Verification of Relativistic Components - Revision history

Vanwdani at 15:56, 4 February 2016

2016-02-04T15:56:22Z

2016-02-04T04:10:43Z

Theta in the CM Frame

2016-02-02T04:51:47Z

Momentum in the CM Frame

2016-02-02T04:48:20Z

Momentum in the CM Frame

2016-02-02T04:47:53Z

Momentum in the CM Frame

2016-02-02T04:42:56Z

Momentum in the CM Frame

2016-02-02T04:41:18Z

Momentum in the CM Frame

2016-02-02T04:40:50Z

Momentum in the CM Frame

2016-02-02T04:32:02Z

Momentum in the CM Frame

2016-02-02T04:25:16Z

Momentum in the CM Frame

@@ Line 15: / Line 15: @@
 <center>[[File:FnlTheta_reverse.png]][[File:MolTheta_reverse.png]]</center>
 =Momentum in the CM Frame=
@@ Line 74: / Line 76: @@
 <center>[[File:Screen_Shot_2016-02-01_at_9.29.40_PM.png]]</center>
-=Theta in the CM Frame=
 =Conclusion=
 The energy loss must be dealt with by using both momentum components from a GEANT Moller Scattering data file.  By using both components, they can be transformed to a CM Frame, then have the phi angle varied to cover 2π radians.  A quick awk search shows that there are no Moller electrons with energy over 5500 MeV.  This might be able to be fixed by switching the scattered electron with the Moller electron, allowing a larger range of energy to be covered.

← Older revision		Revision as of 04:10, 4 February 2016
Line 76:		Line 76:
	=Theta in the CM Frame=		=Theta in the CM Frame=
	<center>[[File:FnlThetaCM_reverse.png]][[File:MolThetaCM_reverse.png]]</center>		<center>[[File:FnlThetaCM_reverse.png]][[File:MolThetaCM_reverse.png]]</center>
		+
		+	=Conclusion=
		+
		+	The energy loss must be dealt with by using both momentum components from a GEANT Moller Scattering data file. By using both components, they can be transformed to a CM Frame, then have the phi angle varied to cover 2π radians. A quick awk search shows that there are no Moller electrons with energy over 5500 MeV. This might be able to be fixed by switching the scattered electron with the Moller electron, allowing a larger range of energy to be covered.

@@ Line 67: / Line 67: @@
 |}
-The particles start out with p=11000.511 GeV and have on average ~11000 GeV by the time they interact
+The particles start out with p=11000.511 MeV and have on average ~11000 MeV by the time they interact
 <center>[[File:Screen_Shot_2016-02-01_at_9.30.23_PM.png]]</center>

@@ Line 67: / Line 67: @@
 |}
-The particles start out with p=11000.511 GeV and have on average 11000 GeV by the time they interact
+The particles start out with p=11000.511 GeV and have on average ~11000 GeV by the time they interact
 <center>[[File:Screen_Shot_2016-02-01_at_9.30.23_PM.png]]</center>

@@ Line 51: / Line 51: @@
 | 0
 | -510
-| 10999.1
+| 10931.3
-| 0.433025
+| -7.51848
-| -0.858867
+| -3.62463
-| 10999.6
+| 10931.8
 | 0
 | 0
-| -509.276
+| -509.361
-| 0.905324
+| 68.5938
-| -0.433025
+| 7.51848
-| 0.858867
+| 3.62463
-| 0.905366
+| 68.597
 | 0
 | 0
-| -509.276
+| -509.361
 |}

@@ Line 20: / Line 20: @@
 The differences in these plots come from fact that the "Forward" plots come from a GEANT simulation in which a small amount of energy was lost traveling through the target material.
-<center>{| border="1"
+{| border="1"
 |-
 ! KE<sub>i</sub>
@@ Line 65: / Line 65: @@
 | 0
 | -509.276
-|}</center>
+|}
 The particles start out with p=11000.511 GeV and have on average 11000 GeV by the time they interact