Adan Ruben Rodriguez Dominguez

Universidad Autónoma de San Luis Potosí

H-index: 77

Latin America-Mexico

About Adan Ruben Rodriguez Dominguez

Adan Ruben Rodriguez Dominguez, With an exceptional h-index of 77 and a recent h-index of 56 (since 2020), a distinguished researcher at Universidad Autónoma de San Luis Potosí, specializes in the field of theoretical physics, condensed matter, mathematical physics, electronic and magnetic structure of small TM clusters, their stabi.

His recent articles reflect a diverse array of research interests and contributions to the field:

Structures of Ni-doped Bn (n= 1-13) clusters: A Computational Study

Helium identification with LHCb

Evaluation of the implementation of a community health worker-led COVID-19 contact tracing intervention in Chiapas, Mexico, from March 2020 to December 2021

Observation of and decays

Performance of a modular ton-scale pixel-readout liquid argon Time Projection Chamber

The DUNE Far Detector Vertical Drift Technology, Technical Design Report

Measurement of the CKM angle γ in the B 0 → D K ∗ 0 channel using self-conjugate D → K S 0 h + h - decays

Doping liquid argon with xenon in ProtoDUNE Single-Phase: effects on scintillation light

Adan Ruben Rodriguez Dominguez Information

University	Universidad Autónoma de San Luis Potosí
Position	Instituto de Física-
Citations(all)	19734
Citations(since 2020)	12609
Cited By	5559
hIndex(all)	77
hIndex(since 2020)	56
i10Index(all)	217
i10Index(since 2020)	185
Email	Access Email
University Profile Page	Universidad Autónoma de San Luis Potosí

Adan Ruben Rodriguez Dominguez Skills & Research Interests

theoretical physics

condensed matter

mathematical physics

electronic and magnetic structure of small TM clusters

their stabi

Authors

A Abed Abud,B Abi,R Acciarri,MA Acero,MR Adames,G Adamov,M Adamowski,D Adams,M Adinolfi,C Adriano,A Aduszkiewicz,J Aguilar,Z Ahmad,J Ahmed,B Aimard,F Akbar,K Allison,S Alonso Monsalve,M Alrashed,C Alt,A Alton,R Alvarez,P Amedo,J Anderson,DA Andrade,C Andreopoulos,M Andreotti,MP Andrews,F Andrianala,S Andringa,N Anfimov,WL Anicézio Campanelli,A Ankowski,M Antoniassi,M Antonova,A Antoshkin,S Antusch,A Aranda-Fernandez,L Arellano,LO Arnold,MA Arroyave,J Asaadi,L Asquith,A Aurisano,V Aushev,D Autiero,M Ayala-Torres,F Azfar,A Back,H Back,JJ Back,I Bagaturia,L Bagby,N Balashov,S Balasubramanian,P Baldi,B Baller,B Bambah,F Barao,G Barenboim,GJ Barker,W Barkhouse,C Barnes,G Barr,J Barranco Monarca,A Barros,N Barros,JL Barrow,A Basharina-Freshville,A Bashyal,V Basque,C Batchelor,JBR Battat,F Battisti,F Bay,MCQ Bazetto,JLL Bazo Alba,JF Beacom,E Bechetoille,B Behera,E Belchior,L Bellantoni,G Bellettini,V Bellini,O Beltramello,N Benekos,C Benitez Montiel,D Benjamin,F Bento Neves,J Berger,S Berkman,P Bernardini,RM Berner,A Bersani,S Bertolucci,M Betancourt,A Betancur Rodríguez,A Bevan,Y Bezawada,AT Bezerra,TJ Bezerra,J Bhambure,A Bhardwaj,V Bhatnagar,M Bhattacharjee,D Bhattarai,S Bhuller,B Bhuyan,S Biagi,J Bian,M Biassoni,K Biery,B Bilki,M Bishai,V Bisignani,A Bitadze,A Blake,FD Blaszczyk,GC Blazey,D Blend,E Blucher,J Boissevain,S Bolognesi,T Bolton,L Bomben,M Bonesini,C Bonilla-Diaz,F Bonini,A Booth,F Boran,S Bordoni,A Borkum,N Bostan,P Bour,D Boyden,J Bracinik,D Braga,D Brailsford,A Branca,A Brandt,J Bremer,C Brew,SJ Brice,C Brizzolari,C Bromberg,J Brooke,A Bross,G Brunetti,M Brunetti,N Buchanan

Journal

Physical Review D

Published Date

2023/5/30

First observation of a doubly charged tetraquark and its neutral partner

Authors

R Aaij,ASW Abdelmotteleb,C Abellan Beteta,F Abudinén,T Ackernley,B Adeva,M Adinolfi,P Adlarson,H Afsharnia,C Agapopoulou,CA Aidala,S Aiola,Z Ajaltouni,S Akar,K Akiba,J Albrecht,F Alessio,M Alexander,A Alfonso Albero,Z Aliouche,P Alvarez Cartelle,R Amalric,S Amato,JL Amey,Y Amhis,L An,L Anderlini,M Andersson,A Andreianov,M Andreotti,D Andreou,D Ao,F Archilli,A Artamonov,M Artuso,E Aslanides,M Atzeni,B Audurier,S Bachmann,Marie Bachmayer,JJ Back,A Bailly-Reyre,P Baladron Rodriguez,V Balagura,W Baldini,J Baptista de Souza Leite,M Barbetti,RJ Barlow,S Barsuk,W Barter,M Bartolini,F Baryshnikov,JM Basels,G Bassi,B Batsukh,A Battig,A Bay,A Beck,M Becker,F Bedeschi,IB Bediaga,A Beiter,V Belavin,S Belin,V Bellee,K Belous,I Belov,I Belyaev,G Benane,G Bencivenni,E Ben-Haim,A Berezhnoy,R Bernet,S Bernet Andres,D Berninghoff,HC Bernstein,C Bertella,A Bertolin,C Betancourt,F Betti,Ia Bezshyiko,S Bhasin,J Bhom,L Bian,MS Bieker,NV Biesuz,S Bifani,P Billoir,A Biolchini,M Birch,FCR Bishop,A Bitadze,A Bizzeti,MP Blago,T Blake,F Blanc,JE Blank,S Blusk,D Bobulska,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,CS Bolognani,R Bolzonella,N Bondar,F Borgato,S Borghi,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,J Brodzicka,A Brossa Gonzalo,J Brown,D Brundu,A Buonaura,L Buonincontri,AT Burke,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,S Cali,R Calladine,M Calvi,M Calvo Gomez,P Campana,DH Campora Perez,AF Campoverde Quezada,S Capelli,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,P Carniti,L Carus,A Casais Vidal

Journal

Physical review letters

Published Date

2023/7/27

A combined amplitude analysis is performed for the decays B 0→ DD 0 s+ π− and B+→ D− D s+ π+, which are related by isospin symmetry. The analysis is based on data collected by the LHCb detector in proton-proton collisions at center-of-mass energies of 7, 8, and 13 TeV. The full data sample corresponds to an integrated luminosity of 9 fb− 1. Two new resonant states with masses of 2.908±0.011±0.020 GeV and widths of 0.136±0.023±0.013 GeV are observed, which decay to D s+ π+ and D s+ π− respectively. The former state indicates the first observation of a doubly charged open-charm tetraquark state with minimal quark content [c s u d], and the latter state is a neutral tetraquark composed of [c s u d] quarks. Both states are found to have spin-parity of 0+, and their resonant parameters are consistent with each other, which suggests that they belong to an isospin triplet.

Search for in decays

Authors

Roel Aaij,Ahmed Sameh Wagih Abdelmotteleb,C Abellan Beteta,F Abudinén,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,P Adlarson,Hossein Afsharnia,Christina Agapopoulou,Christine Angela Aidala,Ziad Ajaltouni,Simon Akar,Kazuyoshi Akiba,Pietro Albicocco,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,P Alvarez Cartelle,Renaud Amalric,Sandra Amato,Jake Lewis Amey,Yasmine Amhis,Liupan An,Lucio Anderlini,Martin Andersson,Aleksei Andreianov,Mirco Andreotti,Dimitra Andreou,Dong Ao,Flavio Archilli,Alexander Artamonov,Marina Artuso,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Irene Bachiller Perea,Sebastian Bachmann,Marie Bachmayer,JJ Back,Aurelien Bailly-Reyre,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista de Souza Leite,Matteo Barbetti,Ivanildo Rui Barbosa,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,Giovanni Bassi,B Batsukh,A Battig,A Bay,A Beck,M Becker,F Bedeschi,IB Bediaga,A Beiter,S Belin,V Bellee,K Belous,I Belov,I Belyaev,G Benane,G Bencivenni,E Ben-Haim,A Berezhnoy,R Bernet,S Bernet Andres,D Berninghoff,HC Bernstein,C Bertella,A Bertolin,C Betancourt,F Betti,Ia Bezshyiko,J Bhom,L Bian,MS Bieker,NV Biesuz,P Billoir,A Biolchini,M Birch,FCR Bishop,A Bitadze,A Bizzeti,MP Blago,T Blake,F Blanc,JE Blank,S Blusk,D Bobulska,VB Bocharnikov,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,CS Bolognani,R Bolzonella,N Bondar,F Borgato,S Borghi,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,N Breer,J Brodzicka,A Brossa Gonzalo,J Brown,D Brundu,A Buonaura,L Buonincontri,AT Burke,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,S Cali,M Calvi,M Calvo Gomez,P Campana,DH Perez,AF Quezada,S Capelli,L Capriotti,A Carbone,R Cardinale,A Cardini,P Carniti,L Carus,A Casais Vidal,R Caspary

Journal

The European Physical Journal C

Published Date

2023/7

The very rare decay is searched for by analysing decays. The analysis uses a sample of beauty mesons produced in proton–proton collisions collected with the LHCb detector between 2011 and 2018, corresponding to an integrated luminosity of 9$\text {\, fb}^{-1}$. The signal signature corresponds to simultaneous peaks in the and invariant masses. No evidence for an excess of events over background is observed and an upper limit is set on the branching fraction of the decay at at confidence level. This is the first limit on the branching fraction of decays and the most stringent limit on decays to leptonic final states. The analysis is the first search for a rare charm-meson decay exploiting production via beauty decays.

Authors

A Abed Abud,A Friedland,M Smy,P Hamacher-Baumann,Z Djurcic,E Goudzovski,D Totani,E Mazzucato,C Densham,B Russell,E Calvo,P Green,A Penzo,D Shooltz,L Singh,J Crnkovic,P Vahle,CS Mishra,J Smolik,MA Acero,H Meyer,DH Koh,D Moretti,G Cerati,M Adamowski,J Zennamo,AS Dyshkant,R Gran,J Stewart,D Marfatia,T Patzak,K Yonehara,JBR Battat,D Kwak,P Dunne,C Brizzolari,K Cho,G Lehmann Miotto,H Newton,C Mariani,S Vallecorsa,S Prakash,IK Furic,A Gabrielli,A Ankowski,PC De Holanda,A Barros,C Benitez Montiel,S Sacerdoti,E Smith,P Keener,X Wang,V Pec,O Palamara,L Strigari,J Brooke,P Rosier,P Lasorak,CA Moura,MA Delgado,E Guerard,W Ketchum,C Petta,G Miller,Z Hulcher,DA Dwyer,LW Koerner,J Maalmi,B Szczerbinska,V Tishchenko,A Thea,JRT de Mello Neto,T Gamble,J Matthews,K Moffat,F Muheim,M Chen,L Di Giulio,F Battisti,R Cross,T Cai,GC Blazey,P Novella,B Howard,S Prince,V Ayala Lara,N Talukdar,A Laundrie,L Suter,MHLS Wang,A Robert,FDM Blaszczyk,J Kvasnicka,X Ji,Y Onel,J Nesbit,H Duyang,A De Roeck,J Franc,A Gago,D Last,K Nishimura,JWF Valle,V Papadimitriou,Y Suvorov,C Thorn,S Uzunyan,S Manly,F Matichard,D Carber,L Paulucci,T Junk,S Copello,F Di Capua,R Mohanta,G Barr,P Gauzzi,B Lunday,S Dolan,SD Reitzner,LS Fajardo,F Psihas,J Heise,S Antusch,P Clarke,S Miryala,H Mendez,L Rochester,K Fahey,C Mossey,L Kolupaeva,N Samios,N Gallice,E Pennacchio,X Qian,E Parozzi,D Torbunov,S Rosauro-Alcaraz,C Wret,M Fernandez Morales,O Goodwin,M Worcester,N McConkey,S Gent,A Gallego-Ros,MP Decowski,M Kirby,ED Zimmerman,A Surdo,L Da Silva Peres

Published Date

2022/3/11

The Deep Underground Neutrino Experiment (DUNE) is a next-generation international particle physics experiment seeking to answer fundamental questions about the neutrino. It will use a new high-intensity neutrino beam that will be generated at the US Department of Energy’s Fermi National Accelerator Laboratory (Fermilab). The experiment will consist of a far detector (FD) located approximately 1.5 km underground at the Sanford Underground Research Facility (SURF) in Lead, South Dakota, at a distance of 1285 km from Fermilab, and a near detector (ND) that will be located on the Fermilab site in Illinois. The FD will consist of a large, modular liquid-argon time projection chamber (LArTPC) with a fiducial mass of roughly 40 kt (total mass of 68 kton).The reference ND will be located approximately 574 m from DUNE’s neutrino target, which is the starting point for the Long-Baseline Neutrino Facility (LBNF) beam. The conceptual design for the DUNE ND is described in detail in Ref.[2]. The reference ND design consists of several different components shown in Fig. 1: an upstream modular non-magnetized LArTPC (ND-LAr), a magnetized tracker containing a pressurized gaseous-argon time projection chamber (ND-GAr), and a large, magnetized tracking spectrometer (SAND). SAND will remain fixed on the beam axis, while ND-LAr and ND-GAr will move transverse to the beam to collect data at various off-axis positions, providing different neutrino energy spectra by the PRISM concept [3]. In a conventional neutrino beam, the peak energy of the neutrino spectrum decreases and the size of the high energy tail is reduced when the detection …

Structural and electronic properties for Be-doped Pt n (n= 1–12) clusters obtained by DFT calculations

Authors

Peter L Rodríguez-Kessler,Adán R Rodríguez-Domínguez,Pedro Alonso-Dávila,Pedro Navarro-Santos,Alvaro Muñoz-Castro

Journal

Physical Chemistry Chemical Physics

Published Date

2022

In this work, we have performed a computational study on the structure and electronic properties for Be-doped Ptn (n = 1–12) clusters in the framework of density functional theory (DFT). The most stable structures of the clusters are obtained by a structure search procedure based in simulated annealing. The results show that the PtnBe clusters adopt compact structure motifs with Be situated at the edge sites while only in Pt11Be the Be atom occupies the center site. The energetic parameters showed that Pt5Be, Pt7Be and Pt10Be are the most stable ones. The PtnBe clusters with (n = 5–7) have similar vertical ionization potential (vIP) and vertical electron affinity (vEA) parameters compared to the unary Pt clusters, while Pt9Be and Pt11Be have the higher vEA values. In particular, the d-band center is slightly higher for the doped clusters, suggesting an enhanced reactivity. The σ-holes are found more remarkable for …

Measurement of the Nuclear Modification Factor and Prompt Charged Particle Production in -Pb and Collisions at

Authors

Roel Aaij,C Abellan Beteta,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Jake Lewis Amey,Yasmine Amhis,Liupan An,Lucio Anderlini,Aleksei Andreianov,Mirco Andreotti,F Archilli,A Artamonov,M Artuso,K Arzymatov,E Aslanides,M Atzeni,B Audurier,S Bachmann,M Bachmayer,JJ Back,P Baladron Rodriguez,V Balagura,W Baldini,J Baptista Leite,RJ Barlow,S Barsuk,W Barter,M Bartolini,F Baryshnikov,JM Basels,G Bassi,B Batsukh,A Battig,A Bay,M Becker,F Bedeschi,I Bediaga,A Beiter,V Belavin,S Belin,V Bellee,K Belous,I Belov,I Belyaev,G Bencivenni,E Ben-Haim,A Berezhnoy,R Bernet,D Berninghoff,HC Bernstein,C Bertella,A Bertolin,C Betancourt,F Betti,Ia Bezshyiko,S Bhasin,J Bhom,L Bian,MS Bieker,S Bifani,P Billoir,M Birch,FCR Bishop,A Bitadze,A Bizzeti,M Bjørn,MP Blago,T Blake,F Blanc,S Blusk,D Bobulska,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,A Bondar,N Bondar,S Borghi,M Borisyak,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,M Brodski,J Brodzicka,A Brossa Gonzalo,D Brundu,A Buonaura,AT Burke,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,L Calero Diaz,S Cali,R Calladine,M Calvi,M Calvo Gomez,P Camargo Magalhaes,P Campana,AF Campoverde Quezada,S Capelli,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,I Carli,P Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,G Casse,M Cattaneo,G Cavallero,S Celani,J Cerasoli,AJ Chadwick,MG Chapman,M Charles,Ph Charpentier,G Chatzikonstantinidis,CA Chavez Barajas,M Chefdeville,C Chen

Journal

Physical review letters

Published Date

2022/4/7

The production of prompt charged particles in proton-lead collisions and in proton-proton collisions at the nucleon-nucleon center-of-mass energy s N N= 5 TeV is studied at LHCb as a function of pseudorapidity (η) and transverse momentum (p T) with respect to the proton beam direction. The nuclear modification factor for charged particles is determined as a function of η between− 4.8< η<− 2.5 (backward region) and 2.0< η< 4.8 (forward region), and p T between 0.2< p T< 8.0 GeV/c. The results show a suppression of charged particle production in proton-lead collisions relative to proton-proton collisions in the forward region and an enhancement in the backward region for p T larger than 1.5 GeV/c. This measurement constrains nuclear PDFs and saturation models at previously unexplored values of the parton momentum fraction down to 10− 6.

First Measurement of the Angular Coefficients in the Forward Region of Collisions at

Authors

R Aaij,ASW Abdelmotteleb,C Abellan Beteta,F Abudinén,T Ackernley,B Adeva,M Adinolfi,H Afsharnia,C Agapopoulou,CA Aidala,S Aiola,Z Ajaltouni,S Akar,J Albrecht,F Alessio,M Alexander,A Alfonso Albero,Z Aliouche,G Alkhazov,P Alvarez Cartelle,S Amato,JL Amey,Y Amhis,L An,L Anderlini,M Andersson,A Andreianov,M Andreotti,D Andreou,D Ao,F Archilli,A Artamonov,M Artuso,K Arzymatov,E Aslanides,M Atzeni,B Audurier,S Bachmann,M Bachmayer,JJ Back,P Baladron Rodriguez,V Balagura,W Baldini,J Baptista de Souza Leite,M Barbetti,RJ Barlow,S Barsuk,W Barter,M Bartolini,F Baryshnikov,JM Basels,G Bassi,B Batsukh,A Battig,A Bay,A Beck,M Becker,F Bedeschi,I Bediaga,A Beiter,V Belavin,S Belin,V Bellee,K Belous,I Belov,I Belyaev,G Bencivenni,E Ben-Haim,A Berezhnoy,R Bernet,D Berninghoff,HC Bernstein,C Bertella,A Bertolin,C Betancourt,F Betti,Ia Bezshyiko,S Bhasin,J Bhom,L Bian,MS Bieker,NV Biesuz,S Bifani,P Billoir,A Biolchini,M Birch,FCR Bishop,A Bitadze,A Bizzeti,M Bjørn,MP Blago,T Blake,F Blanc,S Blusk,D Bobulska,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,A Bondar,N Bondar,S Borghi,M Borisyak,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,J Brodzicka,A Brossa Gonzalo,D Brundu,A Buonaura,L Buonincontri,AT Burke,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,S Cali,R Calladine,M Calvi,M Calvo Gomez,P Camargo Magalhaes,P Campana,DH Campora Perez,AF Campoverde Quezada,S Capelli,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,I Carli,P Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,R Caspary,G Casse,M Cattaneo

Journal

Physical Review Letters

Published Date

2022/8/24

The first study of the angular distribution of μ+ μ− pairs produced in the forward rapidity region via the Drell-Yan reaction p p→ γ*/Z+ X→ ℓ+ ℓ−+ X is presented, using data collected with the LHCb detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.1 fb− 1. The coefficients of the five leading terms in the angular distribution are determined as a function of the dimuon transverse momentum and rapidity. The results are compared to various theoretical predictions of the Z-boson production mechanism and can also be used to probe transverse-momentum-dependent parton distributions within the proton.

A comparison of CPU and GPU implementations for the LHCb Experiment Run 3 Trigger

Authors

R Aaij,Marta Adinolfi,Salvatore Aiola,S Akar,J Albrecht,M Alexander,S Amato,Yasmine Amhis,F Archilli,M Bala,G Bassi,L Bian,MP Blago,T Boettcher,A Boldyrev,S Borghi,A Brea Rodriguez,Lukas Calefice,M Calvo Gomez,DH Cámpora Pérez,A Cardini,Marco Cattaneo,V Chobanova,G Ciezarek,X Cid Vidal,JL Cobbledick,JAB Coelho,Tommaso Colombo,A Contu,Benjamin Couturier,Daniel C Craik,R Currie,P d’Argent,Michel De Cian,Denis Derkach,F Dordei,Marco Dorigo,L Dufour,Paolo Durante,A Dziurda,A Dzyuba,S Easo,S Esen,P Fernandez Declara,S Filippov,Conor Fitzpatrick,M Frank,Paolo Gandini,Vladimir V Gligorov,Elisabet Golobardes,G Graziani,L Grillo,PA Günther,S Hansmann-Menzemer,Arthur M Hennequin,Louis Henry,D Hill,SE Hollitt,J Hu,W Hulsbergen,RJ Hunter,Mikhail Hushchyn,Brij Kishor Jashal,Christopher Robert Jones,S Klaver,Konrad Klimaszewski,R Kopecna,Wojciech Krzemien,Marcin Kucharczyk,R Lane,F Lazzari,R Le Gac,P Li,JH Lopes,M Lucio Martinez,A Lupato,Oliver Lupton,X Lyu,F Machefert,O Madejczyk,S Malde,JF Marchand,S Mariani,C Marin Benito,D Martinez Santos,F Martinez Vidal,R Matev,Michal Mazurek,B Mitreska,DS Mitzel,MJ Morello,H Mu,P Muzzetto,P Naik,M Needham,N Neri,Niko Neufeld,NS Nolte,Daniel O’Hanlon,A Oyanguren,M Pepe Altarelli,S Petrucci,Marco Petruzzo,L Pica,Flavio Pisani,A Piucci,Francesco Polci,A Poluektov,E Polycarpo,C Prouve,Giovanni Punzi,Renato Quagliani,RI Rabadan Trejo,M Ramos Pernas,MS Rangel,Fedor Ratnikov,G Raven,F Reiss,V Renaudin,P Robbe,Artem Ryzhikov,Marco Santimaria,M Saur,M Schiller,Rainer Schwemmer,Barbara Sciascia,A Solomin,F Suljik,N Skidmore,Michael D Sokoloff,P Spradlin,M Stahl,S Stahl,H Stevens,L Sun,A Szabelski,Tomasz Szumlak,M Szymanski,DY Tou,G Tuci,A Usachov,N Valls Canudas,R Vazquez Gomez,Stefania Vecchi,Mika Vesterinen,Xavier Vilasis-Cardona,D Vom Bruch,Z Wang,Tomasz Wojton,Mark Whitehead

Journal

Computing and Software for Big Science

Published Date

2022/12

The Large Hadron Collider beauty (LHCb) experiment at CERN is undergoing an upgrade in preparation for the Run 3 data collection period at the Large Hadron Collider (LHC). As part of this upgrade, the trigger is moving to a full software implementation operating at the LHC bunch crossing rate. We present an evaluation of a CPU-based and a GPU-based implementation of the first stage of the high-level trigger. After a detailed comparison, both options are found to be viable. This document summarizes the performance and implementation details of these options, the outcome of which has led to the choice of the GPU-based implementation as the baseline.

Measurement of the charm mixing parameter using two-body meson decays

Authors

Roel Aaij,Ahmed Sameh Wagih Abdelmotteleb,C Abellan Beteta,F Abudinen,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christina Agapopoulou,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Jake Lewis Amey,Yasmine Amhis,Liupan An,Lucio Anderlini,Martin Andersson,Aleksei Andreianov,Mirco Andreotti,Dong Ao,Flavio Archilli,Alexander Artamonov,Marina Artuso,Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,JJ Back,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista de Souza Leite,Matteo Barbetti,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,Giovanni Bassi,Baasansuren Batsukh,Alexander Battig,Aurelio Bay,Anja Beck,Maik Becker,Franco Bedeschi,Ignacio Bediaga,Andrew Beiter,Vladislav Belavin,Samuel Belin,Violaine Bellee,Konstantin Belous,Ilia Belov,Ivan Belyaev,Giovanni Bencivenni,Eli Ben-Haim,Alexander Berezhnoy,Roland Bernet,Daniel Berninghoff,Harris Conan Bernstein,Claudia Bertella,Alessandro Bertolin,Christopher Betancourt,Federico Betti,Ia Bezshyiko,S Bhasin,J Bhom,L Bian,MS Bieker,NV Biesuz,S Bifani,P Billoir,A Biolchini,M Birch,FCR Bishop,A Bitadze,A Bizzeti,M Bjørn,MP Blago,T Blake,F Blanc,S Blusk,D Bobulska,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,A Bondar,N Bondar,S Borghi,M Borisyak,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,J Brodzicka,A Brossa Gonzalo,D Brundu,A Buonaura,L Buonincontri,AT Burke,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,S Cali,R Calladine,M Calvi,M Calvo Gomez,P Camargo Magalhaes,P Campana,AF Campoverde Quezada,S Capelli,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,I Carli,P Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,R Caspary,G Casse,M Cattaneo,G Cavallero,S Celani

Journal

Physical Review D

Published Date

2022/5/25

A measurement of the ratios of the effective decay widths of D 0→ π− π+ and D 0→ K− K+ decays over that of D 0→ K− π+ decays is performed with the LHCb experiment using proton–proton collisions at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 6 fb− 1. These observables give access to the charm mixing parameters y C P π π− y C P K π and y C P K K− y C P K π, and are measured as y C P π π− y C P K π=(6.57±0.53±0.16)× 10− 3, y C P K K− y C P K π=(7.08±0.30±0.14)× 10− 3, where the first uncertainties are statistical and the second systematic. The combination of the two measurements is y C P− y C P K π=(6.96±0.26±0.13)× 10− 3, which is four times more precise than the previous world average.

Observation of the doubly charmed baryon decay

Authors

Roel Aaij,Ahmed Sameh Wagih Abdelmotteleb,Carlos Abellán Beteta,F Abudinen,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christina Agapopoulou,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Jake Lewis Amey,Yasmine Amhis,Liupan An,Lucio Anderlini,Martin Andersson,Aleksei Andreianov,Mirco Andreotti,Dong Ao,Flavio Archilli,Alexander Artamonov,Marina Artuso,Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,JJ Back,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista de Souza Leite,Matteo Barbetti,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,Giovanni Bassi,Baasansuren Batsukh,Alexander Battig,Aurelio Bay,Anja Beck,Maik Becker,Franco Bedeschi,Ignacio Bediaga,Andrew Beiter,Vladislav Belavin,Samuel Belin,Violaine Bellee,Konstantin Belous,Ilia Belov,Ivan Belyaev,Giovanni Bencivenni,Eli Ben-Haim,Alexander Berezhnoy,Roland Bernet,Daniel Berninghoff,Harris Conan Bernstein,Claudia Bertella,Alessandro Bertolin,Christopher Betancourt,Federico Betti,Ia Bezshyiko,Srishti Bhasin,Jihyun Bhom,Lingzhu Bian,Martin Stefan Bieker,Nicolo Vladi Biesuz,Simone Bifani,Pierre Billoir,Alice Biolchini,Matthew Birch,Fionn Caitlin Ros Bishop,Alexander Bitadze,Andrea Bizzeti,Mikkel Bjørn,Michele Piero Blago,Thomas Blake,Frederic Blanc,Steven Blusk,Dana Bobulska,Julian Alexander Boelhauve,O Boente Garcia,Thomas Boettcher,Alexey Boldyrev,Alexander Bondar,Nikolay Bondar,Silvia Borghi,Maxim Borisyak,Martino Borsato,Jozef Tomasz Borsuk,Sonia Amina Bouchiba,TJV Bowcock,Alexandre Boyer,Concezio Bozzi,Matthew John Bradley,Svende Braun,A Brea Rodriguez,Jolanta Brodzicka,A Brossa Gonzalo,Davide Brundu,Annarita Buonaura,Laura Buonincontri,Aodhan Tomas Burke,Christopher Burr,Albert Bursche,Anatoly Butkevich,Jordy Sebastiaan Butter,Jan Buytaert,Wiktor Byczynski,Sandro Cadeddu,Hao Cai,Roberto Calabrese,Lukas Calefice,Stefano Cali,Ryan Calladine,Marta Calvi,M Calvo Gomez,P Camargo Magalhaes,Pierluigi Campana,AF Campoverde Quezada,Simone Capelli,Lorenzo Capriotti,Angelo Carbone,Giovanni Carboni,Roberta Cardinale,Alessandro Cardini,Ina Carli,Paolo Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,Rowina Caspary,Gianluigi Casse,Marco Cattaneo,Giovanni Cavallero,Sara Celani

Journal

Journal of High Energy Physics

Published Date

Authors

A Abed Abud,A Friedland,M Smy,P Hamacher-Baumann,Z Djurcic,E Goudzovski,D Totani,I Katsioulas,C Densham,B Russell,E Calvo,P Green,A Penzo,D Shooltz,D Blend,L Singh,J Crnkovic,P Vahle,CS Mishra,MA Acero,H Meyer,DH Koh,D Moretti,G Cerati,M Adamowski,J Zennamo,AS Dyshkant,R Gran,J Stewart,D Marfatia,J Tamara,T Patzak,C Pernas,A Thompson,K Yonehara,JBR Battat,D Kwak,P Dunne,C Brizzolari,K Cho,R Rivera,G Lehmann Miotto,H Newton,C Mariani,S Vallecorsa,S Prakash,IK Furic,A Gabrielli,A Ankowski,PC De Holanda,A Barros,C Benitez Montiel,S Sacerdoti,E Smith,P Keener,X Wang,V Pec,O Palamara,JC Carceller,J Brooke,P Lasorak,CA Moura,A De la Torre,MA Delgado,E Guerard,W Ketchum,C Petta,G Miller,Z Hulcher,DA Dwyer,LW Koerner,J Maalmi,B Szczerbinska,V Tishchenko,A Thea,JRT de Mello Neto,T Gamble,J Matthews,K Moffat,F Muheim,M Chen,L Di Giulio,I Kotler,K Dugas,R Cross,T Cai,GC Blazey,P Novella,B Howard,L Jiang,N Talukdar,A Laundrie,L Suter,MHLS Wang,A Robert,J Soto-Oton,J Kvasnicka,X Ji,Y Onel,N Carrara,H Duyang,A De Roeck,J Franc,A Gago,D Last,J Bhambure,JWF Valle,P De Almeida,V Papadimitriou,Y Suvorov,C Thorn,S Uzunyan,S Manly,F Matichard,D Carber,L Paulucci,T Junk,S Copello,F Di Capua,R Mohanta,G Barr,P Gauzzi,JLL Bazo Alba,S Dolan,SD Reitzner,LS Fajardo,F Psihas,J Heise,S Antusch,K Duffy,S Miryala,D Whittington,L Rochester,C Mossey,L Kolupaeva,N Samios,N Gallice,E Pennacchio,X Qian,E Parozzi,D Torbunov,S Rosauro-Alcaraz,C Wret,O Goodwin,M Worcester,N McConkey,S Gent,A Gallego-Ros,P Laycock,MP Decowski

Published Date

2022/11/2

Measurements of electrons from νe interactions are crucial for the Deep Underground Neutrino Experiment (DUNE) neutrino oscillation program, as well as searches for physics beyond the standard model, supernova neutrino detection, and solar neutrino measurements. This article describes the selection and reconstruction of low-energy (Michel) electrons in the ProtoDUNE-SP detector. ProtoDUNE-SP is one of the prototypes for the DUNE far detector, built and operated at CERN as a charged particle test beam experiment. A sample of lowenergy electrons produced by the decay of cosmic muons is selected with a purity of 95%. This sample is used to calibrate the low-energy electron energy scale with two techniques. An electron energy calibration based on a cosmic ray muon sample uses calibration constants derived from measured and simulated cosmic ray muon events. Another calibration technique makes use of the theoretically well-understood Michel electron energy spectrum to convert reconstructed charge to electron energy. In addition, the effects of detector response to lowenergy electron energy scale and its resolution including readout electronics threshold effects are quantified. Finally, the relation between the theoretical and reconstructed low-energy electron energy spectrum is derived and the energy resolution is characterized. The low-energy electron selection presented here accounts for about 75% of the total electron deposited energy. After the addition of missing energy using a Monte Carlo simulation, the energy resolution improves from about 40% to 25% at 50 MeV. These results are used to validate the expected …

Constraints on the CKM angle γ from B±→ Dh±decays using D→ h±h′∓ π0 final states

Authors

Roel Aaij,Ahmed Sameh Wagih Abdelmotteleb,Carlos Abellán Beteta,FJ Abudinen Gallego,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christina Agapopoulou,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Jake Lewis Amey,Yasmine Amhis,Liupan An,Lucio Anderlini,N Andersson,Aleksei Andreianov,Mirco Andreotti,Flavio Archilli,Alexander Artamonov,Marina Artuso,Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,JJ Back,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista Leite,Matteo Barbetti,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,S Bashir,G Bassi,B Batsukh,A Battig,A Bay,A Beck,M Becker,F Bedeschi,I Bediaga,A Beiter,V Belavin,S Belin,V Bellee,K Belous,I Belov,I Belyaev,G Bencivenni,E Ben-Haim,A Berezhnoy,R Bernet,D Berninghoff,HC Bernstein,C Bertella,A Bertolin,C Betancourt,F Betti,Ia Bezshyiko,S Bhasin,J Bhom,L Bian,MS Bieker,NV Biesuz,S Bifani,P Billoir,A Biolchini,M Birch,FCR Bishop,A Bitadze,A Bizzeti,M Bjørn,MP Blago,T Blake,F Blanc,S Blusk,D Bobulska,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,A Bondar,N Bondar,S Borghi,M Borisyak,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,J Brodzicka,A Brossa Gonzalo,D Brundu,A Buonaura,L Buonincontri,AT Burke,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,S Cali,R Calladine,M Calvi,M Calvo Gomez,P Camargo Magalhaes,P Campana,AF Campoverde Quezada,S Capelli,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,I Carli,P Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,R Caspary,G Casse,M Cattaneo,G Cavallero,S Celani

Journal

Journal of High Energy Physics

Published Date

2022/7

A data sample collected with the LHCb detector corresponding to an integrated luminosity of 9 fb− 1 is used to measure eleven CP violation observables in B±→ Dh±decays, where h is either a kaon or a pion. The neutral D meson decay is reconstructed in the three-body final states: K±π∓ π 0; π+ π− π 0; K+ K− π 0 and the suppressed π±K∓ π 0 combination. The mode where a large CP asymmetry is expected, B±→[π±K∓ π 0] D K±, is observed with a significance greater than seven standard deviations. The ratio of the partial width of this mode relative to that of the favoured mode, B±→[K±π∓ π 0] D K±, is R ADS (K)=(1. 27±0. 16±0. 02)× 10− 2. Evidence for a large CP asymmetry is also seen: A ADS (K)=− 0. 38±0. 12±0. 02. Constraints on the CKM angle γ are calculated from the eleven reported observables.

Response of a CMS HGCAL silicon-pad electromagnetic calorimeter prototype to 20–300 GeV positrons

Authors

B Acar,G Adamov,C Adloff,S Afanasiev,N Akchurin,B Akgün,F Alam Khan,M Alhusseini,J Alison,A Alpana,G Altopp,M Alyari,S An,S Anagul,I Andreev,P Aspell,IO Atakisi,O Bach,A Baden,G Bakas,A Bakshi,S Bannerjee,P Bargassa,D Barney,F Beaudette,F Beaujean,E Becheva,A Becker,P Behera,A Belloni,T Bergauer,M Besancon,S Bhattacharya,D Bhowmik,B Bilki,P Bloch,A Bodek,M Bonanomi,A Bonnemaison,S Bonomally,J Borg,F Bouyjou,N Bower,D Braga,J Brashear,E Brondolin,P Bryant,A Buchot Perraguin,J Bueghly,B Burkle,A Butler-Nalin,O Bychkova,S Callier,D Calvet,X Cao,A Cappati,B Caraway,S Caregari,A Cauchois,L Ceard,YC Cekmecelioglu,S Cerci,G Cerminara,M Chadeeva,N Charitonidis,R Chatterjee,YM Chen,Z Chen,HJ Cheng,KY Cheng,S Chernichenko,H Cheung,CH Chien,S Choudhury,D Čoko,G Collura,F Couderc,M Danilov,D Dannheim,W Daoud,P Dauncey,A David,G Davies,O Davignon,E Day,P Debarbaro,F De Guio,C de La Taille,M De Silva,P Debbins,MM Defranchis,E Delagnes,JM Deltoro Berrio,G Derylo,PG Dias De Almeida,D Diaz,P Dinaucourt,J Dittmann,M Dragicevic,S Dugad,F Dulucq,I Dumanoglu,V Dutta,S Dutta,M Dünser,J Eckdahl,TK Edberg,M El Berni,F Elias,SC Eno,Yu Ershov,P Everaerts,S Extier,F Fahim,C Fallon,G Fedi,BA Fontana Santos Alves,E Frahm,G Franzoni,J Freeman,T French,P Gandhi,S Ganjour,X Gao,A Garcia-Bellido,F Gastaldi,Z Gecse,Y Geerebaert,H Gerwig,O Gevin,S Ghosh,A Gilbert,W Gilbert,K Gill,C Gingu,S Gninenko,A Golunov,I Golutvin,T Gonzalez,N Gorbounov,L Gouskos,AB Gray,Y Gu,F Guilloux,Y Guler,E Gülmez,J Guo,E Gurpinar Guler,M Hammer,HM Hassanshahi

Journal

Journal of instrumentation

Published Date

2022/5/12

The Compact Muon Solenoid (CMS) collaboration will replace the existing calorimeters in the endcaps with a new high-granularity calorimeter (HGCAL)[1] for the High Luminosity-LHC (HLLHC). It will be a sampling calorimeter with hexagonal multipad large-area silicon sensors and plastic scintillator tiles as the active media. The calorimeter endcaps (CE) have both electromagnetic (CE-E) and hadronic (CE-H) sections. The absorber layers of the CE-E section are alternating plates of either lead cladded with stainless steel or copper and copper-tungsten plates; the active layers are all segmented silicon (Si) sensors. The CE-H section uses stainless steel as the absorber and a combination of scintillator and silicon is used as the active material, with Si in the regions of highest radiation. The choice of this particular design was made to cope with the significantly higher radiation levels and the contribution of …

Snowmass Neutrino Frontier: DUNE Physics Summary

Authors

A Abed Abud,B Abi,R Acciarri,MA Acero,MR Adames,G Adamov,M Adamowski,D Adams,M Adinolfi,C Adriano,A Aduszkiewicz,J Aguilar,Z Ahmad,J Ahmed,B Aimard,F Akbar,B Ali-Mohammadzadeh,T Alion,K Allison,S Alonso Monsalve,M AlRashed,C Alt,A Alton,R Alvarez,P Amedo,J Anderson,C Andreopoulos,M Andreotti,MP Andrews,F Andrianala,S Andringa,N Anfimov,A Ankowski,M Antoniassi,M Antonova,A Antoshkin,S Antusch,A Aranda-Fernandez,L Arellano,LO Arnold,MA Arroyave,J Asaadi,L Asquith,A Aurisano,V Aushev,D Autiero,V Ayala Lara,M Ayala-Torres,F Azfar,A Back,H Back,JJ Back,C Backhouse,I Bagaturia,L Bagby,N Balashov,S Balasubramanian,P Baldi,B Baller,B Bambah,F Barao,G Barenboim,GJ Barker,W Barkhouse,C Barnes,G Barr,J Barranco Monarca,A Barros,N Barros,JL Barrow,A Basharina-Freshville,A Bashyal,V Basque,C Batchelor,E Belchior,JBR Battat,F Battisti,F Bay,MCQ Bazetto,JL Alba,JF Beacom,E Bechetoille,B Behera,C Beigbeder,L Bellantoni,G Bellettini,V Bellini,O Beltramello,N Benekos,C Benitez Montiel,F Bento Neves,J Berger,S Berkman,P Bernardini,RM Berner,A Bersani,S Bertolucci,M Betancourt,A Betancur Rodríguez,A Bevan,Y Bezawada,AT Bezerra,TJC Bezerra,A Bhardwaj,V Bhatnagar,M Bhattacharjee,D Bhattarai,S Bhuller,B Bhuyan,S Biagi,J Bian,M Biassoni,K Biery,B Bilki,M Bishai,A Bitadze,A Blake,FDM Blaszczyk,GC Blazey,E Blucher,J Boissevain,S Bolognesi,T Bolton,L Bomben,M Bonesini,M Bongrand,C Bonilla-Diaz,F Bonini,A Booth,F Boran,S Bordoni,A Borkum,N Bostan,P Bour,C Bourgeois,D Boyden,J Bracinik,D Braga,D Brailsford,A Branca,A Brandt,J Bremer,D Breton,C Brew,SJ Brice,C Brizzolari,C Bromberg,J Brooke,A Bross,G Brunetti

Journal

arXiv preprint arXiv:2203.06100

Published Date

2022/3/11

The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino oscillation experiment with a primary physics goal of observing neutrino and antineutrino oscillation patterns to precisely measure the parameters governing long-baseline neutrino oscillation in a single experiment, and to test the three-flavor paradigm. DUNE's design has been developed by a large, international collaboration of scientists and engineers to have unique capability to measure neutrino oscillation as a function of energy in a broadband beam, to resolve degeneracy among oscillation parameters, and to control systematic uncertainty using the exquisite imaging capability of massive LArTPC far detector modules and an argon-based near detector. DUNE's neutrino oscillation measurements will unambiguously resolve the neutrino mass ordering and provide the sensitivity to discover CP violation in neutrinos for a wide range of possible values of . DUNE is also uniquely sensitive to electron neutrinos from a galactic supernova burst, and to a broad range of physics beyond the Standard Model (BSM), including nucleon decays. DUNE is anticipated to begin collecting physics data with Phase I, an initial experiment configuration consisting of two far detector modules and a minimal suite of near detector components, with a 1.2 MW proton beam. To realize its extensive, world-leading physics potential requires the full scope of DUNE be completed in Phase II. The three Phase II upgrades are all necessary to achieve DUNE's physics goals: (1) addition of far detector modules three and four for a total FD fiducial mass of at least 40 kt, (2 …

Precise determination of the – oscillation frequency

Journal

Nature Physics

Published Date

2022/1

Mesons comprising a beauty quark and strange quark can oscillate between particle () and antiparticle () flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, Δms. Here we present a measurement of Δms using π+ decays produced in proton–proton collisions collected with the LHCb detector at the Large Hadron Collider. The oscillation frequency is found to be Δms = 17.7683 ± 0.0051 ± 0.0032 ps−1, where the first uncertainty is statistical and the second is systematic. This measurement improves on the current Δms precision by a factor of two. We combine this result with previous LHCb measurements to determine Δms = 17.7656 ± 0.0057 ps−1, which is the legacy measurement of the original LHCb detector.

Measurement of the photon polarization in decays

Authors

Roel Aaij,Ahmed Sameh Wagih Abdelmotteleb,C Abellan Beteta,F Abudinen,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christina Agapopoulou,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Jake Lewis Amey,Yasmine Amhis,Liupan An,Lucio Anderlini,Aleksei Andreianov,Mirco Andreotti,Flavio Archilli,Alexander Artamonov,Marina Artuso,Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,JJ Back,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista Leite,Matteo Barbetti,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,Saliha Bashir,Giovanni Bassi,Baasansuren Batsukh,Alexander Battig,Aurelio Bay,Anja Beck,Maik Becker,Franco Bedeschi,Ignacio Bediaga,Andrew Beiter,Vladislav Belavin,Samuel Belin,Violaine Bellee,Konstantin Belous,Ilia Belov,Ivan Belyaev,Giovanni Bencivenni,Eli Ben-Haim,Alexander Berezhnoy,Roland Bernet,Daniel Berninghoff,Harris Conan Bernstein,Claudia Bertella,Alessandro Bertolin,Christopher Betancourt,Federico Betti,Ia Bezshyiko,S Bhasin,J Bhom,L Bian,MS Bieker,S Bifani,P Billoir,M Birch,FCR Bishop,A Bitadze,A Bizzeti,M Bjørn,MP Blago,T Blake,F Blanc,S Blusk,D Bobulska,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,A Bondar,N Bondar,S Borghi,M Borisyak,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,J Brodzicka,A Brossa Gonzalo,D Brundu,A Buonaura,L Buonincontri,AT Burke,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,L Calero Diaz,S Cali,R Calladine,M Calvi,M Calvo Gomez,P Camargo Magalhaes,P Campana,AF Campoverde Quezada,S Capelli,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,I Carli,P Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,G Casse,M Cattaneo,G Cavallero,S Celani,J Cerasoli,D Cervenkov,AJ Chadwick

Journal

Physical Review D

Published Date

2022/3/23

Authors

Journal

Journal of High Energy Physics

Published Date

2021/11

An angular analysis of the rare decay→ ϕμ+ μ− is presented, using proton-proton collision data collected by the LHCb experiment at centre-of-mass energies of 7, 8 and 13 TeV, corresponding to an integrated luminosity of 8.4 fb− 1. The observables describing the angular distributions of the decay→ ϕμ+ μ− are determined in regions of q 2, the square of the dimuon invariant mass. The results are consistent with Standard Model predictions.

Structural Evolution and Electronic Properties of Intermediate Sized Tin Clusters

Authors

Peter L Rodríguez‐Kessler,Adán R Rodríguez‐Domínguez,Alvaro Muñoz‐Castro

Journal

Advanced Theory and Simulations

Published Date

2021/12

The structural evolution of Tin () clusters has been investigated by using the systematic cluster growth method together with the many‐body Gupta potential. The lowest energy structures are further refined by using density functional theory computations within the accuracy of the Perdew‐Burke‐Ernzerhof (PBE) exchange‐correlation functional and a plane‐wave basis set. Using this approach, the structures and stability trends of Tin clusters in the size range previously reported, are reproduced. New clusters with enhanced stability are found for , 38, 41, 43, 46, 48, 50, 53, 55, and 58 sizes. Tightly packed structures dominate principally for these clusters in which the shape of the structures can be understood based on the encapsulated motif. The geometries of the clusters from Ti33 up to Ti60 adopt oblate forms which is in contrast to the smaller clusters. The vertical ionization potential (vIP) and …

Search for time-dependent violation in and decays

Authors

Roel Aaij,C Abellan Beteta,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Yasmine Amhis,Liupan An,Lucio Anderlini,Aleksei Andreianov,Mirco Andreotti,Flavio Archilli,Alexander Artamonov,Marina Artuso,Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,JJ Back,Sophie Baker,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista Leite,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,Giovanni Bassi,Baasansuren Batsukh,Alexander Battig,Aurelio Bay,Maik Becker,Franco Bedeschi,Ignacio Bediaga,Andrew Beiter,Vladislav Belavin,Samuel Belin,Violaine Bellee,Konstantin Belous,Ilia Belov,Ivan Belyaev,Giovanni Bencivenni,Eli Ben-Haim,Alexander Berezhnoy,Roland Bernet,Daniel Berninghoff,Harris Conan Bernstein,Claudia Bertella,Alessandro Bertolin,Christopher Betancourt,Federico Betti,Ia Bezshyiko,Srishti Bhasin,Jihyun Bhom,Lingzhu Bian,Martin Stefan Bieker,Simone Bifani,Pierre Billoir,Matthew Birch,Fionn Caitlin Ros Bishop,Alexander Bitadze,Andrea Bizzeti,Mikkel Bjørn,Michele Piero Blago,Thomas Blake,Frederic Blanc,Steven Blusk,Dana Bobulska,Julian Alexander Boelhauve,O Boente Garcia,Thomas Boettcher,Alexey Boldyrev,Alexander Bondar,Nikolay Bondar,Silvia Borghi,Maxim Borisyak,Martino Borsato,Jozef Tomasz Borsuk,Sonia Amina Bouchiba,TJV Bowcock,Alexandre Boyer,Concezio Bozzi,Matthew John Bradley,Svende Braun,A Brea Rodriguez,Michael Brodski,Jolanta Brodzicka,A Brossa Gonzalo,Davide Brundu,Annarita Buonaura,Christopher Burr,Albert Bursche,Anatoly Butkevich,Jordy Sebastiaan Butter,Jan Buytaert,Wiktor Byczynski,Sandro Cadeddu,Hao Cai,Roberto Calabrese,Lukas Calefice,L Calero Diaz,Stefano Cali,Ryan Calladine,Marta Calvi,M Calvo Gomez,P Camargo Magalhaes,Alessandro Camboni,Pierluigi Campana,AF Campoverde Quezada,Simone Capelli,Lorenzo Capriotti,Angelo Carbone,Giovanni Carboni,Roberta Cardinale,Alessandro Cardini,Ina Carli,Paolo Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,Gianluigi Casse,Marco Cattaneo,Giovanni Cavallero,Sara Celani,Jacopo Cerasoli,Abbie Jane Chadwick,Matthew George Chapman,Matthew Charles,Ph Charpentier,Georgios Chatzikonstantinidis,CA Chavez Barajas,Maximilien Chefdeville,Chen Chen

Journal

Physical Review D

Published Date

2021/10/26

A search for time-dependent violation of the charge-parity symmetry in D 0→ K+ K− and D 0→ π+ π− decays is performed at the LHCb experiment using proton-proton collision data recorded from 2015 to 2018 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 6 fb− 1. The D 0 meson is required to originate from a D*(2010)+→ D 0 π+ decay, such that its flavor at production is identified by the charge of the accompanying pion. The slope of the time-dependent asymmetry of the decay rates of D 0 and D 0 mesons into the final states under consideration is measured to be Δ Y K+ K−=(− 2.3±1.5±0.3)× 10− 4, Δ Y π+ π−=(− 4.0±2.8±0.4)× 10− 4, where the first uncertainties are statistical and the second are systematic. These results are compatible with the conservation of the charge-parity symmetry at the level of 2 standard deviations and improve the precision by nearly a factor of 2.

Observation of excited baryons in decays

Authors

Roel Aaij,C Abellán Beteta,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Yasmine Amhis,Liupan An,Lucio Anderlini,Aleksei Andreianov,Mirco Andreotti,Flavio Archilli,Alexander Artamonov,Marina Artuso,Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,JJ Back,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista Leite,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,Giovanni Bassi,Baasansuren Batsukh,Alexander Battig,Aurelio Bay,Maik Becker,Franco Bedeschi,Ignacio Bediaga,Andrew Beiter,Vladislav Belavin,Samuel Belin,Violaine Bellee,Konstantin Belous,Ilia Belov,Ivan Belyaev,Giovanni Bencivenni,Eli Ben-Haim,Alexander Berezhnoy,Roland Bernet,Daniel Berninghoff,Harris Conan Bernstein,Claudia Bertella,Alessandro Bertolin,Christopher Betancourt,Federico Betti,Ia Bezshyiko,Srishti Bhasin,Jihyun Bhom,Lingzhu Bian,Martin Stefan Bieker,Simone Bifani,Pierre Billoir,Matthew Birch,Fionn Caitlin Ros Bishop,Alexander Bitadze,Andrea Bizzeti,Mikkel Bjørn,Michele Piero Blago,Thomas Blake,Frederic Blanc,Steven Blusk,Dana Bobulska,Julian Alexander Boelhauve,O Boente Garcia,Thomas Boettcher,Alexey Boldyrev,Alexander Bondar,Nikolay Bondar,Silvia Borghi,Maxim Borisyak,Martino Borsato,Jozef Tomasz Borsuk,Sonia Amina Bouchiba,TJV Bowcock,Alexandre Boyer,Concezio Bozzi,Matthew John Bradley,Svende Braun,A Brea Rodriguez,Michael Brodski,Jolanta Brodzicka,A Brossa Gonzalo,Davide Brundu,Annarita Buonaura,Christopher Burr,Albert Bursche,Anatoly Butkevich,Jordy Sebastiaan Butter,Jan Buytaert,Wiktor Byczynski,Sandro Cadeddu,Hao Cai,Roberto Calabrese,Lukas Calefice,L Calero Diaz,Stefano Cali,Ryan Calladine,Marta Calvi,M Calvo Gomez,P Camargo Magalhaes,Pierluigi Campana,AF Campoverde Quezada,Simone Capelli,Lorenzo Capriotti,Angelo Carbone,Giovanni Carboni,Roberta Cardinale,Alessandro Cardini,Ina Carli,Paolo Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,Gianluigi Casse,Marco Cattaneo,Giovanni Cavallero,Sara Celani,Jacopo Cerasoli,Abbie Jane Chadwick,Matthew George Chapman,Matthew Charles,Ph Charpentier,Georgios Chatzikonstantinidis,CA Chavez Barajas,Maximilien Chefdeville,Chen Chen,Shanzhen Chen,Aleksei Chernov

Journal

Physical Review D

Published Date

2021/11/24

The first observation of the Ω b−→ Ξ c+ K− π− decay is reported using p p collision data at center of mass energies of 7, 8, and 13 TeV collected by the LHCb experiment, corresponding to an integrated luminosity of 9 fb− 1. Four excited Ω c 0 baryons are observed in the Ξ c+ K− mass projection of the Ω b−→ Ξ c+ K− π− decays with the significance of each exceeding five standard deviations. They coincide with the states previously observed in prompt p p and e+ e− production. Relative production rates, masses, and natural widths of the states are measured, and a test of spin hypotheses is performed. Moreover, the branching ratio of Ω b−→ Ξ c+ K− π− is measured relative to the Ω b−→ Ω c 0 π− decay mode and a precise measurement of the Ω b− mass of 6044.3±1.2±1. 1− 0.22+ 0.19 MeV is obtained.

Searching for solar KDAR with DUNE

Authors

A Abed Abud,B Abi,R Acciarri,MA Acero,MR Adames,G Adamov,D Adams,M Adinolfi,A Aduszkiewicz,J Aguilar,Z Ahmad,J Ahmed,B Ali-Mohammadzadeh,T Alion,K Allison,S Alonso Monsalve,M Alrashed,C Alt,A Alton,P Amedo,J Anderson,C Andreopoulos,M Andreotti,MP Andrews,F Andrianala,S Andringa,N Anfimov,A Ankowski,M Antoniassi,M Antonova,A Antoshkin,S Antusch,A Aranda-Fernandez,A Ariga,LO Arnold,MA Arroyave,J Asaadi,L Asquith,A Aurisano,V Aushev,D Autiero,M Ayala-Torres,F Azfar,A Back,H Back,JJ Back,C Backhouse,P Baesso,I Bagaturia,L Bagby,N Balashov,S Balasubramanian,P Baldi,B Baller,B Bambah,F Barao,G Barenboim,GJ Barker,W Barkhouse,C Barnes,G Barr,J Barranco Monarca,A Barros,N Barros,JL Barrow,A Basharina-Freshville,A Bashyal,V Basque,E Belchior,JBR Battat,F Battisti,F Bay,JL Bazo Alba,JF Beacom,E Bechetoille,B Behera,L Bellantoni,G Bellettini,V Bellini,O Beltramello,D Belver,N Benekos,C Benitez Montiel,F Bento Neves,J Berger,S Berkman,P Bernardini,RM Berner,H Berns,S Bertolucci,M Betancourt,A Betancur Rodríguez,A Bevan,TJC Bezerra,V Bhatnagar,M Bhattacharjee,S Bhuller,B Bhuyan,S Biagi,J Bian,M Biassoni,K Biery,B Bilki,M Bishai,A Bitadze,A Blake,FDM Blaszczyk,GC Blazey,E Blucher,J Boissevain,S Bolognesi,T Bolton,L Bomben,M Bonesini,M Bongrand,F Bonini,A Booth,C Booth,F Boran,S Bordoni,A Borkum,T Boschi,N Bostan,P Bour,C Bourgeois,SB Boyd,D Boyden,J Bracinik,D Braga,D Brailsford,A Branca,A Brandt,J Bremer,C Brew,E Brianne,SJ Brice,C Brizzolari,C Bromberg,G Brooijmans,J Brooke,A Bross,G Brunetti,M Brunetti,N Buchanan,H Budd,I Butorov,I Cagnoli,D Caiulo,R Calabrese,P Calafiura

Journal

Journal of Cosmology and Astroparticle Physics

Published Date

2021/10/22

The observation of 236MeV muon neutrinos from kaon-decay-at-rest (KDAR) originating in the core of the Sun would provide a unique signature of dark matter annihilation. Since excellent angle and energy reconstruction are necessary to detect this monoenergetic, directional neutrino flux, DUNE with its vast volume and reconstruction capabilities, is a promising candidate for a KDAR neutrino search. In this work, we evaluate the proposed KDAR neutrino search strategies by realistically modeling both neutrino-nucleus interactions and the response of DUNE. We find that, although reconstruction of the neutrino energy and direction is difficult with current techniques in the relevant energy range, the superb energy resolution, angular resolution, and particle identification offered by DUNE can still permit great signal/background discrimination. Moreover, there are non-standard scenarios in which searches at DUNE …

First measurement of the-violating phase in) decays

Authors

R Aaij,C Abellán Beteta,T Ackernley,B Adeva,M Adinolfi,H Afsharnia,CA Aidala,S Aiola,Z Ajaltouni,S Akar,J Albrecht,F Alessio,M Alexander,A Alfonso Albero,Z Aliouche,G Alkhazov,P Alvarez Cartelle,S Amato,Y Amhis,L An,L Anderlini,A Andreianov,M Andreotti,F Archilli,A Artamonov,M Artuso,K Arzymatov,E Aslanides,M Atzeni,B Audurier,S Bachmann,M Bachmayer,JJ Back,S Baker,P Baladron Rodriguez,V Balagura,W Baldini,J Baptista Leite,RJ Barlow,S Barsuk,W Barter,M Bartolini,F Baryshnikov,JM Basels,G Bassi,V Batozskaya,B Batsukh,A Battig,A Bay,M Becker,F Bedeschi,I Bediaga,A Beiter,V Belavin,S Belin,V Bellee,K Belous,I Belov,I Belyaev,G Bencivenni,E Ben-Haim,A Berezhnoy,R Bernet,D Berninghoff,HC Bernstein,C Bertella,E Bertholet,A Bertolin,C Betancourt,F Betti,MO Bettler,Ia Bezshyiko,S Bhasin,J Bhom,L Bian,MS Bieker,S Bifani,P Billoir,M Birch,FCR Bishop,A Bizzeti,M Bjørn,MP Blago,T Blake,F Blanc,S Blusk,D Bobulska,JA Boelhauve,O Boente Garcia,T Boettcher,A Boldyrev,A Bondar,N Bondar,S Borghi,M Borisyak,M Borsato,JT Borsuk,SA Bouchiba,TJV Bowcock,A Boyer,C Bozzi,MJ Bradley,S Braun,A Brea Rodriguez,M Brodski,J Brodzicka,A Brossa Gonzalo,D Brundu,A Buonaura,C Burr,A Bursche,A Butkevich,JS Butter,J Buytaert,W Byczynski,S Cadeddu,H Cai,R Calabrese,L Calefice,L Calero Diaz,S Cali,R Calladine,M Calvi,M Calvo Gomez,P Camargo Magalhaes,A Camboni,P Campana,DH Campora Perez,AF Campoverde Quezada,S Capelli,L Capriotti,A Carbone,G Carboni,R Cardinale,A Cardini,I Carli,P Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,G Casse,M Cattaneo,G Cavallero,S Celani,J Cerasoli,AJ Chadwick,MG Chapman,M Charles,Ph Charpentier,G Chatzikonstantinidis

Journal

The European Physical Journal C

Published Date

2021/11/1

A flavour-tagged time-dependent angular analysis of decays is presented where the meson is reconstructed through its decay to an pair. The analysis uses a sample of pp collision data recorded with the LHCb experiment at centre-of-mass energies of 7 and , corresponding to an integrated luminosity of . The -violating phase and lifetime parameters of the system are measured to be , and where the first uncertainty is statistical and the second systematic. This is the first time that -violating parameters are measured in the decay with an pair in the final state. The results are consistent with previous measurements in other channels and with the Standard Model predictions.

Observation of the suppressed decay with and measurement of its asymmetry

Authors

Roel Aaij,Ahmed Sameh Wagih Abdelmotteleb,C Abellan Beteta,FJ Abudinen Gallego,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,Christina Agapopoulou,Christine Angela Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A Alfonso Albero,Zakariya Aliouche,Georgy Alkhazov,P Alvarez Cartelle,Sandra Amato,Jake Lewis Amey,Yasmine Amhis,Liupan An,Lucio Anderlini,Aleksei Andreianov,Mirco Andreotti,Flavio Archilli,Alexander Artamonov,Marina Artuso,Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,JJ Back,P Baladron Rodriguez,Vladislav Balagura,Wander Baldini,J Baptista Leite,Matteo Barbetti,RJ Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov,Jan-Marc Basels,Saliha Bashir,Giovanni Bassi,Baasansuren Batsukh,Alexander Battig,Aurelio Bay,Anja Beck,Maik Becker,Franco Bedeschi,Ignacio Bediaga,Andrew Beiter,Vladislav Belavin,Samuel Belin,Violaine Bellee,Konstantin Belous,Ilia Belov,Ivan Belyaev,Giovanni Bencivenni,Eli Ben-Haim,Alexander Berezhnoy,Roland Bernet,Daniel Berninghoff,Harris Conan Bernstein,Claudia Bertella,Alessandro Bertolin,Christopher Betancourt,Federico Betti,Ia Bezshyiko,Srishti Bhasin,Jihyun Bhom,Lingzhu Bian,Martin Stefan Bieker,Simone Bifani,Pierre Billoir,Matthew Birch,Fionn Caitlin Ros Bishop,Alexander Bitadze,Andrea Bizzeti,Mikkel Bjørn,Michele Piero Blago,Thomas Blake,Frederic Blanc,Steven Blusk,Dana Bobulska,Julian Alexander Boelhauve,O Boente Garcia,Thomas Boettcher,Alexey Boldyrev,Alexander Bondar,Nikolay Bondar,Silvia Borghi,Maxim Borisyak,Martino Borsato,Jozef Tomasz Borsuk,Sonia Amina Bouchiba,TJV Bowcock,Alexandre Boyer,Concezio Bozzi,Matthew John Bradley,Svende Braun,A Brea Rodriguez,Michael Brodski,Jolanta Brodzicka,A Brossa Gonzalo,Davide Brundu,Annarita Buonaura,Laura Buonincontri,Aodhan Tomas Burke,Christopher Burr,Albert Bursche,Anatoly Butkevich,Jordy Sebastiaan Butter,Jan Buytaert,Wiktor Byczynski,Sandro Cadeddu,Hao Cai,Roberto Calabrese,Lukas Calefice,L Calero Diaz,Stefano Cali,Ryan Calladine,Marta Calvi,M Calvo Gomez,P Camargo Magalhaes,Pierluigi Campana,AF Campoverde Quezada,Simone Capelli,Lorenzo Capriotti,Angelo Carbone,Giovanni Carboni,Roberta Cardinale,Alessandro Cardini,Ina Carli,Paolo Carniti,L Carus,K Carvalho Akiba,A Casais Vidal,Gianluigi Casse,Marco Cattaneo,Giovanni Cavallero,Sara Celani,Jacopo Cerasoli,Daniel Cervenkov

Journal

Physical Review D

Published Date

2021/12/27

A study of Λ b 0 baryon decays to the D p K− final state is presented based on a proton-proton collision data sample corresponding to an integrated luminosity of 9 fb− 1 collected with the LHCb detector. Two Λ b 0 decays are considered, Λ b 0→ D p K− with D→ K− π+ and D→ K+ π−, where D represents a superposition of D 0 and D 0 states. The latter process is expected to be suppressed relative to the former, and is observed for the first time. The ratio of branching fractions of the two decays is measured, and the C P asymmetry of the suppressed mode, which is sensitive to the Cabibbo-Kobayashi-Maskawa angle γ, is also reported.

See List of Professors in Adan Ruben Rodriguez Dominguez University(Universidad Autónoma de San Luis Potosí)

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What is Adan Ruben Rodriguez Dominguez's h-index at Universidad Autónoma de San Luis Potosí?

The h-index of Adan Ruben Rodriguez Dominguez has been 56 since 2020 and 77 in total.

What are Adan Ruben Rodriguez Dominguez's top articles?

The articles with the titles of

Structures of Ni-doped Bn (n= 1-13) clusters: A Computational Study

Helium identification with LHCb

Evaluation of the implementation of a community health worker-led COVID-19 contact tracing intervention in Chiapas, Mexico, from March 2020 to December 2021

Observation of and decays

Performance of a modular ton-scale pixel-readout liquid argon Time Projection Chamber

The DUNE Far Detector Vertical Drift Technology, Technical Design Report

Measurement of the CKM angle γ in the B 0 → D K ∗ 0 channel using self-conjugate D → K S 0 h + h - decays

Doping liquid argon with xenon in ProtoDUNE Single-Phase: effects on scintillation light

...

are the top articles of Adan Ruben Rodriguez Dominguez at Universidad Autónoma de San Luis Potosí.

What are Adan Ruben Rodriguez Dominguez's research interests?

The research interests of Adan Ruben Rodriguez Dominguez are: theoretical physics, condensed matter, mathematical physics, electronic and magnetic structure of small TM clusters, their stabi

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Adan Ruben Rodriguez Dominguez has 19,734 citations in total.

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