hand calculations of magnetic modes

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Hand calculations of magnetic modes A. Daoud-Aladine (ISIS)

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Hand calculations of magnetic modes. A. Daoud-Aladine (ISIS). Physical problem. Ideal cubic Perovskite. Site A. LaMnO 3 T N =150K k=(0 0 0). La/Tb. TbMnO 3 T N =41K k=(0.28 0 0). O. Mn. P nma. m. [010] O [001] C. [101] O [010] C. n. m. n. a. a. Physical problem. - PowerPoint PPT Presentation

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Page 1: Hand calculations of magnetic modes

Hand calculations of magnetic modes

A. Daoud-Aladine (ISIS)

Page 2: Hand calculations of magnetic modes

Physical problem

Site A

Ideal cubic Perovskite

Pnma

[010]O

[001]C

[101]O

[010]C

La/Tb

n

n

aa

m

m

Mn O

LaMnO3 TN=150K k=(0 0 0)

TbMnO3 TN=41K k=(0.28 0 0)

Page 3: Hand calculations of magnetic modes

(b)

(a)

Pnma

[101]O

[010]C m

m

LaMnO3 TN=150K k=(0 0 0)

TbMnO3 TN=41K k=(0.28 0 0)

Physical problem

Page 4: Hand calculations of magnetic modes

(b)

(a)

a

b

c

1z

2y

3x

Linear algebra problem

Sk1

Sk2

Sk3

Sk4

Pnma

Page 5: Hand calculations of magnetic modes

a

b

c

1z

2y

3x

Linear algebra problem

Sk1

Sk2

Sk3

Sk4

Hermitian vector space

(complex)of dimension 12

Pnma

Page 6: Hand calculations of magnetic modes

The group G=Pnma

Zero blocks elements

Page 7: Hand calculations of magnetic modes

The group of k: Gk

G = Pnmaa (x)

b (y)

c (z)

k

mxy mxz

(a) Gk = Pnma

(b) Gk=

P21ma

2x

Page 8: Hand calculations of magnetic modes

Irreps of Gk

(a)

(b)

Page 9: Hand calculations of magnetic modes

Representation of gGk

c

b

a

Sk1

Sk2

Sk3

Sk4

(a and b) Trivial Ex1: Identity operation 1

Page 10: Hand calculations of magnetic modes

Representation of gGk

(a and b) Trivial Ex1: Identity operation 1

Page 11: Hand calculations of magnetic modes

Representation of gGk

(a only) Trivial Ex2: Inversion -1

c

b

a

Sk1

Sk2

Sk3

Sk4

Page 12: Hand calculations of magnetic modes

Representation of gGk

(a only) Trivial Ex2: Inversion -1

Page 13: Hand calculations of magnetic modes

Representation of gGk

c

b

a

Sk1

Sk2

Sk3

Sk4

Point

Sk . SkSpin

Mn1: 0,0,1/2 1/2, 1/2, 0 = Mn3

(a and b) Ex1: 21 axis along x

Page 14: Hand calculations of magnetic modes

Representation of gGk

1z

2y

3x 3x

ap(21,3)

1

1z

1y1x

1’c

b

a Sk1’

Sk1

(a and b) Ex1: 21 axis along x

Page 15: Hand calculations of magnetic modes

Representation of gGk(a and b) Ex1: 21 axis along x

Page 16: Hand calculations of magnetic modes

Representation of gGk(a only) Ex2: Glide plane n axis x

1z

2y

3x

Page 17: Hand calculations of magnetic modes

Representation of gGk(a only) Ex2: Glide plane n axis x

1z

2y

3x

Page 18: Hand calculations of magnetic modes

Representation of gGk(a only) Ex2: Glide plane n axis x

Page 19: Hand calculations of magnetic modes

Decomposition

Page 20: Hand calculations of magnetic modes

Decomposition

= 12

Page 21: Hand calculations of magnetic modes

Decomposition

= 0 etc…

Page 22: Hand calculations of magnetic modes

Decomposition

Page 23: Hand calculations of magnetic modes

Projection

Page 24: Hand calculations of magnetic modes

Projection

Page 25: Hand calculations of magnetic modes

Projection

Page 26: Hand calculations of magnetic modes

Projection

Page 27: Hand calculations of magnetic modes

Magnetic structure

(b) TbMnO3 TN=41K k=(0.28 0 0)

Page 28: Hand calculations of magnetic modes

Magnetic structure

Page 29: Hand calculations of magnetic modes

Magnetic structure(b)

Page 30: Hand calculations of magnetic modes

Example (a)

Magnetic structure

Page 31: Hand calculations of magnetic modes

Magnetic structure