Kaon LT Meetings » History » Version 3
Richard Trotta, 07/16/2018 12:34 PM
1 | 1 | Richard Trotta | {{>toc}} |
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3 | h1. *Kaon LT Meetings* |
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5 | 2 | Richard Trotta | ---- |
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7 | 1 | Richard Trotta | h2. February 22, 2018 |
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9 | *Links to talks->* "Andres":https://redmine.jlab.org/documents/19 |
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11 | * Discussion of Andres' slides on elastic W calculation in hcana - initial issue with negative W values seems to be due to outdated information in standard.kinematics file. Additional investigation ongoing. |
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12 | * Brief description of Samip's work - working on coincidence timing decoding with JLab staff and re-optimization of kinematics |
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13 | * Discussion of Richard's slides on run plan kinematics and preparations - |
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14 | ** everyone agrees that in general want to have as many L/T cross section separations as possible in a robust run plan balancing statistics vs. systematics |
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15 | ** before actual run may want to do a 3D optimization in all kinematic variables to get the best possible delta(epsilon) for the L/T separations |
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16 | ** for each setting will need 1-2 shifts for calibrations - need to negotiate with other experiments in run group |
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17 | ** kinematics plots W-Q2 show that still need to do some optimization |
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18 | ** run sheets: include raster size, update coincidence count labeling, and carbon target labeling |
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19 | * Discussion of next meeting. Garth at JLab 8-16 March - might have meeting during that time. |
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21 | * *Action Items:* |
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22 | ** Post slides/notes from this meeting and procedure to set up hcana in Redmine (Tanja) |
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23 | ** Update run sheet and kinematic optimization for W/Q2 (Garth) |
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24 | ** Circulate elastic calculations for kinematic settings (Samip) |
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25 | ** Continue investigation of elastic data and run plan kinematics (Andres/Richard) |
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26 | ** Test software installation instructions (Pete) |
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27 | ** Draft email to JLab management about need for small angle beam pipe - need to have HMS minimum angle of less than 13 degrees for kaon L/T separations (Tanja) |
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31 | h2. March 29, 2018 |
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33 | *Links to talks->* "Richard, ":https://redmine.jlab.org/documents/16 "Samip":https://redmine.jlab.org/documents/27 |
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35 | * Details of adding points to fall run plan - will be ready sooner, likely in week of 4/1 (Garth, Samip, Tanja) |
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36 | * Luminosity scans (Ryan, Andres, Richard, Pete) |
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37 | * Macros, SIDIS analysis (Hem, Anashe) |
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38 | * Elastic data (TBD) |
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42 | h2. April 26, 2018 |
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44 | *Links to talks->* "Richard,":https://redmine.jlab.org/documents/18 "Ryan, ":https://redmine.jlab.org/documents/20 "Samip":https://redmine.jlab.org/documents/25 |
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46 | * Discussion luminosity scan analysis (earlier scan) - Richard |
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47 | ** Shown is a scaler-based analysis using scalers from report file and from ROOT tree - the values are different, why that is has to be checked |
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48 | ** Notes on efficiencies in report file: |
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49 | *** DT (EDTM) is not electronic deadtime. Instead use for now 50ns* trigger rate for HMS and 100ns* trigger rate for SHMS |
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50 | *** Cherenkov efficiency seems low (check if that is due to PID, thresholds, pi/e, etc) |
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51 | *** Tracking efficiency needs to be checked |
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52 | *** 3/4 trigger efficiency seems ok |
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53 | * Discussion luminosity scan analysis (later scan) - Ryan |
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54 | ** Fewer carbon runs than earlier scan |
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55 | ** Shown is a tracking-based analysis using data from the ROOT trees |
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56 | ** First results for carbon, LH2, and LD2, but efficiencies need to be checked |
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57 | * SIDIS analysis - Hem |
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58 | ** Shown is a data/MC comparison for different kinematic settings. Agreement in shape is very good. Normalization has yet to be applied. |
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59 | ** Discussion about agreement in z and apparent offset - relation of this offset with spectrometer offset |
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60 | * Analysis of exclusive events in SIDIS - Samip |
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61 | ** Shown is a look at the first kaon events in exclusive limit of SIDIS data |
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62 | ** Ongoing work on implementing coincidence time into tree |
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63 | * Discussion of run plan, and in particular possible low Q2/low energy |
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64 | ** Assume that kaon low Q2=0.4 already included - have kinematics with specified beam energies, if needed |
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65 | ** For pion form factor and LT, have two possible settings that can use the prescribed beam energies: Q2=1.45 and 0.35 GeV2 - prioritize towards the higher Q2 as not as sensitive to offsets |
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66 | ** Garth will put this together in a draft email |
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70 | 1 | Richard Trotta | h2. May 10, 2018 |
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72 | *Links to talks->* "Hem":https://redmine.jlab.org/documents/24, "Richard":https://redmine.jlab.org/documents/23, "Ryan, ":https://redmine.jlab.org/documents/20 "Samip":https://redmine.jlab.org/documents/26 |
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74 | * Luminosity Scans January 2018 (Richard) |
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75 | ** Tracking-based analysis for Runs 1415-1423, .. for now focus on HMS, typical HMS S1X rates are < |
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76 | ** Cuts applied: PID for electrons (Cer, Cal), acceptance (delta) |
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77 | ** Efficiency calculation was investigated in detail and applied using scalers from trees |
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78 | ** Results for carbon (normalized to 30uA) show large variation - need to understand |
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79 | ** *Next steps:* |
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80 | *** Double check calculation of computer lifetime, look for differences in TRIG and PRETRIG scalers |
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81 | *** Check stability of pre-scale (Ryan saw changes within runs) |
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82 | *** Check if detector calibrations for runs are implemented correctly |
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83 | *** Analyze with Ryan's cuts |
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85 | * Luminosity Scans April 2018 (Ryan) |
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86 | ** Confirms Richard's earlier finding that scaler-based analysis is not reliable and that it's best to analyze event-by-event |
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87 | ** Tracking-based analysis for runs 2073-2095 |
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88 | ** Cuts applied: PID for electrons (TOF, Cal, Chi2), acceptance (delta and angles), BCM4a |
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89 | ** Included most recent detector calibrations in replay of these runs |
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90 | ** Efficiencies from report file mainly, may need to update tracking efficiency implementation |
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91 | ** Found that calculations of computer deadtime requires different set of scalers for runs from January to those from April 2018 |
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92 | ** Results show carbon yields consistent with unity within error (0.5% error bars), and boiling for hydrogen and deuterium |
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93 | ** *Next steps:* |
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94 | *** Check tracking efficiency |
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96 | * *Global comments on Luminosity Scans (so far)* |
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97 | ** April 2018 scans show hydrogen and deuterium target boiling on level of 3-4%, Carbon is consistent with no boiling, as expected - based on description, new targets are expected to have less boiling than those used previously, e.g. in FPI2. Double check this. |
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98 | ** Efficiencies in report files need to be updated, e.g. CPU deadtime (Richard) |
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99 | ** Check if BCM4a is the one closest to the target - get a map of the hall (Richard, Ryan) |
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100 | ** Uncertainties on current |
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101 | ** Detector calibrations |
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102 | ** HMS vs. SHMS |
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104 | * eK+ coincidence time from SIDIS Spring 2018 run (Samip) |
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105 | ** Worked with Mark Jones on coincidence time calculation - now available in hcana (see Samip's 10 May 2018 email for more details) |
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106 | ** runs used in this analysis: 3423 with Q2=3.1 GeV2 and W=2.78 GeV |
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107 | ** Coincidence time spectrum shows peak separations >2 ns corresponding to different accelerator frequency |
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108 | ** Missing mass spectra: Kaon peak clearly visible, also see pions even after cuts |
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109 | ** Found that pions appear localized in phase space - seems to be due to end point in kinematic phase space |
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110 | ** *Next steps:* |
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111 | *** Look for a run with kaon momentum closer to 3 GeV/c (aerogel threshold is ~3 GeV/c for kaons for n=1.015) |
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113 | * Yield normalized ratios from SIDIS (Hem) |
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114 | ** Yield ratios of data to MC match well in shape, but normalization seems not quite right |
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115 | ** *Next steps:* |
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116 | *** Check if efficiencies, currents, run time etc. are taken into account correctly |
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120 | h2. May 17, 2018 |
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122 | *Links to talks->* "Richard":https://redmine.jlab.org/documents/29, "Ryan":https://hallcweb.jlab.org/DocDB/0009/000968/001/Presentation.pdf, "Samip":https://redmine.jlab.org/documents/30 |
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124 | * Luminosity scans (Richard, Ryan) |
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125 | ** Carbon scan from April seems consistent with no boiling, LH2 and LD2 show deviation from unity, should check effect of EDTM events on efficiencies |
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126 | ** Carbon scans from January (low rates) have large deviations from unity, in particular behavior at higher currents (>40uA), e.g. cpu dead time, that is not yet understood |
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127 | ** discussion about pre-scale factors |
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129 | * Discussion about Richard's script extracting and printing information from report files and trees including histograms |
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130 | ** Add option for looking at yields with cuts on cointime, target window, and missing mass |
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131 | ** Add option to look at real peak vs. background level |
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133 | * H(e,e'p) kinematics investigation for fall run (Samip) |
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134 | ** Optimal range is between electron angles of 17-20 degrees, time required ranges from ~1 hour at 17 degrees to ~3 hour at 20 degrees, other angles may be of interest for disentangling charge and current dependent effects |
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136 | * *Action Items* |
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137 | ** Luminosity scans at low rates from January (Richard) |
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138 | ** Luminosity scans from April with corrected efficiencies, e.d. DT (Ryan) |
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139 | ** H(e,e'p) and H(e,e') kinematics for upcoming Kaon LT run (Samip) |
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140 | ** Kaon LT detailed run plan (Garth, Pete, Tanja) |
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141 | ** Preparations, e.g. report files, diagnostic histograms and real time monitoring, shift worker instructions, optimization of trees (all) |
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143 | 2 | Richard Trotta | ---- |
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145 | 1 | Richard Trotta | h2. May 31, 2018 |
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147 | *Links to talks->* "Samip":https://redmine.jlab.org/documents/30 |
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149 | 3 | Richard Trotta | ---- |
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151 | 1 | Richard Trotta | h2. June 28, 2018 |
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153 | *Links to talks->* "Richard":https://redmine.jlab.org/documents/34 |
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155 | * Ryan |
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156 | ** resolving differences between his analysis and Richard's |
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157 | |||
158 | * Richard |
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159 | ** Discussed with Mark Jones and is cross checking his January luminosity scan analysis against Mark's. Realized that BCM calibrations (gains, offsets etc) are different - currently working on fixing that, presents current results - low curent point is ~10% below unity, discussion that this seems to indicate that BCM offsets are the issue as low current points would be most sensitive, is planning to also double-check the BCM calibration procedure - had discussion with Dave Mack at JLab |
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160 | ** Presents a script developed for luminosity scans that determines yields for a run number input on command line. Discussion this could be good to adapt for kaon counting during experiment. |
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164 | 1 | Richard Trotta | h2. July 11, 2018 |
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166 | 2 | Richard Trotta | *Ongoing Tasks->* #381 #382 #383 #384 |
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