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

4 Vacuum Pump

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Page 1: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Vacuum techniques

Pumps

Page 2: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Vacuum theory and pumping laws

Vacuum theory and pumping laws

How the vacuum is created?

Page 3: 4 Vacuum Pump

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

Page 4: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Vacuum pumps and their characteristics

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).

Page 5: 4 Vacuum 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).

Page 6: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Low vacuum pumps (1atm-10-3)

mbarRoughing Pumps

1

Page 7: 4 Vacuum Pump

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

Page 8: 4 Vacuum Pump

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

Page 9: 4 Vacuum Pump

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

Page 10: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

PUMP OPERATING RANGES

10-12 10-10 10-8 10-6 10-4 10-2 1 10+2

P (mbar)

Rough VacuumHigh VacuumUltra High Vacuum

Venturi Pump

Rotary Vane Mechanical Pump

Rotary Piston Mechanical Pump

Sorption PumpDry Mechanical Pump

Blower/Booster Pump

High Vac. PumpsUltra-High Vac. Pumps

Page 11: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

VACUUM SYSTEM USE

1

2

4

6

5

9

8

8

7

123

3a456789

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

7

33a

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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

PK

P

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Dr. G. Mirjalili, Physics Dept. Yazd University

Rotary Vane, Oil-Sealed Mechanical Pump

Page 14: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Pump Mechanism

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Dr. G. Mirjalili, Physics Dept. Yazd University

Gas ballastting

Page 16: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

The Molecular Sieve/Zeolite Trap

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Dr. G. Mirjalili, Physics Dept. Yazd University

Rotary pump Trap

Page 18: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Single &Dual Stage

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Dr. G. Mirjalili, Physics Dept. Yazd University

How 2-stage rotary pump Works

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Dr. G. Mirjalili, Physics Dept. Yazd University

OIL BACKSTREAMING

2

PRESSURE LEVELS: LESS THAN 0.2 mbar

Page 21: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Other types of Mechanical pumps

Rotary Piston

Roots

Rotary Vane

Dry pump

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Dr. G. Mirjalili, Physics Dept. Yazd University

Dry Vacuum Pumps

Page 23: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Root pump

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Dr. G. Mirjalili, Physics Dept. Yazd University

How Root Pump works

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Dr. G. Mirjalili, Physics Dept. Yazd University

One Stage Roots Blower Pump Assembly

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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

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Dr. G. Mirjalili, Physics Dept. Yazd University

Diaphragm pumps

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Dr. G. Mirjalili, Physics Dept. Yazd University

Diaphragm pumps

Page 29: 4 Vacuum Pump

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

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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

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Dr. G. Mirjalili, Physics Dept. Yazd University

Diaphragm pump

Page 32: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Sorption Pump Components

Page 33: 4 Vacuum Pump

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

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Dr. G. Mirjalili, Physics Dept. Yazd University

HIGH VACUUM PUMPS

2

Page 35: 4 Vacuum Pump

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

Page 36: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

PUMP OPERATING RANGES

10-12 10-10 10-8 10-6 10-4 10-2 1 10+2

P (Torr)

Rough VacuumHigh VacuumUltra High Vacuum

Roughing Pumps

Turbo Pump

Diffusion Pump

Cryo Pump

Ion Pump

Tit. Subl. Pump

Liquid Nitrogen Trap

Page 37: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

VACUUM SYSTEM USE (high vacuum)

1

4

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5

9

8

8123

3a456789

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

7

33a

28

2

Page 38: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Diffusion pumps

Page 39: 4 Vacuum Pump

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)

Page 40: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Water ejector pump (Liquid Jet pump)

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Dr. G. Mirjalili, Physics Dept. Yazd University

Pump Construction

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Dr. G. Mirjalili, Physics Dept. Yazd University

How the Pump Works

Page 43: 4 Vacuum Pump

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.

Page 44: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

First stage vapors are separated from others

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Dr. G. Mirjalili, Physics Dept. Yazd University

Pumping Speed

10-10 10--3 10--1

Pu

mp

ing

Sp

eed

(A

ir)

1 2 3 4

Inlet Pressure (Torr)

Critical Point

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

Page 46: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Maximum Tolerable Foreline Pressure

(critical pressure)

Page 47: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

LN2 reservoir with baffles

Page 48: 4 Vacuum Pump

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 <10 -10

Page 49: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Diffusion pump characters

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Dr. G. Mirjalili, Physics Dept. Yazd University

Diffusion pump Fluids

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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

Page 52: 4 Vacuum Pump

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

Page 53: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

•Turbomolecular pumps

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Dr. G. Mirjalili, Physics Dept. Yazd University

Turbomolecular pumps (high vacuum and UHV)

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

Page 55: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Pump OperationMolecule V

Moving Wall with Speed V

Principle of the Turbomolecular Pump

Page 56: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Turbomolecular pumps• Operation can be extended to higher pressure

by adding a drag stage

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Dr. G. Mirjalili, Physics Dept. Yazd University

Principal of Turbomolecular pump

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Dr. G. Mirjalili, Physics Dept. Yazd University

Rotor - stator assembly

Page 59: 4 Vacuum Pump

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 α12 is the forward transmission probability

• and α21 is the reverse transmission probability

• It can be shown that

• where Vb is the blade velocity

12

21

out

in

PK

P

0

exp2bV M

KTkN

Page 60: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Compression ratio

Page 61: 4 Vacuum Pump

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”

Page 62: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Turbomolecular Pump

ROTOR BODY

HIGH PUMPING SPEED

HIGH COMPRESSION

EXHAUST

HIGH FREQ. MOTOR

INLET FLANGE

STATOR BLADES

BEARING

BEARING

Page 63: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

A typical turbomolecular pumpA typical turbomolecular pump

Page 64: 4 Vacuum 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

Page 65: 4 Vacuum Pump

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.

Page 66: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Turbopump (con’t)

• 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)

Page 67: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Turbo pumps speed

Page 68: 4 Vacuum Pump

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

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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: <10 mTorr

Foreline pressure: < 1 Torr

Requires a rough pump

Good choice for toxic and explosive gases –

-gases are not trapped in pump

All gases are pumped at approx. the same rate

Pumping Speeds:

20 – 2000 liters per sec

foreline

adapted from Lesker.com

Page 70: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Ion Pumps

Page 71: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Ion Getter Pump

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

Page 72: 4 Vacuum Pump

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

Page 73: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

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

Page 74: 4 Vacuum 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.

Page 75: 4 Vacuum Pump

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 (<10-12 torr)

Page 76: 4 Vacuum Pump

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

Page 77: 4 Vacuum Pump

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

Page 78: 4 Vacuum 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 < 1.2

Pump 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

Page 79: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Ion Pumps

Page 80: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Ion PumpsDiode Differential

DiodeStarcell Triode

Voltage +7kV +7kV +2-5kV -5kV

Pumping Speed (Active gases)

Highest Good Good Lowest

Pumping Speed (Noble gases)

Lowest Good Higher Highest

Starting Pressure Lowest Lowest Good Highest

UHV Low Low Good Highest

Cost Lowest Higher Low Highest

Page 81: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Page 82: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Ion PumpsPumping in the basic diode Penning cell

Page 83: 4 Vacuum Pump

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

Page 84: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

•Cryopumps

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Dr. G. Mirjalili, Physics Dept. Yazd University

Cryo-condensation

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Dr. G. Mirjalili, Physics Dept. Yazd University

Cryopumps

Page 87: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Pumping by Cryocondensation

Cold surface

molecules

Page 88: 4 Vacuum Pump

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

Page 89: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Cryosorption in charcoal

Page 90: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Charcoal placement

Page 91: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

CryopumpsCryopumps condense gases on cold

surfaces to produce vacuum

Typically there are three cold surfaces:

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

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

(3) 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)

Page 92: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

CryopumpsCryopumps

• Expensive per unit pumping speed

• Very high pumping speeds are possible

• Pumping hydrogen (pumps everything)

• Requires periodic recharging

• Vibration can be a serious problem

Page 93: 4 Vacuum Pump

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

Page 94: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Cyro pump (Liquid Pool)

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Dr. G. Mirjalili, Physics Dept. Yazd University

Cyro pump (Closed cycle )

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Dr. G. Mirjalili, Physics Dept. Yazd University

Cryogenic Pump Speed

Page 97: 4 Vacuum Pump

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.

Page 98: 4 Vacuum Pump

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

Page 99: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Getter Pumps

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

Page 100: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Titanium sublimation pumps (HV and UHV)

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)

Page 101: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

A typical titanium sublimation pumpA typical titanium sublimation pump

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Dr. G. Mirjalili, Physics Dept. Yazd University

Page 103: 4 Vacuum Pump

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

Page 104: 4 Vacuum Pump

Dr. G. Mirjalili, Physics Dept. Yazd University

Getter Pumps

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Dr. G. Mirjalili, Physics Dept. Yazd University

Getter Pumps

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Dr. G. Mirjalili, Physics Dept. Yazd University

•Vacuum cycle

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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

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Dr. G. Mirjalili, Physics Dept. Yazd University

Pumpdown procedure

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Dr. G. Mirjalili, Physics Dept. Yazd University

Venting procedure

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Dr. G. Mirjalili, Physics Dept. Yazd University

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Dr. G. Mirjalili, Physics Dept. Yazd University

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Dr. G. Mirjalili, Physics Dept. Yazd University

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Dr. G. Mirjalili, Physics Dept. Yazd University

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Dr. G. Mirjalili, Physics Dept. Yazd University

System pumpdown

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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

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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

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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

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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

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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

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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.