unitary tensor
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2019 ◽  
Vol 21 (7) ◽  
pp. 073059 ◽  
Author(s):  
Ding Liu ◽  
Shi-Ju Ran ◽  
Peter Wittek ◽  
Cheng Peng ◽  
Raul Blázquez García ◽  
...  

Author(s):  
Stephan Haefner ◽  
Reiner Thomä

Estimating the parameters of a geometric propagation model from MIMO channel sounding measurements will be considered, which requires the solution of an inverse problem. Thus, a model of the measured data is derived, which incorporates a model of the measurement system as well as the parameters of interest. Based on the data model a maximum-likelihood estimator will be derived to infer the model parameters. Because virtual antenna arrays are considerer, formed by step-wise rotating directive antennas at transmitter and receiver side, the MIMO measurements are conducted in the beam-space. Hence, the data model can be described by a multidimensional convolution of the measurement system and the propagation channel. Based on the convolutional modelling, the parameter estimation problem is transformed into a harmonic retrieval problem, which can be solved by an Unitary Tensor-ESPRIT algorithm. The maximum-likelihood and ESPRIT estimator are compared by Monte-Carlo simulations according to their root-mean-square estimation error.


2017 ◽  
Vol 222 (1) ◽  
pp. 223-260 ◽  
Author(s):  
Ada Boralevi ◽  
Jan Draisma ◽  
Emil Horobeţ ◽  
Elina Robeva

2012 ◽  
Vol 85 (16) ◽  
Author(s):  
Andrew J. Ferris ◽  
Guifre Vidal

1. The symmetry breaking interactions The fact that the meson or baryon states observed to have a particular spin-parity value appear grouped into unitary patterns of charge multiplets has made it apparent that the strong nuclear interactions satisfy SU 3 symmetry . At the same time, the large mass differences which exist between the charge multiplets constituting a given unitary multiplet show clearly that there also exist moderately strong interactions which do not have this symmetry, although they satisfy the SU 2 symmetry of charge independence and the gauge symmetry of hypercharge conservation. The simplest hypothesis possible for these symmetry breaking interactions is that they have the following unitary tensor form: L m . s . = λ T 3 3 .


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