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Semiconductor Nanostructures Ultrafast Laser Spectroscopy Spintronics: A new twist in electronics Bipul Pal Indian Institute of Science Education & Research – Kolkata 02/07/09 1 st Platinum Jubilee Meeting of the Indian Academy of Sciences
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Page 1: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Spintronics: A new twist in electronics

Bipul PalIndian Institute of Science Education & Research – Kolkata

02/07/09

1st Platinum Jubilee Meeting of the Indian Academy of Sciences

Page 2: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Electronics all around …

02/07/09

Page 3: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Trend in electronic devices …

Smaller size

Added functionality

Better performance

Less power consumption

Reduced cost

02/07/09

Page 4: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Trend in electronic devices …

Smaller sizeAdded functionalityBetter performanceLess power consumptionReduced cost

02/07/09

Electronic diary, Radio, Music player, Television, Camera, Web surfing, GPS, Money transaction

Just in size of a small paper back novel, weight ~ 1.1 Kg, 1.6 GHz CPU speed, 160 GB Hard disk, Battery life ~ 9.5 hours!

Page 5: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Moor’s law ‐ 1965

No. of transistor that can be cost‐effectively placed on a IC chip willdouble approximately every two years!

02/07/09

Page 6: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Moor’s law ‐ 1965

02/07/09

Feature size reducingNow 65 nm node2010: 45 nm node2013: 32 nm node2016: 22 nm node

1 nm = 10‐6 mmHuman hair  0.1 mm

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Limitation to miniaturization …

• Heating 

• Leakage current

• Limitation of lithography

• Cost effectiveness

• Laws of quantum mechanics takes over

• Alternatives required!!

02/07/09

Page 8: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Electron has spin!

02/07/09

Tiny magnets!

Spins are randomized in nonmagnetic materialsIts presence was ignored in conventional electronics

Page 9: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Spintronics: spin‐based‐electronics

Utilize “spin‐polarized” electrons to• Store

• Process

• Transmit

information 

02/07/09

Page 10: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Spintronics: benefits …

• Spin interaction weaker than Coulomb interaction – Less interference from environment

• Spin current flows almost without dissipation– Less heating

• Spin can flip very fast; requires small energy– Fast operation,  Less power consumption

• Non‐volatile memory– Storage and manipulation in single chip

• Manipulation by polarized photons– Easy external control

02/07/09

MoreMiniaturization;Higher speed

New features

Page 11: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Spintronics device already in market

• Nonvolatile magnetic memory (MRAM)

• Magnetic read‐head (uses GMR device)

• Magnetic sensors

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Spintronics: dream …

• Personal computers mayBecome small and super fast and yet cheapBoast terabytes of memoryKeep data in active memory even when switched off Boot up instantlyConsume less power

• Futuristic application …– Quantum computation– Quantum information processing 

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Quantum computation: spin as qubit

Quantum computer

Classical bits (0 or 1) replaced by quantum bits (qubits) that can be in 

a superposition of states.

Use spin ½ as a qubit.

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Quantum dot based quantum computers

• Coupled-GaAs quantum dots containing one electron per dot

• D. Loss and D.P. DiVincenzo, Phys. Rev. A 57, 120 (1998)

Long spin lifetime is essential for quantum computation!

• Quantum dot defined in 2DEG by side gates• Coulomb blocked used to get one electron per dot• Spin of electron is qubit• Controllable coupling of dots by point‐contact gate voltage• Readout by gatable magnetic barrier

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

We study spin dynamics in single electron doped InP QDs using 

optical spectroscopy 

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Photon polarization      electron spin

Band structure and symmetry of crystal

Selection rule of optical transition

σ+ polarization σ− polarization

02/07/09

Page 17: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Photon polarization      electron spin1) Spin dynamics can be studied using polarization 

selective optical spectroscopy2) Electron spin may be used for quantum information 

processing

02/07/09

Page 18: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Why QDs are interesting?

QDs are called artificial atoms Carriers spatially confined in all 3D within ~10 nm

3D quantum confinement  discrete statesMany spin relaxation mechanisms suppressed

Long spin lifetime expected [†]

[†] See, e.g., Khaetskii et al., PRB 61, 12639 (2000); PRB 64, 125316 (2001);Woods et al., PRB 66, 161318 (2002).

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Sample structure

Charge state of the QDs is controlled by external electric bias (Ub). For Ub= −0.1V, QDs are singly negatively charged [ ]

Schematic of the sample growth structure.

100 nm

100 nm

300 nm

[ ] Kozin et al., PRB 65, 241312 (20002)

Dot density ~1010 /cm2

02/07/09

Page 20: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

How to probe spin dynamics?

Measure the degree of circular polarization (P)of photoluminescence (PL) to probe the spindynamics

Here          is the PL intensity for     excitation and          detection 

−+++

−+++

+−

=IIIIP

)(−++I +σ)(−+σ

02/07/09

Page 21: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

How to probe spin dynamics?

Degree of PL circular polarization:                        where           is PL 

intensity for      excitation and         detection −+++

−+++

+−

=IIIIP )(−++I

+σ )(−+σ

σ+ polarization σ− polarization

P maximum P  zeroP reduced

02/07/09

Page 22: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time‐resolved measurement of P

02/07/09

Page 23: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time‐resolved polarized PL

0.0 0.2 0.4 0.6 0.8 1.0-60

-40

-20

0

20

40

0.0 0.2 0.4 0.6 0.8 1.00

2

4

6

8

Pol

ariz

ed P

L (a

rb. u

nits

)

Time (ns)

Ι + −

Ι + +

T = 2 K, Ub = −0.1 VB = 0.1 T, P = 5 mW Ι + ++ Ι + −

Time (ns)

Deg

ree

of P

Lci

rcul

ar p

olar

izat

ion

(%)

P = Ι + +− Ι + −

Degree of PL circular polarization reached a negative value and remained constant up to the PL decay time

ANCP

02/07/09

Page 24: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time‐resolved polarized PL

0.0 0.2 0.4 0.6 0.8 1.0-60

-40

-20

0

20

40

0.0 0.2 0.4 0.6 0.8 1.00

2

4

6

8

Pol

ariz

ed P

L (a

rb. u

nits

)

Time (ns)

Ι + −

Ι + +

T = 2 K, Ub = −0.1 VB = 0.1 T, P = 5 mW Ι + ++ Ι + −

Time (ns)

Deg

ree

of P

Lci

rcul

ar p

olar

izat

ion

(%)

P = Ι + +− Ι + −

Excitation: ~1.77 eV → e‐h pair in excited stateDetection: ~1.73 eV → ground state luminescence

ANCP is maximum under this condition

ANCP

02/07/09

Page 25: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Excitation and detection energy

1.70 1.75 1.80 1.85 1.90 1.950

2

4

6

exci

tatio

n

Energy (eV)

PL s

igna

l (ar

b. u

nits

)

dete

ctio

n

InPQDs

InGaPbarrier

PL spectrumT = 4.2 Kλexc = 532 nm

Excitation: ~1.77 eV→ e‐h pair in excited stateDetection: ~1.73 eV→ ground state luminescence

02/07/09

Page 26: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

A simple model of PL polarization

Depending on parallel or antiparallel orientation of photo‐created and resident electron spins, two types of QDs: P‐typeand A‐type QDs

02/07/09

Page 27: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

A simple model of PL polarization

02/07/09

Page 28: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

A simple model of PL polarization

Degree of PL circular polarization is negative (positive) for P‐type (A‐type) QDs

Net PL polarization from the QD ensemble is determined by the ratio of P‐ & A‐type QDs

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time‐resolved polarized PL

0.0 0.2 0.4 0.6 0.8 1.0-60

-40

-20

0

20

40

0.0 0.2 0.4 0.6 0.8 1.00

2

4

6

8

Pol

ariz

ed P

L (a

rb. u

nits

)

Time (ns)

Ι + −

Ι + +

T = 2 K, Ub = −0.1 VB = 0.1 T, P = 5 mW Ι + ++ Ι + −

Time (ns)

Deg

ree

of P

Lci

rcul

ar p

olar

izat

ion

(%)

P = Ι + +− Ι + −

Degree of PL circular polarization reached a negative valuePhoto‐excitation converted A‐type QDs to P‐type QDs!!

02/07/09

Page 30: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time‐resolved polarized PL

0.0 0.2 0.4 0.6 0.8 1.0-60

-40

-20

0

20

40

0.0 0.2 0.4 0.6 0.8 1.00

2

4

6

8

Pol

ariz

ed P

L (a

rb. u

nits

)

Time (ns)

Ι + −

Ι + +

T = 2 K, Ub = −0.1 VB = 0.1 T, P = 5 mW Ι + ++ Ι + −

Time (ns)

Deg

ree

of P

Lci

rcul

ar p

olar

izat

ion

(%)

P = Ι + +− Ι + −

PL polarization remained constant up to PL decay time  spin memory longer than electron‐hole recombination lifetime !!

02/07/09

Page 31: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

A pump‐probe schemeNet PL polarization determined by ratio of P‐ & A‐type QDs.

A pump pulse create optical orientation which is thenmonitored by measuring PL polarization of a delayed probe

When pump and probe are co‐circularly polarized more P‐type QDs at zero pump‐probe delay (τ)When pump and probe are cross‐circularly polarized moreA‐type QDs at τ = 0Difference (PCR – PCO) is a good measure of pump induced spinpolarization

02/07/09

Page 32: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Pump‐probe setup

02/07/09

PMT

Page 33: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Pump‐probe scheme

02/07/09

Detect probe PL by time‐gated measurement

ProbePump

Page 34: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Pump‐probe scheme

02/07/09

Detect probe PL by time‐gated measurement

Probe

Pump

Page 35: Spintronics: A new twist in electronics · 2019-04-09 · Spintronics: dream … • Personal computers may. 9. Become small and super fast and yet cheap. 9. Boast terabytes of memory.

Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Millisecond‐range spin memory

0.0 0.4 0.8 1.2 1.6 2.0

1

10

100T = 2 K B = 0.1 TUbias= −0.1 V

Delay (ms)

P CR−

P CO (%

) Wpump= 0.5 W/cm2

Wprobe= 0.05 W/cm2

Spin memory decays by 1 order of magnitude in 1 ms

Nonexponential decay  distribution of decay rates due to size distribution of QDs, presence of paramagnetic defects… 

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

More spin dynamics study

• “Sub‐millisecond electron spin relaxation in InP quantum dots”, Phys. Rev. B 72, 153302 (2005).

• “Millisecond‐range electron spin memory in singly charged InP quantum dots”, J. Phys. Soc. Jpn. 75, 054702 (2006). 

• “Spin dephasing of doped electrons in charge‐tunable InP quantum dots: Hanle‐effect measurements”, Phys. Rev. B 74, 205332 (2006). 

• “Nuclear‐spin effects in singly negatively charged InP quantum dots”, Phys. Rev. B 75, 125322 (2007). 

• Collaborators• Y. Masumoto and M. Ikezawa, Univeristy of Tsukuba, Japan• I. Ignatiev and S. Yu. Vervin, St. Petersburg State University, 

Russia

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Summery

• Introduced spintronics = spin based electronics

• Boost to the electronics industry

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

ElectronCharge

Photon Polarisation

ElectronSpin

Semiconductor Spintronics

Summery

Benefits: Fast, small, low dissipation devices

Quantum computation?

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Summery

• Optical study of spin dynamics in QDs

• Long spin lifetime in charged InP QDs

02/07/09

0.0 0.4 0.8 1.2 1.6 2.0

1

10

100T = 2 K B = 0.1 TUbias= −0.1 V

Delay (ms)

P CR−

P CO (%

)

Wpump= 0.5 W/cm2

Wprobe= 0.05 W/cm2

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Model of optical pumping

Optical pumping is conversion of aresident electron spin parallel tothe helicity of incident light

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time synchronization

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time synchronization

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time synchronization

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time synchronization

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Time synchronization

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

PL spectrum

1.70 1.75 1.80 1.85 1.90 1.950

2

4

6

Energy (eV)

PL

sign

al (a

rb. u

nits

) InPQDs

InGaPbarrier

PL spectrumT = 4.2 Kλexc = 532 nm

02/07/09

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Semiconductor Nanostructures

Ultrafast Laser Spectroscopy

Why charged  QDs?

Neutral QDs

Spin lifetime (τs) ≤ recombination lifetime (τr) 

eh

Charged QDs

Resident electron:infinite lifetime

Optical pumping

eh

Photo‐generated electron

Resident electron

τs not limited by τr

QDs – artificial atom – discrete energy states

Bulk spin relaxation mechanisms suppressed 

Long electron spin relaxation time expected

02/07/09


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