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Electrothermal Model-based Analysis for Novel Phase-Change Memory Structure with Decoupled Program and Read Paths Date : 2021. 03. 31 Inhyuk Choi Neuromorphic Materials and Devices Laboratory (NMDL) Department of Materials and Science and Engineering, Seoul National University 1

Electrothermal Model-based Analysis for Novel Phase-Change

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Page 1: Electrothermal Model-based Analysis for Novel Phase-Change

Electrothermal Model-based Analysis for Novel Phase-Change

Memory Structure with Decoupled Program and Read Paths

Date : 2021. 03. 31

Inhyuk Choi

Neuromorphic Materials and Devices Laboratory (NMDL)

Department of Materials and Science and Engineering, Seoul National University

1

Page 2: Electrothermal Model-based Analysis for Novel Phase-Change

Outline 2

Introductionβ€’ Phase Change Memory (PCM)β€’ Issues on conventional PCM structure

Novel PCM structureβ€’ Conceptβ€’ Electrothermal model: Joule heating β€’ Electrothermal model: Joule heating + Thermoelectric effectsβ€’ Possibility of cyclic endurance enhancement

Summary

Page 3: Electrothermal Model-based Analysis for Novel Phase-Change

Outline 3

Introductionβ€’ Phase Change Memory (PCM)β€’ Issues on conventional PCM structure

Novel PCM structureβ€’ Conceptβ€’ Electrothermal model: Joule heating β€’ Electrothermal model: Joule heating + Thermoelectric effectsβ€’ Possibility of cyclic endurance enhancement

Summary

Page 4: Electrothermal Model-based Analysis for Novel Phase-Change

Introduction 4

Storage Class Memory Neuromorphic Computing

A. Lotnyk et al., Nanoscale Adv., (2019)

Q. Z. Wan et al., Adv. Mater. Technol. Rev., (2019)

Page 5: Electrothermal Model-based Analysis for Novel Phase-Change

Introduction 5

Non-Volatile

Memory

Key properties Endurance

Power consumption

Write & Read Speed

PRAM RRAM MRAM

S. Bhatti et al., Materials Today, (2017)

G. W. Burr et al., Adv. Physics X, (2017)

Page 6: Electrothermal Model-based Analysis for Novel Phase-Change

Motivation 6

Issues in conventional PCM structures: 1) πˆπˆπ‘π‘π‘π‘π‘π‘π‘π‘π‘π‘ 𝐯𝐯𝐯𝐯 𝐑𝐑𝐑𝐑𝐑𝐑𝐑𝐑 Trade-off

Reduction of RESET power by increasing 𝑹𝑹𝒕𝒕𝒕𝒕 Contact / Cell size reduction increases both 𝑅𝑅𝑑𝑑𝑑 & 𝑅𝑅𝑒𝑒𝑒𝑒 Material doping increases both πœŒπœŒπ‘‘π‘‘π‘‘ & πœŒπœŒπ‘’π‘’π‘’π‘’ (by W-F Law)

However, for fast readout (< πŸ“πŸ“πŸ“πŸ“πŸ“πŸ“πŸ“πŸ“),

𝑹𝑹𝑺𝑺𝑺𝑺𝑺𝑺 < ~πŸπŸπŸ“πŸ“πŸ“πŸ“πŸπŸπ›€π›€ is required!Boniardi, M. et al., IEDM, (2014)

Lacaita, A. L. et al., Microelectron. Eng., (2013)

Page 7: Electrothermal Model-based Analysis for Novel Phase-Change

7Motivation

β€’ Stuck SET: Gradual elemental segregation

β€’ Stuck RESET: Void formation near the contact

Burr, G. W. et al., J. Vac. Sci. Technol., (2010) Yang, T-Y. et al., Appl. Phys. Lett., (2009)

High electric fields in phase change material is one of the main driving forces.

Due to integrated program and read paths

Issues in conventional PCM structures: 2) Cyclic Endurance Failure

Page 8: Electrothermal Model-based Analysis for Novel Phase-Change

Outline 8

Introductionβ€’ Phase Change Memory (PCM)β€’ Issues on conventional PCM structure

Novel PCM structureβ€’ Conceptβ€’ Electrothermal model: Joule heating β€’ Electrothermal model: Joule heating + Thermoelectric effectsβ€’ Possibility of cyclic endurance enhancement

Summary

Page 9: Electrothermal Model-based Analysis for Novel Phase-Change

Novel PCM structure 9

Separated program and read paths.

Breaks out of the 𝑰𝑰𝑹𝑹𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺 vs 𝑹𝑹𝑺𝑺𝑺𝑺𝑺𝑺 trade-off.

Enhancement of the cyclic endurance.: Significant reduction of the electromigration.

Thermoelectric effects can be maximized.: Reduction of the power consumption.

Concept

Page 10: Electrothermal Model-based Analysis for Novel Phase-Change

Model-based Analysis 10

Geometry Equations

𝛻𝛻 οΏ½ 𝐽𝐽 = βˆ’π›»π›» οΏ½ 𝜎𝜎 𝛻𝛻𝛻𝛻 = 0

𝑑𝑑𝐢𝐢𝑃𝑃𝑑𝑑𝑑𝑑𝑑𝑑𝑑𝑑 βˆ’ 𝛻𝛻 οΏ½ (πœ…πœ…π›»π›»π‘‘π‘‘) =

𝐽𝐽 � 𝐽𝐽𝜎𝜎

2D Axisymmetric analysis

The heater needs to be stable at high temperatures (e.g. Refractory metals)

Comparison of 𝑰𝑰𝑹𝑹𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺 π’—π’—πŸ“πŸ“ 𝑹𝑹𝑺𝑺𝑺𝑺𝑺𝑺 curve with reducing β€˜r’ of heating materials

Electrothermal model: Joule Heating effects

𝐽𝐽: Current density𝜎𝜎: Electrical Cond.𝛻𝛻: Electric potential𝑑𝑑: Mass density𝐢𝐢𝑝𝑝: Heat capacityπœ…πœ…: Thermal Cond.

Page 11: Electrothermal Model-based Analysis for Novel Phase-Change

Results 11

(𝐼𝐼𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅: when 𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅/𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅 β‰ˆ 103)

Consistent 𝑹𝑹𝑺𝑺𝑺𝑺𝑺𝑺 while reducing 𝑰𝑰𝑹𝑹𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺.: Cell scaling no longer affects read speed.

Energy efficiency should be improved.: Thermoelectric effects for additional heat.

Thermoelectric effects- Seebeck + Peltier + Thomson effect.- Conversion between heat and electricity.

Comparison of πˆπˆπ‘π‘π‘π‘π‘π‘π‘π‘π‘π‘ 𝐯𝐯𝐯𝐯 𝐑𝐑𝐑𝐑𝐑𝐑𝐑𝐑 Trend

Page 12: Electrothermal Model-based Analysis for Novel Phase-Change

12Model-based Analysis Electrothermal model: Joule heating + Thermoelectric effects

Geometry Equations

𝛻𝛻 οΏ½ 𝐽𝐽 = βˆ’π›»π›» οΏ½ 𝜎𝜎 𝛻𝛻𝛻𝛻 + 𝑆𝑆𝛻𝛻𝑑𝑑 = 0

𝑑𝑑𝐢𝐢𝑃𝑃𝑑𝑑𝑑𝑑𝑑𝑑𝑑𝑑

βˆ’ 𝛻𝛻 οΏ½ πœ…πœ…π›»π›»π‘‘π‘‘ =𝐽𝐽 οΏ½ 𝐽𝐽𝜎𝜎

βˆ’ 𝑑𝑑𝐽𝐽 οΏ½ βˆ†π‘†π‘† βˆ’ 𝑑𝑑𝐽𝐽 �𝑑𝑑𝑆𝑆𝑑𝑑𝑑𝑑

𝛻𝛻𝑑𝑑

Assumption: Two heater materials

𝐽𝐽: Current density𝜎𝜎: Electrical Cond.

𝐢𝐢𝑝𝑝: Heat capacityπœ…πœ…: Thermal Cond.

𝛻𝛻: Electric potential𝑑𝑑: Mass density

Page 13: Electrothermal Model-based Analysis for Novel Phase-Change

Results 13

R-I curve change according to the β€˜S’ value

< Seebeck effect only > < Peltier effect only >

Page 14: Electrothermal Model-based Analysis for Novel Phase-Change

14

Temperature distribution

Joule Heating(JH)

JH + PH(βˆ†π‘Ίπ‘Ί = πŸπŸπŸ“πŸ“πŸ“πŸ“)

JH + PC(βˆ†π‘Ίπ‘Ί = βˆ’πŸπŸπŸ“πŸ“πŸ“πŸ“)

(Under positive polarity)

𝑺𝑺𝑨𝑨 > πŸ“πŸ“, 𝑺𝑺𝑩𝑩 < πŸ“πŸ“ Heaters become resistive by

the Seebeck effect.

βˆ†π‘Ίπ‘Ί = 𝑺𝑺𝑨𝑨 βˆ’ 𝑺𝑺𝑩𝑩 > πŸ“πŸ“ βˆ†π‘†π‘† > 0: Peltier Heating(PH). βˆ†π‘†π‘† < 0: Peltier Cooling(PC).

Reduction of πˆπˆπ‘π‘π‘π‘π‘π‘π‘π‘π‘π‘

(Under the same voltage)

Results

𝐑𝐑𝐦𝐦𝐦𝐦𝐦𝐦 = πŸπŸπŸ“πŸ“πŸπŸπŸ“πŸ“πŸπŸπ‘π‘π¦π¦π¦π¦π¦π¦ = πŸπŸπŸπŸπŸπŸπŸ“πŸ“πŸπŸ 𝐑𝐑𝐦𝐦𝐦𝐦𝐦𝐦 = πŸπŸπŸπŸπŸπŸπŸ“πŸ“πŸπŸ

Page 15: Electrothermal Model-based Analysis for Novel Phase-Change

15ResultsComparison of πˆπˆπ‘π‘π‘π‘π‘π‘π‘π‘π‘π‘ 𝐯𝐯𝐯𝐯 𝐑𝐑𝐑𝐑𝐑𝐑𝐑𝐑 Trend, Power consumption

101 102 10310-1

100

101

102

R(I)

/R(I=

200Β΅

A)

IRESET [Β΅A]

Confined cell Confined cell (+TE) Novel cell Novel cell(+TE) Ref. 1 Ref. 2

r = 4nm, π‘Ίπ‘ΊπŸ“πŸ“= 100 β†’ 500

Page 16: Electrothermal Model-based Analysis for Novel Phase-Change

Discussions 16

Possibility of cyclic endurance enhancement

Page 17: Electrothermal Model-based Analysis for Novel Phase-Change

Summary 17

Based on the electrothermal model, the novel PCM structure with the separated program and read paths no longer has a πˆπˆπ‘π‘π‘π‘π‘π‘π‘π‘π‘π‘ 𝐯𝐯𝐯𝐯 𝐑𝐑𝐑𝐑𝐑𝐑𝐑𝐑 trade-off of the existing PCM structures.

Energy efficiency can be greatly improved by maximizing the thermoelectric effects in the novel PCM structure.

Cyclic endurance can be enhanced in the novel PCM structure since the electromigration in the phase change material is expected to be significantly reduced during the program.