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Published byRandall Wilcox Modified over 9 years ago
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U(1) Abelian Symmetry The Lagrangian is invariant under the phase transformation of the field operator: invariant
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If A,B,C become complex, they carry charges!
The interaction is invariant only if U(1) symmetry is related to charge conservation!
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The Dirac Fermion Lagrangian is also invariant under U(1)
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SU(N) Non-Abelian Symmetry
Assume there are N kinds of fields If they are similar, we have a SU(N) symmetry! are invariant under SU(N)!
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量子力學下互換群卻變得更大! 量子力學容許量子態的疊加 u a u + b d u d d c u + d d 古典 量子 u-d 互換對稱
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They are invariant under SU(N)!
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Gauge symmetry
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Global Symmetry Gauge (Local) symmetry Kinetic energy is not invariant under gauge transformation!
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Could we find a new “derivative” that works as if the transformation is global?
To get rid of the extra term, we introduce a new vector field:
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Global Symmetry Gauge (Local) symmetry Replacing derivative with covariant derivative, is invariant under gauge transformation!
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The scalar photon interaction vertices
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To force it to be gauge invariant,
you only need to replace derivative with coariant derivative. is gauge invariant!
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This gauge invariant Lagrangian gives a definite interaction between fermions and photons
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This form is forced upon us by gauge symmetry!
It is really a Fearful Symmetry! Tony Zee Tyger! Tyger! burning bright In the forests of the night What immortal hand or eye Could frame thy fearful symmetry! William Blake
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Let there be light! In the name of gauge symmetry!
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Hermann Weyl,
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Yang and Mills
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SU(N) Non-Abelian Symmetry
Assume there are N kinds of fields If they are similar, we have a SU(N) symmetry! are invariant under SU(N)!
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Non-Abelian Gauge Symmetry
We need one gauge field for each generator. Gauge fields transform as: is invariant under gauge transformation!
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2 × 2 matrices
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Vacua happen at: Choose: For infinitesimal transformation: SU(2)χU(1)Y is broken into U(1)EM
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Z become massive W become massive Photon is massless.
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