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S Kanjanachuchai
2102-584 Intro to Nanoelectronics
1
5. Lithography
1. photolithography• intro: overall, clean room
2. principle3. tools4. pattern transfer5. resolution6. next-gen
References:Semiconductor Devices: Physics and Technology. 2nd Ed. SM Sze. Ch 12 Fundamental of Semiconductor Fabrication. GS May & SM Sze. Ch 4
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
2
Photolithography process
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Clean room:
lithography must be carried out in a clean-room environment [A] because the presence of dust particles [B] will lower yields.
[A] [B]
1. Pinhole2. Current constriction3. S/C or O/C
yield = # good chips / # total chips
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
4
Figure 12.2.Particle-size distribution curve for
English (---) and metric (—) classes of clean rooms.4
ENGLISH SystemClass 100 = 100 particles/ft3
(particle size >= 0.5 µm)
or 100×103 particles / m3
(particle size >= 0.1 µm)
"clean" quantified:
cleanliness – cost trade-off
1 ft = 0.3048 m1 ft3 = 0.0283 m3
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
5
Clean room & HEPA filter
HEPA = high efficiency particulate air.
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Lithography
1. photolithography2. principle
• shadow, projection3. tools4. pattern transfer5. resolution6. next-gen
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Shadow
λ
g
λ (µm) g (µm) CD (µm)
0.4 50 4.5
0.25 15 2
Contact: dust particles can be transferred between mask and wafer low yieldProximity: dust not transferred high yield (poor resolution due to diffraction) yield-resolution trade-off gCD λ≅
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
8
Image partitioning techniques for projection printing: (a) annual-field wafer scan, (b) 1:1 step-and-repeat,
(c) M:1 reduction step-and-repeat, and (d) M:1 reduction step-and-scan.
Projection
Stepper(step-and-repeat system)
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Lithography
1. photolithography2. principle3. tools
• light source• mask• photoresist
4. pattern transfer5. resolution6. next-gen
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Pre-1990: high-pressure mercury-arc lamp
source λ(nm) resolution (nm)Hg 365 300KrF 248 180ArF 193 100F2 157 70
Mercury (Hg) sourceline λ(nm)G 436H 405I 365
Hg
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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CMOS scaling necessitates the development of low-λ light source
Light source roadmap
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Lithography
1. photolithography2. principle3. tools
• light source• mask• photoresist
4. pattern transfer5. resolution6. next-gen
ITRS2009. Table LITH5A
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Mask
How to make masks?Mask blank electron-beam lithography IC Mask (reticle)[Cr / SiO2] [CAD]
info, alignment marks, test structures, etc.
alignment marks
test structures
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Yield for a 10-mask lithographic process with various defect densities per level.
In order to improve yield, masks are cleaned / inspected regularly
Yield
the yield of a lithographic step depends critically on mask cleanliness, or how many fatal defects are presence:
see fig. [B] slide #3
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
15
Lithography
1. photolithography2. principle3. tools
• light source• mask• photoresist
4. pattern transfer5. resolution6. next-gen
source: ITRS2011, Table LITH3A
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Suppliers: AZ, Shipley, Sumitomo
There are two types of resists: positive and negative. The final pattern on wafer is the same as (+) or opposite to (–) those on mask.
It is called photo-resist because:photo – it responds to photonsresist – it resists etching / dopant atoms, protecting the layer underneath
Photoresist
photo
resist
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
17
Figure 12.9. Exposure-response curve and cross section of the resist image after development.1 (a)
Positive photoresist; (b) negative photoresist.
The “quality” of the resist and the exposure / development process is measured by the steepness of the resist wall, or the contrast ratio:
source: ITRS2011, Table LITH3B
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Lithography
1. photolithography2. principle3. tools4. pattern transfer5. resolution6. next-gen
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Pattern transfertransfers the pattern which appears on the photoresist onto the substrate (Si). The transfer process can be subtractive [A], or additive [B] in nature.
[A] Subtractive: etching(for oxide removal, interconnect)
[B] Additive: metallization(S/D metal, via filling)
Some process (such as doping through photoresist) is neither subtractive nor additive.
Lift-Off process
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
20source: ITRS2011, Fig. LITH1
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Lithography
1. photolithography2. principle3. tools4. pattern transfer5. resolution
• limit• enhancement (PSM, OPC, Immersion)
6. next-gen
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
22
( )22
1
sin
NAkDOF
nNANA
klm
λθ
λ
=
=
=
NA: numerical apertureDOF: depth of focus
Q) How to improve resolution (lm)?A) ↓λ, ↑NA
Resolution of photolithographyminimum printed line / feature size / resolution(lm)
trigonometry:
Requirements:lm,↓, DOF↑
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
23
Diffraction strong when L ~< λ
L
λ
Diffractiondiffraction is the limiting factor in printing two closely-spaced lines.
mask
wafer
λ>L λ≤L
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
24
Lithography
1. photolithography2. principle3. tools4. pattern transfer5. resolution
• limit• enhancement (PSM, OPC, Immersion)
6. next-gen
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
25source: ITRS2009, Table LITH1
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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A schematic of an optical lithography system showing the methods that can improve the technique's performance. Key: λ is the wavelength of the illumination source; OAI is off-axis illumination; IIL is imaging interferometric illumination; OPC is optical proximity correction; and PSM is phase-shift masks.
Link
Resolution Enhancement Techniques
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
27
Figure 12.12. The principle of phase-shift technology. (a) Conventional technology; (b) phase-shift technology.9
diffraction
intensity
d = λ/2(n-1)
Phase-Shift Mask (PSM)
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Optical Proximity Correction (OPC)a purely mathematical process
The automated algorithmic link between DesignGauge, the application system for CD scanning electron microscopy (CD-SEM), and Proteus OPC for pre-processing OPC model building data allows Proteus customers to seamlessly obtain a large sampling of metrology data to account for process variations across the entire process window.
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
30
Immersion
θ
λ
sin
1
nNANA
klm
=
=
use n > 1
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
31sour
ce: IT
RS20
11, T
able
LITH2
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
32
High-Index Lenses Push Immersion Beyond 32 nmAaron Hand -- Semiconductor International, 4/1/2006
water's refractive index (n) = 1.44high-index fluids n~1.65photoresist n = 1.7lens (n=1.56) becomes the limiter: calcium fluoride (CaF2) higher-index lens materials: lutetium aluminum garnet (LuAG), n = 2.1
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
33
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
34
Lithography
1. photolithography2. principle3. tools4. pattern transfer5. resolution6. next-gen
• EUV, XRL, EBL, IBL, NIL
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
35
sour
ce: IT
RS20
11, F
ig. L
ITH3
Aso
urce
: ITRS
2011
, Fig.
LIT
H3B
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
36
EUV: extreme-ultra violet lithography
In an laser produced plasma (LPP)-based system, EUV light is produced by bombarding a sliver of tin with a high-power laser. The light is then gathered by specially engineered EUV mirrors, which then focus an EUV beam in the EUV scanner to produce microchip patterns.
ITRS2009: Table LITH5C
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
37
XRL: X-ray lithography
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Schematic of an electron-beam machine.
Direct-write (serial)
Figure 12.16. Schematic of positive and negative resists
used in electron-beam lithography.
EBL: electron-beam lithography
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
39
RSiNx100-150nmsmall scattering angle
LCr/W30-60nmlarge scattering angle
RL
100 keV
Scattering with angular limitation projection electron beam lithography system
EBL: parallel
Basic SCALPEL principle of operation showing contrast generation by differentiating more- or less-scattered electrons.
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
40
IBL: Trajectories of 60 keV H* ions traveling through PMMA into Au, Si, and PMMA.18
EBL: Proximity effect: (a) Simulated trajectories of 100
electrons in PMMA for a 20-keV electron beam.15 (b) Dose distribution for forward
scattering and backscattering at the resist-substrate interface.
IBL: ion-beam lithography
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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NIL: Nano-imprint lithography
ITRS2009: Table LITH5D
S Kanjanachuchai
2102-584 Intro to Nanoelectronics
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Conclusions• photolithography
– process, principle, tools– resolution limits– resolution-enhancement techniques
• PSM, OPC, Immersion, DP,…• future lithographic systems
– EUV, XRL, ML2 (EBL, IBL), NIL, ...
from ITRS2009:
... To continue as the dominant technique for leading-edge critical layer lithography, resolution enhancement techniques (RETs) such as off-axis illumination (OAI), phase shifting masks (PSMs), and optical proximity corrections (OPCs) are being used with imaging systems at the 193 nm wavelength. In addition to RETs, lenses with increasing numerical apertures and decreasing aberrations will be required to extend the life of optical lithography. Liquid immersion imaging with a fluid between the final lens element and the wafer is also being used to extend optical lithography.