# Chiral theories and matter gauges

1. Feb 18, 2009

### sirchasm

Is it true that classical theories tend to treat matter 'in the limit' of large N, or it encodes matter in $$N_A$$ as $$N_A(m_e,e)$$ say, and chiral theories need to include $$\hbar$$ which classicality sees as $$\{G(h),c\}$$?

We use 'mass-free' theories that treat charge and spin momentum in circuits = manifolds with linear/nonlinear operators.
Algebraically these manifolds can operate at linear (<<nonlinear) limits that treat charge algebraically and do not rotate spin or they operate in a N(e + s) domain that keeps N(s) at 0.

We need theories that include a mass-spin term?

2. Feb 20, 2009

### sirchasm

that N(e + s) thing should be able to explain how N gauges charge e (in my notation), and spin-potential s, in a mass-free index; When we use much smaller N than $$N_A\,$$ of charge and spin,we see distributed phase momenta = discrete products.

We haven't been able to connect the enumerable side of Avogadro's number to the way spin and charge evolve over the 'mass-field', or extend algebraically.