19
7. Deposition Deposition systems may be divided into two groups: a) Chemical Vapor Deposition (CVD) systems Which rely on the chemical reaction of the constituents of a vapor phase at the substrate surface to deposit a solid film on this surface. b) Physical Vapor Deposition (PVD) systems Which directly deposit the source material onto a given substrate in a “line-of-site impingement type deposition”. Vito Logiudice 53

Nanoscience and Nanotechnology 180/198-534Apeter/534A/MEMS3.pdf · Thermal Evaporation – e-Beam b.1) Thermal Evaporation - General Vito Logiudice 62. 7. Deposition b.1) Thermal

  • Upload
    others

  • View
    0

  • Download
    0

Embed Size (px)

Citation preview

  • 7. DepositionDeposition systems may be divided into two groups:

    a) Chemical Vapor Deposition (CVD) systemsWhich rely on the chemical reaction of the constituents of a vapor

    phase at the substrate surface to deposit a solid film on this

    surface.

    b) Physical Vapor Deposition (PVD) systemsWhich directly deposit the source material onto a given substrate

    in a “line-of-site impingement type deposition”.

    Vito Logiudice 53

  • 7. Deposition

    Vito Logiudice 54

    a) CVD: Summary of transport and reaction processes

    © L.M. Landsberger

  • 7. Depositiona) CVD: Common film types & sample chemistries

    Polysilicon:

    Silicon Nitride:

    Silicon Dioxide:

    Vito Logiudice 55

  • 7. Depositiona) CVD: Chemistry & system selection

    Factors to be considered:

    – deposition temperature (ex:

    depositing over metals?)

    – film quality (tensile/compressive;

    grain boundary size, etc.)

    – growth rate

    – deposition system compatibility

    – throughput

    Tensile Compressive

    Stress in deposited films

    Deposited polysilicon grain size

    Vito Logiudice 56

  • 7. Depositiona) CVD: Atmospheric Systems (APCVD)

    Vito Logiudice 57

    Cold-wall induction type with tilted susceptor

    Barrel type

    Poly Si deposition: Note the use of a liquid source in this example (SiCl4)

    Rotating pancake type

    Induction heating: RF energy couples with the graphite susceptor, thereby heating it rather than heating the process gases and substrates themselves (improved contamination control)

  • 7. Depositiona) CVD: Low-Pressure Systems (LPCVD)One disadvantage of APCVD systems is that the diffusion, D, of the reacting species to the surface of the substrate is a limiting step. Thus, few wafers can be processed at the same time (mass-transport limited). Since “D” is inversely proportional to pressure, This issue may be overcome by lowering the pressure within the reaction chamber. Ie., @ 1 Torr, D increases by a factor of 1000. In this case, the diffusion of the species through the boundary layer through to the reaction site is no longer a limiting step and the system is said to be surface reaction limited.

    Vito Logiudice 58

  • 7. Depositiona) Overview of CVD process types (Madou, p. 109)

    Vito Logiudice 59

  • 7. Deposition

    b) Physical Vapor Deposition (PVD) systems

    – In these types of thin film deposition systems, the source materials to be deposited take on a variety of forms:

    • Solid• Liquid• Vapor

    – In the case of PVD systems, the materials to be deposited are physically deposited using a variety of methods including:

    • Thermal Evaporation • Sputtering• Etc. (Laser Ablation, Molecular Beam Epitaxy)

    Vito Logiudice 60

  • 7. Depositionb) Physical Vapor Deposition (PVD) systems - continued

    – The range of materials that may be deposited using these methodsinclude:

    • Metals such as: – Al – Cu– Au– Ag– etc.

    • Compound & hard materials such as:

    – Cr– TiN– CrN– AlCuSi– etc.

    Vito Logiudice 61

  • 7. Deposition

    – The material to be deposited is placed in a crucible within a high-vacuum chamber.

    – After the chamber is pumped down, the source is heated via (typically) resistive or e-beam heating. The material is heated to its boiling point such that it sublimates onto all exposed surfaces in the vacuum chamber.

    – The amount of material deposited is controlled via a thickness monitor which is placed within the deposition chamber.

    – The source material must be of high purity.

    – Vacuum levels are on the order of 10-5to 10-7 Torr.

    Thermal Evaporation – Resistive Heating

    Thermal Evaporation – e-Beam

    b.1) Thermal Evaporation - General

    Vito Logiudice 62

  • 7. Depositionb.1) Thermal Evaporation - drawbacks

    – Resistive heating is the simplest method of evaporating metals such as Al or Au, but it is also the “dirtiest” in that contaminants which find their way onto the filament tend to be evaporated along with the metal.

    – The purity issue can be addressed via e-beam evaporation since the cooled, non-molten high-purity material to be deposited acts as a crucible during the process (see schematic on previous slide).

    – In the case of resistive heating, temperature uniformity across the filament is difficult to control and therefore, evaporation uniformity onto the substrates may be a problem. This is not an issue with e-beam evaporation

    – E-beam evaporation may cause surface damage due to ionizing radiation and/or X-rays (@ voltages above 10kV, the incident electron beam will give rise to X-ray

    Vito Logiudice 63emission).

  • 7. Depositionb.1) Thermal Evaporation - drawbacks

    – The different components of certain alloys such as NiCr have different evaporation rates, hence, the composition of the deposited material will not be the same as that of the starting material. Thus, thermal evaporation does not lend itself well to the deposition of all alloys.

    – The previous problem may be tackled via the use of multi-pocket e-beam systems.

    – Due to the point-source nature of the material being evaporated, shadowing effects may hamper the uniformity of the deposited layer over steps existing on the substrate (bad step coverage) in both the e-beam & resistive heating cases. Step Coverage

    Issues

    Vito Logiudice 64

  • 7. Depositionb.2) Sputtering – principle of operation• A solid slab (ie., target) of the material to be deposited is placed in a vacuum chamber along with the substrate on which the deposition is to take place.

    • The target is grounded.

    • Argon gas is introduced into the chamber and ionized to a positive charge.

    • The Ar ions bombard the target and cause the target atoms to scatter, with some of them landing on the substrate.

    • The plasma is composed of the Ar atoms, Ar ions, the sputtered material, gas atoms and electrons generated by the sputtering process.

    • Allows the deposition of a large assortment of materials on any type of substrate Sputtering

    Vito Logiudice 65

  • 7. Deposition

    Vito Logiudice 66

    b.2) Sputtering – advantages/disadvantages

    M.J. Madou

  • 8. Dry Etchinga) Mechanism

    Sample reactions

    In general, any material that forms a volatile fluoride or chloride can be plasma etched.

    Typical setupVito Logiudice 67

  • 8. Dry Etchingb) Species to use for various material types

    M.J. MadouVito Logiudice 68

  • 8. Dry Etching

    Vito Logiudice 69

    c) Etch profiles

    Photoresist with sloped sidewalls leads to sloped etch profiles

    SiO2

    Si

    PR

    Pre-Etch PR Profile

    SiO2

    Si

    Pre-Etch PR Profile

  • 8. Dry Etchingd) Process parameters to consider

    Vito Logiudice 70

    1. Gas flows

    2. Pressure (in process chamber)

    3. RF Power (for generating the plasma)

    4. Magnetic Field (for focusing the plasma)

    5. Cathode temperatureCluster tool: Four-chamber, magnetically

    enhanced RIE

    Model shown is a Precision 5000 manufactured by Applied Materials

  • 8. Dry Etchinge) Effect of varying etch parameters

    Courtesy: Applied Materials

    Vito Logiudice 71