Part One of the Second Session of Course 17 About the Ricci Scalar

To start, as I have said before, both matter, electromagnetic energy, plain kinetic energy, and entropic photons are forms of energy.  So, both matter, electromagnetic energy, plain kinetic energy, and entropic photons are different forms of the same thing -- that bear different conditions of interaction, that appertain to a tense of having a capacity of being able to be converted into being of the same general format of holonomic substrate.  Energy -- as a general concept of phenomenology -- is a disturbance that occurs in a medium.  A medium, here, being a given arbitrary operand in which a given arbitrary operator is acted upon within.  Also, what I mean by a disturbance is an activity that is to happen over a discrete period of time  -- in which the so-eluded-to medium is existent, in order for the so-stated disturbance to be able to occur.  So, when any given arbitrary activity happens in any given arbitrary region in any given arbitrary discrete period of time -- in what I term of as the globally distinguishable, then, one is then to have here a disturbance in a medium.  So -- in the substringular -- any given arbitrary Hamiltonian operator that is to function in any given arbitrary Hamiltonian operand over a discrete period of time, works to comply to the condition of an activity that happens in a region,that happens in a sequential series of iterations of instanton, or, in other  words, this works to comply to the condition of a disturbance that is then here occurring in a medium.  This is the case of all general phenomenology that would here work to describe any format or genus of energy -- when one is to here consider the kinematic display of any given arbitrary form of energy.  All of such so-stated disturbances are alterations in any given arbitrary directly corresponding respective field of the so-eluded to given arbitrary directly corresponding medium.  What I mean by an alteration here, is a perturbation in the delineations of those field indices -- that would here appertain to a kinematic change in the distribution-based indices -- that are here associated with a directly corresponding respective eigenset of delineation-based eigenmembers -- as such Hodge-based eigenmembers are "shuffled" in one respect or another, over a discrete period of time.  More specifically, such so-eluded-to eigenmemebers would here specifically mean discrete superstrings of any given directly appertaining eigenbasis  -- that are projected kinematically from one genus of delineation-based distribution to another, over a discrete period of time.  So, when one has any given arbitrary set of superstrings -- that are redelineatd over a successive series of group instanton -- then, such an eigenbasis of redistribution may be determinable as a tense of activity, that may be then termed of as one format or another of what we would call energy.  To keep it simple, the superstrings of any given arbitrary case in tact would be considered to be the given arbitrary Hamiltonian operators.  The activity of the so-stated superstrings would then be the given arbitrary Hamiltonian operation.  So, the regions in which such Hamiltonian operations are occurring would then be considered to be the directly corresponding given arbitrary Hamiltonian operands. The general tense of gauge-metric that would then be directly associated with such a general genus of operation, would then here be based upon any directly related sequential series of covariant, codeterminable, and codifferentiable instantons -- of which would here be described of as group instantons ( in terms of their iterations and reiterations, that would here be more directly appertaining to the interdependence of all unfrayed superstrings -- as such superstrings of discrete energy permittivty are displaced and redisplaced over what we term of as time.)  More speicifically, the superstrings -- of which I mentioned of as Hamiltonian operators -- are the phenomenology of discrete energy permittivty.  Their directly corresponding Fadeev-Popove-Trace eigenstates are the directly related respective units of discrete energy impedance.  The directly corresponding counterstrings are the eigenbase of phenomenology that directly appertains to the basis of the wave-function of discrete energy permittivity.  And, the directly corresponding first-ordered light-cone-gauge eigenstates would here work to act as the basis of the wave-function of discrete energy impedance.  Let us just absorb that for now!  On to the second part of this session later!  To Be Continued!!  Sincerely, Sam Roach.