C5-2(41-Plasma Etching Part 1)

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    Plasma etchingPlasma etching

    K - JISTK - JISTMaterials Science & Engineering

    Nanophotonic semiconductor Materials Lab.1

    Bibliography

    1. B. Chapman, Glow discharge processes, (Wiley, New York, 1980).

    - Classical plasma processing of etching and sputtering

    2. D. M. Manos and D. L. Flamm, Plasma etching; An introduction,

    (Academic, Boston, 1989).

    - Most helpful textbook for the researcher majoring the dry etching.

    3. M. Sugawara, Plasma etching; Fundamentals and applications,

    (Oxford Univ. Press, New York, 1998).

    - Mostly dedicated to the high density plasma sources such as ICP and ECR

    4. W. N. G. Hitchon, Plasma processes for semiconductor fabrication,

    (Cambridge Univ. Press, Cambridge, 1999)

    - Theoretical approach to the plasma etching and plasma deposition process

    5. R. J. Shul and S. J. Pearton, Handbook of advanced plasma processing techniques,

    (Springer, Heidelberg, 2000).

    - Helpful textbook for the researcher in the field of compound semiconductor process

    6. http://newton.hanyang.ac.kr/plasma/

    - Dedicated to the plasma physics for graduate student in physics

    http://newton.hanyang.ac.kr/plasma/http://newton.hanyang.ac.kr/plasma/
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    7. 1. Introduction

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    Nanophotonic semiconductor Materials Lab.3

    Etch

    removal of unwanted area during the fabrication of

    semiconductor

    Etching is the most important step in the fabrication ofsemiconductor devices along with a lithography technique.

    InGaN mesa for LED

    etched by ICPInP via-hole etched by RIE GaAs laser-facet etched by ICP

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    Advantage of plasma etching

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    Etching can be anisotropic

    Less consumption of chemicals; cost, environment impact

    Clean process (vacuum)Compatible with automation

    Precise pattern transfer

    Deep silicon etching for sensor application

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    Formation of sheath region

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    The fast-moving electrons hitthe wall before the ions do andsome stick to the wall.

    The wall charges up negativelyand this negative charge pushesother electrons away at thesame time as attracting positiveions.

    The field near the wall holds theelectrons away from the walland accelerates the positiveions toward the wall.

    High energy ion bombardment

    cf) Generally, the voltage drop couldnt be measured. In practice process

    engineers usually monitor the dc potential (relative to ground) of the electrode

    instead, which is called dc-bias.

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    Materials Science & Engineering

    Nanophotonic semiconductor Materials Lab.7

    Processes in the sheath region

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    Nanophotonic semiconductor Materials Lab.8

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    7. 4. Mechanism of plasma etching

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    (a) Physical sputtering - purely

    physical process by energetic ion

    bombardment

    (b) Chemical etching - purely chemical

    process by forming volatile by-

    product through chemical reaction

    between substrate and active

    radicals in plasma

    (c) Accelerated ion-enhanced etching -

    chemical etching + physical

    etching: removal of volatile product

    is accelerated by energetic ion

    bombardment(d) Sidewall-protected (inhibitor driven)

    ion-enhanced etching deposition

    of etch-resistant layer with ion

    bombardment isotropic etching

    7. 4. 1. Etch mechanism

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    7. 4. 2. Sequential steps in etching

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    Formation of active etchant byelectron collisions

    Transport of active etchant to thewafer surface

    Adsorption of etchant to wafer surface Reaction of etchant and wafer to form

    etch-product

    Desorption of etch-product form the

    wafer surface

    Acceleration of desorption of etch-product by ion bombardment

    Transport of etch-product to the bulk

    plasma

    Redissociation of etch-product in theplasma or pumped out

    Redeposited on the reactor wall or

    pumped out

    cf) If any of these steps fails to occur,

    the overall etch cycle ceases and the step

    failed is a rate-limiting step

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    7. 4. 3. Radicals in plasma

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    Radicals are generated through dissociation and ionization

    ex) e + O2 O+ + O* + 2e,

    e + CF4

    CF3+

    + F* + 2eRadicals are much more abundant than ions in plasma because;

    (1) They are generated at a higher rate due to;

    - lower threshold energy and ionization is often dissociative

    (2) Radicals survive longer than ions

    Although the concentration of radicals is much larger than that of

    positive ions, the reactive fluxes incident on the surfaces can be

    comparable, since ions are moving faster because they have

    large energy obtained from the electric field in the sheath.

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    7. 4. 4. Volatility and evaporation

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    Volatility of etch-products is a key distinction between plasma

    etching and sputtering.

    In general, desorption is a rate-limiting steps in the plasma

    etching Highly volatile by-product formation is important.

    Evaporation rate of material (a) of molecular weight Ma is

    proportional to its vapor pressure, pa, (refer to Chap. II)

    The evaporation rate is increased with increasing temperature.

    However, plasma etching generally done at room temperature.

    formation of volatile product at RT is most important.

    RTHa

    aa

    RTH

    aaaa

    a

    eRT

    M

    C

    eCppRT

    M

    =

    =

    =

    2

    1

    2

    1

    2

    ,2

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    Boiling point of etch product (Si and metal)

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    Nanophotonic semiconductor Materials Lab.13

    Etch product Boiling point() Comment

    Si

    (SiO2, Si

    3N

    4)

    SiH4

    -111.6 Gas at RT

    SiF4

    -95.7 Gas at RT

    Si2H

    6-15 Gas at RT

    SiHCl3

    31.7

    SiCl4

    56.7

    Si2OCl6 135.5Si

    2Cl

    6147

    Metal

    (Ag, Al, Ti, Au, Co, Cr, Cu, Ni,

    Pb, Pt, Ta, W, Zn)

    AgCl 1550

    AlCl3

    182.7 Sublimation

    TiCl4

    136.45

    TiF4

    284 Sublimation

    Au2Cl3 - Non volatileAu

    2Br

    3- Non volatile

    CoCl2

    1050

    CrO2Cl

    2117

    Cr(CO)6

    151

    CuCl2

    655 Non volatile

    CuBr2 900 Non volatileNi(CO)

    4-25

    PbCl2

    954

    PtF6

    69.1

    TaF5

    229.5

    WF6

    17 Sublimation

    (CH3)2Zn 46ZnCl2

    756 Non volatile

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    Boiling point of etch product (III-V semiconductor)

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    Nanophotonic semiconductor Materials Lab.14

    Etch product Boiling point() Comment

    III-V semiconductor

    (GaAs, InP, GaN)

    Ga2H

    6-63 Gas at RT

    GaCl3

    201.3

    GaCl2

    535

    GaF3

    ~ 1000

    GaBr3

    279

    GaI3 < 345(CH

    3)

    3Ga 55.7

    (C2H

    5)3In -32 Gas at RT

    (CH3)3In 88

    InCl3

    418 Sublimation

    InBr3

    371 Sublimation

    AsH3 -54.8 Gas at RTAsF

    5-52.9 Gas at RT

    AsF3

    63

    AsCl3

    130.4

    AsBr3

    221

    PF3

    -101 Gas at RT

    PH3

    -88 Gas at RT

    PF5 -75 Gas at RTPCl

    562

    NCl3

    < 71

    NF3

    -129 Gas at RT

    NI3

    - Explode

    NH3

    -33 Gas at RT

    N2 -196 Gas at RT(CH3)

    3N -33 Gas at RT

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    Typical gases used for plasma etching

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    Feed gas Mechanism Selective to

    n type Si

    Cl2

    Chemical

    SiO2

    Cl2/C

    2F

    6Ion-inhibitor

    SiCl4

    Si

    Cl2

    Ion-energetic SiO2CCl4/O2

    SiCl4/O

    2

    Al

    Sl2/SiCl

    4

    Ion inhibitor

    /energetic

    SiO2, some resist,

    Si3N4

    Cl2/CCl

    4

    Cl2/CHCl

    3

    Cl2/BCl

    3

    III-V semiconductor

    Cl2

    Chemical

    SiO2, resist

    Cl2/BCl

    3

    Ion-inhibitor

    Cl2/CH4

    Cl2/CCl

    4

    CCl4/ O

    2

    SiCl4/O

    2

    III-V semiconductor

    Without Al

    Cl2/O

    2Chemical Al-containing alloy,

    SiO2CF2Cl2 Ion-inhibitor

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    7. 5. Dry etch method and reactor type

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    7.5.1. Dry etch method

    Plasma method

    (a) Plasma etching (PE)(b) Reactivel ion etching (RIE)

    (c) High density plasma etching: Electron cyclotron resonance

    etching (ECR) and inductively coupled plasma etching (ICP)

    Ion beam method

    (a) Ion beam etching (IBE)

    (b) Reactive ion beam etching (RIBE)

    (c) Chemically-assisted ion beam etching (CAIBE)

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    Detailed characteristics of dry etching technique

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    Parameter PE RIE MERIE ICP ECR IBE

    (sputter)

    frequency 13.56MHz 13.56MHz 13.56MHz 13.56MHz 2.45GHz -

    Pressure

    (torr)

    0.1 ~ 10 0.01 ~ 0.1 0.010.001

    ~ 0.01

    0.001

    ~ 0.01

    0.001 ~ 0.1

    Te (eV) ~ 8 ~ 8 ~ 5 ~ 4 ~ 4

    Plasma

    density~ 3e8-3 ~ 1e10-3 ~5e10-3 ~5e11-3 ~5e11-3 -

    Wafer

    location

    Grounded

    electrode

    Powered

    electrode

    Powered

    electrode

    Powered

    electrode

    Powered

    electrode

    Powered

    electrode

    Ion voltage25 ~

    100 V

    250 ~

    500 V

    400 ~

    1000 V

    0 ~

    1000 V

    0 ~

    1000 V

    500 ~

    2000 V

    Ion energyNot

    Controllable

    Not

    Controllable

    Not

    controllableControllable Controllable Controllable

    Chemical

    reaction

    Yes Yes Yes Yes Yes No

    Physical

    reactionNo Yes Yes Yes Yes Yes

    Selectivity Excellent Good Good Good Good Poor

    Anisotropy poor Good Good Good Good Excellent

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    Comparison of dry etching technique

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    advantage disadvantage

    RIE economicalslow etch rate,

    plasma damage

    CAIBE

    Relatively fast etch

    rate low versatility

    ECR fast etch ratehigh price,

    low scalability

    ICP fast etch rate,low plasma damage

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    7. 5. 2. Reactor types of dry etch

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    (a) Plasma etching (PE) and Reactive ion etch (RIE)

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    Plasma etching (PE) Same reactor geometry as PECVD system

    Low ion bombardment energy due to the low sheath voltagedrop sample was loaded on the grounded electrode (anode)

    Mainly chemical reactions and negligible physical etching

    Isotropic etch profile

    At relatively high pressure: 0.1 ~ 10 TorrReactive ion etch (RIE) Combination of chemical activity of reactive radicals with

    physical effects due to high sheath drop sample was loaded

    on the powered electrode (cathode) Ion bombardment strongly enhances the chemical process

    Anisotropic etch profile due to ion bombardment

    Lower operation pressure of 0.01 ~ 0.1 Torr

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    (b) Magnetically enhanced reactive ion etching (MERIE)

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    Reduce the plasma loss on the chamber wall using magnetic field byelectromagnet bucket

    Electron collisional efficiency increase by interaction of E and B field

    Substrate rotation for uniformity increase

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    (d) Inductively coupled plasma

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    13.56 MHz currents pass through ICP coil

    RF magnetic field formation along z axis

    Induction of vortex electric field

    Electrons oscillation

    Increase of electron collision efficiency

    More effective plasma generation than

    conventional RIE high radical density

    Electrostatic shield configuration eliminates

    capacitive coupling

    Independent ion energy control by table

    power

    Z

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    Types of Inductively coupled plasma

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    Cylindrical type ICP

    Contamination-free geometry

    Planar type ICP

    Contamination of wafer by

    sputtering of window material.

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    Laser interferometer on chamber-top

    Optical emission spectroscopy throughsidewall window

    Electrostatic shield btw quartz and coil

    ICP/PECVD cluster tool in K-JIST

    Inductively Coupled Plasma in K-JIST

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    (e) Ion beam-based reactor

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    IBE inert gas ion (Ar+) formation in

    external RF ion source and extracted

    to the reaction chamber by

    acceleration electrode (grid).RIBE reactive gas besides inert gas

    ions are extracted from the external

    source to the reaction chamber. Etch

    rate is increased by the additionalchemical reaction

    CAIBE inert gas ion (Ar+) are

    extracted from the external sourceand the reactive gas are

    independently supplied to the wafer

    surface through shower-ring just

    above the wafer.