Nanomagnetometry
- W. Wernsdorfer, E. Bonet Orozco and B. Barbara
Lab L. Néel - CNRS, Grenoble, France
- A. Benoit
CRTBT - CNRS , Grenoble, France
- D. Mailly
L2M, Bagneux, Paris, France and a lot of collaborators
Nanomagnetometry W. Wernsdorfer, E. Bonet Orozco and B. Barbara Lab - - PowerPoint PPT Presentation
Nanomagnetometry W. Wernsdorfer, E. Bonet Orozco and B. Barbara Lab L. Nel - CNRS, Grenoble, France A. Benoit CRTBT - CNRS , Grenoble, France D. Mailly L2M, Bagneux, Paris, France and a lot of collaborators Different techniques Torque
Lab L. Néel - CNRS, Grenoble, France
CRTBT - CNRS , Grenoble, France
L2M, Bagneux, Paris, France and a lot of collaborators
H I V
Principle: Deviation of electrons induced by a magnetic field (Lorentz force) Semi-conductor heterostructure : GaAs - GaAlAs (à 4K) electron density : n = 3 1011 cm-2 mobility : 800 000 cm2V-1s-1 Hall resistant : 2000
resistance : 20
✁at 4K and 2000
✁at 300K
A.D. Kent, D.D. Awschalom et al., JAP, 76, 6656 (1994) sensitivity of 106 µB A.K. Geim et al. APL, 71 (16), (1997) Luise Theil Hansen, <theil@meyer.fys.ku.dk> sensitivity of 104 µB
depinning of a domain wall in an isolated Ni wires
Single domain switching of small ErAs clusters investigated using telegraph noise spectroscopy
Co/Cu/Co structures
L.F. Schelp, A. Fert et al., PRB, 56. R5747 (1997) Co/Al2O3/Co tunnel junctions with cobalt clusters in the Al2O3 layer
Different types of Josephson junctions :
Theoretical limit : 1 µ B !!!
with a coupling factor of 4*107 µB/Φo
0 3 nm
S = 10
20 10 10 10 8 10 6 10 5 10 4 10 3 10 2 10 1
clusters individual spins molecular clusters nanoparticles wires submicron particles
10 -4 Φ Φ Φ Φo
(D. Mailly, LPM, Paris)
stray field
10-18 – 10-17 emu
1 - 2 µm
Nb
< 7K
10-4 Φo
104 µB i.e. (6nm)3 of Co
10-16 emu conventional SQUID : 10-7 emu
2 4 conne ct e d SQUIDs
1 0 A/ 1 0 V
1 0 A/ 1 0 V
1 0 A/ 1 0 V
Macint os h
Curre nt s ource s Ele ct roniq ue SQUID Scann e r 2 PCI cart e s
1 ...2 4 1 µ A - 3 mA
t I
0 .0 3 - 6 K
? 300 ns
Ic I t
5 10 15
50 100 150 U(mV) I(µA)
A E F C B D
Ic min Ic
40 50 60 70 80 90 100 110 120 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 I c(µA) µ µ µ µο ο ο ο Η(µΤ) Η(µΤ) Η(µΤ) Η(µΤ)
Φ Φ Φ Φ ο
ο ο ο
100 200 300 400 500 600 700 count Ic -180µA 0.5 1 1.5 2
Histogram of 60000 Ic measurements
measurements of Ic precision increases with
length of the current ramp
cooling of SQUID
10000 measurements per second :
cluster of Co of 5 nm in diameter
0.1 0.2 0.3
50 100 150 Flux( ) Φ/Φο Φ/Φο Φ/Φο Φ/Φο
ο ο ο ο
µ µ µ µ Η(µΤ) Η(µΤ) Η(µΤ) Η(µΤ)
40 50 60 70 80 90 100 110 120 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Α Α Α Α Β Β Β Β I c (µA)
µ0 H –
H M T t t + 1
0.04 K 0.04 K < T measure < 30 K Hsat
( i) t est
H
² t t
0.1 0.2 0.3
50 100 150 Flux( ) Φ/Φο Φ/Φο Φ/Φο Φ/Φο
ο ο ο ο
µ µ µ µ Η(µΤ) Η(µΤ) Η(µΤ) Η(µΤ)
Co particle: 70 nm x 50 nm x 25nm
0.5 1 0¡ 30¡ 60¡ 90¡ 120¡
hsw
S < 1 S = 1.4 S = 2.4
Ni wires: (40-100) nm x (4-5) µm
50 100 150 200 250 0¡ 30¡ 60¡ 90¡ 120¡ 210¡ 240¡ 270¡ 300¡ 330¡ µ µ µ µ
ο ο ο ο
Η Η Η Η
σω σω σω σω
(µΤ) (µΤ) (µΤ) (µΤ)
0.1 0.2 0.3 0.4 0¡ 30¡ 60¡ 90¡ 120¡ 210¡ 240¡ 270¡ 300¡ 330¡ µ µ µ µο
ο ο ο
Η Η Η Η
σω σω σω σω
(Τ) (Τ) (Τ) (Τ) 0
0.1 0.2 0.3 0¡ 30¡ 60¡ 90¡ 120¡ 210¡ 240¡ 270¡ 300¡ 330¡
µ0 H(T)
0.14 0.145 0.15 0.155 0.16 0.165
µ oHy(T) µ oHx(T)
dH/dt
DPM - Villeurbanne: LASER vaporization and inert gas condensation source Low Energy Cluster Beam Deposition regime
HRTEL along a [110] direction fcc - structure, faceting Ideal case: truncated octagedron with 1289 or 2406 atoms for diameters of 3.1 or 3.8 nm blue: 1289-atoms truncated octahedron grey: added atomes, total of 1388 atomes
SQUID is fabricated by electron beam lithography
sensitivity :
i.e.
clusters in Nb - matrix
Acknowledgment: B. Pannetier, F. Balestro, J.-P. Nozières
embedded clusters
Josephson junctions 1 µm embedded clusters
✁3 nm