Principio: [ de súper-conducción de electrones coherentes ]
H(x,y,t) = int-int[ sin(ut)·f(ax)·d[ut]-[&]-d[ax]+cos(ut)·g(ay)·d[ut]-[&]-d[ay] ]
T·( (-1)·cos(ut)·F(ax)+sin(ut)·G(ay) [o] H(x,y,t) ) = T+(-1)·T_{0}
Principio: [ de súper-conducción de gravitones coherentes ]
H(x,y,t) = int-int[ sinh(ut)·f(ax)·d[ut]-[&]-d[ax]+(1/i)·cosh(ut)·g(ay)·d[ut]-[&]-d[ay] ]
T·( cosh(ut)·F(ax)+(1/i)·sinh(ut)·G(ay) [o] H(x,y,t) ) = T+(-1)·T_{0}
Principio: [ de láser de fotones eléctricos coherentes ]
H(x,y,t) = int-int[ e^{uti}·f(ax)·d[uti]-[&]-d[ax]+e^{(-1)·uti}·g(ay)·d[uti]-[&]-d[ay] ]
z·( e^{uti}·F(ax)+(-1)·e^{(-1)·uti}·G(ay) [o] H(x,y,t) ) = z+(-1)·z_{0}
Principio: [ de láser de fotones gravitatorios coherentes ]
H(x,y,t) = int-int[ e^{ut}·f(ax)·d[ut]-[&]-d[ax]+e^{(-1)·ut}·g(ay)·d[ut]-[&]-d[ay] ]
z·( e^{ut}·F(ax)+(-1)·e^{(-1)·ut}·G(ay) [o] H(x,y,t) ) = z+(-1)·z_{0}
Principio: [ de estabilizador de carga de electrones ]
H(x,y,t) = int-int[ sin(ut)·f(ax)·d[ut]-[ || ]-d[ax]+cos(ut)·g(ay)·d[ut]-[ || ]-d[ay] ]
q·( (-1)·cos(ut)·F(ax)+sin(ut)·G(ay) [o] H(x,y,t) ) = 2q+(-1)·q_{0}
H(x,y,t) = (-1)·cos(ut)·(1/F(ax))+sin(ut)·(1/G(ay))
Principio: [ de estabilizador de carga de gravitones ]
H(x,y,t) = int-int[ sinh(ut)·f(ax)·d[ut]-[ || ]-d[ax]+(1/i)·cosh(ut)·g(ay)·d[ut]-[ || ]-d[ay] ]
p·( cosh(ut)·F(ax)+(1/i)·sinh(ut)·G(ay) [o] H(x,y,t) ) = 2p+(-1)·p_{0}
H(x,y,t) = cosh(ut)·(1/F(ax))+(1/i)·sinh(ut)·(1/G(ay))
Anexo:
El estabilizador de conducción,
es un chip de diagonal-hipérbola y semi-círculo y hipérbola-diagonal.
Principio: [ de estabilizador de rotación de corriente eléctrico ]
H(x,y,t) = int-int[ sin(ut)·f(ax)·d[ut]-[ || ]-d[ax]+cos(ut)·g(ay)·d[ut]-[ || ]-d[ay] ]
v·( (-1)·cos(ut)·F(ax)+sin(ut)·G(ay) [o] H(x,y,t) ) = 2v+(-1)·v_{0}
H(x,y,t) = (-1)·cos(ut)·(1/F(ax))+sin(ut)·(1/G(ay))
Principio: [ de estabilizador de rotación de corriente gravitatorio ]
H(x,y,t) = int-int[ sinh(ut)·f(ax)·d[ut]-[ || ]-d[ax]+(1/i)·cosh(ut)·g(ay)·d[ut]-[ || ]-d[ay] ]
v·( cosh(ut)·F(ax)+(1/i)·sinh(ut)·G(ay) [o] H(x,y,t) ) = 2v+(-1)·v_{0}
H(x,y,t) = cosh(ut)·(1/F(ax))+(1/i)·sinh(ut)·(1/G(ay))
Anexo:
El estabilizador de rotación,
es un mecanismo donde circula un corriente,
de diagonal-hipérbola y semi-circulo y hipérbola-diagonal.
Teorema:
int-int[ z^{2n+(-1)}·d[y]-[&]-d[z]+z^{2n+(-1)}·d[z]-[&]-d[x]+(-1)·d[x]-[&]-d[y] ] = ...
... nx+ny+z^{2n}
Teorema:
int-int[ e^{2nz}·d[y]-[&]-d[z]+e^{2nz}·d[z]-[&]-d[x]+(-1)·d[x]-[&]-d[y] ] = ...
... nx+ny+e^{2nz}
Teorema:
int-int[ z^{3n+(-1)}·d[y]-[ || ]-d[z]+x^{3n+(-1)}·d[z]-[ || ]-d[x]+y^{3n+(-1)}·d[x]-[ || ]-d[y] ] = ...
... (1/z)^{3n}·(n/y)+(1/x)^{3n}·(n/z)+(1/y)^{3n}·(n/x)
Teorema:
int-int[ e^{3nz}·d[y]-[ || ]-d[z]+e^{3nx}·d[z]-[ || ]-d[x]+e^{3ny}·d[x]-[ || ]-d[y] ] = ...
... e^{(-3)·nz}·(n/y)+e^{(-3)·nx}·(n/z)+e^{(-3)·ny}·(n/x)
Teorema:
Sea d_{tt}^{2}[x_{k}]+H_{ij}^{k}·d_{t}[x_{i}]·d_{t}[x_{j}] = 0 ==>
Si H_{kk}^{k} = d_{t}[f_{k}(t)] ==> x_{k}(t) = ( t /o(t)o/ int[ f_{k}(t) ]d[t] )
H_{ij}^{k} = ( 1/f_{k}(t) )^{2}·d_{t}[f_{k}(t)]·f_{i}(t)·f_{j}(t)
Teorema:
Sea d_{tt}^{2}[x_{k}]+H_{ij}^{k}·d_{t}[x_{i}]·d_{t}[x_{j}] = 0 ==>
Si H_{kk}^{k} = k ==> x_{k}(t) = (1/k)·ln(t)
H_{ij}^{k} = (1/k)·ij
Teorema:
Sea d_{tt}^{2}[x_{k}]+H_{ij}^{k}·d_{t}[x_{i}]·d_{t}[x_{j}] = 0 ==>
Si H_{kk}^{k} = e^{kt} ==> x_{k}(t) = (-1)·e^{(-1)·kt}
H_{ij}^{k} = k^{2}·e^{(-1)·kt}·(1/(ij))·e^{it+jt}
