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Thin Film Deposition Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003
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Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Dec 22, 2015

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Page 1: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Thin Film DepositionThin Film Deposition

Prof. Dr. Ir. Djoko Hartanto MScProf. Dr. Ir. Djoko Hartanto MSc

Electrical Engineering DepartmentFaculty of Engineering University of Indonesia

February 14, 2003

Page 2: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

IntroductionIntroduction

The need of layers of semiconductor, dielectrics, and conductors to complete the device

Beside the circuits have shrunk, they also have grown in the vertical direction.– Through increased numbers of deposit layers.

Page 3: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

OverviewOverview

List of common deposition systems

Atmospheric Pressure (AP)1. Horizontal

2. Vertical

3. Barel

4. Vapor phase epitaxy

Page 4: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

List of common deposition systemsList of common deposition systems

Low Pressure (LP) and

Ultra High Vacuum (UHV)

1. Horizontal

2. Vertical

3. Barel

4. Vapor phase epitaxy

Page 5: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

OverviewOverview

There two primary techniques for layer deposition :

1. Physical Vapor Deposition (PVD)

2. Chemical Vapor Deposition (CVD)

Page 6: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Physical Vapor Deposition (PVD)Physical Vapor Deposition (PVD)Physical vapor deposition (PVD) refers to a

family of processes in which a material is converted to its vapor phase in a vacuum chamber and condensed onto a substrate surface as a thin film.

PVD can be used to produce coatings of a wide variety of materials: metals alloys ceramics glasses semiconductors polymers

Page 7: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Physical Vapor Deposition (PVD)Physical Vapor Deposition (PVD)

All PVD processes consist of the following steps: synthesis of coating vapor, vapor transport to the substrate, condensation of vapors onto the substrate

surface to form a thin film. These steps are carried out inside a vacuum

chamber, so evacuation of the chamber always precedes the PVD process.

Page 8: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Physical Vapor Deposition (PVD)Physical Vapor Deposition (PVD)

Pressure Units: 1 atm = 14.7 psia = 29.92 inches Hg = 760 mm Hg = 760 torr = 1.013 bar = 1.013 x 105 Pa

1 Pa = 1 N/m2 = 7.5 x 10-3 torr

Page 9: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Physical Vapor Deposition (PVD)Physical Vapor Deposition (PVD)The two most common PVD processes are: evaporation sputtering

We have already covered the basics of evaporation.

For evaporation, the background pressure in the vacuum chamber is typically ~10-6 Torr (~10-4 Pa) or lower.

For sputtering, the background pressure in the vacuum chamber is typically 10-3 to 10-2 Torr (~1 Pa).

Page 10: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

EvaporationEvaporation

In order to evaporate a material, it must be heated to a temperature at which its vapor pressure is 10-3 Torr or higher.

E.g., aluminum must be heated to 1000°C or more.

Page 11: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

EvaporationEvaporation

There are two common ways to heat the source material : resistive heating electron-beam heating.

Resistive heating uses electric current flow through a tungsten filament to heat the source material.

The source material can be placed directly on the tungsten filament, or it can be put in a crucible that is heated by the filament.

Page 12: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

EvaporationEvaporation Evaporation from a filament-heated crucible.

Aluminum Vapor

Aluminum Film

Silicon Wafer

Page 13: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

EvaporationEvaporation In electron-beam (e-beam) evaporation systems,

a high intensity beam of electrons, with energy up to 15 keV, is focused on the source material.

Electron bombardment heats the source material to the temperature required for evaporation.

Heating can be restricted to the source material itself . The surroundings stay cool.

Because pressure is so low in the vacuum chamber, in evaporation the source material travels in a straight line from the source to the substrate shadowing

Page 14: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Physical Vapor Deposition (PVD)Physical Vapor Deposition (PVD)The mean free path, of atoms or molecules in

a chamber at pressure P is given by

T is the absolute temperature, k is Boltzmann’s constant, and d is the diameter of the gas atoms or molecules

The mean free path is the average distance between collisions in the chamber.

2dP2

kT

Page 15: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Physical Vapor Deposition (PVD)Physical Vapor Deposition (PVD) At room temperature and for a typical atom/molecule

diameter of 4 Å, the previous equation becomes

The pressure P is in pascals (Pa). 1 Pa = 1 N/m2 = 7.5 10-3 Torr What is the mean free path for typical evaporation and

sputtering conditions?

)(108.5 3

mP

Page 16: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

SputteringSputtering

In sputtering, the source material is usually in the form of a sheet or plate, called a target.

Sputtering is achieved by bombarding the target with energetic ions, typically Ar+.

Atoms on the surface of the target are dislodged by this bombardment and fly off .

These atoms then impinge on the substrate, resulting in deposition of a thin film.

Page 17: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Chemical Vapor DepositionChemical Vapor Deposition

Chemical Vapor Deposition (CVD) is the formation of a solid material (insulator, metal, or semiconductor) from the reaction of source gases (or vaporized liquids).

The solid material is usually in the form of coating (a “thin film”) 20-5000nm thick (200-50,000Å or 0.02-5m).

Page 18: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

CVD of Zinc Oxide (ZnO)CVD of Zinc Oxide (ZnO)A simple Chemical Vapor Deposition system for

the preparation of thin film coatings of ZnO on a substrate (e.g., a Si or GaAs wafer) is shown:

Exhaust

N2 + H2O +

Zn(OOCCH3)2

Air

Furnace

Wafer

Page 19: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Chemical Vapor DepositionChemical Vapor Deposition

Materials deposited by CVD are usually amorphous or polycrystalline.

If a “clean” crystalline substrate is used, it can sometimes act as a seed, resulting in a single crystal deposited layer.

A crystalline layer deposited on a crystalline substrate is called an epitaxial layer.

Page 20: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

Chemical Vapor DepositionChemical Vapor Deposition

Examples in microelectronics -- insulators (dielectrics)

Silica (SiO2) deposition (400-500ºC)

SiH4 + O2 SiO2 + 2H2

Silicon Nitride (Si3N4) deposition (700-800ºC)

3SiH4 + 4NH3 Si3N4 + 12H2

Page 21: Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc Electrical Engineering Department Faculty of Engineering University of Indonesia February 14, 2003.

LPCVD SystemsLPCVD Systems