Using the single-particle commands in PISA, throw particles (5 GeV muons) into the N endcap like this:
run | the phi | zvertex | side view |
---|---|---|---|
121 | 20° 20° | 0 | pic |
122 | 10° 04° | 0 | pic |
123 | 27° 04° | 0 | pic |
124 | 10° 04° | -10 | pic |
125 | 19° 04° | -10 | pic |
pisa exec single (capture drawing) exit pisaRootRead mv ancsvx.root ancsvx_nnn.root ln -sf ancsvx_nnn.root ancsvx_softlink.root root -l .x residual.C .x resid2.C (capture plots) .q
Results
Theta, phi of the track at the origin are projected onto the endcaps (red dot), and compared with the actual hit, which falls in a distribution around this point. This distribution is projected onto two orthogonal axes, using the simplifying assumption that the Si surface is perpendicular to the track, which is roughly true. |
Residual distributions (in cm) in the theta
and r-phi directions for the 4 lampshades of the N endcaps.
This run was for run 125: 5 GeV muons, centered on the = 19° and phi = 4°, in a 1° cone. |
Results: (output from residual.C + resid2.C)
cfmgmc.input5 5 20 20 1 10 0 0 0 0 layer 09: 35 33 layer 10: 49 44 layer 11: 65 53 layer 12: 87 75 cfmgmc.input5 5 10 3.75 1 10 0 0 0 0 layer 09: 25 25 layer 10: 33 37 layer 11: 51 54 layer 12: 74 75 cfmgmc.input5 5 27 3.75 1 10 0 0 0 0 layer 09: 46 48 layer 10: 68 60 layer 11: 93 87 layer 12: 131 134 fmgmc.input5 5 19 3.75 1 10 0 0 -10 0 layer 09: 86 92 layer 10: 78 88 layer 11: 111 114 layer 12: 131 143 fmgmc.input5 5 10 3.75 1 10 0 0 -10 0 layer 09: 65 73 layer 10: 82 89 layer 11: 127 134 layer 12: 127 149The residuals in the table below are the average of the sigma_theta, sigma_phi of the gaussian fits to the residual distributions.
5 GeV mu+ | residuals (um) | |||||||
---|---|---|---|---|---|---|---|---|
run | the phi | zvertex | side view | 9 | 10 | 11 | 12 | comments |
121 | 20° 20° | 0 | pic | 33 | 45 | 63 | 82 | 1 barrel, center of 4 endcaps |
122 | 10° 04° | 0 | pic | 24 | 34 | 52 | 70 | no barrel, bottom of 4 endcaps |
123 | 27° 04° | 0 | pic | 45 | 60 | 98 | 112 | 2 barrel, top of 4 endcaps |
124 | 10° 04° | -10 | pic | 77 | 94 | 128 | 156 | z= -10 cm, bottom of mu acceptance |
125 | 19° 04° | -10 | pic | 79 | 95 | 124 | 151 | z = -10 cm, 2 barrel + 4 endcaps |
2 GeV mu+ | residuals (um) | ||||||
---|---|---|---|---|---|---|---|
run | the phi | zvertex | 9 | 10 | 11 | 12 | comments |
126 | 10° 04° | 0 | 89 | 83 | 103 | 137 | no barrel, bottom of 4 endcaps |
127 | 27° 04° | 0 | 117 | 163 | 250 | 467 | 2 barrel, top of 4 endcaps |
128 | 10° 04° | -10 | 208 | 237 | 338 | 355 | z= -10 cm, bottom of mu acceptance |
129 | 19° 04° | -10 | 300 | 210 | 285 | 308 | z = -10 cm, 2 barrel + 4 endcaps |
10 GeV mu+ | residuals (um) | ||||||
---|---|---|---|---|---|---|---|
run | the phi | zvertex | 9 | 10 | 11 | 12 | comments |
130 | 10° 04° | 0 | 12 | 17 | 26 | 35 | no barrel, bottom of 4 endcaps |
131 | 27° 04° | 0 | 24 | 31 | 49 | 68 | 2 barrel, top of 4 endcaps |
132 | 10° 04° | -10 | 40 | 52 | 66 | 77 | z= -10 cm, bottom of mu acceptance |
133 | 19° 04° | -10 | 38 | 42 | 60 | 69 | z = -10 cm, 2 barrel + 4 endcaps |
5 GeV mu+ | residuals (um) | ||||||
---|---|---|---|---|---|---|---|
run | the phi | zvertex | 9 | 10 | 11 | 12 | comments |
134 | 10° 04° | 0 | 20 | 28 | 45 | 62 | no barrel, bottom of 4 endcaps |
135 | 27° 04° | 0 | 20 | 24 | 35 | 52 | 2 barrel, top of 4 endcaps |
136 | 10° 04° | -10 | 38 | 47 | 62 | 73 | z= -10 cm, bottom of mu acceptance |
137 | 19° 04° | -10 | 32 | 42 | 52 | 63 | z = -10 cm, 2 barrel + 4 endcaps |