The Jiangmen Underground Neutrino Observatory (JUNO) started physics data taking on 26 August 2025. JUNO consists of a 20-kton liquid scintillator central detector, surrounded by a 35 kton water pool serving as a Cherenkov veto, and almost 1000 m$^{2}$ of plastic scintillator veto on top. The detector is located in a shallow underground laboratory with an overburden of 1800 m.w.e. This paper presents the performance results of the detector, extensively studied during the commissioning of the water phase, the subsequent liquid scintillator filling phase, and the first physics runs. The liquid scintillator achieved an attenuation length of 20.6 m at 430 nm, while the high coverage PMT system and scintillator together yielded about 1785 photoelectrons per MeV of energy deposit at the detector centre, measured using the 2.223 MeV $\textit{γ}$ from neutron captures on hydrogen with an Am-C calibration source. The reconstructed energy resolution is 3.4% for two 0.511 MeV $\textit{γ}$ at the detector centre and 2.9% for the 0.93 MeV quenched $^{214}$Po alpha decays from natural radioactive sources. The energy non-linearity is calibrated to better than 1%. Intrinsic contaminations of $^{238}$U and $^{232}$Th in the liquid scintillator are below 10$^{-16}$ g/g, assuming secular equilibrium. The water Cherenkov detector achieves a muon detection efficiency better than 99.9% for muons traversing the liquid scintillator volume. During the initial science runs, the data acquisition duty cycle exceeded 97.8%, demonstrating the excellent stability and readiness of JUNO for high-precision neutrino physics.

Chile

Angel Abusleme

France

Thomas Adam

Germany

Kai Adamowicz

China

David Adey

Pakistan

Shakeel Ahmad

Rizwan Ahmed

Finland

Timo Ahola

Italy

Sebastiano Aiello

Fengpeng An

Guangpeng An

United Kingdom

Costas Andreopoulos

Giuseppe Andronico

João Pedro Athayde Marcondes de André

Russia

Nikolay Anfimov

Vito Antonelli

Tatiana Antoshkina

Thailand

Burin Asavapibhop

Didier Auguste

Margherita Buizza Avanzini

Slovakia

Andrej Babic

Jingzhi Bai

Weidong Bai

Nikita Balashov

Roberto Barbera

Andrea Barresi

Davide Basilico

Eric Baussan

Beatrice Bellantonio

Marco Bellato

JeanLuc Beney

Marco Beretta

Antonio Bergnoli

Enrico Bernieri

Nikita Bessonov

David Biaré

Daniel Bick

Lukas Bieger

Svetlana Biktemerova

Thilo Birkenfeld

David Blum

Simon Blyth

Sara Boarin

Manuel Boehles

Anastasia Bolshakova

Mathieu Bongrand

Aurélie Bonhomme

Clément Bordereau

Matteo Borghesi

Augusto Brigatti

Timothee Brugiere

Riccardo Brugnera

Riccardo Bruno

Jonas Buchholz

Antonio Budano

Max Buesken

Mario Buscemi

Severino Bussino

Jose Busto

Ilya Butorov

Marcel Büchner

Anatael Cabrera

Barbara Caccianiga

Boshuai Cai

Hao Cai

Xiao Cai

Yanke Cai

Yi-zhou Cai

Zhiyan Cai

Stéphane Callier

Steven Calvez

Antonio Cammi

Agustin Campeny

Dechang Cai

Chuanya Cao

Dewen Cao

Guofu Cao

Jun Cao

Yaoqi Cao

Rossella Caruso

Aurelio Caslini

Cédric Cerna

Vanessa Cerrone

Daniele Cesini

Chi Chan

Jinfan Chang

Yun Chang

Milo Charavet

Tim Charissé

Auttakit Chatrabhuti

Chao Chen

Guoming Chen

Haitao Chen

Haotian Chen

Jiahui Chen

Jian Chen

Jing Chen

Junyou Chen

Lihao Chen

Mali Chen

Mingming Chen

Initial performance results of the JUNO detector * We acknowledge financial and institutional supportfrom the Chinese Academy of Sciences, the National KeyR&D Program of China, the People's Government of Guangdong Province, and the Tsung–Dao Lee Institute of Shanghai Jiao Tong University in China.We appreciate the contributions from the Institut Na-tional de Physique Nucléaire et de Physique des Partic-ules (IN2P3) in France, the Istituto Nazionale di Fisica Nucleare (INFN) in Italy, the Fonds de la Recherche Sci-entifique (F.R.S.–FNRS) and the Institut Interuni-versitaire des Sciences Nucléaires (IISN) in Belgium, and the Conselho Nacional de Desenvolvimento Científico eTecnológico (CNPq) in Brazil.We also acknowledge the support of the AgenciaNacional de Investigación y Desarrollo (ANID) and the ANID–Millennium Science Initiative Program (ICN2019044) in Chile; the European Structural and In-vestment Funds, the Ministry of Education, Youth and Sports, and the Charles University Research Center inthe Czech Republic; the Deutsche Forschungsgemeinsch-aft (DFG), the Helmholtz Association, and the Cluster ofExcellence PRISMA+ in Germany; and the Joint Insti-tute for Nuclear Research (JINR) and Lomonosov Mo-scow State University in Russia.We further thank the Slovak Research and Develop-ment Agency in the Slovak Republic, the National Science and Technology Council (NSCT) and MOE, China, the Program Management Unit for Hu-man Resources & Institutional Development, Research and Innovation (PMU–B), Chulalongkorn University, and Suranaree University of Technology in Thailand, the Science and Technology Facilities Council (STFC) in the United Kingdom, and the University of California atIrvine and the National Science Foundation (NSF) in the United States

<p>The absence of definitive results for WIMP dark matter has sparked growing interest in alternative dark matter candidates, such as axions and axionlike particles (ALPs), which also provide insight into the strong CP problem. The Mitchell Institute Neutrino Experiment at Reactor (MINER), conducted at the Nuclear Science Center of Texas A&M University, investigated ALPs near a 1 MW h TRIGA nuclear reactor core, positioned approximately 4 m away. This experiment employed cryogenic sapphire detectors with a low detection threshold (<math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mo>≈</mo><mn>100</mn><mtext> </mtext><mtext> </mtext><mi>eV</mi></math>), equipped with a transition edge sensor capable of detecting athermal phonons. Due to the low-background environment, we were able to exclude ALPs with axion-photon coupling and axion-electron coupling as small as <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><msub><mi>g</mi><mrow><mi>a</mi><mi>γ</mi><mi>γ</mi></mrow></msub><mo>=</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>5</mn></mrow></msup></math> and <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><msub><mi>g</mi><mrow><mi>a</mi><mi>e</mi><mi>e</mi></mrow></msub><mo>=</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>7</mn></mrow></msup></math>, respectively. Energy depositions below 3 keV were not considered and remain blinded for our coherent elastic neutrino-nucleus scattering analysis. This is the first result demonstrating the MINER experiment’s potential to probe low-mass ALPs, enabled by its low-threshold detector and proximity to a reactor.</p>

United States

M. Mirzakhani

W. Baker

India

M. Chaudhuri

J.B. Dent

R. Dey

B. Dutta

Canada

V. Iyer

A. Jastram

V.K.S. Kashyap

A. Kubik

K. Lang

R. Mahapatra

S. Maludze

N. Mirabolfathi

B. Mohanty

D. Mondal

H. Neog

Australia

J.L. Newstead

M. Platt

S. Sahoo

J. Sander

L.E. Strigari

J. Walker

MINER reactor based search for axionlike particles using sapphire (<math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><msub><mtext>Al</mtext><mn>2</mn></msub><msub><mi mathvariant="normal">O</mi><mn>3</mn></msub></math>) detectors

The structure of the proton-unbound nucleus <math altimg='si1.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Al</mi></mrow><mprescripts /><none /><mrow><mn>21</mn></mrow></mmultiscripts></math> has been studied via proton transfer from a <math altimg='si2.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Be</mi></mrow><mprescripts /><none /><mrow><mn>9</mn></mrow></mmultiscripts></math> target to a <math altimg='si3.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Mg</mi></mrow><mprescripts /><none /><mrow><mn>20</mn></mrow></mmultiscripts></math> beam at <math altimg='si4.svg'><mi>E</mi><mo stretchy='false'>/</mo><mi>A</mi></math> = 103 MeV. Three resonant states in <math altimg='si1.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Al</mi></mrow><mprescripts /><none /><mrow><mn>21</mn></mrow></mmultiscripts></math> are identified by the invariant-mass reconstruction of <math altimg='si5.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Ne</mi></mrow><mprescripts /><none /><mrow><mn>18</mn></mrow></mmultiscripts></math> + 3 <italic>p</italic> events. The decay-energy spectra for the two subsystems of <math altimg='si1.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Al</mi></mrow><mprescripts /><none /><mrow><mn>21</mn></mrow></mmultiscripts></math>, i.e. <math altimg='si5.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Ne</mi></mrow><mprescripts /><none /><mrow><mn>18</mn></mrow></mmultiscripts></math> + 1 <italic>p</italic> and <math altimg='si5.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Ne</mi></mrow><mprescripts /><none /><mrow><mn>18</mn></mrow></mmultiscripts></math> + 2 <italic>p</italic>, indicate that the observed resonant state with the lowest energy has decay branches consisting of three sequential steps of one-proton decay. Based on the <italic>ab initio</italic> and the distorted-wave Born approximation (DWBA) calculations, this resonant state at <math altimg='si7.svg'><msup><mrow><mi>E</mi></mrow><mrow><mo>&#8270;</mo></mrow></msup></math> = 6.09(11) MeV likely has a spin-parity of <math altimg='si8.svg'><mo stretchy='false'>(</mo><mn>1</mn><mo stretchy='false'>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo linebreak='badbreak' linebreakstyle='after'>+</mo></mrow></msup></math>- <math altimg='si9.svg'><mn>7</mn><mo stretchy='false'>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo linebreak='badbreak' linebreakstyle='after'>+</mo></mrow></msup><mo stretchy='false'>)</mo></math>. Meanwhile, the possibility that the observed resonant peak represents an admixture of several states cannot be ruled out. The good isospin-symmetry of the low-lying states with <math altimg='si10.svg'><msub><mrow><mi>d</mi></mrow><mrow><mn>5</mn><mo stretchy='false'>/</mo><mn>2</mn></mrow></msub></math>, <math altimg='si11.svg'><msub><mrow><mi>d</mi></mrow><mrow><mn>3</mn><mo stretchy='false'>/</mo><mn>2</mn></mrow></msub></math> configurations in the <math altimg='si1.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Al</mi></mrow><mprescripts /><none /><mrow><mn>21</mn></mrow></mmultiscripts></math>- <math altimg='si12.svg'><mmultiscripts><mrow><mi mathvariant='normal'>O</mi></mrow><mprescripts /><none /><mrow><mn>21</mn></mrow></mmultiscripts></math> pair and the <italic>ab initio</italic> calculations indicate weak configuration mixing between the <italic>s</italic>- and <italic>d</italic>-orbital components. The systematics of experimental energy differences between the <math altimg='si13.svg'><mn>5</mn><mo stretchy='false'>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo linebreak='badbreak' linebreakstyle='after'>+</mo></mrow></msup></math> ground state and lowest-lying <math altimg='si14.svg'><mn>3</mn><mo stretchy='false'>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo linebreak='badbreak' linebreakstyle='after'>+</mo></mrow></msup></math> excited state for isotopes (isotones) of <math altimg='si15.svg'><mi>Z</mi><mo stretchy='false'>(</mo><mi>N</mi><mo stretchy='false'>)</mo></math> = 13 suggest a likely semimagic nature of <math altimg='si1.svg'><mmultiscripts><mrow><mi mathvariant='normal'>Al</mi></mrow><mprescripts /><none /><mrow><mn>21</mn></mrow></mmultiscripts></math>.

L. Ni

Y. Jin

Z.H. Li

K.W. Brown

H. Hua

C.Y. Niu

J.G. Li

A.K. Anthony

J. Barney

R.J. Charity

D. Dell'Aquila

J.M. Elson

J. Estee

G. Jhang

W.G. Lynch

N. Michel

L.G. Sobotka

S. Sweany

F.C.E. Teh

A. Thomas

C.Y. Tsang

M.B. Tsang

S.M. Wang

H.Y. Wu

C.X. Yuan

K. Zhu

Observation of three-proton-decaying resonant states in <sup>21</sup>Al

Reported here are transverse single-spin asymmetries (<math><msub><mi>A</mi><mi>N</mi></msub></math>) in the production of charged hadrons as a function of transverse momentum (<math><msub><mi>p</mi><mi>T</mi></msub></math>) and Feynman-<math><mi>x</mi></math> (<math><msub><mi>x</mi><mi>F</mi></msub></math>) in polarized <math><msup><mi>p</mi><mo>↑</mo></msup><mo>+</mo><mi>p</mi></math>, <math><mrow><msup><mrow><mi>p</mi></mrow><mrow><mo>↑</mo></mrow></msup><mo>+</mo><mi>Al</mi></mrow></math>, and <math><mrow><msup><mrow><mi>p</mi></mrow><mrow><mo>↑</mo></mrow></msup><mo>+</mo><mi>Au</mi></mrow></math> collisions at <math><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>200</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math>. The measurements have been performed at forward and backward rapidity (<math><mn>1.4</mn><mo>&lt;</mo><mo>|</mo><mi>η</mi><mo>|</mo><mo>&lt;</mo><mn>2.4</mn></math>) over the range of <math><mn>1.5</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi><mo>/</mo><mi>c</mi><mo>&lt;</mo><msub><mi>p</mi><mi>T</mi></msub><mo>&lt;</mo><mn>7.0</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi><mo>/</mo><mi>c</mi></math> and <math><mn>0.04</mn><mo>&lt;</mo><mo>|</mo><msub><mi>x</mi><mi>F</mi></msub><mo>|</mo><mo>&lt;</mo><mn>0.2</mn></math>. A nonzero asymmetry is observed for positively charged hadrons at forward rapidity (<math><msub><mi>x</mi><mi>F</mi></msub><mo>&gt;</mo><mn>0</mn></math>) in <math><msup><mi>p</mi><mo>↑</mo></msup><mo>+</mo><mi>p</mi></math> collisions, whereas the <math><mrow><msup><mrow><mi>p</mi></mrow><mrow><mo>↑</mo></mrow></msup><mo>+</mo><mi>Al</mi></mrow></math> and <math><mrow><msup><mrow><mi>p</mi></mrow><mrow><mo>↑</mo></mrow></msup><mo>+</mo><mi>Au</mi></mrow></math> results show smaller asymmetries. This finding provides new opportunities to investigate the origin of transverse single-spin asymmetries and a tool to study nuclear effects in <math><mi>p</mi><mo>+</mo><mi>A</mi></math> collisions.

Hungary

N. J. Abdulameer

U. Acharya

C. Aidala

Japan

Y. Akiba

M. Alfred

V. Andrieux

N. Apadula

H. Asano

B. Azmoun

V. Babintsev

N. S. Bandara

K. N. Barish

S. Bathe

A. Bazilevsky

M. Beaumier

R. Belmont

A. Berdnikov

Y. Berdnikov

L. Bichon

B. Blankenship

D. S. Blau

J. S. Bok

V. Borisov

M. L. Brooks

J. Bryslawskyj

V. Bumazhnov

S. Campbell

V. Canoa Roman

Transverse single-spin asymmetry of charged hadrons at forward and backward rapidity in polarized <math><mi>p</mi><mo>+</mo><mi>p</mi></math>, <math><mrow><mi>p</mi><mo>+</mo><mi>Al</mi></mrow></math>, and <math><mrow><mi>p</mi><mo>+</mo><mi>Au</mi></mrow></math> collisions at <math><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>200</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math>