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Magnetism at Oxide Interface
Sanjay Kumar NayakPh.D. Student
Epitaxy Lab
CPMU Seminar
Outline
Introduction
Materials under Studies
Magnetic Measurements
Microscopic Origin
Approach towards Devices
Conclusion
Introduction
Conductance and Operation
Role of Electron in Modern Technology
Charge Spin Magnetism and
Information Storage
Nobel Prize (2007)
Peter Grünberg Albert FertNobel Prize (1956)
Role of Electron in Modern Technology
Goal Multifunctional devicePut both charge and spin together for faster and smaller devices
What is the obstacle ?
Lack of suitable material !Does oxide have potential?
May be!
e-±1/2 ħ ±1/2 ħ
e-
Conventional Semiconductor
Physics:
• Large overlap of s/p orbitals gives extended wave functions
• No intrinsic magnetism or other correlations
Technology:
• Quality: High - Can be fabricated into complex structures
• Understanding: Semiconductor modeling is straightforward
• Tunability: control charge with modest doping/ E fields
Complex Oxide Materials
Physics:
• localization of 3d/2p orbitals gives strong Coulomb interactions
• diverse magnetic and other strong Correlations
Technology:
• Quality: Materials chemistry challenging; fabrication less developed
• Understanding: Strong correlations challenging to theoretical tools
• Tunability: High - due to competing ordered states
Conventional Semiconductors versus
Complex Oxides
Importance of Oxides
Co existence of charge, spin, orbital and lattice degree of freedom
Correlation between these degree of freedom and related coupling
generates rich varieties of phases which are highly tunable to
internal and external parameters
Virtually all phases of matter are found in Oxide family
High temp. Superconductivity
Metal insulator transition
Colossal magneto resistance
(anti-)Ferromagnetism
(anti-)Ferro electricity
Piezoelectricity
Multiferroics
For understanding of fundamental nature of existing materials
well as application, oxides are important.
Why Surfaces or Interfaces ?
Herbert Kroemer:
“The interface is the device’’
Oxide based electronics:
Put the many-body properties of correlated
electrons: superconductivity, magnetism,
multiferroicity , metal-insulator transitions.....
to practical use.
Prof. Herbert Kroemer
Noble prize (2000) in
physics for developing
semiconductor
heterostructures used in
high-speed- and opto-
electronics
Image adopted from Wikipedia
Materials under Studies
Emerging Oxide Materials
• LaAlO3 /SrTiO3
• La0.7Ca0.3MnO3/YBa2Cu3O7
• La0.7Ca0.3MnO3/PrBaCu3O7
• BiFeO3/La0.7Sr0.3MnO3
• CaMnO3/CaRuO3
• LaMnO3/SrMnO3
LaAlO3 /SrTiO3
“Drosophila of Oxide Physics”
SrTiO3 (STO)
• Band insulator (band gap of 3.2 eV)
• Non magnetic
• Good for substrate
LaAlO3 (LAO)
• Band insulator (5.6 eV)
• Non magnetic
Both have ABO3 (Perovskite) crystal structure
When both Oxides meet face to face
Reyren et al. Science 317,1196(2007) Ariando et al Nat commun. 2, 188 (2011)
H(kOe)
(kΩ
cm-2
)
Magnetic Studies
Magnetic Measurement Tools
• SQUID (Overall magnetization of sample)
• Torque magnetometer
• XMCD (Elemental sensitivity)
• Magneto resistance
SQUID Results
Ariando et al Nat commun. 2, 188 (2011)No sign of any magnetic impurity in SIMS measurement
H(kOe)
H(kOe) H(kOe)
H(kOe)
Scanning SQUID Results
Kalisky et al Nat.Comm.,3,922(2012)
Critical Thickness: 3.3 unit cell of LAO
Annealed STO 2 uc of LAO 5 uc of LAO 10 uc of LAO
Torque τ = M HDeflection of cantilever
Torque
Lu Li et al. Nature Physics 7 ,762(2011)
Torque magnetometry
Sensitivity:10-13-10-12 A m-2 at 10T
M proportional to HTorque = M×H H2
For H → 0 , m → 5 10-10 A m-2
0.3 to 0.4 μB per interface Unit Cell
Lu Li et al. Nature Physics 7 ,762(2011)
Torque magnetometry Results
• SQUID and Torque magnetometer can give idea about whether material is magnetic or not
• Can not tell whether magnetic properties are intrinsic or because of impurity
• Can not explain the origin of magnetism
Intrinsic Magnetism or Not?
Microscopic Origin
Microscopic Origin of Interface Magnetism
X-ray Magnetic Circular Dichroism
XMCD = XAS with Polarized photons(circularly or linearly)
Element Specificity
Orbital Selectivity
Sensitivity is very high (0.005 μB per atom )
Electron – Electron Interaction through Exchange Coupling
I N(Ef) > 1, I = coupling strength
ms= -2 <Sz> μB/ ħ = (N↑-N ↓) μB
Stoner’s model for Ferromagnetism
Principle Behind XMCD
Core Electron excited in absorption process
in to empty state above the Fermi level
Right Circular Photons (RCP) transfer
the opposite momentum to the electron as
Left Circular Photons (LCP)
www-ssrl.slac.stanford.edu/stohr/xmcd.htm
unoccupied, CB
occupied, VB
variable hn
core level
Excitation of electron 2p core level to 3d unfilled state (L-edge x-ray
absorption spectra)
Sum of IL3 and IL2 will give total vacant “d- hole”
Principle Behind XMCD
Theoretical Predictions on the Origin of Magnetism
In absence of extrinsic magnetic impurities, interface ferromagnetic
originate from Ti atom.
Pentcheva et al., PRB ,74,035112(2006)
Popovic et al., PRL, 101,256801(2008)
Pavlenko et al., PRB, 85,020407(2012)
Micheali et al., PRL, 108,117003(2012)
Lee et al. Nature Materials 12, 703 (2013)
Observations
L-edge spectra of Ti atom
Experimental and theoretically
calculated spectra match for Ti3+
Bulk SrTiO3 : Ti4+ valence state
Ti4+ = d0 configuration
Are some extra electrons coming towards interface?
High electron beam energy(200 keV)
Spot size of 1-3 Å
• Free carrier at n type interface with density 3.5 1014 cm-2
• Confined within a few nm of the interface (quasi 2 DEG)
EELS
Muller et al. Nature, 5,206(2006)
• Oxygen vacancies at interface
• Cation intermixing (LaxSr1‐xTiO3)
• Electronic reconstruction at interface
Possibilities of Formation of 2DEG
??
Electronic Reconstruction
LaAlO3 on TiO2 terminated SrTiO3 (001) (n type)
SrTiO3(001):Alternate layer of SrO and TiO2
LaAlO3(001):Alternate layer of charged LaO+
and AlO2-
Polar Catastrophe
• ½ electron per unit cell• Carrier density:3.5×1014 cm-2
Muller et al ,Nat. Mat.,5,204(2006)
Is Electronics Reconstruction enough for Interface Ferromagnetism?
SrTiO3 can be doped with p type or n type material
Metallic and Superconducting phases are observed
No Sign of ferromagnetism
Electronics Reconstruction is
Necessary but Not Sufficient
Symmetry breaking at interface
eg
dz2
47 meV
dxy
3d
t2g
dxz/yz
dx2
-y2
26 meV
Crystal field
Experimentally confirmed from
XAS data (J. Park et al., PRL,
110, 017401 (2013))
dxy is lowest energy state
Removal of Degeneracy and Orbital Reconstruction
Lee et al. Nat material 12,703(2013)
Double Exchange
Ti3+ (t2g) Ti4+ (t2g )
O2-
dxy
dxy
dxz/yz
Double exchange interaction leads to ferromagnetism
Competition between Double exchange and Spiral
magnetism
Interface magnetism for LAO/STO originates from dxy
orbital of Ti t2g band
dxz/yz
Recent studies on Oxide Interface
Approach towards Applications
LaALO3
LaALO3
Co
Conventional 3-T measurement technique
Spin accumulation at interface
Hanle effect: Change the voltage due to spin dephasing
Spin Injection
N. Reyren et al. PRL 108 , 186802(2012)
Spin Injection
Spin relaxation time=50psSpin diffusion length=1micrometre
A.Ohtomo et al. NATURE 427,423(2004)
Suitable material for D-S channel
FETs
Forg et al , APL ,100 ,053506 (2012)
LAO as gate dielectric (εr=18)
Electrical Contacts : Ar ion milled hole
refilled with sputtered Titanium for
source and drain
Gold contact for Gate
A change of VGS 700 mV causing a
change of 4 order of magnitude of IDS
I-V characteristics
Forg et al , APL ,100 ,053506 (2012)
Temp. Dependence of I-V Characteristics
At +ve VGS decrease with temp
Enhancement of IDS
reduction of Turn On voltage
G > 1 obtained
G = 40, For IGS= 5μA and
VDS = 450 mV
Some Other possible Applications
L Li et al. Science 2011;332:825-828
40%
enhancement
Sensors
Photo detectors
Some Other possible Applications
Multifunctional Oxide Heterostructures, Oxford University Press (2010)
Thermoelectric
Solar cells
Conclusions
Advantages of Oxide Materials are discussed
Interfaces of Oxide Materials show interesting
properties
Ferromagnetism at room temperature is observed
Spin injection and detection is successfully realized
Very high mobility 2DEG is observed
Standard FET device is demonstrated and have
advantages over scaling limits of silicon based
transistor
Could be a very prominent candidate for spin based
devices
Acknowledgement
1. Prof. S.M. Shivaprasad For Topic
2. My Labmates, Satish, Malli, Arpan, Nagaraja, Varun, Shivkumar,
Sandheep, Ankit for useful discussion and preparing slides
3. My friends, Dheeraj, Sunil,Vikas, Sukanya, Shantanu.
I = coupling strength
0.6 eV for early 3d element
1.0 eV for late 3d element
Stoner criterion
Using PLD 4-5 unit cell thickness of
LAO on TiO2 terminated STO
Ferromagnetic Cobalt of Thickness 15
nm deposited at room temp by
sputtering then capped with Gold
Spin injection
Spin polarized current passed from
ferromagnetic material Co through
tunnel contact and one of the Ohmic
contact
LAO film a band insulator play the role
of tunnel barrier
Induced imbalance of spin population at
the channel side (Spin accumulation)
creates additional voltage at contacts
Electrical Henley effect Causes
decrease of voltage
Growth of LAO on TiO2 terminated
STO (approx. 9 unit cell) using PLD –
780 C , P (O2) = 9 10-5 mbar
Gate Contacts of 40 nm YBCO
deposited at 760 C at 0.11 mbar of O2
Annealed for 1hr at 600 C, 30 min at
460 C & 30 min at 430 C at 400 mbar
of O2
Two approaches
1) SrTiO3 as gate, Turn On voltage 60 V
2) Using Tip of SPM to write line on
LAO/STO interface , Turn On Voltage
less than 1 volt
FETs