Difference between revisions of "DV Creating LUND Files"
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where E<sub>i</sub> and E<sub>f</sup> are the initial and final electron energies. | where E<sub>i</sub> and E<sub>f</sup> are the initial and final electron energies. | ||
+ | |||
+ | {| border=1 align=center | ||
+ | |+ LUND Header | ||
+ | |- | ||
+ | ! Column | ||
+ | ! Quantity | ||
+ | |- | ||
+ | | <center>1</center> | ||
+ | | <center>Index</center> | ||
+ | |- | ||
+ | |<center>2</center> | ||
+ | | <center>Charge</center> | ||
+ | |- | ||
+ | | <center>3</center> | ||
+ | | <center>'''Type (1 is active)'''</center> | ||
+ | |- | ||
+ | | <center>4</center> | ||
+ | | <center>'''Particle ID'''</center> | ||
+ | |- | ||
+ | | <center>5</center> | ||
+ | | <center>Parent Index</center> | ||
+ | |- | ||
+ | | <center>6</center> | ||
+ | | <center>Daughter Index</center> | ||
+ | |- | ||
+ | | <center>7</center> | ||
+ | | <center>'''Momentum x (GeV)'''</center> | ||
+ | |- | ||
+ | | <center>8</center> | ||
+ | | <center>'''Momentum y (GeV)'''</center> | ||
+ | |- | ||
+ | | <center>9</center> | ||
+ | | <center>'''Momentum z (GeV)'''</center> | ||
+ | |- | ||
+ | | <center>10</center> | ||
+ | | <center><math>E</math></center> | ||
+ | |- | ||
+ | | <center>11</center> | ||
+ | | <center>Mass</center> | ||
+ | |- | ||
+ | | <center>12</center> | ||
+ | | <center>'''Vertex x (cm)'''</center> | ||
+ | |- | ||
+ | | <center>13</center> | ||
+ | | <center>'''Vertex y (cm)'''</center> | ||
+ | |- | ||
+ | | <center>14</center> | ||
+ | | <center>'''Vertex z (cm)'''</center> | ||
+ | |} | ||
=Writing LUND files= | =Writing LUND files= | ||
=Correct for vertex location= | =Correct for vertex location= |
Revision as of 19:14, 29 March 2016
The LUND format
Column | Quantity |
---|---|
Where
1:Number of Particles
This line tells how many particles follow the header line. For Moller Scattering, this number should always be 2.
2:Number of Target Nucleons
For this simulation, only an electron-electron collision is considered. This quantity is always set to 1 for the one stationary electron we consider the incident electron scattering from.
3:Number of Target Protons
For Moller Scattering, there are no target protons. This number is set to 1, but does not have any effect within the GEMC simulations.
4:Target Polarization
This represents the polarization of the target material, either positive or negative 1. This value is always set to 1 and has no effect within the GEMC simulations.
5:Beam Polarization
This represents the polarization of the electron beam, either negative or positive 1. This value is always set to positive 1.
6:x
This represents the Bjorken x scaling variable.
Where M is the rest mass-energy of the proton
7:y
8:W
The invariant mass of the final hadronic system
9:
This represents the squared 4-momentum-transfer vector q of the exchanged virtual photon.
Where q is the momentum transfer betwwn the incident electron and target via the virtual photon.
10:
This represents the energy loss between scattering electrons.
This can be written in the Lab frame as:
where Ei and Ef are the initial and final electron energies.
Column | Quantity |
---|---|