Physics NotePublished
Quantum Bound on the Specific Entropy in Strong-Coupled Scalar Field Theory
M. Aparicio Alcalde; G. Menezes; N.F. Svaiter
Publication details
- Authors
- M. Aparicio Alcalde; G. Menezes; N.F. Svaiter
- Type
- Physics Note
- Status
- Published
- Publication date
- 02/08/2010
- Description
- Using the Euclidean path integral approach with functional methods, we discuss the $(g_{0}\,\varphi^{\,p})_{d}$ self-interacting scalar field theory, in the strong-coupling regime. We assume the presence of macroscopic boundaries confining the field in a hypercube of side $L$. We also consider that the system is in thermal equilibrium at temperature $\beta^{\,-1}$. For spatially bounded free fields, the Bekenstein bound states that the specific entropy satisfies the inequality $\frac{S}{E} < 2 \pi R$, where $R$ stands for the radius of the smallest sphere that circumscribes the system. Employing the strong-coupling perturbative expansion, we obtain the renormalized mean energy $E$ and entropy $S$ for the system up to the order $(g_{0})^{-\frac{2}{p}}$, presenting an analytical proof that the specific entropy also satisfies in some situations a quantum bound. Defining $\varepsilon_d^{(r)}$ as the renormalized zero-point energy for the free theory per unit length, the dimensionless quantity $\xi=\frac{\beta}{L}$ and $h_1(d)$ and $h_2(d)$ as positive analytic functions of $d$, for the case of high temperature, we get that the specific entropy satisfies $\frac{S}{E} < 2\pi R\,\frac{h_1(d)}{h_2(d)}\,\xi$. When considering the low temperature behavior of the specific entropy, we have $\frac{S}{E} <2\pi R\, \frac{h_1(d)}{\varepsilon_d^{(r)}}\xi^{\,1-d}$. Therefore the sign of the renormalized zero-point energy can invalidate this quantum bound. If the renormalized zero point-energy is a positive quantity, at intermediate temperatures and in the low temperature limit, there is a quantum bound.
- Year
- 2007
- Number
- CBPF-NF-022/07
- Linked to a thesis
- No
- Linked to a grant
- No