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On the Codesign of Scientific Experiments and Industrial Systems
Authors:
Tommaso Dorigo,
Pietro Vischia,
Shahzaib Abbas,
Tosin Adewumi,
Lama Alkhaled,
Lorenzo Arsini,
Muhammad Awais,
Maxim Borisyak,
András Bóta,
Florian Bury,
Sascha Caron,
James Carzon,
Long Chen,
Prakash C. Chhipa,
Paul Christakopoulos,
Jacopo De Piccoli,
Andrea De Vita,
Zlatan Dimitrov,
Michele Doro,
Luigi Favaro,
Francesco Ferranti,
Santiago Folgueras,
Rihab Gargouri,
Nicolas R. Gauger,
Andrea Giammanco
, et al. (62 additional authors not shown)
Abstract:
The optimization of large experiments in fundamental science, such as detectors for subnuclear physics at particle colliders, shares with the optimization of complex systems for industrial or societal applications the common issue of addressing the inter-relation between parameters describing the hardware used in data production and parameters used to analyse those data. While in many cases this c…
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The optimization of large experiments in fundamental science, such as detectors for subnuclear physics at particle colliders, shares with the optimization of complex systems for industrial or societal applications the common issue of addressing the inter-relation between parameters describing the hardware used in data production and parameters used to analyse those data. While in many cases this coupling can be ignored -- when the problem can be successfully factored into simpler sub-tasks and the latter addressed serially -- there are situations in which that approach fails to converge to the absolute maximum of expected performance, as it results in a mis-alignment of the optimized hardware and software solutions. In this work we consider a few use cases of interest in fundamental science collected primarily from particle physics and related areas, and a pot-pourri of industrial and societal applications where the matter is similarly of relevance. We discuss the emergence of strong hardware-software coupling in some of those systems, as well as co-design procedures that may be deployed to identify the global maximum of their relevant utility functions.
We observe how numerous opportunities exist to advance methods and tools for hardware-software co-design optimization, bridging fundamental science and industry through application- and challenge-driven projects, and shaping the future of scientific experiments and industrial systems.
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Submitted 27 March, 2026;
originally announced March 2026.
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Large Language Models for Physics Instrument Design
Authors:
Sara Zoccheddu,
Shah Rukh Qasim,
Patrick Owen,
Nicola Serra
Abstract:
We study the use of large language models (LLMs) for physics instrument design and compare their performance to reinforcement learning (RL). Using only prompting, LLMs are given task constraints and summaries of prior high-scoring designs and propose complete detector configurations, which we evaluate with the same simulators and reward functions used in RL-based optimization. Although RL yields s…
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We study the use of large language models (LLMs) for physics instrument design and compare their performance to reinforcement learning (RL). Using only prompting, LLMs are given task constraints and summaries of prior high-scoring designs and propose complete detector configurations, which we evaluate with the same simulators and reward functions used in RL-based optimization. Although RL yields stronger final designs, we find that modern LLMs consistently generate valid, resource-aware, and physically meaningful configurations that draw on broad pretrained knowledge of detector design principles and particle--matter interactions, despite having no task-specific training. Based on this result, as a first step toward hybrid design workflows, we explore pairing the LLMs with a dedicated trust region optimizer, serving as a precursor to future pipelines in which LLMs propose and structure design hypotheses while RL performs reward-driven optimization. Based on these experiments, we argue that LLMs are well suited as meta-planners: they can design and orchestrate RL-based optimization studies, define search strategies, and coordinate multiple interacting components within a unified workflow. In doing so, they point toward automated, closed-loop instrument design in which much of the human effort required to structure and supervise optimization can be reduced.
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Submitted 12 January, 2026;
originally announced January 2026.
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Ultra-Fast Muon Transport via Histogram Sampling on GPUs
Authors:
Luis Felipe P. Cattelan,
Shah Rukh Qasim,
Patrick H. Owen,
Nicola Serra
Abstract:
We present a GPU-accelerated method for muon transport based on histogram sampling that delivers orders of magnitude faster performance than CPU-based Geant4 simulation. Our method employs precomputed histograms of momentum loss and scattering, derived from detailed Geant4 simulations, to statistically reproduce all the non-decaying physics processes during muon traversal through matter. Implement…
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We present a GPU-accelerated method for muon transport based on histogram sampling that delivers orders of magnitude faster performance than CPU-based Geant4 simulation. Our method employs precomputed histograms of momentum loss and scattering, derived from detailed Geant4 simulations, to statistically reproduce all the non-decaying physics processes during muon traversal through matter. Implemented as a CUDA kernel, the parallel algorithm enables the concurrent simulation of tens of thousands of particles on a single GPU whilst taking into account a complex geometry and a magnetic field force integrated using a fourth-order Runge-Kutta method. Validation against Geant4 in both simple and realistic detector geometries shows that the approach preserves key physical features while achieving speedups of several orders of magnitude, even compared to CPU-based simulations on a large CPU farm with over a thousand cores. This work highlights the significant potential of GPU-based implementations for particle transport, with applicability extending to neutrino propagation and future implementations including discrete processes such as particle decay.
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Submitted 11 December, 2025;
originally announced December 2025.
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Towards replacing detector simulation with heterogeneous GNNs in flavour physics analyses
Authors:
Guillermo Hijano,
Davide Lancierini,
Alexander Mclean Marshall,
Andrea Mauri,
Patrick Owen,
Mitesh Patel,
Konstantinos Petridis,
Shah Rukh Qasim,
Nicola Serra,
William Sutcliffe,
Hanae Tilquin
Abstract:
Driven by the increasing volume of recorded data, the demand for simulation from experiments based at the Large Hadron Collider will rise sharply in the coming years. Addressing this demand solely with existing computationally intensive workflows is not feasible. This paper introduces a new fast simulation tool designed to address this demand at the LHCb experiment. This tool emulates the detector…
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Driven by the increasing volume of recorded data, the demand for simulation from experiments based at the Large Hadron Collider will rise sharply in the coming years. Addressing this demand solely with existing computationally intensive workflows is not feasible. This paper introduces a new fast simulation tool designed to address this demand at the LHCb experiment. This tool emulates the detector response to arbitrary multibody decay topologies at LHCb. Rather than memorising specific decay channels, the model learns generalisable patterns within the response, allowing it to interpolate to channels not present in the training data. Novel heterogeneous graph neural network architectures are employed that are designed to embed the physical characteristics of the task directly into the network structure. We demonstrate the performance of the tool across a range of decay topologies, showing the networks can correctly model the relationships between complex variables. The architectures and methods presented are generic and could readily be adapted to emulate workflows at other simulation-intensive particle physics experiments.
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Submitted 14 January, 2026; v1 submitted 7 July, 2025;
originally announced July 2025.
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Future Circular Collider Feasibility Study Report: Volume 2, Accelerators, Technical Infrastructure and Safety
Authors:
M. Benedikt,
F. Zimmermann,
B. Auchmann,
W. Bartmann,
J. P. Burnet,
C. Carli,
A. Chancé,
P. Craievich,
M. Giovannozzi,
C. Grojean,
J. Gutleber,
K. Hanke,
A. Henriques,
P. Janot,
C. Lourenço,
M. Mangano,
T. Otto,
J. Poole,
S. Rajagopalan,
T. Raubenheimer,
E. Todesco,
L. Ulrici,
T. Watson,
G. Wilkinson,
A. Abada
, et al. (1439 additional authors not shown)
Abstract:
In response to the 2020 Update of the European Strategy for Particle Physics, the Future Circular Collider (FCC) Feasibility Study was launched as an international collaboration hosted by CERN. This report describes the FCC integrated programme, which consists of two stages: an electron-positron collider (FCC-ee) in the first phase, serving as a high-luminosity Higgs, top, and electroweak factory;…
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In response to the 2020 Update of the European Strategy for Particle Physics, the Future Circular Collider (FCC) Feasibility Study was launched as an international collaboration hosted by CERN. This report describes the FCC integrated programme, which consists of two stages: an electron-positron collider (FCC-ee) in the first phase, serving as a high-luminosity Higgs, top, and electroweak factory; followed by a proton-proton collider (FCC-hh) at the energy frontier in the second phase.
FCC-ee is designed to operate at four key centre-of-mass energies: the Z pole, the WW production threshold, the ZH production peak, and the top/anti-top production threshold - delivering the highest possible luminosities to four experiments. Over 15 years of operation, FCC-ee will produce more than 6 trillion Z bosons, 200 million WW pairs, nearly 3 million Higgs bosons, and 2 million top anti-top pairs. Precise energy calibration at the Z pole and WW threshold will be achieved through frequent resonant depolarisation of pilot bunches. The sequence of operation modes remains flexible.
FCC-hh will operate at a centre-of-mass energy of approximately 85 TeV - nearly an order of magnitude higher than the LHC - and is designed to deliver 5 to 10 times the integrated luminosity of the HL-LHC. Its mass reach for direct discovery extends to several tens of TeV. In addition to proton-proton collisions, FCC-hh is capable of supporting ion-ion, ion-proton, and lepton-hadron collision modes.
This second volume of the Feasibility Study Report presents the complete design of the FCC-ee collider, its operation and staging strategy, the full-energy booster and injector complex, required accelerator technologies, safety concepts, and technical infrastructure. It also includes the design of the FCC-hh hadron collider, development of high-field magnets, hadron injector options, and key technical systems for FCC-hh.
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Submitted 25 April, 2025;
originally announced May 2025.
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Future Circular Collider Feasibility Study Report: Volume 3, Civil Engineering, Implementation and Sustainability
Authors:
M. Benedikt,
F. Zimmermann,
B. Auchmann,
W. Bartmann,
J. P. Burnet,
C. Carli,
A. Chancé,
P. Craievich,
M. Giovannozzi,
C. Grojean,
J. Gutleber,
K. Hanke,
A. Henriques,
P. Janot,
C. Lourenço,
M. Mangano,
T. Otto,
J. Poole,
S. Rajagopalan,
T. Raubenheimer,
E. Todesco,
L. Ulrici,
T. Watson,
G. Wilkinson,
P. Azzi
, et al. (1439 additional authors not shown)
Abstract:
Volume 3 of the FCC Feasibility Report presents studies related to civil engineering, the development of a project implementation scenario, and environmental and sustainability aspects. The report details the iterative improvements made to the civil engineering concepts since 2018, taking into account subsurface conditions, accelerator and experiment requirements, and territorial considerations. I…
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Volume 3 of the FCC Feasibility Report presents studies related to civil engineering, the development of a project implementation scenario, and environmental and sustainability aspects. The report details the iterative improvements made to the civil engineering concepts since 2018, taking into account subsurface conditions, accelerator and experiment requirements, and territorial considerations. It outlines a technically feasible and economically viable civil engineering configuration that serves as the baseline for detailed subsurface investigations, construction design, cost estimation, and project implementation planning. Additionally, the report highlights ongoing subsurface investigations in key areas to support the development of an improved 3D subsurface model of the region.
The report describes development of the project scenario based on the 'avoid-reduce-compensate' iterative optimisation approach. The reference scenario balances optimal physics performance with territorial compatibility, implementation risks, and costs. Environmental field investigations covering almost 600 hectares of terrain - including numerous urban, economic, social, and technical aspects - confirmed the project's technical feasibility and contributed to the preparation of essential input documents for the formal project authorisation phase. The summary also highlights the initiation of public dialogue as part of the authorisation process. The results of a comprehensive socio-economic impact assessment, which included significant environmental effects, are presented. Even under the most conservative and stringent conditions, a positive benefit-cost ratio for the FCC-ee is obtained. Finally, the report provides a concise summary of the studies conducted to document the current state of the environment.
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Submitted 25 April, 2025;
originally announced May 2025.
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Future Circular Collider Feasibility Study Report: Volume 1, Physics, Experiments, Detectors
Authors:
M. Benedikt,
F. Zimmermann,
B. Auchmann,
W. Bartmann,
J. P. Burnet,
C. Carli,
A. Chancé,
P. Craievich,
M. Giovannozzi,
C. Grojean,
J. Gutleber,
K. Hanke,
A. Henriques,
P. Janot,
C. Lourenço,
M. Mangano,
T. Otto,
J. Poole,
S. Rajagopalan,
T. Raubenheimer,
E. Todesco,
L. Ulrici,
T. Watson,
G. Wilkinson,
P. Azzi
, et al. (1439 additional authors not shown)
Abstract:
Volume 1 of the FCC Feasibility Report presents an overview of the physics case, experimental programme, and detector concepts for the Future Circular Collider (FCC). This volume outlines how FCC would address some of the most profound open questions in particle physics, from precision studies of the Higgs and EW bosons and of the top quark, to the exploration of physics beyond the Standard Model.…
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Volume 1 of the FCC Feasibility Report presents an overview of the physics case, experimental programme, and detector concepts for the Future Circular Collider (FCC). This volume outlines how FCC would address some of the most profound open questions in particle physics, from precision studies of the Higgs and EW bosons and of the top quark, to the exploration of physics beyond the Standard Model. The report reviews the experimental opportunities offered by the staged implementation of FCC, beginning with an electron-positron collider (FCC-ee), operating at several centre-of-mass energies, followed by a hadron collider (FCC-hh). Benchmark examples are given of the expected physics performance, in terms of precision and sensitivity to new phenomena, of each collider stage. Detector requirements and conceptual designs for FCC-ee experiments are discussed, as are the specific demands that the physics programme imposes on the accelerator in the domains of the calibration of the collision energy, and the interface region between the accelerator and the detector. The report also highlights advances in detector, software and computing technologies, as well as the theoretical tools /reconstruction techniques that will enable the precision measurements and discovery potential of the FCC experimental programme. This volume reflects the outcome of a global collaborative effort involving hundreds of scientists and institutions, aided by a dedicated community-building coordination, and provides a targeted assessment of the scientific opportunities and experimental foundations of the FCC programme.
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Submitted 25 April, 2025;
originally announced May 2025.
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Scalable Multi-Task Learning for Particle Collision Event Reconstruction with Heterogeneous Graph Neural Networks
Authors:
William Sutcliffe,
Marta Calvi,
Simone Capelli,
Jonas Eschle,
Julián García Pardiñas,
Abhijit Mathad,
Azusa Uzuki,
Nicola Serra
Abstract:
The growing luminosity frontier at the Large Hadron Collider is challenging the reconstruction and analysis of particle collision events. Increased particle multiplicities are straining latency and storage requirements at the data acquisition stage, while new complications are emerging, including higher background levels and more frequent particle vertex misassociations. This in turn necessitates…
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The growing luminosity frontier at the Large Hadron Collider is challenging the reconstruction and analysis of particle collision events. Increased particle multiplicities are straining latency and storage requirements at the data acquisition stage, while new complications are emerging, including higher background levels and more frequent particle vertex misassociations. This in turn necessitates the development of more holistic and scalable reconstruction methods that take advantage of recent advances in machine learning. We propose a novel Heterogeneous Graph Neural Network (HGNN) architecture featuring unique representations for diverse particle collision relationships and integrated graph pruning layers for scalability. Trained with a multi-task paradigm in an environment mimicking the LHCb experiment, this HGNN significantly improves beauty hadron reconstruction performance. Notably, it concurrently performs particle vertex association and graph pruning within a single framework. We quantify reconstruction and pruning performance, demonstrate enhanced inference time scaling with event complexity, and mitigate potential performance loss using a weighted message passing scheme.
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Submitted 3 November, 2025; v1 submitted 30 April, 2025;
originally announced April 2025.
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Physics Instrument Design with Reinforcement Learning
Authors:
Shah Rukh Qasim,
Patrick Owen,
Nicola Serra
Abstract:
We present a case for the use of Reinforcement Learning (RL) for the design of physics instrument as an alternative to gradient-based instrument-optimization methods. It's applicability is demonstrated using two empirical studies. One is longitudinal segmentation of calorimeters and the second is both transverse segmentation as well longitudinal placement of trackers in a spectrometer. Based on th…
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We present a case for the use of Reinforcement Learning (RL) for the design of physics instrument as an alternative to gradient-based instrument-optimization methods. It's applicability is demonstrated using two empirical studies. One is longitudinal segmentation of calorimeters and the second is both transverse segmentation as well longitudinal placement of trackers in a spectrometer. Based on these experiments, we propose an alternative approach that offers unique advantages over differentiable programming and surrogate-based differentiable design optimization methods. First, Reinforcement Learning (RL) algorithms possess inherent exploratory capabilities, which help mitigate the risk of convergence to local optima. Second, this approach eliminates the necessity of constraining the design to a predefined detector model with fixed parameters. Instead, it allows for the flexible placement of a variable number of detector components and facilitates discrete decision-making. We then discuss the road map of how this idea can be extended into designing very complex instruments. The presented study sets the stage for a novel framework in physics instrument design, offering a scalable and efficient framework that can be pivotal for future projects such as the Future Circular Collider (FCC), where most optimized detectors are essential for exploring physics at unprecedented energy scales.
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Submitted 13 December, 2024;
originally announced December 2024.
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FunTuple: A new N-tuple component for offline data processing at the LHCb experiment
Authors:
Abhijit Mathad,
Martina Ferrillo,
Sacha Barré,
Patrick Koppenburg,
Patrick Owen,
Gerhard Raven,
Eduardo Rodrigues,
Nicola Serra
Abstract:
The offline software framework of the LHCb experiment has undergone a significant overhaul to tackle the data processing challenges that will arise in the upcoming Run 3 and Run 4 of the Large Hadron Collider. This paper introduces FunTuple, a novel component developed for offline data processing within the LHCb experiment. This component enables the computation and storage of a diverse range of o…
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The offline software framework of the LHCb experiment has undergone a significant overhaul to tackle the data processing challenges that will arise in the upcoming Run 3 and Run 4 of the Large Hadron Collider. This paper introduces FunTuple, a novel component developed for offline data processing within the LHCb experiment. This component enables the computation and storage of a diverse range of observables for both reconstructed and simulated events by leveraging on the tools initially developed for the trigger system. This feature is crucial for ensuring consistency between trigger-computed and offline-analysed observables. The component and its tool suite offer users flexibility to customise stored observables, and its reliability is validated through a full-coverage set of rigorous unit tests. This paper comprehensively explores FunTuple's design, interface, interaction with other algorithms, and its role in facilitating offline data processing for the LHCb experiment for the next decade and beyond.
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Submitted 25 February, 2024; v1 submitted 3 October, 2023;
originally announced October 2023.
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The LHCb upgrade I
Authors:
LHCb collaboration,
R. Aaij,
A. S. W. Abdelmotteleb,
C. Abellan Beteta,
F. Abudinén,
C. Achard,
T. Ackernley,
B. Adeva,
M. Adinolfi,
P. Adlarson,
H. Afsharnia,
C. Agapopoulou,
C. A. Aidala,
Z. Ajaltouni,
S. Akar,
K. Akiba,
P. Albicocco,
J. Albrecht,
F. Alessio,
M. Alexander,
A. Alfonso Albero,
Z. Aliouche,
P. Alvarez Cartelle,
R. Amalric,
S. Amato
, et al. (1298 additional authors not shown)
Abstract:
The LHCb upgrade represents a major change of the experiment. The detectors have been almost completely renewed to allow running at an instantaneous luminosity five times larger than that of the previous running periods. Readout of all detectors into an all-software trigger is central to the new design, facilitating the reconstruction of events at the maximum LHC interaction rate, and their select…
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The LHCb upgrade represents a major change of the experiment. The detectors have been almost completely renewed to allow running at an instantaneous luminosity five times larger than that of the previous running periods. Readout of all detectors into an all-software trigger is central to the new design, facilitating the reconstruction of events at the maximum LHC interaction rate, and their selection in real time. The experiment's tracking system has been completely upgraded with a new pixel vertex detector, a silicon tracker upstream of the dipole magnet and three scintillating fibre tracking stations downstream of the magnet. The whole photon detection system of the RICH detectors has been renewed and the readout electronics of the calorimeter and muon systems have been fully overhauled. The first stage of the all-software trigger is implemented on a GPU farm. The output of the trigger provides a combination of totally reconstructed physics objects, such as tracks and vertices, ready for final analysis, and of entire events which need further offline reprocessing. This scheme required a complete revision of the computing model and rewriting of the experiment's software.
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Submitted 10 September, 2024; v1 submitted 17 May, 2023;
originally announced May 2023.
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GNN for Deep Full Event Interpretation and hierarchical reconstruction of heavy-hadron decays in proton-proton collisions
Authors:
Julián García Pardiñas,
Marta Calvi,
Jonas Eschle,
Andrea Mauri,
Simone Meloni,
Martina Mozzanica,
Nicola Serra
Abstract:
The LHCb experiment at the Large Hadron Collider (LHC) is designed to perform high-precision measurements of heavy-hadron decays, which requires the collection of large data samples and a good understanding and suppression of multiple background sources. Both factors are challenged by a five-fold increase in the average number of proton-proton collisions per bunch crossing, corresponding to a chan…
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The LHCb experiment at the Large Hadron Collider (LHC) is designed to perform high-precision measurements of heavy-hadron decays, which requires the collection of large data samples and a good understanding and suppression of multiple background sources. Both factors are challenged by a five-fold increase in the average number of proton-proton collisions per bunch crossing, corresponding to a change in the detector operation conditions for the LHCb Upgrade I phase, recently started. A further ten-fold increase is expected in the Upgrade II phase, planed for the next decade. The limits in the storage capacity of the trigger will bring an inverse relation between the amount of particles selected to be stored per event and the number of events that can be recorded, and the background levels will raise due to the enlarged combinatorics. To tackle both challenges, we propose a novel approach, never attempted before in a hadronic collider: a Deep-learning based Full Event Interpretation (DFEI), to perform the simultaneous identification, isolation and hierarchical reconstruction of all the heavy-hadron decay chains per event. This approach radically contrasts with the standard selection procedure used in LHCb to identify heavy-hadron decays, that looks individually at sub-sets of particles compatible with being products of specific decay types, disregarding the contextual information from the rest of the event. We present the first prototype for the DFEI algorithm, that leverages the power of Graph Neural Networks (GNN). This paper describes the design and development of the algorithm, and its performance in Upgrade I simulated conditions.
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Submitted 28 April, 2023; v1 submitted 17 April, 2023;
originally announced April 2023.
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A High Pressure Time Projection Chamber with Optical Readout
Authors:
Alexander Deisting,
Abigail Victoria Waldron,
Edward Atkin,
Gary Barker,
Anastasia Basharina-Freshville,
Christopher Betancourt,
Steven Boyd,
Dominic Brailsford,
Zachary Chen-Wishart,
Linda Cremonesi,
Adriana Dias,
Patrick Dunne,
Jennifer Haigh,
Philip Hamacher-Baumann,
Sebastian Jones,
Asher Kaboth,
Alexander Korzenev,
William Ma,
Philippe Mermod,
Maria Mironova,
Jocelyn Monroe,
Ryan Nichol,
Toby Nonnenmacher,
Jaroslaw Nowak,
William Parker
, et al. (11 additional authors not shown)
Abstract:
Measurements of proton-nucleus scattering and high resolution neutrino-nucleus interaction imaging are key to reduce neutrino oscillation systematic uncertainties in future experiments. A High Pressure Time Projection Chamber (HPTPC) prototype has been constructed and operated at Royal Holloway University of London and CERN as a first step in the development of a HPTPC capable of performing these…
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Measurements of proton-nucleus scattering and high resolution neutrino-nucleus interaction imaging are key to reduce neutrino oscillation systematic uncertainties in future experiments. A High Pressure Time Projection Chamber (HPTPC) prototype has been constructed and operated at Royal Holloway University of London and CERN as a first step in the development of a HPTPC capable of performing these measurements as part of a future long-baseline neutrino oscillation experiment such as the Deep Underground Neutrino Experiment. In this paper we describe the design and operation of the prototype HPTPC with an argon based gas mixture. We report on the successful hybrid charge and optical readout, using four CCD cameras, of signals from Am-241 sources.
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Submitted 2 June, 2021; v1 submitted 12 February, 2021;
originally announced February 2021.
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Technical design of the phase I Mu3e experiment
Authors:
K. Arndt,
H. Augustin,
P. Baesso,
N. Berger,
F. Berg,
C. Betancourt,
D. Bortoletto,
A. Bravar,
K. Briggl,
D. vom Bruch,
A. Buonaura,
F. Cadoux,
C. Chavez Barajas,
H. Chen,
K. Clark,
P. Cooke,
S. Corrodi,
A. Damyanova,
Y. Demets,
S. Dittmeier,
P. Eckert,
F. Ehrler,
D. Fahrni,
S. Gagneur,
L. Gerritzen
, et al. (80 additional authors not shown)
Abstract:
The Mu3e experiment aims to find or exclude the lepton flavour violating decay $μ\rightarrow eee$ at branching fractions above $10^{-16}$. A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of $2\cdot 10^{-15}$. We present an overview of all aspects of the technical design and expected performance of the p…
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The Mu3e experiment aims to find or exclude the lepton flavour violating decay $μ\rightarrow eee$ at branching fractions above $10^{-16}$. A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of $2\cdot 10^{-15}$. We present an overview of all aspects of the technical design and expected performance of the phase~I Mu3e detector. The high rate of up to $10^{8}$ muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements.
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Submitted 26 August, 2021; v1 submitted 24 September, 2020;
originally announced September 2020.
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Off-Axis Characterisation of the CERN T10 Beam for low Momentum Proton Measurements with a High Pressure Gas Time Projection Chamber
Authors:
S. B. Jones,
T. S. Nonnenmacher,
E. Atkin,
G. J. Barker,
A. Basharina-Freshville,
C. Betancourt,
S. B. Boyd,
D. Brailsford,
Z. Chen-Wishart,
L. Cremonesi,
A. Deisting,
A. Dias,
P. Dunne,
J. Haigh,
P. Hamacher-Baumann,
A. Kaboth,
A. Korzenev,
W. Ma,
P. Mermod,
M. Mironova,
J. Monroe,
R. Nichol,
J. Nowak,
W. Parker,
H. Ritchie-Yates
, et al. (11 additional authors not shown)
Abstract:
We present studies of proton fluxes in the T10 beamline at CERN. A prototype high pressure gas time projection chamber (TPC) was exposed to the beam of protons and other particles, using the 0.8 GeV/c momentum setting in T10, in order to make cross section measurements of low energy protons in argon. To explore the energy region comparable to hadrons produced by GeV-scale neutrino interactions at…
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We present studies of proton fluxes in the T10 beamline at CERN. A prototype high pressure gas time projection chamber (TPC) was exposed to the beam of protons and other particles, using the 0.8 GeV/c momentum setting in T10, in order to make cross section measurements of low energy protons in argon. To explore the energy region comparable to hadrons produced by GeV-scale neutrino interactions at oscillation experiments, i.e., near 0.1 GeV of kinetic energy, methods of moderating the T10 beam were employed: the dual technique of moderating the beam with acrylic blocks and measuring scattered protons off the beam axis was used to decrease the kinetic energy of incident protons, as well as change the proton/minimum ionising particle (MIP) composition of the incident flux. Measurements of the beam properties were made using time of flight systems upstream and downstream of the TPC. The kinetic energy of protons reaching the TPC was successfully changed from $\sim0.3$ GeV without moderator blocks to less than 0.1 GeV with four moderator blocks (40 cm path length). The flux of both protons and MIPs off the beam axis was increased. The ratio of protons to MIPs vary as a function of the off-axis angle allowing for possible optimisation of the detector to select the type of required particles. Simulation informed by the time of flight measurements show that with four moderator blocks placed in the beamline, ($5.6 \pm 0.1$) protons with energies below 0.1 GeV per spill traversed the active TPC region. Measurements of the beam composition and energy are presented.
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Submitted 30 July, 2020;
originally announced July 2020.
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SND@LHC
Authors:
SHiP Collaboration,
C. Ahdida,
A. Akmete,
R. Albanese,
A. Alexandrov,
M. Andreini,
A. Anokhina,
S. Aoki,
G. Arduini,
E. Atkin,
N. Azorskiy,
J. J. Back,
A. Bagulya,
F. Baaltasar Dos Santos,
A. Baranov,
F. Bardou,
G. J. Barker,
M. Battistin,
J. Bauche,
A. Bay,
V. Bayliss,
G. Bencivenni,
A. Y. Berdnikov,
Y. A. Berdnikov,
M. Bertani
, et al. (319 additional authors not shown)
Abstract:
We propose to build and operate a detector that, for the first time, will measure the process $pp\toνX$ at the LHC and search for feebly interacting particles (FIPs) in an unexplored domain. The TI18 tunnel has been identified as a suitable site to perform these measurements due to very low machine-induced background. The detector will be off-axis with respect to the ATLAS interaction point (IP1)…
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We propose to build and operate a detector that, for the first time, will measure the process $pp\toνX$ at the LHC and search for feebly interacting particles (FIPs) in an unexplored domain. The TI18 tunnel has been identified as a suitable site to perform these measurements due to very low machine-induced background. The detector will be off-axis with respect to the ATLAS interaction point (IP1) and, given the pseudo-rapidity range accessible, the corresponding neutrinos will mostly come from charm decays: the proposed experiment will thus make the first test of the heavy flavour production in a pseudo-rapidity range that is not accessible by the current LHC detectors. In order to efficiently reconstruct neutrino interactions and identify their flavour, the detector will combine in the target region nuclear emulsion technology with scintillating fibre tracking layers and it will adopt a muon identification system based on scintillating bars that will also play the role of a hadronic calorimeter. The time of flight measurement will be achieved thanks to a dedicated timing detector. The detector will be a small-scale prototype of the scattering and neutrino detector (SND) of the SHiP experiment: the operation of this detector will provide an important test of the neutrino reconstruction in a high occupancy environment.
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Submitted 20 February, 2020;
originally announced February 2020.
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zfit: scalable pythonic fitting
Authors:
Jonas Eschle,
Albert Puig Navarro,
Rafael Silva Coutinho,
Nicola Serra
Abstract:
Statistical modeling is a key element in many scientific fields and especially in High-Energy Physics (HEP) analysis. The standard framework to perform this task in HEP is the C++ ROOT/RooFit toolkit; with Python bindings that are only loosely integrated into the scientific Python ecosystem. In this paper, zfit, a new alternative to RooFit written in pure Python, is presented. Most of all, zfit pr…
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Statistical modeling is a key element in many scientific fields and especially in High-Energy Physics (HEP) analysis. The standard framework to perform this task in HEP is the C++ ROOT/RooFit toolkit; with Python bindings that are only loosely integrated into the scientific Python ecosystem. In this paper, zfit, a new alternative to RooFit written in pure Python, is presented. Most of all, zfit provides a well defined high-level API and workflow for advanced model building and fitting, together with an implementation on top of TensorFlow, allowing a transparent usage of CPUs and GPUs. It is designed to be extendable in a very simple fashion, allowing the usage of cutting-edge developments from the scientific Python ecosystem in a transparent way. The main features of zfit are introduced, and its extension to data analysis, especially in the context of HEP experiments, is discussed.
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Submitted 20 May, 2020; v1 submitted 29 October, 2019;
originally announced October 2019.
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Plastic scintillator detector with the readout based on an array of large-area SiPMs for the ND280/T2K upgrade and SHiP experiments
Authors:
A. Korzenev,
C. Betancourt,
A. Blondel,
D. Breton,
A. Datwyler,
D. Gascon,
S. Gomez,
M. Khabibullin,
Y. Kudenko,
J. Maalmi,
P. Mermod,
E. Noah,
N. Serra,
D. Sgalaberna,
B. Storaci
Abstract:
Plastic scintillator detectors have been extensively used in particle physics experiments for decades. A large-scale detector is typically arranged as an array of staggered long bars which provide a fast trigger signal and/or particle identification via time-of-flight measurements. Scintillation light is collected by photosensors coupled to both ends of every bar. In this article, we present our s…
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Plastic scintillator detectors have been extensively used in particle physics experiments for decades. A large-scale detector is typically arranged as an array of staggered long bars which provide a fast trigger signal and/or particle identification via time-of-flight measurements. Scintillation light is collected by photosensors coupled to both ends of every bar. In this article, we present our study on a direct replacement of commonly used vacuum photomultiplier tubes (PMTs) by arrays of large-area silicon photomultipliers (SiPMs). An SiPM array which is directly coupled to the scintillator bulk, has a clear advantage with respect to a PMT: compactness, mechanical robustness, high PDE, low operation voltage, insensitivity to magnetic field, low material budget, possibility to omit light-guides. In this study, arrays of eight 6 x 6 mm2 area SiPMs were coupled to the ends of plastic scintillator bars with 1.68 m and 2.3 m lengths. An 8 channel SiPM anode readout ASIC (eMUSIC) was used for the readout, amplification and summation of signals of individual SiPMs. Timing characteristics of a large-scale detector prototype were studied in test-beams at the CERN PS. This technology is proposed for the ToF system of the ND280/T2K II upgrade at J-PARC and the timing detector of the SHiP experiment at the CERN SPS.
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Submitted 23 January, 2019;
originally announced January 2019.
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Application of large area SiPMs for the readout of a plastic scintillator based timing detector
Authors:
C. Betancourt,
A. Blondel,
R. Brundler,
A. Datwyler,
Y. Favre,
D. Gascon,
S. Gomez,
A. Korzenev,
P. Mermod,
E. Noah,
N. Serra,
D. Sgalaberna,
B. Storaci
Abstract:
In this study an array of eight 6 mm x 6 mm area SiPMs was coupled to the end of a long plastic scintillator counter which was exposed to a 2.5 GeV/c muon beam at the CERN PS. Timing characteristics of bars with dimensions 150 cm x 6 cm x 1 cm and 120 cm x 11 cm x 2.5 cm have been studied. An 8-channel SiPM anode readout ASIC (MUSIC R1) based on a novel low input impedance current conveyor has bee…
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In this study an array of eight 6 mm x 6 mm area SiPMs was coupled to the end of a long plastic scintillator counter which was exposed to a 2.5 GeV/c muon beam at the CERN PS. Timing characteristics of bars with dimensions 150 cm x 6 cm x 1 cm and 120 cm x 11 cm x 2.5 cm have been studied. An 8-channel SiPM anode readout ASIC (MUSIC R1) based on a novel low input impedance current conveyor has been used to read out and amplify SiPMs independently and sum the signals at the end. Prospects for applications in large-scale particle physics detectors with timing resolution below 100 ps are provided in light of the results.
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Submitted 16 December, 2017; v1 submitted 26 September, 2017;
originally announced September 2017.
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FlavBit: A GAMBIT module for computing flavour observables and likelihoods
Authors:
Florian U. Bernlochner,
Marcin Chrzaszcz,
Lars A. Dal,
Ben Farmer,
Paul Jackson,
Anders Kvellestad,
Farvah Mahmoudi,
Antje Putze,
Christopher Rogan,
Pat Scott,
Nicola Serra,
Christoph Weniger,
Martin White
Abstract:
Flavour physics observables are excellent probes of new physics up to very high energy scales. Here we present FlavBit, the dedicated flavour physics module of the global-fitting package GAMBIT. FlavBit includes custom implementations of various likelihood routines for a wide range of flavour observables, including detailed uncertainties and correlations associated with LHCb measurements of rare,…
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Flavour physics observables are excellent probes of new physics up to very high energy scales. Here we present FlavBit, the dedicated flavour physics module of the global-fitting package GAMBIT. FlavBit includes custom implementations of various likelihood routines for a wide range of flavour observables, including detailed uncertainties and correlations associated with LHCb measurements of rare, leptonic and semileptonic decays of B and D mesons, kaons and pions. It provides a generalised interface to external theory codes such as SuperIso, allowing users to calculate flavour observables in and beyond the Standard Model, and then test them in detail against all relevant experimental data. We describe FlavBit and its constituent physics in some detail, then give examples from supersymmetry and effective field theory illustrating how it can be used both as a standalone library for flavour physics, and within GAMBIT.
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Submitted 28 November, 2017; v1 submitted 22 May, 2017;
originally announced May 2017.
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The active muon shield in the SHiP experiment
Authors:
SHiP collaboration,
A. Akmete,
A. Alexandrov,
A. Anokhina,
S. Aoki,
E. Atkin,
N. Azorskiy,
J. J. Back,
A. Bagulya,
A. Baranov,
G. J. Barker,
A. Bay,
V. Bayliss,
G. Bencivenni,
A. Y. Berdnikov,
Y. A. Berdnikov,
M. Bertani,
C. Betancourt,
I. Bezshyiko,
O. Bezshyyko,
D. Bick,
S. Bieschke,
A. Blanco,
J. Boehm,
M. Bogomilov
, et al. (207 additional authors not shown)
Abstract:
The SHiP experiment is designed to search for very weakly interacting particles beyond the Standard Model which are produced in a 400 GeV/c proton beam dump at the CERN SPS. An essential task for the experiment is to keep the Standard Model background level to less than 0.1 event after $2\times 10^{20}$ protons on target. In the beam dump, around $10^{11}$ muons will be produced per second. The mu…
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The SHiP experiment is designed to search for very weakly interacting particles beyond the Standard Model which are produced in a 400 GeV/c proton beam dump at the CERN SPS. An essential task for the experiment is to keep the Standard Model background level to less than 0.1 event after $2\times 10^{20}$ protons on target. In the beam dump, around $10^{11}$ muons will be produced per second. The muon rate in the spectrometer has to be reduced by at least four orders of magnitude to avoid muon-induced combinatorial background. A novel active muon shield is used to magnetically deflect the muons out of the acceptance of the spectrometer. This paper describes the basic principle of such a shield, its optimization and its performance.
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Submitted 18 May, 2017; v1 submitted 10 March, 2017;
originally announced March 2017.
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Three dimensional chaotic advection by mixed layer baroclinic instabilities
Authors:
Daniel Mukiibi,
Gualtiero Badin,
Nuno Serra
Abstract:
Three dimensional (3D) Finite Time Lyapunov Exponents (FTLEs) are computed from numerical simulations of a freely evolving mixed layer (ML) front in a zonal channel undergoing baroclinic instability. The 3D FTLEs show a complex structure, with features that are less defined than the two-dimensional (2D) FTLEs, suggesting that stirring is not confined to the edges of vortices and along filaments an…
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Three dimensional (3D) Finite Time Lyapunov Exponents (FTLEs) are computed from numerical simulations of a freely evolving mixed layer (ML) front in a zonal channel undergoing baroclinic instability. The 3D FTLEs show a complex structure, with features that are less defined than the two-dimensional (2D) FTLEs, suggesting that stirring is not confined to the edges of vortices and along filaments and posing significant consequences on mixing. The magnitude of the FTLEs is observed to be strongly determined by the vertical shear. A scaling law relating the local FTLEs and the nonlocal density contrast used to initialize the ML front is derived assuming thermal wind balance. The scaling law only converges to the values found from the simulations within the pycnocline, while it displays differences within the ML, where the instabilities show a large ageostrophic component. The probability distribution functions of 2D and 3D FTLEs are found to be non Gaussian at all depths. In the ML, the FTLEs wavenumber spectra display -1 slopes, while in the pycnocline, the FTLEs wavenumber spectra display -2 slopes, corresponding to frontal dynamics. Close to the surface, the geodesic Lagrangian Coherent Structures (LCSs) reveal a complex stirring structure, with elliptic structures detaching from the frontal region. In the pycnocline, LCSs are able to detect filamentary structures that are not captured by the Eulerian fields.
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Submitted 11 March, 2016; v1 submitted 6 November, 2015;
originally announced November 2015.
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A facility to Search for Hidden Particles (SHiP) at the CERN SPS
Authors:
SHiP Collaboration,
M. Anelli,
S. Aoki,
G. Arduini,
J. J. Back,
A. Bagulya,
W. Baldini,
A. Baranov,
G. J. Barker,
S. Barsuk,
M. Battistin,
J. Bauche,
A. Bay,
V. Bayliss,
L. Bellagamba,
G. Bencivenni,
M. Bertani,
O. Bezshyyko,
D. Bick,
N. Bingefors,
A. Blondel,
M. Bogomilov,
A. Boyarsky,
D. Bonacorsi,
D. Bondarenko
, et al. (211 additional authors not shown)
Abstract:
A new general purpose fixed target facility is proposed at the CERN SPS accelerator which is aimed at exploring the domain of hidden particles and make measurements with tau neutrinos. Hidden particles are predicted by a large number of models beyond the Standard Model. The high intensity of the SPS 400~GeV beam allows probing a wide variety of models containing light long-lived exotic particles w…
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A new general purpose fixed target facility is proposed at the CERN SPS accelerator which is aimed at exploring the domain of hidden particles and make measurements with tau neutrinos. Hidden particles are predicted by a large number of models beyond the Standard Model. The high intensity of the SPS 400~GeV beam allows probing a wide variety of models containing light long-lived exotic particles with masses below ${\cal O}$(10)~GeV/c$^2$, including very weakly interacting low-energy SUSY states. The experimental programme of the proposed facility is capable of being extended in the future, e.g. to include direct searches for Dark Matter and Lepton Flavour Violation.
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Submitted 20 April, 2015;
originally announced April 2015.
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Extracting Angular Observables without a Likelihood and Applications to Rare Decays
Authors:
Frederik Beaujean,
Marcin Chrząszcz,
Nicola Serra,
Danny van Dyk
Abstract:
Our goal is to obtain a complete set of angular observables arising in a generic multi-body process. We show how this can be achieved without the need to carry out a likelihood fit of the angular distribution to the measured events. Instead, we apply the method of moments that relies both on the orthogonality of angular functions and the estimation of integrals by Monte Carlo techniques. The big a…
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Our goal is to obtain a complete set of angular observables arising in a generic multi-body process. We show how this can be achieved without the need to carry out a likelihood fit of the angular distribution to the measured events. Instead, we apply the method of moments that relies both on the orthogonality of angular functions and the estimation of integrals by Monte Carlo techniques. The big advantage of this method is that the joint distribution of all observables can be easily extracted, even for very few events. The method of moments is shown to be robust against mismodeling of the angular distribution. Our main result is an explicit algorithm that accounts for systematic uncertainties from detector-resolution and acceptance effects. Finally, we present the necessary process-dependent formulae needed for direct application of the method to several rare decays of interest.
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Submitted 13 March, 2015;
originally announced March 2015.
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Performance of the LHCb Outer Tracker
Authors:
LHCb Outer Tracker group,
R. Arink,
S. Bachmann,
Y. Bagaturia,
H. Band,
Th. Bauer,
A. Berkien,
Ch. Färber,
A. Bien,
J. Blouw,
L. Ceelie,
V. Coco,
M. Deckenhoff,
Z. Deng,
F. Dettori,
D. van Eijk,
R. Ekelhof,
E. Gersabeck,
L. Grillo,
W. D. Hulsbergen,
T. M. Karbach,
R. Koopman,
A. Kozlinskiy,
Ch. Langenbruch,
V. Lavrentyev
, et al. (30 additional authors not shown)
Abstract:
The LHCb Outer Tracker is a gaseous detector covering an area of 5x6 m2 with 12 double layers of straw tubes. The detector with its services are described together with the commissioning and calibration procedures. Based on data of the first LHC running period from 2010 to 2012, the performance of the readout electronics and the single hit resolution and efficiency are presented. The efficiency to…
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The LHCb Outer Tracker is a gaseous detector covering an area of 5x6 m2 with 12 double layers of straw tubes. The detector with its services are described together with the commissioning and calibration procedures. Based on data of the first LHC running period from 2010 to 2012, the performance of the readout electronics and the single hit resolution and efficiency are presented. The efficiency to detect a hit in the central half of the straw is estimated to be 99.2%, and the position resolution is determined to be approximately 200 um. The Outer Tracker received a dose in the hottest region corresponding to 0.12 C/cm, and no signs of gain deterioration or other ageing effects are observed.
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Submitted 22 January, 2014; v1 submitted 15 November, 2013;
originally announced November 2013.
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Performance of the LHCb muon system
Authors:
A. A. Alves Jr,
L. Anderlini,
M. Anelli,
R. Antunes Nobrega,
G. Auriemma,
W. Baldini,
G. Bencivenni,
R. Berutti,
A. Bizzeti,
V. Bocci,
N. Bondar,
W. Bonivento,
B. Botchin,
S. Cadeddu,
P. Campana,
G. Carboni,
A. Cardini,
M. Carletti,
P. Ciambrone,
E. Dané S. De Capua,
V. De Leo,
C. Deplano,
P. De Simone,
F. Dettori,
A. Falabella
, et al. (48 additional authors not shown)
Abstract:
The performance of the LHCb Muon system and its stability across the full 2010 data taking with LHC running at ps = 7 TeV energy is studied. The optimization of the detector setting and the time calibration performed with the first collisions delivered by LHC is described. Particle rates, measured for the wide range of luminosities and beam operation conditions experienced during the run, are comp…
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The performance of the LHCb Muon system and its stability across the full 2010 data taking with LHC running at ps = 7 TeV energy is studied. The optimization of the detector setting and the time calibration performed with the first collisions delivered by LHC is described. Particle rates, measured for the wide range of luminosities and beam operation conditions experienced during the run, are compared with the values expected from simulation. The space and time alignment of the detectors, chamber efficiency, time resolution and cluster size are evaluated. The detector performance is found to be as expected from specifications or better. Notably the overall efficiency is well above the design requirements
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Submitted 15 February, 2013; v1 submitted 6 November, 2012;
originally announced November 2012.
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Absolute luminosity measurements with the LHCb detector at the LHC
Authors:
The LHCb Collaboration,
R. Aaij,
B. Adeva,
M. Adinolfi,
C. Adrover,
A. Affolder,
Z. Ajaltouni,
J. Albrecht,
F. Alessio,
M. Alexander,
G. Alkhazov,
P. Alvarez Cartelle,
A. A. Alves Jr,
S. Amato,
Y. Amhis,
J. Anderson,
R. B. Appleby,
O. Aquines Gutierrez,
F. Archilli,
L. Arrabito,
A. Artamonov,
M. Artuso,
E. Aslanides,
G. Auriemma,
S. Bachmann
, et al. (549 additional authors not shown)
Abstract:
Absolute luminosity measurements are of general interest for colliding-beam experiments at storage rings. These measurements are necessary to determine the absolute cross-sections of reaction processes and are valuable to quantify the performance of the accelerator. Using data taken in 2010, LHCb has applied two methods to determine the absolute scale of its luminosity measurements for proton-prot…
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Absolute luminosity measurements are of general interest for colliding-beam experiments at storage rings. These measurements are necessary to determine the absolute cross-sections of reaction processes and are valuable to quantify the performance of the accelerator. Using data taken in 2010, LHCb has applied two methods to determine the absolute scale of its luminosity measurements for proton-proton collisions at the LHC with a centre-of-mass energy of 7 TeV. In addition to the classic "van der Meer scan" method a novel technique has been developed which makes use of direct imaging of the individual beams using beam-gas and beam-beam interactions. This beam imaging method is made possible by the high resolution of the LHCb vertex detector and the close proximity of the detector to the beams, and allows beam parameters such as positions, angles and widths to be determined. The results of the two methods have comparable precision and are in good agreement. Combining the two methods, an overall precision of 3.5% in the absolute luminosity determination is reached. The techniques used to transport the absolute luminosity calibration to the full 2010 data-taking period are presented.
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Submitted 11 January, 2012; v1 submitted 13 October, 2011;
originally announced October 2011.