# An ECCD--Electronic Charge Compensation Device--As a Quantum Dissipative System
## 4 Operation of an ECCD on a Tentative Quantum Scheme
The super-absorption process [12], as the reciprocal process of super-emission introduced 65 years ago by [PERSON] [13], happens over a set of N \"quantum entities\" that cooperatively interact with a surrounding electromagnetic field. In general, these quantum entities can be atoms, molecules, ions, semiconductor quantum dots, bio-synthetic molecular ring structures, etc. They have an allowed resonant and discrete dipolar transition. \"Unlocated excitons\" are also adequate quantum entities. An exciton may be visualized as a couple consisting of an electron and the associated hole, attracted to each other via Coulomb forces. Therefore, an exciton represents a quasi-particle or a \"free exciton\" in the Wannier exciton sense. A set of M electrons associated with M holes is also an exciton--an \"exciton cluster\" or \"exciton cell\". It can collaboratively interact with a surrounding electromagnetic field. A set of P \"exciton clusters\" could be available to collaboratively interact if the surrounding field has a spatial and temporal coherence--length of pulse--larger than the spatial dimension for the ubication of the P collaborative set of an \"exciton cluster\". In principle, these are the candidates to be considered able to adapt to a super-absorption process. The ECCD works in environmental temperatures (5\({}^{\circ}\)-25 \({}^{\circ}\)C \(\approx\) 278\({}^{\circ}\)-298 \({}^{\circ}\)K, average: 280 \({}^{\circ}\)K) and will be associated from statistic thermodynamic bases to a \"binding energy\" (or ionization energy) E\({}_{\rm x}\)\(\geq\) kT, where k is Boltzmann constant. In these conditions, the binding energy E\({}_{\rm x}\)\(\approx\) 8.3 10\({}^{-6}\) eV involves a singled exciton electron-hole, and the ratio between these two energies gives N; the approximated number of exciton clusters. M \(\geq\) 3000. The value of binding energy E\({}_{\rm g}\) is compatible with the Columbian energy E\({}_{\rm C}\) of an exciton cluster, if distance r \(\approx\) 16 cm and relative electric permeability \(\varepsilon_{\rm r}\)\(\approx\) 2.4. This last value is realistic for a cold plasma in low frequencies (GHz)  
\[{\rm E}_{\rm C}=({\rm N}_{\rm e})^{2}\,/\,4\pi\varepsilon_{\rm o}\varepsilon_{ \rm r}. \tag{3}\]  
A density of charges N\({}_{\rm e}\), N\({}_{\rm h}\) (electron and hole) can be derived from of Debye length considered in the order of micrometers, and is well-compatible with the take electric permeability value, N\({}_{\rm e}\)\(\approx\) 4 \(\times\) 10\({}^{10}\) m\({}^{-3}\). These values show that squaring possible number P of exciton clusters in an ECCD (DDCE 100 model) wavelength of radiofrequency field P, must result in P \(<\) 20 = ring length/\(\lambda\), and in consequence  
\[{\rm N}_{\rm e},{\rm N}_{\rm h}\geq{\rm N}={\rm P}\,{\rm M}. \tag{4}\]  
There is an inefficiency of about two orders of magnitude in the exciton clusters' formation, but the values is possibly less in the single excitons' formation. In an ECCD, the excitons are  
Figure 10: One potential realization of superabsorption [12]. confined independently into the set of N\({}_{\rm e}\) electrons and N\({}_{\rm h}\) holes in specific areas around the device. The numerical simulation analysis of radiofrequency field--Section 3--showed the quality of multi-resonator behavior of an ECCD. At the same time, the spatial distribution of the evanescent field, mainly of electric field of radiofrequency, opens up the possibly confined electric charges to two local zones, near to the environmental union of each ECCD cap with a dielectric isolator ring. These confinements are not permanent but temporary: we estimated the total effective time in a temporary fraction \(\approx\) 4/9 of one period time, divided into two short times \(\approx\) 2/9 of one period time. In our case of DINNTECO ECCD 100, the short time of pulse confinements is \(\approx\) 0.15 ns with a cadence repetition of \(\approx\) 0.65 ns.