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**Physics Note****Published**

# **Quantum Bound on the Specific Entropy in Strong-Coupled Scalar Field Theory**

**M. Aparicio Alcalde; G. Menezes; N.F. Svaiter**

08/02/2010

[**Download PDF **0.2 MB](https://index.cbpf.br/files/publicacao/6ad2a767639f62b11adbb02f/pdf) [**Contact owner**](mailto:apub@cbpf.br?subject=Quantum%20Bound%20on%20the%20Specific%20Entropy%20in%20Strong-Coupled%20Scalar%20Field%20Theory)

## **Publication details**

<dl>

<dt>Authors</dt>
<dd>M. Aparicio Alcalde; G. Menezes; N.F. Svaiter</dd>

<dt>Type</dt>
<dd>Physics Note</dd>

<dt>Status</dt>
<dd>Published</dd>

<dt>Publication date</dt>
<dd>02/08/2010</dd>

<dt>Description</dt>
<dd>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 $\frac{S}{E} &lt; 2 \pi R$, 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 $\frac{S}{E} &lt; 2\pi R\,\frac{h_1(d)}{h_2(d)}\,\xi$. When considering the low temperature behavior of the specific entropy, we have $\frac{S}{E} &lt;2\pi R\, \frac{h_1(d)}{\varepsilon_d^{(r)}}\xi^{\,1-d}$. 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.</dd>

<dt>Year</dt>
<dd>2007</dd>

<dt>Number</dt>
<dd>CBPF-NF-022/07</dd>

<dt>Linked to a thesis</dt>
<dd>No</dd>

<dt>Linked to a grant</dt>
<dd>No</dd>

</dl>

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