Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.086704
H Arava, D Sanz-Hernandez, J Grollier, A K Petford-Long
A possible spintronic route to hardware implementation for decision-making involves injecting a domain wall into a bifurcated magnetic nanostrip resembling a Y-shaped junction. A decision is made when the domain wall chooses a particular path through the bifurcation. Recently, it was shown that a structure like a nanomagnetic Galton board, which is essentially an array of interconnected Y-shaped junctions, produces outcomes that are stochastic and therefore relevant to artificial neural networks. However, the exact mechanism leading to the robust nature of randomness is unknown. Here, we directly image the decision-making process in nanomagnetic Galton boards using Lorentz transmission electron microscopy. We identify that the stochasticity in nanomagnetic Galton boards arises as a culmination of (1) the topology of the injected domain wall, (2) dissimilarly sized vertices, and (3) the strength of the applied field. Our results pave the way to a detailed understanding of stochasticity in nanomagnetic networks.
实现决策硬件的一个可能的自旋电子途径是将一个域壁注入一个类似于 Y 型结点的分叉磁性纳米带。当域壁选择通过分叉的特定路径时,就会做出决策。最近的研究表明,像纳米磁性高尔顿板这样的结构(本质上是相互连接的 Y 型结点阵列)会产生随机结果,因此与人工神经网络相关。然而,导致随机性稳健性的确切机制尚不清楚。在这里,我们利用洛伦兹透射电子显微镜直接对纳米磁性高尔顿板的决策过程进行了成像。我们发现,纳米磁性高尔顿板中的随机性是由以下因素造成的:(1) 注入域壁的拓扑结构;(2) 大小不一的顶点;(3) 外加磁场的强度。我们的研究结果为详细了解纳米磁网络中的随机性铺平了道路。
{"title":"Real Space Imaging of Field-Driven Decision-Making in Nanomagnetic Galton Boards.","authors":"H Arava, D Sanz-Hernandez, J Grollier, A K Petford-Long","doi":"10.1103/PhysRevLett.134.086704","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.086704","url":null,"abstract":"<p><p>A possible spintronic route to hardware implementation for decision-making involves injecting a domain wall into a bifurcated magnetic nanostrip resembling a Y-shaped junction. A decision is made when the domain wall chooses a particular path through the bifurcation. Recently, it was shown that a structure like a nanomagnetic Galton board, which is essentially an array of interconnected Y-shaped junctions, produces outcomes that are stochastic and therefore relevant to artificial neural networks. However, the exact mechanism leading to the robust nature of randomness is unknown. Here, we directly image the decision-making process in nanomagnetic Galton boards using Lorentz transmission electron microscopy. We identify that the stochasticity in nanomagnetic Galton boards arises as a culmination of (1) the topology of the injected domain wall, (2) dissimilarly sized vertices, and (3) the strength of the applied field. Our results pave the way to a detailed understanding of stochasticity in nanomagnetic networks.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"086704"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630799","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.080401
Ken Funo, Hiroyasu Tajima
Symmetry imposes constraints on open quantum systems, affecting the dissipative properties in nonequilibrium processes. Superradiance is a typical example in which the decay rate of the system is enhanced via a collective system-bath coupling that respects permutation symmetry. Such a model has also been applied to heat engines. However, a generic framework that addresses the impact of symmetry in finite-time thermodynamics is not well established. Here, we show a symmetry-based framework that describes the fundamental limit of collective enhancement in finite-time thermodynamics. Specifically, we derive a general upper bound on the average jump rate, which quantifies the fundamental speed set by thermodynamic speed limits and trade-off relations. We identify the symmetry condition that achieves the obtained bound, and explicitly construct an open quantum system model that goes beyond the enhancement realized by the conventional superradiance model.
{"title":"Symmetry Induced Enhancement in Finite-Time Thermodynamic Trade-Off Relations.","authors":"Ken Funo, Hiroyasu Tajima","doi":"10.1103/PhysRevLett.134.080401","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.080401","url":null,"abstract":"<p><p>Symmetry imposes constraints on open quantum systems, affecting the dissipative properties in nonequilibrium processes. Superradiance is a typical example in which the decay rate of the system is enhanced via a collective system-bath coupling that respects permutation symmetry. Such a model has also been applied to heat engines. However, a generic framework that addresses the impact of symmetry in finite-time thermodynamics is not well established. Here, we show a symmetry-based framework that describes the fundamental limit of collective enhancement in finite-time thermodynamics. Specifically, we derive a general upper bound on the average jump rate, which quantifies the fundamental speed set by thermodynamic speed limits and trade-off relations. We identify the symmetry condition that achieves the obtained bound, and explicitly construct an open quantum system model that goes beyond the enhancement realized by the conventional superradiance model.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"080401"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630822","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.081003
Glennys R Farrar
We propose that ultrahigh energy cosmic rays (UHECRs) are produced in binary neutron star (BNS) mergers. This scenario can account for the heretofore inexplicable narrow rigidity range of UHECRs because the jets of BNS mergers are generated by a gravitationally driven dynamo and thus are nearly identical due to the narrow range of BNS masses. Observed UHECRs with energies well beyond 100 EeV can be explained as r-process nuclei, without invoking an exotic source class. Evidence for this mechanism, and its prediction of coincidences between neutrinos above 10 PeV and gravitational waves, are discussed.
{"title":"Binary Neutron Star Mergers as the Source of the Highest Energy Cosmic Rays.","authors":"Glennys R Farrar","doi":"10.1103/PhysRevLett.134.081003","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.081003","url":null,"abstract":"<p><p>We propose that ultrahigh energy cosmic rays (UHECRs) are produced in binary neutron star (BNS) mergers. This scenario can account for the heretofore inexplicable narrow rigidity range of UHECRs because the jets of BNS mergers are generated by a gravitationally driven dynamo and thus are nearly identical due to the narrow range of BNS masses. Observed UHECRs with energies well beyond 100 EeV can be explained as r-process nuclei, without invoking an exotic source class. Evidence for this mechanism, and its prediction of coincidences between neutrinos above 10 PeV and gravitational waves, are discussed.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"081003"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630393","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.086501
Sibei Li, Hui Shao, Anders W Sandvik
We study the Heisenberg S=1/2 chain with random ferro- and antiferromagnetic couplings using quantum Monte Carlo simulations at ultra-low temperatures, converging to the ground state. Finite-size scaling of correlation functions and excitation gaps demonstrate an exotic critical state in qualitative agreement with previous strong-disorder renormalization group calculations but with scaling exponents depending on the coupling distribution. We find dual scaling regimes of the transverse correlations versus the distance, with an L independent form C(r)=r^{-μ} for r≪L and C(r,L)=L^{-η}f(r/L) for r/L>0, where μ>η and the scaling function is delivered by our analysis. These results are at variance with previous spin-wave and density-matrix renormalization group calculations, thus highlighting the power of unbiased quantum Monte Carlo simulations.
{"title":"Ground State of the S=1/2 Heisenberg Spin Chain with Random Ferromagnetic and Antiferromagnetic Couplings.","authors":"Sibei Li, Hui Shao, Anders W Sandvik","doi":"10.1103/PhysRevLett.134.086501","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.086501","url":null,"abstract":"<p><p>We study the Heisenberg S=1/2 chain with random ferro- and antiferromagnetic couplings using quantum Monte Carlo simulations at ultra-low temperatures, converging to the ground state. Finite-size scaling of correlation functions and excitation gaps demonstrate an exotic critical state in qualitative agreement with previous strong-disorder renormalization group calculations but with scaling exponents depending on the coupling distribution. We find dual scaling regimes of the transverse correlations versus the distance, with an L independent form C(r)=r^{-μ} for r≪L and C(r,L)=L^{-η}f(r/L) for r/L>0, where μ>η and the scaling function is delivered by our analysis. These results are at variance with previous spin-wave and density-matrix renormalization group calculations, thus highlighting the power of unbiased quantum Monte Carlo simulations.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"086501"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630740","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.081002
Zhen Cao, F Aharonian, Axikegu, Y X Bai, Y W Bao, D Bastieri, X J Bi, Y J Bi, W Bian, A V Bukevich, Q Cao, W Y Cao, Zhe Cao, J Chang, J F Chang, A M Chen, E S Chen, H X Chen, Liang Chen, Lin Chen, Long Chen, M J Chen, M L Chen, Q H Chen, S Chen, S H Chen, S Z Chen, T L Chen, Y Chen, N Cheng, Y D Cheng, M C Chu, M Y Cui, S W Cui, X H Cui, Y D Cui, B Z Dai, H L Dai, Z G Dai, Danzengluobu, X Q Dong, K K Duan, J H Fan, Y Z Fan, J Fang, J H Fang, K Fang, C F Feng, H Feng, L Feng, S H Feng, X T Feng, Y Feng, Y L Feng, S Gabici, B Gao, C D Gao, Q Gao, W Gao, W K Gao, M M Ge, T T Ge, L S Geng, G Giacinti, G H Gong, Q B Gou, M H Gu, F L Guo, J Guo, X L Guo, Y Q Guo, Y Y Guo, Y A Han, O A Hannuksela, M Hasan, H H He, H N He, J Y He, Y He, Y K Hor, B W Hou, C Hou, X Hou, H B Hu, Q Hu, S C Hu, C Huang, D H Huang, T Q Huang, W J Huang, X T Huang, X Y Huang, Y Huang, Y Y Huang, X L Ji, H Y Jia, K Jia, H B Jiang, K Jiang, X W Jiang, Z J Jiang, M Jin, M M Kang, I Karpikov, D Khangulyan, D Kuleshov, K Kurinov, B B Li, C M Li, Cheng Li, Cong Li, D Li, F Li, H B Li, H C Li, Jian Li, Jie Li, K Li, S D Li, W L Li, W L Li, X R Li, Xin Li, Y Z Li, Zhe Li, Zhuo Li, E W Liang, Y F Liang, S J Lin, B Liu, C Liu, D Liu, D B Liu, H Liu, H D Liu, J Liu, J L Liu, M Y Liu, R Y Liu, S M Liu, W Liu, Y Liu, Y N Liu, Q Luo, Y Luo, H K Lv, B Q Ma, L L Ma, X H Ma, J R Mao, Z Min, W Mitthumsiri, H J Mu, Y C Nan, A Neronov, K C Y Ng, L J Ou, P Pattarakijwanich, Z Y Pei, J C Qi, M Y Qi, B Q Qiao, J J Qin, A Raza, D Ruffolo, A Sáiz, M Saeed, D Semikoz, L Shao, O Shchegolev, X D Sheng, F W Shu, H C Song, Yu V Stenkin, V Stepanov, Y Su, D X Sun, Q N Sun, X N Sun, Z B Sun, J Takata, P H T Tam, Q W Tang, R Tang, Z B Tang, W W Tian, L H Wan, C Wang, C B Wang, G W Wang, H G Wang, H H Wang, J C Wang, Kai Wang, Kai Wang, L P Wang, L Y Wang, P H Wang, R Wang, W Wang, X G Wang, X Y Wang, Y Wang, Y D Wang, Y J Wang, Z H Wang, Z X Wang, Zhen Wang, Zheng Wang, D M Wei, J J Wei, Y J Wei, T Wen, C Y Wu, H R Wu, Q W Wu, S Wu, X F Wu, Y S Wu, S Q Xi, J Xia, G M Xiang, D X Xiao, G Xiao, Y L Xin, Y Xing, D R Xiong, Z Xiong, D L Xu, R F Xu, R X Xu, W L Xu, L Xue, D H Yan, J Z Yan, T Yan, C W Yang, C Y Yang, F Yang, F F Yang, L L Yang, M J Yang, R Z Yang, W X Yang, Y H Yao, Z G Yao, L Q Yin, N Yin, X H You, Z Y You, Y H Yu, Q Yuan, H Yue, H D Zeng, T X Zeng, W Zeng, M Zha, B B Zhang, F Zhang, H Zhang, H M Zhang, H Y Zhang, J L Zhang, Li Zhang, P F Zhang, P P Zhang, R Zhang, S B Zhang, S R Zhang, S S Zhang, X Zhang, X P Zhang, Y F Zhang, Yi Zhang, Yong Zhang, B Zhao, J Zhao, L Zhao, L Z Zhao, S P Zhao, X H Zhao, F Zheng, W J Zhong, B Zhou, H Zhou, J N Zhou, M Zhou, P Zhou, R Zhou, X X Zhou, X X Zhou, B Y Zhu, C G Zhu, F R Zhu, H Zhu, K J Zhu, Y C Zou, X Zuo
The diffuse Galactic gamma-ray emission is a very important tool used to study the propagation and interaction of cosmic rays in the Milky Way. In this Letter, we report the measurements of the diffuse emission from the Galactic plane-covering Galactic longitudes from 15° to 235° and latitudes from -5° to +5°, in an energy range of 1 to 25 TeV-made with the Water Cherenkov Detector Array (WCDA) of the Large High Altitude Air Shower Observatory. After the sky regions of known sources are masked, the diffuse emission is detected with 24.6σ and 9.1σ significance in the inner Galactic plane (15°
{"title":"Measurement of Very-High-Energy Diffuse Gamma-Ray Emissions from the Galactic Plane with LHAASO-WCDA.","authors":"Zhen Cao, F Aharonian, Axikegu, Y X Bai, Y W Bao, D Bastieri, X J Bi, Y J Bi, W Bian, A V Bukevich, Q Cao, W Y Cao, Zhe Cao, J Chang, J F Chang, A M Chen, E S Chen, H X Chen, Liang Chen, Lin Chen, Long Chen, M J Chen, M L Chen, Q H Chen, S Chen, S H Chen, S Z Chen, T L Chen, Y Chen, N Cheng, Y D Cheng, M C Chu, M Y Cui, S W Cui, X H Cui, Y D Cui, B Z Dai, H L Dai, Z G Dai, Danzengluobu, X Q Dong, K K Duan, J H Fan, Y Z Fan, J Fang, J H Fang, K Fang, C F Feng, H Feng, L Feng, S H Feng, X T Feng, Y Feng, Y L Feng, S Gabici, B Gao, C D Gao, Q Gao, W Gao, W K Gao, M M Ge, T T Ge, L S Geng, G Giacinti, G H Gong, Q B Gou, M H Gu, F L Guo, J Guo, X L Guo, Y Q Guo, Y Y Guo, Y A Han, O A Hannuksela, M Hasan, H H He, H N He, J Y He, Y He, Y K Hor, B W Hou, C Hou, X Hou, H B Hu, Q Hu, S C Hu, C Huang, D H Huang, T Q Huang, W J Huang, X T Huang, X Y Huang, Y Huang, Y Y Huang, X L Ji, H Y Jia, K Jia, H B Jiang, K Jiang, X W Jiang, Z J Jiang, M Jin, M M Kang, I Karpikov, D Khangulyan, D Kuleshov, K Kurinov, B B Li, C M Li, Cheng Li, Cong Li, D Li, F Li, H B Li, H C Li, Jian Li, Jie Li, K Li, S D Li, W L Li, W L Li, X R Li, Xin Li, Y Z Li, Zhe Li, Zhuo Li, E W Liang, Y F Liang, S J Lin, B Liu, C Liu, D Liu, D B Liu, H Liu, H D Liu, J Liu, J L Liu, M Y Liu, R Y Liu, S M Liu, W Liu, Y Liu, Y N Liu, Q Luo, Y Luo, H K Lv, B Q Ma, L L Ma, X H Ma, J R Mao, Z Min, W Mitthumsiri, H J Mu, Y C Nan, A Neronov, K C Y Ng, L J Ou, P Pattarakijwanich, Z Y Pei, J C Qi, M Y Qi, B Q Qiao, J J Qin, A Raza, D Ruffolo, A Sáiz, M Saeed, D Semikoz, L Shao, O Shchegolev, X D Sheng, F W Shu, H C Song, Yu V Stenkin, V Stepanov, Y Su, D X Sun, Q N Sun, X N Sun, Z B Sun, J Takata, P H T Tam, Q W Tang, R Tang, Z B Tang, W W Tian, L H Wan, C Wang, C B Wang, G W Wang, H G Wang, H H Wang, J C Wang, Kai Wang, Kai Wang, L P Wang, L Y Wang, P H Wang, R Wang, W Wang, X G Wang, X Y Wang, Y Wang, Y D Wang, Y J Wang, Z H Wang, Z X Wang, Zhen Wang, Zheng Wang, D M Wei, J J Wei, Y J Wei, T Wen, C Y Wu, H R Wu, Q W Wu, S Wu, X F Wu, Y S Wu, S Q Xi, J Xia, G M Xiang, D X Xiao, G Xiao, Y L Xin, Y Xing, D R Xiong, Z Xiong, D L Xu, R F Xu, R X Xu, W L Xu, L Xue, D H Yan, J Z Yan, T Yan, C W Yang, C Y Yang, F Yang, F F Yang, L L Yang, M J Yang, R Z Yang, W X Yang, Y H Yao, Z G Yao, L Q Yin, N Yin, X H You, Z Y You, Y H Yu, Q Yuan, H Yue, H D Zeng, T X Zeng, W Zeng, M Zha, B B Zhang, F Zhang, H Zhang, H M Zhang, H Y Zhang, J L Zhang, Li Zhang, P F Zhang, P P Zhang, R Zhang, S B Zhang, S R Zhang, S S Zhang, X Zhang, X P Zhang, Y F Zhang, Yi Zhang, Yong Zhang, B Zhao, J Zhao, L Zhao, L Z Zhao, S P Zhao, X H Zhao, F Zheng, W J Zhong, B Zhou, H Zhou, J N Zhou, M Zhou, P Zhou, R Zhou, X X Zhou, X X Zhou, B Y Zhu, C G Zhu, F R Zhu, H Zhu, K J Zhu, Y C Zou, X Zuo","doi":"10.1103/PhysRevLett.134.081002","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.081002","url":null,"abstract":"<p><p>The diffuse Galactic gamma-ray emission is a very important tool used to study the propagation and interaction of cosmic rays in the Milky Way. In this Letter, we report the measurements of the diffuse emission from the Galactic plane-covering Galactic longitudes from 15° to 235° and latitudes from -5° to +5°, in an energy range of 1 to 25 TeV-made with the Water Cherenkov Detector Array (WCDA) of the Large High Altitude Air Shower Observatory. After the sky regions of known sources are masked, the diffuse emission is detected with 24.6σ and 9.1σ significance in the inner Galactic plane (15°<l<125°, |b|<5°) and outer Galactic plane (125°<l<235°, |b|<5°), respectively. The WCDA spectra in both regions can be well described by a power-law function, with spectral indices of -2.67±0.05_{stat} in the inner region and -2.83±0.19_{stat} in the outer region, respectively. Combined with the Square Kilometer Array (KM2A) measurements at higher energies, a clear softening of the spectrum is found in the inner region, with change of spectral indices by ∼0.5 at a break energy around 30 TeV. The fluxes of the diffuse emission are higher by a factor of 1.5-2.7 than the model prediction assuming local cosmic ray spectra and the gas column density, which are consistent with those measured by the KM2A. Along the Galactic longitude, the spatial distribution of the diffuse emission shows deviation from that of the gas column density. The spectral shape of the diffuse emission may vary in different longitude regions. The WCDA measurements bridge the gap between the low-energy measurements by space detectors and the ultra-high-energy observations by KM2A and other experiments. These results suggest that improved modeling of the wideband diffuse emission is required.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"081002"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630776","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.088201
Robert G Felsted, Jaehun Chun, Gregory K Schenter, Alexander B Bard, Xiaojing Xia, Peter J Pauzauskie
Rigorous understanding of assembly in colloidal systems is crucial to the development of tailored nanostructured materials. Despite extensive studies, a mechanistic understanding of the dynamics governing encounters of colloidal particles remains an ongoing challenge. We study colloidal encounter dynamics by inducing assembly through optical tweezers that impose an external attractive field for cubic-phase sodium yttrium fluoride nanocrystals. We show that surface roughness of the nanocrystals is a decisive factor for contact leading to assembly between the nanocrystals, manifested by the roughness-dependent hydrodynamic resistivity. This provides direct evidence that dynamics are equally important to energetics in understanding assembly.
{"title":"Mediation of Colloidal Encounter Dynamics by Surface Roughness.","authors":"Robert G Felsted, Jaehun Chun, Gregory K Schenter, Alexander B Bard, Xiaojing Xia, Peter J Pauzauskie","doi":"10.1103/PhysRevLett.134.088201","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.088201","url":null,"abstract":"<p><p>Rigorous understanding of assembly in colloidal systems is crucial to the development of tailored nanostructured materials. Despite extensive studies, a mechanistic understanding of the dynamics governing encounters of colloidal particles remains an ongoing challenge. We study colloidal encounter dynamics by inducing assembly through optical tweezers that impose an external attractive field for cubic-phase sodium yttrium fluoride nanocrystals. We show that surface roughness of the nanocrystals is a decisive factor for contact leading to assembly between the nanocrystals, manifested by the roughness-dependent hydrodynamic resistivity. This provides direct evidence that dynamics are equally important to energetics in understanding assembly.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"088201"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630777","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.081804
M A Acero, B Acharya, P Adamson, N Anfimov, A Antoshkin, E Arrieta-Diaz, L Asquith, A Aurisano, A Back, N Balashov, P Baldi, B A Bambah, E F Bannister, A Barros, A Bat, K Bays, R Bernstein, T J C Bezerra, V Bhatnagar, D Bhattarai, B Bhuyan, J Bian, A C Booth, R Bowles, B Brahma, C Bromberg, N Buchanan, A Butkevich, S Calvez, T J Carroll, E Catano-Mur, J P Cesar, A Chatla, R Chirco, B C Choudhary, A Christensen, M F Cicala, T E Coan, A Cooleybeck, C Cortes-Parra, D Coveyou, L Cremonesi, G S Davies, P F Derwent, P Ding, Z Djurcic, K Dobbs, M Dolce, D Doyle, D Dueñas Tonguino, E C Dukes, A Dye, R Ehrlich, E Ewart, P Filip, M J Frank, H R Gallagher, F Gao, A Giri, R A Gomes, M C Goodman, M Groh, R Group, A Habig, F Hakl, J Hartnell, R Hatcher, H Hausner, M He, K Heller, V Hewes, A Himmel, T Horoho, A Ivanova, B Jargowsky, J Jarosz, M Judah, I Kakorin, A Kalitkina, D M Kaplan, B Kirezli-Ozdemir, J Kleykamp, O Klimov, L W Koerner, L Kolupaeva, R Kralik, A Kumar, V Kus, T Lackey, K Lang, J Lesmeister, A Lister, J Liu, J A Lock, M Lokajicek, M MacMahon, S Magill, W A Mann, M T Manoharan, M Manrique Plata, M L Marshak, M Martinez-Casales, V Matveev, B Mehta, M D Messier, H Meyer, T Miao, V Mikola, W H Miller, S Mishra, S R Mishra, A Mislivec, R Mohanta, A Moren, A Morozova, W Mu, L Mualem, M Muether, D Myers, D Naples, A Nath, S Nelleri, J K Nelson, R Nichol, E Niner, A Norman, A Norrick, H Oh, A Olshevskiy, T Olson, M Ozkaynak, A Pal, J Paley, L Panda, R B Patterson, G Pawloski, R Petti, R K Plunkett, L R Prais, M Rabelhofer, A Rafique, V Raj, M Rajaoalisoa, B Ramson, B Rebel, P Roy, O Samoylov, M C Sanchez, S Sánchez Falero, P Shanahan, P Sharma, A Sheshukov, A Shmakov, Shivam, W Shorrock, S Shukla, D K Singha, I Singh, P Singh, V Singh, E Smith, J Smolik, P Snopok, N Solomey, A Sousa, K Soustruznik, M Strait, L Suter, A Sutton, K Sutton, S Swain, C Sweeney, A Sztuc, B Tapia Oregui, N Talukdar, P Tas, T Thakore, J Thomas, E Tiras, M Titus, Y Torun, D Tran, J Tripathi, J Trokan-Tenorio, J Urheim, P Vahle, Z Vallari, J D Villamil, K J Vockerodt, M Wallbank, C Weber, M Wetstein, D Whittington, D A Wickremasinghe, T Wieber, J Wolcott, M Wrobel, S Wu, W Wu, W Wu, Y Xiao, B Yaeggy, A Yahaya, A Yankelevich, K Yonehara, S Zadorozhnyy, J Zalesak, R Zwaska
We report a search for neutrino oscillations to sterile neutrinos under a model with three active and one sterile neutrinos (3+1 model). This analysis uses the NOvA detectors exposed to the NuMI beam, running in neutrino mode. The data exposure, 13.6×10^{20} protons on target, doubles that previously analyzed by NOvA, and the analysis is the first to use ν_{μ} charged-current interactions in conjunction with neutral-current interactions. Neutrino samples in the near and far detectors are fitted simultaneously, enabling the search to be carried out over a Δm_{41}^{2} range extending 2 (3) orders of magnitude above (below) 1 eV^{2}. NOvA finds no evidence for active-to-sterile neutrino oscillations under the 3+1 model at 90% confidence level. New limits are reported in multiple regions of parameter space, excluding some regions currently allowed by IceCube at 90% confidence level. We additionally set the most stringent limits for anomalous ν_{τ} appearance for Δm_{41}^{2}≤3 eV^{2}.
{"title":"Dual-Baseline Search for Active-to-Sterile Neutrino Oscillations in NOvA.","authors":"M A Acero, B Acharya, P Adamson, N Anfimov, A Antoshkin, E Arrieta-Diaz, L Asquith, A Aurisano, A Back, N Balashov, P Baldi, B A Bambah, E F Bannister, A Barros, A Bat, K Bays, R Bernstein, T J C Bezerra, V Bhatnagar, D Bhattarai, B Bhuyan, J Bian, A C Booth, R Bowles, B Brahma, C Bromberg, N Buchanan, A Butkevich, S Calvez, T J Carroll, E Catano-Mur, J P Cesar, A Chatla, R Chirco, B C Choudhary, A Christensen, M F Cicala, T E Coan, A Cooleybeck, C Cortes-Parra, D Coveyou, L Cremonesi, G S Davies, P F Derwent, P Ding, Z Djurcic, K Dobbs, M Dolce, D Doyle, D Dueñas Tonguino, E C Dukes, A Dye, R Ehrlich, E Ewart, P Filip, M J Frank, H R Gallagher, F Gao, A Giri, R A Gomes, M C Goodman, M Groh, R Group, A Habig, F Hakl, J Hartnell, R Hatcher, H Hausner, M He, K Heller, V Hewes, A Himmel, T Horoho, A Ivanova, B Jargowsky, J Jarosz, M Judah, I Kakorin, A Kalitkina, D M Kaplan, B Kirezli-Ozdemir, J Kleykamp, O Klimov, L W Koerner, L Kolupaeva, R Kralik, A Kumar, V Kus, T Lackey, K Lang, J Lesmeister, A Lister, J Liu, J A Lock, M Lokajicek, M MacMahon, S Magill, W A Mann, M T Manoharan, M Manrique Plata, M L Marshak, M Martinez-Casales, V Matveev, B Mehta, M D Messier, H Meyer, T Miao, V Mikola, W H Miller, S Mishra, S R Mishra, A Mislivec, R Mohanta, A Moren, A Morozova, W Mu, L Mualem, M Muether, D Myers, D Naples, A Nath, S Nelleri, J K Nelson, R Nichol, E Niner, A Norman, A Norrick, H Oh, A Olshevskiy, T Olson, M Ozkaynak, A Pal, J Paley, L Panda, R B Patterson, G Pawloski, R Petti, R K Plunkett, L R Prais, M Rabelhofer, A Rafique, V Raj, M Rajaoalisoa, B Ramson, B Rebel, P Roy, O Samoylov, M C Sanchez, S Sánchez Falero, P Shanahan, P Sharma, A Sheshukov, A Shmakov, Shivam, W Shorrock, S Shukla, D K Singha, I Singh, P Singh, V Singh, E Smith, J Smolik, P Snopok, N Solomey, A Sousa, K Soustruznik, M Strait, L Suter, A Sutton, K Sutton, S Swain, C Sweeney, A Sztuc, B Tapia Oregui, N Talukdar, P Tas, T Thakore, J Thomas, E Tiras, M Titus, Y Torun, D Tran, J Tripathi, J Trokan-Tenorio, J Urheim, P Vahle, Z Vallari, J D Villamil, K J Vockerodt, M Wallbank, C Weber, M Wetstein, D Whittington, D A Wickremasinghe, T Wieber, J Wolcott, M Wrobel, S Wu, W Wu, W Wu, Y Xiao, B Yaeggy, A Yahaya, A Yankelevich, K Yonehara, S Zadorozhnyy, J Zalesak, R Zwaska","doi":"10.1103/PhysRevLett.134.081804","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.081804","url":null,"abstract":"<p><p>We report a search for neutrino oscillations to sterile neutrinos under a model with three active and one sterile neutrinos (3+1 model). This analysis uses the NOvA detectors exposed to the NuMI beam, running in neutrino mode. The data exposure, 13.6×10^{20} protons on target, doubles that previously analyzed by NOvA, and the analysis is the first to use ν_{μ} charged-current interactions in conjunction with neutral-current interactions. Neutrino samples in the near and far detectors are fitted simultaneously, enabling the search to be carried out over a Δm_{41}^{2} range extending 2 (3) orders of magnitude above (below) 1 eV^{2}. NOvA finds no evidence for active-to-sterile neutrino oscillations under the 3+1 model at 90% confidence level. New limits are reported in multiple regions of parameter space, excluding some regions currently allowed by IceCube at 90% confidence level. We additionally set the most stringent limits for anomalous ν_{τ} appearance for Δm_{41}^{2}≤3 eV^{2}.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"081804"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630552","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.081402
Thomas F M Spieksma, Vitor Cardoso, Gregorio Carullo, Matteo Della Rocca, Francisco Duque
The ringdown phase following a binary black hole coalescence is a powerful tool for measuring properties of the remnant black hole. Future gravitational wave detectors will increase the precision of these measurements and may be sensitive to the environment surrounding the black hole. This work examines how environments affect the ringdown from a binary coalescence. Our analysis shows that for astrophysical parameters and sensitivity of planned detectors, the ringdown signal is indistinguishable from its vacuum counterpart, suggesting that ringdown-only analyses can reliably extract the (redshifted) mass and spin of the remnant black hole. These conclusions include models with spectral instabilities, suggesting that these are not relevant from an observational viewpoint. Deviations from inspiral-only estimates could then enhance the characterisation of environmental effects present during the coalescence.
{"title":"Black Hole Spectroscopy in Environments: Detectability Prospects.","authors":"Thomas F M Spieksma, Vitor Cardoso, Gregorio Carullo, Matteo Della Rocca, Francisco Duque","doi":"10.1103/PhysRevLett.134.081402","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.081402","url":null,"abstract":"<p><p>The ringdown phase following a binary black hole coalescence is a powerful tool for measuring properties of the remnant black hole. Future gravitational wave detectors will increase the precision of these measurements and may be sensitive to the environment surrounding the black hole. This work examines how environments affect the ringdown from a binary coalescence. Our analysis shows that for astrophysical parameters and sensitivity of planned detectors, the ringdown signal is indistinguishable from its vacuum counterpart, suggesting that ringdown-only analyses can reliably extract the (redshifted) mass and spin of the remnant black hole. These conclusions include models with spectral instabilities, suggesting that these are not relevant from an observational viewpoint. Deviations from inspiral-only estimates could then enhance the characterisation of environmental effects present during the coalescence.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"081402"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630563","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.083802
Vagharshak Hakobyan, Etienne Brasselet
We report on the extension of the q-plate concept, a hallmark of spin-orbit optical vortex generation since its introduction in 2006, to the generation of optical skyrmions. Stokes skyrmions of arbitrary order with polarization-controlled Skyrme number and reconfigurable multiskyrmions are obtained. This is done by endowing q-plates with a winding number associated with the radial degree of freedom that adds to the usual one associated with the azimuthal degree of freedom.
{"title":"Q-Plates: From Optical Vortices to Optical Skyrmions.","authors":"Vagharshak Hakobyan, Etienne Brasselet","doi":"10.1103/PhysRevLett.134.083802","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.083802","url":null,"abstract":"<p><p>We report on the extension of the q-plate concept, a hallmark of spin-orbit optical vortex generation since its introduction in 2006, to the generation of optical skyrmions. Stokes skyrmions of arbitrary order with polarization-controlled Skyrme number and reconfigurable multiskyrmions are obtained. This is done by endowing q-plates with a winding number associated with the radial degree of freedom that adds to the usual one associated with the azimuthal degree of freedom.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"083802"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630796","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}
Pub Date : 2025-02-28DOI: 10.1103/PhysRevLett.134.083801
Naresh Aggarwal, Ajay Kumar Poonia, Dmitry N Dirin, Ihor Cherniukh, Arijit Sinha, Umesh V Waghmare, Maryna I Bodnarchuk, Sebastian Wüster, Maksym V Kovalenko, K V Adarsh
Superfluorescence, a coherent burst of light from an excited ensemble of emitters, is a crucial quantum optical phenomenon with far-reaching implications in nanophotonics and many-body optical processes. Despite its observation in various systems, realizing superfluorescence in an electron-hole plasma (EHP) at room temperature has remained a formidable challenge, hindering the development of continuous-wave and electrically excited superfluorescence devices. Herein, we address this challenge by condensing the high-density EHP into an electron-hole liquid (EHL) at room temperature, thereby preserving quantum coherence. Using a model system of nanocrystal thin films, we demonstrate the first experimental observation of room temperature superfluorescence from an EHL. Key attributes heralding superfluorescence include a redshift of ∼94 meV from uncorrelated exciton emission, a fluence-dependent delayed growth of macroscopic coherence with abrupt radiative decay ∼1250 times faster than spontaneous emission, a distinct quadratic fluence dependence with a clear threshold, and Burnham-Chiao ringing. These findings open up exciting possibilities for developing electrically pumped colloidal nanocrystals lasers and quantum technologies operating at room temperature.
{"title":"Room Temperature Superfluorescence from an Electron-Hole Liquid.","authors":"Naresh Aggarwal, Ajay Kumar Poonia, Dmitry N Dirin, Ihor Cherniukh, Arijit Sinha, Umesh V Waghmare, Maryna I Bodnarchuk, Sebastian Wüster, Maksym V Kovalenko, K V Adarsh","doi":"10.1103/PhysRevLett.134.083801","DOIUrl":"https://doi.org/10.1103/PhysRevLett.134.083801","url":null,"abstract":"<p><p>Superfluorescence, a coherent burst of light from an excited ensemble of emitters, is a crucial quantum optical phenomenon with far-reaching implications in nanophotonics and many-body optical processes. Despite its observation in various systems, realizing superfluorescence in an electron-hole plasma (EHP) at room temperature has remained a formidable challenge, hindering the development of continuous-wave and electrically excited superfluorescence devices. Herein, we address this challenge by condensing the high-density EHP into an electron-hole liquid (EHL) at room temperature, thereby preserving quantum coherence. Using a model system of nanocrystal thin films, we demonstrate the first experimental observation of room temperature superfluorescence from an EHL. Key attributes heralding superfluorescence include a redshift of ∼94 meV from uncorrelated exciton emission, a fluence-dependent delayed growth of macroscopic coherence with abrupt radiative decay ∼1250 times faster than spontaneous emission, a distinct quadratic fluence dependence with a clear threshold, and Burnham-Chiao ringing. These findings open up exciting possibilities for developing electrically pumped colloidal nanocrystals lasers and quantum technologies operating at room temperature.</p>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"134 8","pages":"083801"},"PeriodicalIF":8.1,"publicationDate":"2025-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143630802","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}