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nD Gravity with n-2 Killing vectors Tonatiuh Matos http://www.fis.cinvestav.mx/~tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral fields The invariance group of chiral fields. Methods of solutions

ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

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Page 1: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

nD Gravity with n-2 Killing vectors

Tonatiuh Matoshttp://www.fis.cinvestav.mx/~tmatos/

• nD-Einstein equations with n-2 commuting Killing vectors

• Chiral fields• The invariance group of chiral fields.• Methods of solutions

Page 2: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The nD-Einstein equationswith n-2 commuting

Killing Vectors

Page 3: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The Ricci Tensor

• i

Page 4: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Ricci tensor in matrix notation

Page 5: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

In vacuum

• Implies:

Page 6: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Brane Cosmology

• Inflation

Page 7: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The matter components of the Universe

M ~ 0.27 0.1, ~ 0.73 0.1

• 0 ~ 1.

• The matter component

M = b + + ~

• 0.04 + DM,

• where DM ~ 0.23.

• but• DM ni ??.

DM + ~ 0.96

• Concordance!!.

Page 8: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The Dark Energy

• p= • =A0+A1a=0+a z/(1+z)

• Constante Cosmológica: 0 = -1, 1 = 0

• Quintessence: • Phantom: K=-,,

• Quintom:

Page 9: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The Dark Energy

Page 10: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The Dark Energy

Page 11: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The Dark Energy

Page 12: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

5D Gravity

• Potential Space

Page 13: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The corresponding Lie Algebra

• Then:

• Define:

Page 14: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The metric and the Lagrangian

• The equivalent Lagrangian

Page 15: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The field equations in the potential space

=0

implies

If we define

Page 16: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The ansatz

A= A( i)

• And the Killing equation:

Page 17: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Implies

Page 18: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The main theorem

Page 19: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The harmonic maps

• The monopole:

• The dipole:

Page 20: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

The rotating solutions

• The gravitational potential:

• The scalar field potential:

Page 21: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Charged solutions

Page 22: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Rotating Wormhole

Page 23: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Rotating Wormhole

Page 24: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Rotating Wormhole

Page 25: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormholes

• Pelicula

Page 26: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormholes

Page 27: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormholes

Page 28: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormholes

• Pelicula

Page 29: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormholes

Page 30: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormholes

Page 31: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormholes

Page 32: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Rotating Wormhole

• Then

Page 33: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Wormhole Rotante•Ejemplo: Ejemplo: J=10J=10-10-10, ,

•Entonces Entonces 11»» 1.4 1.4££101055

•Para una estrella fantasma (phantom) Para una estrella fantasma (phantom) con la masa de la tierra, la carga escalar con la masa de la tierra, la carga escalar eses q q 0.003 m0.003 mPlankPlank por metro. por metro.

• v- = 15 km/seg• v+ = 7 c

Page 34: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Across the Universe

Page 35: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Across the Universe

• Milenio

Page 36: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

Across the UniverseLas palabras surgen a raudales como una lluvia infinita en un vaso de papel

Se deslizan al pasar Desaparecen a través del universo

Charcos de tristeza, olas de alegría flotan en mi mente abierta Poseyéndome y acariciándome

Jai Guru De Va Om Nada cambiará mi mundo Nada cambiará mi mundo

Imágenes de luz que bailan ante mí como un millón de ojos Que me llaman y me llaman a través del universo

Pensamientos serpenteando como un viento inquieto en un buzón Tambaleándose ciegamente mientras hacen su camino a través del universo

Jai Guru De Va Om Nada cambiará mi mundo Nada cambiará mi mundo

Sonidos de risas y sombras de tierra suenan a través de mi vista abierta Incitándome e invitándome

Un amor eterno y sin límites brilla a mí alrededor como un millón de soles Llamándome y llamándome a través del universo

Jai Guru De Va Om Nada cambiará mi mundo Nada cambiará mi mundo

Page 37: ND Gravity with n-2 Killing vectors Tonatiuh Matos tmatos/ nD-Einstein equations with n-2 commuting Killing vectors Chiral

• and

• ω = sin()

• Magnetic monopole