NANOELECTRONICS beyond CMOS

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NANOELECTRONICS beyond CMOS David Pulfrey 1 NNI definition of Nanotechnology 1-10 nm is better But Intel prefer... 2 Bourianoff04 1

3 Bourianoff04 4 Moravec04 2

Increasing the Integration Level functional density nanoelectronics functional design 3- D CMOS structural dimensions 1960 2010 year 5 Goser04 Nanotransistors: : the Candidates Molecular switches Spin FETs Single electron transistors Nanotube FETs Nanowire transistors 6 3

Molecular Electronics Use few molecules instead of multi- material transistors *Gates scaleable to densities of greater than 10 12 gates per cm 2. Few electrons/bit - low power Approx 100 molecules Compare: 1fF at 1V 10 4 electrons Billions of identical molecules are easily formed Natural self- assembly Compositional flexibility of organic molecules Tailor properties to achieve device functionality *Memory density of 10 15 bits per cm 3. Human brain 10 13 bytes 7 *DARPA04 Self-assembled Molecular Switch Self-assembly of molecule containing nitroamine redox centre in nitride nanopore 8 Chen99 Neutral Conductive anion Insulating dianion 2 -amino-4-ethynylphenyl-4 -ethynylphenyl-5 -nitro-1-benzenethiol 4

Self-assembled reversible switch 9 MEC01 Molecular electronics: prognosis 10 Chris Gintz, President, MEC March 7, 2003 "It's simply too early to commercialize molecular memory technology at this point," he said. "The problem has turned out to be much more difficult that we anticipated. I think it is very unlikely that we are going to see hybrid molecular electronic and silicon systems anytime soon. It turns out that the processes are extremely difficult." Gintz03 5

SPINTRONICS Generic &inflated term -implies use or spin for information storage and manipulation An extra degree of freedom Nonvolatile and increased data storage Faster data processing (10x) and low power (10-50x) Perhaps not relying on transport Addressing CMOS deficiency 11 Morkoc04 Giant Magnetoresistive Effect Scattering is energy and spin dependent R depends on: spin, and magnetization of medium (controllable by B). Effect is much larger in artificial thin films than in metals Used in hard disk read heads 12 Stoner04 6

What is a Spin Valve? Magnetic analog of an optical polarizer/analyzer Unpolarized light Polarizer Polarized light Analyzer Transmission No transmission 13 Morkoc04 Spin valve AFM/FM combination gives immunity to external fields Modest R change Free FM can be changed by external field 14 Wolf01 7

Magnetic Tunnel junction Replace non- magnetic metal with thin insulating layer 5-10X higher R change Lower I 15 Zorpette01 Spin FET fixed Gate fixed FM thin film Source Dielectric non-conducting Drain Substrate Electrons move from S to D at high (relativistic) velocities Stationary E gate appears to have a B component B causes spin-dependent band splitting and precession (Rashba Effect) Spin under gate is modulated by E gate, e.g., a normally-on FET Flipping is a fast process requiring little energy. This device has not yet left the drawing board! modulated 16 8

Single-electron electron Transistor Principal motivation: greatly reduced power dissipation. Also: increased speed (tunneling) 17 Geppert00 Coulomb Blockade 1 ( nq) Energy of n electrons on capacitor : En = 2 C 2 1 (( n + 1) q) Add another electron : En+ 1 = 2 C 2 1 q (2n + 1) Energy change : E = 2 C Energy change of the electron is qv G 2 1 q (2n + 1) Transfer only allowed if VG = 2 C Use 2 tunnel junctions and make a FET 2 q Need : >> kt 2C i. e. C af 18 Devoret98 9

Room temperature SET Anodization using water-coated tip as cathode 19 Matsumoto04 ETH, TI, UCSB CMOS (high- speed drive, voltage gain) + SET (ultra- low power consumption) = SETMOS (dense, low- power, analog circuits, e.g., NDR, NN, ADC) Coulomb blockade oscillations and operation at - 100C 20 Mahapatra03 10

Nanotubes and Nanowires 21 David04 Single-Walled Carbon Nanotube Hybridized carbon atom graphene monolayer carbon nanotube 2p orbital, 1e - (π-bonds) Metallic or semiconducting Bandgap depends on d 22 UBCnano (Castro) 11

Compelling Properties of Carbon Nanotubes NANOSCALE -- no photolithography BANDGAP TUNABILITY -- 0.5-1.5eV METALS AND SEMICONDUCTORS -- all-carbon ICs BALLISTIC TRANSPORT -- 20-300nm STRONG COVALENT BONDING -- strength and stability of graphite -- no surface states (less scattering, compatibility with many insulators) HIGH THERMAL CONDUCTIVITY -- almost as high as diamond (dense circuits) SELF- ASSEMBLY -- biological, recognition-based assembly 23 UBCnano CNT formation by catalytic CVD 5µm islands in PMMA patterned by EBL 2000nm LPD of Fe/Mo/Al catalyst No field Lift-off PMMA CVD from methane at 1000C 24 Kong98, Ural02 Growth in field (1V/micron) 12

Fabricated Carbon Nanotube FETs Few prototypes [Tans98]: 1 st published device [Wind02]: Top-gated CNFET [Rosenblatt02]: Electrolyte-gated Nanotube 25 UBCnano (Castro) The Ultimate Multi-gate FET chirality: (16,0) radius: 0.62 nm bandgap: 0.63 ev length: 15-100 nm oxide thickness: (R G -R T ): 2-6 nm Boundary Conditions : Φ G V ( RG, z) = VGS q Φ S V ( ρ,0) = q Φ D V ( ρ, L) = VDS q 26 UBCnano 13

MODE CONSTRICTION and TRANSMISSION E T Doubly degenerate lowest mode k z k x CNT (few modes) 27 UBCnano k x METAL (many modes) Interfacial G: even when transport is ballistic in CNT 155 µs for M=2 I-V V dependence on S,D workfunction I D, sat 5µ Intel 15nm 0.4µ A / nm A / nm Negative barrier (p-type) device Positive barrier (p-type) device g m 50µ S/ nm Intel 15nm 1µ S/ nm V GS = - 0.4 V 28 John04 14

Self-assembly of DNA-templated CNFETs 29 Keren03 Carbon Nanotube Summary CNs have excellent thermal and mechanical properties. High DC currents and transconductances are feasible. CNFETs can be self-assembled via biological recognition. CNFETs are promising molecular transistors. But: Presently, cannot pre-determine conductivity type. Presently, coaxial FETs have not been made. 30 15

Coaxial Nanowires Au nanocluster catalyst Axial growth from Au by CVD Radial growth on nanowire surface by changing T and C 31 Lauhon03 Multi-shell Crystalline Heteronanowires 50 nm 5 nm e.g., p- Sion i- Si 32 Lauhon03 16

Ge Nanowire coaxial FET g m 0.15µS/nm 33 Lauhon03 Conclusions Molecular electronics, spintronics: far future. SETs: simulations of dense, low power circuitry, fabrication of single FETs: future. Carbon nanotubes: fabrication of devices and circuits, integration with Si: near future. Nanowires: fabrication of devices: near future. Complementing CMOS will be the key. 34 17

Carbon nanotube on Si IC Proof- of- concept : decoder Possibilities: massive memory, dense sensors. 35 Tseng04 Complementing CMOS CMOS 36 18

References Bourianoff04 - ftp://download.intel.com/research/silicon/bourianoff_nanotrends_052604.pdf Calmec04 - http://www.calmec.com/molecula1.htm Chen99 - J. Chen et al., Science, 286, 1550, 1999 DARPA04 - http://www.darpa.mil/mto/mole/ David04 - ftp://download.intel.com/research/silicon/ken_david_gsf_030604.pdf Devoret98 - http://physicsweb.org/article/world/11/9/7#world-11-9-7-3 Geppert00 - L. Geppert, Spectrum, 46, 2000 Gintz03 - http://www.nanoelectronicsplanet.com/nanochannels/circuit/article/0,4028,10501_2106751,00.html Goser04 - K. Goser et al., Nanoelectronics and Nanosystems, Springer, 2004 John04 - D.L. John et al., Nanotech04, March 2004 Keren03 - K. Keren et al., Science, 302, 1380, 2003 Kong98 - J.Kong et al., Nature, 395, 878, 1998 Lauhon03 - L.J. Lauhon et al., Nature, 420, 57, 2003 Mahapatra03 - S. Mahapatra et al., IEDM, 706, 2003 Matsumoto04 - http://luciano.stanford.edu/~shimbo/set.html MEC01 - http://www.molecularelectronics.com/logicswitch.html Moravec04 - http://www.frc.ri.cmu.edu/~hpm/talks/revo.slides/power.aug.curve/power.aug.html Morkoc04 - Morkoc H., WOCSDICE, Slovakia, 2004 Stoner04 - http://www.stoner.leeds.ac.uk/research/gmr.htm Tseng04 - Y-C. Tseng, Nano Letters, 4(1), 123, 2004 UBCnano - http://nano.ece.ubc.ca Ural02 - A. Ural et al., Appl. Phys. Lett., 81, 3464, 2002 Wolf01 - S.A. Wolf et al., Science, 294, 1488, 2001 Zorpette01 - G. Zorpette, Spectrum, 33, Dec. 2001 37 19