# An ECCD--Electronic Charge Compensation Device--As a Quantum Dissipative System
## 3 Simulation Study of the Electromagnetic Radiofrequency Field in an ECCD
### Resonant Modes
Figure 8 show simulations results obtained for the vector electric field (V/m) in an ECCD-DINTECO DDCE 100 model: (A) 3D representation, (B) YZ plane cut, and (C) XZ plane cut. All of them for 1.153 GHz. The secondary lateral mode at 1.153 GHz for the ECCD--DINTECO DDCE 100 model--uniquely presents an intense outdoor electric field, but with a limited range (\(<\)50 cm radius) normal (X, Y) to the vertical (Z) axis. This mode corresponds to a \"confocal\" resonator scheme that works at approximately 4d \(\approx\uplambda\)/2. All modes, but most substantially the other modes that make up the quasi-continuous  
Figure 7: Distribution of the radiofrequency electric field (V/m): (**A**) at 1.153 GHz and (**B**) at 1.71 GHz, both in the nearby free space in an ECCD—DINTECO DDCE 100 model. background, contribute to the outdoor field with an equivalent but less intense range, although many modes make up the quasi-continuous background. This radiofrequency field forms a ring--a flattened toroid with an almost rectangular section (5-6 x 12-14 cm for the ECCD--DINNTECO DDCE 100 model). This ring surrounds the DDCE externally by the lower cap, and its average circumference corresponds with a resonance of the radiofrequency field of a high order, 12 to 14 times the wavelength. It reminds us of the so-called \"whispering gallery\" resonators [10]. The distance corresponds to half the length of a pulse travelling from the main modes (\(\cong\)7.5 m), while the continuous bottom with the pulse length being 0.8 m for ECCD--DINNTECO DDCE 100 model. This results in compliance with the condition of transient stationery due to the possible interference of the pulse itself (given the length of the pulse, which evens overlaps once with itself), may be an indicator of the distributed functionality of each set of modal distributions and their dimensional incidence in ECCD performances. Radiofrequency fields--as they are oscillating at high frequency--do not induce charge shifts, but--as they are resonant, and therefore stationary--they cause retention or entrapment of electric charges, which increase the effective recombination section to enhance charges compensation. Our working hypothesis is that the upper toroid ring traps and confines electrons or eventual negative ions. And the largest and farthest toroid ring, close to the lower caps and even to the stem, traps and confines positive charges (ions +), or most probable holes (positive electron charges). Due the fact that the positive ions have bigger masses, they will have difficulties for migrating from the earth to the lower caps. In Figure 9 is a representative presentation of this on an ECCD--the DINNTECO DDCE 100 model--photography. Figure 8: Simulations obtained from the vector electric field (V/m) in an ECCD-DINNTECO DDCE 100 model: (**A**) 3D representation, (**B**) YZ plane cut, and (**C**) XZ plane cut. All of them for 1.153 GHz. Figure 9: Graphical representation of spatial distributions of confined and intense evanescent field zones, corresponding to possible confinement of negative charges (in beige) and positive charges or holes (in blue).