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RICH UPGRADE PROJECTSTATUS REPORT
09-06-2015 @CERN
Alessandro PetroliniDipartimento di Fisica dell’Università di Genova
and INFN
on behalf of the RICH group
2
OutlineA necessarily incomplete and biased selection of topics.
Common components to RICH1 and RICH2: MAPMT, BaseBoard, CLARO/FEB, BackBoard, MagneticShield
(MS),+ case …ElementaryCell (EC);
EC + PDMDB+ column structure … PhotoDetectorModule (PDM).
PhotoDetectorAssembly (PDA) Mechanics/Thermal engineering: RICH2, well advanced design; RICH1, working hard, more challenging design
(constraints). HV, LV, signal; grounding and shielding. Irradiation test program. QA. Test Beam.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
3
The photo-sensors: MAPMT
Hamamatsu R11265 (one inch, 64 px): RICH1 AND RICH2; “Small PMT”.
Hamamatsu R12699 (two inch, 64 px): RICH2 ONLY; “Large PMT”.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
4
R11265 characterization
Several devices were tested.All devices were able to detect single photons in almost all pixels.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
5
R11265 characterization
Typical gain uniformity: 2.5÷3.5 (pix to pix and tube to tube).
Low dark current rate: ∼ 60 Hz/cm2. Low cross-talk amplitude: ∼ 5 % with a fast bipolar
shape. Effects of magnetic field recovered by a magnetic
shield. According to the manufacturer the gain variation
strongly depends on the thickness of the cesium layer grown on the dynodes surface (a parameter hard to keep under control during the production). Hard to define a typical device behavior (both
positive and negative gain variation observed: ΔG ≅ ∓20% after 3000 h).
Aging data from Hamamatsu are ok for us.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
6
MaPMT R12699 (H12700)
To be used in the outer part of the RICH2. Four devices have been tested so far:
2 tubes equipped with the embedded socked: H12700;
2 tubes without socket and biased though a custom made voltage divider (standard voltage ratio): R12699.
It is being used at CBM RICH DETECTOR, FAIR lab in Darmstadt.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
Feature R12699
Geometricaldimension 52×52 mm2
Photocathode minimum active
area48.5×48.5 mm2
Number of pixel and dimension 64 / 6×6 mm2
7
The CLARO chipfast single photon counting with PMT
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
809-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
The CLARO chip
0.35 µm CMOS technology from ams. Rad tolerant up to ≈ 1 MRad (10 kGy),
≈ 1013 cm-2 1-MeV equivalent neutrons. Thresholds ranges from 30 ke- to 15 Me-. ≈ 1 mW/channel power consumption. < 25 ns recovery time. 8 channels per chip.
9
CLARO8v2 – design
Aiming to build the best detector possible, within the constraints, a new version of the chip, CLARO8v2, was submitted in April.
Improvements with respect to the previous versions: improved channel-to-channel matching; larger (6x) test capacitors to inject test signals up
to 4 Me- with 1 V test signals; adjusted attenuation settings:
from 1, 1/4, 1/7, 1/10 to 1, 1/2, 1/4, 1/8; configuration register redesigned for compatibility
with rad-hard cells; power-on reset to switch on the chip in a known
state; additional measures to enhance yield.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
10
CLARO8v2 – channel matching
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
CLARO8v0 CLARO8v1 CLARO8v2
11
FEB housing 8 CLARO chips
New FEB and BackBoard have been designed to be compatible with the changes of the CLARO8v2.
They are still compatible with previous versions of the CLARO and with the existing data acquisition hardware for beam test.
A very dense board…
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
12
A partially assembled EC
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
13
BackBoard Every PCB is also
a structural element and part of the passive cooling system.
Jumper between signal ground and chassis Metallization of the mounting holes. Creation of copper filler areas. Improvements to electrical design.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
14
EC (no MS) exploded view
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
15
EC front-view (no MS)
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
16
EC back-view (no MS)
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
17
Behavior of the R11265 MAPMTin magnetic fields
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
Efficiency: number of events for a given B-field strength normalized to the number of events at zero B-field.
Efficiency curves averaged over all pixels of the R11265 and the R7600 as a function of the magnetic field applied in both transverse directions (x and y) and in the longitudinal direction (z).
18
Magnetic shield
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
19
Behavior of the R11265 MAPMTin magnetic fields with magnetic
shield
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
20
MS prototypes made at CERNpreliminary results
Longitudinal B field:similar performance, efficiency≥ 90%;
Transverse B field:slightly better performance of full shield, efficiency≥ 95%.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
21
PDMDBDigital Electronic Board for a PDM
The limited number of sample components is not enough to make one fully-assembled PDMDB. Aim for a partially-assembled module modules
using DCDC, GBTX, VTTX, VTRX & GBT-SCA samples.
Design & layout is underway: motherboard with Kintex7; two different plugins, ECS & DAQ; motherboard could be made with production
PDMDB geometry: it would allow mechanical and thermal studies.
May need to replace the PDMDB due to radiation damage, after a certain number of years of operation.
Using sub-modules might be a benefit for the production.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
227
RICH2 thermo/mechanics
Structure composed by a cooled aluminum structural bar.
Support for harness coupled to cold bar.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
23
RICH2 column first prototypesAW5083 cast aluminum alloy plate
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
24
Housing of the EC and PDMDB
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
25
Overall dissipation per EC: 15 W/EC (total). Cooling of CLARO and BaseBoard depends on the
conductivity of PCB and connectors. Conductivity of connectors?
A factor 1000 between the conductivities of Cu and FR4: small quantities of copper changes dramatically the expected conductivity and thermal simulation results.
Neglected: contact resistances, convection, irradiation…
Thermal Conduction simulation
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
26
Both ducts with cylindrical inserts to leave 1 mm thick anularx-section...
Two ducts, 8 and 18 mm diam... Larger duct quite inefficient ..
Very preliminary CFD simulations(duct to coolant thermal exchange)
To reduce gradient 2 or more ducts shall be fluxed in opposite directions.
Large ducts: low speed and coolant stratification:inefficient exchange.
Ducts cross section to be modified to reduce stratification and increase exchange coefficient (e.g. inserts).
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
27
RICH2 PDA layout
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
28
Converging on a RICH1engineering design
Large boost in the last months, regular meetings. The intention is to design the RICH1 photon detector
region to allow an emergency intervention in a short technical stop of 5÷7 days (e.g. to replace EC).
Optical design finalized (i.e. fine tuned) via iterations taking into account a realistic engineering design.
Position of the photo-detector plane: now closer to beam line.
Mirror radius of curvature adjusted (3800 mm 3650 mm).
Quartz window position: at around its position in current RICH1.
The iron shielding box will be shaved by around ~70 mm (with gas enclosure tapered from 30 mm to 10 mm).
Converging on an open geometry for MAPMT housing. Can remove about 20 mm (10mm) from the top
(bottom) of the flat mirrors without any loss.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
29
Re-Using RICH2 components
RICH1 will inherit as much of the RICH2 design as possible.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
30
One Option
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
31
Current option
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
32
Patch Panel End
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
33
Cooling system end
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
34
Column insertion
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
35
RICH1 engineeringsummary status
Also good progress on the development of the gas enclosure, photon funnel, quartz window, exit window, mirrors and mounts.
Things are progressing quite nicely, although no room for complacency.
EDRs still on schedule for the end of the year.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
36
SYSTEM: grounding/shielding Started investigating closely grounding and shielding
issues.
HV and signal are coupled.
HV and LV couple different EC/PDM.
Kick-off meeting sponsored by Ken with a CERN G/S expert (Georges Blanchot).
Analyzed PDA at system level and decided architecture aiming at minimizing EMI at design level.
The required improvements have been implemented into the design.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
Past irradiation tests CLARO-CMOS chip (4 channels prototype):
23 MeV neutrons (Louvain); X-rays (50 kV tube, Legnaro); 60 MeV protons (Krakow).
CLARO8v0 chip: 28 MeV protons (Legnaro).
Hamamatsu UV-glass and borosilicate windows: 28 MeV protons (Legnaro).
BaseBoard and HV cables: CHARM facility (CERN).
CLARO8v1 chip: Ions (Louvain and Legnaro); 28 MeV protons (Legnaro).
MAROC3 chip 13 MeV protons and X-rays (Bucharest).
3709-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
Future irradiation tests
CLARO8v2 (SEE and total ionizing dose). PDMDB (test of FPGA +memory, radiation tolerance). MAPMT (degradation of QE, gain, uniformity; unfold
window transmittance). Other EC single components. Complete PDM (EC + PDMDB). Other thermo/mechanical and optical components.
3809-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
39
QA workshop in Edinburgh (april 2015)
Comprehensive review of Quality Assurance (QA): photo-sensors (MAPMT); CLARO chip; FEB & CLARO; full EC; data-bases, logistics, integration, commissioning,
… Emphasis on discussions:
schedules; procedural and technical solutions; manpower….
Outcome: agreed plans: all players are pulling in the same
direction!
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
40
What will be tested MAPMT: full characterization: tube & pixel gain (HV) (at
low and high illumination rate), dark counts, peak-to-valley ratio, signal loss, cross-talk, relative light yield (for some tubes: QE).
CLARO: currents, configure, readback, test pulse, charge injection.
FEB: s-curves for test pulse and charge injection (yielding thresholds and offsets).
EC: threshold scans with constant pulsed illumination at nominal HV (yielding optimum attenuation/threshold for each pixel).
Column functionality tests: communication and configuration fully functional, dark counts, signal from illumination at nominal HV.
Commissioning: initial configuration from QA results, HV scans with
dark counts and illumination, threshold/attenuation scans with target HV;
refinement of configuration.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
41
Workflow / Logistics
shipments: by industry
electronic components
Photon Detectors
no shipment needed
ECs
CERN site to pit
LH
Cb
QA
centr
es
CE
RN
Ind
ust
ry
R11265 & R12669production
CLARO chipproduction
FEBproduction
Base Boardproduction
EC mechanicsproduction
Ferrara Milano Krakow
CERN
LHCb pit
EC Assembly EC Assembly
EC QA EC QA
FEB QA
Hamamatsu ? ? ??
m-metal Assembly
Commissioning
Column Functionality Test
Edinburgh Padova
Photon Detector QA Photon Detector QA CLARO QA
Genova
FEB QA
CLARO QA*
FEB QA BB QA
CLARO QA mech QA?
EC Assembly:2x2 R112651x1 H12699
* = outsourced
EC Mounting on Columns
+ Digital Boards
Cambridge
+ m-metal
CERN?
DB QA
Back Boardproduction
?
BB QA
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
42
Column Assembly and Commissioning
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
43
Test-Beam 2014 An easy and robust concept was
developed. Cherenkov light was immediately
observed. We learnt many things, but still a
lot to learn… A paper is being written.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
At first the light is totally internal reflected
Reflective layer on the spherical surface
Absorber layer to choose the photons created in 1 cm of material.
44
Photo of one TB module.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
45
Defining proceduresof threshold scan
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
46
RICH testbeam 2015
Follow the same concept as 2014. Main objectives:
Test CLARO8v2 Reach lower threshold
Understand better detection efficiency Test a bigger system
More/full elementary cells Test under different loads/temperatures Test prototype mechanics?
If time allows: Test with gas radiator.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
47
New full circular lens
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
A few materials were investigated for lenses: Glass, Quartz, LiF, CaF2; different sizes and radiuses.
Although with some materials a better resolution can be achieved, the dominant part is always the pixel size.
Borosilicate glass is cheap and readily available.
48
First concept
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
49
RICH upgrade status summary
Tests of both types of MAPMT are continuing (R11265 and R12699). BaseBoard for MAPMT ready for pre-production; case in pre-
production. CLARO8v2.0 submitted beginning of April; back mid-August. FEB and BackBoard design finalized. Last adjustments to all EC components, following EDR and TB. Study/definition of grounding/shielding scheme (LV, HV, Signal,
safety…). Design of components for the low-occupancy parts of RICH2
(R12699) started. Prototypes of column thermo/mechanics are ready. Cooling studies/design started. RICH1 challenging engineering is progressing fast; optical layout
fine-tuned. Irradiation program on-going. QA and tests facilities sorted out; labs are setting-up. Paper on 2014 TB 2014 is being written; preparing for the test
beams of 2015. Inventory/Bookkeeping/Connectivity DB is being built. Infrastructure Document for Technical Coordination being finalized. Order for MAPMT and common components will soon go out.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.
50
The End
Good progress all over the project.
Schedule and Milestones are being tuned, in agreement and via negotiations with the management, to also take into account external (varying) schedules.
09-06-2015 @CERNAlessandro Petrolini
Dipartimento di Fisica UNIGE and INFN.