Defining Group Multiplication in Particle Physics

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In particle physics, the multiplication of groups like SU(2) and U(1) is defined through the concept of direct products rather than traditional multiplication. The direct product G x H consists of all pairs (g, h) with g in G and h in H, using the natural composition (g, h)(g', h') = (gg', hh'). Additionally, the direct sum notation \bigoplus_{i=1}^n G_i represents a Cartesian product of groups G_i, structured by defining a binary operation similar to the direct product. This framework is essential for understanding how different groups interact and combine in the context of particle physics. Understanding these definitions is crucial for grasping the underlying mathematics of gauge theories.
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Everyone must be familiar with U(1),SU(2) and SU(3) Lie groups in particle physics .
But how does one define the multiplication of two groups of different dimensions
aka SU(2) X U(1) or SU(3) X SU(2) X U(1).
 
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You aren't multiplying them. That is the direct product of the groups. Give two groups the direct product GxH is the set of all pairs (g,h) g in G, h in H with the natural composition

(g,h)(g',h')=(gg',hh')
 
It's also the direct sum. If ever you encounter the notation \bigoplus_{i=1}^n G_i, this is what it means. Take the cartesian product of the G_i and give them a group structure by defining the binary operation as in matt grime's post. (g1,...,gn)(g1',...,gn'1)=(g1g1',...,gngn')
 
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