Beam time @Julich -2016.

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Presentation transcript:

Beam time @Julich -2016

Status of the MVD activities in Torino I ) Presentation at the mec. session II) Results from beam tests of pixel prototypes Daniela Calvo

Update of MVD services and requests DCDC circuits Optoelectronic (GBTx + VTRX) boards Cooling plant Services on platform in front of the magnet Daniela Calvo MVD group

MVD services - DCDC circuits

MVD service - DCDC circuits 24 blocks arranged in 3 sectors (2112 DCDC circuits) 4 PCBs (left and right difference) housing 22 DCDC circuits each

MVD services – first prototype 88 DCDC circuits (22 DCDC circuits each row) Weight (without cables): ~ 1.3 Kg Dimension (without cables): 455 mm (with cooling connectors) x 85 mm x 63 mm

MVD services - Request Available cross section: 56000 mm2 ONLY HALF of the needed CROSS SECTION is AVAILABLE for cables IT IS NECESSARY MORE SPACE around the beam pipe for the MVD Available cross section: 56000 mm2 (between beam pipe and inner BEMC diameter) Cooling pipes and supports: 9000 mm2 (dashed ring – challenge solution!) DCDC circuits leave only ~ half of cross section for cables (needed cross section: 22300 mm2) and the cables will fill the empty parts between the circuits anyway. (not reccommended!)

MVD services – Optoelectronic boards

Optoelectronics board, old version 76 mm 60 mm 12 bars with 16 GBT boards each (192 circuits) Interspace between PCBs: 20 mm

Optoelectronic board, new version – GBTx + VTRX GBTx and VTRX on opposite sides, then 4.8 Gbit/s signals routed using vias Two power supply connectors to fit the routing of the power supply cables, in fact two mounting configuration of the boards are foreseen. Additional chip to distribute the SC out signal to the two connectors towards the FEE. The cooling of the GBTx in this configuration should be easier (to be verified!). The board dimension is larger than the estimated values ( 3 years ago) anyway. 86 mm 25.4 mm 15.5 mm

Opto. board, new version – board routing Interference between optical fiber connectors and signal cables !! Opto. board, new version – board routing 16,5 mm Signal cable Thermal bridge (copper) 20 mm

Opto. board, new version – board number Each connector includes : 5 e-links + SC signal 22 additional boards to maintain the symmetry left– right during the routing of the semi disks and semi cylinders of the barrel part to be able to send the SC signal to each pixel or strip module without connection between different modules 86 mm 25.4 mm It is necessary to increase the GBT board number from 192 to 214. It means 2 additional optoelectronic boards each bar, one each side

Requests Interdistance: 15 mm longer Additional 80 mm to arrange the 192 longer optoelectronics boards Additional 86 mm to arrange an additional board along the rod Additional 120 mm to avoid interference between optical fibers and signal cables Possible solution ?: to shift upstream the beam pipe flange A DCDC block (or partial block) has to be cut out, anyway! IT IS NECESSARY MORE SPACE around the beam pipe for the MVD

MVD services – Cooling plant

Cooling plant ouside the pit PLC INLET RACKS (PIXEL, STRIP, SERVICES)

Cooling plant inside the pit RETURN RACKS (PIXEL, STRIP, SERVICES) INLET PUMP + WATER CLEANING UNIT TANK+ VACUUM PUMP

Cooling plant - line paths inside PANDA Hall RETURN LINES INLET LINES

MVD services in front of the magnet

Racks - request MVD Use the racks starting from the top (222 U – 50% left and 50% right). The reduction to 188 U is still under investigation.

Patch panels for cables - request for MVD cables Patch panels for MVD cables positioned close the BEMC support (left and right) with duct to route cables from racks. A specific system could move and rotate the duct for positioning the patch panels at the external side of the racks, during the installation of detectors. The system could be positioned on the top of the racks

Routing of the cooling pipes and patch panel - request The duct for the cooling pipes to the patch panels needs to be positioned under the platform floor It should be a solution to foresee also the patch panel (for the cooling part) under the platform during the detectors installation. A system could move and rotate the patch panel to the final position, near the BEMC support. But it is necessary to go trough the platform floor. platform Vertical section Patch panel Duct - cooling pipes

Results from beam tests of pixel prototypes Daniela Calvo Torino MVD group

Test at LNL - July 2015 To complete the study of SEU of the pixel configuration registers of ToPix4 (to study the best trade off of the area vs protection level) half of the matrix implements D-type Flip-Flops circuits with the Triple Modular Redundancy (TMR) error detection and correction circuitry the second half of the matrix uses Hamming encoding that detects and corrects errors (ToPix3 used TMR with latches) July 2014 July 2015 ? < 1.3 x10-6 upsets/hour in the MVD

Test in Julich - May 2015 Pixel tracking station equipped with assemblies based on ToPix4, to perform: ToT measurements as a function of the feedback current Double Data Rate test Efficiency evaluation

Test in Julich - 1 Measured voltage [V] @ test point, 5,00 nA/pixel 7,5 9,65 Measured voltage [V] @ test point, to regulate feedback current

Test in Julich - 2

Test in Julich - 3 Efficiency vs Freeze Stop Efficiency vs threshold

Test at CERN - July 2015 To perform tests with different particles and momentum (pions and protons, positive and negative polarity, the momentum ranges between 20 GeV/c up to 150 GeV/c). To mask the furthest pixels in the long columns To check the chip at different voltage supply To run without the filter used in the daq to cut out the events without hits 4 pixel assemblies under test 2 scintillator stations each composed by a cross of two small scintillators to count the particle number in the sensor area ( 6.4 mm2) 1 cross between two scintillator to count the particle number/cm2

Test at CERN - 1 Unfortunately, tests with positive polarity were possible only In addition, higher momentum corresponds to higher beam intensity Tests @ 4 different momentum 20 GeV/c 50 GeV/c 100 GeV/c 150 GeV/c

Preliminary plot ! Test at CERN - 1 2.9 GeV/c protons at Julich Different % of pions and protons at 20, 50 and 100 GeV/c, at CERN ToT and error values: most probable values and the gaussian sigma obtained using the convolution fit to the ToT distributions

Test at Cern - 2 Momentum: 150 GeV/c, th: 1200 electrons The furthest pixels in the long columns were masked The evaluated number of hits/cm2 is ~ 3 Mhits/cm2 (also measured) The masked pixels show hits in the raw map of the assembly, anyway. A possible explanation is that they are created in the end column circuits. To be investigated!

Test at Cern – 3 and 4 Tests at different voltage supply need to evaluate the new working point of the chip. We have achieved this conclusion during the data acquisition!!!! Then the acquired data are meaningless. The comparison of acquired data with and without filter at the level of data acquisition has to be still done