Synchronization of activity among myocytes constituting vital organs, e.g., the heart, is crucial for physiological functions. Self-organized coordination in such heterogeneous ensemble of excitable and oscillatory cells is therefore of clinical importance. We show by varying the strength of intercellular coupling and the electrophysiological diversity, a wide range of collective behavior emerges including clusters of synchronized activity. Strikingly, stretch-activated currents allow waves of mechanical deformation to alter the activity of neighboring cells, promoting robust global coherence.
{"title":"Mechanics Promotes Coherence in Heterogeneous Active Media.","authors":"Soling Zimik, Sitabhra Sinha","doi":"10.1103/8gqg-rsrl","DOIUrl":"https://doi.org/10.1103/8gqg-rsrl","url":null,"abstract":"<p><p>Synchronization of activity among myocytes constituting vital organs, e.g., the heart, is crucial for physiological functions. Self-organized coordination in such heterogeneous ensemble of excitable and oscillatory cells is therefore of clinical importance. We show by varying the strength of intercellular coupling and the electrophysiological diversity, a wide range of collective behavior emerges including clusters of synchronized activity. Strikingly, stretch-activated currents allow waves of mechanical deformation to alter the activity of neighboring cells, promoting robust global coherence.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"135 24","pages":"248401"},"PeriodicalIF":9.0,"publicationDate":"2025-12-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145893218","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Driving materials using light with more than one frequency component is an emerging technique, enabled by advanced pulse-shaping capabilities in recent years. Here, we translate this technique to lattice vibrations by exciting multicolor phonons using terahertz cavities. In contrast to light, phonon frequencies are determined by the crystal structure and cannot readily be changed. We overcome this problem by tuning the frequencies of phonon polaritons in terahertz cavities to achieve the desired frequency ratios necessary for phononic Lissajous figures. This methodology enables dynamical crystallographic symmetry breaking and the creation of staggered phonon angular momentum and magnetic moment patterns.
{"title":"Multicolor Phonon Excitation in Terahertz Cavities.","authors":"Omer Yaniv, Dominik M Juraschek","doi":"10.1103/fwr7-6jj6","DOIUrl":"https://doi.org/10.1103/fwr7-6jj6","url":null,"abstract":"<p><p>Driving materials using light with more than one frequency component is an emerging technique, enabled by advanced pulse-shaping capabilities in recent years. Here, we translate this technique to lattice vibrations by exciting multicolor phonons using terahertz cavities. In contrast to light, phonon frequencies are determined by the crystal structure and cannot readily be changed. We overcome this problem by tuning the frequencies of phonon polaritons in terahertz cavities to achieve the desired frequency ratios necessary for phononic Lissajous figures. This methodology enables dynamical crystallographic symmetry breaking and the creation of staggered phonon angular momentum and magnetic moment patterns.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"135 24","pages":"246901"},"PeriodicalIF":9.0,"publicationDate":"2025-12-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145893262","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Tangyou Huang, Akshay Gaikwad, Ilya Moskalenko, Anuj Aggarwal, Tahereh Abad, Marko Kuzmanović, Yu-Han Chang, Ognjen Stanisavljević, Emil Hogedal, Christhopher Warren, Irshad Ahmad, Janka Biznárová, Amr Osman, Mamta Dahiya, Marcus Rommel, Anita Fadavi Rousari, Andreas Nylander, Liangyu Chen, Jonas Bylander, Gheorghe Sorin Paraoanu, Anton Frisk Kockum, Giovanna Tancredi
Accurate and robust quantum process tomography (QPT) is crucial for verifying quantum gates and diagnosing implementation faults in experiments aimed at building universal quantum computers. However, the reliability of QPT protocols is often compromised by faulty probes, particularly state preparation and measurement (SPAM) errors, which introduce fundamental inconsistencies in traditional QPT algorithms. We propose and investigate enhanced QPT for multiqubit systems by integrating the error matrix in a digital twin of the identity process matrix, enabling statistical refinement of SPAM error learning and improving QPT precision. Through numerical simulations, we demonstrate that our approach enables highly accurate and faithful process characterization. We further validate our method experimentally in superconducting quantum processors, achieving at least an order-of-magnitude fidelity improvement over standard QPT. Our results provide a practical and precise method for assessing quantum gate fidelity and enhancing QPT on a given hardware.
{"title":"Quantum Process Tomography with Digital Twins of Error Matrices.","authors":"Tangyou Huang, Akshay Gaikwad, Ilya Moskalenko, Anuj Aggarwal, Tahereh Abad, Marko Kuzmanović, Yu-Han Chang, Ognjen Stanisavljević, Emil Hogedal, Christhopher Warren, Irshad Ahmad, Janka Biznárová, Amr Osman, Mamta Dahiya, Marcus Rommel, Anita Fadavi Rousari, Andreas Nylander, Liangyu Chen, Jonas Bylander, Gheorghe Sorin Paraoanu, Anton Frisk Kockum, Giovanna Tancredi","doi":"10.1103/dpgy-rtxr","DOIUrl":"https://doi.org/10.1103/dpgy-rtxr","url":null,"abstract":"<p><p>Accurate and robust quantum process tomography (QPT) is crucial for verifying quantum gates and diagnosing implementation faults in experiments aimed at building universal quantum computers. However, the reliability of QPT protocols is often compromised by faulty probes, particularly state preparation and measurement (SPAM) errors, which introduce fundamental inconsistencies in traditional QPT algorithms. We propose and investigate enhanced QPT for multiqubit systems by integrating the error matrix in a digital twin of the identity process matrix, enabling statistical refinement of SPAM error learning and improving QPT precision. Through numerical simulations, we demonstrate that our approach enables highly accurate and faithful process characterization. We further validate our method experimentally in superconducting quantum processors, achieving at least an order-of-magnitude fidelity improvement over standard QPT. Our results provide a practical and precise method for assessing quantum gate fidelity and enhancing QPT on a given hardware.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"135 23","pages":"230601"},"PeriodicalIF":9.0,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145794419","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Content-addressable memory, i.e., stored information that can be retrieved from content-based cues, is key to computation. Besides natural and artificial neural networks, physical learning systems have recently been shown to have remarkable ability in this domain. While classical neural network models encode memories as energy minima, biochemical systems have been shown to be able to process information based on purely kinetic principles. This raises the question of whether neural networks can also encode information kinetically. Here, we propose a minimal model for content-addressable memory in which the kinetics, and not the energy function, are used to encode patterns. We find that the performance of this kinetic encoding is comparable to that of classical energy-based approaches. This highlights the fundamental significance of the kinetic stability of kinetic traps as an alternative to the thermodynamic stability of energy minima, offering new insights into the principles of computation in physical and synthetic systems.
{"title":"Content-Addressable Memory with a Content-Free Energy Function.","authors":"Félix Benoist, Luca Peliti, Pablo Sartori","doi":"10.1103/tcqx-586g","DOIUrl":"https://doi.org/10.1103/tcqx-586g","url":null,"abstract":"<p><p>Content-addressable memory, i.e., stored information that can be retrieved from content-based cues, is key to computation. Besides natural and artificial neural networks, physical learning systems have recently been shown to have remarkable ability in this domain. While classical neural network models encode memories as energy minima, biochemical systems have been shown to be able to process information based on purely kinetic principles. This raises the question of whether neural networks can also encode information kinetically. Here, we propose a minimal model for content-addressable memory in which the kinetics, and not the energy function, are used to encode patterns. We find that the performance of this kinetic encoding is comparable to that of classical energy-based approaches. This highlights the fundamental significance of the kinetic stability of kinetic traps as an alternative to the thermodynamic stability of energy minima, offering new insights into the principles of computation in physical and synthetic systems.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"135 23","pages":"237102"},"PeriodicalIF":9.0,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145794464","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
One of the most remarkable features that distinguish open systems from closed ones is the presence of exceptional points (EPs), where two or more eigenvectors of a non-Hermitian operator coalesce, accompanying the convergence of the corresponding eigenvalues. So far, EPs have been demonstrated on a number of platforms, ranging from classical optical systems to fully quantum-mechanical spin-boson models. In these demonstrations, the reservoir that induced the non-Hermiticity was treated as a Markovian one, without considering its memory effect. We here present the first experimental demonstration of non-Markovian quantum EPs, engineered by coupling a Josephson-junction-based qubit to a leaky electromagnetic resonator, which acts as a non-Markovian reservoir. We map out the spectrum of the extended Liouvillian superoperator by observing the quantum state evolution of the qubit and the pseudomode, in which the memory of the reservoir is encoded. We identify a twofold second-order EP and a third-order EP in the Liouvillian spectrum, which cannot be realized with a Markovian reservoir. Our results pave the way for experimental exploration of exotic phenomena associated with non-Markovian quantum EPs.
{"title":"Experimental Observation of Non-Markovian Quantum Exceptional Points.","authors":"Hao-Long Zhang, Pei-Rong Han, Fan Wu, Wen Ning, Zhen-Biao Yang, Shi-Biao Zheng","doi":"10.1103/jk6y-55xp","DOIUrl":"https://doi.org/10.1103/jk6y-55xp","url":null,"abstract":"<p><p>One of the most remarkable features that distinguish open systems from closed ones is the presence of exceptional points (EPs), where two or more eigenvectors of a non-Hermitian operator coalesce, accompanying the convergence of the corresponding eigenvalues. So far, EPs have been demonstrated on a number of platforms, ranging from classical optical systems to fully quantum-mechanical spin-boson models. In these demonstrations, the reservoir that induced the non-Hermiticity was treated as a Markovian one, without considering its memory effect. We here present the first experimental demonstration of non-Markovian quantum EPs, engineered by coupling a Josephson-junction-based qubit to a leaky electromagnetic resonator, which acts as a non-Markovian reservoir. We map out the spectrum of the extended Liouvillian superoperator by observing the quantum state evolution of the qubit and the pseudomode, in which the memory of the reservoir is encoded. We identify a twofold second-order EP and a third-order EP in the Liouvillian spectrum, which cannot be realized with a Markovian reservoir. Our results pave the way for experimental exploration of exotic phenomena associated with non-Markovian quantum EPs.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"135 23","pages":"230203"},"PeriodicalIF":9.0,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145794564","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Interference between scattering channels is observed in resonant inelastic x-ray scattering (RIXS) at the Ne K threshold. Final states with |2p^{-1}np⟩ as the main configuration are populated via |1s^{-1}n^{'}p⟩ resonances, where large-amplitude one-electron (n^{'}=n) channels interfere with small-amplitude two-electron (n^{'}≠n) channels. The interference is manifested in an asymmetric line profile where the two-electron resonance occurs in the tail region of the one-electron resonance. In RIXS, this slowly varying tail plays the role of the continuum for the Fano effect. The asymmetric profile is well modeled by means of a single asymmetry parameter, determined by the amplitudes of the scattering channels and the energy separation between the resonances.
{"title":"Interference between One- and Two-Electron Channels in Resonant Inelastic X-Ray Scattering.","authors":"Johan Söderström,Marcus Agåker,Ji-Cai Liu,Takashi Tokushima,Anirudha Ghosh,Conny Såthe,Jian Wang,Andreas Pantelis Frey Koudouridis,Moritz Grunwald-Delitz,Thomas M Baumann,Michael Meyer,Manuel Harder,Zhong Yin,Olle Björneholm,Joseph Nordgren,Stephan Fritzsche,Victor Kimberg,Jan-Erik Rubensson,Faris Gel'mukhanov","doi":"10.1103/c5mk-trlz","DOIUrl":"https://doi.org/10.1103/c5mk-trlz","url":null,"abstract":"Interference between scattering channels is observed in resonant inelastic x-ray scattering (RIXS) at the Ne K threshold. Final states with |2p^{-1}np⟩ as the main configuration are populated via |1s^{-1}n^{'}p⟩ resonances, where large-amplitude one-electron (n^{'}=n) channels interfere with small-amplitude two-electron (n^{'}≠n) channels. The interference is manifested in an asymmetric line profile where the two-electron resonance occurs in the tail region of the one-electron resonance. In RIXS, this slowly varying tail plays the role of the continuum for the Fano effect. The asymmetric profile is well modeled by means of a single asymmetry parameter, determined by the amplitudes of the scattering channels and the energy separation between the resonances.","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"33 1","pages":"233001"},"PeriodicalIF":8.6,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145785869","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
G Aad,E Aakvaag,B Abbott,S Abdelhameed,K Abeling,N J Abicht,S H Abidi,M Aboelela,A Aboulhorma,H Abramowicz,Y Abulaiti,B S Acharya,A Ackermann,C Adam Bourdarios,L Adamczyk,S V Addepalli,M J Addison,J Adelman,A Adiguzel,T Adye,A A Affolder,Y Afik,M N Agaras,A Aggarwal,C Agheorghiesei,F Ahmadov,S Ahuja,X Ai,G Aielli,A Aikot,M Ait Tamlihat,B Aitbenchikh,M Akbiyik,T P A Åkesson,A V Akimov,D Akiyama,N N Akolkar,S Aktas,G L Alberghi,J Albert,U Alberti,P Albicocco,G L Albouy,S Alderweireldt,Z L Alegria,M Aleksa,I N Aleksandrov,C Alexa,T Alexopoulos,F Alfonsi,M Algren,M Alhroob,B Ali,H M J Ali,S Ali,S W Alibocus,M Aliev,G Alimonti,W Alkakhi,C Allaire,B M M Allbrooke,J S Allen,J F Allen,P P Allport,A Aloisio,F Alonso,C Alpigiani,Z M K Alsolami,A Alvarez Fernandez,M Alves Cardoso,M G Alviggi,M Aly,Y Amaral Coutinho,A Ambler,C Amelung,M Amerl,C G Ames,T Amezza,D Amidei,B Amini,K Amirie,A Amirkhanov,S P Amor Dos Santos,K R Amos,D Amperiadou,S An,C Anastopoulos,T Andeen,J K Anders,A C Anderson,A Andreazza,S Angelidakis,A Angerami,A V Anisenkov,A Annovi,C Antel,E Antipov,M Antonelli,F Anulli,M Aoki,T Aoki,M A Aparo,L Aperio Bella,M Apicella,C Appelt,A Apyan,M Arampatzi,S J Arbiol Val,C Arcangeletti,A T H Arce,J-F Arguin,S Argyropoulos,J-H Arling,O Arnaez,H Arnold,G Artoni,H Asada,K Asai,S Asatryan,N A Asbah,R A Ashby Pickering,A M Aslam,K Assamagan,R Astalos,K S V Astrand,S Atashi,R J Atkin,H Atmani,P A Atmasiddha,K Augsten,A D Auriol,V A Austrup,A S Avad,G Avolio,K Axiotis,A Azzam,D Babal,H Bachacou,K Bachas,A Bachiu,E Bachmann,M J Backes,A Badea,T M Baer,P Bagnaia,M Bahmani,D Bahner,K Bai,J T Baines,L Baines,O K Baker,E Bakos,D Bakshi Gupta,L E Balabram Filho,V Balakrishnan,R Balasubramanian,E M Baldin,P Balek,E Ballabene,F Balli,L M Baltes,W K Balunas,J Balz,I Bamwidhi,E Banas,M Bandieramonte,A Bandyopadhyay,S Bansal,L Barak,M Barakat,E L Barberio,D Barberis,M Barbero,M Z Barel,T Barillari,M-S Barisits,T Barklow,P Baron,D A Baron Moreno,A Baroncelli,A J Barr,J D Barr,F Barreiro,J Barreiro Guimarães da Costa,M G Barros Teixeira,S Barsov,F Bartels,R Bartoldus,A E Barton,P Bartos,M Baselga,S Bashiri,A Bassalat,M J Basso,S Bataju,R Bate,R L Bates,S Batlamous,M Battaglia,D Battulga,M Bauce,M Bauer,P Bauer,L T Bayer,L T Bazzano Hurrell,J B Beacham,T Beau,J Y Beaucamp,P H Beauchemin,P Bechtle,H P Beck,K Becker,A J Beddall,V A Bednyakov,C P Bee,L J Beemster,M Begalli,M Begel,J K Behr,J F Beirer,F Beisiegel,M Belfkir,G Bella,L Bellagamba,A Bellerive,C D Bellgraph,P Bellos,K Beloborodov,I Benaoumeur,D Benchekroun,F Bendebba,Y Benhammou,K C Benkendorfer,L Beresford,M Beretta,E Bergeaas Kuutmann,N Berger,B Bergmann,J Beringer,G Bernardi,C Bernius,F U Bernlochner,A Berrocal Guardia,T Berry,P Berta,A Berthold,A Berti,R Bertrand,S Bethke,A Betti,A J Bevan,L Bezio,N K Bhalla,S Bharthuar,S Bhatta,P Bhattarai,Z M Bhatti,K D Bhide,V S Bhopatkar,R M Bianchi,G Bianco,O Biebel,M Biglietti,C S Billingsley,Y Bimgdi,M Bindi,A Bingham,A Bingul,C Bini,G A Bird,M Birman,M Biros,S Biryukov,T Bisanz,E Bisceglie,J P Biswal,D Biswas,I Bloch,A Blue,U Blumenschein,V S Bobrovnikov,L Boccardo,M Boehler,B Boehm,D Bogavac,A G Bogdanchikov,L S Boggia,V Boisvert,P Bokan,T Bold,M Bomben,M Bona,M Boonekamp,A G Borbély,I S Bordulev,G Borissov,D Bortoletto,D Boscherini,M Bosman,K Bouaouda,N Bouchhar,L Boudet,J Boudreau,E V Bouhova-Thacker,D Boumediene,R Bouquet,A Boveia,J Boyd,D Boye,I R Boyko,L Bozianu,J Bracinik,N Brahimi,G Brandt,O Brandt,B Brau,J E Brau,R Brener,L Brenner,R Brenner,S Bressler,G Brianti,D Britton,D Britzger,I Brock,R Brock,G Brooijmans,A J Brooks,E M Brooks,E Brost,L M Brown,L E Bruce,T L Bruckler,P A Bruckman de Renstrom,B Brüers,A Bruni,G Bruni,D Brunner,M Bruschi,N Bruscino,T Buanes,Q Buat,D Buchin,A G Buckley,O Bulekov,B A Bullard,S Burdin,C D Burgard,A M Burger,B Burghgrave,O Burlayenko,J Burleson,J C Burzynski,E L Busch,V Büscher,P J Bussey,J M Butler,C M Buttar,J M Butterworth,W Buttinger,C J Buxo Vazquez,A R Buzykaev,S Cabrera Urbán,L Cadamuro,H Cai,Y Cai,Y Cai,V M M Cairo,O Cakir,N Calace,P Calafiura,G Calderini,P Calfayan,L Calic,G Callea,L P Caloba,D Calvet,S Calvet,R Camacho Toro,S Camarda,D Camarero Munoz,P Camarri,C Camincher,M Campanelli,A Camplani,V Canale,A C Canbay,E Canonero,J Cantero,Y Cao,F Capocasa,M Capua,A Carbone,R Cardarelli,J C J Cardenas,M P Cardiff,G Carducci,T Carli,G Carlino,J I Carlotto,B T Carlson,E M Carlson,J Carmignani,L Carminati,A Carnelli,M Carnesale,S Caron,E Carquin,I B Carr,S Carrá,G Carratta,C Carrion Martinez,A M Carroll,M P Casado,P Casolaro,M Caspar,W R Castiglioni,F L Castillo,L Castillo Garcia,V Castillo Gimenez,N F Castro,A Catinaccio,J R Catmore,T Cavaliere,V Cavaliere,L J Caviedes Betancourt,E Celebi,S Cella,V Cepaitis,K Cerny,A S Cerqueira,A Cerri,L Cerrito,F Cerutti,B Cervato,A Cervelli,G Cesarini,S A Cetin,P M Chabrillat,R Chakkappai,S Chakraborty,A Chambers,J Chan,W Y Chan,J D Chapman,E Chapon,B Chargeishvili,D G Charlton,C Chauhan,Y Che,S Chekanov,S V Chekulaev,G A Chelkov,B Chen,B Chen,H Chen,H Chen,J Chen,J Chen,M Chen,S Chen,S J Chen,X Chen,X Chen,Z Chen,C L Cheng,H C Cheng,S Cheong,A Cheplakov,E Cherepanova,R Cherkaoui El Moursli,E Cheu,K Cheung,L Chevalier,V Chiarella,G Chiarelli,G Chiodini,A S Chisholm,A Chitan,M Chitishvili,M V Chizhov,K Choi,Y Chou,E Y S Chow,K L Chu,M C Chu,X Chu,Z Chubinidze,J Chudoba,J J Chwastowski,D Cieri,K M Ciesla,V Cindro,A Ciocio,F Cirotto,Z H Citron,M Citterio,D A Ciubotaru,A Clark,P J Clark,N Clarke Hall,C Clarry,S E Clawson,C Clement,Y Coadou,M Cobal,A Coccaro,R F Coelho Barrue,R Coelho Lopes De Sa,S Coelli,L S Colangeli,B Cole,P Collado Soto,J Collot,R Coluccia,P Conde Muiño,M P Connell,S H Connell,E I Conroy,M Contreras Cossio,F Conventi,A M Cooper-Sarkar,L Corazzina,F A Corchia,A Cordeiro Oudot Choi,L D Corpe,M Corradi,F Corriveau,A Cortes-Gonzalez,M J Costa,F Costanza,D Costanzo,J Couthures,G Cowan,K Cranmer,L Cremer,D Cremonini,S Crépé-Renaudin,F Crescioli,T Cresta,M Cristinziani,M Cristoforetti,E Critelli,V Croft,G Crosetti,A Cueto,H Cui,Z Cui,B M Cunnett,W R Cunningham,F Curcio,J R Curran,M J Da Cunha Sargedas De Sousa,J V Da Fonseca Pinto,C Da Via,W Dabrowski,T Dado,S Dahbi,T Dai,D Dal Santo,C Dallapiccola,M Dam,G D'amen,V D'Amico,J Damp,J R Dandoy,M D'Andrea,D Dannheim,G D'anniballe,M Danninger,V Dao,G Darbo,R O Darragh,S J Das,F Dattola,S D'Auria,A D'Avanzo,T Davidek,J Davidson,I Dawson,K De,C De Almeida Rossi,R De Asmundis,N De Biase,S De Castro,N De Groot,P de Jong,H De la Torre,A De Maria,A De Salvo,U De Sanctis,F De Santis,A De Santo,J B De Vivie De Regie,J Debevc,D V Dedovich,J Degens,A M Deiana,J Del Peso,L Delagrange,F Deliot,C M Delitzsch,M Della Pietra,D Della Volpe,A Dell'Acqua,L Dell'Asta,M Delmastro,C C Delogu,P A Delsart,S Demers,M Demichev,S P Denisov,H Denizli,L D'Eramo,D Derendarz,F Derue,P Dervan,A M Desai,K Desch,F A Di Bello,A Di Ciaccio,L Di Ciaccio,A Di Domenico,C Di Donato,A Di Girolamo,G Di Gregorio,A Di Luca,B Di Micco,R Di Nardo,K F Di Petrillo,M Diamantopoulou,F A Dias,M A Diaz,A R Didenko,M Didenko,S D Diefenbacher,E B Diehl,S Díez Cornell,C Diez Pardos,C Dimitriadi,A Dimitrievska,A Dimri,Y Ding,J Dingfelder,T Dingley,I-M Dinu,S J Dittmeier,F Dittus,M Divisek,B Dixit,F Djama,T Djobava,C Doglioni,A Dohnalova,Z Dolezal,K Domijan,K M Dona,M Donadelli,B Dong,J Donini,A D'Onofrio,M D'Onofrio,J Dopke,A Doria,N Dos Santos Fernandes,I A Dos Santos Luz,P Dougan,M T Dova,A T Doyle,M P Drescher,E Dreyer,I Drivas-Koulouris,M Drnevich,D Du,T A du Pree,Z Duan,M Dubau,F Dubinin,M Dubovsky,E Duchovni,G Duckeck,P K Duckett,O A Ducu,D Duda,A Dudarev,M M Dudek,E R Duden,M D'uffizi,L Duflot,M Dührssen,I Duminica,A E Dumitriu,M Dunford,K Dunne,A Duperrin,H Duran Yildiz,A Durglishvili,G I Dyckes,M Dyndal,B S Dziedzic,Z O Earnshaw,G H Eberwein,B Eckerova,S Eggebrecht,E Egidio Purcino De Souza,G Eigen,K Einsweiler,T Ekelof,P A Ekman,S El Farkh,Y El Ghazali,H El Jarrari,A El Moussaouy,D Elitez,M Ellert,F Ellinghaus,T A Elliot,N Ellis,J Elmsheuser,M Elsawy,M Elsing,D Emeliyanov,Y Enari,S Epari,D Ernani Martins Neto,F Ernst,M Errenst,M Escalier,C Escobar,E Etzion,G Evans,H Evans,L S Evans,A Ezhilov,S Ezzarqtouni,F Fabbri,L Fabbri,G Facini,V Fadeyev,R M Fakhrutdinov,D Fakoudis,S Falciano,L F Falda Ulhoa Coelho,F Fallavollita,G Falsetti,J Faltova,C Fan,K Y Fan,Y Fan,Y Fang,M Fanti,M Faraj,Z Farazpay,A Farbin,A Farilla,K Farman,T Farooque,J N Farr,S M Farrington,F Fassi,D Fassouliotis,L Fayard,P Federic,P Federicova,O L Fedin,M Feickert,L Feligioni,D E Fellers,C Feng,Y Feng,Z Feng,M J Fenton,L Ferencz,B Fernandez Barbadillo,P Fernandez Martinez,M J V Fernoux,J Ferrando,A Ferrari,P Ferrari,R Ferrari,D Ferrere,C Ferretti,M P Fewell,D Fiacco,F Fiedler,P Fiedler,S Filimonov,M S Filip,A Filipčič,E K Filmer,F Filthaut,M C N Fiolhais,L Fiorini,W C Fisher,T Fitschen,P M Fitzhugh,I Fleck,P Fleischmann,T Flick,M Flores,L R Flores Castillo,L Flores Sanz De Acedo,F M Follega,N Fomin,J H Foo,A Formica,A C Forti,E Fortin,A W Fortman,L Foster,L 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Yardley,J Ye,S Ye,X Ye,Y Yeh,I Yeletskikh,B Yeo,M R Yexley,T P Yildirim,K Yorita,C J S Young,C Young,N D Young,Y Yu,J Yuan,M Yuan,R Yuan,L Yue,M Zaazoua,B Zabinski,I Zahir,A Zaio,Z K Zak,T Zakareishvili,S Zambito,J A Zamora Saa,J Zang,R Zanzottera,O Zaplatilek,C Zeitnitz,H Zeng,J C Zeng,D T Zenger,O Zenin,T Ženiš,S Zenz,D Zerwas,M Zhai,D F Zhang,G Zhang,J Zhang,J Zhang,K Zhang,L Zhang,L Zhang,P Zhang,R Zhang,S Zhang,T Zhang,Y Zhang,Y Zhang,Y Zhang,Y Zhang,Z Zhang,Z Zhang,Z Zhang,H Zhao,T Zhao,Y Zhao,Z Zhao,Z Zhao,A Zhemchugov,J Zheng,K Zheng,L Zheng,X Zheng,Z Zheng,D Zhong,B Zhou,H Zhou,N Zhou,Y Zhou,Y Zhou,Y Zhou,C G Zhu,J Zhu,X Zhu,Y Zhu,Y Zhu,X Zhuang,K Zhukov,N I Zimine,J Zinsser,M Ziolkowski,L Živković,A Zoccoli,K Zoch,A Zografos,T G Zorbas,O Zormpa,L Zwalinski,
A search for the dimuon decay of the Higgs boson is presented based on pp collision data recorded by ATLAS during Run 3 of the Large Hadron Collider, corresponding to an integrated luminosity of 165 fb^{-1} at sqrt[s]=13.6 TeV. To enhance the sensitivity, the results are combined with those from Run 2. An excess of events over the background is observed with a significance of 3.4σ (2.5σ expected). The best-fit signal strength is μ=1.4±0.4. This result provides evidence for the H→μμ decay with ATLAS data and offers a direct probe of the Higgs-boson Yukawa coupling to second-generation fermions.
基于ATLAS在大型强子对撞机第3次运行期间记录的pp碰撞数据，提出了对希格斯玻色子的次介子衰变的搜索，对应的积分光度为165 fb^{-1} at sqrt[s]=13.6 TeV。为了提高灵敏度，将结果与Run 2的结果相结合。观测到事件在背景上的过剩，显著性为3.4σ（预期为2.5σ）。最佳拟合信号强度为μ=1.4±0.4。这一结果为用ATLAS数据证明H→μμ衰变提供了证据，并提供了对希格斯-玻色子汤川耦合到第二代费米子的直接探测。
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Plotnikova,G Poddar,R Poettgen,L Poggioli,S Polacek,G Polesello,A Poley,A Polini,C S Pollard,Z B Pollock,E Pompa Pacchi,N I Pond,D Ponomarenko,L Pontecorvo,S Popa,G A Popeneciu,A Poreba,D M Portillo Quintero,S Pospisil,M A Postill,P Postolache,K Potamianos,P A Potepa,I N Potrap,C J Potter,H Potti,J Poveda,M E Pozo Astigarraga,R Pozzi,A Prades Ibanez,S R Pradhan,J Pretel,D Price,M Primavera,L Primomo,M A Principe Martin,R Privara,T Procter,M L Proffitt,N Proklova,K Prokofiev,G Proto,J Proudfoot,M Przybycien,W W Przygoda,A Psallidas,J E Puddefoot,D Pudzha,H I Purnell,D Pyatiizbyantseva,J Qian,R Qian,D Qichen,Y Qin,T Qiu,A Quadt,M Queitsch-Maitland,G Quetant,R P Quinn,G Rabanal Bolanos,D Rafanoharana,F Raffaeli,F Ragusa,J L Rainbolt,S Rajagopalan,E Ramakoti,L Rambelli,I A Ramirez-Berend,K Ran,D S Rankin,N P Rapheeha,H Rasheed,D F Rassloff,A Rastogi,S Rave,S Ravera,B Ravina,I Ravinovich,M Raymond,A L Read,N P Readioff,D M Rebuzzi,A S Reed,K Reeves,J A Reidelsturz,D Reikher,A Rej,C Rembser,H Ren,M Renda,F Renner,A G Rennie,M Repik,A L Rescia,S Resconi,M Ressegotti,S Rettie,W F Rettie,M M Revering,E Reynolds,O L Rezanova,P Reznicek,H Riani,N Ribaric,B Ricci,E Ricci,R Richter,S Richter,E Richter-Was,M Ridel,S Ridouani,P Rieck,P Riedler,E M Riefel,J O Rieger,M Rijssenbeek,M Rimoldi,L Rinaldi,P Rincke,G Ripellino,I Riu,J C Rivera Vergara,F Rizatdinova,E Rizvi,B R Roberts,S S Roberts,D Robinson,M Robles Manzano,A Robson,A Rocchi,C Roda,S Rodriguez Bosca,Y Rodriguez Garcia,A M Rodríguez Vera,S Roe,J T Roemer,O Røhne,R A Rojas,C P A Roland,A Romaniouk,E Romano,M Romano,A C Romero Hernandez,N Rompotis,L Roos,S Rosati,B J Rosser,E Rossi,E Rossi,L P Rossi,L Rossini,R Rosten,M Rotaru,B Rottler,D Rousseau,D Rousso,S Roy-Garand,A Rozanov,Z M A Rozario,Y Rozen,A Rubio Jimenez,V H Ruelas Rivera,T A Ruggeri,A Ruggiero,A Ruiz-Martinez,A Rummler,Z Rurikova,N A Rusakovich,S Ruscelli,H L Russell,G Russo,J P Rutherfoord,S Rutherford Colmenares,M Rybar,P Rybczynski,A Ryzhov,J A Sabater Iglesias,H F-W Sadrozinski,F Safai Tehrani,S Saha,M Sahinsoy,B Sahoo,A Saibel,B T Saifuddin,M Saimpert,G T Saito,M Saito,T Saito,A Sala,A Salnikov,J Salt,A Salvador Salas,F Salvatore,A Salzburger,D Sammel,E Sampson,D Sampsonidis,D Sampsonidou,M A A Samy,J Sánchez,V Sanchez Sebastian,H Sandaker,C O Sander,J A Sandesara,M Sandhoff,C Sandoval,L Sanfilippo,D P C Sankey,T Sano,A Sansoni,M Santana Queiroz,L Santi,C Santoni,H Santos,A Santra,E Sanzani,K A Saoucha,J G Saraiva,J Sardain,O Sasaki,K Sato,C Sauer,E Sauvan,P Savard,R Sawada,C Sawyer,L Sawyer,C Sbarra,A Sbrizzi,T Scanlon,J Schaarschmidt,U Schäfer,A C Schaffer,D Schaile,R D Schamberger,C Scharf,M M Schefer,V A Schegelsky,D Scheirich,M Schernau,C Scheulen,C Schiavi,M Schioppa,B Schlag,S Schlenker,J Schmeing,E Schmidt,M A Schmidt,K Schmieden,C Schmitt,N Schmitt,S Schmitt,N A Schneider,L Schoeffel,A Schoening,P G Scholer,E Schopf,M Schott,S Schramm,T Schroer,H-C Schultz-Coulon,M Schumacher,B A Schumm,Ph Schune,H R Schwartz,A Schwartzman,T A Schwarz,Ph Schwemling,R Schwienhorst,F G Sciacca,A Sciandra,G Sciolla,F Scuri,C D Sebastiani,K Sedlaczek,S C Seidel,A Seiden,B D Seidlitz,C Seitz,J M Seixas,G Sekhniaidze,L Selem,N Semprini-Cesari,A Semushin,D Sengupta,V Senthilkumar,L Serin,M Sessa,H Severini,F Sforza,A Sfyrla,Q Sha,E Shabalina,H Shaddix,A H Shah,R Shaheen,J D Shahinian,M Shamim,L Y Shan,M Shapiro,A Sharma,A S Sharma,P Sharma,P B Shatalov,K Shaw,S M Shaw,Q Shen,D J Sheppard,P Sherwood,L Shi,X Shi,S Shimizu,C O Shimmin,I P J Shipsey,S Shirabe,M Shiyakova,M J Shochet,D R Shope,B Shrestha,S Shrestha,I Shreyber,M J Shroff,P Sicho,A M Sickles,E Sideras Haddad,A C Sidley,A Sidoti,F Siegert,Dj Sijacki,F Sili,J M Silva,I Silva Ferreira,M V Silva Oliveira,S B Silverstein,S Simion,R Simoniello,E L Simpson,H Simpson,L R Simpson,S Simsek,S Sindhu,P Sinervo,S N Singh,S Singh,S Sinha,S Sinha,M Sioli,K Sioulas,I Siral,E Sitnikova,J Sjölin,A Skaf,E Skorda,P Skubic,M Slawinska,I Slazyk,I Sliusar,V Smakhtin,B H Smart,S Yu Smirnov,Y Smirnov,L N Smirnova,O Smirnova,A C Smith,D R Smith,J L Smith,M B Smith,R Smith,H Smitmanns,M Smizanska,K Smolek,P Smolyanskiy,A A Snesarev,H L Snoek,S Snyder,R Sobie,A Soffer,C A Solans Sanchez,E Yu Soldatov,U Soldevila,A A Solodkov,S Solomon,A Soloshenko,K Solovieva,O V Solovyanov,P Sommer,A Sonay,A Sopczak,A L Sopio,F Sopkova,J D Sorenson,I R Sotarriva Alvarez,V Sothilingam,O J Soto Sandoval,S Sottocornola,R Soualah,Z Soumaimi,D South,N Soybelman,S Spagnolo,M Spalla,D Sperlich,B Spisso,D P Spiteri,L Splendori,M Spousta,E J Staats,R Stamen,E Stanecka,W Stanek-Maslouska,M V Stange,B Stanislaus,M M Stanitzki,B Stapf,E A Starchenko,G H Stark,J Stark,P Staroba,P Starovoitov,R Staszewski,C Stauch,G Stavropoulos,A Stefl,A Stein,P Steinberg,B Stelzer,H J Stelzer,O Stelzer,H Stenzel,T J Stevenson,G A Stewart,J R Stewart,G Stoicea,M Stolarski,S Stonjek,A Straessner,J Strandberg,S Strandberg,M Stratmann,M Strauss,T Strebler,P Strizenec,R Ströhmer,D M Strom,R Stroynowski,A Strubig,S A Stucci,B Stugu,J Stupak,N A Styles,D Su,S Su,X Su,D Suchy,A D Sudhakar Ponnu,K Sugizaki,V V Sulin,D M S Sultan,L Sultanaliyeva,S Sultansoy,S Sun,W Sun,N Sur,M R Sutton,M Svatos,P N Swallow,M Swiatlowski,T Swirski,A Swoboda,I Sykora,M Sykora,T Sykora,D Ta,K Tackmann,A Taffard,R Tafirout,Y Takubo,M Talby,A A Talyshev,K C Tam,N M Tamir,A Tanaka,J Tanaka,R Tanaka,M Tanasini,Z Tao,S Tapia Araya,S Tapprogge,A Tarek Abouelfadl Mohamed,S Tarem,K Tariq,G Tarna,G F Tartarelli,M J Tartarin,P Tas,M Tasevsky,E Tassi,A C Tate,Y Tayalati,G N Taylor,W Taylor,R J Taylor Vara,A S Tegetmeier,P Teixeira-Dias,J J Teoh,K Terashi,J Terron,S Terzo,M Testa,R J Teuscher,A Thaler,O Theiner,T Theveneaux-Pelzer,D W Thomas,J P Thomas,E A Thompson,P D Thompson,E Thomson,R E Thornberry,C Tian,Y Tian,V Tikhomirov,Yu A Tikhonov,S Timoshenko,D Timoshyn,E X L Ting,P Tipton,A Tishelman-Charny,K Todome,S Todorova-Nova,L Toffolin,M Togawa,J Tojo,S Tokár,O Toldaiev,G Tolkachev,M Tomoto,L Tompkins,E Torrence,H Torres,D I Torres Arza,E Torró Pastor,M Toscani,C Tosciri,M Tost,D R Tovey,T Trefzger,P M Tricarico,A Tricoli,I M Trigger,S Trincaz-Duvoid,D A Trischuk,A Tropina,L Truong,M Trzebinski,A Trzupek,F Tsai,M Tsai,A Tsiamis,P V Tsiareshka,S Tsigaridas,A Tsirigotis,V Tsiskaridze,E G Tskhadadze,Y Tsujikawa,I I Tsukerman,V Tsulaia,S Tsuno,K Tsuri,D Tsybychev,Y Tu,A Tudorache,V Tudorache,S B Tuncay,S Turchikhin,I Turk Cakir,R Turra,T Turtuvshin,P M Tuts,S Tzamarias,Y Uematsu,F Ukegawa,P A Ulloa Poblete,E N Umaka,G Unal,A Undrus,G Unel,J Urban,P Urrejola,G Usai,R Ushioda,M Usman,F Ustuner,Z Uysal,V Vacek,B Vachon,T Vafeiadis,A Vaitkus,C Valderanis,E Valdes Santurio,M Valente,S Valentinetti,A Valero,E Valiente Moreno,A Vallier,J A Valls Ferrer,D R Van Arneman,A Van Der Graaf,H Z Van Der Schyf,P Van Gemmeren,M Van Rijnbach,S Van Stroud,I Van Vulpen,P Vana,M Vanadia,U M Vande Voorde,W Vandelli,E R Vandewall,D Vannicola,L Vannoli,R Vari,M Varma,E W Varnes,C Varni,D Varouchas,L Varriale,K E Varvell,M E Vasile,L Vaslin,M D Vassilev,A Vasyukov,L M Vaughan,R Vavricka,T Vazquez Schroeder,J Veatch,V Vecchio,M J Veen,I Veliscek,I Velkovska,L M Veloce,F Veloso,S Veneziano,A Ventura,A Verbytskyi,M Verducci,C Vergis,M Verissimo De Araujo,W Verkerke,J C Vermeulen,C Vernieri,M Vessella,M C Vetterli,A Vgenopoulos,N Viaux Maira,T Vickey,O E Vickey Boeriu,G H A Viehhauser,L Vigani,M Vigl,M Villa,M Villaplana Perez,E M Villhauer,E Vilucchi,M Vincent,M G Vincter,A Visibile,A Visive,C Vittori,I Vivarelli,M I Vivas Albornoz,E Voevodina,F Vogel,J C Voigt,P Vokac,Yu Volkotrub,L Vomberg,E Von Toerne,B Vormwald,K Vorobev,M Vos,K Voss,M Vozak,L Vozdecky,N Vranjes,M Vranjes Milosavljevic,M Vreeswijk,N K Vu,R Vuillermet,O Vujinovic,I Vukotic,I K Vyas,J F Wack,A Wada,S Wada,C Wagner,J M Wagner,W Wagner,S Wahdan,H Wahlberg,C H Waits,J Walder,R Walker,K Walkingshaw Pass,W Walkowiak,A Wall,E J Wallin,T Wamorkar,K Wandall-Christensen,A Wang,A Z Wang,C Wang,C Wang,H Wang,J Wang,P Wang,P Wang,R Wang,R Wang,S M Wang,S Wang,T Wang,T Wang,W T Wang,W Wang,X Wang,X Wang,X Wang,Y Wang,Y Wang,Z Wang,Z Wang,Z Wang,C Wanotayaroj,A Warburton,A L Warnerbring,S Waterhouse,A T Watson,H Watson,M F Watson,E Watton,G Watts,B M Waugh,J M Webb,C Weber,H A Weber,M S Weber,S M Weber,C Wei,Y Wei,A R Weidberg,E J Weik,J Weingarten,C Weiser,C J Wells,T Wenaus,T Wengler,N S Wenke,N Wermes,M Wessels,A M Wharton,A S White,A White,M J White,D Whiteson,L Wickremasinghe,W Wiedenmann,M Wielers,R Wierda,C Wiglesworth,H G Wilkens,J J H Wilkinson,D M Williams,H H Williams,S Williams,S Willocq,B J Wilson,D J Wilson,P J Windischhofer,F I Winkel,F Winklmeier,B T Winter,M Wittgen,M Wobisch,T Wojtkowski,Z Wolffs,J Wollrath,M W Wolter,H Wolters,M C Wong,E L Woodward,S D Worm,B K Wosiek,K W Woźniak,S Wozniewski,K Wraight,C Wu,C Wu,J Wu,M Wu,M Wu,S L Wu,S Wu,X Wu,Y Q Wu,Y Wu,Z Wu,Z Wu,J Wuerzinger,T R Wyatt,B M Wynne,S Xella,L Xia,M Xie,A Xiong,D Xu,H Xu,L Xu,R Xu,T Xu,Y Xu,Z Xu,R Xue,B Yabsley,S Yacoob,Y Yamaguchi,E Yamashita,H Yamauchi,T Yamazaki,Y Yamazaki,S Yan,Z Yan,H J Yang,H T Yang,S Yang,T Yang,X Yang,X Yang,Y Yang,Y Yang,W-M Yao,C L Yardley,J Ye,S Ye,X Ye,Y Yeh,I Yeletskikh,B Yeo,M R Yexley,T P Yildirim,K Yorita,C J S Young,C Young,N D Young,Y Yu,J Yuan,M Yuan,R Yuan,L Yue,M Zaazoua,B Zabinski,I Zahir,A Zaio,Z K Zak,T Zakareishvili,S Zambito,J A Zamora Saa,J Zang,R Zanzottera,O Zaplatilek,C Zeitnitz,H Zeng,J C Zeng,D T Zenger,O Zenin,T Ženiš,S Zenz,D Zerwas,M Zhai,D F Zhang,G Zhang,J Zhang,J Zhang,K Zhang,L Zhang,L Zhang,P Zhang,R Zhang,S Zhang,T Zhang,Y Zhang,Y Zhang,Y Zhang,Y Zhang,Z Zhang,Z Zhang,Z Zhang,H Zhao,T Zhao,Y Zhao,Z Zhao,Z Zhao,A Zhemchugov,J Zheng,K Zheng,L Zheng,X Zheng,Z Zheng,D Zhong,B Zhou,H Zhou,N Zhou,Y Zhou,Y Zhou,Y Zhou,C G Zhu,J Zhu,X Zhu,Y Zhu,Y Zhu,X Zhuang,K Zhukov,N I Zimine,J Zinsser,M Ziolkowski,L Živković,A Zoccoli,K Zoch,A Zografos,T G Zorbas,O Zormpa,L Zwalinski, ","doi":"10.1103/gzdh-p159","DOIUrl":"https://doi.org/10.1103/gzdh-p159","url":null,"abstract":"A search for the dimuon decay of the Higgs boson is presented based on pp collision data recorded by ATLAS during Run 3 of the Large Hadron Collider, corresponding to an integrated luminosity of 165 fb^{-1} at sqrt[s]=13.6 TeV. To enhance the sensitivity, the results are combined with those from Run 2. An excess of events over the background is observed with a significance of 3.4σ (2.5σ expected). The best-fit signal strength is μ=1.4±0.4. This result provides evidence for the H→μμ decay with ATLAS data and offers a direct probe of the Higgs-boson Yukawa coupling to second-generation fermions.","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"29 1","pages":"231802"},"PeriodicalIF":8.6,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145785870","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Relaxed quantum systems with conservation laws are believed to be approximated by the generalized Gibbs ensemble (GGE), which incorporates the constraints of certain conserved quantities serving as integrals of motion. By drawing an analogy between eigenstate reduced density matrix and GGE, we conjecture that a natural set of conserved quantities for GGE can emerge from the reduced density matrices of properly chosen eigenstates by the entanglement Hamiltonian superdensity matrix (EHSM) framework, and we demonstrate this explicitly for models mappable to free fermions. The framework proposes that such conserved quantities are linear superpositions of eigenstate entanglement Hamiltonians of a larger auxiliary system, where the eigenstates are Fock states occupying what we call the common eigenmodes, which remain eigenmodes when truncated within the physical subsystem. For 1D homogeneous free fermions with (anti)periodic boundary conditions, which maps to 1D hardcore bosons with nearest neighbor hoppings, these conserved quantities lead to a non-Abelian GGE, which predicts the relaxation of both fermion and boson bilinears more accurately than the conventional Abelian GGE. Generalization of this framework may provide novel numerical insights for quantum integrability.
{"title":"Generalized Gibbs Ensemble from Eigenstate Entanglement Hamiltonian.","authors":"Hao Chen,Biao Lian","doi":"10.1103/dn82-y159","DOIUrl":"https://doi.org/10.1103/dn82-y159","url":null,"abstract":"Relaxed quantum systems with conservation laws are believed to be approximated by the generalized Gibbs ensemble (GGE), which incorporates the constraints of certain conserved quantities serving as integrals of motion. By drawing an analogy between eigenstate reduced density matrix and GGE, we conjecture that a natural set of conserved quantities for GGE can emerge from the reduced density matrices of properly chosen eigenstates by the entanglement Hamiltonian superdensity matrix (EHSM) framework, and we demonstrate this explicitly for models mappable to free fermions. The framework proposes that such conserved quantities are linear superpositions of eigenstate entanglement Hamiltonians of a larger auxiliary system, where the eigenstates are Fock states occupying what we call the common eigenmodes, which remain eigenmodes when truncated within the physical subsystem. For 1D homogeneous free fermions with (anti)periodic boundary conditions, which maps to 1D hardcore bosons with nearest neighbor hoppings, these conserved quantities lead to a non-Abelian GGE, which predicts the relaxation of both fermion and boson bilinears more accurately than the conventional Abelian GGE. Generalization of this framework may provide novel numerical insights for quantum integrability.","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"4 1","pages":"233402"},"PeriodicalIF":8.6,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145785874","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Lisa Bombieri, Torsten V Zache, Gabriele Calliari, Mikhail D Lukin, Hannes Pichler, Daniel González-Cuadra
Fluctuations can drive continuous phase transitions between two distinct ordered phases-so-called deconfined quantum critical points (DQCPs)-which lie beyond the Landau-Ginzburg-Wilson paradigm. Despite several theoretical predictions over the past decades, experimental evidence of DQCPs remains elusive. We show that a DQCP can be explored in a system of Rydberg atoms arranged on a triangular lattice and coupled through van der Waals interactions. Specifically, we investigate the nature of the phase transition between two ordered phases at 1/3 and 2/3 Rydberg excitation density, which were recently probed experimentally in [Scholl et al., Quantum simulation of 2D antiferromagnets with hundreds of Rydberg atoms, Nature (London) 595, 233 (2021).NATUAS0028-083610.1038/s41586-021-03585-1]. Using a field-theoretical analysis, we predict both the critical exponents for infinitely long cylinders of increasing circumference and the emergence of a conformal field theory near criticality showing an enlarged U(1) symmetry-a signature of DQCPs-and confirm these predictions numerically. Finally, we extend these results to ladder geometries and show how the emergent U(1) symmetry could be probed experimentally using finite tweezer arrays.
{"title":"Deconfined Quantum Criticality on a Triangular Rydberg Array.","authors":"Lisa Bombieri, Torsten V Zache, Gabriele Calliari, Mikhail D Lukin, Hannes Pichler, Daniel González-Cuadra","doi":"10.1103/4rg4-zbnn","DOIUrl":"https://doi.org/10.1103/4rg4-zbnn","url":null,"abstract":"<p><p>Fluctuations can drive continuous phase transitions between two distinct ordered phases-so-called deconfined quantum critical points (DQCPs)-which lie beyond the Landau-Ginzburg-Wilson paradigm. Despite several theoretical predictions over the past decades, experimental evidence of DQCPs remains elusive. We show that a DQCP can be explored in a system of Rydberg atoms arranged on a triangular lattice and coupled through van der Waals interactions. Specifically, we investigate the nature of the phase transition between two ordered phases at 1/3 and 2/3 Rydberg excitation density, which were recently probed experimentally in [Scholl et al., Quantum simulation of 2D antiferromagnets with hundreds of Rydberg atoms, Nature (London) 595, 233 (2021).NATUAS0028-083610.1038/s41586-021-03585-1]. Using a field-theoretical analysis, we predict both the critical exponents for infinitely long cylinders of increasing circumference and the emergence of a conformal field theory near criticality showing an enlarged U(1) symmetry-a signature of DQCPs-and confirm these predictions numerically. Finally, we extend these results to ladder geometries and show how the emergent U(1) symmetry could be probed experimentally using finite tweezer arrays.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"135 23","pages":"233602"},"PeriodicalIF":9.0,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145794425","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
We develop a Fermi liquid theory of d-wave altermagnets and apply it to describe their collective excitation spectrum. We predict that in addition to a conventional undamped plasmon mode, where both spin components oscillate in phase, there is an acoustic plasmon (or demon) mode with out-of-phase spin dynamics. By analyzing the dynamical structure factor, we reveal a strong dependence of the demon's frequency and spectral weight both on the Landau parameters and on the direction of propagation. Notably, as a function of the propagation angle, we show that the acoustic mode evolves from a hidden state, which has zero spectral weight in the density excitation spectrum, to a weakly damped propagating demon mode and then (below a critical interaction parameter) to a Fano-demon mixed state, which is marked by a strong hybridization with particle-hole excitations and a corresponding asymmetric line shape in the structure factor. Our Letter paves the way for applications of altermagnetic materials in optospintronics by harnessing collective electron spin oscillations beyond traditional magnon spin waves.
{"title":"Fermi Liquid Theory of d-Wave Altermagnets: Demon Modes and Fano-Demon States.","authors":"Habib Rostami, Johannes Hofmann","doi":"10.1103/zqz6-sq2n","DOIUrl":"https://doi.org/10.1103/zqz6-sq2n","url":null,"abstract":"<p><p>We develop a Fermi liquid theory of d-wave altermagnets and apply it to describe their collective excitation spectrum. We predict that in addition to a conventional undamped plasmon mode, where both spin components oscillate in phase, there is an acoustic plasmon (or demon) mode with out-of-phase spin dynamics. By analyzing the dynamical structure factor, we reveal a strong dependence of the demon's frequency and spectral weight both on the Landau parameters and on the direction of propagation. Notably, as a function of the propagation angle, we show that the acoustic mode evolves from a hidden state, which has zero spectral weight in the density excitation spectrum, to a weakly damped propagating demon mode and then (below a critical interaction parameter) to a Fano-demon mixed state, which is marked by a strong hybridization with particle-hole excitations and a corresponding asymmetric line shape in the structure factor. Our Letter paves the way for applications of altermagnetic materials in optospintronics by harnessing collective electron spin oscillations beyond traditional magnon spin waves.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"135 23","pages":"236701"},"PeriodicalIF":9.0,"publicationDate":"2025-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145794538","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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