manipulating molecular spins at the nanometer scale
TRANSCRIPT
Manipulating Molecular Spins at the Nanometer Scale
薛其坤
清华大学物理系
Acknowledgements段文晖 (Tsinghua University, Beijing)裘晓辉 (National Center for Nanoscience & Technology, Beijing)张 平 (Institute of Appl. Phys. & Computa. Math. Beijing)
Members: 陈 曦 马旭村 贾金锋
季帅华 付英双 张 童 吴 蕊
Molecule Based Spintronics
NO
COOH
NO
COOH
electrode electrode
N
S1. Molecule-electrode (metal)
interaction
2. Molecule-molecule interaction
3. Spin-polarized electrons
(injection, transport, manipulation, detection…)
(under external fields)
……
Essential but Challenging!
Content
I. IntroductionII. ExperimentIII. Kondo Effect (MnPc)IV. Zeeman Effect (CoPc)V. Gap States (Mn & Cr)VI. Summary
localized spin + surface
I. Introduction
Anderson Model
I. Introduction
Three parameters: Ed: energy of molecular levelU: Coulomb energy
△~|V|2N: peak width
metal molecule
I. IntroductionAnderson Model Parameters: Ed , U, △
I. Introduction
Kondo Effect Discovered in the 1930sExplained in the 1960s
Interaction between spin and environment
I. Introduction
Kondo
DOS(EF)
I. IntroductionAnderson Model
localized spin + surface
I. Introduction
Kondo
ZeemanQuantum Size Effect (thin film)
Superconducivity
substrate
film
localized spin + surface
I. Introduction
Quantum Size Effect ZeemanKondo
MagnetismSuperconductivity
………
Platform
II. Experiment
Our Molecules
II. Experiment
Our Surface
(111)
Tc=7.2K
Pb (111) thin films on Si
Si
Pb thin films on Si
Superconductivity (Tc): SCIENCE 306, 1915 (2004) Growth kinetics: PRL 92, 106104 (2004)Electron-phonon coupling : PRL 95, 096802 (2005) Upper critical field : PRL 95, 247005 (2005) Surface diffusion: PRL 95, 266102 (2006) Kondo resonance: PRL 99, 156601 (2007) Surface chemical reactivity: PNAS 104, 9204 (2007) ……
Si(111)Pb
Material Properties Modulated by QSE
Superconductivity (Tc) oscillation
PHYSICAL REVIEW LETTERS 15 April 1963
J. M. Blatt and C. J. ThompsonPRL 10, 332 (1963)
22 23 24 25 26 27 28
5.1
5.4
5.7
6.0
6.3
6.6
Tc (K
)
Thickness (ML)22 23 24 25 26 27 28
Thickness (ML)
Guo, Zhang et al., SCIENCE 306, 1915 (2004)Zhang et al., PRL 96, 096802 (2005)
Our tool: STM
Imaging ManipulationSpectroscopy
II. Experiment
Our Instrument
Unisoku UHV ultra-LT (400mK) high magnetic field (11T) STM
II. Experiment
II. ExperimentOur Instrument
Ji et al., PRL (in press)
III. Kondo EffectManipulation
III. Kondo Effect
Kondo Effect
0
122 J
KT D eD
ρ
π
−Δ=
0
1 1( )d d
JUπρ ε ε
Δ= +
+2
0Vπ ρΔ =
Energy spectra for an Anderson impurity system
Without hybridization With hybridization In the Kondo regime below TK.
20
11 12 ( )2
02 d dV
UKT D V e
ρε ερ
−+
+=
J: coupling of spins and conduction electrons
ρ0: density of states of host
Direct observation at single atoms/molecule level by STM
Science 280, 567(1998) M. CrommiePRL80, 2893 (1998)
Wolf-Dieter Schneider
Ce/Ag(111)Co/Au(111)
3d transition metal on Au (111): Ti, V, Cr, Mn, Fe, Co, and Ni.
Nature 403, 512(2000) D. M. Eigler
Co/Cu(111)
MnPc on Pb(111)
CoPc
1.4nm
III. Kondo EffectMnPc
Modulation of Kondo Effect by QSE
III. Kondo Effect
STM Manipulation
III. Kondo Effect
Kondo Resonance
The same molecule
on the same surface under the same measurement conditions!
Fano Lineshape
In tunneling experiments:
Resonance width: 2 2 B KK TΓ =
' 2
'2
( )( )1
dI qVdV
εε+
∝+
0'B K
eV EK T
ε −=
STM tip
Magnetic atom
III. Kondo EffectKondo Temperature Fu et al., PRL 99, 156601 (2007)
III. Kondo Effect
Oxide surface
Pb(111)PbO
III. Kondo Effect
Splitted Kondo
III. Kondo Effect
Kondo Mapping
IV. Zeeman
IV. Zeeman
Pb
CoPc/Pb(111)
IV. Zeeman
T=0.4K
△ ↑
IV. Zeeman
IETS via Single Spin Flipping
on 2nd layer
123
45
Pb
Spin-flip IETS
σe + σie
dI/dV
eV0-gμBB gμBB
σe
Ef
Ef
gμBB
gμBB eV
Mn Atom Chains
Hirjibehedin et al., Science 312, 1021(2006)
IV. Zeeman
Measurement of g-factor of single molecule
1
11
N
N i ii
H J S S−
+=
= ⋅∑Heisenberg model:
Dimer:(3rd layer CoPc)
2 2 21 2 1 2[( ) ]
2JH S S S S= + − −
1E JΔ =
Model Calculations
Trimer:(4th layer)
2 2 21 2 3 1 3 2[( ) ( ) ]
2JH S S S S S S= + + − + − 1 AE JSΔ =
12AS >
1E JΔ =12AS =
Tetramer:(5th layer)
2 21 2 3 1 3
2 2 22 3 4 2 4 2 3
[( ) ( )2
( ) ( ) ( ) ]
JH S S S S S
S S S S S S S
= + + − +
+ + + − + − +
1E JΔ =12AS =only for 2 1.5E JΔ =
Manipulation of single-molecule spin-states
-6 -4 -2 0 2 4 6
0.4
0.6
0.8
1.0
1.2
Sca
led
dI/d
V
Sample bias(mV)
3T 5T 7T 9T 11T
g=2.038
Spin-flip IETS
Bg BμΔ=
Isolated momentZeeman ↔ Kondo
-6 -5 -4 -3 -2 -1 0 1 2 3 4 5 6
0.5
1.0
1.5
2.0
2.5
Sca
led
dI/d
V
Sample bias(mV)
3T 5T 7T 9T 11T
Kondo resonance
1st
Ji et al., PRL (in press)
V. Gap StatesGap States
Pb Mn
U ↑
V. Magnetic
Superconductor Gap States
Cr, Mn on Pb(111)U ↑
Single Atom Spectroscopy
VI. SummaryTopic
Spin states of adsorbatesToolbox
Low temperature (B) STMSingle molecule manipulation
Scanning tunneling spectroscopyInelastic tunneling spectroscopy (IETS) via single spin flip
Gap states in superconductorProgress
Kondo effect modulation via QSEMagnetic coupling between molecules
Manipulating spin states at single molecular levelPerspective
Organic magnetismMolecular spintronicsMolecular recognition
Single atom reaction detection……
Thank you very much!!!
localized spin + surface
I. Introduction
Quantum Size Effect ZeemanKondo
MagnetismSuperconductivity
………
Superconductive film
Platform
magnetic atom/molecule
Atomically flat Pb films on Si(111)
2μmx2μm
Si(111) 0.1º
Thickness: 7nm (24ML)Uniformity: ~centimeter
Pb(bulk): coherent length 87nm
2D electronic system1D Square Potential Well-tunable L
Pb
QSE对电子结构和超导的影响
Superconductivity (Tc) oscillation
PHYSICAL REVIEW LETTERS 15 April 1963
J. M. Blatt and C. J. ThompsonPRL 10, 332 (1963)
22 23 24 25 26 27 28
5.1
5.4
5.7
6.0
6.3
6.6
Tc (K
)
Thickness (ML)22 23 24 25 26 27 28
Thickness (ML)
Guo, Zhang et al., SCIENCE 306, 1915 (2004)Zhang et al., PRL 96, 096802 (2005)
Single domain (111) structure
Si
N N+1N-1
500nm x500nm
10ML 12ML
Oxygen adsorption on PbO2 (~120L @LN2)
10ML, 12ML: more sites11ML: less sites
10ML: θ=0.2453
11ML: θ=0.0831
3 times!
11ML
Oscillating oxidation on Pb(111) surface
121411 13
1512ML
11ML
13ML
QSE on Surface Oxidation of Pb(111)
400nmx400nm
400nmx400nm
SiPb
odd even odd evenodd eveneven
12 1411 1315
PNAS 104, 9204 (2007)Xucun Ma et al.,
PbO
12 14 16
Silicon
e e
In the same metal Pb island,
the behaviors of electrons are different
o2
Surface Reactivity & LDOS at EF (O2/Pb)
• oxygen clusters
■ oxides
Reactivity
LDOS at EF
Xucun Ma et al., PNAS 104, 9202 (2007)
Kondo EffectMagnetic impurity
Metal host
Kondo Temperature TK
Initial state
final stateTK