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**Physics Note****Published**

# **What are the Numbers that Experiments Provide?**

**C. Tsallis**

1994

[**Download PDF **0.4 MB](https://index.cbpf.br/files/publicacao/6ad2a767639f62b11adbb5d2/pdf) [**Contact owner**](mailto:apub@cbpf.br?subject=What%20are%20the%20Numbers%20that%20Experiments%20Provide%3F)

## **Publication details**

<dl>

<dt>Authors</dt>
<dd>C. Tsallis</dd>

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

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

<dt>Publication date</dt>
<dd>1994</dd>

<dt>Description</dt>
<dd>On the basis of a recently proposed generalization of Boltzmann-Gibbs Statistical Mechanics and Thermodynamics, we argue that the numbers provided by experimental measurements are to be interpreted as q-expectation values &lt;math&gt;\left \langle \hat O \right \rangle \equiv &lt;/math&gt; &lt;math&gt;Tr \hat \rho^{q}\hat O \,\!&lt;/math&gt;, where &lt;math&gt;\hat O\,\!&lt;/math&gt; is the observable, &lt;math&gt; \hat \rho\,\!&lt;/math&gt; is the density operator and the real index &lt;math&gt;q\,\!&lt;/math&gt; characterizes the corresponding (generically nonextensive) entropy and depends on some general characteristics of the system. The familiar association with the mean value &lt;math&gt;\left \langle \hat O \right \rangle _{1} \equiv \,\!&lt;/math&gt; &lt;math&gt;Tr \hat{\rho}\hat O\,\!&lt;/math&gt; as well as the extensivity of standard additive observables are recovered only for the Boltzmann-Gibbs particular case &lt;math&gt;(q = 1), \forall \hat{\rho}&lt;/math&gt;, or for pure states, &lt;math&gt;\forall q\,\!&lt;/math&gt;. This interpretation leaves untouched the standard additivity and conservation of energy for ''pure states'', but, unless &lt;math&gt;q = 1\,\!&lt;/math&gt;, modifies the definition and additivity of internal energies for '' statistical mixtures''.</dd>

<dt>Year</dt>
<dd>1994</dd>

<dt>Number</dt>
<dd>CBPF-NF-035/94</dd>

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

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

</dl>

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