Lie superalgebras extend Lie algebras by incorporating both bosonic and fermionic elements. This powerful mathematical framework unifies the description of particles with different spins, providing a foundation for supersymmetry in physics.
Supersymmetry, a key application of Lie superalgebras, proposes a symmetry between bosons and fermions. This concept has far-reaching implications in particle physics and quantum field theory, potentially addressing fundamental questions about the nature of our universe.
Z2-grading in Lie superalgebras
Definition and properties of Z2-grading
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A Class of Lie 2-Algebras in Higher-Order Courant Algebroids View original
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Frontier Orbitals, Combustion and Redox Transfer from a Fermionic-Bosonic Orbital Perspective View original
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Construction of bosonic symmetry-protected-trivial states and their topological terms via $G ... View original
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A Class of Lie 2-Algebras in Higher-Order Courant Algebroids View original
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A is a vector space g=g0⊕g1
g0 represents the even part (bosonic)
g1 represents the odd part (fermionic)
The Z2-grading is compatible with the Lie bracket [gi,gj]⊆gi+j (mod 2) for i,j∈{0,1}
Ensures the closure of the Lie bracket within the superalgebra
Elements in g0 are called even (bosonic) elements, while elements in g1 are called odd (fermionic) elements
Bosonic elements follow commutation relations (like in ordinary Lie algebras)
Fermionic elements follow anticommutation relations
Graded versions of anticommutativity and Jacobi identity
The Lie bracket in a Lie superalgebra satisfies graded versions of anticommutativity and the Jacobi identity
Graded anticommutativity: [x,y]=−(−1)∣x∣∣y∣[y,x]
∣x∣ and ∣y∣ represent the Z2-grading of elements x and y (0 for even, 1 for odd)
Reduces to ordinary anticommutativity for even elements and commutation for odd elements