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Kaluza–Klein spectrum of the gauge vector field in the thin-string and

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Kaluza–Klein spectrum of the gauge vector field in the thin-string and
Bulk fields localization on thick string-like brane in f(T

Bulk fields localization on thick string-like brane in f(T

Fraction H²/ρ for oscillating solution depending on γ: γ > γcrit (upper

Fraction H²/ρ for oscillating solution depending on γ: γ > γcrit (upper

AdS-QCD correspondence in nLab

AdS-QCD correspondence in nLab

Gauge field and brane-localized kinetic terms on the chiral square

Gauge field and brane-localized kinetic terms on the chiral square

August 2009 – Quantum field theory

August 2009 – Quantum field theory

Spectral dimension of the target spacetime in string field theory

Spectral dimension of the target spacetime in string field theory

Weigand Introduction To String Theory, PDF

Weigand Introduction To String Theory, PDF

The ratio n ≡ L equatorial L meridional is plotted as a function of β

The ratio n ≡ L equatorial L meridional is plotted as a function of β

Fields and Symmetry. The Four Fundamental Forces, Part 2…

Fields and Symmetry. The Four Fundamental Forces, Part 2…

PDF) Kinetic mixing from Kaluza-Klein modes: A simple construction

PDF) Kinetic mixing from Kaluza-Klein modes: A simple construction

Check of the condition fR=ϕ for the core with Schwarzschild exterior.

Check of the condition fR=ϕ for the core with Schwarzschild exterior.

Localization of limit-from𝒒-form field on the brane-world by

Localization of limit-from𝒒-form field on the brane-world by

Fraction H²/ρ for oscillating solution depending on γ: γ > γcrit (upper

Fraction H²/ρ for oscillating solution depending on γ: γ > γcrit (upper

The oscilating part˜hpart˜ part˜h i (t) = [a i (t)] 2 − [c i + b i t]

The oscilating part˜hpart˜ part˜h i (t) = [a i (t)] 2 − [c i + b i t]

Critical trajectory of second kind. Photons are coming from distances

Critical trajectory of second kind. Photons are coming from distances