Naoki Kasai 1 , Shoji Ikeda 1,2 , Takahiro Hanyu 1,3 , Tetsuo Endoh 1,4 , and Hideo Ohno 1,2 1 Center for Spintronics Integrated Systems, Tohoku University, JAPAN 2 Laboratory for Nanoelectronics and Spintronics, Research Institute of Electrical Communication, Tohoku University, JAPAN 3 Laboratory for Brainware Systems, Research Institute of Electrical Communication, Tohoku University, JAPAN 4 Center for Interdisciplinary Research, Tohoku University, JAPAN http://www.csis.tohoku.ac.jp/ November 7, 2011 2011 11th Non-Volatile Memory Technology Symposium Embedded MRAM Technology For logic VLSI Application 1 Work supported by the FIRST program of JSPS.
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Embedded MRAM Technology For logic VLSI …For logic VLSI Application 1 Work supported by the FIRST program of JSPS. Existing Embedded Memory Market 2 WW Market @ 2010 MOS Micro 61B
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Cell size scaling Low operation power Low standby power
Key challenge Low Power Voltage scaling
Wide temp. range Low cost
Voltage scaling Low cost
World Semiconductor Trade Statistics
3
Trade-off relation between “performance” and “cost”
10M
100M
1G
100 50 10 5 Cell Area Factor, a ( a =cell area/F 2 )
Rea
d C
lock
Fre
quen
cy (H
z)
High-speed eSRAM
eSRAM
SRAM
eDRAM
EEPROM NOR Flash
NAND Flash
eFLASH DRAM
MRAM, FRAM
Low Cost
Hig
h P
erfo
rman
ce
Logic
eSRAM
MPU, ASIC ...
Graphics …
Wide Bandwidth Low Power Large Capacity
High Speed RAM Logic Compatibility
• Low Voltage • Design
Logi
c MCU
eDRAM
Logic
eSRAM
eFlash
High Speed NVM Various Application
• Wide Temp. Range • High Reliability
Memory Portfolio
Alternative eMRAM
4
10M
100M
1G
100 50 10 5 Cell Area Factor, a ( a =cell area/F ) 2
Rea
d C
lock
Fre
quen
cy (H
z)
High-speed eSRAM
eSRAM
SRAM
eDRAM
EEPROM NOR Flash
NAND Flash
eFLASH DRAM
MRAM, FRAM
Low Cost
Hig
h P
erfo
rman
ce
No universal embedded MRAM, but some types of MRAMs must be suitable for embedded applications.
High speed eMRAM
High density eMRAM
Embedded MRAM Issues
5
Standard CMOS Process compatible Suitable memory cell structure Number of cell components; MTJ, transistor, wiring Data write scheme; Magnetic Field, STT, ….
MTJ: Magnetic Tunnel Junction MR ratio Magnetic anisotropy; Materials of stacked thin magnetic layers and tunnel barrier film
Free Layer Tunnel Barrier Fixed Layer
in-plane anisotropy
perpendicular anisotropy
Free Layer Tunnel Barrier Fixed Layer
CMOS Process Compatible
6
Standard CMOS Logic
MTJs formed in back-end of line, BEOL CMOS characteristics unchanged No Yoke (magnetic clad) lines Cu & low-k interconnect applicable 350 ºC thermal stability in BEOL fabrication process MTJ
Spintronics CMOS Logic
MTJ Formation
Typical MRAM Cells
7
MTJ
No Transistor 0Tr + 1MTJ
One Transistor 1Tr + 1MTJ
Two Transistors 2Tr + 1MTJ
Magnetic Field
induced by write current through metal wires
Domain Wall Motion (DWM)
by current through free layer
write word-line
Write bit-line
Spin Transfer Torque (STT) by current through MTJ
Cell Type Data Write Scheme
Domain Wall
MTJ MTJ
MTJ
MTJ
half-selected cell
unselected cell
selected cell
unselected cell
selected cell
Current
Prob
abili
ty Read
Write
Barrier Breakdown
High Density eMRAM Cell
8
Simple cell structure without snake path Random access read/write in cell array Scalable MTJ size & write current Large magneto-resistance(MR) ratio BEOL process temperature 350 ºC Reliability Low tunnel current density Non-volatality Δ=E/k BT
0Tr + 1MTJ 1Tr + 1MTJ 2Tr + 1MTJ
Magnetic Field STT
DWM
In plane Perpendicular
Al2O5
MgO
MgO
Requirements Choices
CoFeB/MgO/CoFeB MTJ
9
S. Ikeda et. al., Appl. Phys. Lett. 93, 082508 (2008).
0
100
200
300
400
500
600
700
1994 1996 1998 2000 2002 2004 2006 2008 2010
トンネル
磁気抵抗比
(%)
年
AlOx-barrier MTJs
CanonANELVA & AIST
AIST
Tohoku Univ. & Hitachi
604%@RT(1144%@5K)
IBMAIST
AIST
TMR
rati
o (%
)Tohoku Univ.
MgO-barrier MTJs
Year
CoFeB
MgO
CoFeB
bcc (001) rock salt (001) bcc(001)
SiO2/Si sub.
Ta(5) Ru(10) Ta(5)
CoFeB(5 ) →
MgO(2.1) CoFeB(6) →
Ta(5) Ru (5) Cr/Au
In-plane anisotropy pseudo-SV
Large MR Ratio
Dependence of tCoFeB on Anisotropy
10
Ikeda et al., Nat. Mat., 9 (2010) pp.721-724
-1
0
1
-0.5 0.0 0.5 1.0
-1
0
1
tCoFeB = 2.0 nm
in-plane out-of-plane
M (
T)
tCoFeB = 1.3 nm
µ0H (T)
In-plane anisotropy
Perpendicular anisotropy
Ta=300oC
Ta=300oC
CoFeB(tCoFeB ) MgO(1)
SiO2/Si sub. Ta(5)
Ru(10) Ta(5)
m0Hs_in-plane = 0.34 T Ms = 1.58 T K = 2.1x105 J/m3
100 50 10 5 Cell Area Factor, a ( a =cell area/F ) 2
Rea
d C
lock
Fre
quen
cy (H
z)
High-speed eSRAM
eSRAM
SRAM
eDRAM
EEPROM NOR Flash
NAND Flash
eFLASH DRAM
MRAM, FRAM DRAM (1T+1C)
STTRAM (1T+1R)
1T+1R STT MRAM must have potential to be substituted for not only embedded DRAM but also commodity DRAM.
MRAM (2T+1R)
Alternative High Speed RAM
16
High speed RAM
10M
100M
1G
100 50 10 5 Cell Area Factor, a ( a =cell area/F ) 2
Rea
d C
lock
Fre
quen
cy (H
z)
High-speed eSRAM
eSRAM
SRAM
eDRAM
EEPROM NOR Flash
NAND Flash
eFLASH DRAM
MRAM, FRAM
High density RAM
DRAM (1T+1C)
STTRAM (1T+1R)
Current
Prob
abili
ty Read
Write
Barrier Breakdown
Current Path (Read & Write)
SRAM (6T)
Write Current
Read Current
High Speed eMRAM Cell
17
0Tr + 1MTJ 1Tr + 1MTJ 2Tr + 1MTJ
Magnetic Field STT
DWM
In plane Perpendicular
Al2O5
MgO
Requirements Choices
Disturb free cell structure High speed random access read/write Scalable MTJ size & write current Large magneto-resistance(MR) ratio BEOL process temperature 350 ºC Reliability Low tunnel current density Non-volatality Δ=E/k BT
Domain Wall
Domain Wall Motion(DWM) Writing
18
Domain Wall
R. Nebashi, et. al., Sym. VLSI Circuits. p. 300, 2011.
1T+1MTJ STT(Spin Torque Transfer) MRAM has the potentials for substitution of embedded DRAM to apply high density embedded NVM application.
2T+1MTJ DWM(Domain Wall Motion) MRAM has the potentials for substitution of embedded SRAM to apply high speed NVM application.
These embedded MRAM technology leads to “logic-in-memory architecture” for future new energy saving SoC(System on a Chip).
Acknowledgements
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This research is granted by the Japan Society for the Promotion of Science (JSPS) through the “Funding Program for World-Leading Innovative R&D on Science and Technology (FIRST Program),” initiated by the Council for Science and Technology Policy (CSTP). Prof. Hideo Ohno has been conducting the program “Research and Development of Ultra-low Power Spintronics-based VLSIs“ as the core researcher.
Thanks to K. Miura, H. Yamamoto, K. Misunuma, H. D. Gan, M, Endo, S. Kanai, J. Hayakawa, F. Matsukura, M. Yamanouchi, J. Hayakawa, R. Kiizumi, S. Fukami, T. Suzuki, K. Nagahara, N. Ohshima, Y. Ozaki, S. Saito, R. Nebashi, N. Sakimura, H. Honjo, K. Mori, C. Igarashi, S. Miura, N. Ishiwata, K. Kinoshita, Y. Nakatani, Y. Tsuji, R. Nebashi, N. Sakimura, H. Honjo, K. Mori, H. Tanigawa, S. Miura, and T. Sugibayashi