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Sept. 14th 2004 Montauk, Long Island, NY
Jason S. Gardner
NIST, Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg, MD 20899-8562
Department of Physics,Brookhaven National Laboratory,Upton, NY 11973-5000.
Neutron Scattering Studies of
Magnetically Frustrated Pyrochlores
Pyrochlore Lattice
?
Diffuse Scattering
(0,0,l)
(h,h
,0)
Tb2Ti2O7
JS Gardner et al., Phys. Rev. B 64, 224416 (2001).
0
200
400
600
800
1000
1200
1400
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6
Net
Inte
nsi
ty (
coun
ts/2
min
)
Q ( Å -1)
Y2Mo2O7
J S Gardner et al., Phys. Rev. Lett., 83, 211 (1999).
Ho2Ti2O7
ST Bramwell et al. PRL 87, 047205 (2001).
S.-H. Lee et al. Nature 418, 856 (2002)
Outline Spin dynamicsSpin dynamics
3 Compounds3 Compounds
Antiferromagnetic frustrated Antiferromagnetic frustrated systemssystems–YbYb22TiTi22OO77, Gd, Gd22TiTi22OO77
»Strange dynamics and partial ordering
Ferromagnetic frustrated Ferromagnetic frustrated systemssystems–HoHo22TiTi22OO77
»Spin Ice (Uniquely frozen)
Sept. 14th 2004 Montauk, Long Island, NY
Spin Echo Principle
I(Q,t) = S(Q,)cos(t)dCosine transform
New Spectrometer
Typical Magnetic Neutron Spin Echo
0
0.2
0.4
0.6
0.8
1
1.2
1.4
0.01 0.1 1
25.0K22.5K
18.9K10.0K
S(Q
,t)/S
(Q,0
)
Time (ns)
50 %
0.009
0.01
0.011
0.012
0.013
0.014
0.015
5 10 15 20 25 30 35 40
M/H
(em
u/m
ol)
Temperature (K)
22.5 KZFC
FC
Sept. 14th 2004 Montauk, Long Island, NY
Spin Ice
FM Spin Ices – RE2Ti2O7 (Ho and Dy)
K. Matsuhira et al., J. Phys.: Condens. Matter 12 (2000) L649–L656 and 13 (2001) L737-L746
Ho2Ti2O7
FM Spin Ice
Correlation
J Snyder et al. PRB 69 064414 (2004)
Mag
(ar
b. u
nits
)
Ho2Ti2O7
Dy2Ti2O7
Spin Echo Results
New Spectrometer
New territory
New Data
Sept. 14th 2004 Montauk, Long Island, NY
Partial Order
Gd2Ti2O7 -- ½ filled orbital -- Experimental realisation of a Heisenberg spin on a pyrochlore lattice-- found to order????-- very anisotropic??
Gd2Ti2O7 - Partially ordered
A. P. Ramirez, et al.. Rev. Lett. 89, 067202 (2002)
1.1K
0.7K
Powder diffraction
Magnetic Structure
A B
C D
1k 4k
NPD (Champion et al. Rev. B 64, 140407 (2001))
Kagome Planes
INTERSTITIAL SITE
∑ = 0N=1
∞
0.77 K Transition
50 mK StructureA B
C D
1k 4k
RED circlesBLUE balls
0.77 K Transition
What else do we know….A. P. Ramirez, et al.. Rev. Lett. 89, 067202 (2002)
(000)
(½½½)
Neutron Spin Echo (preliminary results)
¾
¼
T > 1K Entire spin system is inelastic and
T < 1K 25% of the spin system is static
REM: NPD revealed 75% of the system is static below the 1st transition; At all T, NSE fits results in a S(Q,t)/S(q,0)
as t 0 of 75%.
Sept. 14th 2004 Montauk, Long Island, NY
More Unusual Magnetism
-Yb-Yb22TiTi22OO77
Yb2Ti2O7
New Data
Conclusions
Exotic Magnetic Order
Large moment systems
Big crystals
NSE ideal time () window
Sept. 14th 2004 Montauk, Long Island, NY
Collaborators
G Ehlers (SNS)
A Cornelius (UNLV)
R Stewart (ILL)
S Bramwell, A Wills and T Fennell(UCL)
Nick Rosov (NIST)