Performance Trade-Off Scenarios for GAA Nanosheet FETs ...

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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 Liu Belgium rawat67@ imec.com

Transcript of Performance Trade-Off Scenarios for GAA Nanosheet FETs ...

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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

[email protected]

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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

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Outline

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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

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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

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TCAD Deck Calibration

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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

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ISP removal decreases NMOS on-current

𝑲𝒐𝒖𝒕 = 4𝑲𝒊𝒏 = 7.5

Stress = 0 GPa

NMOS PMOS

Vd = 0.7 V Vd = -0.7 V

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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

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Methodology to estimate RO performance using device parasitcs

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Simplified RC network of device

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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

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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

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On state capacitance and admittance

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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

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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

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Impact of stress and device architecture on delay performance

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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

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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

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Estimation of 9-stage RO frequency using individual device delay information

𝑫𝑰𝒏𝒗 𝑭 =𝟏

𝟐 × 𝟗 × 𝑫𝑰𝒏𝒗

𝑶𝒖𝒕

Inverter stage delay, 𝑫𝑰𝒏𝒗 = 𝑫𝒑 +𝑫𝒏

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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 %

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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)

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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

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Self-heating performance comparison

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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.)

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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

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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)

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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.

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References

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Thank you