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Spintronics
“A Spin to Remember”
Presented By :- Presented To :-
Md. Saown Khan Mr. Tariqul Islam Shakil
ID:153-23-4454 Department of EEE
Lecturer
Daffodil international university
Outline
• Spintronics basics
• The giant magneto resistance
• Applications of GMR
• Spin devices
• Injections & detection of spin
• The MRAM
• Recent trends
What is Spintronics?
• Utilizes the bizarre
property of spin of
electron.
• Intrinsic angular
momentum is spin.
• Two arbitrary
orientations, and its
magnitudes are ± ħ / 2 (ħ
is Plank constant).
• Directional and coherent
motion of electron spin
circulates a spin current,
which will carry or
transport information and
control quantum spin in
an spintronic device.
Why Spintronics?
• Moore’s Law:
No. of Transistor doubles in every 18 months.
• Complexity:
Complex Chip Design & Power Loss.
• Motivation:
Spintronics-Information is carried not by electron
charge but by it’s spin.
Moore’s law
Combining the best of both worlds
Ferro magnets
• Stable Memory
• Fast switching
• High ordering temp
• Spin transport
• Technological base
(magnetic recordings)
Semiconductors
• Bandgap engineering
• Carrier density & type
• Electrical gating
• Long spin lifetime
• Technological base
(Electronics)
The Giant Magneto Resistance
• A Nano scale phenomena .
• Giant refers to giant change in resistance due to current.
• It is a quantum mechanical magneto resistance effect
observed in thin-film structures composed of alternating
ferromagnetic and non-magnetic layers.
Magnetic tunneling junction
• Like GMR but better.
• More sensitive
• Multilayer junction filter
• Quantum mechanical
principle
• Tunneling effect
• 2 layers of magnetic
metal, separated by an
ultrathin layer of
insulator, about 1 nm.
Spin transistor
• Supriyo Datta and Biswajit Das Transistor
Spin injection into silicon
• Injection
Spin manipulation
• Hanle effect :- Suppression of spin accumulation
Ferro magnet
Oxide
B
Spin
Silicon
Magnetic field along the spin
• Hanle curve for a) Ge , b) Si
Detection of spin polarization in
silicon
Ferro magnet Al2O3
Tunnel barrier
e-
n type Silicon
Spin accumulation
u
Tunnel resistance in proportional to u
I = G * ( V - u/2)
I = G * ( V + u/2)
MRAM
Magneto resistive RAM
Reading process
• Measurement of the bit
cell resistance by
applying a current in the
‘bit line’
• Comparison with a
reference value mid-
way between the bit
high and low resistance
values
MRAM
Magneto resistive RAM
Writing process
• Currents applied in both
lines : 2 magnetic fields
• Both fields are necessary
to reverse the free layer
magnetization
• When currents are
removed : Same
configuration
MRAM
Magneto resistive RAM
Array structure of MRAM
• Reading: transistor of the
selected bit cell turned
‘on’ + current applied in
the bit line
• Writing: transistor of the
selected bit cell turned
‘off’ + currents applied in
the bit and word lines
• Need of 2 magnetic fields
for writing
MRAM vs …..
MRAM
Magneto resistive RAM
• MTJ test structures developed at SPINTEC: the die area with 1x5 μm
• 0.2 μm width isolated MTJ element after etch
Advantages of Spintronics
 Low power consumption.
 Less heat dissipation.
 Spintronic memory is non-volatile.
 Takes up lesser space on chip, thus more compact.
 Spin manipulation is faster , so greater read & write speed.
 Spintronics does not require unique and specialized
semiconductors.
Common metals such as Fe, Al, Ag , etc. can be used.
Conclusion
• Spin property of electrons are yet to mastered.
• Researcher and scientist are taking keen interest.
• Universities and electronic industries collaborating .
• Span of last two decade major milestones.
• It holds vast opportunities for physics , material & device
engineering & technology
• Last year PTB, Germany, have achieved a (2GBit/s)
write cycle
• Potential of the field is colossal and
continuous development is required.
Basic electrical and electronic engineering

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Basic electrical and electronic engineering

  • 1. Spintronics “A Spin to Remember” Presented By :- Presented To :- Md. Saown Khan Mr. Tariqul Islam Shakil ID:153-23-4454 Department of EEE Lecturer Daffodil international university
  • 2.
  • 3. Outline • Spintronics basics • The giant magneto resistance • Applications of GMR • Spin devices • Injections & detection of spin • The MRAM • Recent trends
  • 4. What is Spintronics? • Utilizes the bizarre property of spin of electron. • Intrinsic angular momentum is spin. • Two arbitrary orientations, and its magnitudes are ± ħ / 2 (ħ is Plank constant). • Directional and coherent motion of electron spin circulates a spin current, which will carry or transport information and control quantum spin in an spintronic device.
  • 5. Why Spintronics? • Moore’s Law: No. of Transistor doubles in every 18 months. • Complexity: Complex Chip Design & Power Loss. • Motivation: Spintronics-Information is carried not by electron charge but by it’s spin.
  • 7. Combining the best of both worlds Ferro magnets • Stable Memory • Fast switching • High ordering temp • Spin transport • Technological base (magnetic recordings) Semiconductors • Bandgap engineering • Carrier density & type • Electrical gating • Long spin lifetime • Technological base (Electronics)
  • 8. The Giant Magneto Resistance • A Nano scale phenomena . • Giant refers to giant change in resistance due to current. • It is a quantum mechanical magneto resistance effect observed in thin-film structures composed of alternating ferromagnetic and non-magnetic layers.
  • 9.
  • 10.
  • 11. Magnetic tunneling junction • Like GMR but better. • More sensitive • Multilayer junction filter • Quantum mechanical principle • Tunneling effect • 2 layers of magnetic metal, separated by an ultrathin layer of insulator, about 1 nm.
  • 12.
  • 13. Spin transistor • Supriyo Datta and Biswajit Das Transistor
  • 14. Spin injection into silicon • Injection
  • 15. Spin manipulation • Hanle effect :- Suppression of spin accumulation Ferro magnet Oxide B Spin Silicon
  • 16. Magnetic field along the spin • Hanle curve for a) Ge , b) Si
  • 17. Detection of spin polarization in silicon Ferro magnet Al2O3 Tunnel barrier e- n type Silicon Spin accumulation u Tunnel resistance in proportional to u I = G * ( V - u/2) I = G * ( V + u/2)
  • 18. MRAM Magneto resistive RAM Reading process • Measurement of the bit cell resistance by applying a current in the ‘bit line’ • Comparison with a reference value mid- way between the bit high and low resistance values
  • 19. MRAM Magneto resistive RAM Writing process • Currents applied in both lines : 2 magnetic fields • Both fields are necessary to reverse the free layer magnetization • When currents are removed : Same configuration
  • 20. MRAM Magneto resistive RAM Array structure of MRAM • Reading: transistor of the selected bit cell turned ‘on’ + current applied in the bit line • Writing: transistor of the selected bit cell turned ‘off’ + currents applied in the bit and word lines • Need of 2 magnetic fields for writing
  • 22. MRAM Magneto resistive RAM • MTJ test structures developed at SPINTEC: the die area with 1x5 μm • 0.2 μm width isolated MTJ element after etch
  • 23. Advantages of Spintronics  Low power consumption.  Less heat dissipation.  Spintronic memory is non-volatile.  Takes up lesser space on chip, thus more compact.  Spin manipulation is faster , so greater read & write speed.  Spintronics does not require unique and specialized semiconductors. Common metals such as Fe, Al, Ag , etc. can be used.
  • 24. Conclusion • Spin property of electrons are yet to mastered. • Researcher and scientist are taking keen interest. • Universities and electronic industries collaborating . • Span of last two decade major milestones. • It holds vast opportunities for physics , material & device engineering & technology • Last year PTB, Germany, have achieved a (2GBit/s) write cycle • Potential of the field is colossal and continuous development is required.