eigenstates

An eigenvalue is the mathematical determination of an eigenvector. An eigenvector -- or an eigentensor (an eigenvector that has alterior directorals that work to represent the projection of an eluded to eigensate) is the actual physical mapping of an eigenstate that is mathematically determinied by the so stated given arbitrary eigenvalue. As this is true, an eigenstate refers to a specific physical phenomenon that may be represented in one manner or another as a wave -- whether such a wave is determined over a Laplacian-based mapping or whether the said wave is projected over time through either a unitary-based spatial medium or is propagated through any given arbitrary Lagrangian over time. Let us say that one is considering, here, a basic physical genus of phenomena -- such as the Rarita Structure. The Rarita Structure here represents that substringular field-like basis through which gravity -- via the Ricci Scalar -- is able to bear a physical interconnectivity with other phenomena so that gravity may be able to take into effect. An eigenstate of the Rarita Structure would then be a specific operational substrate in which the Rarita Structure is able to occur so that a specific relatively limited quantum of substringular phenomena may be able to be effected by a relatively limited quantum of gravitational-like particles. Any substringular phenomenon -- whether such phenomena are intrinsically considered as particle-nature-based, energy-nature-based, or wave-nature-based, may be, in one manner or another, be considered in part as wave-like in nature. The substringular is filled with analogous examples of this. I will continue with this later! Sam Roach.