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Decomposition of Variables and Duality in non-Abelian Models A. P

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Presentation on theme: "Decomposition of Variables and Duality in non-Abelian Models A. P"— Presentation transcript:

1 Decomposition of Variables and Duality in non-Abelian Models A. P
Decomposition of Variables and Duality in non-Abelian Models A. P. Protogenov Institute of Applied Physics of the RAS, N. Novgorod V. A. Verbus Institute for Physics of Microstructures of the RAS, N. Novgorod

2 Outline Phase diagram SU(2) and U(1) mean field theory states
Knots of the order parameter distributions Current pseudogap phases SU(2) decomposition of variables Conclusion

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5 Standard t-J model

6 Two-component order parameter
P.A. Lee, N. Nagaosa, X.-G. Wen, Rev. Mod. Phys. 78, 17 (2006) Iwasawa decomposition

7 SU(2) mean field theory

8 Two-component Ginzburg-Landau-Wilson functional
E. Babaev, L.D. Faddeev, A.J. Niemi, PR B ‘02

9 Some useful identities

10 О(3) Skyrme-Faddeev sigma model

11 Hopf invariant, Q, for a map is the linking number in S3 of the preimages of two generic points in S2.

12 Examples of knots

13 Knot scales

14 Packing degree, α of the knot filaments
is a small parameter of the model α = Vknot / V ~ ξ2 R / R3 ~ ξ2/R2 < 1 α ~ æ-2

15 The result of this “surgical cut” is the following structure of phase distributions on a crystal surface

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17 Gain in current pseudogap states (V. Verbus, А. P. , JETP Lett

18 Current pseudogap states

19 SU(2) decomposition of variables: Hamiltonian in the infrared limit

20 SU(3) case Problem: 2-form F does not exact!
Flag manifold F2 = SU(3)/(U(1)×U(1)) instead of CP1 = SU(2)/U(1) = S2 dimF2 = 6 instead of dimCP1 = 2 How does Hopf invariant Q for the flag maniford F2 look like? Problem: 2-form F does not exact! Note that π3(F2)=Z as well as π3(CP1)=Z

21 Conclusion universal character of the phase stratification
1. The origin of the internal inhomogeneity and universal character of the phase stratification is the multi-vacuum structure in the form of the knotted vortex-like order parameter distributions. 2. As a result of phase competition, we have a natural window: α/ξ < c < 1/ξ , for the existence of the free energy gain due to supercurrent with large value of the momentum, c. Here, α = ξ2/R2 < 1 is a knot packing degree, ξ is the correlation length.


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