Pixel Operation Plots 2018

Contact: Alexander Froehlich (Alexander.Froehlich@cernNOSPAMPLEASE.ch)

ROC Thresholds during Commissioning 2018

Figure in png format other formats Description
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 1 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 2 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. Modules that were damaged in 2017 and could not be replaced are shown in yellow, while the modules showing normal behavior are shown in blue. The damaged modules have a higher threshold. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 3 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 4 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for all four layers of the pixel barrel detector normalized to the number of ROCs in the respective layer. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for ring 1 of the pixel forward detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. Modules that were damaged in 2017 and could not be replaced are shown in yellow, while the modules showing normal behavior are shown in blue. The damaged modules have a higher threshold. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for ring 2 of the pixel forward detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for the whole pixel forward detector normalized to the number of ROCs in the respective ring. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed during the commissioning phase in 2018. The number of electrons were calculated from the measured calibration units (VCal).

ROC Thresholds during TS1 (June) 2018

Figure in png format other formats Description
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 1 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 2 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. Modules that were damaged in 2017 and could not be replaced are shown in yellow, while the modules showing normal behavior are shown in blue. The damaged modules have a higher threshold. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 3 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for layer 4 of the pixel barrel detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for all four layers of the pixel barrel detector normalized to the number of ROCs in the respective layer. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for ring 1 of the pixel forward detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. Modules that were damaged in 2017 and could not be replaced are shown in yellow, while the modules showing normal behavior are shown in blue. The damaged modules have a higher threshold. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for ring 2 of the pixel forward detector. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).
.eps .pdf The distribution of the readout chip (ROC) threshold in number of electrons for the whole pixel forward detector normalized to the number of ROCs in the respective ring. The threshold is measured as the value where the turn-on of the ROC reaches an efficiency of 0.5. The shown measurement was performed in June 2018. The number of electrons were calculated from the measured calibration units (VCal).

Conversion factors for VCal to electrons

The conversion factors for VCal to number of electrons is given in the following tables per layer for pixel barrel and per ROC row and ring in pixel forward: Commissioning
ROC gain pedestal
BPix L1 53.866 -670
BPix L2 49.833 -60
BPix L3 49.539 -60
BPix L4 49.294 -60
FPix R1 - ROC7,ROC8 53.523 -60
FPix R1 - ROC6,ROC9 53.326 -60
FPix R1 - ROC5,ROC10 53.157 -60
FPix R1 - ROC4,ROC11 53.009 -60
FPix R1 - ROC3,ROC12 52.879 -60
FPix R1 - ROC2,ROC13 52.761 -60
FPix R1 - ROC1,ROC14 52.654 -60
FPix R1 - ROC0,ROC15 52.557 -60
FPix R2 - ROC7,ROC8 52.954 -60
FPix R2 - ROC6,ROC9 52.858 -60
FPix R2 - ROC5,ROC10 52.770 -60
FPix R2 - ROC4,ROC11 52.688 -60
FPix R2 - ROC3,ROC12 52.611 -60
FPix R2 - ROC2,ROC13 52.539 -60
FPix R2 - ROC1,ROC14 52.471 -60
FPix R2 - ROC0,ROC15 52.407 -60

June

ROC gain pedestal
BPix L1 55.601 -670
BPix L2 50.274 -60
BPix L3 49.735 -60
BPix L4 49.416 -60
FPix R1 - ROC7,ROC8 53.523 -60
FPix R1 - ROC6,ROC9 53.326 -60
FPix R1 - ROC5,ROC10 53.157 -60
FPix R1 - ROC4,ROC11 53.009 -60
FPix R1 - ROC3,ROC12 52.879 -60
FPix R1 - ROC2,ROC13 52.761 -60
FPix R1 - ROC1,ROC14 52.654 -60
FPix R1 - ROC0,ROC15 52.557 -60
FPix R2 - ROC7,ROC8 52.954 -60
FPix R2 - ROC6,ROC9 52.858 -60
FPix R2 - ROC5,ROC10 52.770 -60
FPix R2 - ROC4,ROC11 52.688 -60
FPix R2 - ROC3,ROC12 52.611 -60
FPix R2 - ROC2,ROC13 52.539 -60
FPix R2 - ROC1,ROC14 52.471 -60
FPix R2 - ROC0,ROC15 52.407 -60

DCDC Characterization

Classification based on I-V curve measurement

Figure in png format other formats Description
.eps .pdf Two tests are performed to classify the DCDC converters as either working normally, having high-current or being broken. The first test is the disable test, where the DCDC converter is disabled and the input voltage is scanned from 0 V to 5.5 V (upper plot). The second test is the enable test, where the DCDC is enabled and a load of 1.5A is connected. The input voltage is then scanned from 0 V to 10 V. There is a difference in the behavior between a high-current DCDC and a normal working DCDC in the disabled test, while the converters show the same behavior in the enable test. A DCDC converter is considered as having high-current, when the input current at 5.5V is larger than 4mA. The behavior of a broken DCDC converter is not shown. A DCDC converter is considered broken, when the input current at 10V in the enabled test is less than 400mA.
.eps .pdf The input current of the DCDC converters that were extracted from the detector after the 2017 run. The current was measured at an input voltage of 5.5V while the DCDC is disabled. DCDCs with an input current less than 4mA are considered as working normally. DCDCs with an input current greater than 4mA are considered as high-current.
.eps .pdf The input current of the DCDC converters that were extracted from the detector after the 2017 run. The current was measured at an input voltage of 10V while the DCDC is enabled. A clear separation between the broken DCDC converters (input current less than 400 mA), the working analog converters (input current between 400 and 540 mA) and the working digital converters (input current greater 540 mA) is observed. While a DCDC converter is enabled no difference between the normal behavior and the high-current behavior is visible in this distribution.

Maps with DCDC classifications after run 2017

Pixel Barrel

Figure in png format other formats DescriptionSorted ascending
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in minus direction wrt. the beam on the inner side (BmI) of the barrel pixel detector. The coordinates correspond to the position of the DCDC converter in the detector during the run. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in minus direction wrt. the beam on the outer side (BmO) of the barrel pixel detector. The coordinates correspond to the position of the DCDC converter in the detector during the run. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in plus direction wrt. the beam on the inner side (BpI) of the barrel pixel detector. The coordinates correspond to the position of the DCDC converter in the detector during the run. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in plus direction wrt. the beam on the outer side (BpO) of the barrel pixel detector. The coordinates correspond to the position of the DCDC converter in the supply tube in the detector. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.pdf Summary of the characterization of the 2017 DCDC converters for the barrel pixel detector. The number of normal behaving, high-current and broken DCDC converters is given for each half-cylinder separately and for the total barrel pixel detector.

Pixel Forward

Figure in png format other formats Description
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in minus direction wrt. the beam on the inner side (BmI) of the forward pixel detector. The converters are grouped into readout groups (ROG) and the coordinates correspond to the position in the detector. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in minus direction wrt. the beam on the outer side (BmO) of the forward pixel detector. The coordinates correspond to the position of the DCDC converter in the detector during the run. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in plus direction wrt. the beam on the inner side (BpI) of the forward pixel detector. The coordinates correspond to the position of the DCDC converter in the detector during the run. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.eps .pdf Overview of the DCDC converter classification after the 2017 run for the half-cylinder in plus direction wrt. the beam on the outer side (BpO) of the forward pixel detector. The coordinates correspond to the position of the DCDC converter in the detector during the run. Analog DCDC converter are marked with an a, digital DCDC converter are marked with a d.
.pdf Summary of the characterization of the 2017 DCDC converters for the forward pixel detector. The number of normal behaving, high-current and broken DCDC converters is given for each half-cylinder separately and for the total forward pixel detector.

-- BenediktVormwald - 2018-08-17

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