Signal integrity of TSV

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IEEE EMC Society Distinguished Lecturer Seminar:
Signal Integrity of TSV-Based 3D IC
July 21,
21 2010
Joungho Kim at KAIST
joungho@ee.kaist.ac.kr
joungho@ee
kaist ac kr
http://tera.kaist.ac.kr
TERA
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1
Contents
1)
Driving Forces of 3D Package and IC
2)
Signal Integrity Design
3)
N i C
Noise
Coupling
li Issues
I
4)
Noise Isolations
5)
Summary
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2
3D Movie
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3
3D Housings
Sk L
Sky
Lounge
Apartment
Medical care
center
Restaurant
Fitness & Spa
Parking
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4
16GB Samsung NAND Flash, 8Gbx16
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5
Sharp, Laboratory
Morihiro Kada
3D Hamburger
SDRAM
Di it l Core
Digital
C
RF
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Analog
6
Terahertz Interconnection and Package Laboratory
6
Expected Market of 3D IC
Market Driving Forces of 3D IC
“More than Moore”
Heterogeneous integration
Æ Co-integration of RF + logic +
Performance
driven
memory + sensors in a reduced space
Electrical performance
Æ”Mid term”
t
”
driver: > 2010
Logic
Æ Interconnect speed and
reduced parasitic power
consumption
DRAM
MEMS
3D vs. “More Moore”
Æ Can 3D be cheaper
than going to the next
lithography node?
3D IC
Optimum Market
Access Conditions
Flash
Cost
Æ “Long
Long term
term”
driven
(NAND & NOR)
driver: > 2012
CIS
RFSiP
Form factor
driven
Density
Æ Achieving the highest
capacity / volume ratio
Æ “Short term”
driver: > 2008
Source: “3D
3D IC & TSV Report”
Report , Yole Development
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Relatiive wiring p
pitch, I/O pitch, and
I/O in
nterconnecttion density ranges (I/O
O per cm2)
Technology Trend of 3D IC
* ref:
f IBM JJ. RES
RES. & DEV.
DEV VOL.
VOL 52 NO.6
NO 6 NOVEMBER 2008,
2008
p555
3D-IC integration
I/O: 0.4 - 10.0μm pitch
105 – 108 I/O per cm2
Wiring pitch: 45nm
Si-on-Si package
p stacking
g
and chip
I/O: 10-50μm pitch
103 - 106 I/O per cm2
Wiring pitch: 0.5μm
Organic and ceramic package
(SCM and MCM)
I/O: 200
200-μm
μm pitch
102 - 103 I/O per cm2
Wiring pitch: 25 - 200μm
2000
Time
2010
Relative comparison of I/O densities for 3D silicon, 3D die stacking,
and silicon packaging, for both ceramic and organic packaging
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Core Technologies of 3D IC
Substrate
Via
Ball
Attachment
TSV
Unified
Design/CAD
Environment
and Test
PCB
3D Thermal
& Reliability Analysis
And Design
Methodologies
Chip & SoC
Architecture and
Design Methodologies
3D IC
Low Cost Interposer
p
Process and Design
Technology
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Chip
Chipp-to
to--Wafer
Stacking & Bonding,
TSV Technology
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99
Signal Integrity Design Issues in 3D IC
Signal Integrity I:
Loading Effect & Reflection
Port 1
Signal via
Cox
SiO2
Cvia_ox
Ground via
Csil
Cvia_ox
Cvia_ox
Cvia_ox
Lvia
Gsil
Rvia
Gsil
Si
Cvia_ox
0
Cox
Csil
Lvia
Gsil
Lvia
Rvia
Gsil
Rvia
Cvia_ox Cvia_ox
Csil
Cox
3D IC using
g TSV
(Through Silicon Via)
()
S21(Phase) [Degree]
Ground via
Signal Integrity II:
Crosstalk & Jitter
-10
-20
-30
-40
Cvia_ox
Csil
Solid line = model
Symbol line = measurement
0.1
Cox
1
Frequency [GHz]
10
CIS
20
Port 2
Logic
- Limitation of High Speed Signaling
by Capacitive Loading
- Impedance Mismatching, Reflection
RF
Analog
- Crosstalk Between TSVs
- Die-to-Die Vertical Coupling
- Jitter by Inter-Symbol-Interference
DRAM
EMI
Si-Interposer
p
Power Integrity
DSP
Chip 7
Chip 6
Chip 5
Chi 4
Chip
Chip 3
Chip 2
Chip 1
Through
Throughwafer via
- Vertical Die-to-Die
Die to Die EMI Coupling
- RF Sensitivity Reduction by EMI
- EM Radiation Increase
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VSSN
Power
Ground
- Simultaneous Switching Noise caused
by Insufficient Power
- High freq Noise Coupling & Transfer
Terahertz Interconnection and Package Laboratory
10
10
Disadvantages of Wire Bonding Stacked Chip Package
• Long Interconnection
Æ Long RC Delays
Æ High Impedance for Power Distribution Network
Æ High
Hi h Power
P
Consumption
C
ti
Æ Poor Heat Dissipation (Thick Substrate)
• Bonding Wire located in Chip Perimeter
Æ Low Density Chip Wiring
Æ Limited Number of I/O
Æ Limited I/O Pitch
Æ Large Area Package
3D Stacked Chip Package
with Wire Bonding
• Complex Interposer
Æ Long Redistribution Interconnection
Æ Bonding Wire located in Interposer Periphery
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11
Key Technology : TSV (Through Silicon Via)
• Short Interconnection
Æ Reduced RC Delays
Æ Low Impedance for Power Distribution Network
Æ Low Power Consumption
Æ Heat Dissipation Through Via
3rd Chip
(Thinned
Substrate)
Under fill
Dielectric
2nd Chip
(Thinned
Substrate)
• No Space
p
Limitation for Interconnection
Dielectric
Under fill
Multi-level
On-chip
On
chip Interconnect
Æ High Density Chip Wiring
Æ No Limitation of I/O Number
Æ No Limitation of I/O Pitch
ÆS
Small
a Area
ea Package
ac age
SiO2
1st Chip
Si-Substrate
3D TSV Stacked IC
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★ Why does TSV Family happy ^^ ?
Elevator !!
Happy TSV Family~!
So fast! ♬
It’s awesome!!
Sad Wire-bonding Family~!
4th Floor
So tired T^T !
It takes too
much
energy !!
• Shorter distance !
• Lower loss of energy !
3rd Floor
T^T
Stairs !!
T0T
2nd Floor
^^
^^
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13
10 chip stacked Package by KAIST
10
9
8
7
6
5
4
3
2
1
55 μm TSV diameter
150 μm Pitch
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Background(1): High-frequency Channel Loss in TSV
Gsil
-Significant
Significant high
high-frequency
frequency signal loss occur at Signal Transmission
Cvia_ox Through TSV
-The signal loss through TSV is caused by substrate leakage and coupling
S21(mag
gnitude) [ddB]
0.1μm
Frequency [GHz]
Si
SiO2
Ta Cu
Close up of through wafer via
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Magnitude of S21
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15
Background(2): Increased Channel Loss in Multi-Stack TSV
-Signal loss increases substantially with number of stacks/TSVs
-The
Th signal
i
l lloss through
h
h TSV iis caused
db
by substrate
b
lleakage
k
and
d coupling
li
Increased Total Resistance Increased Total Capacitance (Slopes)
10
9
8
2-Stack TSVs
7
6
5
4
3
5-Stack TSVs
10-Stacked TSVs
2
1
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A Through Silicon Via Structure on Double-sided Silicon
Substrate
Underfill
Bump
Metal (M1,M2)
Inter-metal Dielectric
Insulation layer
y
Double-sided
Double
sided
Silicon Substrate
TSV
1111111111111
Cinsulator GSi sub
Inter-metal Dielectric
Underfill
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Bump
Cu
SiO2
Si
Terahertz Interconnection and Package Laboratory
17
17
Frequency-dependent Loss of Through Silicon Via
Frequency
dependent term
0
Cinsulator
GSi subb
i
l t
Leakage current
Cu
SiO2
Si
Loss term
I
Insertion
loss (dB
B)
-1
-2
-3
-4
Capacitive
region
Resistive
region
-5
-6
6
0.1
1
10 20
Frequency (GHz)
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18
Scalable Equivalent Circuit Model of a TSV
Signal
TSV
CBump
Cinsulator
Cinsulator
LTSV
RTSV
TERA
Cinsulator
Cinsulator
LTSV
CSi sub
GSi subb
Cinsulator
Cinsulator
Cinsulator
Cinsulator
B
Bump
Terahertz Interconnection and Package Laboratory
Ground
TSV
CBump
RTSV
B
Bump
Structural Parameters
TSV diameter
:d
TSV-to-TSV pitch : p
SiO2 thickness : t
Height
:h
Bump diameter : D
Equations
Cinsulator (d,h,t)
(d h t)
CSi sub (d,h,p,t)
CBump (p,D)
GSi sub (d,h,p,D)
(d h p D)
RTSV (d,h)
LTSV (d,h,p)
Terahertz Interconnection and Package Laboratory
19
19
Analysis of a TSV Channel with Insulator Thickness of TSV
ƒ Insulator thickness of TSV (t)
0
Signal
Ground
Top
-0.5
S21 magnitude
e (dB)
Top
CInsulator/2
CInsulator/2
CInsulator/2
-1.5
-2
Bottom
Bottom
Leakage current
CInsulator=7.8
=7 8 pF
Insulator thickness of TSV ↓
-2.5
-3.5
3.5
0.1
Ground
Signal
CInsulator=2.6 pF
-1
-3
CInsulator/2
CInsulator=1.6 pF
[A]
1
10
20
Frequency (GHz)
Equivalent circuit model ( t = 0.5um )
E i l t circuit
Equivalent
i it model
d l(t=0
0.3um
3
)
Equivalent circuit model ( t = 0.1um )
Î Leakage through silicon substrate dominantly increases due to lowered impedance
with increased Cinsulator in region [A].
Î Insulator thickness dominantly affects frequency dependent loss of a TSV channel
in region [A].
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Analysis of a TSV Channel with Pitch between TSVs
ƒ Pitch between Signal & Ground TSV (p)
Top
LTSV
0
Ground
Top
CSi sub
LTSV
GSi sub
CSi sub=3.14 fF
-0.5
05
S21 magnitu
ude (dB)
Signal
CUnderfill, IMD
LTSV ↓
CSi sub=3.48 fF
-1
-1.5
CSi sub=4.26 fF
-2
-2.5
Pitch between TSVs ↓
-3
-3.5
0.1
Signal
Bottom
CUnderfill, Bottom
Ground
Bottom
[B]
1
10
[C
] 20
Frequency (GHz)
Equivalent circuit model ( p = 190um )
Equivalent circuit model ( p = 150um )
Equivalent circuit model ( p = 100um )
ÎDue to relative small capacitance, pitch affects frequency dependent loss of a TSV
channel from region [B].
Î From region [C], inductance effect becomes dominant.
Î Pitch dominantly affects frequency dependent loss of a TSV channel in region [B].
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2121
Analysis of a TSV Channel with TSV Diameter
ƒ Via diameter of TSV (d)
CInsulator ↑
CUnderfill, IMD
Signal
Ground
Top
CSi sub ↑
LTSV ↓
0
Top
CInsulator
I
l t
CSi sub
LTSV
LTSV
GSi sub
RTSV
RTSV
S21 magn
nitude (dB)
CInsulator
I
l t
-0.5
-1
-1.5
-2
-2.5
-3
CInsulator
Signal
CInsulator
CUnderfill, IMD
Bottom
Ground
B tt
Bottom
-3.5
0.1
Via diameter ↑
Î The effect of decrease of
pitch between TSVs
[A]
[B]
1
10
[C
]
20
Frequency (GHz)
Equivalent circuit model ( d = 32um )
Equivalent circuit model ( d = 20um )
Signal
TSV
CSi sub ↑
Ground
TSV
Equivalent circuit model ( d = 10um )
CInsulator ↑
Î Via diameter affects frequency dependent loss of a TSV channel, dominantly
Terahertz Interconnection and Package Laboratory 2222
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in region [A] and [B].
Terahertz Interconnection and Package Laboratory
Analysis of a TSV Channel with Via Height of TSV
ƒ Via height of TSV (h)
CInsulator ↑
Signal
Ground
Top
CSi sub ↑
LTSV ↑
[B]
[C
]
0
Top
CInsulator
CSi sub
LTSV
LTSV
GSi sub
RTSV
RTSV
CInsulator
Ground
Bottom
Bottom
CSi sub ↑
-1
-1.5
-2
LTSV ↑
Via Height ↑
-2.5
-3
CInsulator
Signal
S21 magnitude
e (dB)
CInsulator
-0.5
-3.5
-3
5
0.1
[A]
1
10
20
Frequency (GHz)
Equivalent circuit model ( h = 110um )
Equivalent circuit model ( h = 80um )
Equivalent circuit model ( h = 50um )
Signal
TSV
CInsulator ↑
Ground
TSV
Î Via height affects frequency dependent loss of a TSV channel in all frequency ranges.
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2323
Inter-symbol Interference (ISI) by Channel Loss
‰ InterInter-symbol Interference is the interference between adjacent pulses
of a data
-
The channel BW Limit degrades the signal quality
It depends on line
line--length
length,, data rate and sub. materials on PCB
Long Channel
600
600
500
500
Voltage [mV]
Voltage [mV]
Short Channel
400
300
200
400
300
200
100
100
0
0
-100
0110110
0000
40 % reduction
-100
0
5
10
15
0
5
Time [ns]
10
15
Time [ns]
– Channel Length = 10 cm
– 3 Gbps
– FR4 (Loss Tangent = 0.03)
– Channel Length = 40 cm
– 3 Gbps
– FR4 (Loss Tangent = 0.03)
[ ISI effect due to line-length ]
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24
24
Inter-Symbol Interference at the TSV Equalizer
S21(ma
agnitude) [[dB]
Voltage (V)
0 25
0.25
0
-0.25
Frequency [GHz]
0
20
40
60
80
100
Ti
Time
((ps))
Magnitude of S21
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25
25
The Proposed TSV Equalizer using an Ohmic Contact
Ohmic contact
((Al/n+ type)
yp )
Signal
TSV
n+ high
doped Silicon
Ground
TSV
n-type
Silicon
Substrate
Bump
Bump
ƒ We intentionally made leakage by using an Ohmic contact
resulting in DC attenuation between signal and ground TSV
TSV.
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26
Frequency Domain Simulation-based Verification of the TSV
Equalizer Performance
0
Inse
ertion losss (dB)
Insertion loss of 8 TSVs
without TSV equalizer
-2
-4.8 dB
-3.8 dB
-4
- 4.5
-6
1 dB
0 7dB
0.7dB
Flattened from DC to 10GHz
(Nyquist frequency of 20Gbps)
Insertion loss of 8 TSVs with TSV equalizer
-8
0.1
1
10 20
F
Frequency(GHz)
(GH )
• We successfully flattened frequency dependent loss by 3.8 dB
by using TSV Equalizer
Equalizer.
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27
27
Time Domain Simulation-based Verification of the TSV
Equalizer Performance
0 25
0.25
Voltage (V)
Voltage (V)
0 25
0.25
0
-0.25
0
20
40
60
Ti
Time
(ps)
( )
80
100
Pk-pk jitter : 16 ps
0
-0.25
0
Eye opening: 100mV
20
40
60
80
100
Ti
Time
( )
(ps)
• We successfully achieved normalized pk
pk-pk
pk jitter and eye
eye-opening,
opening
32% and 20%,
meanwhile the unequalized eye is completely closed.
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28
Time-Domain Measurement Results
Eye-opening : 904 mV
= 90.4% Vin (1V)
0.5
Pk-pk jitter : 50 ps
= 0.5%
0 5% UI
0
2
4
6
8
0.5
Pk-pk jitter : 12.5 ps
= 1.25%
1 25% UI
Data rate : 100 Mb/s
Data Pattern : PRBS 211-1,
Source amplitude : 1 V
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0.2
0.4
0.6
0.8
0
1
Time (nsec)
Time (nsec)
ƒ
ƒ
ƒ
0.5
Pk-pk jitter : 27.8 ps
= 18.9%
18 9% UI
0
0
10
Eye-opening : 685 mV
= 68.5% Vin (1V)
1
0
0
ƒ
ƒ
ƒ
Eye-opening : 720 mV
= 72% Vin (1V)
1
Voltage (V)
1
Voltage (V)
Measured Eye-diagrams of a TSV channel
Voltage (V)
ƒ
Data rate : 1 Gb/s
Data Pattern : PRBS 211-1,
Source amplitude : 1 V
40
80
120
160 200
Time (psec)
ƒ
ƒ
ƒ
Data rate : 5 Gb/s
Data Pattern : PRBS 211-1,
Source amplitude : 1 V
Terahertz Interconnection and Package Laboratory
2929
Coupling Issues in Stacked Dies using TSV
Bonding
Adhesive
Bonding
Adhesive
P-Substrate
3rd Chip
Inductor
TSV
TSV
TSV
N+ P+
P+ N+
N-Well
N
Well
2
N+ P+
N+ P+ N+
N-Well
N
Well
P-Substrate
TSV to Active Circuit
Coupling
N+ P+ N+
Metal
to Metal
N-Well
Coupling
3
TSV
N+ P+
P+ N+
N W ll
N-Well
2nd Chip
Inductor
1
TSV to TSV
Coupling
TSV
N+ P+
N+ P+ N+
N W ll
N-Well
P-Substrate
N+ P+
TSV
N+
N W ll
N-Well
1st Chip
< CROSSSECTIONAL VIEW >
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30
Measurement Result of Coupling between TSVs
S
G
S
G
< Top
p view>
Coupling coefficient [dB]
-10
-20
20
Csi
-30
Gsi
+ Cparasitics
-40
Cox
Measurement
-50
Model
-60
Cm
Cox
R
L
Cp1
0.1
1
10
20
Freq [GHz]
Csi
Gsi
M
• Analytic model of coupling between TSVs shows good
g
agreement
with measurement result
< Equivalent circuit model of coupled TSV>
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-31-
31
Shielding Methods for TSV Coupling
1)
Re-design of TSV materials and dimensions
2)
Separation
3)
G d Ri
Guard
Ring
4)
GND Shield TSV
5)
Metal Ring
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32
Shielding Effect Measurement – (1) Metal Ring
-10
G
S
< Top view>
Cm
Coupling coeffficient [dB]
C
G
-20
-30
-40
Cox
R
L
Csi
Gsi
M
w/ metal ring
-60
01
0.1
Cp1
w/o metal ring
-50
1
10
20
Freq [GHz]
• Metal ring has shielding effect only in high frequency
because it blocks coupling in IMD layer
< Equivalent circuit model of coupled TSV>
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-33-
33
Shielding Effect Measurement– (2) Guard Ring
-10
G
S
< Top view>
Cm
Coupling coeffficient [dB]
C
G
-20
-30
-40
Cox
R
L
Csi
Gsi
M
w/ guard ring
-60
01
0.1
Cp1
w/o guard ring
-50
1
10
20
Freq [GHz]
• Guard ring has good shielding effect in every frequency
range because guard ring structure can partly block substrate
coupling between TSVs
< Equivalent circuit model of coupled TSV>
• Main factor of coupling between TSVs is silicon substrate
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34
Shielding Effect Measurement– (3) Guard Ring + Metal Ring
-10
G
S
< Top view>
Coupling coeffficient [dB]
C
G
-20
-30
-40
w/o guard ring
-50
w/ guard ring
w/ guard ring + metal ring
Cm
-60
01
0.1
Cox
R
L
Cp1
1
Csi
Gsi
M
10
2x10
Freq [GHz]
• Metal ring structure with guard ring can further decrease
coupling between TSVs
< Equivalent circuit model of coupled TSV>
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35
Measurement Environments for Model Verification
Vector Network Analyzer (VNA)
ƒ Measurement instrument
g
Technology
gy PNA-L N5230A
: Agilent
ƒ Frequency range : 10MHz ~ 20GHz
ƒ Frequency sweep : log scale, 1601 point
ƒ microprobe : GGB industries inc. 40A-GS250-P
microprobe
microprobe
Port1
Port2
RDL
RDL
ILD/IMD
FOX
P+
substrate
contact
FOX
P+
FOX
P+
TSV
Open
silicon substrate
[ Cross
C
sectional
ti
l view
i
off test
t t sample
l ]
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36
Designed Test Sample Images
RDL(Redistribution layer)
G
G
Contact
IMD / ILD
Silicon substrate
S
RDL(Redistribution layer)
Dummy skip layer
coupling
TSV
S
Contact
[ Top view of test sample ]
TSV
[ Cross sectional view
ie of test sample ]
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37
Analysis of Noise Coupling based on the 3D TLM Model
Csub
Rsub
CTSV
TSV
silicon
substrate
Distance
Di
t
b
between
t
contact
t t and
d TSV :
100 μm
Substrate height : 100 μm
TSV diameter : 30 μm
TSV SiO2 thickness : 0.5 μm
Coup
pling coefficient [dB]
conta
ct
-30
ILD/IM
D
A
B
-35
35
Silicon resistance
dominant
-40
-50
TSV SiO2 capacitance
d i
dominant
t
-55
-60
10M
100M
1G
Frequency [GHz]
Coupling can be divided into 3-regions
3 regions
ƒ
In region A, B, and C TSV SiO2 capacitance , silicon resistance, silicon
capacitance is the dominant factor to the coupling
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Silicon
capacitance
dominant
-45
ƒ
Terahertz Interconnection and Package Laboratory
C
10G
Terahertz Interconnection and Package Laboratory
38
38
Substrate contact to TSV Coupling 3D TLM Model Verification by
Measurement – with Distance Variation
Coup
pling coeffiicient [dB]]
-10
50 um
Distance Increases
100 um
-20
200 um
-30
-40
Measurement
The p
proposed
p
model
-50
10M
100M
1G
Frequency [Hz]
10G
ƒ
Proposed model’s coupling coefficient estimation is less than measurement
over 1GHz
ƒ
But model follows same tendency as the distance increases
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39
Analysis of Noise Coupling based on the 3D TLM Model
– with TSV SiO2 Thickness Variation
Csub
Rsub
CTSV
TSV
silicon
substrate
TSV SiO2 thickness
(tox TSV)
Di t
Distance
b
between
t
contact
t t and
d TSV :
100 μm
Substrate height : 100 μm
TSV diameter : 30 μm
TSV SiO2 thickness : 0.3, 0.5, 0.7 μm
Substrate conductivity : 10S/m
Coup
pling coefficient [dB]
conta
ct
-20
ILD/IM
D
-30
A
tox_TS
V
C
B
CTS
V
Coupli
ng
-40
-50
-60
10M
Coupling
coefficient
d
decreases
tox_TSV = 0.3um
tox_TSV = 0.5um
tox_TSV = 0.7um
100M
1G
Frequency [GHz]
ƒ
TSV SiO2 thickness determine the coupling coefficient in the region A
ƒ
If we increases TSV SiO2 thickness, coupling coefficient decreases in the
region A
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40
40
Analysis of Noise Coupling based on the 3D TLM Model
– with Silicon substrate Height Variation (1)
Csub
Rsub
CTSV
height (h)
TSV
silicon
substrate
Distance
Di
t
b
between
t
contact
t t and
d TSV :
100 μm
Substrate height : 30, 70, 100 μm
TSV diameter : 30 μm
TSV SiO2 thickness : 0.3 μm
Substrate conductivity : 10S/m
Coup
pling coefficient [dB]
conta
ct
-20
ILD/IM
D
A
h
-30
-40
-50
-60
10M
C
B
CTS
V
Coupli
ng
,
,
Rsub
Csub
Coupling
coefficient
increases
h = 30um
h = 70um
h = 100um
100M
1G
Frequency [GHz]
10G
ƒ
If silicon substrate height decreases
decreases, all component value is changed
ƒ
At the whole frequency, the coupling coefficient increases as silicon substrate
height increases
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41
Analysis of Guard-ring based on the 3D TLM Model
– with Guard-ring Location Variation
guardring
conta
ct
TSV
silicon
substrate
Distance between contact and TSV :
100 μm
Substrate height : 100 μm
TSV diameter : 30 μm
μm
TSV SiO2 thickness : 0.5 μ
Guard-ring distance from contact : 10
μm
Guard-ring width : 10 μm
Coup
pling coefficient [dB]
-30
A
C
B
A’
C’
B’
-40
-50
w/o guard-ring
with guard-ring around TSV
with guard-ring around contac
-60
0
-70
10M
100M
1G
Frequency [Hz]
10G
ƒ
Guard-ring
Guard
ring around contact shows more isolation effect compared to guard-ring
guard ring
around TSV
ƒ
Guard ring around contact does not have frequency dependent isolation effect
Guard-ring
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42
PLL Coupling Simulation Environment
½
noise source
Is assumed as
square wave
(500mV ,
305MHz )
[ Active circuit noise ]
PFD
LPF
CP
½ ½
½
½
VCO
Output
½
[ PLL ]
ILD / IMD
metal
S
contact
G
S TSV
TSV
ili
b
silicon
substrate
[ Active circuit to TSV coupling model ]
[ PLL external clock ]
ƒ
Contact to TSV coupling model was proposed and verified in the previous
chapter
ƒ
HSPICE simulation was performed using the contact to TSV coupling model
and PLL schematic
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43
43
Substrate Noise Coupling to TSV
0
305 MHz
305*3 MHz
305*5
305
5 MHz
-30
20
-20
305*7 MHz
305*9 MHz
...
-40
-60
-50
-60
10M
-80
100M
1G
Frequency [Hz]
10G
ƒ
305MHz square wave noise is coupled to TSV by the coupling coefficient
ƒ
Up to 9th harmonic frequency, coupling coefficient is almost constant
TERA
-40
Terahertz Interconnection and Package Laboratory
No
oise voltag
ge (dBV)
Co
oupling coefficient
betwee
en contact a
and TSV [d
dB]
-20
-100
Terahertz Interconnection and Package Laboratory
44
44
PLL Phase Noise Degradation due to Active Circuit to TSV Coupling
-50
Pha
ase Noise (dBc/Hz)
60
-60
-70
No noise
305MHz, 500mV
coupled noise
Phase noise spur generated
due to TSV coupled noise
Externa
l
Clock
PLL
Output
3rd harmonic of
2.4GHz output
2nd harmonic of
2.4GHz output
-80
-90
-100
1M
10M
100M
Frequency [Hz]
1G
5G
ƒ
PLL phase noise shows spurs at 5MHz due to coupled 305MHz noise
ƒ
PLL phase noise spur at 75MHz, 2.4GHz, 4.8GHz is due to circuit design
TERA
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45
45
Substrate Noise Coupling to TSV
Co
oupling coefficient
betwee
en contact a
and TSV [d
dB]
w/o guard-ring
0
305 MHz
Guard-ring around TSV
305*3 MHz
305*5
305
5 MHz
-30
20
-20
305*7 MHz
305*9 MHz
...
-40
Guard-ring
around TSV
-60
-50
-60
10M
-80
100M
1G
Frequency [Hz]
10G
ƒ
Guard ring around TSV decreased coupling coefficient
Guard-ring
ƒ
PLL coupled noise also decreased by the guard-ring around TSV
TERA
Terahertz Interconnection and Package Laboratory
-40
No
oise voltag
ge (dBV)
-20
-100
Terahertz Interconnection and Package Laboratory
46
46
PLL Phase Noise Degradation due to Active Circuit to TSV Coupling
-50
w/o guard-ring
Pha
ase Noise (dBc/Hz)
60
-60
-70
Guard-ring around TSV
Externa
l
Clock
Phase noise decreased
~4dBc/Hz
PLL
Output
3rd harmonic of
2.4GHz output
2nd harmonic of
2.4GHz output
-80
-90
-100
1M
10M
100M
Frequency [Hz]
1G
5G
ƒ
PLL phase noise spur at 5 MHz decreased by the guard
guard-ring
ring
ƒ
Guard-ring around TSV can improve coupling degraded circuit performance
TERA
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47
47
BER Calculation in Mixed-Signal System Model
Spec
ctrum [dBm]
tr
T
-20dB/dec
f = 1
Coupling
coefficient
π tr
-40dB/dec
data from
RX
raw data
from TX
BER
teste
r
data from
RX
raw data
bit error occurs
3
5
7 9
Harmonic
number
frequency
Generated noise
from digital clock
Transmitte
r of RF
Signal
Digital
noise
Coupling
coefficien
t
Receiver RF
signal
RF signal
g
Baseband
(BER
tester)
Raw Data
Delay
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Amp
Terahertz Interconnection and Package Laboratory
48
48
Dimension Region with Coupled TSV Parameters
Constant BER curve
BER
50 um
1
d = 1 ~ 50um
p = 200um
30 um
TSV
V diameterr
tox = 0.5um
hTSV =
30um ~
200um
3x10-1
20 um
2x10-1
10 um
10-1
5 um
1 um
Dimension region
for acceptable BER
30 um
50 um
70 um
100 um
150 um
200 um
0
Silicon thickness
• In certain digital application, dimension region of TSV design parameters for
p
BER can be obtained from the modeling
g of coupled
p
TSVs
acceptable
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49
49
Dimension Region with Coupled RDL Parameters
Constant BER curve
BER
200 um
1
Dimension region
for acceptable BER
Edge-tto-edge sp
pace
150 um
3x10-1
100 um
2x10-1
60 um
s = 20 ~100 um
40 um
w = 20um
20 um
50 um
70 um
100 um
150 um
t = 1um
l = 100
~500 um
200 um
300 um
10-1
0
Coupled length
• In certain digital application, dimension region of RDL interconnects design
parameters for acceptable
p
p
BER can be obtained from the modeling
g of coupled
p
RDL
interconnects
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50
50
Dimension Region with Coupled TSV Parameters with Guard
Ring
Constant BER curve
BER
50 um
1
d = 1 ~ 50um
p = 200um
30 um
TSV
V diameterr
tox = 0.5um
hTSV =
30um ~
200um
3x10-1
20 um
2x10-1
10 um
I
Increased
d di
dimension
i
region for acceptable
BER
5 um
1 um
30 um
50 um
70 um
10-1
100 um
150 um
200 um
0
Silicon thickness
• By applying guard ring structure, dimension region for acceptable BER is
significantly increased
Æ Target BER can be satisfied within realizable dimensions
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51
51
Vertical Coupling of DDR3 to ZigBee Transceiver
Zigbee Tranceiver
VDD
N+ P+
P+
Guardring
VCO of ZigBee Transceiver
Differential
Spiral Inductor
2nd Chip
Die-to-Die
Die
to Die
Vertical
Coupling
N+ P+
N-Well
TSV
N+
N+ P+
N+
N Well
N-Well
20dB/decade
TERA
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40dB/decad
e
1
ㅡ
T
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1st Chip
Amplittude
DDR 3
1
ㅡ
Pi*Tr
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F
Frequenc
m
3
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52
52
Experimental Verification of Proposed Model
(Line Type Clock Tree to Two Turn Spiral Inductor)
C Clock
40
L
20
0
-20
Inductor
L
-80
-100
-120
0.1G
40
20
0
Inductor
-40
-60
60
L Clock
C Clock
L
Inductor
LM
C epoxy
1G
-20
L
-40
Clock
L
Inductor
LM
-60
R,C csub -80
-100
10G
-120
20G
Voltage Trransfer Ratio [dB]
Impedance
e [dBΩ]
60
2 Turn
Z11=Clock Tree Impedance
Z21=Transfer Impedance
Z21/Z11=V2/V1
Measurement
Frequency[Hz]
• Before clock tree resonance, voltage transfer ratio is determined by Cclock and Linductor.
• After clock tree resonance, voltage transfer ratio is determined by Lclock and Linductor.
TERA
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5353
53
Investigation of Vertical Coupling Effect on VCO Spur
0
2.4 GHz
-40
-20
20
High-frequency
Multiplicative Noise
-60
-80
-100
-120
0 1G
0.1G
VCO Outpu
ut Spectrum [dBm]
20
1G
10G
Frequency(Hz)
Voltage Transfer R
Ratio [dB]
Clock Spectrum [d
dBV]
Clock spectrum
p
(before
(
vertical
coupling)
Voltage Transfer Ratio
1 Z 21 V2 /I1 V2
=
=
=
A Z11 V1/I1 V1
1
)dB = 20log(V2 )dB
A
1
20log(V1 )dB + 20log( )dB
A
= 20log(V2 )dB
20log(V1 *
20G
20
• Main mechanism of spur
0
generation
ti is
i high-frequency
hi h f
-20
2.4 GHz
multiplicative noise
-40
• To reduce the spur at 10MHz offset
-60
from center frequency, design
guide has to be proposed.
VCO Output Spectrum (before vertical coupling)
-80
VCO Output Spectrum (after vertical coupling)
-100
100
2.38
TERA
Terahertz Interconnection and Package Laboratory
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2.42
2.44
Frequency(GHz)
Terahertz Interconnection and Package Laboratory
54
54
Investigation of Design Guide for Spur Reduction (Epoxy Thickness)
0
-20
20
-40
-60
-80
-100
-120
0 1G
0.1G
VCO Outpu
ut Spectrum [dBm]
20
1G
10G
Frequency(Hz)
Voltage Transfer R
Ratio [dB]
Clock Spectrum [d
dBV]
Clock spectrum
p
(before
(
vertical
coupling)
Voltage Transfer Ratio
Port 2
Port 1
Spiral Inductor Chip
90um
80um
20um
Clock Tree Chip
20G
20
• Spurs at 5MHz and 10MHz offset
0
f
from
center
t frequency
f
satisfy
ti f the
th
-20
spur spec of ZigBee system.
-40
• Increasing epoxy thickness is
-60
highly effective for spur reduction.
VCO Output Spectrum (before vertical coupling)
-80
VCO Output Spectrum (after vertical coupling)
-100
100
2.38
TERA
Terahertz Interconnection and Package Laboratory
2.4
2.42
2.44
Frequency(GHz)
Terahertz Interconnection and Package Laboratory
55
55
Summary
-TSV is the most critical interconnection structure in 3D IC.
- TSV can cause significant channel loss for high-speed signaling.
- Equalizer
E
li
or specific
ifi I/O schemes
h
are needed
d d to
t supportt low
l
power
and high-speed data transmissions.
- Crosstalk and coupling between TSV and active circuit need to be
considered when designing the TSV arrangement configurations.
- Shielding structures are needed to reduce the TSV crosstalks and noise
couplings.
TERA
Terahertz Interconnection and Package Laboratory
Terahertz Interconnection and Package Laboratory
56
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