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The nEXO Radioassay Program
Authors:
R. MacLellan,
P. Acharya,
B. Aharmim,
S. Alcantar Anguiano,
A. Anker,
I. J. Arnquist,
D. Auty,
T. Bhatta,
D. Chernyak,
J. S. Choe,
B. Cleveland,
J. Daughhetee,
A. Der Mesrobian-Kabakian,
Y. Y. Ding,
M. L. di Vacri,
J. Farine,
A. D. French,
O. Gileva,
R. Gornea,
K. Harouaka,
K. P. Hobbs,
E. W. Hoppe,
L. K. S. Horkley,
M. Hughes,
L. Kieser
, et al. (126 additional authors not shown)
Abstract:
Material radioactivity compilations, such as the one presented here, are important enablers of science. They are useful for the selection of radiopure materials used in the design and construction of low-energy rare-event search experiments. They allow researchers developing such experiments to save time on material studies and avoid costly duplication of effort. The data presented here were gener…
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Material radioactivity compilations, such as the one presented here, are important enablers of science. They are useful for the selection of radiopure materials used in the design and construction of low-energy rare-event search experiments. They allow researchers developing such experiments to save time on material studies and avoid costly duplication of effort. The data presented here were generated in support of the planned nEXO double-beta decay search. This work contains among the most restrictive constraints on the natural radioactivity content of materials of general interest to the low-radioactivity community, found in any tabulation of this kind. In this study, various techniques were employed; they are described here.
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Submitted 16 April, 2026;
originally announced April 2026.
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Design of a high voltage delivery system for noble liquid time projection chambers
Authors:
R. Saldanha,
L. Pagani,
E. Angelico,
E. P. Bernard,
B. Chana,
S. Delaquis,
R. DeVoe,
M. Elbeltagi,
S. Ferrara,
D. Goeldi,
R. Gornea,
A. Odian,
G. S. Ortega,
C. T. Overman,
L. Placzek,
P. C. Rowson,
K. Skarpaas,
F. Spadoni,
P. Acharya,
A. Amy,
A. Anker,
I. J. Arnquist,
A. Atencio,
J. Bane,
V. Belov
, et al. (107 additional authors not shown)
Abstract:
Noble liquid time projection chambers (TPCs) are a leading technology in the detection of ionizing radiation, particularly in applications such as accelerator neutrino physics, dark matter detection, and neutrinoless double beta decay. This paper addresses the design considerations for implementing stable high voltage (HV) systems within large noble liquid TPCs, with a focus on the nEXO experiment…
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Noble liquid time projection chambers (TPCs) are a leading technology in the detection of ionizing radiation, particularly in applications such as accelerator neutrino physics, dark matter detection, and neutrinoless double beta decay. This paper addresses the design considerations for implementing stable high voltage (HV) systems within large noble liquid TPCs, with a focus on the nEXO experiment. Utilizing insights from prior HV research and experimental investigations, we outline factors influencing HV stability and discuss design choices to improve stability and prevent electrical discharges. A novel HV delivery system concept is presented, tailored for the nEXO TPC, which incorporates these design considerations while also meeting the stringent radiopurity requirements of the nEXO neutrinoless double beta decay search. These design considerations and their specific implementation towards a HV delivery system offer guidance to future experiments applying high voltage in noble liquid environments.
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Submitted 26 February, 2026;
originally announced February 2026.
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Characterization of CRYO ASIC for charge readout in the nEXO experiment
Authors:
Z. Li,
M. Yu,
E. Angelico,
A. Atencio,
A. Gupta,
P. Knauss,
A. Pena-Perez,
B. G. Lenardo,
P. Acharya,
A. Amy,
A. Anker,
I. J. Arnquist,
J. Bane,
V. Belov,
T. Bhatta,
A. Bolotnikov,
J. Breslin,
P. A. Breur,
J. P. Brodsky,
E. Brown,
T. Brunner,
B. Burnell,
E. Caden,
G. F. Cao,
L. Q. Cao
, et al. (119 additional authors not shown)
Abstract:
nEXO is a proposed next-generation experiment searching for the neutrinoless double beta decay of $^{136}$Xe using a tonne-scale liquid xenon (LXe) time projection chamber (TPC). To image the ionization signals from events in the liquid xenon, the detector will employ metallized fused-silica charge collection tiles instrumented with cryogenic application-specific integrated circuits (ASICs), refer…
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nEXO is a proposed next-generation experiment searching for the neutrinoless double beta decay of $^{136}$Xe using a tonne-scale liquid xenon (LXe) time projection chamber (TPC). To image the ionization signals from events in the liquid xenon, the detector will employ metallized fused-silica charge collection tiles instrumented with cryogenic application-specific integrated circuits (ASICs), referred to as CRYO ASIC, which are designed to operate directly in LXe to minimize input capacitance and pick-up noise. Here we present the performance of the CRYO ASIC mounted on an auxiliary printed circuit board and evaluated both in a cryogenic environmental chamber and in a dedicated LXe test stand. We demonstrate that the ASICs achieve the desired performance at liquid xenon temperatures, showing a gain stability better than 0.2% over 24-hour operation and reliable in-situ calibration using an on-chip pulser. In the LXe test stand, we show that boiling caused by the chip heat dissipation can be mitigated by operating the system above ~0.1 MPa. The in-LXe noise measured agrees with simulation, which indicates it the $150~e^-$ design requirement can be satisfied. These results establish CRYO ASIC as a viable low-noise in-LXe charge readout solution for nEXO.
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Submitted 11 December, 2025;
originally announced December 2025.
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From Commissioning to Precision Data-Taking: Resolving Operational Challenges in the Nab Detector Systems
Authors:
L. J. Broussard,
H. Acharya,
R. Alarcon,
S. Baeßler,
M. Benoit,
K. Borah,
C. L. Britton,
E. Brown,
J. Choi,
S. Clymer,
C. Crawford,
N. Ericson,
L. Fabris,
N. Fomin,
J. Fry,
R. Godri,
F. M. Gonzalez,
A. Hagemeier,
J. Hamblen,
S. Hollander,
A. Jezghani,
K. Leung,
N. Macsai,
M. Makela,
D. Mathews
, et al. (14 additional authors not shown)
Abstract:
Our understanding of the weak mixing of quarks, described by the Cabibbo Kobayashi Maskawa (CKM) matrix, currently presents an anomaly. Thanks to major strides in both theory and experiment, improved precision in determinations of the first row of matrix elements has revealed disagreement with the expectation of unitarity. The Nab experiment at the Spallation Neutron Source is designed to precisel…
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Our understanding of the weak mixing of quarks, described by the Cabibbo Kobayashi Maskawa (CKM) matrix, currently presents an anomaly. Thanks to major strides in both theory and experiment, improved precision in determinations of the first row of matrix elements has revealed disagreement with the expectation of unitarity. The Nab experiment at the Spallation Neutron Source is designed to precisely extract the first matrix element $V_{ud}$ and shed light on experimental tensions within the neutron beta decay dataset. Nab's asymmetric spectrometer allows coincident reconstruction of the decay proton and electron energies, which will be used to determine the electron-neutrino correlation coefficient, and thus (with the neutron lifetime) determine $V_{ud}$. This unique approach has provided a more comprehensive view of neutron beta decay, including a first observation of the full momentum phase space of the decay above detector thresholds and limits on exotic neutron states. Recent upgrades to the Nab detector system have improved the robustness and stability of the detector performance in terms of proton detection efficiency, noise performance, and detector segment availability, setting the stage for high precision physics data-taking.
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Submitted 10 November, 2025;
originally announced November 2025.
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Ultra-pure Nickel for Structural Components of Low-Radioactivity Instruments
Authors:
T. J. Roosendaal,
C. T. Overman,
G. S. Ortega,
T. D. Schlieder,
N. D. Rocco,
L. K. S. Horkley,
K. P. Hobbs,
K. Harouaka,
J. L. Orrell,
P. Acharya,
A. Amy,
E. Angelico,
A. Anker,
I. J. Arnquist,
A. Atencio,
J. Bane,
V. Belov,
E. P. Bernard,
T. Bhatta,
A. Bolotnikov,
J. Breslin,
P. A. Breur,
J. P. Brodsky,
E. Brown,
T. Brunner
, et al. (101 additional authors not shown)
Abstract:
The next generation of rare-event search experiments in nuclear and particle physics demand structural materials combining exceptional mechanical strength with ultra-low levels of radioactive contamination. This study evaluates chemical vapor deposition (CVD) nickel as a candidate structural material for such applications. Manufacturer-supplied CVD Ni grown on aluminum substrates underwent tensile…
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The next generation of rare-event search experiments in nuclear and particle physics demand structural materials combining exceptional mechanical strength with ultra-low levels of radioactive contamination. This study evaluates chemical vapor deposition (CVD) nickel as a candidate structural material for such applications. Manufacturer-supplied CVD Ni grown on aluminum substrates underwent tensile testing before and after welding alongside standard Ni samples. CVD Ni exhibited a planar tensile strength of ~600 MPa, significantly surpassing standard nickel. However, welding and heat treatment were found to reduce the tensile strength to levels comparable to standard Ni, with observed porosity in the welds likely contributing to this reduction. Material assay via inductively coupled plasma mass spectrometry (ICP-MS) employing isotope-dilution produced measured bulk concentration of 232-Th, 238-U, and nat-K at the levels of ~70 ppq, <100 ppq, and ~900 ppt, respectively, which is the lowest reported in nickel. Surface-etch profiling uncovered higher concentrations of these contaminants extending ~10 micrometer beneath the surface, likely associated with the aluminum growth substrate. The results reported are compared to the one other well documented usage of CVD Ni in a low radioactive background physics research experiment and a discussion is provided on how the currently reported results may arise from changes in CVD fabrication or testing process. These results establish CVD Ni as a promising low-radioactivity structural material, while outlining the need for further development in welding and surface cleaning techniques to fully realize its potential in large-scale, low radioactive background rare-event search experiments.
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Submitted 11 August, 2025;
originally announced August 2025.
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Sensitivity of nEXO to $^{136}$Xe Charged-Current Interactions: Background-free Searches for Solar Neutrinos and Fermionic Dark Matter
Authors:
G. Richardson,
B. G. Lenardo,
D. Gallacher,
R. Saldanha,
P. Acharya,
S. Al Kharusi,
A. Amy,
E. Angelico,
A. Anker,
I. J. Arnquist,
A. Atencio,
J. Bane,
V. Belov,
E. P. Bernard,
T. Bhatta,
A. Bolotnikov,
J. Breslin,
P. A. Breur,
J. P. Brodsky,
S. Bron,
E. Brown,
T. Brunner,
B. Burnell,
E. Caden,
G. F. Cao
, et al. (113 additional authors not shown)
Abstract:
We study the sensitivity of nEXO to solar neutrino charged-current interactions, $ν_e + ^{136}$Xe$\rightarrow ^{136}$Cs$^* + e^-$, as well as analogous interactions predicted by models of fermionic dark matter. Due to the recently observed low-lying isomeric states of $^{136}$Cs, these interactions will create a time-delayed coincident signal observable in the scintillation channel. Here we develo…
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We study the sensitivity of nEXO to solar neutrino charged-current interactions, $ν_e + ^{136}$Xe$\rightarrow ^{136}$Cs$^* + e^-$, as well as analogous interactions predicted by models of fermionic dark matter. Due to the recently observed low-lying isomeric states of $^{136}$Cs, these interactions will create a time-delayed coincident signal observable in the scintillation channel. Here we develop a detailed Monte Carlo of scintillation emission, propagation, and detection in the nEXO detector to model these signals under different assumptions about the timing resolution of the photosensor readout. We show this correlated signal can be used to achieve background discrimination on the order of $10^{-9}$, enabling nEXO to make background-free measurements of solar neutrinos above the reaction threshold of 0.668 MeV. We project that nEXO could measure the flux of CNO solar neutrinos with a statistical uncertainty of 25%, thus contributing a novel and competitive measurement towards addressing the solar metallicity problem. Additionally, nEXO could measure the mean energy of the $^7$Be neutrinos with a precision of $σ\leq 1.5$ keV and could determine the survival probability of $^{7}$Be and $pep$ solar $ν_e$ with precision comparable to state-of-the-art. These quantities are sensitive to the Sun's core temperature and to non-standard neutrino interactions, respectively. Furthermore, the strong background suppression would allow nEXO to search for for charged-current interactions of fermionic dark matter in the mass range $m_χ$ = $0.668$-$7$ MeV with a sensitivity up to three orders of magnitude better than current limits.
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Submitted 27 June, 2025;
originally announced June 2025.
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Imaging of single barium atoms in a second matrix site in solid xenon for barium tagging in a $^{136}$Xe double beta decay experiment
Authors:
M. Yvaine,
D. Fairbank,
J. Soderstrom,
C. Taylor,
J. Stanley,
T. Walton,
C. Chambers,
A. Iverson,
W. Fairbank,
S. Al Kharusi,
A. Amy,
E. Angelico,
A. Anker,
I. J. Arnquist,
A. Atencio,
J. Bane,
V. Belov,
E. P. Bernard,
T. Bhatta,
A. Bolotnikov,
J. Breslin,
P. A. Breur,
J. P. Brodsky,
E. Brown,
T. Brunner
, et al. (112 additional authors not shown)
Abstract:
Neutrinoless double beta decay is one of the most sensitive probes for new physics beyond the Standard Model of particle physics. One of the isotopes under investigation is $^{136}$Xe, which would double beta decay into $^{136}$Ba. Detecting the single $^{136}$Ba daughter provides a sort of ultimate tool in the discrimination against backgrounds. Previous work demonstrated the ability to perform s…
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Neutrinoless double beta decay is one of the most sensitive probes for new physics beyond the Standard Model of particle physics. One of the isotopes under investigation is $^{136}$Xe, which would double beta decay into $^{136}$Ba. Detecting the single $^{136}$Ba daughter provides a sort of ultimate tool in the discrimination against backgrounds. Previous work demonstrated the ability to perform single atom imaging of Ba atoms in a single-vacancy site of a solid xenon matrix. In this paper, the effort to identify signal from individual barium atoms is extended to Ba atoms in a hexa-vacancy site in the matrix and is achieved despite increased photobleaching in this site. Abrupt fluorescence turn-off of a single Ba atom is also observed. Significant recovery of fluorescence signal lost through photobleaching is demonstrated upon annealing of Ba deposits in the Xe ice. Following annealing, it is observed that Ba atoms in the hexa-vacancy site exhibit antibleaching while Ba atoms in the tetra-vacancy site exhibit bleaching. This may be evidence for a matrix site transfer upon laser excitation. Our findings offer a path of continued research toward tagging of Ba daughters in all significant sites in solid xenon.
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Submitted 28 June, 2024;
originally announced July 2024.
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An integrated online radioassay data storage and analytics tool for nEXO
Authors:
R. H. M. Tsang,
A. Piepke,
S. Al Kharusi,
E. Angelico,
I. J. Arnquist,
A. Atencio,
I. Badhrees,
J. Bane,
V. Belov,
E. P. Bernard,
A. Bhat,
T. Bhatta,
A. Bolotnikov,
P. A. Breur,
J. P. Brodsky,
E. Brown,
T. Brunner,
E. Caden,
G. F. Cao,
L. Q. Cao,
D. Cesmecioglu,
C. Chambers,
E. Chambers,
B. Chana,
S. A. Charlebois
, et al. (135 additional authors not shown)
Abstract:
Large-scale low-background detectors are increasingly used in rare-event searches as experimental collaborations push for enhanced sensitivity. However, building such detectors, in practice, creates an abundance of radioassay data especially during the conceptual phase of an experiment when hundreds of materials are screened for radiopurity. A tool is needed to manage and make use of the radioassa…
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Large-scale low-background detectors are increasingly used in rare-event searches as experimental collaborations push for enhanced sensitivity. However, building such detectors, in practice, creates an abundance of radioassay data especially during the conceptual phase of an experiment when hundreds of materials are screened for radiopurity. A tool is needed to manage and make use of the radioassay screening data to quantitatively assess detector design options. We have developed a Materials Database Application for the nEXO experiment to serve this purpose. This paper describes this database, explains how it functions, and discusses how it streamlines the design of the experiment.
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Submitted 20 June, 2023; v1 submitted 12 April, 2023;
originally announced April 2023.
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Neutrinoless Double Beta Decay
Authors:
C. Adams,
K. Alfonso,
C. Andreoiu,
E. Angelico,
I. J. Arnquist,
J. A. A. Asaadi,
F. T. Avignone,
S. N. Axani,
A. S. Barabash,
P. S. Barbeau,
L. Baudis,
F. Bellini,
M. Beretta,
T. Bhatta,
V. Biancacci,
M. Biassoni,
E. Bossio,
P. A. Breur,
J. P. Brodsky,
C. Brofferio,
E. Brown,
R. Brugnera,
T. Brunner,
N. Burlac,
E. Caden
, et al. (207 additional authors not shown)
Abstract:
This White Paper, prepared for the Fundamental Symmetries, Neutrons, and Neutrinos Town Meeting related to the 2023 Nuclear Physics Long Range Plan, makes the case for double beta decay as a critical component of the future nuclear physics program. The major experimental collaborations and many theorists have endorsed this white paper.
This White Paper, prepared for the Fundamental Symmetries, Neutrons, and Neutrinos Town Meeting related to the 2023 Nuclear Physics Long Range Plan, makes the case for double beta decay as a critical component of the future nuclear physics program. The major experimental collaborations and many theorists have endorsed this white paper.
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Submitted 21 December, 2022;
originally announced December 2022.
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A Review of NEST Models for Liquid Xenon and Exhaustive Comparison to Other Approaches
Authors:
M. Szydagis,
J. Balajthy,
G. A. Block,
J. P. Brodsky,
E. Brown,
J. E. Cutter,
S. J. Farrell,
J. Huang,
A. C. Kamaha,
E. S. Kozlova,
C. S. Liebenthal,
D. N. McKinsey,
K. McMichael,
R. McMonigle,
M. Mooney,
J. Mueller,
K. Ni,
G. R. C. Rischbieter,
K. Trengove,
M. Tripathi,
C. D. Tunnell,
V. Velan,
S. Westerdale,
M. D. Wyman,
Z. Zhao
, et al. (1 additional authors not shown)
Abstract:
This paper will discuss the microphysical simulation of interactions in liquid xenon, the active detector medium in many leading rare-event searches for new physics, and describe experimental observables useful for understanding detector performance. The scintillation and ionization yield distributions for signal and background will be presented using the Noble Element Simulation Technique (NEST),…
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This paper will discuss the microphysical simulation of interactions in liquid xenon, the active detector medium in many leading rare-event searches for new physics, and describe experimental observables useful for understanding detector performance. The scintillation and ionization yield distributions for signal and background will be presented using the Noble Element Simulation Technique (NEST), which is a toolkit based on experimental data and simple, empirical formulae, which mimic previous microphysics modeling, but are guided by data. The NEST models for light and charge production as a function of the particle type, energy, and electric field will be reviewed, as well as models for energy resolution and final pulse areas. NEST will be compared to other models or sets of models, and vetted against real data, with several specific examples pulled from XENON, ZEPLIN, LUX, LZ, PandaX, and table-top experiments used for calibrations.
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Submitted 19 December, 2024; v1 submitted 19 November, 2022;
originally announced November 2022.
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Horizons: Nuclear Astrophysics in the 2020s and Beyond
Authors:
H. Schatz,
A. D. Becerril Reyes,
A. Best,
E. F. Brown,
K. Chatziioannou,
K. A. Chipps,
C. M. Deibel,
R. Ezzeddine,
D. K. Galloway,
C. J. Hansen,
F. Herwig,
A. P. Ji,
M. Lugaro,
Z. Meisel,
D. Norman,
J. S. Read,
L. F. Roberts,
A. Spyrou,
I. Tews,
F. X. Timmes,
C. Travaglio,
N. Vassh,
C. Abia,
P. Adsley,
S. Agarwal
, et al. (140 additional authors not shown)
Abstract:
Nuclear Astrophysics is a field at the intersection of nuclear physics and astrophysics, which seeks to understand the nuclear engines of astronomical objects and the origin of the chemical elements. This white paper summarizes progress and status of the field, the new open questions that have emerged, and the tremendous scientific opportunities that have opened up with major advances in capabilit…
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Nuclear Astrophysics is a field at the intersection of nuclear physics and astrophysics, which seeks to understand the nuclear engines of astronomical objects and the origin of the chemical elements. This white paper summarizes progress and status of the field, the new open questions that have emerged, and the tremendous scientific opportunities that have opened up with major advances in capabilities across an ever growing number of disciplines and subfields that need to be integrated. We take a holistic view of the field discussing the unique challenges and opportunities in nuclear astrophysics in regards to science, diversity, education, and the interdisciplinarity and breadth of the field. Clearly nuclear astrophysics is a dynamic field with a bright future that is entering a new era of discovery opportunities.
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Submitted 16 May, 2022;
originally announced May 2022.
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A Next-Generation Liquid Xenon Observatory for Dark Matter and Neutrino Physics
Authors:
J. Aalbers,
K. Abe,
V. Aerne,
F. Agostini,
S. Ahmed Maouloud,
D. S. Akerib,
D. Yu. Akimov,
J. Akshat,
A. K. Al Musalhi,
F. Alder,
S. K. Alsum,
L. Althueser,
C. S. Amarasinghe,
F. D. Amaro,
A. Ames,
T. J. Anderson,
B. Andrieu,
N. Angelides,
E. Angelino,
J. Angevaare,
V. C. Antochi,
D. Antón Martin,
B. Antunovic,
E. Aprile,
H. M. Araújo
, et al. (572 additional authors not shown)
Abstract:
The nature of dark matter and properties of neutrinos are among the most pressing issues in contemporary particle physics. The dual-phase xenon time-projection chamber is the leading technology to cover the available parameter space for Weakly Interacting Massive Particles (WIMPs), while featuring extensive sensitivity to many alternative dark matter candidates. These detectors can also study neut…
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The nature of dark matter and properties of neutrinos are among the most pressing issues in contemporary particle physics. The dual-phase xenon time-projection chamber is the leading technology to cover the available parameter space for Weakly Interacting Massive Particles (WIMPs), while featuring extensive sensitivity to many alternative dark matter candidates. These detectors can also study neutrinos through neutrinoless double-beta decay and through a variety of astrophysical sources. A next-generation xenon-based detector will therefore be a true multi-purpose observatory to significantly advance particle physics, nuclear physics, astrophysics, solar physics, and cosmology. This review article presents the science cases for such a detector.
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Submitted 4 March, 2022;
originally announced March 2022.
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Development of a $^{127}$Xe calibration source for nEXO
Authors:
B. G. Lenardo,
C. A. Hardy,
R. H. M. Tsang,
J. C. Nzobadila Ondze,
A. Piepke,
S. Triambak,
A. Jamil,
G. Adhikari,
S. Al Kharusi,
E. Angelico,
I. J. Arnquist,
V. Belov,
E. P. Bernard,
A. Bhat,
T. Bhatta,
A. Bolotnikov,
P. A. Breur,
J. P. Brodsky,
E. Brown,
T. Brunner,
E. Caden,
G. F. Cao,
L. Cao,
B. Chana,
S. A. Charlebois
, et al. (103 additional authors not shown)
Abstract:
We study a possible calibration technique for the nEXO experiment using a $^{127}$Xe electron capture source. nEXO is a next-generation search for neutrinoless double beta decay ($0νββ$) that will use a 5-tonne, monolithic liquid xenon time projection chamber (TPC). The xenon, used both as source and detection medium, will be enriched to 90% in $^{136}$Xe. To optimize the event reconstruction and…
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We study a possible calibration technique for the nEXO experiment using a $^{127}$Xe electron capture source. nEXO is a next-generation search for neutrinoless double beta decay ($0νββ$) that will use a 5-tonne, monolithic liquid xenon time projection chamber (TPC). The xenon, used both as source and detection medium, will be enriched to 90% in $^{136}$Xe. To optimize the event reconstruction and energy resolution, calibrations are needed to map the position- and time-dependent detector response. The 36.3 day half-life of $^{127}$Xe and its small $Q$-value compared to that of $^{136}$Xe $0νββ$ would allow a small activity to be maintained continuously in the detector during normal operations without introducing additional backgrounds, thereby enabling in-situ calibration and monitoring of the detector response. In this work we describe a process for producing the source and preliminary experimental tests. We then use simulations to project the precision with which such a source could calibrate spatial corrections to the light and charge response of the nEXO TPC.
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Submitted 12 January, 2022;
originally announced January 2022.
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NEXO: Neutrinoless double beta decay search beyond $10^{28}$ year half-life sensitivity
Authors:
nEXO Collaboration,
G. Adhikari,
S. Al Kharusi,
E. Angelico,
G. Anton,
I. J. Arnquist,
I. Badhrees,
J. Bane,
V. Belov,
E. P. Bernard,
T. Bhatta,
A. Bolotnikov,
P. A. Breur,
J. P. Brodsky,
E. Brown,
T. Brunner,
E. Caden,
G. F. Cao,
L. Cao,
C. Chambers,
B. Chana,
S. A. Charlebois,
D. Chernyak,
M. Chiu,
B. Cleveland
, et al. (136 additional authors not shown)
Abstract:
The nEXO neutrinoless double beta decay experiment is designed to use a time projection chamber and 5000 kg of isotopically enriched liquid xenon to search for the decay in $^{136}$Xe. Progress in the detector design, paired with higher fidelity in its simulation and an advanced data analysis, based on the one used for the final results of EXO-200, produce a sensitivity prediction that exceeds the…
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The nEXO neutrinoless double beta decay experiment is designed to use a time projection chamber and 5000 kg of isotopically enriched liquid xenon to search for the decay in $^{136}$Xe. Progress in the detector design, paired with higher fidelity in its simulation and an advanced data analysis, based on the one used for the final results of EXO-200, produce a sensitivity prediction that exceeds the half-life of $10^{28}$ years. Specifically, improvements have been made in the understanding of production of scintillation photons and charge as well as of their transport and reconstruction in the detector. The more detailed knowledge of the detector construction has been paired with more assays for trace radioactivity in different materials. In particular, the use of custom electroformed copper is now incorporated in the design, leading to a substantial reduction in backgrounds from the intrinsic radioactivity of detector materials. Furthermore, a number of assumptions from previous sensitivity projections have gained further support from interim work validating the nEXO experiment concept. Together these improvements and updates suggest that the nEXO experiment will reach a half-life sensitivity of $1.35\times 10^{28}$ yr at 90% confidence level in 10 years of data taking, covering the parameter space associated with the inverted neutrino mass ordering, along with a significant portion of the parameter space for the normal ordering scenario, for almost all nuclear matrix elements. The effects of backgrounds deviating from the nominal values used for the projections are also illustrated, concluding that the nEXO design is robust against a number of imperfections of the model.
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Submitted 22 February, 2022; v1 submitted 30 June, 2021;
originally announced June 2021.
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$β$-decay of $^{61}$V and its Role in Cooling Accreted Neutron Star Crusts
Authors:
W. -J. Ong,
E. F. Brown,
J. Browne,
S. Ahn,
K. Childers,
B. P. Crider,
A. C. Dombos,
S. S. Gupta,
G. W. Hitt,
C. Langer,
R. Lewis,
S. N. Liddick,
S. Lyons,
Z. Meisel,
P. Möller,
F. Montes,
F. Naqvi,
J. Pereira,
C. Prokop,
D. Richman,
H. Schatz,
K. Schmidt,
A. Spyrou
Abstract:
The interpretation of observations of cooling neutron star crusts in quasi-persistent X-ray transients is affected by predictions of the strength of neutrino cooling via crust Urca processes. The strength of crust Urca neutrino cooling depends sensitively on the electron-capture and $β$-decay ground-state to ground-state transition strengths of neutron-rich rare isotopes. Nuclei with mass number…
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The interpretation of observations of cooling neutron star crusts in quasi-persistent X-ray transients is affected by predictions of the strength of neutrino cooling via crust Urca processes. The strength of crust Urca neutrino cooling depends sensitively on the electron-capture and $β$-decay ground-state to ground-state transition strengths of neutron-rich rare isotopes. Nuclei with mass number $A=61$ are predicted to be among the most abundant in accreted crusts, and the last remaining experimentally undetermined ground-state to ground-state transition strength was the $β$-decay of $^{61}$V. This work reports the first experimental determination of this transition strength, a ground-state branching of 8.1$^{+2.2}_{-2.0} \%$, corresponding to a log $ft$ value of 5.5$^{+0.2}_{-0.2}$. This result was achieved through the measurement of the $β$-delayed $γ$ rays using the total absorption spectrometer SuN and the measurement of the $β$-delayed neutron branch using the neutron long counter system NERO at the National Superconducting Cyclotron Laboratory at Michigan State University. This method helps to mitigate the impact of the Pandemonium effect in extremely neutron-rich nuclei on experimental results. The result implies that $A=61$ nuclei do not provide the strongest cooling in accreted neutron star crusts as expected by some predictions, but that their cooling is still larger compared to most other mass numbers. Only nuclei with mass numbers 31, 33, and 55 are predicted to be cooling more strongly. However, the theoretical predictions for the transition strengths of these nuclei are not consistently accurate enough to draw conclusions on crust cooling. With the experimental approach developed in this work all relevant transitions are within reach to be studied in the future.
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Submitted 10 January, 2021;
originally announced January 2021.
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Energy resolution and linearity of XENON1T in the MeV energy range
Authors:
E. Aprile,
J. Aalbers,
F. Agostini,
M. Alfonsi,
L. Althueser,
F. D. Amaro,
V. C. Antochi,
E. Angelino,
J. Angevaare,
F. Arneodo,
D. Barge,
L. Baudis,
B. Bauermeister,
L. Bellagamba,
M. L. Benabderrahmane,
T. Berger,
P. A. Breur,
A. Brown,
E. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
C. Capelli,
J. M. R. Cardoso,
D. Cichon
, et al. (113 additional authors not shown)
Abstract:
Xenon dual-phase time projection chambers designed to search for Weakly Interacting Massive Particles have so far shown a relative energy resolution which degrades with energy above $\sim$200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $^{136}$Xe at its $Q$-value, $Q_{ββ}\simeq$ 2.46 MeV. For the XEN…
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Xenon dual-phase time projection chambers designed to search for Weakly Interacting Massive Particles have so far shown a relative energy resolution which degrades with energy above $\sim$200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $^{136}$Xe at its $Q$-value, $Q_{ββ}\simeq$ 2.46 MeV. For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at 1 $σ/μ$ is as low as (0.80$\pm$0.02) % in its one-ton fiducial mass, and for single-site interactions at $Q_{ββ}$. We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events.
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Submitted 9 September, 2020; v1 submitted 8 March, 2020;
originally announced March 2020.
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Measurements of electron transport in liquid and gas Xenon using a laser-driven photocathode
Authors:
O. Njoya,
T. Tsang,
M. Tarka,
W. Fairbank,
K. S. Kumar,
T. Rao,
T. Wager,
S. Al Kharusi,
G. Anton,
I. J. Arnquist,
I. Badhrees,
P. S. Barbeau,
D. Beck,
V. Belov,
T. Bhatta,
J. P. Brodsky,
E. Brown,
T. Brunner,
E. Caden,
G. F. Cao,
L. Cao,
W. R. Cen,
C. Chambers,
B. Chana,
S. A. Charlebois
, et al. (131 additional authors not shown)
Abstract:
Measurements of electron drift properties in liquid and gaseous xenon are reported. The electrons are generated by the photoelectric effect in a semi-transparent gold photocathode driven in transmission mode with a pulsed ultraviolet laser. The charges drift and diffuse in a small chamber at various electric fields and a fixed drift distance of 2.0 cm. At an electric field of 0.5 kV/cm, the measur…
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Measurements of electron drift properties in liquid and gaseous xenon are reported. The electrons are generated by the photoelectric effect in a semi-transparent gold photocathode driven in transmission mode with a pulsed ultraviolet laser. The charges drift and diffuse in a small chamber at various electric fields and a fixed drift distance of 2.0 cm. At an electric field of 0.5 kV/cm, the measured drift velocities and corresponding temperature coefficients respectively are $1.97 \pm 0.04$ mm/$μ$s and $(-0.69\pm0.05)$\%/K for liquid xenon, and $1.42 \pm 0.03$ mm/$μ$s and $(+0.11\pm0.01)$\%/K for gaseous xenon at 1.5 bar. In addition, we measure longitudinal diffusion coefficients of $25.7 \pm 4.6$ cm$^2$/s and $149 \pm 23$ cm$^2$/s, for liquid and gas, respectively. The quantum efficiency of the gold photocathode is studied at the photon energy of 4.73 eV in liquid and gaseous xenon, and vacuum. These charge transport properties and the behavior of photocathodes in a xenon environment are important in designing and calibrating future large scale noble liquid detectors.
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Submitted 24 November, 2019;
originally announced November 2019.
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Nano-tracking detector for neutrinoless double beta decay characterization
Authors:
Ethan Brown,
Kelly Odgers,
Adam Tidball
Abstract:
Of the many extensions to the standard model that could possibly generate neutrino mass, most necessitate the neutrino being a Majorana fermion. If this is the case, the rare process of neutrinoless double beta decay is predicted with half lives greater than about $10^{25}$ years. Many current and future experiments look for this decay by identifying a summed double beta energy at the Q value of t…
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Of the many extensions to the standard model that could possibly generate neutrino mass, most necessitate the neutrino being a Majorana fermion. If this is the case, the rare process of neutrinoless double beta decay is predicted with half lives greater than about $10^{25}$ years. Many current and future experiments look for this decay by identifying a summed double beta energy at the Q value of the decay, but adding energy and angular measurements of the individual betas allows the underlying decay mechanism to be probed. A novel nano-tracking detector based on a clever combination of thin film CdTe devices will be presented here. This tracker will have order 100 nm spatial resolution in one dimension while measuring the energy deposition across the track length of electron recoils in the detector. This allows energy and angular correlation measurements of a potential neutrinoless double beta decay signal, as well as a unique background suppression capability. Deep learning algorithms will be used to reconstruct the electron paths, the double beta signals and perform the correlation analyses, and will simultaneously allow clear distinction between double betas and single beta or gamma-induced electronic recoils. The detector concept will be presented, along with preliminary studies, to demonstrate its operation and the physics reach for neutrinoless double beta decay. By exploiting recoil discrimination, an array of these detectors can potentially probe beyond the inverted hierarchy to either follow the next generation of neutrinoless double beta decay experiments or to serve as a post-discovery characterization experiment.
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Submitted 15 October, 2019;
originally announced October 2019.
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Simulation of charge readout with segmented tiles in nEXO
Authors:
Z. Li,
W. R. Cen,
A. Robinson,
D. C. Moore,
L. J. Wen,
A. Odian,
S. Al Kharusi,
G. Anton,
I. J. Arnquist,
I. Badhrees,
P. S. Barbeau,
D. Beck,
V. Belov,
T. Bhatta,
J. P. Brodsky,
E. Brown,
T. Brunner,
E. Caden,
G. F. Cao,
L. Cao,
C. Chambers,
B. Chana,
S. A. Charlebois,
M. Chiu,
B. Cleveland
, et al. (128 additional authors not shown)
Abstract:
nEXO is a proposed experiment to search for the neutrino-less double beta decay ($0νββ$) of $^{136}$Xe in a tonne-scale liquid xenon time projection chamber (TPC). The nEXO TPC will be equipped with charge collection tiles to form the anode. In this work, the charge reconstruction performance of this anode design is studied with a dedicated simulation package. A multi-variate method and a deep neu…
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nEXO is a proposed experiment to search for the neutrino-less double beta decay ($0νββ$) of $^{136}$Xe in a tonne-scale liquid xenon time projection chamber (TPC). The nEXO TPC will be equipped with charge collection tiles to form the anode. In this work, the charge reconstruction performance of this anode design is studied with a dedicated simulation package. A multi-variate method and a deep neural network are developed to distinguish simulated $0νββ$ signals from backgrounds arising from trace levels of natural radioactivity in the detector materials. These simulations indicate that the nEXO TPC with charge-collection tiles shows promising capability to discriminate the $0νββ$ signal from backgrounds. The estimated half-life sensitivity for $0νββ$ decay is improved by $\sim$20$~(32)\%$ with the multi-variate~(deep neural network) methods considered here, relative to the sensitivity estimated in the nEXO pre-conceptual design report.
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Submitted 11 October, 2019; v1 submitted 17 July, 2019;
originally announced July 2019.
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First observation of two-neutrino double electron capture in $^{124}$Xe with XENON1T
Authors:
E. Aprile,
J. Aalbers,
F. Agostini,
M. Alfonsi,
L. Althueser,
F. D. Amaro,
M. Anthony,
V. C. Antochi,
F. Arneodo,
L. Baudis,
B. Bauermeister,
M. L. Benabderrahmane,
T. Berger,
P. A. Breur,
A. Brown,
A. Brown,
E. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
C. Capelli,
J. M. R. Cardoso,
D. Cichon,
D. Coderre,
A. P. Colijn
, et al. (106 additional authors not shown)
Abstract:
Two-neutrino double electron capture ($2ν$ECEC) is a second-order Weak process with predicted half-lives that surpass the age of the Universe by many orders of magnitude. Until now, indications for $2ν$ECEC decays have only been seen for two isotopes, $^{78}$Kr and $^{130}$Ba, and instruments with very low background levels are needed to detect them directly with high statistical significance. The…
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Two-neutrino double electron capture ($2ν$ECEC) is a second-order Weak process with predicted half-lives that surpass the age of the Universe by many orders of magnitude. Until now, indications for $2ν$ECEC decays have only been seen for two isotopes, $^{78}$Kr and $^{130}$Ba, and instruments with very low background levels are needed to detect them directly with high statistical significance. The $2ν$ECEC half-life provides an important input for nuclear structure models and its measurement represents a first step in the search for the neutrinoless double electron capture processes ($0ν$ECEC). A detection of the latter would have implications for the nature of the neutrino and give access to the absolute neutrino mass. Here we report on the first direct observation of $2ν$ECEC in $^{124}$Xe with the XENON1T Dark Matter detector. The significance of the signal is $4.4σ$ and the corresponding half-life $T_{1/2}^{2ν\text{ECEC}} = (1.8\pm 0.5_\text{stat}\pm 0.1_\text{sys})\times 10^{22}\;\text{y}$ is the longest ever measured directly. This study demonstrates that the low background and large target mass of xenon-based Dark Matter detectors make them well suited to measuring other rare processes as well, and it highlights the broad physics reach for even larger next-generation experiments.
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Submitted 24 April, 2019;
originally announced April 2019.
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Imaging individual barium atoms in solid xenon for barium tagging in nEXO
Authors:
C. Chambers,
T. Walton,
D. Fairbank,
A. Craycraft,
D. R. Yahne,
J. Todd,
A. Iverson,
W. Fairbank,
A. Alamare,
J. B. Albert,
G. Anton,
I. J. Arnquist,
I. Badhrees,
P. S. Barbeau,
D. Beck,
V. Belov,
T. Bhatta,
F. Bourque,
J. P. Brodsky,
E. Brown,
T. Brunner,
A. Burenkov,
G. F. Cao,
L. Cao,
W. R. Cen
, et al. (126 additional authors not shown)
Abstract:
The search for neutrinoless double beta decay probes the fundamental properties of neutrinos, including whether or not the neutrino and antineutrino are distinct. Double beta detectors are large and expensive, so background reduction is essential for extracting the highest sensitivity. The identification, or 'tagging', of the $^{136}$Ba daughter atom from double beta decay of $^{136}$Xe provides a…
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The search for neutrinoless double beta decay probes the fundamental properties of neutrinos, including whether or not the neutrino and antineutrino are distinct. Double beta detectors are large and expensive, so background reduction is essential for extracting the highest sensitivity. The identification, or 'tagging', of the $^{136}$Ba daughter atom from double beta decay of $^{136}$Xe provides a technique for eliminating backgrounds in the nEXO neutrinoless double beta decay experiment. The tagging scheme studied in this work utilizes a cryogenic probe to trap the barium atom in solid xenon, where the barium atom is tagged via fluorescence imaging in the solid xenon matrix. Here we demonstrate imaging and counting of individual atoms of barium in solid xenon by scanning a focused laser across a solid xenon matrix deposited on a sapphire window. When the laser sits on an individual atom, the fluorescence persists for $\sim$30~s before dropping abruptly to the background level, a clear confirmation of one-atom imaging. No barium fluorescence persists following evaporation of a barium deposit to a limit of $\leq$0.16\%. This is the first time that single atoms have been imaged in solid noble element. It establishes the basic principle of a barium tagging technique for nEXO.
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Submitted 12 December, 2018; v1 submitted 27 June, 2018;
originally announced June 2018.
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nEXO Pre-Conceptual Design Report
Authors:
nEXO Collaboration,
S. Al Kharusi,
A. Alamre,
J. B. Albert,
M. Alfaris,
G. Anton,
I. J. Arnquist,
I. Badhrees,
P. S. Barbeau,
D. Beck,
V. Belov,
T. Bhatta,
F. Bourque,
J. P. Brodsky,
E. Brown,
T. Brunner,
A. Burenkov,
G. F. Cao,
L. Cao,
W. R. Cen,
C. Chambers,
S. A. Charlebois,
M. Chiu,
B. Cleveland,
R. Conley
, et al. (149 additional authors not shown)
Abstract:
The projected performance and detector configuration of nEXO are described in this pre-Conceptual Design Report (pCDR). nEXO is a tonne-scale neutrinoless double beta ($0νββ$) decay search in $^{136}$Xe, based on the ultra-low background liquid xenon technology validated by EXO-200. With $\simeq$ 5000 kg of xenon enriched to 90% in the isotope 136, nEXO has a projected half-life sensitivity of app…
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The projected performance and detector configuration of nEXO are described in this pre-Conceptual Design Report (pCDR). nEXO is a tonne-scale neutrinoless double beta ($0νββ$) decay search in $^{136}$Xe, based on the ultra-low background liquid xenon technology validated by EXO-200. With $\simeq$ 5000 kg of xenon enriched to 90% in the isotope 136, nEXO has a projected half-life sensitivity of approximately $10^{28}$ years. This represents an improvement in sensitivity of about two orders of magnitude with respect to current results. Based on the experience gained from EXO-200 and the effectiveness of xenon purification techniques, we expect the background to be dominated by external sources of radiation. The sensitivity increase is, therefore, entirely derived from the increase of active mass in a monolithic and homogeneous detector, along with some technical advances perfected in the course of a dedicated R&D program. Hence the risk which is inherent to the construction of a large, ultra-low background detector is reduced, as the intrinsic radioactive contamination requirements are generally not beyond those demonstrated with the present generation $0νββ$ decay experiments. Indeed, most of the required materials have been already assayed or reasonable estimates of their properties are at hand. The details described herein represent the base design of the detector configuration as of early 2018. Where potential design improvements are possible, alternatives are discussed.
This design for nEXO presents a compelling path towards a next generation search for $0νββ$, with a substantial possibility to discover physics beyond the Standard Model.
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Submitted 13 August, 2018; v1 submitted 28 May, 2018;
originally announced May 2018.
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Deep crustal heating by neutrinos from the surface of accreting neutron stars
Authors:
F. J. Fattoyev,
Edward F. Brown,
Andrew Cumming,
Alex Deibel,
C. J. Horowitz,
Bao-An Li,
Zidu Lin
Abstract:
We present a new mechanism for deep crustal heating in accreting neutron stars. Charged pions ($π^+$) are produced in nuclear collisions on the neutron star surface during active accretion and upon decay they provide a flux of neutrinos into the neutron star crust. For massive and/or compact neutron stars, neutrinos deposit $\approx 1\textrm{--} 2 \, \mathrm{MeV}$ of heat per accreted nucleon into…
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We present a new mechanism for deep crustal heating in accreting neutron stars. Charged pions ($π^+$) are produced in nuclear collisions on the neutron star surface during active accretion and upon decay they provide a flux of neutrinos into the neutron star crust. For massive and/or compact neutron stars, neutrinos deposit $\approx 1\textrm{--} 2 \, \mathrm{MeV}$ of heat per accreted nucleon into the inner crust. The strength of neutrino heating is comparable to the previously known sources of deep crustal heating, such as from pycnonuclear fusion reactions, and is relevant for studies of cooling neutron stars. We model the thermal evolution of a transient neutron star in a low-mass X-ray binary, and in the particular case of the neutron star MXB~1659-29 we show that additional deep crustal heating requires a higher thermal conductivity for the neutron star inner crust. A better knowledge of pion production cross sections near threshold would improve the accuracy of our predictions.
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Submitted 29 June, 2018; v1 submitted 27 October, 2017;
originally announced October 2017.
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Sensitivity and discovery potential of the proposed nEXO experiment to neutrinoless double beta decay
Authors:
nEXO Collaboration,
J. B. Albert,
G. Anton,
I. J. Arnquist,
I. Badhrees,
P. S. Barbeau,
D. Beck,
V. Belov,
F. Bourque,
J. P. Brodsky,
E. Brown,
T. Brunner,
A. Burenkov,
G. F. Cao,
L. Cao,
W. R. Cen,
C. Chambers,
S. A. Charlebois,
M. Chiu,
B. Cleveland,
M. Coon,
M. Côté,
A. Craycraft,
W. Cree,
J. Dalmasson
, et al. (121 additional authors not shown)
Abstract:
The next-generation Enriched Xenon Observatory (nEXO) is a proposed experiment to search for neutrinoless double beta ($0νββ$) decay in $^{136}$Xe with a target half-life sensitivity of approximately $10^{28}$ years using $5\times10^3$ kg of isotopically enriched liquid-xenon in a time projection chamber. This improvement of two orders of magnitude in sensitivity over current limits is obtained by…
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The next-generation Enriched Xenon Observatory (nEXO) is a proposed experiment to search for neutrinoless double beta ($0νββ$) decay in $^{136}$Xe with a target half-life sensitivity of approximately $10^{28}$ years using $5\times10^3$ kg of isotopically enriched liquid-xenon in a time projection chamber. This improvement of two orders of magnitude in sensitivity over current limits is obtained by a significant increase of the $^{136}$Xe mass, the monolithic and homogeneous configuration of the active medium, and the multi-parameter measurements of the interactions enabled by the time projection chamber. The detector concept and anticipated performance are presented based upon demonstrated realizable background rates.
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Submitted 19 October, 2018; v1 submitted 13 October, 2017;
originally announced October 2017.
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Search for Two-Neutrino Double Electron Capture of $^{124}$Xe with XENON100
Authors:
The XENON Collaboration,
E. Aprile,
J. Aalbers,
F. Agostini,
M. Alfonsi,
F. D. Amaro,
M. Anthony,
F. Arneodo,
P. Barrow,
L. Baudis,
B. Bauermeister,
M. L. Benabderrahmane,
T. Berger,
P. A. Breur,
A. Brown,
E. Brown,
S. Bruenner,
G. Bruno,
R. Budnik,
L. Bütikofer,
J. Calvén,
J. M. R. Cardoso,
M. Cervantes,
D. Cichon,
D. Coderre
, et al. (92 additional authors not shown)
Abstract:
Two-neutrino double electron capture is a rare nuclear decay where two electrons are simultaneously captured from the atomic shell. For $^{124}$Xe this process has not yet been observed and its detection would provide a new reference for nuclear matrix element calculations. We have conducted a search for two-neutrino double electron capture from the K-shell of $^{124}$Xe using 7636 kg$\cdot$d of d…
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Two-neutrino double electron capture is a rare nuclear decay where two electrons are simultaneously captured from the atomic shell. For $^{124}$Xe this process has not yet been observed and its detection would provide a new reference for nuclear matrix element calculations. We have conducted a search for two-neutrino double electron capture from the K-shell of $^{124}$Xe using 7636 kg$\cdot$d of data from the XENON100 dark matter detector. Using a Bayesian analysis we observed no significant excess above background, leading to a lower 90 % credibility limit on the half-life $T_{1/2}>6.5\times10^{20}$ yr. We also evaluated the sensitivity of the XENON1T experiment, which is currently being commissioned, and find a sensitivity of $T_{1/2}>6.1\times10^{22}$ yr after an exposure of 2 t$\cdot$yr.
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Submitted 16 February, 2017; v1 submitted 12 September, 2016;
originally announced September 2016.
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White Paper on Nuclear Astrophysics
Authors:
Almudena Arcones,
Dan W. Bardayan,
Timothy C. Beers,
Lee A. Berstein,
Jeffrey C. Blackmon,
Bronson Messer,
B. Alex Brown,
Edward F. Brown,
Carl R. Brune,
Art E. Champagne,
Alessandro Chieffi,
Aaron J. Couture,
Pawel Danielewicz,
Roland Diehl,
Mounib El-Eid,
Jutta Escher,
Brian D. Fields,
Carla Fröhlich,
Falk Herwig,
William Raphael Hix,
Christian Iliadis,
William G. Lynch,
Gail C. McLaughlin,
Bradley S. Meyer,
Anthony Mezzacappa
, et al. (18 additional authors not shown)
Abstract:
This white paper informs the nuclear astrophysics community and funding agencies about the scientific directions and priorities of the field and provides input from this community for the 2015 Nuclear Science Long Range Plan. It summarizes the outcome of the nuclear astrophysics town meeting that was held on August 21-23, 2014 in College Station at the campus of Texas A&M University in preparation…
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This white paper informs the nuclear astrophysics community and funding agencies about the scientific directions and priorities of the field and provides input from this community for the 2015 Nuclear Science Long Range Plan. It summarizes the outcome of the nuclear astrophysics town meeting that was held on August 21-23, 2014 in College Station at the campus of Texas A&M University in preparation of the NSAC Nuclear Science Long Range Plan. It also reflects the outcome of an earlier town meeting of the nuclear astrophysics community organized by the Joint Institute for Nuclear Astrophysics (JINA) on October 9- 10, 2012 Detroit, Michigan, with the purpose of developing a vision for nuclear astrophysics in light of the recent NRC decadal surveys in nuclear physics (NP2010) and astronomy (ASTRO2010). The white paper is furthermore informed by the town meeting of the Association of Research at University Nuclear Accelerators (ARUNA) that took place at the University of Notre Dame on June 12-13, 2014. In summary we find that nuclear astrophysics is a modern and vibrant field addressing fundamental science questions at the intersection of nuclear physics and astrophysics. These questions relate to the origin of the elements, the nuclear engines that drive life and death of stars, and the properties of dense matter. A broad range of nuclear accelerator facilities, astronomical observatories, theory efforts, and computational capabilities are needed. With the developments outlined in this white paper, answers to long standing key questions are well within reach in the coming decade.
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Submitted 24 March, 2016; v1 submitted 4 March, 2016;
originally announced March 2016.
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A way forward in the study of the symmetry energy: experiment, theory, and observation
Authors:
C. J. Horowitz,
E. F. Brown,
Y. Kim,
W. G. Lynch,
R. Michaels,
A. Ono,
J. Piekarewicz,
M. B. Tsang,
H. H. Wolter
Abstract:
The symmetry energy describes how the energy of nuclear matter rises as one goes away from equal numbers of neutrons and protons. This is very important to describe neutron rich matter in astrophysics. This article reviews our knowledge of the symmetry energy from theoretical calculations, nuclear structure measurements, heavy ion collisions, and astronomical observations. We then present a roadma…
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The symmetry energy describes how the energy of nuclear matter rises as one goes away from equal numbers of neutrons and protons. This is very important to describe neutron rich matter in astrophysics. This article reviews our knowledge of the symmetry energy from theoretical calculations, nuclear structure measurements, heavy ion collisions, and astronomical observations. We then present a roadmap to make progress in areas of relevance to the symmetry energy that promotes collaboration between the astrophysics and the nuclear physics communities.
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Submitted 22 January, 2014;
originally announced January 2014.
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Low-temperature triple-alpha rate in a full three-body model
Authors:
N. B. Nguyen,
F. M. Nunes,
I. J. Thompson,
E. F. Brown
Abstract:
A new full three-body method is introduced to compute the rate of the triple-alpha capture reaction which is the primary source of $^{12}$C in stars. In this work, we combine the Faddeev hyperspherical harmonics and the R-matrix method to obtain a full solution to the three-body $α+α+α$ continuum. Particular attention is paid to the long range effects caused by the pairwise Coulomb interactions. T…
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A new full three-body method is introduced to compute the rate of the triple-alpha capture reaction which is the primary source of $^{12}$C in stars. In this work, we combine the Faddeev hyperspherical harmonics and the R-matrix method to obtain a full solution to the three-body $α+α+α$ continuum. Particular attention is paid to the long range effects caused by the pairwise Coulomb interactions. The new rate agrees with the NACRE rate for temperatures greater than 0.07 GK, but a large enhancement at lower temperature is found ($\approx 10^{14}$ at 0.02 GK). Our results are compared to previous calculations where additional approximations were made. We show that the new rate does not significantly change the evolution of stars around one solar mass. In particular, such stars still undergo a red-giant phase consistent with observations, and no significant differences are found in the final white dwarfs.
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Submitted 2 August, 2012; v1 submitted 9 December, 2011;
originally announced December 2011.
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Time-of-flight mass measurements for nuclear processes in neutron star crusts
Authors:
A. Estrade,
M. Matos,
H. Schatz,
A. M. Amthor,
D. Bazin,
M. Beard,
A. Becerril,
E. F. Brown,
R. Cyburt,
T. Elliot,
A. Gade,
D. Galaviz,
S. George,
S. S. Gupta,
W. R. Hix,
R. Lau,
G. Lorusso,
P. Moller,
J. Pereira,
M. Portillo,
A. M. Rogers,
D. Shapira,
E. Smith,
A. Stolz,
M. Wallace
, et al. (1 additional authors not shown)
Abstract:
The location of electron capture heat sources in the crust of accreting neutron stars depends on the masses of extremely neutron-rich nuclei. We present first results from a new implementation of the time-of-flight technique to measure nuclear masses of rare isotopes at the National Superconducting Cyclotron Laboratory. The masses of 16 neutron-rich nuclei in the scandium -- nickel range were dete…
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The location of electron capture heat sources in the crust of accreting neutron stars depends on the masses of extremely neutron-rich nuclei. We present first results from a new implementation of the time-of-flight technique to measure nuclear masses of rare isotopes at the National Superconducting Cyclotron Laboratory. The masses of 16 neutron-rich nuclei in the scandium -- nickel range were determined simultaneously, improving the accuracy compared to previous data in 12 cases. The masses of $^{61}${V}, $^{63}${Cr}, $^{66}${Mn}, and $^{74}${Ni} were measured for the first time with mass excesses of $-30.510(890)$ MeV, $-35.280(650)$ MeV, $-36.900(790)$ MeV, and $-49.210(990)$ MeV, respectively. With the measurement of the $^{66}$Mn mass, the locations of the two dominant electron capture heat sources in the outer crust of accreting neutron stars that exhibit superbursts are now experimentally constrained. We find that the location of the $^{66}$Fe$\rightarrow^{66}$Mn electron capture transition occurs significantly closer to the surface than previously assumed because our new experimental Q-value is 2.1 MeV (2.6$σ$) smaller than predicted by the FRDM mass model.
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Submitted 23 September, 2011;
originally announced September 2011.
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Possible Resonances in the 12C + 12C Fusion Rate and Superburst Ignition
Authors:
Randall L. Cooper,
Andrew W. Steiner,
Edward F. Brown
Abstract:
Observationally inferred superburst ignition depths are shallower than models predict. We address this discrepancy by reexamining the superburst trigger mechanism. We first explore the hypothesis of Kuulkers et al. that exothermic electron captures trigger superbursts. We find that all electron capture reactions are thermally stable in accreting neutron star oceans and thus are not a viable trig…
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Observationally inferred superburst ignition depths are shallower than models predict. We address this discrepancy by reexamining the superburst trigger mechanism. We first explore the hypothesis of Kuulkers et al. that exothermic electron captures trigger superbursts. We find that all electron capture reactions are thermally stable in accreting neutron star oceans and thus are not a viable trigger mechanism. Fusion reactions other than 12C + 12C are infeasible as well since the possible reactants either deplete at much shallower depths or have prohibitively large Coulomb barriers. Thus we confirm the proposal of Cumming & Bildsten and Strohmayer & Brown that 12C + 12C triggers superbursts. We then examine the 12C + 12C fusion rate. The reaction cross-section is experimentally unknown at astrophysically relevant energies, but resonances exist in the 12C + 12C system throughout the entire measured energy range. Thus it is likely, and in fact has been predicted, that a resonance exists near the Gamow peak energy ~ 1.5 MeV. For such a hypothetical 1.5 MeV resonance, we derive both a fiducial value and upper limit to the resonance strength and find that such a resonance could decrease the theoretically predicted superburst ignition depth by up to a factor of 4; in this case, observationally inferred superburst ignition depths would accord with model predictions for a range of plausible neutron star parameters. Said differently, such a resonance would decrease the temperature required for unstable 12C ignition at a column depth 10^12 g/cm^2 from 6 x 10^8 K to 5 x 10^8 K. Determining the existence of a strong resonance in the Gamow window requires measurements of the 12C + 12C cross-section down to a center-of-mass energy near 1.5 MeV, which is within reach of the proposed DUSEL facility.
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Submitted 26 June, 2009; v1 submitted 23 March, 2009;
originally announced March 2009.
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Understanding Dilepton Production in Heavy Ion Collisions by Vector Mesons of Different Varieties
Authors:
Gerald E. Brown,
Jeremy W. Holt,
Mannque Rho
Abstract:
A simple schematic model anchored on the notion of hadronic freedom inferred from hidden local symmetry in the vector manifestation, the infinite tower of vector mesons in holographic QCD and "stickiness" of $ππ$ interactions inferred from dispersion relations is used to describe the dileptons produced in relativistic heavy ion collisions at PHENIX/RHIC. It is shown that due to the near "blindne…
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A simple schematic model anchored on the notion of hadronic freedom inferred from hidden local symmetry in the vector manifestation, the infinite tower of vector mesons in holographic QCD and "stickiness" of $ππ$ interactions inferred from dispersion relations is used to describe the dileptons produced in relativistic heavy ion collisions at PHENIX/RHIC. It is shown that due to the near "blindness" of dileptons to Brown-Rho scaling, those dileptons with invariant mass less than $m_ρ=770$ MeV come mostly from pion-composites that we interpret as "transient $ρ$'s."
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Submitted 17 August, 2008;
originally announced August 2008.
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A Hidden Local Field Theory Description of Dileptons in Relativistic Heavy Ion Collisions
Authors:
Gerald E. Brown,
Masayasu Harada,
Jeremy W. Holt,
Mannque Rho,
Chihiro Sasaki
Abstract:
This paper has been withdrawn by the authors. Some of the arguments developed in the paper are erroneous. They will be rectified in a later publication.
This paper has been withdrawn by the authors. Some of the arguments developed in the paper are erroneous. They will be rectified in a later publication.
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Submitted 10 January, 2009; v1 submitted 21 April, 2008;
originally announced April 2008.
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Gamow-Teller strength for the analog transitions to the first T=1/2, J^pi=3/2- states in 13C and 13N and the implications for Type Ia supernovae
Authors:
R. G. T. Zegers,
E. F. Brown,
H. Akimune,
Sam M. Austin,
A. M. van den Berg,
B. A. Brown,
D. A. Chamulak,
Y. Fujita,
M. Fujiwara,
S. Gal`es,
M. N. Harakeh,
H. Hashimoto,
R. Hayami,
G. W. Hitt,
M. Itoh,
T. Kawabata,
K. Kawase,
M. Kinoshita,
K. Nakanishi,
S. Nakayama,
S. Okamura,
Y. Shimbara,
M. Uchida,
H. Ueno,
T. Yamagata
, et al. (1 additional authors not shown)
Abstract:
The Gamow-Teller strength for the transition from the ground state of 13C to the T=1/2, J^pi=3/2- excited state at 3.51 MeV in 13N is extracted via the 13C(3He,t) reaction at 420 MeV. In contrast to results from earlier (p,n) studies on 13C, a good agreement with shell-model calculations and the empirical unit cross section systematics from other nuclei is found. The results are used to study th…
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The Gamow-Teller strength for the transition from the ground state of 13C to the T=1/2, J^pi=3/2- excited state at 3.51 MeV in 13N is extracted via the 13C(3He,t) reaction at 420 MeV. In contrast to results from earlier (p,n) studies on 13C, a good agreement with shell-model calculations and the empirical unit cross section systematics from other nuclei is found. The results are used to study the analog 13N(e-,v_e)13C reaction, which plays a role in the pre-explosion convective phase of type Ia supernovae. Although the differences between the results from the (3He,t) and (p,n) data significantly affect the deduced electron-capture rate and the net heat-deposition in the star due to this transition, the overall effect on the pre-explosive evolution is small.
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Submitted 27 March, 2008; v1 submitted 15 October, 2007;
originally announced October 2007.
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NA60 and BR Scaling In Terms of The Vector Manifestation: Formal Consideration
Authors:
G. E. Brown,
Mannque Rho
Abstract:
The arguments developed in the preceding article on how BR scaling would predict for dilepton production in heavy-ion collisions, e.g., NA60, are augmented with more precise and rigorous arguments.
The arguments developed in the preceding article on how BR scaling would predict for dilepton production in heavy-ion collisions, e.g., NA60, are augmented with more precise and rigorous arguments.
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Submitted 1 September, 2005;
originally announced September 2005.
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NA60 and BR Scaling in Terms of the Vector Manifestation: A Model Approach
Authors:
G. E. Brown,
Mannque Rho
Abstract:
It is pointed out that the comparison between the recent NA60 dimuon data and the so-called "Brown-Rho (BR) scaling" as presented at QM2005 is $not$ founded on a correct interpretation of the prediction of BR scaling as formulated in 1991 and modernized recently and hence the conclusion drawn by both the experimental and theoretical speakers that "BR scaling is ruled out by NA60" is erroneous an…
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It is pointed out that the comparison between the recent NA60 dimuon data and the so-called "Brown-Rho (BR) scaling" as presented at QM2005 is $not$ founded on a correct interpretation of the prediction of BR scaling as formulated in 1991 and modernized recently and hence the conclusion drawn by both the experimental and theoretical speakers that "BR scaling is ruled out by NA60" is erroneous and should be disregarded. We use a simplified model description of how the vector manifestation of hidden local symmetry theory enters into the dilepton production, relegating more rigorous discussions to a follow-up paper.
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Submitted 1 September, 2005;
originally announced September 2005.
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STAR $ρ^0/π^-$ Ratio in Au-Au Peripheral Collisions at RHIC and the Vector Manifestation of Hidden Local Symmetry
Authors:
G. E. Brown,
Chang-Hwan Lee,
Mannque Rho
Abstract:
The hidden local symmetry effective theory, Wilsonian matched to QCD at a matching scale near the chiral scale $\sim 4πf_π$ as formulated by Harada and Yamawaki, presents a scenario drastically different from the standard scenario of heavy-ion collisions in that as the temperature approaches the critical temperature $T_c$ of chiral restoration from below, the mass of the vector mesons and their…
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The hidden local symmetry effective theory, Wilsonian matched to QCD at a matching scale near the chiral scale $\sim 4πf_π$ as formulated by Harada and Yamawaki, presents a scenario drastically different from the standard scenario of heavy-ion collisions in that as the temperature approaches the critical temperature $T_c$ of chiral restoration from below, the mass of the vector mesons and their widths go to zero in the chiral limit or nearly zero otherwise, proportionally to some power of the quark condensate at what is called "vector manifestation (VM) fixed point". This scenario makes a striking prediction that as the fire-ball expands and cools from $T_c$ down toward the freezeout temperature $T_{freezeout}$ in heavy ion collisions, what we call "hadronic freedom" sets in in which hadrons do not interact or barely interact. We suggest that this scenario is testable at RHIC and as a specific example, we provide an astonishingly simple explanation in terms of the vector manifestation suitably extended to include axial-vector mesons for the anomalously large $ρ^0/π^-$ ratio measured in peripheral collisions by STAR.
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Submitted 18 October, 2006; v1 submitted 28 July, 2005;
originally announced July 2005.
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The Ideal Liquid Discovered by RHIC, Infrared Slavery Above and Hadronic Freedom Below $T_c$
Authors:
Gerald E. Brown,
Chang-Hwan Lee,
Mannque Rho
Abstract:
We construct the nature of the matter found in RHIC when its temperature has dropped down close to, and below, $T_c$. Just above $T_c$ it is composed of extremely strongly bound quark-antiquark pairs forming chirally restored mesons of the quantum numbers of the $π, S, ρ$ and $a_1$ with very small size and zero energy and just below $T_c$, it is composed of mesons of the same quantum numbers wit…
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We construct the nature of the matter found in RHIC when its temperature has dropped down close to, and below, $T_c$. Just above $T_c$ it is composed of extremely strongly bound quark-antiquark pairs forming chirally restored mesons of the quantum numbers of the $π, S, ρ$ and $a_1$ with very small size and zero energy and just below $T_c$, it is composed of mesons of the same quantum numbers with zero mass. We invoke infrared slavery for the former and the vector manifestation (VM) of hidden local symmetry for the latter. As the temperature drops below $T_c$, the strongly bound quark-antiquark pairs are ejected into what is basically a region of "hadronic freedom" in which the interactions are zero. Experimental evidences for this are seen in the STAR data.
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Submitted 5 July, 2005;
originally announced July 2005.
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Matter formed at the BNL relativistic heavy ion collider
Authors:
G. E. Brown,
B. A. Gelman,
Mannque Rho
Abstract:
We suggest that the "new form of matter" found just above $T_c$ by RHIC is made up of tightly bound quark-antiquark pairs, essentially 32 chirally restored (more precisely, nearly massless) mesons of the quantum numbers of $π$, $σ$, $ρ$ and $a_1$. Taking the results of lattice gauge simulations (LGS) for the color Coulomb potential from the work of the Bielefeld group and feeding this into a rel…
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We suggest that the "new form of matter" found just above $T_c$ by RHIC is made up of tightly bound quark-antiquark pairs, essentially 32 chirally restored (more precisely, nearly massless) mesons of the quantum numbers of $π$, $σ$, $ρ$ and $a_1$. Taking the results of lattice gauge simulations (LGS) for the color Coulomb potential from the work of the Bielefeld group and feeding this into a relativistic two-body code, after modifying the heavy-quark lattice results so as to include the velocity-velocity interaction, all ground-state eigenvalues of the 32 mesons go to zero at $T_c$ just as they do from below $T_c$ as predicted by the vector manifestation (VM in short) of hidden local symmetry. This could explain the rapid rise in entropy up to $T_c$ found in LGS calculations. We argue that how the dynamics work can be understood from the behavior of the hard and soft glue.
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Submitted 18 October, 2006; v1 submitted 12 May, 2005;
originally announced May 2005.
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Matching the QCD and Hadron Sectors and Medium Dependent Meson Masses; Hadronization in Relativistic Heavy Ion Collisions
Authors:
G. E. Brown,
Mannque Rho
Abstract:
The recent developments on the "vector manifestation" of chiral symmetry by Harada and Yamawaki provide a compelling evidence for, and "refine," the in-medium scaling of hadronic properties in dense/hot matter (call it ``BR scaling") proposed by the authors in 1991. We reinterpret the Harada-Yamawaki result obtained in a Wilsonian renormalization-group approach to hidden local symmetry theory ma…
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The recent developments on the "vector manifestation" of chiral symmetry by Harada and Yamawaki provide a compelling evidence for, and "refine," the in-medium scaling of hadronic properties in dense/hot matter (call it ``BR scaling") proposed by the authors in 1991. We reinterpret the Harada-Yamawaki result obtained in a Wilsonian renormalization-group approach to hidden local symmetry theory matched to QCD at near the chiral scale in terms of the Nambu-Jona-Lasinio model and predict that the vector meson mass in medium should scale $m_ρ^\star/m_ρ\sim (\la\bar{q}q\ra^\star/\la\bar{q}q\ra)^{1/2}$ from $n=0$ up to $\sim n=n_0$ (where $n_0$ is nuclear matter density) and then go over to the linear scaling $m_ρ^\star/m_ρ\sim \la\bar{q}q\ra^\star/\la\bar{q}q\ra$ up to the chiral transition density $n_c$ at which the mass is to vanish (in the chiral limit) according to the vector manifestation fixed point. In the regime of the linear scaling above $n_0$, the (vector) gauge coupling constant should fall linearly in $\la\bar{q}q\ra^\star$, vanishing at the critical point, with the width of the vector meson becoming steeply narrower. We suggest the in-medium vector meson mass, {\em both} parametric and pole, which goes smoothly to zero with increasing density, to be an order parameter for chiral symmetry restoration. Some issues related to recent RHIC observations are qualitatively discussed in the appendices. Our main conclusion that follows from these considerations is that the movement towards chiral restoration can be reliably described in Nambu-Jona-Lasinio mean field, with constituent quarks as variables, although there is probably density discontinuity following chiral restoration.
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Submitted 8 May, 2003; v1 submitted 7 June, 2002;
originally announced June 2002.
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On the Manifestation of Chiral Symmetry in Nuclei and Dense Nuclear Matter
Authors:
G. E. Brown,
Mannque Rho
Abstract:
This article reviews our view on how chiral symmetry, its pattern of breaking and restoration under extreme conditions manifest themselves in the nucleon, nuclei, nuclear matter and dense hadronic matter. Topics treated are nucleon structure in terms of chiral symmetry, "first-principle" (QCD) calculations of the properties of finite nuclei effectuated by embedding the ``standard nuclear physics…
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This article reviews our view on how chiral symmetry, its pattern of breaking and restoration under extreme conditions manifest themselves in the nucleon, nuclei, nuclear matter and dense hadronic matter. Topics treated are nucleon structure in terms of chiral symmetry, "first-principle" (QCD) calculations of the properties of finite nuclei effectuated by embedding the ``standard nuclear physics approach" into the framework of effective field theories of nuclei with predictions for certain astrophysical processes, a reinterpretation of the Brown-Rho (BR) scaling that implements chiral symmetry property of baryon-rich medium à la "vector manifestation" of hidden local symmetry, evidences for BR scaling in nuclear processes at normal nuclear matter density and at higher density, the notion of "broadband equilibration" in heavy-ion processes, and the role of strangeness in the formation of compact stars and their collapse into black-holes. We revisit the "Cheshire-Cat phenomenon" recently revived in the form of "quark-hadron continuity" in mapping low-density structure of hadrons to high-density structure of quarks and gluons and suggest how color-flavor locking in terms of QCD variables and hidden local symmetry in terms of hadronic variables may be connected and how BR scaling could fit into this "continuity" scheme.
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Submitted 10 September, 2001; v1 submitted 11 March, 2001;
originally announced March 2001.
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Photon production in heavy-ion collisions at SPS energies
Authors:
G. Q. Li,
G. E. Brown
Abstract:
Single photon spectra in heavy-ion collisions at SPS energies are studied in the relativistic transport model that incorporates self-consistently the change of hadron masses in dense matter. We separate the total photon spectrum into `background' arising from the radiative decays of $π^0$ and $η$ mesons, and the `themal' one from other sources. For the latter we include contributions from radiat…
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Single photon spectra in heavy-ion collisions at SPS energies are studied in the relativistic transport model that incorporates self-consistently the change of hadron masses in dense matter. We separate the total photon spectrum into `background' arising from the radiative decays of $π^0$ and $η$ mesons, and the `themal' one from other sources. For the latter we include contributions from radiative decays of $ρ$, $ω$, $η'$, and $a_1$, radiative decays of baryon resonances, as well as two-body processes such as $ππ\to ργ$ and $πρ\to πγ$. It is found that more than 95% of all photons come from the decays of $π^0$ and $η$ mesons, while the thermal photons account for less than 5% of the total photon yield. The thermal photon spectra in our calculations with either free or in-medium meson masses do not exceed the upper bound set by the experimental measurment of the WA80 Collaboration.
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Submitted 26 June, 1997;
originally announced June 1997.
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Kaons in dense matter, kaon production in heavy-ion collisions, and kaon condensation in neutron stars
Authors:
G. Q. Li,
C. -H. Lee,
G. E. Brown
Abstract:
The recent past witnesses the growing interdependence between the physics of hadrons, the physics of relativistic heavy-ion collisions, and the physics of compact objects in astrophysics. A notable example is the kaon which plays special roles in all the three fields. In this paper, we first review the various theoretical investigations of kaon properties in nuclear medium, focusing on possible…
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The recent past witnesses the growing interdependence between the physics of hadrons, the physics of relativistic heavy-ion collisions, and the physics of compact objects in astrophysics. A notable example is the kaon which plays special roles in all the three fields. In this paper, we first review the various theoretical investigations of kaon properties in nuclear medium, focusing on possible uncertainties in each model. We then present a detailed transport model study of kaon production in heavy-ion collisions at SIS energies. We shall discuss especially the elementary kaon and antikaon production cross sections in hadron-hadron interactions, that represent one of the most serious uncertainties in the transport model study of particle production in heavy-ion collisions. The main purpose of such a study is to constrain kaon in-medium properties from the heavy-ion data. This can provide useful guidances for the development of theoretical models of the kaon in medium. In the last part of the paper, we apply the kaon in-medium properties extracted from heavy-ion data to the study of neutron star properties. Based on a conventional equation of state of nuclear matter that can be considered as one of the best constrained by available experimental data on finite nuclei, we find that the maximum mass of neutron stars is about 2$M_\odot$, which is reduced to about 1.5$M_\odot$ once kaon condensation as constrained by heavy-ion data is introduced.
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Submitted 23 June, 1997;
originally announced June 1997.