FTAAN, Session 8, First Test

1) What is the difference between an arbitrary gauge-metric , and a gauge-metric that is not a Gaussian metric.

2) Give an example of a plain Gaussian metric.

3) Give an example of a gauge-metric.

4) What is the difference between a Cevita condition and a Wess Zumino condition.

5) Describe how superstrings may be mapped out.

6) Describe how Cevita energy may change an orbifold eigenset.

7) Describe how gluons bind sub-atomic particles.

8) Describe how an orbifold eigenset that has Cevita conditions may change to have Wess Zumino conditions.

9) Describe the abelian nature of a photon as it is scattered.

FTAAN, Session 7

Superstrings may be hermitian or Chern-Simmons. Superstrings may be abelian or non-abelian. One-dimensional superstrings may be hermitian or Chern-Simmons. One-dimensional superstrings may be abelian or non-abelian. Two-dimensional superstrings may be hermitian or Cher-Simmons. Two-dimensional superstrings may be abelian or non-abelian. One-dimensional tachyonic supersrings and two-dimensional tachyonic superstrings are Mobiusly hermitian yet euclideanly Chern-Simmons. One-dimensional tachyonic superstrings are completely non-abelian as superstrings, even though this does not condsider the gauge conditions of the given superstrings. When eletromagnetic energy initially scatters upon a surface, the individual two-dimensional bosons that have just struck the given surface will temporarily become tachyonic. These tachyonic superstrings will be completely non-abelian while their gauge structure will be completely abelian. The two-dimensional superstrings will become completely non-abelian as the result of a spring-like action happening to the given superstrings that jiggles the superstrings not to shatter the topology of these superstrings. This jiggling acts as a "shock-absorber" that straightens the non-abelian nature of the gauge structure of the given electromagnetic energy to make the given gauge structure temporarily abelian. This happens because the inertia of the light-cone-gauge eigenstates when a ray of electromagnetic energy strikes a surface pulls into the given two-dimensional superstrings and Planck phenomenon related phenomena on account of the strong metric-gauge and gauge-metric that the light-cone-gauge has relative to the given two-dimensional superstrings and their Planck phenomenon related phenomena. This pull Mobiusly winds the two-dimensional superstrings to make these jiggle to prevent the Planck phenomenon related phenomena from breaking temporarily while also jiggling to help straighten the light-cone-gauge so that the gauge structure will become abelian. Whenever a one or a two-dimensional superstring becomes freshly tachyonic, or whenever a one or a two-dimensional freshly non tachyonic, the superstring given has Cevita conditions. Whenever a supersting remains topologically invariant between two consecutive iterations, the given superstring has Wess-Zumino conditions. Superstrings may be abelian or non-abelian due to the considered wave-tug upon the superstrings via mini-strings. A hermitian superstring tends to be abelian, while a swivel-shaped superstring tends to be non-abelian.

FTAAN, Session 6

A one-dimensional superstring has a topology. A one-dimensional superstring also iterates each time during the core of BRST. The topology of a one-dimensional superstring exists during each iteration. Yet, a one-dimensional superstring does not always remain as a one-dimensional superstring. Often, one-dimensional superstrings convert into two-dimensional superstrings and two-dimensional superstrings often convert into one-dimensional strings. One-dimensional superstrings often have a hermitian topology. When a one-dimensional superstring maintains a homotopological hermitian topology during consecutive iterations, then the given one-dimensional superstring is said to have Wess-Zumino conditions. When a one-dimensional superstring maintains the same topology during consecutive iterations,k then the given one-dimensional superstring is said to have Wess-Zumino conditions. The energy used to cause a superstring to go into Wess-Zumino conditions is said to be an Anti-Cevita energy. Such an energy is not an actual energy because it does not consist of Planck phenomenon related phenomena, so this energy is actually a gauge-metric that acts through a multiplicit substringular metric. This gauge-metric acts as a sub-energy that redistributes topological indices via mini-string differential wave-tugs that happen at the proper angles and with the proper quantum and with the proper metric-gauge quantums and with the appropriate abelian nature to allow a given one or two-dimensional superstring to go from a perturbative topological nature per iteration to a non-perturbative topological nature per iteration as these go from a swiveled oriented Chern-Simmons anharmonic condition per iteration to a hermitian harmonic condition per iteration. This nature of going from Cevita conditions to Wess-Zumino conditions during a series of iterations goes for both one and two-dimensional superstrings, since all two-dimensions since two-dimensional superstring always have a topology. Superstrings as a unit always have homotopy when not at the space-hole. The space-hole always happens right before instanton-quaternionic-field-impulse unless phenomena given goes into a black-hole.

FTAAN, Session 2

The Cevita conditions are the conditions of Cevita energy. Cevita energy is the perturbative energy of substringular states. So, Cevita conditions are the conditions of the perturbative energies of substringular states. Substringular states are the states of Planck phenomena related phenomena, the states of superstrings, the states of counterstrings, the states of cohomologies, and the states of singularities that bind the prior named types of states. Perturbation of substringular states is often short lived. When a perturbative substringular state is brought out of perturbation, the substringular state is brought into a Wess- Zumino condition via Anti-Cevita energy. Just as Cevita energy brings substringular phenomena into perturbation, Anti-Cevita energy brings substringular phenomena out of perturbation. Wess- Zumino conditions are the conditions of substringular phenomena that are not in perturbation. Anti-Cevita energy always produces a framework of certain Wess-Zumino conditions. Often, There are a certain amount of Cevita conditions and a certain amount of Wess-Zumino conditions that apply to an orbifold eigenset at the same time. A mass that is of a neutrino or of an electron is Yau-Exact per orbifold even though the particle itself tends to be perturbative at times. So, the conformal invariance of neutrinos and electrons has Wess-Zumino conditions because conformal invariance involves non-perturbations, and masses tend to be non-perturbative when their inertia is constant. Yet, as the neutrinos and electrons scatter upon something, the Yau-Exact characteristic becomes partially hermitian and perturbative with refference to the particles themselves, and their heat and entropy are non-hermitian and perturbative. Any mass has Kaluza-Klein topology to an extent (at least one orbifold). All Kaluza-Klein topology involves entropy because of the abelian nature of their light-cone-guage as a supplemental Dirac Hamiltonian. All entropy involves heat. Heat is generally displaced via convection because of the Gaussian norm conditions via mini-string of orbifold eigenbases through Real Reimmanian Fock supplementation. Thus, masses inertialwise tend to have a way of being Yau-Exact except for the entropy, heat, and plain energy that happen to exist as these alter differentiation-wise.