Ryotaro Arita Dept. Applied Phys., Univ. Tokyo Theoretical materials design of ferromagnets...
-
date post
22-Dec-2015 -
Category
Documents
-
view
238 -
download
0
Transcript of Ryotaro Arita Dept. Applied Phys., Univ. Tokyo Theoretical materials design of ferromagnets...
Ryotaro AritaDept. Applied Phys., Univ. Tokyo
Theoretical materials design of ferromagnets comprising non-magnetic elements
R.AritaR.Arita
Collaborators
Dr. Y. SuwaProf. K. KurokiProf. H. Aoki
(Univ. Tokyo) (Adv. Res. Lab. Hitachi)(Univ. Electro-Cummun.)
R.AritaR.Arita
Itinerant ferromagnetism
in purely organic polymers ?
C60-TDAE Alkali-metal loaded zeolite Radical polymers
(Al, Si, O) + KC, H, N Tc~16K Tc~8K
Known materials (localized spin systems)
Tc~O(1) K
Theoretical materials design of ferromagnets comprising non-magnetic elements
Motivation
R.AritaR.Arita
Guideline for materials design of ferromagnets :
Rigorous results (theorem) for the Hubbard model
Materials design by
first-principles calculation
+ model calculation
†
,
.ij i j i ii j i
H t c c h c U n n
Flat-band ferromagnetism by Mielke & Tasaki (‘91,’92)
Strategy
R.AritaR.Arita
(1) Half-filled dispersionless band at the bottom of the band structure
(2) Connectivity condition satisfied (Wannier functions overlap no matter how they are linearly combined.) MaxLoc Wannier (Marzari&Vanderbilt) has overlaps with its neighbors
・・・・・・
Overlapping “Wannier” orbits parallel spins favored due to Pauli’s exclusion rule
†GS 0
iii
Example: 1D triangular lattice・・・・・・
= -1
t=1
(1) (2)
Ferromagnetism guaranteed for U > 0 when
Mielke 91, Tasaki 92Flat-band Ferromagnetism
R.AritaR.Arita
・・・・・・t=1
Robustness of Flat-band Ferromagnetism
ε0=-1
ε0≠-1
Flat-band F
Penc et al (1996)
F survives : not pathological
Finite band dispersion
Ferromagnetic phase
R.AritaR.Arita
・・・・・・t=1
Robustness of Flat-band Ferromagnetism
U
Sakamoto-Kubo (1996), Watanabe-Miyashita (1997)
0 2 4
0
-1
1
FM
n=0.375Flat-band
Carrier doping
ε0≠-1
ε0≠-1
n=0.5
n≠0.5
Metallic ferromagnetism
R.AritaR.Arita
In realistic situations…
Flat band ferromagnetism:Proved for the case where the flat band isat the bottom of theBand structure
Flat band isnot always at the bottom
R.AritaR.Arita
(RA et al, PRB 57 R6854(1998))
Ferro
Ferro guaranteed only for U < Uc
Strong coupling regime: AF favored
Ferromagnetism only for U<Uc
0
' cos
( 1 2sin )
t t
t
Connected square lattice
t’
When flat bands is in the middle of the band structure :
R.AritaR.Arita
In realistic situations…
Flat band F:Proved for the case where the flat band isat the bottom of theBand structure
Flat band isnot always the bottom
Stability of the flat-band ferromagnetismdepends on the position of the flat band
R.AritaR.Arita
Asymmetric DOS favors F
F fragileF robust
Not only D(f) but also the position of the peak is in D important cf) Stoner criterion: UD(f) > 1
DMFT study by Wahle,Bluemer,Schlipf,Held, & Vollhardt (1998)
F not favored
F favored
R.AritaR.Arita
Materials design of flat-band ferromagnetism in real materials
(1)Construct a tight-binding model having flat bands
(2) Search for materials which correspond to the tight-binding model (first-principles calculation)
(3) Ferromagnetic ground state ? (LSDA) Estimate Uc and check that Uc is not too small (model calculation)
R.AritaR.Arita
Five membered rings: connectivity condition satisfied for realistic parameters of t and
Chain of five-membered ringsEnergy
Design of flat-band ferromagnetism in organic polymers
0 = +1
t
Many known polymers: polypyrrole, polyazole, polythiophene, etc
Flat band
N
n
S
n
N
nN N
H
.. ..
H
Versatile possibilities of putting on various functional bases
R.AritaR.Arita
GGA calculation (TAPP, Tokyo Ab-initio Program Package)Plane wave basis + ultra-soft pseudo-potential
0 = +1
t
=N
n
N
nN N
.. ..X X
or
X=Na, K, Cl, F, OH, CH3
(low electron affinity)
No flat band
?
dispersive
Polymers of five-membered rings
Difficult to make 0~+1
R.AritaR.Arita
=N
n
N
nN N
.. ..or
X X
X=CN, COOH, NH2 (bases with electrons)
Flat band for polyaminotriazole
N
nN N
..
NH2
Polymers of decorated five-membered rings
RA et al.,PRL., 88,127202 (2002)
Difficult to make 0~+1
Flat band for 0 < 0 ?
R.AritaR.Arita
tight-binding model
Electronic Structure of Polyaminotriazole
GGA calculation
( connectivity condition satisfied )
R.AritaR.Arita
Connectivity condition satisfied ?: How to see it
Maximally localized Wannier fn.< size of unit cell
Periodic part of Bloch fn. (uk )
= Same for all k
R.AritaR.Arita
Connectivity condition satisfied ?: How to see it
Maximally localized Wannier fn.> size of unit cell
Periodic part of Bloch fn. (uk )
depends on k
R.AritaR.Arita
Comparison of the Bloch wave functions
connectivity condition satisfied for GGA
GGA
Tight-bindingmodel
Connectivity condition satisfied for the tight-binding model
X
R.AritaR.Arita
comparison of the total energies
The ferromagnetic state is most stablePeierls instability is weak
LSDA for doped PAT
PAT = promising candidate for flat-band F with an appropriate carrier doping
cf) polyethylene
R.AritaR.Arita
Magnetic phase diagram for the Hubbard model
Ferromagnetism stable unless U is not too strong
R.AritaR.Arita
4-Amino 1,2,4,Triazole
color
statemelting point
white
crystals
86.3 - 87.3 C°
http://www.purechagroup.com/commercially available:
Polymerization?
NN
NH2N
R.AritaR.Arita
Polymethylaminotriazole
Related materials
Oligomer of Methylaminopyrrole
Ferro ~ AF < P
Flat band
Ground state = High spin state (S=1)
Suwa, RA, Kuroki, Aoki, PRB68 174419 (2003)
Suwa, RA, Kuroki, Aoki,in prep. (2009)
R.AritaR.Arita
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
1) n-BuLi THF, reflux
2) NiCl2, r.t.
yield: 60% yield: 15%
1) n-BuLi / t-BuOK THF, -78 oC
2) NiCl2(dppp), r.t.
N
NMe2
N
NMe2
N
NMe2
N
NMe2yield: 23%
N
NMe2
N
NMe2
N
NMe2
N
NMe2
1) n-BuLi THF, reflux
2) NiCl2, r.t.
N
NMe2
N
NMe2
N
NMe2 n
N
NMe2
N
NMe2
N
NMe2 n
m
m SbCl6-
Experiments (actual synthesis)
Nishihara group, Univ. Tokyo4 holes/ 8 rings
dimethylaminopyrrole
R.AritaR.Arita
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
1) n-BuLi THF, reflux
2) NiCl2, r.t.
yield: 60% yield: 15%
1) n-BuLi / t-BuOK THF, -78 oC
2) NiCl2(dppp), r.t.
N
NMe2
N
NMe2
N
NMe2
N
NMe2yield: 23%
N
NMe2
N
NMe2
N
NMe2
N
NMe2
1) n-BuLi THF, reflux
2) NiCl2, r.t.
N
NMe2
N
NMe2
N
NMe2 n
N
NMe2
N
NMe2
N
NMe2 n
m
m SbCl6-
Experiments (actual synthesis)
Nishihara group, Univ. Tokyo4 holes/ 8 rings
dimethylaminopyrrole
ESR
R.AritaR.Arita
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
N
NMe2
1) n-BuLi THF, reflux
2) NiCl2, r.t.
yield: 60% yield: 15%
1) n-BuLi / t-BuOK THF, -78 oC
2) NiCl2(dppp), r.t.
N
NMe2
N
NMe2
N
NMe2
N
NMe2yield: 23%
N
NMe2
N
NMe2
N
NMe2
N
NMe2
1) n-BuLi THF, reflux
2) NiCl2, r.t.
N
NMe2
N
NMe2
N
NMe2 n
N
NMe2
N
NMe2
N
NMe2 n
m
m SbCl6-
Experiments (actual synthesis)
Nishihara group, Univ. Tokyo4 holes/ 8 rings
dimethylaminopyrrole
R.AritaR.Arita
Polyaminotriazole:
promising candidate for
flat-band ferromagnetism
Related materials:
Oligomer of dimethylaminopyrrole:
High-spin state ?
Conclusions