2020
DOI: 10.1109/tvt.2020.3011408
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Geometric Analysis of the Doppler Frequency for General Non-Stationary 3D Mobile-to-Mobile Channels Based on Prolate Spheroidal Coordinates

Abstract: Mobile-to-mobile channels often exhibit timevariant Doppler frequency shifts due to the movement of transmitter and receiver. An accurate description of the Doppler frequency turns out to be very difficult in Cartesian coordinates, and any subsequent algebraic analysis of the Doppler frequency is intractable. In contrast to other approaches, we base our investigation on a geometric description of the Doppler frequency with the following three mathematical pillars: prolate spheroidal coordinate system, algebrai… Show more

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Cited by 10 publications
(20 citation statements)
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“…This is not a coincidence, but can be explained by the fact, that in the air-ground channel, most of the reflectors causing the MPCs are located on the ground comparatively close to the GS. At the same time, each reflector is located on the surface of a prolate spheroid having the transmitter and receiver in its focal points [20]. The size of the spheroid a given reflector is located on is determined by the corresponding MPC's delay.…”
Section: Resultsmentioning
confidence: 99%
“…This is not a coincidence, but can be explained by the fact, that in the air-ground channel, most of the reflectors causing the MPCs are located on the ground comparatively close to the GS. At the same time, each reflector is located on the surface of a prolate spheroid having the transmitter and receiver in its focal points [20]. The size of the spheroid a given reflector is located on is determined by the corresponding MPC's delay.…”
Section: Resultsmentioning
confidence: 99%
“…Besides these unique expressions for the locations of VT and VR, the propagation delay of an MPC caused by SBR allows to constrain the possible locations of the corresponding RP. Specifically, this means that the possible locations of an RP coincide with the locations on the surface of an ellipsoid, each of which equally causes the propagation delay τ l,n [26], [27]. For reflections from surfaces orthogonal to the axis between the transmitting and receiving nodes, e.g., vertical walls of buildings, the possible locations are reduced to the circumference of an ellipse, as shown in Fig.…”
Section: Geometric Properties For Single-bounce Reflectionsmentioning
confidence: 99%
“…far from the propagation path of an MPC for modeling the variance. Specifically, we use the definition of the excess path length describing an ellipse with foci at (virtual) transmitting and receiving nodes, see (26) and (27). By introducing a threshold ξ th for the excess path length, we therefore achieve an inherent geometric separation, i.e., between locations near the propagation path with excess path lengths below the threshold and locations far from the propagation path with excess path lengths above it.…”
Section: Empirical Exponential Modelmentioning
confidence: 99%
“…The authors in [18] address the non-stationarity of the channel by accounting, among others, for the probabilistic presence and movement of clusters of scatterers. Based on their work in [19] and [20] for V2V and A2A channels, respectively, Walter et al proposed in [21] a general way of analytically deriving the delay-dependent and joint delay Doppler probability density functions (pdfs) of M2M channels. The approach is based on defining an infinite arbitrarily-oriented scattering plane where the effective scatterers are located.…”
Section: Introductionmentioning
confidence: 99%
“…This, together with the demonstration that the time-variant squared delay/Dopplerspread function remains proportional to the time-variant joint delay Doppler pdf [22], allows for an analytical description of the time-variant channel in any 3D M2M scenario where the scatterers can be considered to be uniformly distributed over a plane. The potential of such an approach has already been shown with measurement data in V2V [23]- [25] and A2A [26], [27] scenarios. However, the technique proposed in [21] has two key constraints: the scatterers can only be assumed to be distributed over a single plane, which must also be infinite.…”
Section: Introductionmentioning
confidence: 99%