where w ( r ) is the weighting function associated with the basis functions g$_{n}$ . The multiplicity is simply given by c 2 n multiplied by (2J+1) where J is the spin of the hadron. There are a number of special cases, which we address in turn. The pseudo-Goldstones are described by a separate holographic field, θ , in our model and are represented by functions f$_{n}$ ( r ). The relative contributions the fields make to the stress-energy tensor are Δ$_{1}$ , Δ$_{2}$ are functions of r , completely calculable from the holographic model, using the usual definition of the stress-energy tensor: To ensure the fields A$_{µ}$ and θ see the same contribution to the stress- energy tensor we must rescale the Gaussian. If our standard Gaussian is Ψ( r ) then for the energy to be equally divided between all sectors we require ∂$_{r}$θ = √ Δ 2 Δ $_{1}$∂$_{r}$ Ψ. Since the underlying asymptotically free dynamics will distinguish the strange quark from the up and down quarks, we also multiply the Gaussian by a factor of ( γ$_{s}$ ) σ where σ is the strangeness content of the stack. γ$_{s}$ is then the 115 Strangeness Suppression Factor Pseudo-Goldstone Bosons c$_{n}$ = ∫ ∞ 0 Ψ( r ) w ( r ) g$_{n}$ ( r ) dr (8.1) T$_{rr}$ ∼ Δ$_{1}$( r )( ∂$_{r}$θ ) 2 + Δ$_{2}$( r ) η $^{µν}$( ∂$_{r}$A$_{µ}$ )( ∂$_{r}$A$_{ν}$ ) + . . . (8.2) T$_{µν}$ ≡ − 2 1 √ − g δ δg µν ( √ − g L matter ) (8.3)