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1
1
)(21
)(2
)(
)(
B
B
BM
BM
eq
-1
-0.5
0
0.5
1
-0.6 -0.4 -0.2 0 0.2 0.4 0.6
0 s0.1 ms0.5 ms1 ms2 ms3 ms
M/M
s
µ0H (T)
0.04 K11 GHz
0.001 T/s
period: 10 ms
Absorption of microwaves
Max ~ 5 s-1
W. Wernsdorfer et al , EPL (2003)
Gaussian absorption lines
Important broadening by nuclear spins Loss of coherence
R ~ b ~ 30 kHz2~ ~ 0.2 GHz
Rabi oscillations, require larger b.
N = BMax/2 = B2/ ~20
Precession ~ 20 turns
tbBbB
bP 2
1222
22
2
)(2
1sin
)()(
)(
)()(4
2LL Bfb
Photon assisted tunneling in a SMM (Fe8) Absorption of circular polarized microwaves
-10 -5 0 5 10
En
erg
y
quantum number m
²M = +1
tunneling
²M = -1
H = 0
-1 -0.5 0 0.5 1-40
-30
-20
-10
0
En
erg
y (
K)
µ0Hz (T)
²M = ±1
-10
-9
-8
-7
10
9
8
7
Absorption of circular polarized microwaves(115 GHz)
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.091
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.119
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.131
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.151
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.167
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.190
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.207
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.237
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.256
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.292
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.320
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.366
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.458
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.568
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.693
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
00.841
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
-1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
01
M/M
s
µ0H (T)
0.007 T/s
P/P 0 =
Sorace et al, PRB 2003
Photon induced tunnel probabilityPassisted = P - n±10P±10
10-7
10-6
10-5
10-4
10-3
10-2
10-1
0.001 0.01 0.1
P_EPRB
B
PEP
R
(au)
n = 1n = 0
Ts
0.8
n=0
n=1
Ts= T0 + ћmws /Cs
Sorace et al, PRB (2003)
Environmental effects
Central molecule spinMn12, Fe8
Spin-bathEnvironmental spins
Enhance tunnelingMesoscopic spins
Decoherence
Phonon-bath
Spin-phonons transitionBottleneck (TB>>T1)
Electromagnetic radiation bath
Spin-photons transitions(incoherent)
Free carriersStrong decoherenceRKKY interactions
Kondo, Heavy fermions
Central ionic spin Rare-earths
Strong hyperfine interactions
Coherent dynamicsTowards new spin-qubits
V15
Rare-earths ions
A new direction
Tunneling of the angular momentum J ofHo3+ ions in Y0.998Ho0.002LiF4
Example of a metallic matrix: Ho3+ ions in Y0.999Ho0.001Ru2Si2
Mesocopic nanomagnetism
Resonant microwave absorption : towards spin qubits
A new direction:
Tunneling of the angular momentum of rare-earths ions
A quasi- infinite number of systems for the study of mesoscopic quantum dynamics:
- different CF and 4f symmetries - different concentrations - insulating, metallic, semi-conducting …
Ho3+ in Y0.998Ho0.002LiF4
Tetragonal symmetry (Ho in S4); (J = L+S = 8; gJ=5/4)
Dipolar interactions ~ mT << levels separation
-6 -4 -2 0 2 4 6-200
-150
-100
-50
0
50
100
150
-9 -6 -3 0 3 6 9-240
-200
-160
-120
-80
-40b)a) E (K)
<Jz>
E (K)
0H
z (T)
R. Giraud, W. Wernsdorfer, D. Mailly, A. Tkachuk, and B. Barbara, PRL, 87, 057203-1 (2001)
B20 = 0.606 K, B40 = -3.253 mK, B44 =- 42.92 mK, B60 =-8.41mK, B64 =- 817.3mK Sh. Gifeisman et al, Opt. Spect. (USSR) 44, 68 (1978);
N.I. Agladze et al, PRL, 66, 477 (1991)
Barrier short-cuts
Energy barrier ( ~ 10 K)
Strong mixing
Singlet excited state
Doublet ground-state
Large 1 (Orbach
process)
CF levels and energy barrier of Ho3+ in Y0.998Ho0.002LiF4
46
46
44
44
06
06
04
04
02
02 OBOBOBOBOBHCF
Hysteresis loop of Ho3+ ions in YLiF4
-1
-0,5
0
0,5
1
-3 -2 -1 0 1 2 3
1.5K
1.6K
1.9K
2.4K
M/M
S
BL (T)
Comparison with Mn12-ac
dH/dt=0.55 mT/s
-80 -40 0 40 80 120
-1,0
-0,5
0,0
0,5
1,0
200 mK 150 mK 50 mK
M/M
S
0H
z (mT)
-20 0 20 40 60 800
100
200
300
n=0n=3
n=1
n=-1
n=2
dH/dt > 0
1/ 0
dm
/dH
z (1/
T)
Many steps !
L.Thomas, F. Lionti, R. Ballou, R. Sessoli, R. Giraud, W. Wernsdorfer, D. Mailly, A.Tkachuk,
D. Gatteschi,and B. Barbara, Nature, 1996. and B. Barbara, PRL, 2001
Steps at Bn = 450.n (mT) Steps at Bn = 23.n (mT)
Tunneling of Mn12-ac Molecules Tunneling of Ho3+ ion
… Nuclear spins…
Ising CF Ground-state + Hyperfine Interactions
H = HCF-Z + A{JzIz + (J+ I- + J- I+ )/2}
-80 -40 0 40 80 120
-1,0
-0,5
0,0
0,5
1,0
200 mK 150 mK 50 mK
M/M
S
0H
z (mT)
-20 0 20 40 60 800
100
200
300
n=0n=3
n=1
n=-1
n=2
dH/dt > 0
1/ 0
dm/d
Hz (
1/T)
-200 -150 -100 -50 0 50 100 150 200
-180,0
-179,5
-179,0
-178,5
I = 7/2
E (
K)
0H
z (mT)
-7/2
7/2
7/2
5/2
3/2
-7/2
Co-Tunneling of electronic and nuclear momenta: Electro-nuclear entanglement
The ground-state doublet 2(2 x 7/2 + 1) = 16 states
-5/2
5/2
gJBHn = n.A/2 A = 38.6 mK
Avoided Level Crossings between |, Iz and |+, Iz’ if I= (Iz -Iz
’ )/2= odd
-75 -50 -25 0 25 50 75-1.0
-0.5
0.0
0.5
1.0
T = 30 mKv = 0.6 mT/s
HT=190 mT
HT=170 mT
HT=150 mT
HT=130 mT
HT=110 mT
HT=90 mT
HT=70 mT
HT=50 mT
HT=30 mT
HT=10 mT
M/M
S
0H
z (mT)
dB/dt ~ 1 mT/s
Acceleration of quantum dynamicsin a transverse field
…. slow sweeping field: meas >> bott > 1
Near thermodynamical equilibrium at the cryostat temperature…
-1
-0.5
0
0.5
1
-0.08 -0.04 0 0.04 0.08
0.136 mT/s0.068 mT/s0.034 mT/s0.017 mT/s
M/M
s
µ0H (T)
0.04 K
n=1
n=2
Case of a metallic matrix: Ho3+ ions in Y0.999Ho0.001Ru2Si2
n=0
These steps come from tunneling transitions of J+I of single Ho3+ ions,In a sea of free electrons.
Y0.998Ho0.002LiF4
Ho0.001Y0.999Ru2Si2
-1
-0.5
0
0.5
1
-0.08 -0.04 0 0.04 0.08
0.136 mT/s0.068 mT/s0.034 mT/s0.017 mT/s
M/M
s
µ0H (T)
0.04 K
-80 -60 -40 -20 0 20 40 60 80-1,0
-0,5
0,0
0,5
1,0
-80 -60 -40 -20 0 20 40 60 80
-180,0
-179,5
v = 0.11 mT/s
b)
M/M
S
0H
z (mT)
a)
E (
K)
0H
z (mT)
The resonances fields of Ho3+
ions, in YLiF4 and
YCu2Si2 are the same
Y1-HoRu2Si2 ~ 0.1%
Same resonance
fields
Many body tunneling events
mediated by RKKY interactions ?
Multiparticle Kondo ?Screening ?
(See Stamp and Prokofiev, 1997)
Effect of a transverse field: Step 2 merges with the continuous one
-80 -60 -40 -20 0 20-1.0
-0.5
0.0
0.5
1.0v = 0.14 mT/s
n = 2
n = 1
HT = 0
HT = 10 mT
T = 40 mK
M/M
S
0H
z (mT)
Ising CF Ground-state + Hyperfine Interactions
H = HCF-Z + A{JzIz + (J+ I- + J- I+ )/2}
-80 -40 0 40 80 120
-1,0
-0,5
0,0
0,5
1,0
200 mK 150 mK 50 mK
M/M
S
0H
z (mT)
-20 0 20 40 60 800
100
200
300
n=0n=3
n=1
n=-1
n=2
dH/dt > 0
1/ 0
dm/d
Hz (
1/T)
-200 -150 -100 -50 0 50 100 150 200
-180,0
-179,5
-179,0
-178,5
I = 7/2
E (
K)
0H
z (mT)
-7/2
7/2
7/2
5/2
3/2
-7/2
Co-Tunneling of electronic and nuclear momenta: Electro-nuclear entanglement
The ground-state doublet 2(2 x 7/2 + 1) = 16 states
-5/2
5/2
gJBHn = n.A/2 A = 38.6 mK
Avoided Level Crossings between |, Iz and |+, Iz’ if I= (Iz -Iz
’ )/2= odd
-200 -150 -100 -50 0 50 100 150 200
-180,0
-179,5
-179,0
-178,5
I = 7/2
E (
K)
0H
z (mT)
50 mK0.3 T/s
120 160 200 240
0
4
8
-150 -75 0 75 150 225
0
20
40
60
-300 -200 -100 0 100 200 300-1,0
-0,5
0,0
0,5
1,0
-8 -6 -4 -2 0 2 4 6 8 10-180
-120
-60
0
60
120
180
240
n = 6
n = 7n = 8
n = 9
b)
dH/dt<0
n=1
n=0
1/ 0
dm
/dH
z (1/
T)
0H
z (mT)
a)
M/M
S
0H
z (mT)
integer n half integer n
linear fit
0H
n = n x 23 mT
0H
n (
mT
)
n
Giraud et al, PRL 87, 057203 1 (2001)
Additional steps at fields: Hn = (23/2).n (mT)single Ho3+ tunneling being at avoided level crossings at Hn = 23.n (mT)
50 mK 200 mK0.3 T/s
Simultaneous tunneling of Ho3+ pairs (4-bodies entanglement)Two Ho3+ Hamiltonian avoided level crossings at Hn = (23/2).n
Fast measurements: meas ~ bott > 1 >> s
Single-ion level structure En = nE geffBHn/2
Tunneling: gJBHnn’ = (n’-n)A/2
Co-tunneling: gJBHnn’=(n’-n+1/2)A/2
Two-ions Level structureCo-tunnelingBiais tunnelingDiffusive tunneling
-2000 -1000 0 1000 2000
-180.0
-179.5
-179.0
-178.5
-2000 -1000 0 1000 2000
-360
-359
-358
-357
0 100 200 300 400 500
-360.0
-359.6
n=-9b)
a)
n=-8 n=3/2
. . .
. . .
mI=+5/2
mI=+7/2
mI=+5/2
mI=+7/2
I = 7/2E
ner
gy
(K)
Hz (Oe)
87654
32
1
0
En
erg
y (K
)
Hz (Oe)
n = 0
Hbias
n = 2n = 3/2n = 1/2
n = 1
En
erg
y (K
)
Hz (Oe)
Toy model of two coupled effective spins, with gz /gx >> 1
H/J = ijSi
zSjz +
ij(Si
+Sj- + Sj
+Si-)/2 + ij (Si
+Sj+ + Sj
-Si-)
with
= (Jx + Jy)/4J = (Jx - Jy)/4J
This is why dipolar interactions induce co-tunneling
Co-tunnelingDiffusive tunneling
Single-ion level structure En = nE geffBHn/2
Tunneling: gJBHnn’ = (n’-n)A/2
Co-tunneling: gJBHnn’=(n’-n+1/2)A/2
Two-ions Level structureCo-tunnelingBiais tunnelingDiffusive tunneling
-2000 -1000 0 1000 2000
-180.0
-179.5
-179.0
-178.5
-2000 -1000 0 1000 2000
-360
-359
-358
-357
0 100 200 300 400 500
-360.0
-359.6
n=-9b)
a)
n=-8 n=3/2
. . .
. . .
mI=+5/2
mI=+7/2
mI=+5/2
mI=+7/2
I = 7/2E
ner
gy
(K)
Hz (Oe)
87654
32
1
0
En
erg
y (K
)
Hz (Oe)
n = 0
Hbias
n = 2n = 3/2n = 1/2
n = 1
En
erg
y (K
)
Hz (Oe)
Higher temperatures: cross-spin relaxation through excited singlets
R. Giraud et al PRL, 2003 and JMMM (also ICM’2003, Rome).
S. Bertaina, B. Barbara, R. Giraud, B. Malkin, M. Vanyunin, A. Takchuk, PRB submitted.
-Single-ion tunneling (LT: spins-bath and phonons-bath )
- Co-tunneling (LT: spins-bath, HT: phonons-bath )
Extension to N >2 multi-tunneling
gJBHn(N) = nA/2N n-D
Multi-molecule resonant tunneling at gBHn(N) = nD/2N n-D
Case of strong coupling (J>>D): S =S1+S2+…+ SN gBHn(N)=nD …Wrong!
Reason: D decreases when S increases.
Multi-tunneling should fill the space between single spins tunneling
Spin-glass regimeProfile of (Hz/A)
-200 0 200 400 600 8000
2
4
6
8
10 ' T=1.75 K
LiYF4:Ho (0.11%), 1200 Hz
-200 0 200 400 600 800
0
2
4
T=1.75 K
''
-200 0 200 400 600 8000
2
4
6
8
10
T=2.5 K
-200 0 200 400 600 800
0
2
4
T=2.5 K
-200 0 200 400 600 8000
2
4
6
8
10
T=3 K
-200 0 200 400 600 800
0
2
4
T=3 K
-200 0 200 400 600 8000
2
4
6
8
10
T=3.5 K
Magnetic field (Oe)
-200 0 200 400 600 800
0
2
4
T=3.5 K
Magnetic field (Oe)
Numerical fits (Malkin, Vanyunin et al, PRB submitted)
Why D decreases when S increases:
Take N spins with anisotropy energies: En= DnSn2
Assume they are coupled with J >> Dn to form a SMM:
The total energy ET =∑DnSn2 = DT ST
2 DT = ∑DnSn2 / (∑Sn)2 << Dn
Dn=D and Sn=S DT = D/N gBHn(N)=n(D/N) n-D, as for Weak C.
…
1 10 100 1000
Quantum worldClassical world
Mn4
Mn12 Mn84Mn30
Technological applications : Magnetic recording on nm scale Quantum information, Molecular electronic and spintronics,Biomedical applications…
…..
Incredible impact on molecular and supra-molecular chemistry.
Larger and larger molecules DS2
AFTER Mn12-ac…
Co cluster
Assume:
DT
N0
2,8 3,2 3,6 4,0 4,4 4,8 5,2 5,6 6,0 6,4 6,8 7,2 7,640
60
80
100
120
140
160
180
200
220
240
Magnetic field (kOe)
J
frequency 100 GHz
0,00 0,05 0,10 0,15 0,20 0,25 0,30-250
-225
-200
-175
-0,5
0,0
0,5
1,0
1,5
2,0
2,5
3,0
3,5
m=0
Ener
gy (G
Hz)
Magnetic field B (T)
m=2
Hyperfine sublevels of Ho3+ ion in LiYF4
Direct check of hyperfine sublevels from EPR In Ho:YLiF4 (Malkin group)
G. Shakurov et al, Appl. Magn. Res. 2005
250 GHz
0,00 0,05 0,10 0,15 0,20 0,25 0,30-250
-225
-200
-175
-0,5
0,0
0,5
1,0
1,5
2,0
2,5
3,0
3,5
m=0
Ener
gy (G
Hz)
Magnetic field B (T)
m=2
Hyperfine sublevels of Ho3+ ion in LiYF4
…but too small transition amplitude …
0 200 400 600 800 1000 1200 1400 1600
-4000
-2000
0
2000
4000
dI/d
H (
u.a
.)
Champ magnétique (Oe)
LiYF4 - Ho:0.001%
0 200 400 600 800 1000 1200 1400 1600-3000
-2000
-1000
0
1000
2000
dI/d
H (
u.a
.)
Champ magnétique (Oe)
CaWO4 - Ho:0.05%
RPE continue de Ho3+ (9.5 GHz)
CaWO4 :
Same Structure as YLiF4Almost no nuclear spins
0,00 0,05 0,10 0,15
210.80
210.55
210.35
210.90
Magnetic field B (T)
210.25
(GHz)
An example of the direct observation of the anticrossing of hyperfine sublevels (m=2)
in the EPR spectra (G. Shakurov, B. Malkin, B.Barbara. Appl. Magn. Res. 2005 )
7
8
20 22 24 26205,2
205,5
205,8
206,1
206,4
206,7
209,7
210,0
210,3
210,6
210,9
Iz=-3/2, 1/2
w
w
w
Tra
nsi
tion
fre
qu
en
cy (
GH
z)
s
s
s
s
w
Iz=-1/2
68 70 72
Iz=-5/2, -1/2
Iz=-3/2
w
w
w
w
Magnetic field (mT)
s
s
s
s
116 118 120
Iz=-7/2, -3/2
Iz=-5/2
m=0
w
w
w
ws
s
s
s
m=2
The anticrossings detected in the EPR spectra in LiYF4 (0.1% Ho)
0,00 0,05 0,10 0,15 0,20 0,25 0,30-250
-225
-200
-175
-0,5
0,0
0,5
1,0
1,5
2,0
2,5
3,0
3,5
m=0
Ener
gy (G
Hz)
Magnetic field B (T)
m=2
Hyperfine sublevels of Ho3+ ion in LiYF4
…but too smal transition amplitude …
0 200 400 600 800 1000 1200 1400 1600
-4000
-2000
0
2000
4000
dI/d
H (
u.a
.)
Champ magnétique (Oe)
LiYF4 - Ho:0.001%
0 200 400 600 800 1000 1200 1400 1600-3000
-2000
-1000
0
1000
2000
dI/d
H (
u.a
.)
Champ magnétique (Oe)
CaWO4 - Ho:0.05%
Continuous EPR on Ho3+ (9.5 GHz)
CaWO4 :
Structure isomorphe à LiYF4Amost no nuclear spins
CONCLUSION
NanoparticlesThe Micro-SQUID technique : unique tool for single particles measurements
(from micron to nanometer scales)
Classical spins dynamics
Molecular magnetsQuantum Tunneling and quantum dynamics of large spins
Effects of environmental degrees of freedom (spin-bath)
Very short coherent time in molecular magnets (in « normal » conditions)
Rare-Earth in insulating and metalic matrixesEvidence for tunneling of the total angular momentum J
Crucial role of hyperfine interactions
Multi-tunneling effects
Coherent quantum dynamics and new type of spin-qubits