Hilbert Book Model Project/Slide S1

hbmp	Hilbert Book Model Project	S1
	In the The base modelᙜ a set of platforms float over the background parameter space These platforms carry a symmetry center ${\color {yellow}{\mathfrak {S}}_{n}^{x}}$, 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 ${\color {hotpink}\blacktriangle \blacktriangle \blacktriangle \blacktriangle }$ 0000 R N +0 neutrino ${\color {hotpink}\blacktriangle \blacktriangle \blacktriangle }{\color {cyan}\blacktriangledown }$ 0001 L R -1 down quark ${\color {hotpink}\blacktriangle \blacktriangle {\color {cyan}\blacktriangledown }\blacktriangle }$ 0010 R G -1 down quark ${\color {hotpink}\blacktriangle \blacktriangle }{\color {cyan}\blacktriangledown \blacktriangledown }$ 0011 L B -2 up quark ${\color {hotpink}\blacktriangle {\color {cyan}\blacktriangledown }\blacktriangle \blacktriangle }$ 0100 R B -1 down quark ${\color {hotpink}{\blacktriangle \color {cyan}\blacktriangledown }\blacktriangle {\color {cyan}\blacktriangledown }}$ 0101 L G -2 up quark ${\color {hotpink}\blacktriangle {\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }\blacktriangle }$ 0110 R R -2 up quark ${\color {hotpink}{\blacktriangle \color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }}$ 0111 L N -3 electron ${\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle \blacktriangle \blacktriangle }$ 1000 R N 0 A_neutrino ${\color {hotpink}{\color {cyan}\blacktriangledown }\blacktriangle \blacktriangle {\color {cyan}\blacktriangledown }}$ 1001 L R 1 A_down_quark ${\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle {\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle }}$ 1010 R G 1 A_down_ark ${\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }$ 1011 L B 2 A_ up quark ${\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle \blacktriangle }$ 1100 R B 1 A_down_quark ${\color {cyan}\blacktriangledown }{\color {hotpink}{\color {cyan}\blacktriangledown }\blacktriangle {\color {cyan}\blacktriangledown }}$ 1101 L G 2 A_ up quark ${\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {hotpink}\blacktriangle }$ 1110 R R 2 A_ up quark ${\color {hotpink}{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }{\color {cyan}\blacktriangledown }}$ 1111 L N 3 positron ${\color {gray}{\begin{cases}\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\end{cases}}}$ 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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