Deep Underground Neutrino Experiment (DUNE)
1
Technical Proposal
2
23 Feb 2018: First draft of the TP volumes due
3
Volume 2: The Single-Phase Far Detector
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February 26, 2018
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Deep Underground Neutrino Experiment (DUNE) 1 Technical Proposal 2 - - PDF document
Deep Underground Neutrino Experiment (DUNE) 1 Technical Proposal 2 23 Feb 2018: First draft of the TP volumes due 3 Volume 2: The Single-Phase Far Detector 4 February 26, 2018 5 1 Contents 1 Contents i 2 List of Figures iii 3 List
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February 26, 2018
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1
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Contents i
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List of Figures iii
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List of Tables iv
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1 TPC Electronics 1
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1.1 System Overview . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
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1.1.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
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1.1.2 Design Considerations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
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1.1.3 System Requirements . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
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1.2 System Design . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 6
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1.2.1 Grounding and Shielding . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 6
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1.2.2 Distribution of Wire-Bias Voltages . . . . . . . . . . . . . . . . . . . . . . . . 7
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1.2.3 Front-End Mother Board (FEMB) . . . . . . . . . . . . . . . . . . . . . . . . . 9
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1.2.4 Additional FEMB/ASIC Designs . . . . . . . . . . . . . . . . . . . . . . . . . . 15
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1.2.5 Cold Electronics Feedthroughs and Cold Cables . . . . . . . . . . . . . . . . . . 19
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1.2.6 Warm Interface Electronics . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21
16
1.2.7 External Power and Supplies . . . . . . . . . . . . . . . . . . . . . . . . . . . . 24
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1.3 Production and Assembly . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25
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1.4 Interfaces . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25
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1.4.1 Overview . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25
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1.4.2 APAs . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26
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1.4.3 DAQ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27
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1.5 Quality Assurance . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28
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1.5.1 Initial Design Validation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28
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1.5.2 Integrated Test Facilities . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28
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1.6 Quality Control . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33
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1.7 Installation, Integration, and Commissioning . . . . . . . . . . . . . . . . . . . . . . . 33
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1.7.1 Installation and Integration with APAs . . . . . . . . . . . . . . . . . . . . . . 33
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1.7.2 Calibration . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35
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1.8 Safety . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35
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1.9 Organization and Management . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 36
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1.9.1 Single-Phase TPC Electronics Consortium Organization . . . . . . . . . . . . . 36
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1.9.2 Planning Assumptions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 36
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1.9.3 WBS and Responsibilities . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37
34
i
1.9.4 High-level Cost and Schedule . . . . . . . . . . . . . . . . . . . . . . . . . . . 37
1
References 39
2 3
ii
1
1.1 Connections between the signal flange and APA at ProtoDUNE-SP. The interface be-
2
tween the electronics chain, the APAs, and the cryostat will be very similar at the DUNE
3
far detector. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
4
1.2 APA wire bias schematic diagram, including the CR board. . . . . . . . . . . . . . . . . 8
5
1.3 The CE architecture. The basic unit is the 128-channel FEMB. . . . . . . . . . . . . . 9
6
1.4 The complete FEMB assembly as used in the ProtoDUNE-SP detector. The cable shown
7
is the high-speed data, clock, and control cable. . . . . . . . . . . . . . . . . . . . . . 10
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1.5 Measured pulse response with details on gain, peaking time and baseline adjustments. . 11
9
1.6 Baseline cold ADC ASIC block diagram. . . . . . . . . . . . . . . . . . . . . . . . . . 12
10
1.7 Block diagram of COLDATA ASIC design. . . . . . . . . . . . . . . . . . . . . . . . . 14
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1.8 Prototype CE Box used in ProtoDUNE-SP. . . . . . . . . . . . . . . . . . . . . . . . . 15
12
1.9 Overall architecture of the CRYO ASIC. . . . . . . . . . . . . . . . . . . . . . . . . . . 16
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1.10 Depiction of the substrate isolation technique that allows combining analog and digital
14
circuitry on the same CRYO ASIC. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17
15
1.11 Block diagram of the DRE architecture for the ATLAS ADC ASIC. . . . . . . . . . . . 18
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1.12 Block diagram depicting the two-stage SAR design of the ATLAS ADC ASIC. . . . . . . 18
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1.13 TPC CE feedthrough. The WIBs are seen edge-on in the left panel,and in an oblique
18
side-view in the right panel, which also shows the warm crate for a DUNE module in a
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cutaway view. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19
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1.14 Exploded view of the signal flange for ProtoDUNE-SP. . . . . . . . . . . . . . . . . . . 21
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1.15 Power and Timing Card (PTC) and timing distribution to the WIB and FEMBs. . . . . 22
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1.16 LV power distribution to the WIB and FEMBs. 250W is for a fully-loaded crate with the
23
majority of the power dissipated by the 20 cold FEMBs in the LAr. . . . . . . . . . . . 22
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1.17 Warm Interface Board (WIB). Note that front panel inputs include a LEMO connector
25
and alternate inputs for LV power. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23
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1.18 FCi micro TCA power connector at the PTC end of the cable. . . . . . . . . . . . . . . 24
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1.19 ENC (in electrons) and temperature (in degrees Kelvin) as a function of cold cycle time
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in GN2 for ProtoDUNE-SP APA2. At the lowest temperature of 160K, the wrapped
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wires measured 480e− noise and the straight wires 400e−. . . . . . . . . . . . . . . . . 30
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1.20 Picture of the shielded room at Fermilab. . . . . . . . . . . . . . . . . . . . . . . . . . 32
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1.21 Left: one side of the 40% APA with 4 FEMBs. Right: the full CE feedthrough and flange. 32
32 33
iii
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1.1 TPC electronics components and quantities for the DUNE single-phase far detector. . . 3
2
1.2 Baseline cold ADC ASIC configurability. . . . . . . . . . . . . . . . . . . . . . . . . . . 13
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1.3 Performance requirements for the ATLAS-style ADC ASIC. . . . . . . . . . . . . . . . . 17
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iv
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There are some placeholders for citations here; need to revisit how to cite e.g. interface
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25
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This section will be written for the second draft of the technical proposal. . . . . . . . . 33
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This section will be written for the second draft of the technical proposal. . . . . . . . . 35
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Please note that these dates may need to be revisited and that there may be more
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time available prior to the beginning of construction. . . . . . . . . . . . . . . . . . 36
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This section will be written for the second draft of the technical proposal. . . . . . . . . 37
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This section will be written for the second draft of the technical proposal. . . . . . . . . 37
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v
Chapter 1: TPC Electronics 1–1
1
2
ch:fdsp-tpc-elec
3
sec:fdsp-tpc-elec-ov
4
sec:fdsp-tpc-elec-ov-intro
The DUNE single-phase TPC readout electronics are often referred to as the “Cold Electronics”
5
(CE) given that they reside in the liquid argon, mounted directly on the APA. The charge carrier
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mobility in silicon is higher and thermal fluctuations are lower at liquid argon temperature than at
7
room temperature. For CMOS electronics, this results in substantially higher gain and lower noise
8
at liquid argon temperature than at room temperature
LArCMOS
[54]. Mounting the front-end electronics
9
10
multiplexing (MUX) electronics inside of the cryostat allows for a reduction in the total number
11
12
reducing the expense and complexity of the experiment. As the full TPC electronics chain for
13
the single-phase detector includes many components on the warm side of the cryostat as well, the
14
DUNE consortium designated to organize CE development is referred to as the DUNE “Single-
15
Phase TPC Electronics” consortium.
16
The lower noise levels (by about a factor of two) enabled by having the front-end electronics in the
17
cold greatly extends the reach of the DUNE physics program
LArCMOS
[54]. The CP violation and neutrino
18
mass ordering measurements depend on a precise characterization of the reconstructed neutrino
19
energy spectrum; improving the charge resolution as much as possible (by lowering noise levels in
20
the wire readout) allows for one to better resolve features in reconstructed neutrino energy spectrum
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that are relevant for these physics measurements. Decreasing the noise level also allows for smaller
22
charge deposits to be measurable, which acts as a source of risk mitigation in the case that the
23
electron lifetime in the detector is lower than desired (due to the prevelance of electronegative
24
impurities in the detector), and also increases the reach of low-energy physics measurements such
25
as those associated with stellar core-collapse supernova burst neutrinos. Finally, the low noise
26
levels allows the experiment to utilize low-energy 39Ar beta decays for the purpose of precision
27
calibration in the DUNE far detector.
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23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–2
An extensive discussion of the TPC electronics system design is given in Section
sec:fdsp-tpc-elec-design
1.2. What
1
immediately follows is a brief overview of the major design considerations for the cold electronics
2
to be used in the DUNE single-phase far detector.
3
4
sec:fdsp-tpc-elec-ov-consid
The CE signal processing is implemented in application-specific integrated circuit (ASIC) chips
5
using CMOS technology, which has been demonstrated to perform well at cryogenic temperatures,
6
and includes amplification, shaping, digitization, buffering, and multiplexing (MUX) of the signals.
7
The CE is continuously read out, resulting in a digitized ADC sample from each APA channel (wire)
8
up to every 500 ns (2 MHz sampling rate).
9
Each individual APA has 2,560 channels that are read out by 20 Front-End Motherboards (FEMBs),
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with each FEMB providing digitized wire readout from 128 channels. One cable bundle connects
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each FEMB to the outside of the cryostat via a feedthrough (a CE feedthrough) in the signal
12
cable flange at the top of the cryostat, where a single flange services each APA, as shown in Fig-
13
ure
fig:connections
1.1. Each cable bundle contains wires for low-voltage (LV) power, high-speed data readout, and
14
clock/digital-control signal distribution. Eight separate cables carry the TPC wire-bias voltages
15
from the signal flange to the APA wire-bias boards.
16
Figure 1.1: Connections between the signal flange and APA at ProtoDUNE-SP. The interface between the electronics chain, the APAs, and the cryostat will be very similar at the DUNE far detector.
fig:connections
The components of the CE system are the following:
17
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–3
1
2
and the signal flanges (cold cables);
3
4
APA wire-bias voltages between the inside and outside of the cryostat;
5
6
the warm interface boards (WIBs) and power and timing cards (PTCs) for further processing
7
and distribution of the signals entering/exiting the cryostat;
8
9
acquisition (DAQ) and slow control systems;
10
11
supplies (warm cables); and
12
13
The electrical cables for each APA enter the cryostat through a single signal flange, creating an
14
integrated unit that provides local diagnostics for noise and validation testing, and follows the
15
grounding guidelines in Section
sec:fdsp-tpc-elec-design-ground
1.2.1. The components, the quantity of each required for the
16
DUNE far detector, and the number of channels that each component has, are listed in Table
tab:elecNums
1.1.
17
Table 1.1: TPC electronics components and quantities for the DUNE single-phase far detector. Element Quantity Channels per element APA 150 2,560 Front-end mother board (FEMB) 20 per APA 128 FE ASIC chip 8 per FEMB 16 ADC ASIC chip 8 per FEMB 16 COLDATA ASIC chip 2 per FEMB 64 Cold cable bundle 1 per FEMB 128 Signal flange 1 per APA 2,560 CE feedthrough 1 per APA 2,560 Warm interface board (WIB) 5 per APA 512 Warm interface electronics crate (WIEC) 1 per APA 2,560 Power and timing card (PTC) 1 per APA 2,560 Passive Backplane (PTB) 1 per APA 2,560
tab:elecNums
The baseline design for the DUNE far detector single-phase TPC electronics calls for three types
18
19
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Chapter 1: TPC Electronics 1–4
1
2
The front-end ASIC has been prototyped and is close to meeting requirements (discussed in Sec-
3
tion
sec:fdsp-tpc-elec-ov-req
1.1.3). Key portions of the control and communications ASIC (also referred to as the COL-
4
DATA ASIC) have been prototyped and meet requirements. However, it has been determined that
5
the ADC ASIC now being used in ProtoDUNE-SP does not meet requirements, and accordingly,
6
its development has been terminated. A new cold ADC ASIC is being developed by an LBL-
7
FNAL-BNL collaboration and first prototypes are expected by the end of summer 2018. The first
8
full prototype of the controls and communication ASIC is also expected to be available for testing
9
by the end of the summer 2018. In order to maximize the probability of developing a complete
10
design for cold TPC front-end electronics in a timely fashion, an alternative solution is also being
11
investigated, a single 64-channel ASIC that will include all three functions described above. This
12
design is being done at SLAC and first prototypes are expected late in spring or early summer
13
2018.
14
A series of tests are planned to demonstrate that at least one of these designs will meet DUNE
15
16
and one using a new small liquid argon TPC at Fermilab. The latter will also accommodate one
17
half-length DUNE photodetector, and will provide a low noise environment that will allow one to
18
make detailed comparisons of the performance of the new ASICs. It will also enable the study
19
20
and the HV distribution. These test facilities are discussed in more detail in Section
sec:fdsp-tpc-elec-qa-facilities
1.5.2.
21
22
sec:fdsp-tpc-elec-ov-req
The core components of the TPC electronics subsystem are the FEMB ASICs that perform shaping,
23
digitization, and multiplexing of channel data in the cold. Two basic requirements for the ASIC
24
designs are:
25
26
plane in 30 years of operation); and
27
28
If multiple ASIC designs meet these two requirements, the down-select decision will be based
29
30
performance will be given the largest weight.
31
For the FE ASICs, more specific requirements include:
32
33
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23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–5
1
2
3
4
A secondary performance measurement is dynamic range. If noise or linearity depends on the gain
5
setting, then most weight (90%) will be given to the setting with best performance for which an
6
impulse of 85 fC at the input does not saturate the output.
7
Additional ADC ASIC requirements are:
8
9
10
11
12
channel and chip-to-chip.
13
Finally, specific requirements of the COLDATA ASIC design include:
14
15
16
in length.
17
In addition to these requirements on the ASICs, the TPC electronics subsystem must also:
18
19
the DAQ;
20
21
22
23
24
ton conversions, optimize the reconstruction of high-energy and low-energy tracks from
25
accelerator-neutrino interactions, distinguish a minimum-ionizing particle (MIP) from noise
26
with a signal-to-noise ratio of 9:1 or greater, and measure ionization up to 15 times that of
27
a MIP so that stopping kaons from proton decay can be identified;
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23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–6
1
control through the DAQ, and over-current and over-voltage protection circuits; and
2
3
with a maximum specified leakage current in 1-atm argon gas.
4
The quality assurance (QA) process, described in Section
sec:fdsp-tpc-elec-qa
1.5, will make use of both initial valida-
5
tion procedures using electronics test stands as well as integrated test facilities in order to ensure
6
that final component designs satisfy the above requirements. Once component designs have been
7
decided upon, the quality control (QC) process will employ similar requirements to make sure that
8
every component to be installed in the DUNE single-phase far detector is up to standard. This is
9
described in more detail in Section
sec:fdsp-tpc-elec-qc
1.6.
10
11
sec:fdsp-tpc-elec-design
12
sec:fdsp-tpc-elec-design-ground
The goal of the cold electronics system design is to minimize inherent system noise at the input of
13
the FE pre-amplifier while providing sufficient precision and dynamic range to achieve the DUNE
14
physics goals, as detailed in Section
sec:fdsp-tpc-elec-ov-consid
1.1.2. To accomplish this, the electrical cables for each APA
15
enter the cryostat through a single signal flange, creating an integrated unit that provides local
16
diagnostics for noise and validation testing.
17
To avoid structural ground loops, the APA frames described in Section APAFRAME are insulated
18
from each other. Each frame is electrically connected to the cryostat at a single point on the CE
19
feedthrough board in the signal flange where the cables exit the cryostat. Mechanical suspension
20
21
The analog portion of the FEMB contains eight front-end ASICs configured as 16-channel digitizing
22
charge amplifiers. Input amplifiers on the ASICs have their ground terminals connected to the
23
APA frame. All power-return leads and cable shields are connected to both the ground plane of
24
the FEMB and to the signal flange.
25
Filtering circuits for the APA wire-bias voltages are locally referenced to the ground plane of the
26
FEMBs through low-impedance electrical connections. This approach ensures a ground-return
27
path in close proximity to the bias-voltage and signal paths. The close proximity of the current
28
paths minimizes the size of potential loops to further suppress noise pickup.
29
Photon detector signals, described Section PD, are carried directly on shielded, twisted-pair cables
30
to the signal flange. The cable shields are connected to the cryostat at a second feedthrough, the
31
PDS feedthrough, and to the PCB shield layer on the photon detectors. There is no electrical
32
connection between the cable shields and the APA frame except at the signal flange.
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23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–7
The frequency domain of the TPC wire and photon detector signals are separate. The wire readout
1
digitizes at 2 MHz with < 500 kHz bandwidth at 1 µsec peaking time, while the photon readout
2
3
(50 MHz) and common noise frequencies through the FE ASIC and cabling designs. All clock
4
signals are transmitted differentially with individual shield to avoid the interference to power
5
lines.
6
7
sec:fdsp-tpc-elec-design-bias
Each side of an APA includes four wire layers as described in Section APADESIGN. The innermost
8
X-plane layer of wires is nominally biased at +820 Volts, with each wire AC coupled to one of
9
the 128 charge amplifier circuits on the FEMB. The V-plane wire layer is effectively biased at
10
zero volts, with each wire directly connected to one of the charge amplifier circuits. The U-plane
11
wire layer is nominally biased at −370 Volts with each wire AC-coupled to one of the 128 charge
12
amplifier circuits. The outermost G-plane wire layer, which has no connection to the charge
13
amplifier circuits, is biased at −665 Volts.
14
Electrons passing through the wire grid must drift unimpeded until they reach the X-plane col-
15
lection layer. The nominal bias voltages are predicted to result in this electrically transparent
16
configuration.
17
As described in Section APAWIRE the filtering of wire-bias voltages and AC coupling of wire
18
signals passing onto the charge amplifier circuits is done on capacitance-resistance (CR) boards
19
that plug in between the APA wire-board stacks and FEMBs. Each CR board includes single
20
R-C filters for the X- and U-plane wire-bias voltages. In addition, each board has 48 pairs of bias
21
resistors and AC coupling capacitors for X-plane wires, and 40 pairs for the U-plane wires. The
22
coupling capacitors block DC while passing AC signals to the CE motherboards. A schematic
23
diagram of the APA wire bias subsystem is illustrated in Figure
fig:CR-board
1.2.
24
Separate CR boards include a single R-C filter for the G-plane wires and 12 pairs of bias resistors
25
and coupling capacitors. Groups of four wires are tied together to share single bias resistors and
26
filter capacitors. These CR boards do not connect to the charge amplifier circuits on the FEMB.
27
Clamping diodes limit the input voltage received at the amplifier circuits to between 1.8V ± U_D,
28
where U_D is the breakdown voltage of the diode ∼0.7V. The amplifier circuit has a 22-nF coupling
29
capacitor at input to avoid leakage current from the protection clamping diodes.
30
Coupling capacitors for the X-plane and U-plane wires are required to block DC bias voltages.
31
However they also impact the efficiency of the detector circuits. The sense wires are expected
32
to have ∼ 200 pF of capacitance to the APA frame. Induced or collected charges are effectively
33
divided between the wire capacitance and the coupling capacitor. To achieve a charge-calibration
34
accuracy of 0.5 percent or better, the coupling capacitors must be 4.7 nF at ten percent tolerance,
35
Voltage ratings should be at least 1.5 times the expected
36
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23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–8
Figure 1.2: APA wire bias schematic diagram, including the CR board.
fig:CR-board
Bias resistance values should be at least 20 MΩ to maintain negligible noise contributions. A
1
target value of 50 MΩ is desired. The higher value helps to achieve a longer time constant for the
2
high-pass coupling networks. Time constants should be at least 25 times the electron drift time so
3
that the undershoot in the digitized waveform is small and easily correctable. However, leakage
4
currents can develop on PC boards that are exposed to high voltages over extended periods. If the
5
bias resistors are much greater than 50 MΩ, leakage currents may affect the bias voltages applied
6
to the wires.
7
The bias-voltage filters are R-C low-pass networks. Resistance values should be much smaller than
8
the bias resistances to control crosstalk between wires and limit the voltage drop if any of the wires
9
becomes shorted to the APA frame. A value around 2.2 MΩ is desired. Smaller values may be
10
considered although a larger filter capacitor would be required to maintain a given level of noise
11
12
For the grid-plane bias filters, component values are less critical. If possible they will be identical
13
to those used for the bias resistors and coupling capacitors (50 MΩ and 2.2 to 4.7 nF).
14
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–9
1
sec:fdsp-tpc-elec-design-femb
The main component of the CE architecture, illustrated in Figure
fig:ce-scheme
1.3, is the 128-channel FEMB,
2
which itself consists of an analog motherboard and an attached COLDATA mezzanine card for
3
processing the digital outputs. Each APA is instrumented with 20 FEMBs, for a total of 2,560
4
channels per APA. The FEMBs plug directly into the APA CR boards, making the connections
5
from the U- and V-plane induction wires and X-plane collection wires to the charge amplifier
6
circuits as short as possible.
7 COLDATA COLDATA
Figure 1.3: The CE architecture. The basic unit is the 128-channel FEMB.
fig:ce-scheme
1.2.3.1 Overview
8
sec:fdsp-tpc-elec-design-femb-ov
The analog mother board is instrumented with eight 16-channel FE ASICs, eight 16-channel ADC
9
ASICs, LV power regulators, and input-signal protection circuits. The 16-channel FE ASIC pro-
10
vides amplification and pulse shaping. The 16-channel ADC ASIC comprises 12-bit digitizers
11
performaning at speeds up to 2 MS/s, local buffering, and an 8:1 MUX stage with two pairs of
12
serial readout lines in parallel. The 2017 ProtoDUNE Single Phase (ProtoDUNE-SP) version of
13
the FEMB is shown in Figure
fig:femb
1.4.
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23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–10
Figure 1.4: The complete FEMB assembly as used in the ProtoDUNE-SP detector. The cable shown is the high-speed data, clock, and control cable.
fig:femb
1.2.3.2 Front-End ASIC
1
sec:fdsp-tpc-elec-design-femb-fe
Each FE ASIC channel has a charge amplifier circuit with a programmable gain selectable from
2
3
aliasing filter with programmable time constant (peaking time 0.5, 1, 2, and 3 µs), an option to
4
enable AC coupling, and a baseline adjustment for operation with either the collecting (200 mV)
5
6
circuits, programming registers, a temperature monitor, an analog buffer for signal monitoring,
7
and the digital interface. The estimated power dissipation of FE ASIC is about 6 mW per channel
8
at 1.8 V supply.
9
The ASIC was implemented using the commercial CMOS process (0.18 µm and 1.8 V), which is
10
expected to be available for at least another 10 years. The charge amplifier input MOSFET is a
11
p-channel biased at 2 mA with a L/W (channel length/width) ratio of 0.27 µm / 10 µm, followed
12
by dual cascade stages.
13
Each channel also implements a high-performance output driver, which can be used to drive a
14
long cable, but is disabled when interfaced to an ADC ASIC to reduce the power consumption.
15
The ASIC integrates a band-gap reference (BGR) to generate all the internal bias voltages and
16
17
including cryogenic. The ASIC is packaged in a commercial, fully encapsulated plastic QFP 80
18
package.
19
Each FE ASIC channel is equipped with an injection capacitor which can be used for test and
20
calibration and can be enabled or disabled through a dedicated register. The injection capaci-
21
tance has been measured using a calibrated external capacitor. The measurements show that the
22
calibration capacitance is extremely stable, changing from 184 fF at RT to 183 fF at 77 K. This
23
result and the measured stability of the peaking time demonstrate the high stability of the passive
24
components as a function of temperature. Channel-to-channel and chip-to-chip variation in the
25
calibration capacitor are typically less than 1%.
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2 4 6 8 0.0 0.2 0.4 0.6 0.8 Amplitude [V] Time [µs] T=300K T=77K Gain 25 mV/fC Peaking time 1µs Pole-zero cancellation at 77K to be addressed in next revision
⎩ ⎨ ⎧ ° ° ≈ K 77 at V 164 . 1 K 300 at V 185 . 1 VBGR
Bandgap Reference
10 20 30 40 50 Amplitude [a.u.] Time [µs] Peak time [µs] 0.5 1.0 2.0 3.0 collecting mode non-collecting mode gain [mV/fC] 25 14 7.8 4.7
Adjustable gain , peaking time and baseline
maximum charge 55, 100, 180, 300fC
variation = 1.8 % ⎩ ⎨ ⎧ ° ° ≈ K 77 at V m 3 . 259 K 300 at mV . 867 VTMP
Temperature Sensor ~ 2.86 mV / K
Figure 1.5: Measured pulse response with details on gain, peaking time and baseline adjustments.
fig:fe-output
Prototype ASICs have been evaluated and characterized at RT (300 K) and LN2 (77 K) temper-
1
2
and operated without any change in performance. Figure
fig:fe-output
1.5 shows the measured pulse response,
3
both as a function of temperature and the programmable settings of the chip. These results are
4
in close agreement with simulations and indicate that both the analog and the digital circuits and
5
interface operate as expected in a cryogenic environment.
6
1.2.3.3 ADC ASIC
7
sec:fdsp-tpc-elec-design-femb-adc
The baseline option for the DUNE Cold ADC is a 16-channel low-noise ADC ASIC intended to read
8
9
and it digitizes at a rate of 2 MS/s/channel. The ADC accepts single-ended or differential inputs,
10
and outputs a serial data stream to COLDATA, the DUNE digital serializer chip. The ADC ASIC
11
is implemented using 65 nm CMOS technology. The ASIC uses a conservative, industry standard
12
design along with digital calibration. A block diagram of the ADC ASIC is shown in Figure
fig:adc-blockdiagram
1.6.
13
Each Cold ADC receives 16 single-ended voltage outputs from a single LARASIC chip. The voltage
14
is buffered and then sampled at a rate of 2 MS/s. The analog samples are multiplexed by 8 and
15
digitized by calibrated 12-bit pipelined ADCs operating at 16 MS/s. The ADC uses the well-known
16
Pipelined architecture with redundancy to reduce the impact of component non-idealities on the
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S/H Correction Logic Data Formatter IN0 IN7 I2C DIG_OUTA(P/N) DIG_OUTB(P/N) I2C_(SCL,SDA, SDO) CLK_64MHZ(P/N) S/H 12-bit 16 MS/s Pipelined ADC DIG_FRAME(P/N) DIG_CLKOUT(P/N) Ref Generation and Buffers
Cold ADC
8-1 MUX DIG_OUTC(P/N) DIG_OUTD(P/N) LVDS I/O BUFFER BUFFER S/H Correction Logic IN8 IN15 S/H 12-bit 16 MS/s Pipelined ADC 8-1 MUX BUFFER BUFFER UART MISO/MOSI Configuration and Debug Interface Async FIFO Async FIFO IMONITOR VMONITOR DIG_OUTE(P/N) DIG_OUTF(P/N) DIG_OUTG(P/N) DIG_OUTH(P/N) CLK_16MHZ(P/N) CLK_2MHZ(P/N) I2C_ADD SSO_(FRAME, DATA[1:0], CLK) VREF(P,N,CMI,CMO), BGR VDD/VSS domains LVDS_REF Calibration Engine Calibration Engine 30 30 16 30 16 16
Figure 1.6: Baseline cold ADC ASIC block diagram.
fig:adc-blockdiagram
linearity of the ADC
121557
[50]. The linearity of the raw output samples from the ADCs is improved
1
using an on-chip calibration. The corrected ADC output is then multiplexed onto eight LVDS
2
channels and sent to COLDATA for further aggregation and transmission via a copper link to the
3
warm electronics sitting outside the cryostat.
4
The ADC ASIC is designed for low-noise operation. The noise specification is 175 ÂţV-rms. This
5
noise specification was chosen to ensure that LARASIC will dominate the overall noise performance
6
7
The ADC is digitally calibrated using the proven Soenen-Karanicolas algorithm
280084,372864
[51, 52]. The
8
algorithm exploits the observation that in a pipelined ADC with redundancy, the ADC nonlinearity
9
is caused almost entirely by errors in the closed-loop interstage gain
121557
[50]. Traditionally, the ADC
10
11
However, due to unavoidable non-idealities such as finite op-amp gain and capacitor mismatch,
12
the true radix of each stage is slightly different from two. The extent to which the true radix
13
is different from two leads to DNL and INL in the ADC transfer characteristic. The Soenen-
14
Karanicolas algorithm provides a way to measure the radix of a given stage by forcing events
15
at the decision boundaries and using the following stages of the ADC to record the stageâĂŹs
16
17
ADC output is converted from the true radix to radix 2 using pipelined digital adders. This
18
way, static linearity can be greatly improved without any post-processing required. To provide
19
additional ease-of-use, all calibration hardware (including test signal generation) is included on the
20
ADC ASIC. To control power dissipation, the stages of the ADC are scaled in area in power to take
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advantage of the fact that the accuracy requirements of the stages decline down the pipeline
494191
[53].
1
To reduce the number of pads and to improve performance all required reference voltages and
2
currents are generated internally by a resistor-programmed reference generator on the ASIC.
3
The Cold ADC is highly configurable (see Table
tab:ADCconfig
1.2) and includes two redundant slow control
4
interfaces for configuration (either UART or I2C). The configurability of the chip is included
5
primarily to reduce risk by providing a high degree of flexibility and observability. First, many of
6
the components on the ASIC can be bypassed and their functions assumed at the board level if
7
8
can be bypassed. Second, the ADC digital calibration algorithm can be implemented externally
9
with the calculated stage weights loaded back into the chip using the configuration interface. Third,
10
various internal voltages and currents can be monitored and test data can be introduced at various
11
parts of the digital processing to observe the function of the ASIC. Lastly, the bias point of the
12
analog circuits in the ASIC can be adjusted to compensate for expected component variations
13
between room temperature and liquid Argon temperature.
14
Table 1.2: Baseline cold ADC ASIC configurability. BLOCK Configurability Comment Input Buffer Single-ended/differential, bypass, bias current adjust Reduces design risk Sample-and-hold Amplifiers Multiplexer freeze, bias current adjust Simplifies evaluation of prototype ADC Bias currents, clock edge fine adjustment, sync and test modes Simplifies evluation of prototype and reduces risk References All reference voltages can be adjusted in 8 mV in- crements; all references can be powered down and external voltages used Reduces design risk Calibration Number of stages and amount of digital filtering; all calibration commands can be implemented through configuration interface for offline calibration; known data can be injected at various points for testing Simplifies evaluation of prototype and reduces risk Output Monitor Various internal bias voltages and currents can be sent off-chip for evaluation Simplifies evaluation of prototype
tab:ADCconfig
1.2.3.4 COLDATA ASIC
15
sec:fdsp-tpc-elec-design-femb-coldata
The COLDATA ASIC is responsible for all communication between the cold TPC electronics
16
17
18
ADC ASICs and relays commands to the LArASIC front-end and to the Cold ADC ASICs to
19
set operating modes and initiate calibration procedures. COLDATA receives data from the ADC
20
ASICs, reformats these data, merges data streams, formats data packets, and sends these data
21
packets to the warm electronics using 1.28 Gbps links. These links are designed for use with 30
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m long cables and include line drivers with pulse preemphasis. A block diagram of COLDATA is
1
shown in Figure
fig:coldata
1.7.
2
Figure 1.7: Block diagram of COLDATA ASIC design.
fig:coldata
COLDATA is designed in 65 nm CMOS using “cold” transistor models based on data collected by
3
members of the FNAL, BNL, and SMU ASIC groups. A special library of standard cells, based
4
5
6
hot carrier effect. The digital sections of COLDATA use these standard cells and were synthesized
7
from RTL using automatic place and route tools. Key circuit elements of COLDATA, including
8
the control interface and the PLL and serializer, were prototyped successfully in 2017. Submission
9
10
1.2.3.5 Cold Electronics Box
11
sec:fdsp-tpc-elec-design-femb-box
Each FEMB is enclosed in a mechanical “Cold Electronics Box” to provide support, cable strain
12
relief, and control of gas Argon bubbles in the LAr from the FEMB attached to the lower APA. As
13
shown in Figure
fig:ce-box
1.8, the CE Box is designed to make the electrical connection between the FEMB
14
and the APA frame, as defined in Section
sec:fdsp-tpc-elec-design-ground
1.2.1. Mounting hardware inside the CE Box connects
15
the ground plane of the FEMB to the box casing. The box casing is electrically connected to the
16
APA frame via twisted conducting wire (not shown in Figure
fig:ce-box
1.8). This is the only point of contact
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between the FEMB and APA, except for the input amplifier circuits connected to the CR board,
1
which also terminate to ground at the APA frame, as shown in Figure
fig:CR-board
1.2.
2
Figure 1.8: Prototype CE Box used in ProtoDUNE-SP.
fig:ce-box
3
sec:fdsp-tpc-elec-design-alt
In addition to the baseline FEMB and ASIC designs discussed in Section
sec:fdsp-tpc-elec-design-femb
1.2.3, there are other
4
FEMB and ASIC options currently being considered as well. This allows for risk mitigation in the
5
case that the baseline ADC ASIC design does not pass the requirements laid out in Section
sec:fdsp-tpc-elec-ov-scope
??.
6
There is one official alternative design, the SLAC-designed nEXO three-chip “CRYO” ASIC, and
7
8
are described in Section
sec:fdsp-tpc-elec-design-alt-cryo
1.2.4.1 and Section
sec:fdsp-tpc-elec-design-alt-atlas
1.2.4.2, respectively.
9
1.2.4.1 nEXO CRYO ASIC
10
sec:fdsp-tpc-elec-design-alt-cryo
The SLAC CRYO ASIC differs from the "baseline" three-chip design in that it combines the
11
functions of an analog pre-amp, ADC and data serialization/transmission, for 64 wire channels,
12
into a single chip. It is based on a design developed for the nEXO experiment and differs from it
13
14
the DUNE wires compared to the small pads of nEXO. FEMBs constructed using this chip would
15
use only 2 ASICs compared to the 18 (8 FE, 8 ADC and 2 COLDDATA) neeeded in the baseline
16
17
power, and reduce costs related to production and testing.
18
Figure
fig:cryo-architecture
1.9 shows the overall architecture of the CRYO ASIC, which will be implemented in 130
19
nm CMOS. It comprises two identical, 32-channel blocks. The current signal from each wire is
20
amplified using a pre-amp with pole zero cancellation and an anti-alias fifth-order Bessel filter
21
22
to values similar to those of the baseline design.
23
The ADC is 8 MSPS Successive Approximation Registration (SAR), so that four input channels are
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Figure 1.9: Overall architecture of the CRYO ASIC.
fig:cryo-architecture
multiplexed onto a single ADC. The data serialization and transmission block employs a custom
1
12b/14b encoder, so that 32 channels of 12 bit, 2 MSPS data can be transmitted with a digital
2
bandwidth of only 896 Mb/s, which is significantly less than the required bandwidth of the baseline,
3
which is 1.27 Gb/s.
4
One key concern with "mixed signal" ASICs is the possibility of interference from the digital side
5
causing noise on the very sensitive pre-amp. Fortunately, there are well established techniques
6
for "substrate isolation" described in the literature
yeh
[49], which have been successfully employed
7
in previous ASICs produced by the SLAC group. Figure
fig:cryo-substrate
1.10 shows how substrate isolation is
8
achieved.
9
The infrastructure requirements for a CYRO ASIC-based system are similar to those of the baseline
10
11
12
using internal voltage regulators.
13
14
lower than the baseline option due to the custom 12b/14b encoder of the CRYO chip.
15
16
protocol is SACI rather than I2C.
17
The first prototype of the CRYO ASIC is in the final design and simulation stages. Simulation-
18
based studies have already been performed; at 0.8 µS peaking time, the ENC is approximately
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Figure 1.10: Depiction of the substrate isolation technique that allows combining analog and digital circuitry on the same CRYO ASIC.
fig:cryo-substrate
500e−. Submission to the ASIC foundry is imminent and the first protypes should be received in
1
2
for a small test TPC at FNAL and on an APA in the ProtoDUNE-SP cold box; these test facilities
3
are described in Section
sec:fdsp-tpc-elec-qa-facilities
1.5.2.
4
1.2.4.2 ATLAS ADC ASIC
5
sec:fdsp-tpc-elec-design-alt-atlas
An alternative ADC solution is to adapt the ADC chip under development for the ATLAS liquid
6
argon calorimeter readout upgrade for the HL-LHC. The main ATLAS requirements are given
7
in Table
tab:ATLAS-ADC-reqs
1.3. Adapting the chip to DUNE needs would require doubling the number of channels
8
per chip as well as adapting the output architecture. These are both relatively simple changes
9
compared to the overall complexity of the chip.
10
Table 1.3: Performance requirements for the ATLAS-style ADC ASIC. Parameter Specification Channels/chip 8 preferred, 4 minimum Sampling Frequency 40 MHz Dynamic Range 14 bits Precision 11 ENOB Power < 100 mW/channel at 40 MHz Input 2 V differential Output E-link interface operating at 640 Mbps
tab:ATLAS-ADC-reqs
To achieve a 14-bit dynamic range, each analog channel is comprised of two main sections: a
11
Dynamic Range Enhancement (DRE) block that determines the most significant two bits of the
12
14-bit digital code, followed by a 12-bit SAR block.
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The design of the DRE is shown schematically in Figure
fig:65nmADCarchitecture_dre
1.11. The input signal is sampled on two
1
paths, one with unity gain and the other of gain four. A comparator determines which gain to
2
3
to the input of the 12-bit SAR ADC block. The DRE design has been carefully optimized so that
4
its output preserves the required 12-bit performance.
5
Figure 1.11: Block diagram of the DRE architecture for the ATLAS ADC ASIC.
fig:65nmADCarchitecture_dre
Figure 1.12: Block diagram depicting the two-stage SAR design of the ATLAS ADC ASIC.
fig:65nmADCarchitecture_sar
More details of the SAR design are shown in Figure
fig:65nmADCarchitecture_sar
1.12. Following current state-of-the-art
6
ADC development techniques, a two-stage SAR architecture is used, exploiting the high speed
7
Since
8
capacitor matching in this technology might not meet the precision required, the ADC will use bit
9
redundancy, i.e. determine more bits than its actual output, and the redundant bits will be used
10
to both calibrate the ADC and produce correct output codes. Such procedures are well understood
11
and applied to both pipeline
Kuppambatti:2013nfa
[47] and SAR
5999734
[48] ADCs using foreground or background calibration
12
techniques.
13
An ADC testchip, dubbed COLUTA65V1, was designed and submitted for fabrication in May
14
2017 and received in September of 2017. The DRE and SAR blocks of the COLUTA65V1 were
15
first tested independently. Measurements were made of the SAR precision using the sine-wave
16
Fast Fourier Transform method. An effective number of bits (ENOB) of 11.6 bits at 20 MHz
17
(after calibration) was obtained. Similar measurements at 40 MHz do not match the expected
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performance and additional testing and simulation indicates that the layout of the connection
1
between the first SAR stage and the amplifier is not optimal. Similar results were observed with
2
the DRE performance and again simulation indications improvements are possible in the layout.
3
The next submission of the chip, planned for spring 2018, will incorporate this work in the iteration
4
5
6
Tests in liquid nitrogen are planned for spring 2018.
7
8
sec:fdsp-tpc-elec-design-ft
All cold cables originating from inside the cryostat connect to the outside warm electronics through
9
PCB board feedthroughs installed in the signal flanges that are distributed along the cryostat roof.
10
The TPC data rate per APA, with an overall 32:1 MUX and 80 ∼1 Gbps data channels per APA,
11
is sufficiently low that the LVDS signals can be driven over copper twin-axial transmission lines.
12
Additional transmission lines are available for the distribution of LVDS clock signals and I2C
13
control information, which are transmitted at a lower bit rate. Optical fiber is employed externally
14
from the WIBs on the signal flange to the DAQ and slow control systems.
15
Figure 1.13: TPC CE feedthrough. The WIBs are seen edge-on in the left panel,and in an oblique side-view in the right panel, which also shows the warm crate for a DUNE module in a cutaway view.
fig:tpcelec-signal_FT
The design of the signal flange includes a T-shaped pipe, separate PCB feedthroughs for the CE
16
and PDS cables, and an attached crate for the TPC warm electronics, as shown in Figure
fig:tpcelec-signal_FT
1.13. The
17
wire-bias voltage cables connect to standard SHV (safe high voltage) connectors machined directly
18
into the CE feedthrough, ensuring no electrical connection between the wire-bias voltages and other
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signals passing through the signal flange. Each CE feedthrough serves the bias/power/digital IO
1
needs of one APA.
2
Data/control cable bundles are used to send system clock and control signals from the signal flange
3
to the FEMB, stream the ∼1 Gbps high-speed data from the FEMB to the signal flange. Each
4
FEMB connects to a signal flange via one data cable bundle, leading to 20 bundles between one
5
APA and one flange. Each data bundle contains 8 low-skew copper twin-axial cables with a drain
6
wire, to transmit the following differential signals:
7
8
9
10
11
The selected cables are Samtec 26 AWG twin-axial bundles with connectors to both the FEMB
12
mezzanine board and the signal flange. Each twin-axial pair is separately shielded. The Samtec
13
26 AWG cable has been tested and demonstrated to have low enough dispersion such that both
14
the LVDS 50 MHz system clock and ∼1 Gbps high-speed data can be recovered over 30 meters of
15
RT cable.
16
LV power is passed from the signal flange to the FEMB by bundles of 20 AWG twisted-pair wires.
17
Half of the wires are power feeds; the other wires are attached to the grounds of the input amplifier
18
circuits, as described in Section
sec:fdsp-tpc-elec-design-bias
1.2.2. For a single FEMB, the resistance is measured to be < 30 mΩ
19
at RT or < 10 mΩ at LAr temperature. Each APA has a copper cross-section of approximately
20
80 mm2, with a resistance < 1.5 mΩ at RT or < 0.5 mΩ at LAr temperature.
21
The wire-bias voltage cables are required to deliver voltages up to a few thousand Volts and
22
currents up to a few milliAmps.
23
The bias voltages are applied to the X-, U-, and G-plane wire layers, three field cage terminations,
24
and an electron diverter, as shown in Figure
fig:CR-board
1.2. The voltages are supplied through eight SHV
25
connectors mounted on the signal flange. RG-316 coaxial cables carry the voltages from the signal
26
flange to a patch panel PCB which includes noise filtering mounted on the top end of the APA.
27
From there, wire-bias voltages are carried by single wires to various points on the APA frame,
28
including the CR boards, a small PCB mounted on or near the patch panel that houses a noise
29
filter and termination circuits for the field cage voltages, and a small mounted board near the
30
electron diverter that also houses wire-bias voltage filters.
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1
sec:fdsp-tpc-elec-design-warm
The warm interface electronics are housed in warm interface electronics crates (WIECs) attached
2
directly to the signal flange. The WIEC shown in Figure
fig:tpcelec-flange
1.14 contains one Power and Timing
3
Card (PTC), up to five Warm Interface Boards (WIBs) and a passive Power and Timing Backplane
4
(PTB), which fans out signals and LV power from the PTC to the WIBs.
5
Figure 1.14: Exploded view of the signal flange for ProtoDUNE-SP.
fig:tpcelec-flange
The WIB is the interface between the DAQ system and up to four FEMBs. It receives the system
6
clock and control signals from the timing system and provides for processing and fan-out of those
7
signals to the four FEMBs. The WIB also receives the high-speed data signals from the four
8
FEMBs and transmits them to the DAQ system over optical fibers. The data signals are recovered
9
10
feedthrough on the signal flange. The feedthrough board is a PCB with connectors to the cold
11
signal and LV power cables fitted between the compression plate on the cold side, and sockets for
12
the WIB on the warm side. Cable strain relief for the cold cables is supported from the back end
13
14
The PTC provides a bidirectional fiber interface to the timing system. The clock and data streams
15
are separately fanned-out to the five WIBs as shown in Figure
fig:tpcelec-wib_timing
1.15. The PTC fans the clocks out
16
to the WIB over the PTB, which is a passive backplane attached directly to the PTC and WIBs.
17
The received clock on the WIB is separated into clock and data using a clock/data separator.
18
The PTC also receives LV power for all cold electronics connected through the signal flange,
19
approximately 250W at 48V for a fully-loaded flange (one PTC, five WIB, and 20 FEMB). The
20
LV power is then stepped down to 12V via a DC/DC converter onboard the PTC. The output of
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SFP Rx SFP Tx
Fanout 1:6 MUX 6:1 Prio. Enc.
SFP Rx
ADN2814
Clock/Data Recovery Arria V FPGA
Fanout 1:4 Fanout 1:4
PLL
MUX MUX
SFP Tx
Clock to FEMBs
Clock to MBs Encoded Control to MBs
Reply Data Reply enable Control to FEMBs
Power/Timing Backplane
Primary Clock/Control Path through PTC Alternative Clock/Control Path through WIB front panel Laser Enable Reply Data
WIB PTC
Encoded Clock+ Control MUX Encoded clock/control
Figure 1.15: Power and Timing Card (PTC) and timing distribution to the WIB and FEMBs.
fig:tpcelec-wib_timing
Arria 5 GX/T WIB
DC-DC Front Panel FEMB 0 FEMB 1 FEMB 2 FEMB 3 1.5V 2.5V 2.8V 3.6V Enable
Power in 48V (~250W)
DC-DC DC-DC Bias 0-3 linear
To FEMBs
Sense fuse
PTC 5
Fanout 1:5
12V 12V
PTB
48V/12V DC-DC
Figure 1.16: LV power distribution to the WIB and FEMBs. 250W is for a fully-loaded crate with the majority of the power dissipated by the 20 cold FEMBs in the LAr.
fig:tpcelec-wib_power
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the PTC converters is filtered with a common-mode choke and fanned out on the PTB to each
1
WIB, which provides the necessary 12V DC/DC conversions and fans the LV power out to each of
2
the cold FEMBs supplied by that WIB, as shown in Figure
fig:tpcelec-wib_power
1.16. The output of the WIB converters
3
are further filtered by a common-mode choke. The majority of the 250W drawn by a full flange is
4
dissipated in the LAr by the cold FEMB.
5
Each WIB contains a unique IP address for its UDP slow control interface. The IP address for the
6
WIB is derived from a crate and slot address: the crate address is generated on the PTC board via
7
dipswitches and the slot address is generated by the PTB slot, numbered from one to five. Note
8
that the WIBs also have front-panel connectors for receiving LV power; these can be used in place
9
10
The WIB is also capable of receiving the encoded system timing signals over bi-directional optical
11
fibers on the front panel, and processing these using either the on-board FPGA or clock synthesizer
12
chip to provide the 50 MHz clock required by the cold electronics.
13
Figure 1.17: Warm Interface Board (WIB). Note that front panel inputs include a LEMO connector and alternate inputs for LV power.
fig:tpcelec-dune_wib
The FPGA on the WIB is an Altera Arria V GT variant, which has transceivers that can drive
14
the high-speed data to the DAQ system up to 10.3125 Gbps per link, implying that all data from
15
two FEMB (2×5 Gbps) could be transmitted on a single link. The FPGA has an additional
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Gbps Ethernet transceiver I/O based on the 125 MHz clock, which provides real-time digital data
1
readout to the slow control system.
2
3
sec:fdsp-tpc-elec-design-external
Including power for the WIB, a fully loaded WIB (one WIB plus four FEMBs) requires 12V and
4
draws up to approximately 4 Amps. Therefore, the full electronics for one APA (one PTC, five
5
WIBs, and 20 FEMBs) requires 12V and draws approximately 20A, for a total power of almost
6
250W, as described in Section
sec:fdsp-tpc-elec-design-warm
1.2.6.
7
As the LV power is delivered at 48V to the PTC, each LV power mainframe should operate at
8
roughly 30-60V/13.5A/650W maximum capacity. Using 10 AWG cable, an 0.8V drop is expected
9
along the cable with a required power of 306.12W out of 650W available.
10
Four wires will be used for each module, two 10 AWG, shielded, twisted pair for the power and
11
return, two 20 AWG, shielded, twisted pair for the sense. Sense line fusing will be provided on
12
the PTC card. This fusing would serve as a final protection. The primary protection would come
13
from the Over Current protection on the LV supply modules, which is set above the ∼20 Amps.
14
The LV power cable uses FCi micro TCA connectors, shown in Figure
fig:tpcelec-power_conn
1.18.
15
Figure 1.18: FCi micro TCA power connector at the PTC end of the cable.
fig:tpcelec-power_conn
Each APA requires three wire-bias voltage connections at +820V, −370V, and −665V, as described
16
in Section
sec:fdsp-tpc-elec-design-bias
1.2.2. The remaining five wire-bias voltage lines supply between 1 and 1.5 kV to the field
17
cage terminations (3) and electron diverters (2). The current on each of these supplies is expected
18
to be zero at normal operation. However the ripple voltage on the supply must be carefully
19
controlled to avoid noise injection into the front-end electronics. Each HV module supplies all the
20
wire-bias power to one APA via 8 SHV connector feedthroughs at the CE flange.
21
RG-58 coaxial cables connect the wire bias voltages from the mini-crate to the standard SHV
22
connectors machined directly into the CE feedthrough, so there is no electrical connection between
23
the LV power and data connectors and wire-bias voltages. The length of the cables from the
24
Weiner mainframe to the signal flanges is estimated to be 18 meters.
25
Optical fibers provide the connections between the WIECs, which act as Faraday-shielded boxes,
26
to the DAQ and slow control systems.
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Duplex LC optical fiber transmits the one GIG-E connection from each WIB to the slow control
1
2
slow control system, while the current draw for each APA is monitored at the mainframe itself.
3
4
sec:fdsp-tpc-elec-prod
A single 10 kt DUNE single phase detector requires 3000 FEMBs, 750 WIBs, and 50 PTCs. A
5
total of 3300 FEMBs, 900 WIBs, and 60 PTCs will be built.
6
If the three-ASIC FEMB solution is chosen, then two ASIC production contracts will be required,
7
8
the one-ASIC FEMB solution is chosen, only one ASIC production contract will be required.
9
In either case, all ASICs will be packaged in Plastic Quad Flat-Pack (PQFP) or Thin Quad
10
Flat-Pack (TQFP) surface mount packages. No wafer probing will be done before the chips are
11
10 mm from the
12
13
collaborators (see Section
sec:fdsp-tpc-elec-qc
1.6) before being assembled onto printed circuit boards.
14
All printed circuit boards will be fabricated and tested by qualified vendors. Circuit boards will
15
also be assembled by qualified vendors. The completed boards will be acceptance tested by DUNE
16
collaborators promptly after assembly.
17
All cable assemblies (including terminations) will be fabricated and tested by qualified vendors.
18
At least a fraction of the cable assemblies will be retested by DUNE collaborators promptly after
19
purchase.
20
21
sec:fdsp-tpc-elec-intfc
22
sec:fdsp-tpc-elec-intfc-ov
There are some placeholders for citations here; need to revisit how to cite e.g. interface documents.
23
Some of the components designed and built by the CE consortium are mounted or need to work
24
together with detector components provided by other DUNE consortia. Interface documents have
25
been developed to ensure that the boundaries between systems are fully understood and that no
26
detector components is missed or not properly defined when organizing the detector construction
27
project into consortia. These interface documents are a work in progress. With time they will
28
evolve into a very detailed definition of mechanical and electrical interfaces, including in some
29
cases the description of data transmission protocols. These interface documents include a list
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Chapter 1: TPC Electronics 1–26
1
discuss also all the procedures to be followed during the integration of detector components and
2
the following testing and commissioning process. In some cases multiple consortia (APA, PDS,
3
HV, CISC, and DAQ) can be involved, depending on the complexity and maturity of the test
4
setup.
5
The most important interfaces for the CE consortium are with the APA (cite: interface : didceapa)
6
and DAQ (cite: interface : didcedaq) consortia, followed by those with the PDS (cite: interface :
7
didpdsce), HV (cite: interface : didhvce), and CISC (cite: interface : didciscce) consortia. One
8
9
rules and of the separation between electrical circuits to minimize the noise and cross-talk between
10
different detector components. Different APAs should be electrically insulated, and the same
11
should apply for the photon detection system and the CE readout of the anode planes. The
12
flanges on the chimneys are used to provide, separately for the two APAs and for the photon
13
detector system, the reference voltage for all the detector elements. The flanges are electrically
14
connected to the cryostat structure that acts as the detector ground. The same approach has to
15
be implemented also for the CISC instrumentation in the LAr.
16
17
sec:fdsp-tpc-elec-intfc-apa
The CE consortium provides all the electronics used for reading out the charge deposited on the
18
APA wires by particles that ionize the LAr. The APA consortium is responsible for all the printed
19
circuit boards mounted on the APA frame holding the anode wires. These boards provide filtering
20
21
22
FEMBs are also mounted on the APAs and are connected electrically to the CR boards. The CE
23
consortium is responsible for providing the bias voltage to the APAs, and also the bias voltage for
24
the electron diverters and the field cage termination electrodes (these last two items are part of
25
the interface with the HV consortium). The bias voltages are generated in power supplies housed
26
in crates on top of the cryostat, that are brought into the LAr using connectors on the flange
27
mounted on the CE chimneys, and then via cables to the SHV boards mounted on the APA frame
28
from where they are distributed to the various detector components.
29
A crucial aspect of the interface between the CE and APA consortia is the choice of routing for
30
the cables that provide power, control, and read-out for the bottom APA. Studies are ongoing to
31
understand whether it is feasible to route these cables inside the APA frames of the two stacked
32
APAs, and whether it is necessary to modify the size of the APA frame in order to achieve this
33
34
under the assumption that there will be minimal changes in the cross section of cables between
35
protoDUNE and DUNE (we expect to be able to remove one of the seven pairs of power lines used
36
in protoDUNE, when the FPGA on the FEMB is replaced by the COLDATA ASIC). Before Spring
37
2019 we expect to perform a realistic test of the cable insertion in a pair of stacked APAs using
38
mechanical prototypes (i.e. without wires) of the APA. We are also investigating the possibility
39
40
the length of the cables for the central APA, and complicates the installation procedure and the
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Chapter 1: TPC Electronics 1–27
engineering of the support structures inside the cryostat.
1
2
sec:fdsp-tpc-elec-intfc-daq
There are two components in the definition of the interface between the CE and DAQ consortia.
3
The first one is a decision on whether to implement any firmware and buffering related to the
4
trigger decision inside the WIB, or instead transmit the data as they are produced from the
5
FEMBs, possibly with some serialization taking place in the WIB. For the single phase TPC we
6
have chosen to adopt the latter option, which minimizes the requirements on the FPGA inside the
7
WIB, and also reduces the power and cooling requirements for the WIC. Based on this decision,
8
the interface between the CE and DAQ consortia is defined by the fibre plant used to transmit the
9
data from the WIBs to the DAQ components housed in the Central Utility Cavern (CUC), and
10
to broadcast the clock and controls in the opposite direction. Only optical links are used in the
11
connection with the DAQ, which guarantees that the DAQ electronics will not induce any noise
12
13
The interface is fully defined with the selection of the number and type of optical fibre links, their
14
speed, and the type of connectors. The FPGA inside the WIB can be used to reformat the data
15
with changes to the headers and trailers that include time stamps and geographical addresses of
16
the FEMBs. It can also be used to serialize the data from multiple COLDATA ASICs into a single
17
18
fibre, transmitting data at 1.28 Gbit/s. Depending on the availability and cost of transmitters
19
capable of sending data at higher speeds data from multiple electrical links (4, 8 or more) could be
20
serialized onto a single link, reducing the number of fibres and connections needed. Using higher
21
transmission speeds reduces the number of links that are needed, possibly reducing the cost of
22
the DAQ part of the detector. The use of links at speeds of 5 Gbit/s or larger may also present
23
another drawback, in addition to the increases in the cost of fibres, transmitters and receivers. We
24
desire to keep the data of a single FPGA into a single set of DAQ boards, without deserializing
25
the data on the CUC side. Given the granularity of the FEMBs there may be combinations of
26
ithe number of DQ boards and the number of links being used, that cannot be operated for this
27
28
DAQ processing units in the CUC can be delayed until the Technical Design Report.
29
Another aspect of the interface between the DAQ and the CE consortia is the transmission of
30
clock and commands. In protoDUNE there is a single fibre that carries this information to the
31
PTC card, which then re-broadcasts the information to the five WIBs, using the WIC backplane.
32
For DUNE we foresee the possibility of transmitting the information directly to each WIB. This
33
would only require the addition of a receiver on each WIB, and no changes to the FPGA firmware,
34
given that already in the protoDUNE scheme the clock and control information is already decoded
35
inside the FPGA mounted in the WIB. The final aspect of the interface between the DAQ and the
36
CE is the definition of the format of the data transmitted by the cold electronics to the DAQ. This
37
format has been defined for protoDUNE in (cite: proto : dataformat). Some changes are needed
38
for DUNE, to accommodate a larger number of APAs. More extensive changes may be needed if
39
the SLAC CRYO ASIC is selected for the detector’s construction as in that case 64b/66b encoding
40
is used intedad of 8b/10b.
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1
sec:fdsp-tpc-elec-qa
2
sec:fdsp-tpc-elec-qa-initial
The QA for the DUNE single-phase far detector electronics has been ongoing for several years. It
3
includes testing all of the cold components, cables, feedthrough and flange mechanicals, and warm
4
electronics for suitability for the SP detector requirements. The current status of the QA program
5
is the instrumenting of the ProtoDUNE-SP detector with 120 FEMB (960 of each of the current
6
FE and ADC ASIC designs) and 6 full APA readout chains as described in Section
sec:fdsp-tpc-elec-design
1.2.
7
The FE ASIC
sec:fdsp-tpc-elec-design-femb-fe
1.2.3.2 design is fairly mature, and has been tested extensively on the bench and in
8
integrated system tests. The ADC ASIC will be selected from several design options as described in
9
Section
sec:fdsp-tpc-elec-design-femb-adc
1.2.3.3 and Section
sec:fdsp-tpc-elec-design-alt
1.2.4. The ADC candidates will be tested at the institutions responsible
10
for developing the designs. The COLDATA ASIC is a new design for DUNE
sec:fdsp-tpc-elec-design-femb-coldata
1.2.3.4, and will be
11
tested individually at Fermilab both standalone and communicating to FE ASICs currently on
12
FEMB analog motherboards. All tests will be done at both room temperature and in liquid
13
nitrogen.
14
The next step will be a redesign of the FEMB to accommodate the new ADC and COLDATA.
15
The current design of the FEMB for ProtoDUNE-SP uses a 16-channel, 2 MHz ADC to digitize
16
the output of the FE ASICs. Correspondingly, the modification to the baseline ADC option (if
17
used) for DUNE will be fairly minor. Prototypes of the DUNE FEMB will be tested individually
18
at several institutions at both room temperature and in liquid nitrogen. The cold data and LV
19
cables used in ProtoDUNE-SP have been selected to be candidates for DUNE and already verified
20
to successfully transmit the high-speed data over ∼ 35 meters, the longest possible cable length in
21
the far detector.
22
The updates to the DUNE mechanical components and warm interface electronics are expected to
23
be small iterations on the already existing system for ProtoDUNE-SP. Prototypes will be ordered
24
in small batches and tested at the responsible institutions for the different components.
25
After individual testing, integrated system tests will be critical to validate that the performance
26
27
be fed back into the design of the individual components.
28
29
sec:fdsp-tpc-elec-qa-facilities
DUNE will plan for system tests of the baseline and alternative option in both the CERN cold
30
box and a small test TPC at Fermilab. The cold box tests establish performance of the electronics
31
coupled to a full-scale APA in a correctly grounded environment, but in a gaseous environment no
32
colder than 150K, and without TPC drift. The small test TPC will provide tests in an operational
33
LArTPC but at much smaller scale, with quick turn around (2-4 weeks) for changing components
34
and refilling. The 40% APA at BNL employs liquid nitrogen instead of liquid argon, does not
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Chapter 1: TPC Electronics 1–29
integrate the CE with the PDS, and has no TPC drift. However, it allows for quick turn-around
1
and is located very close to where the development is happening (BNL and Fermilab), and is thus
2
invaluable for initial board and component testing.
3
Generic board and component testing often includes (a) the measurement of the baseline noise
4
level and frequency spectrum, (b) the measurement of the response to the calibration input signal
5
provided on the FEMB, and (c) the measurement of the response to cosmic rays in a TPC.
6
Measurements are often done at both room temperature and liquid nitrogen or argon temperature
7
in three configurations: nothing attached to the inputs, dummy capacitive load attached to the
8
inputs, and an APA attached to the inputs as the capacitive coupling of long wires is subtly
9
different than a dummy capacitor with the equivalent capacitance of a single wire. Measurements
10
specific to the characterization of the ADC performance, such as INL and DNL determination, are
11
done before the ADC is mounted on the FEMB.
12
1.5.2.1 ProtoDUNE-SP
13
sec:fdsp-tpc-elec-qa-facilities-pdune
ProtoDUNE-SP is intended to be a full slice of the DUNE far detector as near as possible to the
14
final DUNE Single Phase design. It will instrument 6 full-size DUNE APAs with 20 FEMB each
15
for a total readout channel count of 15,360 digitized sense wires. Critically, the CE on each APA
16
will be read out via a full CE read out system, via a CE flange and WIEC with 5 WIBs and 1
17
18
Once each APA has been validated in the Cold Box at CERN, it will be installed in the ProtoDUNE-
19
SP cryostat. Any issues that are discovered either during the Cold Box tests or the ProtoDUNE-SP
20
commissioning and data-taking will be incorporated into the next iteration of the system design
21
for DUNE.
22
Preliminary results from the ProtoDUNE-SP cold box indicate that the noise performance of the
23
TPC readout will satisfy the DUNE FD noise requirements of ENC < 700e− on DUNE length
24
fig:cb_results
1.19.
25
Tests have also been done on the ProtoDUNE-SP APA to check for any additional noise introduced
26
27
far, no significant increase in the noise on the APA wire readout has been observed when operating
28
these other systems.
29
1.5.2.2 Small Test TPC
30
sec:fdsp-tpc-elec-qa-facilities-small
A small test TPC is essential to qualifying the different prototype ASICs, offering quick turn
31
around for changing components and refilling and a TPC drift and thus the ability to study the
32
response of the electronics to signals from cosmic ray muons. A new reduced-size APA will be
33
constructed, with as many similarities to the DUNE APAs and field cage as possible. The APA
34
will be half the width of a DUNE APA (along the beam direction) or 1.3 m, with half the number
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Chapter 1: TPC Electronics 1–30
Figure 1.19: ENC (in electrons) and temperature (in degrees Kelvin) as a function of cold cycle time in GN2 for ProtoDUNE-SP APA2. At the lowest temperature of 160K, the wrapped wires measured 480e− noise and the straight wires 400e−.
fig:cb_results
This amounts to 10 FEMBs with a total of 1280 channels. The height
1
will be significantly reduced from the DUNE APA height of 6 m to about 1.25 m, and the wire
2
lengths will be reduced by the same factor. The ProtoDUNE wire carrier boards will be used,
3
and the APA will accommodate a single half-length photon detector. The TPC will have the
4
APA in the center and a cathode on either end, creating two drift volumes with drift distance
5
0.5 m each. The TPC will be installed in the cryostat with the wire planes parallel to the floor
6
to optimize the orientation of the cosmic ray tracks. It will be instrumented with a full readout
7
chain of ProtoDUNE electronics, specifically the cables, feedthrough flange, WIB, PTC and warm
8
interface crate. Initially, ProtoDUNE FEMBs will be used for commissioning, and later FEMBs
9
with prototype ASICs will be swapped in.
10
The TPC electronics and photodetector will be read out through a “slice” of the ProtoDUNE
11
data acquisition system. This system will provide a low noise environment that will allow one to
12
make detailed comparisons of the performance of the new ASICs. It will also enable the study
13
14
and the HV distribution.
15
The APA will be housed in new LAr cryostat at Fermilab (in the Proton Assembly Building)
16
that complies with the DUNE grounding and shielding requirements, and connected to an existing
17
recirculation system for argon purification. The cryostat will be a vertical cylinder, inner depth
18
19
the cylinder, the flat top plate will have penetrations dedicated to readout and cryogenic instru-
20
21
these will house the latest version of the FE ASIC, the first prototype of COLDATA and various
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Chapter 1: TPC Electronics 1–31
ADC prototypes (including the SLAC CRYO ASIC). The new APA and the new cryostat will be
1
completed on the same timescale so that tests in both the ProtoDUNE cold box at CERN and the
2
test TPC at Fermilab can be completed and analyzed prior to the submission of the TDR.
3
1.5.2.3 Additional Test Facilities
4
sec:fdsp-tpc-elec-qa-facilities-other
For CE development, testing prototypes at room temperature is the first step, as many problems
5
can be identified quickly and without the expense of cryogens. A quick access test stand with
6
the FEMB connected to an APA inside a shielded environment that is in the same location as
7
the FEMB/ASIC development is invaluable for rapid progress. Two such facilities are available to
8
DUNE: the shielded room at Fermilab and the 40% APA test stand at BNL. In addition, a “cold
9
box” at CERN used in electronics tests for ProtoDUNE-SP is available for additional electronics
10
testing in cold argon gas.
11
The shielded room at Fermilab (see Figure
fig:shieldedroom
1.20) is 2.5 m tall, and 2 m on each side, with a double
12
layer of copper mesh in the walls, floor and ceiling, plus a solid metal plate in the floor all electrically
13
connected to create a faraday cage. A flexible AC distribution and isolated grounding configuration
14
15
a building reference or a detector reference. In addition to evaluating different grounding schemes
16
for the APAs, capacitive coupling issues can be studied by varying the distance between the floor
17
and a copper plate positioned underneath. This room has uniquely easy access to the setup
18
through a shielded door, and a person can remain inside safely with the door closed and probe the
19
electronics directly while operating in a shielded environment. Currently mounted inside are two
20
35-ton APAs with adaptor boards to connect ProtoDUNE electronics. This installation satisfies the
21
ProtoDUNE grounding and shielding guidelines. A rough demonstration of the shielding adequacy
22
for our purposes is the measured noise level of 800 ENC for ProtoDUNE prototype FEMBs. The
23
same noise level was measured at room temperature in the 40% APA at BNL for the same FEMBs.
24
The 40% APA at BNL is a 2.8 m × 1.0 m three-plane APA with two layers of 576 wrapped
25
(U/V) wires and one layer of 448 straight (X) wires. It is read out by 8 ProtoDUNE-SP FEMBs
26
with the full 7 m ProtoDUNE-SP length data and LV power cables, 4 on the top and 4 on the
27
28
and WIEC, 2 WIBs and 1 PTC, as shown in Figure
fig:tpcelec_40APA
1.21. Detailed integration tests of the CE
29
readout performance while following the DUNE grounding and shielding guidelines have been done
30
at the 40% APA. Additional input capacitance (equivalent to longer wire length) have been added
31
to a subset of channels to project the ENC performance from the 40% APA teststand to the
32
ProtoDUNE-SP and SBND detectors. The results from the 40% APA indicate that the full CE
33
system as installed on the teststand at BNL will satisfy the DUNE far detector noise requirements.
34
The cold box at CERN is designed to cycle one full-size DUNE APA with the full compliment of 20
35
FEMB through gaseous Nitrogen temperatures around 150K to check out the APA performance
36
prior to installing the APA into the ProtoDUNE-SP cryostat. It is designed to be a Faraday cage
37
identical to the ProtoDUNE-SP cryostat and is read out by a complete CE system for a single
38
APA, including a CE flange and fully-loaded WIEC with 5 WIBs and 1 PTC.
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Chapter 1: TPC Electronics 1–32
Figure 1.20: Picture of the shielded room at Fermilab.
fig:shieldedroom
Figure 1.21: Left: one side of the 40% APA with 4 FEMBs. Right: the full CE feedthrough and flange.
fig:tpcelec_40APA
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–33
1
sec:fdsp-tpc-elec-qc
This section will be written for the second draft of the technical proposal.
2
3
sec:fdsp-tpc-elec-install
4
sec:fdsp-tpc-elec-install-apa
The installation and commissioning of the detector components built or purchased by the Cold
5
Electronics (CE) consortium takes place both prior to and after the insertion of the Anode Plane
6
Assemblies (APAs) in the detector cryostat, with testing performed after each step, to avoid the
7
need for rework that could cause significant delays. The installation and initial commissioning of
8
the CE electronics is likely to be on the critical path for the completion of the single phase detector
9
and the amount of time available for testing and possibly repairing / replacing components after
10
their installation is going to be very limited. Cold tests of the complete APAs may not be possible
11
for the entire detector, and this requires that all the CE components are qualified for operation in
12
LAr prior to their installation.
13
After the completion of the cryostat, the chimneys that are house all the cables for the CE, PDS,
14
and HV consortia (with the exception of the high voltage feedthrough for the cathode planes) are
15
installed and leak tested. This also includes the installation of the crossing tube cable support and
16
17
house the CE and PDS electronics components on the top of the cryostat, and the corresponding
18
CISC and detector safety system monitoring, controlling, and interlock hardware can be installed.
19
Cable trays between different chimneys belonging to a same set of 6 APAs and 2 CPAs can also
20
be put in place. Readout fibre bundles between the chimneys and the central utility cavern used
21
for the readout of the wire information from the APAs can also be put in place. In the meantime
22
inside the cryostat all the cable trays used to support the CE and PDS cables and to accommodate
23
the slack of the cables can be put in place.
24
In parallel the 20 front-end motherboards (FEMBs) required to read out the wires from one APA
25
are installed with their shielding box onto the APA and connected to the CR boards. This work
26
will be performed at the integration facility (or facilities), because there will not be enough space
27
to perform this type of work in parallel on multiple APAs in the detector cavern. Once the FEMBs
28
are installed a temporary set of cables will be used to connect each FEMB to a temporary power,
29
control, and readout system to ensure that all the wires can be properly read-out. For a more
30
thorough set of tests, this set of temporary cables will be connected to warm interface boards
31
(WIBs) housed in a warm interface crate (WIC) identical to the one used in DUNE. The WIBs
32
would then be read out with a DAQ system identical to the one used after the installation of the
33
APAs into the detector cryostat. With this setup all the wires connected to an APA and also the
34
corresponding PDS components can be read out simultaneously, allowing for the investigation and
35
resolution of possible noise and cross talk issues. While it would be desirable to perform these tests
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23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–34
in a cold box operating at or close to LAr temperature, the tightness of the installation schedule
1
may require that these tests are performed at room temperature for all the APAs. Assuming that
2
all the CE components have already been qualified for operation in LAr, only a sample of the
3
APAs would be tested in cold conditions. Once these tests are completed the temporary cables are
4
disconnected and the APA is prepared for shipment to Sanford Lab. It is not considered feasible
5
to transport the top APA from the integration facility to the detector cryostat with the CE cables
6
already installed. For the bottom APA the final cables can be installed only after the two APAs
7
are mated together in the “toaster" area just outside of the detector cryostat.
8
Further work on the CE components installed on the APAs is performed after the APAs are
9
transported to the clean area outside the cryostat inside Sanford Lab. All the cables that provide
10
power and control and that are used to read out the 20 FEMBs of the top and bottom APAs need
11
to be installed, as well as the cables that connect to the SHV boards that are used to distribute
12
the bias voltage to the APA wires, to the electron diverters, and to the field cage termination
13
14
an operation that can be performed only after the two APAs are mechanically coupled inside the
15
“toaster" area. Quick tests are performed after the installation of the final cables, and then the
16
APAs can be moved to their final position inside the detector cryostat. At that point the CE and
17
PDS cables can be routed through the chimney and connected to the respective flanges and their
18
strain reliefs. The flanges are then moved to the final position on the chimneys and leak tests and
19
electrical connectivity tests can be performed. Then the bottom plate of the crossing tubes with
20
its additional strain relief for the CE and PDS cables can be put in place, and the final slack of the
21
cables can be arranged in the cable trays attached to the supports inside the cryostat. After the
22
cabling work is completed, the WICs for a pair of APAs can be installed on the chimney and more
23
testing of the entire power, control, and readout chain can be performed, first with local control,
24
and later after connection of the readout and timing and control fibres to the WIBs using the final
25
DAQ system.
26
The current plans foresee that six APAs and two CPAs are installed and tested in one week before
27
moving on to the next set. As soon as another set of APAs and CPAs is in place any replacement
28
29
This requires that all readout tests are performed very quickly after each step in the installation.
30
The schedule foresees four work days each week for the installation work (in two eight hours shifts).
31
The testing activities may require that work is performed in parallel, i.e. that the CE components
32
33
control, and readout system. It is also likely that the testing work may require a more extended
34
working schedule (six or seven working days per week). More complex tests, involving readout
35
36
all the detector components are installed inside the cryostat. Final tests should be performed
37
reading out the entire detector through the DAQ system prior to the closure of the TCO and
38
before starting filling the cryostat with Ar and cooling down. There will be a hyatus in the
39
commissioning activities during the filling of the cryostat. The commissioning at LAr temperature
40
will be most likely possible only after the cryostat is completely full.
41
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–35
1
sec:fdsp-tpc-elec-install-calib
This section will be written for the second draft of the technical proposal.
2
3
sec:fdsp-tpc-elec-safety
The TPC electronics will be built and handled in such a way as to ensure the safety of both
4
personnel and equipment. The team will work closely with the project Technical Coordination
5
6
The instrumentation of the TPC electronics will include multiple printed circuit boards and cabling.
7
The cabling includes the high voltage wire bias distribution, low voltage power and signals. Each
8
9
to the review of the project Technical Coordination organization.
10
All printed circuit boards will be designed such that the connectors and copper carrying traces are
11
rated to sustain the maximum current load. In the case of the low voltage warm electronics, all
12
boards will be fused following prescribed safety standards. The cold electronic low voltage boards
13
inside the cryostat will not be fused because these boards will be inaccessible during operations
14
and fire is not a danger once the cryostat is filled with liquid argon. Special precautions should be
15
taken during installation and commissioning of the cold electronics prior to the cryostat being filled
16
with liquid argon. The TPC electronics group will work with the project Technical Coordination
17
to implement this.
18
All cabling and connectors will be selected such that they meet or exceed the possible current
19
ampacity and voltage ratings of the connected power supplies. In the case of high voltage distri-
20
bution, all accessible warm connectors will be SHV type connectors which will limit the possibility
21
22
will be open soldered connections. Care will be taken that ensures personnel safety should these
23
connections need to be energized while the APA is exposed. However, it is not anticipated that
24
APA wire bias will be powered by more than 50 volts unless the APA is enclosed within a Faraday
25
shield.
26
Finally, the safety of the equipment must be taken into account during production, initial check
27
28
at all stages, including use of ESD safe bags for storage and ESD wrist straps used by personnel
29
when handling the cards. The TPC electronics will also make use of shorting connectors on all
30
cables which are attached to the printed circuit cards, but not attached at the far end. During
31
installation, multiple long cables will be attached to front end boards, but will not be attached
32
to the connectors on the flanges for some period of time. Detailed procedures for the use of cable
33
shorting connectors will be written and used.
34
Finally, the handling of the APA and attached front end electronics must follow ESD safe handling
35
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–36
procedures whenever the APA is moved from one ground reference to another, or after it has been
1
left in a “floating” state for any period of time. Whenever the APA is moved and could encounter
2
a step potential, a connection must be made through a slow discharge path which will equalize the
3
APA frame potential to the new environment. Again, ESD safe handling rules will be documented
4
and followed.
5
6
sec:fdsp-tpc-elec-org
7
sec:fdsp-tpc-elec-org-consort
For the moment the CE consortium does not have an official substructure with coordinators ap-
8
pointed to oversee specific areas. This is in part due to the current focus on ASIC development:
9
informal subgroups exist that are following the design of the various ASIC. Hucheng Chen (BNL) is
10
leading the design of the new version of LArASIC, and in parallel following the studies of commer-
11
cial ADCs for SBND. Carl Grace (LBNL) is leading the effort of LBNL, BNL, and FNAL, on the
12
design of a new ADC in 65 nm technology. Terry Shaw (FNAL) is overseeing the development of
13
the new COLDATA ASIC, and Angelo Dragone (SLAC) is overseeing the adaptation of the nEXO
14
CRYO ASIC for use in DUNE. A new working group tasked with studying reliability issues in the
15
CE components and preparing recommendations for the choice of ASICs, the design of printed
16
circuit boards, and testing. This working group could form the basis for the group tasked with
17
developing the QA/QC program for the CE detector components and then monitoring it. We plan
18
to reassess the structure of the group in a few months, with a likely split between components
19
inside and outside the cryostat, a group responsible for testing, and contact people for calibration,
20
physics, software and computing, and integration and installation.
21
22
sec:fdsp-tpc-elec-org-assmp
Please note that these dates may need to be revisited and that there may be more time available prior to the beginning of construction.
23
Plans for the CE consortium are based on the overall schedule for DUNE that assumes that the
24
first APAs need to be fully populated with electronics and tested toward the end of 2020. The APA
25
production needs to be completed about 12 months later and the installation in the cryostat should
26
be finished by mid-2022. This defines the time window for the completion of the R&D program on
27
the ASICs: a set of ASICs (or a single ASIC) meeting all the DUNE requirements needs to have
28
been qualified by Fall 2019, such that preproduction ASICs and the corresponding FEMBs can be
29
assembled and tested in Spring 2020, launching the full production in Summer 2020. Meeting this
30
timeline requires that the development of the ASICs, and in particular of the newly designed ones
31
(the SLAC CRYO ASIC, the joint LBNL-BNL-FNAL ADC, and COLDATA) are prototyped by
32
the end of Summer 2018, with testing completed by the end of 2018. This would allow a second
33
round of prototyping, if necessary, in the first half of 2019. The FEMBs used for protoDUNE will
34
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–37
likely have to be redesigned to house a new ADC and to replace the FPGA used in protoDUNE
1
with the COLDATA ASIC. Multiple variants of this board will be necessary, depending on the
2
success of the various ADC R&D projects being currently pursued. These design changes will be
3
made in the second half of 2018. Additional FEMBs prototypes will be designed and fabricated
4
depending on the outcome of the initial testing of the SLAC CRYO ASIC. A second iteration of
5
FEMB prototype(s) will be necessary in 2019, when the final ASICs (that may have a different
6
channel count from the first prototype) will become available.
7
We assume that for apart from the ASIC, where rapid development is still required, and the
8
FEMBs, which have to be redesigned to accommodate the new ASICs, most of the detector
9
components to be delivered by the CE consortium will require only minor changes relative to the
10
protoDUNE components. For this reason the modifications of these other detector components
11
will be delayed until 2019, which will also help with the availability of funding. Exceptions will
12
be made for further development in test stands, for cabling studies, and for conceptual studies of
13
automated testing assemblies, rack space assignment, and of the interface to the DAQ system.
14
15
sec:fdsp-tpc-elec-org-wbs
This section will be written for the second draft of the technical proposal.
16
17
sec:fdsp-tpc-elec-org-cs
This section will be written for the second draft of the technical proposal.
18
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
Chapter 1: TPC Electronics 1–38 23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
REFERENCES 1–39
1
[1] W. Strunk, Jr. and E. B. White, The Elements of Style. Macmillan, third ed., 1979.
2
[2] DUNE Collaboration, “TDR Volume 1: The LBNF and DUNE Projects,” tech. rep., 2018.
3
http://docs.dunescience.org/cgi-bin/ShowDocument?docid=nnnn.
4
[3] “Study of Hadron Production in Hadron-Nucleus and Nucleus-Nucleus Collisions at the
5
CERN SPS; CERN-SPSC-2006-034,” 2006. http://cds.cern.ch/record/995681?ln=en.
6
[4] NOvA Collaboration, D. Ayres et al., “The NOvA Technical Design Report,”.
7
http://lss.fnal.gov/archive/design/fermilab-design-2007-01.pdf.
8
[5] DUNE Collaboration, “TDR Volume 2: The Physics Program for DUNE at LBNF,” tech.
9
rep., 2018. http://docs.dunescience.org/cgi-bin/ShowDocument?docid=.
10
[6] D. P. et al., “Proton Improvement Plan-II.” http://projectx-docdb.fnal.gov/cgi-bin/
11
RetrieveFile?=1232&filename=1.2%20MW%20Report_Rev5.pdf&version=3, 2013.
12
[7] P. Antonioli et al., “SNEWS: The SuperNova Early Warning System,” New J. Phys. 6
13
(2004) 114, arXiv:astro-ph/0406214.
14
[8] GROND, SALT Group, OzGrav, DFN, INTEGRAL, Virgo, Insight-Hxmt,
15
MAXI Team, Fermi-LAT, J-GEM, RATIR, IceCube, CAASTRO, LWA,
16
ePESSTO, GRAWITA, RIMAS, SKA South Africa/MeerKAT, H.E.S.S., 1M2H
17
Team, IKI-GW Follow-up, Fermi GBM, Pi of Sky, DWF (Deeper Wider Faster
18
Program), Dark Energy Survey, MASTER, AstroSat Cadmium Zinc Telluride
19
Imager Team, Swift, Pierre Auger, ASKAP, VINROUGE, JAGWAR, Chandra
20
Team at McGill University, TTU-NRAO, GROWTH, AGILE Team, MWA,
21
ATCA, AST3, TOROS, Pan-STARRS, NuSTAR, ATLAS Telescopes, BOOTES,
22
CaltechNRAO, LIGO Scientific, High Time Resolution Universe Survey, Nordic
23
Optical Telescope, Las Cumbres Observatory Group, TZAC Consortium,
24
LOFAR, IPN, DLT40, Texas Tech University, HAWC, ANTARES, KU, Dark
25
Energy Camera GW-EM, CALET, Euro VLBI Team, ALMA Collaboration, B. P.
26
Abbott et al., “Multi-messenger Observations of a Binary Neutron Star Merger,” Astrophys.
27
28
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
REFERENCES 1–40
[9] N.Mokhov, “The Mars Code System User’s Guide,” tech. rep., 2009. Fermilab-FN-628.
1
[10] “The G4LBNE Software.”
2
https://cdcvs.fnal.gov/redmine/projects/lbne-beamsim/wiki. Available at
3
https://cdcvs.fnal.gov/redmine/projects/lbne-beamsim/wiki.
4
[11] M. Szleper and A. Para, “Neutrino spectrum at the far detector systematic errors,”
5
arXiv:hep-ex/0110001 [hep-ex].
6
[12] Fields, L. and Weber, A. for the Beam Optimization Task Force, “Beam Optimization Task
7
Force Final Report,” tech. rep., 2017. DUNE DocDB 2901.
8
[13] J. Carron, P. Anne, L. S. How, A. Delbergue, S. Hassanzadeh, D. Cillierre, P. Danto, and
9
10
Sixteenth International Conference on Solid State Lighting and LED-based Illumination
11
Systems 10378 (2017) 20.
12
[14] WA105 Collaboration, S. Murphy, “Status of the WA105-3x1x1 m3 dual phase prototype,”
13
14
//indico.fnal.gov/event/12345/session/1/contribution/5/material/slides/0.pdf.
15
[15] M. Adamowski et al., “The Liquid Argon Purity Demonstrator,” JINST 9 (2014) P07005,
16
arXiv:1403.7236 [physics.ins-det].
17
[16] T. I. Banks et al., “A compact ultra-clean system for deploying radioactive sources inside
18
the KamLAND detector,” Nucl. Instrum. Meth. A769 (2015) 88–96, arXiv:1407.0413
19
[physics.ins-det].
20
[17] KamLAND Collaboration, B. E. Berger et al., “The KamLAND Full-Volume Calibration
21
System,” JINST 4 (2009) P04017, arXiv:0903.0441 [physics.ins-det].
22
[18] S. C. Delaquis, R. Gornea, S. Janos, M. LÃijthi, C. Rudolf von Rohr, M. Schenk, and J. L.
23
Vuilleumier, “Development of a camera casing suited for cryogenic and vacuum
24
applications,” JINST 8 (2013) T12001, arXiv:1310.6601 [physics.ins-det].
25
[19] N. McConkey, N. Spooner, M. Thiesse, M. Wallbank, and T. K. Warburton, “Cryogenic
26
CMOS Cameras for High Voltage Monitoring in Liquid Argon,” JINST 12 no. 03, (2017)
27
P03014, arXiv:1612.06124 [physics.ins-det].
28
[20] M. Auger, A. Blatter, A. Ereditato, D. Goeldi, S. Janos, I. Kreslo, M. Luethi, C. Rudolf von
29
Rohr, T. Strauss, and M. S. Weber, “On the Electric Breakdown in Liquid Argon at
30
Centimeter Scale,” JINST 11 no. 03, (2016) P03017, arXiv:1512.05968
31
[physics.ins-det].
32
[21] B. Carls, G. Horton-Smith, C. C. James, R. M. Kubinski, S. Pordes, A. Schukraft, and
33
34
Inspect the Sense-Wire Planes of the Time Projection Chamber Inside the MicroBooNE
35
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
REFERENCES 1–41
Cryostat,” JINST 10 no. 08, (2015) T08006, arXiv:1507.02508 [physics.ins-det].
1
[22] E. Valencia-Rodriquez and M. Kordosky, “Cameras and lighting: experience,” tech. rep.,
2
3
slides/0.pdf.
4
[23] “Nat-mch.” http://www.nateurope.com/products/NAT-MCH.html.
5
[24] “Om3 fibers.” http://shop.fiber24.net/index.php/en/
6
FO-Patch-Cable-OM3-Multi-mode-50-125-m-Duplex-LC-PC-LC-PC/
7
c-OM3-DUPLEX-1TO1/a-FOPC-F2-O3-DX-LCU-LCU.
8
[25] DUNE Collaboration, C. Cuesta, “Photon detection system for ProtoDUNE dual phase,”
9
JINST 12 no. 12, (2017) C12048, arXiv:1711.08307 [physics.ins-det].
10
[26] WA105 Collaboration, L. Zambelli and S. Murphy, “WA105: A large demonstrator of a
11
liquid argon dual phase TPC,” J. Phys. Conf. Ser. 888 no. 1, (2017) 012202.
12
[27] “Technical Design Report for large-scale neutrino detectors prototyping and phased
13
performance assessment in view of a long-baseline oscillation experiment,” tech. rep., 2014.
14
http://cds.cern.ch/record/1692375/files/arXiv%3A1409.4405.pdf?version=2.
15
[28] http://www.hamamatsu.com.
16
[29] http://www.hamamatsu.com/resources/pdf/etd/LARGE_AREA_PMT_TPMH1286E.pdf.
17
[30] http://www.et-enterprises.com/.
18
[31] http://www.hzcphotonics.com/en_index.html.
19
[32] R. Acciarri et al., “Design and construction of the microboone detector,” Journal of
20
Instrumentation 12 no. 02, (2017) P02017.
21
http://stacks.iop.org/1748-0221/12/i=02/a=P02017.
22
[33] MiniCLEAN Collaboration, A. Hime, “The MiniCLEAN Dark Matter Experiment,” in
23
Particles and fields. Proceedings, Meeting of the Division of the American Physical Society,
24
DPF 2011, Providence, USA, August 9-13, 2011. 2011. arXiv:1110.1005
25
[physics.ins-det].
26
https://inspirehep.net/record/930736/files/arXiv:1110.1005.pdf.
27
[34] ICARUS Collaboration, F. Varanini, “ICARUS detector: present and future,” EPJ Web
28
29
[35] http://www.caen.it/csite/CaenFlyer.jsp?parent=222.
30
[36] https://www.prysmiangroup.com/sites/default/files/business_markets/markets/
31
downloads/datasheets/hf43e_0.pdf.
32
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
REFERENCES 1–42
[37] http://www.caledonian-cables.co.uk/Coaxia_Cable/M17_RG/RG303.html.
1
[38] R. Francini et al., “Vuv-vis optical characterization of tetraphenyl-butadiene films on glass
2
and specular reflector substrates from room to liquid argon temperature,” Journal of
3
Instrumentation 8 no. 09, (2013) P09006.
4
http://stacks.iop.org/1748-0221/8/i=09/a=P09006.
5
[39] https://lartpc-docdb.fnal.gov/0000/000059/001/stycas2850.pdf.
6
[40] https://www.thorlabs.com/thorproduct.cfm?partnumber=FT800UMT.
7
[41] https://www.thorlabs.com/thorproduct.cfm?partnumber=FT200UMT.
8
[42] R. Brun and F. Rademakers, “Root - an object oriented data analysis framework,” Nucl.
9
10
[43] S. Agostinelli et al., “Geant4 - a simulation toolkit,” Nuclear Instruments and Methods in
11
Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated
12
Equipment 506 no. 3, (2003) 250 – 303.
13
http://www.sciencedirect.com/science/article/pii/S0168900203013688.
14
[44] http://sbn-nd.fnal.gov/.
15
[45] https://www.picmg.org/openstandards/microtca/.
16
[46] http://www.allectra.com/index.php/en/.
17
[47] J. Kuppambatti, J. Ban, T. Andeen, P. Kinget, and G. Brooijmans, “A radiation-hard dual
18
channel 4-bit pipeline for a 12-bit 40 MS/s ADC prototype with extended dynamic range for
19
the ATLAS Liquid Argon Calorimeter readout electronics upgrade at the CERN LHC,”
20
JINST 8 (2013) P09008, arXiv:1308.0028 [physics.ins-det].
21
[48] W. Liu, P. Huang, and Y. Chiu, “A 12-bit, 45-ms/s, 3-mw redundant
22
successive-approximation-register analog-to-digital converter with digital calibration,”
23
Solid-State Circuits, IEEE Journal of 46 no. 11, (2011) 2661–2672.
24
[49] W. Yeh et al., “Efficient suppression of substrate noise coupling in cmos technology,”
25
International Conference on Solid State Devices and Materials (2003) 408–409.
26
[50] S. H. Lewis, H. S. Fetterman, G. F. Gross, R. Ramachandran, and T. R. Viswanathan, “A
27
10-b 20-msample/s analog-to-digital converter,” IEEE Journal of Solid-State Circuits 27
28
29
[51] A. N. Karanicolas, H. S. Lee, and K. L. Bacrania, “A 15 b 1 ms/s digitally self-calibrated
30
pipeline adc,” in 1993 IEEE International Solid-State Circuits Conference Digest of
31
Technical Papers, pp. 60–61. Feb, 1993.
32
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal
REFERENCES 1–43
[52] E. G. Soenen and R. L. Geiger, “An architecture and an algorithm for fully digital
1
correction of monolithic pipelined adcs,” IEEE Transactions on Circuits and Systems II:
2
Analog and Digital Signal Processing 42 no. 3, (Mar, 1995) 143–153.
3
[53] D. W. Cline and P. R. Gray, “A power optimized 13-b 5 msamples/s pipelined
4
analog-to-digital converter in 1.2 mu;m cmos,” IEEE Journal of Solid-State Circuits 31
5
6
[54] G. De Geronimo et al., “Front-end ASIC for Liquid Argon TPCs,” 2010 IEEE Nuclear
7
Science Symposium Conference Record, in press (2010) .
8
23 Feb 2018: First draft of the TP volumes due DUNE Technical Proposal