Detector alignment |
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Residual distribution in x, integrated over all hits-on-tracks in the pixel barrel for the nominal geometry and the preliminary aligned geometry. The residual is defined as the measured hit position minus the expected hit position from the track extrapolation. Shown is the projection onto the local x coordinate, which is the precision coordinate. Tracks are selected to have pT > 2 GeV, |d0|<50mm, |z0|<400mm (in other words they are required to go through the pixel L0). The distribution is shown for 5 cosmic runs: 91885, 91888, 91890, 91891, 91900, all have solenoid on - corresponding to ~25% of all the solenoid-on data taken in Sep/Oct 2008. New Tracking is used (in 14.5.2.1). A double Gaus fit is performed but only the mean and sigma of the narrower Gaussian are shown. |
![]() Approved_PixBarResX.eps |
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Residual distribution in y, integrated over all hits-on-tracks in the pixel barrel for the nominal geometry and the preliminary aligned geometry. The residual is defined as the measured hit position minus the expected hit position from the track extrapolation. Shown is the projection onto the local y coordinate, which is the non-precision coordinate. Tracks are selected to have pT > 2 GeV, |d0|<50mm, |z0|<400mm (in other words they are required to go through the pixel L0). The distribution is shown for 5 cosmic runs: 91885, 91888, 91890, 91891, 91900, all have solenoid on - corresponding to ~25% of all the solenoid-on data taken in Sep/Oct 2008. New Tracking is used (in 14.5.2.1). A single Gaussian fit is performed. |
![]() Approved_PixBarResY.eps |
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Residual distribution in x, integrated over all hits-on-tracks in the SCT barrel for the nominal geometry and the preliminary aligned geometry. The residual is defined as the measured hit position minus the expected hit position from the track extrapolation. Shown is the projection onto the local x coordinate, which is the precision coordinate. Tracks are selected to have pT > 2 GeV, |d0|<50mm, |z0|<400mm (in other words they are required to go through the pixel L0). The distribution is shown for 5 cosmic runs: 91885, 91888, 91890, 91891, 91900, all have solenoid on - corresponding to ~25% of all the solenoid-on data taken in Sep/Oct 2008. New Tracking is used (in 14.5.2.1). A single Gaussian fit is performed. |
![]() Approved_SCTBarResX.eps |
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Cosmic tracks crossing the entire ID leave hits in both the upper and lower halves of the ID. These tracks can be split near the interaction point and fit separately, resulting in two collision-like tracks that can then be compared. The plots shows the difference in the d0 track parameter between the two split tracks. Tracks are selected to have pT > 2 GeV, |d0|<50mm, |z0|<400mm (in other words they are required to go through the pixel L0). Tracks also are required to have a hit in the Pixel B layer, 3 Pixel hits and in total 7 Silicon hits. The distribution is shown for 5 cosmic runs: 91885, 91888, 91890, 91891, 91900, all have solenoid on - corresponding to ~25% of all the solenoid-on data taken in Sep/Oct 2008. New Tracking is used (in 14.5.2.1). A single Gaussian fit is performed. |
![]() Approved_DeltaD0.eps |
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Cosmic tracks crossing the entire ID leave hits in both the upper and lower halves of the ID. These tracks can be split near the interaction point and fit separately, resulting in two collision-like tracks that can then be compared. The plots shows the difference in the z0 track parameter between the two split tracks. Tracks are selected to have pT > 2 GeV, |d0|<50mm, |z0|<400mm (in other words they are required to go through the pixel L0). Tracks also are required to have a hit in the Pixel B layer, 3 Pixel hits and in total 7 Silicon hits. The distribution is shown for 5 cosmic runs: 91885, 91888, 91890, 91891, 91900, all have solenoid on - corresponding to ~25% of all the solenoid-on data taken in Sep/Oct 2008. New Tracking is used (in 14.5.2.1). A single Gaussian fit is performed. |
![]() Approved_DeltaZ0.eps |
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Cosmic tracks crossing the entire ID leave hits in both the upper and lower halves of the ID. These tracks can be split near the interaction point and fit separately, resulting in two collision-like tracks that can then be compared. The plots shows the difference in the Q/pT track parameter between the two split tracks. Tracks are selected to have pT > 2 GeV, |d0|<50mm, |z0|<400mm (in other words they are required to go through the pixel L0). Tracks also are required to have a hit in the Pixel B layer, 3 Pixel hits and in total 7 Silicon hits. The distribution is shown for 5 cosmic runs: 91885, 91888, 91890, 91891, 91900, all have solenoid on - corresponding to ~25% of all the solenoid-on data taken in Sep/Oct 2008. New Tracking is used (in 14.5.2.1). A single Gaus fit is performed. |
![]() Approved_DeltaQoPT.eps |
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Cosmic tracks crossing the entire ID leave hits in both the upper and lower halves of the ID. These tracks can be split near the interaction point and fit separately, resulting in two collision-like tracks that can then be compared. The plots shows the difference in the phi track parameter between the two split tracks. Tracks are selected to have pT > 2 GeV, |d0|<50mm, |z0|<400mm (in other words they are required to go through the pixel L0). Tracks also are required to have a hit in the Pixel B layer, 3 Pixel hits and in total 7 Silicon hits. The distribution is shown for 5 cosmic runs: 91885, 91888, 91890, 91891, 91900, all have solenoid on - corresponding to ~25% of all the solenoid-on data taken in Sep/Oct 2008. New Tracking is used (in 14.5.2.1). A double Gaussian fit is performed but only the mean and sigma of the narrower Gaus are shown. |
![]() Approved_DeltaPhi.eps |
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Distributions from cosmic ray tracks |
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Warning: Cosmic ray spectra including comparisons with MC which appeared before on this page are not approved for external use at this stage.
The MC does not model some details of the special cosmic trigger configuration and timing. It includes the two main access shafts, but not
the two lift shafts. Until these effects are taken into account, the MC-data comparison is not useful.
Cosmic muons crossing the entire ATLAS detector leave hits in the Inner Detector (ID) and so tracks can be reconstructed. Two different tracking algorithms are in use for the reconstruction: the CTB (Cosmics and Test Beam) tracking and the New Tracking. The results below show the performance of the CTB. Tracks are characterized by 5 parameters. These are defined in a reference point, the perigee, which is the point of closest approach to the z/beam axis. d0 is the signed distance to the z-axis, z0 is the z-coordinate of the perigee, phi0 is the angle in the x-y plane at the perigee, theta0 is the angle with the z-axis and q/p is the charge of the cosmic muon divided by its momentum. In the next plots, the parameters of these cosmic muon tracks (reconstructed with CTB tracking and release 14.5.0.5, AtlasProduction) from the ATLAS combined cosmic run 91890 (Autumn 2008) are shown. Both toroid and solenoid were on during this run. For the theta0 and z0 distributions, tracks are required to have Silicon hits (since these parameters are not measured by the TRT barrel). | |||||||||||||||||
Cosmic spectra (d0 distribution) as seen in run 91890. |
![]() eps figure |
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Cosmic spectra (z0 distribution) as seen in run 91890. |
![]() eps figure |
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Cosmic spectra (phi0 distribution) as seen in run 91890. |
![]() eps figure |
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Cosmic spectra (theta0 distribution) as seen in run 91890. |
![]() eps figure |
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Cosmic spectra (QoverP distribution) as seen in run 91890. |
![]() eps figure |
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Cosmic ray track statistics |
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Collected track statistics in autumn 2008:
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![]() pdf figure |
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Event displays |
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Inner detector event display for event 757427 of the cosmic run 90270 with field ON. |
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Inner detector event display for event 62340 of the cosmic run 90731 (no Solenoid). Showing hits on track for both TRT endcaps, as well as SCT and pixel barrel and endcap hits. |
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I | Attachment | History | Action | Size | Date | Who![]() |
Comment |
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IDCosmic08_statistics.gif | r1 | manage | 60.4 K | 2009-02-13 - 09:33 | ChristianSchmitt | |
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IDCosmic08_statistics.pdf | r1 | manage | 18.0 K | 2009-02-13 - 09:33 | ChristianSchmitt | |
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trackpar_QoverP.eps | r1 | manage | 12.9 K | 2009-03-09 - 14:16 | PippaWells | |
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trackpar_QoverP.png | r1 | manage | 8.1 K | 2009-03-09 - 14:15 | PippaWells | |
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trackpar_d0.eps | r1 | manage | 11.3 K | 2009-03-09 - 14:18 | PippaWells | |
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trackpar_d0.png | r1 | manage | 7.8 K | 2009-03-09 - 14:18 | PippaWells | |
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trackpar_eta.eps | r1 | manage | 9.5 K | 2009-03-09 - 14:17 | PippaWells | |
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trackpar_eta.png | r1 | manage | 6.1 K | 2009-03-09 - 14:17 | PippaWells | |
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trackpar_phi0.eps | r1 | manage | 12.5 K | 2009-03-09 - 14:17 | PippaWells | |
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trackpar_phi0.png | r1 | manage | 8.3 K | 2009-03-09 - 14:17 | PippaWells | |
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trackpar_theta0.eps | r1 | manage | 10.4 K | 2009-03-09 - 14:15 | PippaWells | |
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trackpar_theta0.png | r1 | manage | 6.9 K | 2009-03-09 - 14:14 | PippaWells | |
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trackpar_z0.eps | r1 | manage | 12.3 K | 2009-03-09 - 14:14 | PippaWells | |
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trackpar_z0.png | r1 | manage | 8.5 K | 2009-03-09 - 14:13 | PippaWells | |
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Atlas_ID_Loops_ON_cy_2008.gif | r1 | manage | 20.9 K | 2009-03-09 - 14:19 | SaverioDAuria | Number of ID Cooling Loops ON as a function of time |
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Approved_DeltaD0.eps | r1 | manage | 32.0 K | 2009-03-05 - 14:19 | TobiasGolling | Delta D0 from cosmic tracks broken down in 2 legs |
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Approved_DeltaD0.png | r1 | manage | 30.6 K | 2009-03-05 - 14:19 | TobiasGolling | Delta D0 from cosmic tracks broken down in 2 legs |
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Approved_DeltaPhi.eps | r1 | manage | 49.1 K | 2009-03-05 - 14:20 | TobiasGolling | Delta Phi from cosmic tracks broken down in 2 legs |
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Approved_DeltaPhi.png | r1 | manage | 31.4 K | 2009-03-05 - 14:21 | TobiasGolling | Delta Phi from cosmic tracks broken down in 2 legs |
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Approved_DeltaQoPT.eps | r1 | manage | 17.6 K | 2009-03-05 - 14:21 | TobiasGolling | Delta QopT from cosmic tracks broken down in 2 legs |
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Approved_DeltaQoPT.png | r1 | manage | 29.8 K | 2009-03-05 - 14:21 | TobiasGolling | Delta QopT from cosmic tracks broken down in 2 legs |
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Approved_DeltaZ0.eps | r1 | manage | 26.0 K | 2009-03-05 - 14:21 | TobiasGolling | Delta Z0 from cosmic tracks broken down in 2 legs |
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Approved_DeltaZ0.png | r1 | manage | 32.7 K | 2009-03-05 - 14:22 | TobiasGolling | Delta Z0 from cosmic tracks broken down in 2 legs |
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Approved_PixBarResX.eps | r1 | manage | 28.5 K | 2009-03-05 - 14:22 | TobiasGolling | Pixel x residuals |
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Approved_PixBarResX.png | r1 | manage | 32.8 K | 2009-03-05 - 14:23 | TobiasGolling | Pixel x residuals |
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Approved_PixBarResY.eps | r1 | manage | 38.8 K | 2009-03-05 - 14:23 | TobiasGolling | Pixel y residuals |
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Approved_PixBarResY.png | r1 | manage | 39.7 K | 2009-03-05 - 14:23 | TobiasGolling | Pixel y residuals |
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Approved_SCTBarResX.eps | r1 | manage | 27.5 K | 2009-03-05 - 14:24 | TobiasGolling | SCT x residuals |
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Approved_SCTBarResX.png | r1 | manage | 31.5 K | 2009-03-05 - 14:24 | TobiasGolling | SCT x residuals |
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PixResX_NewT_D0Z0cut_Mat_vsNominal.png | r2 r1 | manage | 33.4 K | 2008-12-11 - 19:11 | TobiasGolling | Pixel x residuals |
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PixResY_NewT_D0Z0cut.png | r2 r1 | manage | 40.6 K | 2008-12-11 - 19:12 | TobiasGolling | Pixel y residuals |
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SCTResX_NewT_D0Z0cut.png | r2 r1 | manage | 31.8 K | 2008-12-11 - 19:13 | TobiasGolling | SCT x residuals |