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models:toy_models:sine_gordon [2018/03/24 15:08] jakobadmin [Student] |
models:toy_models:sine_gordon [2018/05/05 12:50] (current) jakobadmin ↷ Links adapted because of a move operation |
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- | ====== Sine-Gordon Model: $ \quad \mathcal{L} = \frac{1}{2} \left( (\partial_\mu \phi)^2 \right) - (1-cos \phi) $ ====== | + | <WRAP lag>$ \mathcal{L} = \frac{1}{2} \left( (\partial_\mu \phi)^2 \right) - (1-cos \phi) $</WRAP> |
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- | <tabbox Why is it interesting?> | + | |
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- | The Sine-Gordon model is a toy model that helps to understand fundamental notions like [[advanced_notions:quantum_field_theory:duality|duality]] in a simplified setup. | + | |
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- | In addition, the equations of the theory permit topological non-trivial solutions called solitons. Many basic features of such solitons can be studied in the Sine-Gordon model in a simplified setup. | + | |
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- | The name "Sine-Gordon model" is a wordplay, because the equation of motion of the model is similar to the famous [[equations:klein-gordon_equation|Klein-Gordon equation]] and contains a [[basic_tools:trigonometric_functions|sinus function]]. | + | |
+ | ====== Sine-Gordon Model ====== | ||
- | <tabbox Layman> | + | <tabbox Intuitive> |
The Sine-Gordon model describes a coupled set of pendulums that hang from a common support rod. | The Sine-Gordon model describes a coupled set of pendulums that hang from a common support rod. | ||
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- | <tabbox Student> | + | <tabbox Concrete> |
**Specification of the Model** | **Specification of the Model** | ||
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- | <tabbox Researcher> | + | <tabbox Abstract> |
- | The Sine-Gordon model is [[advanced_notions:quantum_field_theory:duality|dual]] to the massive Thirring model. | + | The Sine-Gordon model is [[advanced_notions:duality|dual]] to the massive Thirring model. |
This is surprising since the Sine-Gordon model is a purely scalar theory, while the massive Thirring model is a purely fermionic theory. However, the solitons in the Sine-Gordon model are fermionic, while the solitons in the Thirring model are scalars. | This is surprising since the Sine-Gordon model is a purely scalar theory, while the massive Thirring model is a purely fermionic theory. However, the solitons in the Sine-Gordon model are fermionic, while the solitons in the Thirring model are scalars. | ||
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* Coleman, S. (1975). [[https://journals.aps.org/prd/abstract/10.1103/PhysRevD.11.2088|"Quantum sine-Gordon equation as the massive Thirring model"]]. Physical Review D. 11 (8): 2088. | * Coleman, S. (1975). [[https://journals.aps.org/prd/abstract/10.1103/PhysRevD.11.2088|"Quantum sine-Gordon equation as the massive Thirring model"]]. Physical Review D. 11 (8): 2088. | ||
+ | <tabbox Why is it interesting?> | ||
+ | The Sine-Gordon model is a toy model that helps to understand fundamental notions like [[advanced_notions:duality|duality]] in a simplified setup. | ||
+ | |||
+ | |||
+ | In addition, the equations of the theory permit topological non-trivial solutions called solitons. Many basic features of such solitons can be studied in the Sine-Gordon model in a simplified setup. | ||
+ | |||
+ | |||
+ | |||
+ | The name "Sine-Gordon model" is a wordplay, because the equation of motion of the model is similar to the famous [[equations:klein-gordon_equation|Klein-Gordon equation]] and contains a [[basic_tools:trigonometric_functions|sinus function]]. | ||
- | <tabbox FAQ> | ||
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<tabbox History> | <tabbox History> | ||
The Sine-Gordon equation was originally | The Sine-Gordon equation was originally |