mecanismo-de-Gauge y álgebra

Ley:

Sea m·d_{tt}^{2}[z] = pE_{e}(z,q) ==>

Si q = 0 ==> p = m

Ley:

Sea m·d_{tt}^{2}[z] = pE_{g}(z,q) ==>

Si q = 0 ==> p = m

Electro-débil de leptones orbitales:

Ley:

F(t)·G(t) = e^{(1/m)·(q+(-W))}·e^{(1/m)·(W+(-q))}·f(t)·g(t)

d_{t}[F(t)]·d_{t}[G(t)] = ...

... d_{t}[f(t)]·d_{t}[g(t)]+(1/m)^{2}·d_{t}[q+(-W)]·d_{t}[W+(-q)]·f(t)·g(t)

Ley:

Sea A(x,y) = (1/m)·< x,y > ==>

F(x,y)·G(x,y) = e^{ Anti-Potencial[ A(x,y)·a^{2}·< q+(-W),W+(-q) > ] }·f(x,y)·g(x,y)

d_{y}[F(x,y)]·d_{x}[G(x,y)] = ...

... d_{y}[f(x,y)]·d_{x}[g(x,y)]+( A_{x}·A_{y} )·a^{4}·(q+(-W))·(W+(-q))·f(x,y)·g(x,y)

Deducción:

F(x,y) = e^{ int[ A_{x}·a^{2}·(q+(-W)) ]d[y] }·f(x,y)

G(x,y) = e^{ int[ A_{y}·a^{2}·(W+(-q)) ]d[x] }·g(x,y)

Ley:

d_{y}[F(x,y)]·d_{x}[G(x,y)] = 0 <==> ...

f(x,y) = e^{ int[ ia^{2}·A_{x}·(q+(-W)) ]d[y] }

g(x,y) = e^{ int[ ia^{2}·A_{y}·(W+(-q)) ]d[x] }

Ley:

Sea A(y,x) = (1/m)·< y,x > ==>

F(x,y)·G(x,y) = e^{ Potencial[ A(y,x)·a^{2}·< q+(-W),W+(-q) > ] }·f(x,y)·g(x,y)

d_{x}[F(x,y)]·d_{y}[G(x,y)] = ...

... d_{x}[f(x,y)]·d_{y}[g(x,y)]+( A_{y}·A_{x} )·a^{4}·(q+(-W))·(W+(-q))·f(x,y)·g(x,y)

Deducción:

F(x,y) = e^{ int[ A_{y}·a^{2}·(q+(-W)) ]d[x] }·f(x,y)

G(x,y) = e^{ int[ A_{x}·a^{2}·(W+(-q)) ]d[y] }·g(x,y)

Gravito-débil de leptones orbitales:

Ley:

F(t)·G(t) = e^{(1/m)·(p+(-Z))}·e^{(1/m)·(Z+(-p))}·f(t)·g(t)

d_{t}[F(t)]·d_{t}[G(t)] = ...

... d_{t}[f(t)]·d_{t}[g(t)]+(1/m)^{2}·d_{t}[p+(-Z)]·d_{t}[Z+(-p)]·f(t)·g(t)

Ley:

Sea A(x,y) = (1/m)·< x,y > ==>

F(x,y)·G(x,y) = e^{ Anti-Potencial[ A(x,y)·a^{2}·< p+(-Z),Z+(-p) > ] }·f(x,y)·g(x,y)

d_{y}[F(x,y)]·d_{x}[G(x,y)] = ...

... d_{y}[f(x,y)]·d_{x}[g(x,y)]+( A_{x}·A_{y} )·a^{4}·(p+(-Z))·(Z+(-p))·f(x,y)·g(x,y)

Ley:

Sea A(y,x) = (1/m)·< y,x > ==>

F(x,y)·G(x,y) = e^{ Potencial[ A(y,x)·a^{2}·< p+(-Z),Z+(-p) > ] }·f(x,y)·g(x,y)

d_{x}[F(x,y)]·d_{y}[G(x,y)] = ...

... d_{x}[f(x,y)]·d_{y}[g(x,y)]+( A_{y}·A_{x} )·a^{4}·(p+(-Z))·(Z+(-p))·f(x,y)·g(x,y)

Desintegración alfa:

Ley:

F(t)·G(t) = e^{(1/m)·(n·(q+(-q))+W+(-q))}·e^{(1/m)·(q+(-W))}·f(t)·g(t)

d_{t}[F(t)]·d_{t}[G(t)] = ...

... d_{t}[f(t)]·d_{t}[g(t)]+(1/m)^{2}·d_{t}[n·(q+(-q))+W+(-q)]·d_{t}[q+(-W)]·f(t)·g(t)

Ley:

Sea A(x,y) = (1/m)·< x,y > ==>

F(x,y)·G(x,y) = e^{ Anti-Potencial[ A(x,y)·a^{2}·< n·(q+(-q))+W+(-q),q+(-W) > ] }·f(x,y)·g(x,y)

d_{y}[F(x,y)]·d_{x}[G(x,y)] = ...

... d_{y}[f(x,y)]·d_{x}[g(x,y)]+( A_{x}·A_{y} )·a^{4}·(n·(q+(-q))+W+(-q))·(q+(-W))·f(x,y)·g(x,y)

Desintegración beta:

Ley:

F(t)·G(t) = e^{(1/m)·(n·(q+(-q))+q+(-W))}·e^{(1/m)·(W+(-q))}·f(t)·g(t)

d_{t}[F(t)]·d_{t}[G(t)] = ...

... d_{t}[f(t)]·d_{t}[g(t)]+(1/m)^{2}·d_{t}[n·(q+(-q))+q+(-W)]·d_{t}[W+(-q)]·f(t)·g(t)

Ley:

Sea A(x,y) = (1/m)·< x,y > ==>

F(x,y)·G(x,y) = e^{ Anti-Potencial[ A(x,y)·a^{2}·< n·(q+(-q))+q+(-W),W+(-q) > ] }·f(x,y)·g(x,y)

d_{y}[F(x,y)]·d_{x}[G(x,y)] = ...

... d_{y}[f(x,y)]·d_{x}[g(x,y)]+( A_{x}·A_{y} )·a^{4}·(n·(q+(-q))+q+(-W))·(W+(-q))·f(x,y)·g(x,y)

Desintegración gamma:

Ley:

F(t)·G(t) = e^{(1/m)·n·(q+(-q))}·e^{(1/m)·(W+(-W))}·f(t)·g(t)

d_{t}[F(t)]·d_{t}[G(t)] = ...

... d_{t}[f(t)]·d_{t}[g(t)]+(1/m)^{2}·d_{t}[n·(q+(-q))]·d_{t}[W+(-W)]·f(t)·g(t)

Ley:

Sea A(x,y) = (1/m)·< x,y > ==>

F(x,y)·G(x,y) = e^{ Anti-Potencial[ A(x,y)·a^{2}·< n·(q+(-q)),W+(-W) > ] }·f(x,y)·g(x,y)

d_{y}[F(x,y)]·d_{x}[G(x,y)] = ...

... d_{y}[f(x,y)]·d_{x}[g(x,y)]+( A_{x}·A_{y} )·a^{4}·n·(q+(-q))·(W+(-W))·f(x,y)·g(x,y)

Anunchiare-po gaudium,

el exelentisimus et reberendisimus cardinale,

Jûanes Garriga,

q-este año habreti-po marchatered al Chelo.

20 añi de mi morti,

a 22 añi de la resurreczione de li morti meni 2 añi,

que sere-po de la ecuazione iguale a q-esto:

((-0)/0)+((-0)/0) = (-2)

Teorema:

x^{4}+ax^{2}+bx+c = 0 es resoluble

Demostración:

Sea x = u+iv ==>

(u+iv)^{4}+a·(u+iv)^{2}+b·(u+iv)+c = 0

(-6)·(uv)^{2}+2ai·(uv)+c = 0

uv = (1/(6i))·( (-a)+( a^{2}+(-1)·6c )^{(1/2)} ) ...

... || ...

uv = (1/(6i))·( (-a)+(-1)·( a^{2}+(-1)·6c )^{(1/2)} )

4i·(uv)·( u^{2}+(-1)·v^{2} ) = w·( u^{2}+(-1)·v^{2} )

w = (2/3)·( (-a)+( a^{2}+(-1)·6c )^{(1/2)} )

... || ...

w = (2/3)·( (-a)+(-1)·( a^{2}+(-1)·6c )^{(1/2)} )

u^{4}+(a+w)·u^{2}+bu = 0

v^{4}+(-1)·(a+w)·v^{2}+biv = 0

u^{3}+(a+w)·u+b = 0

v^{3}+(-1)·(a+w)·v+bi = 0

Teorema:

x^{6}+ax^{4}+bx^{3}+cx^{2}+dx+p = 0 es irresoluble

Demostración:

(-20)·i·(uv)^{3}+(-6)·a·(uv)^{2}+2ic·(uv)+p·(uv)^{0} = 0

F(uv) = vu = uv

El polinomio tiene 7 puntos fijos y es irresoluble

uv = (z+(-1)·(1/10i)·a)

h^{3}+ph+q = 0

uv = (1/10i)·a+( (1/2)·( (-h)+2i·(h+p)^{(1/2)} )

uv = (1/10i)·a+( (1/2)·( (-h)+(-1)·2i·(h+p)^{(1/2)} )

Teorema:

x^{6}+ax^{5}+bx^{3}+cx^{2}+dx+p = 0 es irresoluble

Demostración:

(-20)·i·(uv)^{3}+2ic·(uv)+p·(uv)^{0} = 0

F(uv) = vu = uv

El polinomio tiene 5 puntos fijos y es irresoluble