Performance Trade-Off Scenarios for GAA Nanosheet FETs ...
Transcript of Performance Trade-Off Scenarios for GAA Nanosheet FETs ...
public
1
Performance Trade-Off Scenarios for GAA Nanosheet FETs Considering Inner-spacers and Epi-induced Stress: Understanding & Mitigating Process Risks
IMEC: Amita Rawat, Philippe Matagne, Bjorn Vermeersch, Geert Hellings, Julien Ryckaert
Huawei: Krishna Bhuwalka, Wu Hao, Changze LiuBelgium
public
Motivation and Introduction
TCAD deck calibration
Circuit delay and RO frequency estimation methodology
RO performance comparison and design space study
Self-heating performance comparison
Conclusion
2
Outline
public
3
Motivation
Reduced stress control with introduced inner spacers
-2000
-1500
-1000
-500
0
500
1000
Top
Middle
Bottom
Str
ess
alo
ng
ch
an
nel (M
Pa)
Air-gap
horiz.
Top wire
Middle wire
Bottom wire
Air-
gap
vert.
Air-
gap
lateral
Air-gap
hor.+
vert+
lateral
(1nm)
Ref:no
air-
gap
Channel stress at end of process
Verti
cal
Cross-section
The ‘vertical’ interface is the most critical to maintain channel stress: stress is lost completely when epi from neighboring gates doesn’t join properly
public
4
Introduction
SD
With Inner Spacer
SD
WithoutInner Spacer
W ISP W/O ISP
Stress engineering No Yes
Parasitic cap. Low High
Parasitic res. High Low
Self-heating High Low
Considered cases for electrical performance comparison▪ Option I: With inner spacer and 100 % stress▪ Option II: With inner spacer and 0 % stress▪ Option III: Without inner spacer and 100 % stress
𝜿 = 𝟕. 𝟓 𝜿 = 𝟏𝟏. 𝟗
TCAD Deck Calibration
public
6
NMOS: Width = 11 nm, Str: 100 %
Without With
Vths (V) 0.188 0.180
Ion-lin (uA) 15.96 16.45
Ion-sat (uA) 46.3 49.2
SS (mV/dec) 75.5 71.05
DIBL (mV/V) 35.3 30.7
PMOS: Width = 11 nm; Str = 100 %
Without With
Vths (V) -0.185 -0.178
Ion-lin (uA) 19.6 18.64
Ion-sat (uA) 54.8 55.4
SS (mV/dec) 68.8 65.98
DIBL (mV/V) 29.23 40
DOPING CONCENTRATION PROFILE
Parameters NMOS PMOS
L (nm) 15 15
TNS (nm) 11 11
HNS (nm) 5 5
Spacer (nm) 5 5
100 % Stress (GPa)
0.7 -1.7
NSD (𝐜𝐦−𝟑) 1e21 1e21
NSD ext (𝐜𝐦−𝟑) 1e17 1e17
Nchannel (𝐜𝐦−𝟑) 1e15 1e15
w/ ISP w/o ISP
public
7
ISP removal decreases NMOS on-current
𝑲𝒐𝒖𝒕 = 4𝑲𝒊𝒏 = 7.5
Stress = 0 GPa
NMOS PMOS
Vd = 0.7 V Vd = -0.7 V
public
8
ISP Removal increases carrier scattering
45 𝝁A
64 𝝁A
40 𝝁A
68 𝝁A
𝑲𝒐𝒖𝒕 = 4𝑲𝒊𝒏 = 7.5
Stress = 0 GPa
w/o ISPw ISP
Scattering: Carrier-carrier and carrier-ion
Without scattering
With scattering
x
x
Methodology to estimate RO performance using device parasitcs
public
Simplified RC network of device
10
D
G
S
Ceff1/Aeff
𝐶𝐷𝐺 = 𝐶𝑆𝐺𝐴𝐷𝐺 = 𝐴𝑆𝐺
In on state, D and G terminals are shorted
Effect parasitic network in on-state𝐶𝑒𝑓𝑓 = 𝐶𝑆𝐺 + 𝐶𝐷𝑆𝐴𝑒𝑓𝑓 = 𝐴𝑆𝐺 + 𝐴𝐷𝑆
D
G
S
CSG
1/ASG
CDS1/ADS
D
G
S
CDG
1/ADG
CSG
1/ASG
CDS1/ADS
public
11
RO frequency estimation
𝑫𝑰𝒏𝒗 𝑭 =𝟏
𝟐 × 𝟗 × 𝑫𝑰𝒏𝒗
𝑶𝒖𝒕
Charging
𝐂𝐞𝐟𝐟−𝐧
𝟏/𝐀
𝐞𝐟𝐟−𝐧
𝐂𝐞𝐟𝐟−𝐩
𝟏/𝐀
𝐞𝐟𝐟−𝐩
𝑮𝑵𝑫
𝑽𝑫𝑫
Load
𝐂𝐞𝐟𝐟−𝐧
𝟏/𝐀
𝐞𝐟𝐟−𝐧
𝐂𝐞𝐟𝐟−𝐩
𝟏/𝐀
𝐞𝐟𝐟−𝐩
𝑮𝑵𝑫
𝑽𝑫𝑫
Discharging
Load
Charging delay of inverter:
𝐷𝑝 = 𝐶𝑒𝑓𝑓−𝑝/𝐴𝑒𝑓𝑓−𝑝 Discharging delay of inverter: 𝐷𝑛 = 𝐶𝑒𝑓𝑓−𝑛/𝐴𝑒𝑓𝑓−𝑛
Inverter stage delay, 𝑫𝑰𝒏𝒗 = 𝑫𝒑 +𝑫𝒏
On state capacitance and admittance
public
13
ISP removal increases parasitic capacitance by 40 %
𝑲𝒐𝒖𝒕 = 4𝑲𝒊𝒏 = 7.5𝑲𝑺𝒊 = 11.9
~ 40 %
~ 38 %Opt. III: w/o ISP; Stress = 0.7 GPa
Opt. II: w ISP; Stress = 0.0 GPa
Opt. 1: w ISP;Stress = 0.7
GPa
Opt. III: w/o ISP; Stress = -1.7 GPa
Opt. II: w ISP;
Stress = 0.0 GPa
Opt. I: w ISP; Stress = -1.7 GPa
NMOS versus PMOS: D-G Terminals
NMOS PMOS
public
14
ISP removal significantly increases admittance (thanks to max. stress)
NMOS PMOS
~ 6 %
~ 8
2 %
Opt. III: w/o ISP; Stress = 0.7 GPa
Opt. II: w ISP; Stress = 0.0 GPa
Opt. I: w ISP; Stress = 0.7 GPa
Opt. III: w/o ISP; Stress = -1.7 GPa
Opt. II: w ISP;
Stress = 0.0 GPa
Opt. I: w ISP; Stress = -1.7 GPa
NMOS versus PMOS: D-S Terminals
Impact of stress and device architecture on delay performance
public
16
ISP removal increases NMOS effective delay by 15 %
Opt. II: w ISP
Opt. I: w ISP
Opt. III: w/o ISP
Process Advantage: w/o ISP
~15 %
13
5%
10
0 %
0 %
Discharging delay (𝐷𝑛): with and without inner spacer
public
17
ISP removal lowers PMOS effective delay by 36 %
Opt. II: w ISP
Opt. I: w ISP
Opt. III: w/o ISP
Process Advantage: w/o ISP
~36 %
13
5%
10
0 %
0 %
Charging delay (𝐷𝑝): with and without inner spacer
Estimation of 9-stage RO frequency using individual device delay information
𝑫𝑰𝒏𝒗 𝑭 =𝟏
𝟐 × 𝟗 × 𝑫𝑰𝒏𝒗
𝑶𝒖𝒕
Inverter stage delay, 𝑫𝑰𝒏𝒗 = 𝑫𝒑 +𝑫𝒏
public
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6N
orm
. Freq
uen
cy
Opt. II:w ISP
Str. = 0 %
Opt. I:w ISP
Str. = 100 %
Opt. III:w/o ISP
Str. = 100 %19
ISP removal increases RO frequency by 11 % (at realistic stress)
(143.5 GHz)
~50 %
~11 %
public
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6N
orm
. Freq
uen
cy
Opt. II:w ISP
Str. = 0 %
Opt. I:w ISP
Str. = 100 %
Opt. V:w/o ISP
Str. = 135 %20
Applying extra stress can further boost RO frequency
~18 %(143.5 GHz)
public
21
Reducing 𝜅 of ISP offer minor RO frequency improvement
Normalisation Frequency = 143.5 GHz
▪ The RO frequency is less sensitive to inner spacer 𝜿 variation
~4 %
Stress = 0 %
Opt. II: w ISP
Self-heating performance comparison
public23
ISP Removal facilitates heat removal towards substrate
IDEAL HEAT SINK IDEAL HEAT SINK IDEAL HEAT SINK
IDEAL HEAT SINK IDEAL HEAT SINK IDEAL HEAT SINK
2 200 uW/um220
Si SiGe TiN SiN lowK highK W Ru
NS regular
NS w/o inner spacer
finFET (iN3 dim.)
10 1005 50Heat flux
Continuous Si path(inner spacer removed)allows increased heatremoval to substrate
Vertical streaks in fin= ballistic transport
100 nm100 nm100 nm100 nm100 nm100 nm
NS regular
NS w/o inner spacer
finFET (iN3 dim.)
public
24
ISP removal lowers self-heating: NS thermal performance becomes competitive with FinFET
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
-105 -35 35 105
Longitudinal position x [nm]
Finger 1
Finger 2 Finger 3
Finger 4
NMOS side
NS regular
NS w/o inner spacer
finFET
Tem
pera
ture
ris
e [°
C/u
W]
NSregular
NS withoutinner spacer
finFET(iN3 dim.)
A A’ A A’ AA’
A A’
IDEAL HEAT SINK IDEAL HEAT SINK IDEAL HEAT SINK
IDEAL HEAT SINK IDEAL HEAT SINK IDEAL HEAT SINK
public
25
Conclusion
Parasitic capacitance
Admittance
Delay
RO Frequency
RO Frequency (extra stress)
ISP Dielectric
Self-heating
Effects of ISP removal
+40 %
N: +6 % P: +82 %
N: +15 % P: -36 %
+11 %
+18 %
+4 %
-7 %
(Due to increased stress)
(Due to carrier scattering)
(Due to increased stress)
(Due to improved heat removal)
public
Bae, Geumjong, et al. "3nm GAA technology featuring multi-bridge-channel FET for low power and high-performance
applications." 2018 IEEE International Electron Devices Meeting (IEDM). IEEE, 2018.
Barraud, S., et al. "Performance and design considerations for gate-all-around stacked-NanoWires FETs." 2017 IEEE
international electron devices meeting (IEDM). IEEE, 2017.
Loubet, N., et al. "Stacked nanosheet gate-all-around transistor to enable scaling beyond FinFET." 2017 Symposium on VLSI
Technology. IEEE, 2017.
Bardon, M. Garcia, et al. "Power-performance trade-offs for lateral nanosheets on ultra-scaled standard cells." 2018 IEEE
Symposium on VLSI Technology. IEEE, 2018.
Ritzenthaler, R., et al. "Vertically stacked gate-all-around Si nanowire CMOS transistors with reduced vertical nanowires
separation, new work function metal gate solutions, and DC/AC performance optimization." 2018 IEEE International
Electron Devices Meeting (IEDM). IEEE, 2018.
Zhang, Jingyun, et al. "High-k metal gate fundamental learning and multi-V t options for stacked nanosheet gate-all-around
transistor." 2017 IEEE International Electron Devices Meeting (IEDM). IEEE, 2017.
Eneman, Geert, et al. "Stress Simulations of Fins, Wires, and Nanosheets." ECS Transactions 98.5 (2020): 253.
Sentaurus TCAD Design Suite [online]. Available: http://www.synopsys.com.
Ohishi, Yuji, et al. "Thermoelectric properties of heavily boron-and phosphorus-doped silicon." Japanese journal of applied
physics 54.7 (2015): 071301.
26
References
Thank you