# Hilbert Book Model Project/Slide S1

hbmp Hilbert Book Model Project S1

In the The base model a set of platforms float over the background parameter space
These platforms carry a symmetry center ${\displaystyle {\color {yellow}{\mathfrak {S}}_{n}^{x}}}$, which represents a private parameter space

Each symmetry center owns a private sequencing, which determines its symmetry flavor

Symmetry Flavor

sequence binary R/L color charge SM type

${\displaystyle {\color {hotpink}\blacktriangle \blacktriangle \blacktriangle \blacktriangle }}$

0000 R N +0 neutrino

${\displaystyle {\color {hotpink}\blacktriangle \blacktriangle \blacktriangle }{\color {cyan}\blacktriangledown }}$

0001 L R -1 down quark

${\displaystyle {\color {hotpink}\blacktriangle \blacktriangle {\color {cyan}\blacktriangledown }\blacktriangle }}$

0010 R G -1 down quark

${\displaystyle {\color {hotpink}\blacktriangle \blacktriangle }{\color {cyan}\blacktriangledown \blacktriangledown }}$

0011 L B -2 up quark

${\displaystyle {\color {hotpink}\blacktriangle {\color {cyan}\blacktriangledown }\blacktriangle \blacktriangle }}$

0100 R B -1 down quark

${\displaystyle {\color {hotpink}{\blacktriangle \color {cyan}\blacktriangledown }\blacktriangle {\color {cyan}\blacktriangledown }}}$

0101 L G -2 up quark

${\displaystyle {\color {hotpink}\blacktriangle {\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }\blacktriangle }}$

0110 R R -2 up quark

${\displaystyle {\color {hotpink}{\blacktriangle \color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }}}$

0111 L N -3 electron

${\displaystyle {\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle \blacktriangle \blacktriangle }}$

1000 R N 0 A_neutrino

${\displaystyle {\color {hotpink}{\color {cyan}\blacktriangledown }\blacktriangle \blacktriangle {\color {cyan}\blacktriangledown }}}$

1001 L R 1 A_down_quark

${\displaystyle {\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle {\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle }}}$

1010 R G 1 A_down_ark

${\displaystyle {\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }}$

1011 L B 2 A_ up quark

${\displaystyle {\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle \blacktriangle }}$

1100 R B 1 A_down_quark

${\displaystyle {\color {cyan}\blacktriangledown }{\color {hotpink}{\color {cyan}\blacktriangledown }\blacktriangle {\color {cyan}\blacktriangledown }}}$

1101 L G 2 A_ up quark

${\displaystyle {\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle }}$

1110 R R 2 A_ up quark

${\displaystyle {\color {hotpink}{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }}}$

1111 L N 3 positron

${\displaystyle {\color {gray}{\begin{cases}\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\end{cases}}}}$

• The difference in sequencing symmetry between a floating parameter space
and the sequencing symmetry of the background parameter space
defines the symmetry flavor of the platform on which the floating parameter space resides

• The symmetry flavor determines its symmetry-related charge.

• The charge locates at the geometric center of the platform and it interacts
with a symmetry-related field.

• The symmetry-related charge combines electric charge and color charge.

• Color charge relates to the dimension in which anisotropy occurs.

• The electric charge follows from the number of the dimensions
in which the sequencing symmetries differ.

• Antiparticles show opposite charge.

• The electric charges can attract or repel other electric charges.

• For that reason, they also take part in the binding of modules.

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