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Home > Documents > Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

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Crystallization temperature To crystallize
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New State of Matter in White Dwarfs Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09
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Page 1: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

New State of Matter in White Dwarfs

Gregory Gabadadze (NYU, CCPP)

with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09

Page 2: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

d -- average interparticle separation

1 Fermi << d << 1 Angstrom

???

10 eV < T << 10 KeV

..

He or C nuclei

and Electrons

Page 3: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Crystallization temperature

To crystallize

Page 4: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Temperature at which thermal de Broglie wavelengths begin to overlap

Uncertainties in particle position as large as inter-particle separation

Critical Temperature

Critical T > Crystallization T => Charged Condensation!

Page 5: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.
Page 6: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.
Page 7: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Heavier Stars End Up Either As Neutron Stars Or As Black Holes

Relatively Light Stars End Up As White Dwarfs

Typical density:

Page 8: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

versus

Outward Directed Electron Pressure

Inward Directed Gravitational Pull

What Keeps White Dwarfs Stable?

Electrons - Nuclei +

Page 9: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Standard Theory: Carbon, Oxygen, …,Containing WD’s Crystallize As they Cool Down

(Mestel, Ruderman)

Specific heat dominated by the crystal phonon contribution

Cooling time: ~10 Gyr

Page 10: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Helium White Dwarfs In Binary Systems 0.2-0.5 solar mass dwarfs with helium

core

Page 11: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Some characteristics for helium white dwarfs

Page 12: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Average carbon white dwarf

Page 13: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Building up effective field theory

• Order parameter: complex scalar

• U(1) symmetries for scalars and fermions

• Rotational symmetry• Galilean invariance• Schrodinger equation in the lowest

order

.

.

Page 14: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Effective Order Parameter Lagrangian for Charged Condensation

Greiter, Wilczek,Witten in BCS superconductivity

Solution

Page 15: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Small perturbations (simplified)

Page 16: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Spectrum of small perturbations

Phonon contribution to specific heat:

Page 17: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Impurity Interactions (H, He3,…)

Page 18: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Gap-less Fermion Excitations

Page 19: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Gap-less Fermions and Phonon

Page 20: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

White dwarf cooling

Page 21: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.
Page 22: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.
Page 23: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.
Page 24: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.
Page 25: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Magnetic Vortices in Superconductors and White Dwarfs

Rotation and Magnetic Properties of Helium White Dwarfs

Page 26: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Magnetic flux lines

Page 27: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Magnetic Flux Lines

Page 28: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Critical Magnetic Field

Disruption of Condensate

Page 29: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

London Magnetic Field

Page 30: Gregory Gabadadze (NYU, CCPP) with R. A. Rosen, JCAP, JHEP 08,09 D. Pirtskhalava, JCAP 09.

Conclusions and Outlook

Charge Condensate – new state of matter in the Universe Fast cooling of helium white dwarfs (super-massive carbon dwarfs ?) Magnetic field in flux tubes, high critical field; small London fieldOther possible applications: neutron star crust,…???


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