basic training 2009– lecture 01 competing ferroic orders
TRANSCRIPT
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Cornell University
“I would found an institution where any person can find instruction in any study.” − Ezra Cornell, 1868
Competing Ferroic Orders The magnetoelectric effect
Basic Training in Condensed Matter Theory 2009
Craig J. Fennie School of Applied and Engineering Physics [email protected]
Basic Training 2009– Lecture 01
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Module Outline (Extremely tentative) 1. Overview and Background
• Ferro ordering, the magnetoelectric effect • Complex oxides basics: Types of insulators (i.e., ZSA classifications), Coordination chemistry
2. Structure and Ferroelectricity • Basics of space groups • Soft mode theory, lattice dynamics, group theoretic methods • Competing lattice instabilities • microscopic mechanisms, improper FE • Modern theory of polarization (Berry Phase)
3. Magnetism • Basics, exchange interactions, superexchange, Dzyaloshinskii-Moria • How spins couple to the lattice! Phenomenology and microscopics (spin-phonon, spin-lattice, etc) • Competing magnetic orders
4. Lets start putting things together • Phase competition: magnetic and polar orders and colossal magnetoelectric responses • Magnetic order induced ferroelectricity • Ferroelectric induced ferromagnetism, switching magnetism 180˚ with an electric field aren't these
forbidden by some symmetry? NO!)
5. Finish up loose ends and recent papers I wish I understood better
• Toroidal moments
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Ab initio
What does my title mean? “ferro” derived from the Latin “ferrum”→ Iron
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• Iron is the sixth most abundant element in the Universe
• While it makes up about 5% of the Earth's crust, the Earth's core is believed to consist largely of an iron-nickel alloy constituting 35% of the mass of the Earth as a whole.
• Iron is consequently the most abundant element on Earth, but only the fourth most abundant element in the Earth's crust.
• Most of the iron in the crust is found combined with oxygen as iron oxide minerals such as hematite and magnetite.
http://en.wikipedia.org/wiki/Iron
Yes a play on what I do.
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Ferromagnetism
Magnetization
Energy
F(M) = αM2 + βM4 - MH Spontaneous time-reversal, R, symmetry breaking
M(t)
j(t)
Ordering of spins → spontaneous magnetization
M(-t)
j(-t)
M ≡∑
i
〈Si〉 $= 0
Symmetry properties M(-t) = -M(t)
Time inversion R t → -t
M(t)
j(t)
Space inversion I r → -r M and H are Axial vectors
j(t)
M(t)
M(t)
j(t)
j(t)
M(t)
Mirror reflection m
M(t)
j(t)
M(-t)
j(-t)
Unit cell
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Centrosymmetric lattice
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Ferroelectricity
u ∝ polarization
Energy
F(u) = α u2 + β u4 – Z*⋅u⋅E or
F(P) = αP2 + βP4 - PE
Spontaneous space-inversion, ,I, symmetry breaking
Symmetry properties P(-x) = -P(x)
Time inversion R t → -t Space inversion I r → -r P and E are Polar vectors
P(x,y,z)
P(x,y,-z)
Mirror reflection m
P(x,y,z) P(-x,y,z)
Unit cell
Pα ≈∑
i
Z∗α,β;i〈uβ;i〉 $= 0
Noncentrosymmetric lattice - + -
- + -
+ -
+ -
P(x) P(x)
+ -
P(x)
+ - P(-x)
+ -
+ - +
- + -
x-y
y-z
Spontaneous polarization ⇒ Dipole moment per unit volume
Ordering of polar mode in many cases, this turns out to be a lattice mode
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AntiFerromagnetism
L
Energy
F(M) = αL2 + βL4 - LHq
q≠ 0, Ordering of spins
Symmetry properties L(-t) = -L(t) ; L(-x) = ± L(x)
Unit cell
M ≡∑
i
〈Si〉 = 0
L = S1 − S2
e.g., two sublattice spin system
Depends on details of crystallographic structure!
Cant ignore structure!! i.e., LATTICE + BASIS (don’t just pick your favorite sublattice and ignore the rest!!!)
Does the AFM ordering of spins spontaneously break time-reversal, R, symmetry breaking ? First, what does the question mean? Does the point group of the space group contain R?
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AntiFerromagnetism Does the AFM ordering of spins spontaneously break time-reversal, R, symmetry breaking ? Symmetry properties L(-t) = -L(t) ; L(-x) = ± L(x)
Unit cell L = S1 − S2
e.g., two sublattice spin system (in the ordered phase)
Example 1: two spins sit in the same unit cell in the paramagnetic phase, Yes! R is not a symmetry element. Crystallographic
Unit cell
Magnetic Unit cell
Example 2: two spins sit in different unit cells in the paramagnetic phase, No! the space group contains {R|τ} ⇒ the point group, τ→ 0 contains {R|0}.
n n+{0|τ}
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Ab initio
Def: Linear magnetoelectric effect Landau and Lifshitz, “Electrodynamics of continuous media” Dzyaloshinskii, JETP 1957; Astrov JETP 1960 -> Cr2O3 Hans Schmid, Geneva; Smolenskii USSR
Requirements: 1) broken space-inversion symmetry 2) broken time-reversal symmetry
γ ≡ linear magnetoelectric coefficient
What does my title mean?
Yes a play on what I do.
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Crystal structure of Cr2O3
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From Max Mostovoy
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Cr2O3
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'"
0≠zL
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zzzzz HEHEL ||αλ =
()**+,-.+(/01/23-3*345+,.6/273(+
( )yyxxz HEHEL +'583-.35,(9
zL∝⊥αα ,||
:;</0-=+-/23-3*+,+-/ >? @/!ABC
m3
z
z
m 3),(3,1
3),2(3,1
±
±
⊥
⊥
point group
From Max Mostovoy
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Cr2O3 m′′3
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y
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2
13/2πR
3/2πR
1− 1− 1+
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1− 1− 1+
ITI =′
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345(6%(/1/'("
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!"#1%'1"/&: ( )yyxxzz HEHEHEF +−−= ⊥αα ||me
;<++$/%'$&)(=)2(.6>)801&$:/zz m 3),(3,1,3),2(3,1 // ±± ⊥⊥
From Max Mostovoy
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Linear magnetoelectric effect
!"#$%
+= EP eχ Hα
=M Eα Hmχ+
!"#$"#%&'()*+,-.+/-- 0$12#&' 345#67898:;#%"#<"#=+>?*@;#0$12#&& AB5#6783B:
C"1"#D(E* 2DF#&% GG9#6783H:
From Max Mostovoy
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Next time
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ME revisited, and basic oxide physics • ME effect revisited: Toroidal moments • Complex oxides basics: Types of insulators (i.e., ZSA classifications), Coordination
chemistry