Fe, Al which

    after heating in vacuo present an active surface where active gases may be gettered

    Traditionally, the getters take the form of a sintered powder either pressed into the surface of a metal ribbon or formed into a pellet

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Getter Pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Getter Pumps

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Vacuum cycle

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pumpdown Curve Conditions:

    Chamber closed and sealed Vacuum pump on and all isolation valves open No gas flowing into the chamber

    What would an ideal pumpdown curve look like?

    What effect would the following have on the ideal curve? Real (Gross) Leak Virtual Leak Permeation Leak Outgassing Backstreaming

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Pumpdown procedure

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Venting procedure

  • Dr. G. Mirjalili, Physics Dept. Yazd University

  • Dr. G. Mirjalili, Physics Dept. Yazd University

  • Dr. G. Mirjalili, Physics Dept. Yazd University

  • Dr. G. Mirjalili, Physics Dept. Yazd University

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    System pumpdown

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Standard Vacuum Cycle Step 0: Start at atmospheric pressure at t=o

    load wafer and close chamber alternative, start at loadlock pressure (~100mT)

    a loadlock is a separate vacuum chamber that prevents the chamber from being exposed to atmosphere

    Step 1: Pump down to base pressure remove atmospheric contaminants from the

    chamber verify system integrity continue to next step: when pressure falls below a

    trigger point abort: if base pressure is not reached within a

    certain amount of time, indicating a leak or a pump problem

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Standard Vacuum Cycle Step 2: Introduce gasses and stabilize

    pressure pressure increases from base pressure to process

    pressure most reactive gas is introduced last throttle valve controls conductance to achieve

    desired process pressure (effects residence time of gasses)

    continue to next step: when pressure reads within a specified range

    abort: if process pressure is not reached within a certain amount of time, indicating a pressure control problem

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Standard Vacuum Cycle Step 3: Process

    equilibrium is maintained through controlled gas flow and controlled (throttled) pressure

    RF power (if applicable) is introduced continue to next step: when pre-set time is reached,

    or endpoint is detected (for etch process) abort: if pressure drifts outside of desired range

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Standard Vacuum Cycle Step 4: Pump Out

    gas flows and RF Power (if applicable) are turned off throttle valve opens wide purpose is to remove the majority of the reactive

    gasses from the chamber continue to next step: when base pressure is

    reached for a minimum length of time Step 5: Purge

    inert gas (usually nitrogen - why?) is introduced into the chamber

    pressure inside the chamber increases to a trigger point

    presence of nitrogen restores viscous flow allowing residual reactive gasses to be efficiently pumped (rinsed) out

    continue to next step: when a minimum pressure is reached indicating adequate nitrogen has entered the chamber

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Standard Vacuum Cycle Step 6: Second Pump Out

    turn off nitrogen pump out nitrogen and residual reactive gasses to

    base pressure continue to next step: when base pressure is

    reached for a minimum length of time Note: steps 5 and 6 may be repeated

    Step 7: Vent close all valves between chamber and pump flow nitrogen directly into chamber pressure increases from base pressure to

    atmospheric (or loadlock) pressure continue to next step: when atmospheric pressure is

    reached Step 8: Open Chamber and Unload Wafer

  • Dr. G. Mirjalili, Physics Dept. Yazd University

    Abort Conditions Abort = Failure to meet all conditions required

    to continue processing. Pressure not in range, Gas flow not in range,

    Electrical or mechanical malfunction, Timeout, Interlock tripped.

    Accompanied by an audible and visible alarm. Abort Priority:

    1. System immediately goes to safest possible state. 2. Possible recovery of product material.

    Safest Possible State: Shut off all gas flows. Shut off RF power (if applicable). Pump(s) on, all isolation and throttle valve(s) wide

    open.