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In the case of SU(3), the weight of the fundamental representation can be a bit more involved compared to SU(2), as SU(3) is a larger group with more complex representations. The fundamental representation of SU(3) is often denoted as \((1,0)\). It corresponds to the triplet representation, which is commonly used in particle physics to describe the properties of quarks, which are the fundamental constituents of protons, neutrons, and other hadrons. In SU(3), the representations are labeled by two integers \( (p,q) \), where \( p \) and \( q \) are the numbers of boxes in the first and second rows of the Young diagram, respectively. The fundamental representation \((1,0)\) corresponds to a single box in the first row and no boxes in the second row. Each weight of the fundamental representation corresponds to a combination of charges under the group's generators. The weight diagram of the fundamental representation of SU(3) consists of three points arranged at the vertices of an equilateral triangle. These points correspond to the three fundamental weights of SU(3), which can be expressed in terms of the group's generators. In summary, the weight of the fundamental representation of SU(3) is represented by the triplet \((1,0)\), and it encompasses the properties of quarks under the SU(3) symmetry of the strong interaction. #SU(3), #representation theory, #fundamental representation, #quarks, #particle physics #Group theory, #Lie groups, #Quantum chromodynamics (QCD), #Particle properties, #Quantum field theory (QFT), #Symmetry breaking, #Young diagrams, #Particle interactions, #Standard model What: Fundamental representation, SU(3), Group theory Why: Representation theory, Particle physics, Symmetry When: Particle physics research, Representation theory development Where: Particle accelerators, Theoretical physics research centers Who: Physicists, Mathematicians, Researchers How: Representation decomposition, Particle property prediction, Quantum field theory applications