Javascript must be enabled to continue!
The XLZD Design Book: towards the next-generation liquid xenon observatory for dark matter and neutrino physics
View through CrossRef
Abstract
This report describes the experimental strategy and technologies for XLZD, the next-generation xenon observatory sensitive to dark matter and neutrino physics. In the baseline design, the detector will have an active liquid xenon target of 60 tonnes, which could be increased to 80 tonnes if the market conditions for xenon are favorable. It is based on the mature liquid xenon time projection chamber technology used in current-generation experiments, LZ and XENONnT. The report discusses the baseline design and opportunities for further optimization of the individual detector components. The experiment envisaged here has the capability to explore parameter space for Weakly Interacting Massive Particle (WIMP) dark matter down to the neutrino fog, with a 3
$$\sigma $$
σ
evidence potential for WIMP-nucleon cross sections as low as
$$3\times 10^{-49}\mathrm \,cm^2$$
3
×
10
-
49
c
m
2
(at 40 GeV/c
$$^2$$
2
WIMP mass). The observatory will also have leading sensitivity to a wide range of alternative dark matter models. It is projected to have a 3
$$\sigma $$
σ
observation potential of neutrinoless double beta decay of
$$^{136}$$
136
Xe at a half-life of up to
$$5.7\times 10^{27}$$
5.7
×
10
27
years. Additionally, it is sensitive to astrophysical neutrinos from the sun and galactic supernovae.
Springer Science and Business Media LLC
J. Aalbers
K. Abe
M. Adrover
S. Ahmed Maouloud
D. S. Akerib
A. K. Al Musalhi
F. Alder
L. Althueser
D. W. P. Amaral
C. S. Amarasinghe
A. Ames
B. Andrieu
N. Angelides
E. Angelino
B. Antunovic
E. Aprile
H. M. Araújo
J. E. Armstrong
M. Arthurs
M. Babicz
A. Baker
M. Balzer
J. Bang
E. Barberio
J. W. Bargemann
E. Barillier
A. Basharina-Freshville
L. Baudis
D. Bauer
M. Bazyk
K. Beattie
N. Beaupere
N. F. Bell
L. Bellagamba
T. Benson
A. Bhatti
T. P. Biesiadzinski
R. Biondi
Y. Biondi
H. J. Birch
E. Bishop
A. Bismark
C. Boehm
K. Boese
A. Bolotnikov
P. Brás
R. Braun
A. Breskin
C. A. J. Brew
S. Brommer
A. Brown
G. Bruni
R. Budnik
S. Burdin
C. Cai
C. Capelli
G. Carini
M. C. Carmona-Benitez
M. Carter
A. Chauvin
A. Chawla
H. Chen
J. J. Cherwinka
Y. T. Chin
N. I. Chott
A. P. Cimental Chavez
K. Clark
A. P. Colijn
D. J. Colling
J. Conrad
M. V. Converse
L. J. Cooper
R. Coronel
D. Costanzo
A. Cottle
G. Cox
J. J. Cuenca-García
D. Curran
D. Cussans
V. D’Andrea
L. C. Daniel Garcia
I. Darlington
S. Dave
A. David
G. J. Davies
M. P. Decowski
A. Deisting
J. Delgaudio
S. Dey
C. Di Donato
L. Di Felice
P. Di Gangi
S. Diglio
C. Ding
J. E. Y. Dobson
M. Doerenkamp
G. Drexlin
E. Druszkiewicz
C. L. Dunbar
K. Eitel
A. Elykov
R. Engel
S. R. Eriksen
S. Fayer
N. M. Fearon
A. D. Ferella
C. Ferrari
N. Fieldhouse
H. Fischer
H. Flaecher
T. Flehmke
M. Flierman
E. D. Fraser
T. M. A. Fruth
K. Fujikawa
W. Fulgione
C. Fuselli
P. Gaemers
R. Gaior
R. J. Gaitskell
N. Gallice
M. Galloway
F. Gao
N. Garroum
A. Geffre
J. Genovesi
C. Ghag
S. Ghosh
R. Giacomobono
R. Gibbons
F. Girard
R. Glade-Beucke
F. Glück
S. Gokhale
L. Grandi
J. Green
J. Grigat
M. G. D. van der Grinten
R. Größle
H. Guan
M. Guida
P. Gyorgy
J. J. Haiston
C. R. Hall
T. Hall
R. Hammann
V. Hannen
S. Hansmann-Menzemer
N. Hargittai
E. Hartigan-O’Connor
S. J. Haselschwardt
M. Hernandez
S. A. Hertel
A. Higuera
C. Hils
K. Hiraoka
L. Hoetzsch
M. Hoferichter
G. J. Homenides
N. F. Hood
M. Horn
D. Q. Huang
S. Hughes
D. Hunt
M. Iacovacci
Y. Itow
E. Jacquet
J. Jakob
R. S. James
F. Joerg
S. Jones
A. C. Kaboth
F. Kahlert
A. C. Kamaha
Y. Kaminaga
M. Kara
P. Kavrigin
S. Kazama
M. Keller
P. Kemp-Russell
D. Khaitan
P. Kharbanda
B. Kilminster
J. Kim
R. Kirk
M. Kleifges
M. Klute
M. Kobayashi
D. Kodroff
D. Koke
A. Kopec
E. v Korolkova
H. Kraus
S. Kravitz
L. Kreczko
B. von Krosigk
V. A. Kudryavtsev
F. Kuger
N. Kurita
H. Landsman
R. F. Lang
C. Lawes
J. Lee
B. Lehnert
D. S. Leonard
K. T. Lesko
L. Levinson
A. Li
I. Li
S. Li
S. Liang
Z. Liang
J. Lin
Y.-T. Lin
S. Lindemann
S. Linden
M. Lindner
A. Lindote
W. H. Lippincott
K. Liu
J. Loizeau
F. Lombardi
J. A. M. Lopes
M. I. Lopes
W. Lorenzon
M. Loutit
C. Lu
G. M. Lucchetti
T. Luce
S. Luitz
Y. Ma
C. Macolino
J. Mahlstedt
B. Maier
P. A. Majewski
A. Manalaysay
A. Mancuso
L. Manenti
R. L. Mannino
F. Marignetti
T. Marley
T. Marrodán Undagoitia
K. Martens
J. Masbou
E. Masson
S. Mastroianni
C. Maupin
V. Mazza
C. McCabe
M. E. McCarthy
D. N. McKinsey
J. B. McLaughlin
A. Melchiorre
J. Menéndez
M. Messina
E. H. Miller
B. Milosovic
S. Milutinovic
K. Miuchi
R. Miyata
E. Mizrachi
A. Molinario
C. M. B. Monteiro
M. E. Monzani
K. Morå
S. Moriyama
E. Morrison
E. Morteau
Y. Mosbacher
B. J. Mount
J. Müller
M. Murdy
A. St. J. Murphy
M. Murra
A. Naylor
H. N. Nelson
F. Neves
J. L. Newstead
A. Nguyen
K. Ni
J. O’Dell
C. O’Hare
U. Oberlack
M. Obradovic
I. Olcina
K. C. Oliver-Mallory
G. D. Orebi Gann
J. Orpwood
S. Ouahada
K. Oyulmaz
B. Paetsch
K. J. Palladino
J. Palmer
Y. Pan
M. Pandurovic
N. J. Pannifer
S. Paramesvaran
J. Patton
Q. Pellegrini
B. Penning
G. Pereira
R. Peres
E. Perry
T. Pershing
F. Piastra
J. Pienaar
A. Piepke
M. Pierre
G. Plante
T. R. Pollmann
F. Pompa
L. Principe
J. Qi
K. Qiao
Y. Qie
J. Qin
S. Radeka
V. Radeka
M. Rajado
D. Ramírez García
A. Ravindran
A. Razeto
J. Reichenbacher
C. A. Rhyne
A. Richards
G. R. C. Rischbieter
H. S. Riyat
R. Rosero
A. Roy
T. Rushton
D. Rynders
R. Saakyan
L. Sanchez
P. Sanchez-Lucas
D. Santone
J. M. F. dos Santos
G. Sartorelli
A. B. M. R. Sazzad
A. Scaffidi
R. W. Schnee
J. Schreiner
P. Schulte
H. Schulze Eißing
M. Schumann
A. Schwenck
A. Schwenk
L. Scotto Lavina
M. Selvi
F. Semeria
P. Shagin
S. Sharma
S. Shaw
W. Shen
L. Sherman
S. Shi
S. Y. Shi
T. Shimada
T. Shutt
J. J. Silk
C. Silva
H. Simgen
G. Sinev
R. Singh
J. Siniscalco
M. Solmaz
V. N. Solovov
Z. Song
P. Sorensen
J. Soria
O. Stanley
M. Steidl
T. Stenhouse
A. Stevens
K. Stifter
T. J. Sumner
A. Takeda
P.-L. Tan
D. J. Taylor
W. C. Taylor
D. Thers
T. Thümmler
D. R. Tiedt
F. Tönnies
Z. Tong
F. Toschi
D. R. Tovey
J. Tranter
M. Trask
G. Trinchero
M. Tripathi
D. R. Tronstad
R. Trotta
C. D. Tunnell
P. Urquijo
A. Usón
M. Utoyama
A. C. Vaitkus
O. Valentino
K. Valerius
S. Vecchi
V. Velan
S. Vetter
L. de Viveiros
G. Volta
D. Vorkapic
A. Wang
J. J. Wang
Y. Wang
D. Waters
K. M. Weerman
C. Weinheimer
M. Weiss
D. Wenz
T. J. Whitis
K. Wild
M. Williams
M. Wilson
S. T. Wilson
C. Wittweg
J. Wolf
F. L. H. Wolfs
S. Woodford
D. Woodward
M. Worcester
C. J. Wright
V. H. S. Wu
S. Wüstling
M. Wurm
Q. Xia
Y. Xing
D. Xu
J. Xu
Y. Xu
Z. Xu
M. Yamashita
L. Yang
J. Ye
M. Yeh
B. Yu
G. Zavattini
W. Zha
M. Zhong
K. Zuber
Title: The XLZD Design Book: towards the next-generation liquid xenon observatory for dark matter and neutrino physics
Description:
Abstract
This report describes the experimental strategy and technologies for XLZD, the next-generation xenon observatory sensitive to dark matter and neutrino physics.
In the baseline design, the detector will have an active liquid xenon target of 60 tonnes, which could be increased to 80 tonnes if the market conditions for xenon are favorable.
It is based on the mature liquid xenon time projection chamber technology used in current-generation experiments, LZ and XENONnT.
The report discusses the baseline design and opportunities for further optimization of the individual detector components.
The experiment envisaged here has the capability to explore parameter space for Weakly Interacting Massive Particle (WIMP) dark matter down to the neutrino fog, with a 3
$$\sigma $$
σ
evidence potential for WIMP-nucleon cross sections as low as
$$3\times 10^{-49}\mathrm \,cm^2$$
3
×
10
-
49
c
m
2
(at 40 GeV/c
$$^2$$
2
WIMP mass).
The observatory will also have leading sensitivity to a wide range of alternative dark matter models.
It is projected to have a 3
$$\sigma $$
σ
observation potential of neutrinoless double beta decay of
$$^{136}$$
136
Xe at a half-life of up to
$$5.
7\times 10^{27}$$
5.
7
×
10
27
years.
Additionally, it is sensitive to astrophysical neutrinos from the sun and galactic supernovae.
Related Results
Neutrinoless double beta decay sensitivity of the XLZD rare event observatory
Neutrinoless double beta decay sensitivity of the XLZD rare event observatory
Abstract
The XLZD collaboration is developing a two-phase xenon time projection chamber with an active mass of 60–80 t capable of probing the remaining weakly intera...
Xenon doping of liquid argon in ProtoDUNE single phase
Xenon doping of liquid argon in ProtoDUNE single phase
Abstract
The Deep Underground Neutrino Experiment (DUNE) will be the next generation long-baseline neutrino experiment. The far detector is designed as a complex of ...
Physician and miracle worker. The cult of Saint Sampson the Xenodochos and his images in eastern Orthodox medieval painting
Physician and miracle worker. The cult of Saint Sampson the Xenodochos and his images in eastern Orthodox medieval painting
Saint Sampson, whose feast is celebrated on June 27, was depicted among holy
physicians. However, his images were not frequent. He was usually
accompanied with Saint Mokios (...
Molecular dynamics study of diffusion of xenon in water at different temperatures
Molecular dynamics study of diffusion of xenon in water at different temperatures
Molecular Dynamics simulation was performed using 2 xenon atoms as solute and 300 water molecules as solvent. We have studied the structural properties as well as transport propert...
Yifang Wang: high energy physics in China
Yifang Wang: high energy physics in China
Abstract
On 8 March 2012, Yifang Wang, co-spokesperson of the Daya Bay Experiment and Director of Institute of High Energy Physics, Chinese Academy of Sciences, anno...
Neutrinos from WIMP annihilations obtained using a full three-flavor Monte Carlo approach
Neutrinos from WIMP annihilations obtained using a full three-flavor Monte Carlo approach
Weakly interacting massive particles (WIMPs) are one of the main candidates for making up the dark matter in the Universe. If these particles make up the dark matter, then they can...
Faint and Extended Galaxies as Probes for Understanding the Nature of Dark Matter Particles
Faint and Extended Galaxies as Probes for Understanding the Nature of Dark Matter Particles
Dark matter remains one of the most enigmatic components of the universe, constituting approximately 27% of its total mass-energy content, yet its fundamental nature is still poorl...
History of solar neutrino observations
History of solar neutrino observations
Abstract
The first solar neutrino experiment, led by Raymond Davis Jr, showed a deficit of neutrinos relative to the solar model prediction, referred to as the “sola...

