hedgehog antihedgehog annihilation to a static soliton

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4-6 November 2004 Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 1 Leslie-Ericksen

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Page 1: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 1

Leslie-Ericksen

Page 2: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 2

Hedgehog-Antihedgehog Annihilation to a

Static Soliton

Nematic Liquid Crystals

Cylindrical Geometry

Point Defect Dynamics

Page 3: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 3

Uniaxial NematicsOrientationally ordered 3D liquids

nunit pseudo-vector

director, nDefine

Only 1 line defect – the Möbius Defect (S=±1/2)Theorem:

S=+1/2 homotopic to S=-1/2Corollary:

Energy ∝ S2Corollary:

Corollary:

Page 4: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 4

3D Möbius Defects

+1/2 +1/2 +1/2 -1/2

Y. Bouligand, P.E. Cladis, L. Liébert, and L. Strzelecki, Study of thin Films of Polymerized Liquid Crystals, Mol. Cryst. Liq. Cryst. 25, 355 (1973).

Page 5: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 5

Yves Bouligand Lemma

In nematics, only 1 line defect, the Möbius line.

Lemma: Includes edge disclinations.

Page 6: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 6

S=1 is homotopic to the Uniform State

Frank Free Energy

Page 7: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 7

Solutions: A=0

A is constant of integration

A=0

Page 8: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 8

Solutions: Energy Minimum, A=1

A=1

Static Solitons

Dresden 1999

P.E. Cladis and M. Kléman

J. de Phys. (Paris) 33, 591 (1972) per unit length

Page 9: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 9

Point DefectsAsymptotic Freedom

Spherical estimate

P.E. Cladis and H.R. Brand, Physica A 326, 322 (2003)

Page 10: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 10

Point Defects

z

x

C.E. Williams, P. Pieranski and P.E. Cladis, Phys. Rev. Lett. 29, 90 (1972)

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 11

Dresden 1999

mk hrb pp

mb ikpec

Happy Birthday, Jerry! From all of us.

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 12

∆z-t (time) Plots

z

x

Space-time plots:

Video-line sampling

∆z

Tube diameter=d=2R

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 13

Asymptotic Freedom

P.E. Cladis and H.R. Brand, Physica A 326, 322 (2003)

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 14

Solutions: A≥1

Elliptic function of the first kind

A=1/sinα

Complete

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 15

Solutions: A≥1 (continued)

2ro

Page 16: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 16

F vs α

π/2

: Constant of integration A=1/sinα

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 17

Model Dynamics with α(z,t) in region between Hedgehog and Anti-Hedgehog

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 18

MODEL

α(z,t) Situation Sketch Feature

π/2 stationary Asymptotic freedom

≠ π/2Out of

equilibriumClosing to annihilation

π/2NA

No defectsAnnihilated

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 19

Observed Countdown to Annihilation

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 20

+Smectic Fluctuations

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 21

Model

Page 22: Hedgehog Antihedgehog Annihilation to a Static Soliton

4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 22

Point Defect Dynamics

-depends sensitively on perturbation magnitude

sufficiently small � asymptotic freedom

sufficiently large � 2 regimes: z/R>1 and z/R<1

-asymmetric � larger effective mass of antihedgehog

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4-6 November 2004Jerry’s B’day Party, MN Advanced Liquid Crystal Technologies, Inc. 23

Acknowledgements

Photos of Dresden 1999 Defect Meeting by Dr. Isabelle Kraus

Hedgehog sketch from: http://hem.passagen.se/hedgehogs/hedgehogs.html

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Hedgehog

Hedgehog

http://hem.passagen.se/hedgehogs/hedgehogs.html

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Not Monopoles

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Toulouse TheoremYou cannot lassoe a basket ball.

Proof:

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Mayola Walters and PEC (1980)

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Monochromatic Scan

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Pawel and PEC Dresden 1999