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| − | <center><math>\textbf{\underline{Navigation}}</math> | + | <center><math>\underline{\textbf{Navigation}}</math> |
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| − | [[New_4-momentum_quantities|<math>\vartriangleleft </math>]] | + | [[4-momenta|<math>\vartriangleleft </math>]] |
| − | [[VanWasshenova_Thesis#Weighted_Isotropic_Distribution_in_Lab_Frame|<math>\triangle </math>]] | + | [[VanWasshenova_Thesis#Moller_Scattering|<math>\triangle </math>]] |
| − | [[4-vectors|<math>\vartriangleright </math>]] | + | [[S-Channel|<math>\vartriangleright </math>]] |
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| | </center> | | </center> |
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| − | ==s Channel==
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| − | The s quantity is known as the square of the center of mass energy (invariant mass)
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| − | <center><math>s \equiv \left({\mathbf P_1^*}+ {\mathbf P_2^{*}}\right)^2=\left({\mathbf P_1^{'*}}+ {\mathbf P_2^{'*}}\right)^2</math></center>
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| − | <center><math>s \equiv \left({\mathbf P_1^*}+ {\mathbf P_2^{*}}\right)^2</math></center>
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| − | <center><math>s \equiv \mathbf P_1^{*2}+2 \mathbf P_1^* \mathbf P_2^*+ \mathbf P_2^{*2}</math></center>
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| − | As shown earlier, the square of a 4-momentum is
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| − | <center><math>\mathbf P^{2} \equiv m^2</math></center>
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| − | <center><math>s \equiv m^{2}+2 \mathbf P_1^* \mathbf P_2^*+ m_2^{2}</math></center>
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| − | This gives
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| − | <center><math>s \equiv 2m^{2}+2 \mathbf P_1^* \mathbf P_2^*</math></center>
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| − | Similarly, the scalar product of two 4-momentums
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| − | <center><math>s \equiv 2m^2+2(E_1^*E_2^*-\vec p_1^* \vec p_2^*)</math></center>
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| − | In the center of mass frame of reference,
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| − | <center><math>E_1^*=E_2^* \quad and \quad \vec p_1^*=-\vec p_2^*</math></center>
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| − | <center><math>s \equiv 2m^2+2(E_1^{*2}+\vec p_1^{*2} )</math></center>
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| − | Using the relativistic energy equation
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| − | <center><math>E^2 \equiv p^2+m^2</math></center>
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| − | <center><math>s \equiv 2m^2+2((m^2+p_1^{*2})+p_1^{*2})</math></center>
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| − | <center><math>s=4(m_{CM}^2+p_{CM}^2)</math></center>
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| − | ==t Channel==
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| − | The t quantity is known as the square of the 4-momentum transfer
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| − | <center><math>t \equiv \left({\mathbf P_1^*}- {\mathbf P_1^{'*}}\right)^2=\left({\mathbf P_2^{*}}+ {\mathbf P_2^{'*}}\right)^2</math></center>
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| − | <center>[[File:400px-CMcopy.png]]</center>
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| − | <center><math>t \equiv \left({\mathbf P_1^*}- {\mathbf P_1^{'*}}\right)^2</math></center>
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| − | <center><math>t \equiv P_1^{*2}-2P_1^*P_1^{'*}+P_1^{'*2}</math></center>
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| − | <center><math>t \equiv 2m_1^2-2E_1^*E_1^{'*}+2p_1^*p_1^{'*}</math></center>
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| − | <center><math>t \equiv 2m_1^*-2E_1^{*2}+2p_1^{*2}cos\ \theta</math></center>
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| − | <center><math>t \equiv -2p_1^{*2}(1-cos\ \theta)</math></center>
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| − | ==u Channel==
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| − | <center><math>\textbf{\underline{Navigation}}</math> | + | <center><math>\underline{\textbf{Navigation}}</math> |
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| − | [[New_4-momentum_quantities|<math>\vartriangleleft </math>]] | + | [[4-momenta|<math>\vartriangleleft </math>]] |
| − | [[VanWasshenova_Thesis#Weighted_Isotropic_Distribution_in_Lab_Frame|<math>\triangle </math>]] | + | [[VanWasshenova_Thesis#Moller_Scattering|<math>\triangle </math>]] |
| − | [[4-vectors|<math>\vartriangleright </math>]] | + | [[S-Channel|<math>\vartriangleright </math>]] |
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| | </center> | | </center> |
