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XII International School-seminar “The Actual Problems of Microworld Physics” July 22 – August 2, 2013, Gomel, Belarus Vacuum polarization effects in the.

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Presentation on theme: "XII International School-seminar “The Actual Problems of Microworld Physics” July 22 – August 2, 2013, Gomel, Belarus Vacuum polarization effects in the."— Presentation transcript:

1 XII International School-seminar “The Actual Problems of Microworld Physics” July 22 – August 2, 2013, Gomel, Belarus Vacuum polarization effects in the cosmic string background and primordial magnetic fields in the Universe Yu. A. Sitenko (BITP, Kyiv, Ukraine)

2 Outline 1. Spontaneous symmetry breaking and topological defects of 2. Abrikosov-Nielsen-Olesen vortex and cosmic strings 3. Induced vacuum current and magnetic field in the cosmic string background 4. Induced vacuum energy-momentum tensor in the cosmic string background 5. Primordial magnetic fields in the Universe

3 Casimir effect vacuum polarization

4 Aharonov-Bohm effect

5 Casimir-Aharonov-Bohm effect vacuum polarization

6 Casimir-Aharonov-Bohm effect vacuum polarization

7 U(1) gauge Higgs model upon quantization:

8 Topological defect of : Abrikosov-Nielsen-Olesen vortex stress-energy tensor and are nonvanishing inside the vortex core

9 Einstein-Hilbert equation scalar curvature Global characteristics of ANO vortex: linear energy density: flux of the gauge field:

10 The space-time metric outside the string core: where, a deficit angle is equal to

11 Cosmic strings were introduced in T.W.B.Kibble, J. Phys. A 9, 1387 (1976); Phys. Rep. 67, 183 (1980)‏ A.Vilenkin, Phys. Rev. D 23, 852 (1981); D 24, 2082 (1981)‏ Earlier studies in M.Fierz (unpublished)‏ J.Weber, J.A.Wheeler, Rev.Mod.Phys. 29, 509 (1957)‏ L.Marder, Proc. Roy. Soc. London A 252, 45 (1959)‏ A cosmic string resulting from a phase transition at the scale of the grand unification of all interactions is characterized by the values of the deficit angle

12 Generalization: d+1-dimensional space-time with a codimension-2 brane ANO vortex

13 stress-energy tensor scalar curvature metric tension flux

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18 Vacuum current induced by a codimension-2 brane where g/2π Yu.A.S., N.D.Vlasii, Fortschr.Phys. 57, 705 (2009)‏

19 Induced vacuum magnetic field Maxwell equation magnetic field strength and its flux

20 Identifying with the transverse size of the string core, then and Yu.A.S., N.D.Vlasii, Class. Quantum Grav. 26, 195009 (2009)‏

21 Energy-momentum tensor of charged massive scalar field point-splitting regularization where

22 Equation for Green's function decomposition of the VEV of the chronological operator product Renormalized VEV of the energy-momentum tensor

23 Induced vacuum energy-momentum tensor in the cosmic string background Yu.A.S., Vlasii. Class. Quantum Grav. 29, 095002 (2012) where

24 Conservation: Trace: conformal invariance is achieved in the massless limit at

25 For a global string

26 For a vanishing string tension Yu. A. S. and V. M. Gorkavenko, Phys. Rev. D 67, 085015 (2003). Yu. A. S. and A. Yu. Babansky, Mod. Phys. Lett. A 13, 379 (1998). Yu. A. S. and A. Yu. Babansky, Phys. At. Nucl. 61, 1594 (1998).

27 For a vanishing mass of scalar field: Trace: V. P. Frolov and E. M. Serebriany, Phys. Rev. D 35, 3779 (1987). J. S. Dowker, Phys. Rev. D 36, 3742 (1987).

28 -dimensional space-time where

29 Transverse size of a codimension-2 brane temporal component of the vacuum energy-momentum tensor (vacuum energy density) V.M.Gorkavenko,Yu.A.S., O.B.Stepanov. Intern.J.Mod.Phys.A 26, 3889 (2011)

30 Dimensionless energy density r 3 t 00 as a function of mr (singular brane) ξ = -1 ξ = 0 ξ = 1/8 ξ = 1/4 ξ = 1/2 ξ = 1

31 Dimensionless energy density r 3 t 00 as a function of mr (the case of mr 0 =1) ξ = -1 ξ = 0 ξ = 1/8 ξ = 1/4 ξ = 1/2 ξ = 1

32 Dimensionless energy density r 3 t 00 as a function of mr (the case of mr 0 =10 -1 ) ξ = -1 ξ = 0 ξ = 1/4 ξ = 1/2 ξ = 1

33 Dimensionless energy density r 3 t 00 as a function of mr (the case of mr 0 =10 -2 ) original zoomed ξ = -1 ξ = 0 ξ = 1/8 ξ = 1/2 ξ = 1

34 Total energy V.M.Gorkavenko,Yu.A.S., O.B.Stepanov. Intern.J.Mod.Phys.A 26, 3889 (2011)

35 Magnetic fields in galaxies and galactic clusters: 10 -6 ÷10 -5 Gauss Extragalactic magnetic fields: 10 -16 ÷10 -10 Gauss galactic dynamo Seed (primordial) magnetic field: ≥10 -20 Gauss Superconducting cosmic string (Witten et al, 1986) Gauge cosmic string inducing vacuum polarization L.V.Zadorozhna, B.I.Hnatyk, Yu.A.S. Ukrain.J.Phys.58,398(2013)

36 Conclusion Cosmic string induces current and magnetic field in the vacuum The magnetic field strength is directed along a cosmic string where where m H is the mass of the string-forming Higgs field. is the gauge flux, is the coupling constant of the quantized field with the string-forming gauge field, is the mass of the quantized field, is its electric charge. Thus, owing to the vacuum polarization by a cosmic string, the latter is dressed in a shell of the force lines of the magnetic field. The flux of the magnetic shell is

37 Thank you


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