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)
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)
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)
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)
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
u^{3}+(a+w)·u+b = 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
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
