spin order in correlated electron systems yukawa institute for theoretical physics zhi li

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Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

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Page 1: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

Spin order in correlated electron systems

Yukawa Institute for Theoretical Physics

Zhi Li

Page 2: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

Outline1. Variety of spin order in condensed matter

1.1 Collinear spin order

1.2 Non-collinear spin order

2. Theory and calculation

2.1 The form of wave function

2.2 Introduction about DFT calculation

2.3 Helical spin order in BaFeO3

3. Summary

Page 3: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

1. Variety of spin order

1.1 Collinear spin order

Ferromagnetism

Such as, Fe

Anti-ferromagnetism

Such as, NiO

Ferrimagnetism

Such as, Fe3O4,

yttrium iron garnet

Spin density wave state in Cr

Page 4: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

1. Variety of spin order

1.2 Non-collinear spin order

Example: Spiral spin (fcc Fe)

The position dependent spin moment could be written as

Vector q is the wave vector of the spiral spin order

)()(

)sin()(

)cos()(

rmrM

rqrM

rqrM

z

y

x

Page 5: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

2.1 The form of wave function If the electronic system is spin ordered, the form of the wave

function has a constraint.

A concrete example: Spiral spin

n, l : lattice and orbital index

Basis function could be plane wave, or Wannier function, or atomic orbital wave function.

nlnlaR

2

1

2

2

0

0)()()(

rqi

rqi

e

errUrc

nla

Page 6: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

2.1 The form of wave function

• Check the spin moment in this from of wave function:

1221

22

12

22

12

01

10,)()(

riqriq

rqi

rqirq

irq

i

xx ee

e

eeecrcrM

)cos(sincos rqrqmrqm yx

xm

cos22yx mm 1221 xm 1221 iimy

)sin(0

0,)()(

22

12

22

12

rq

e

ei

ieecrcrM rq

i

rqirq

irq

i

yy

zrqi

rqirq

irq

i

zz m

e

eeecrcrM

2211

22

12

22

12

10

01,)()(

Page 7: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

2.1 The form of wave function

• Many-body Hamiltonian:• Total energy

note:

1. The wave vector q is coupled to the momentum

2. Generally speaking, the interacting term should be in form of matrix

3. It is almost impossible to get the wave vector q by analytical method

)()()'()'()'()'()'()()('

))()(()(2

)()( 22

rrUrrUrrgrUrrUrdrdr

rrUrVm

rUrdrE

)()'()'()'()('

4

4)(2

22

22

2

12

11

2

2

rrrrgrrdrdrVdriq

q

iqq

rdrm

E

ip

ij

jiii rrgrVm

H )()](2

[ 22

Page 8: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

2.2 Introduction about DFT Calculation

• The first-principles calculation based on density functional theory (DFT)

The total energy of system is in the functional of density matrix expressed in single electronic state

Single electron equation

][)()(|'|

)'()('][][

,

XCErrwdrrr

rnrndrdrTE

iir )(

)()(][ XCLSDAXC rdrE

)()( rtrrn

][2

trJU

EE DFTUDFT

Page 9: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

2.3 Helical spin order in BaFeO3

Wave vector dependent total energy

0.0 0.1 0.2 0.3 0.4 0.5

-0.00015

-0.00010

-0.00005

0.00000

0.00005

0.00010

0.00015

0.00020

0.00025

Ene

rgy

(Ry/

Cel

l)

q

U-0 U-0.1Ry U-0.3Ry U-0.3Ry-G U-0.4Ry U-0.5RY-G U-0.5Ry

G: q(1,1,1)

Page 10: Spin order in correlated electron systems Yukawa Institute for Theoretical Physics Zhi Li

Summary

• This is a simple introduction about the spin order in correlated electron system.

1. The form of the wave function

2. DFT calculation