The OSI model extended including the Deep Physical Layer; the Deep Physical Layer (DPL) is a further layer placed under the Physical Layer; while the Physical Layer is focused on the 'bits' level, the Deep Physical Layer is focused on the 'electromagnetic field' configurations.

The OSI model extended including the Deep Physical Layer; the Deep Physical Layer (DPL) is a further layer placed under the Physical Layer; while the Physical Layer is focused on the 'bits' level, the Deep Physical Layer is focused on the 'electromagnetic field' configurations.

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In this paper a series of concepts concerning the relationships between electromagnetic theory and information transmitted in communication systems using electromagnetic waves are organized in a systematic framework through the introduction of the "Deep Physical Layer" (DPL), a layer placed under the Physical Layer (PL) of the OSI model. While the...

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... consider the OSI (Open Systems Interconnection) model (Fig. 1). The layer closest to the physical characteristics of the communication system is the Physical Layer. This layer is focused on the ability of the system to transmit information in terms of bits in a reliable and effective ...
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... Fixed bemforming antennas, phased arrays, adaptive antennas, SU-MIMO, MU-MIMO, Massive MIMO, as well as Holographica antennas and Intelligent surface antennas are basically radiating systems that optimize the use of the available NDF at the DPL level to reach different goals at the PL level [12]. Now, let us consider the geometry shown in Fig. 11, in which a reflective surface (drawn as a black line and indicated as B) is present. An electromagnetic opaque object, drawn as a grey rectangle, is placed between the source and the receiver, preventing a LOS ...
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... to λ/2 as a transmitting antenna. Each symbol is associated to a (complex) radiation pattern. Consequently, the TX antenna radiates a field that is the interference of three different radiated field configurations (one for each subscriber). As first step, let us consider the standard Zero-Forcing solution adopted in Massive MIMO synthesis. In Fig. 14 the (total) radiated pattern is drawn for all the possible combinations of the QPSK symbols transmitted toward the three subscribers. We can note that the sidelobe level does not meet the requirement outside the (−45 • , 45 • ) angular region. Now, let us consider the synthesis process proposed in [6], based on the theory summarized in ...
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... • , 45 • ) angular region. Now, let us consider the synthesis process proposed in [6], based on the theory summarized in this paper, and slightly modified to handle Massive MIMO (see also Appendix III). The (total) radiated pattern drawn for all the possible combinations of the QPSK symbols transmitted toward the three subscribers is shown in Fig. 15. In terms of communication parameters, the solution causes a loss in the power received by the three users equal to 0.01 dB, 0.01 dB and 0.05 dB compared to the Zero Forcing, while the SIR is respectively 36.5 dB 48.0 dB and 38.2 dB, confirming the underuse of the available spatial degrees of freedom in standard mMIMO ...
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... the problem discussed is the following. Suppose an "innocent" antenna transmits a stream of bits using BPSK constellation. We want to replace the "innocent" antenna with a different antenna that can transmit secret messages to an authorized receiver without anyone outside the direction of the authorized receiver noticing anything suspicious (see Fig. 16). The problem is conceptually close to the grille cipher, in which a pierced sheet, placed on an "innocent" cover text, is used to select the letters of the message hidden by the cover ...
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... strategy adopted in this paper to obtain a steganographic system is based on the identification of a set of four field configurations that are distinguishable on Ω a but collapse into only two distinguishable field configurations on Ω h . (see Fig. 17). Accordingly, communication at the DPL involves four different field ...
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... Fig. 18 the amplitude (upper figure) and the phase (lower figure) of the y 1 pattern is plotted. In the same figure the two vertical green bars show the φ = 18 o angular range ouside which the Ω h domain is positioned. The y 2 pattern (amplitude upper figure and phase lower figure) is plotted in Fig. 19. The two patterns y 1 and y 2 are ...
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... Fig. 18 the amplitude (upper figure) and the phase (lower figure) of the y 1 pattern is plotted. In the same figure the two vertical green bars show the φ = 18 o angular range ouside which the Ω h domain is positioned. The y 2 pattern (amplitude upper figure and phase lower figure) is plotted in Fig. 19. The two patterns y 1 and y 2 are indistinguishable for a receiver placed in Ω h . We can use the two solutions y 1 and y 2 to obtain the four field configurations required at the DPL. In particular, at the VOLUME 4, 2016 DPL the four cases are encoded in the following four field configurations: 1) case 1: y 1 ; 2) case 2: −y 1 ; 3) ...
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... the above definition, we have that a set of points are distinguishable in presence of an level of uncertainty if they belong to a 2 distinguishable set. Consequently, the maximum amount of information identifiable reliably in a set A at an level of uncertainty is equal to C 2 (see Fig. ...
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... example shown in Fig. 14 considers an equispaced linear array of 31 λ/2 long elements with an inter element distance equal to λ/2 as a transmitting antenna, and three users each of them modelled as a λ/2 long wire antenna as the receiving antenna. Two scattering point objects are placed at (x = 40λ; y = −30λ) and (x = 70λ; y = 50λ) respectively. The far-field ...
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... an inter element distance equal to λ/2 as a transmitting antenna, and three users each of them modelled as a λ/2 long wire antenna as the receiving antenna. Two scattering point objects are placed at (x = 40λ; y = −30λ) and (x = 70λ; y = 50λ) respectively. The far-field sidelobes of the transmitting antenna outside the angular range (−α, α) ( Fig. 13) with α = 45 o are required to be lower than −40 dB as per design specification. The method is a straightforward modification of the procedure introduced in [6] in case of SU-MIMO synthesis with pattern ...
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... [6] (see also Fig. ...

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Chapter
The objective of this chapter is a description of the wireless communication process from a physical point of view. The analysis of the communication system is carried out considering an extended version of the OSI stack that includes an additional layer placed below the Physical Layer (PL). In this further layer, called the Deep Physical Layer (DPL), the communication process is analyzed in terms of distinguishable electromagnetic field configurations on the receiving antenna. The DPL contains all the resources potentially available to the telecommunication system in terms of space/time/polarization field configurations, while the PL implements specific solutions to exploit the potential offered by the DPL. Such a potential is limited only by the physical laws, which are inviolable. Consequently, the limits imposed at the level of DPL are absolute. In this sense, the DPL is a more fundamental level than the PL. The numerous solutions proposed for 6G that include intelligent modifications of the propagation environment can be seen as “data processing” at the DPL level in order to preserve information lost in previous generations of communication systems.