theorems:fabri-picasso
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theorems:fabri-picasso [2017/12/04 08:01] 127.0.0.1 external edit |
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| ====== Fabri-Picasso Theorem====== | ====== Fabri-Picasso Theorem====== | ||
| - | <tabbox Why is it interesting?> | ||
| - | <tabbox Layman> | + | |
| + | <tabbox Intuitive> | ||
| <note tip> | <note tip> | ||
| Explanations in this section should contain no formulas, but instead colloquial things like you would hear them during a coffee break or at a cocktail party. | Explanations in this section should contain no formulas, but instead colloquial things like you would hear them during a coffee break or at a cocktail party. | ||
| </note> | </note> | ||
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| - | <tabbox Student> | + | <tabbox Concrete> |
| Fabri and Picasso showed in 1966 that if the vacuum state $|0\rangle$ is invariant under translations, it follows that the vacuum state is invariant under the internal symmetry or there is no state corresponding to $\hat Q |0\rangle$ in the Hilbert space of the theory. ($\hat Q $ is the Noether charge that corresponds to the internal symmetry.) | Fabri and Picasso showed in 1966 that if the vacuum state $|0\rangle$ is invariant under translations, it follows that the vacuum state is invariant under the internal symmetry or there is no state corresponding to $\hat Q |0\rangle$ in the Hilbert space of the theory. ($\hat Q $ is the Noether charge that corresponds to the internal symmetry.) | ||
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| <cite>http://publish.uwo.ca/~csmeenk2/files/HiggsMechanism.pdf</cite></blockquote> | <cite>http://publish.uwo.ca/~csmeenk2/files/HiggsMechanism.pdf</cite></blockquote> | ||
| - | <tabbox Researcher> | + | <tabbox Abstract> |
| <note tip> | <note tip> | ||
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| - | <tabbox Examples> | + | <tabbox Why is it interesting?> |
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| - | --> Example1# | + | |
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| - | <-- | + | |
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| - | --> Example2:# | + | |
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| - | <-- | + | |
| <tabbox FAQ> | <tabbox FAQ> | ||
theorems/fabri-picasso.1512370870.txt.gz · Last modified: 2017/12/04 07:01 (external edit)
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