Researchers from Stanford University propose Representation Finetuning (ReFT), a method for adapting language models by directly learning interventions on their hidden representations. Their flagship method, LoReFT, achieves competitive or superior task performance across various benchmarks while being 15 to 65 times more parameter-efficient than existing PEFT methods like LoRA.
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Location Intelligence (LI), the science of transforming location-centric geospatial data into actionable knowledge, has become a cornerstone of modern spatial decision-making. The rapid evolution of Geospatial Representation Learning is fundamentally reshaping LI development through two successive technological revolutions: the deep learning breakthrough and the emerging large language model (LLM) paradigm. While deep neural networks (DNNs) have demonstrated remarkable success in automated feature extraction from structured geospatial data (e.g., satellite imagery, GPS trajectories), the recent integration of LLMs introduces transformative capabilities for cross-modal geospatial reasoning and unstructured geo-textual data processing. This survey presents a comprehensive review of geospatial representation learning across both technological eras, organizing them into a structured taxonomy based on the complete pipeline comprising: (1) data perspective, (2) methodological perspective and (3) application perspective. We also highlight current advancements, discuss existing limitations, and propose potential future research directions in the LLM era. This work offers a thorough exploration of the field and providing a roadmap for further innovation in LI. The summary of the up-to-date paper list can be found in this https URL and will undergo continuous updates.
The proliferation of online toxic speech is a pertinent problem posing threats to demographic groups. While explicit toxic speech contains offensive lexical signals, implicit one consists of coded or indirect language. Therefore, it is crucial for models not only to detect implicit toxic speech but also to explain its toxicity. This draws a unique need for unified frameworks that can effectively detect and explain implicit toxic speech. Prior works mainly formulated the task of toxic speech detection and explanation as a text generation problem. Nonetheless, models trained using this strategy can be prone to suffer from the consequent error propagation problem. Moreover, our experiments reveal that the detection results of such models are much lower than those that focus only on the detection task. To bridge these gaps, we introduce ToXCL, a unified framework for the detection and explanation of implicit toxic speech. Our model consists of three modules: a (i) Target Group Generator to generate the targeted demographic group(s) of a given post; an (ii) Encoder-Decoder Model in which the encoder focuses on detecting implicit toxic speech and is boosted by a (iii) Teacher Classifier via knowledge distillation, and the decoder generates the necessary explanation. ToXCL achieves new state-of-the-art effectiveness, and outperforms baselines significantly.
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We report the first measurement of charged particle elliptic flow in Pb-Pb collisions at 2.76 TeV with the ALICE detector at the CERN Large Hadron Collider. The measurement is performed in the central pseudorapidity region (|η\eta|<0.8) and transverse momentum range 0.2< pTp_{\rm T}< 5.0 GeV/cc. The elliptic flow signal v2_2, measured using the 4-particle correlation method, averaged over transverse momentum and pseudorapidity is 0.087 ±\pm 0.002 (stat) ±\pm 0.004 (syst) in the 40-50% centrality class. The differential elliptic flow v2(pT)_2(p_{\rm T}) reaches a maximum of 0.2 near pTp_{\rm T} = 3 GeV/cc. Compared to RHIC Au-Au collisions at 200 GeV, the elliptic flow increases by about 30%. Some hydrodynamic model predictions which include viscous corrections are in agreement with the observed increase.
CNRS logoCNRSAcademia SinicaCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloUniversity of Waterloo logoUniversity of WaterlooGhent UniversityUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of EdinburghETH Zürich logoETH ZürichNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterUniversidade de LisboaLancaster UniversityUniversity of GranadaUniversité Paris-Saclay logoUniversité Paris-SaclayHelsinki Institute of PhysicsStockholm University logoStockholm UniversityUniversity of HelsinkiThe University of ManchesterPerimeter Institute for Theoretical Physics logoPerimeter Institute for Theoretical PhysicsUniversité de GenèveUniversity of California, MercedLeiden University logoLeiden UniversityUniversity of GenevaLiverpool John Moores UniversityESOUniversity of LeidenICREAUniversitat de BarcelonaConsejo Superior de Investigaciones CientíficasUniversität BonnUniversity of IcelandUniversidade do PortoUniversity of SussexEcole Polytechnique Fédérale de LausanneTechnical University of DenmarkDurham University logoDurham UniversityUniversity of Groningen logoUniversity of GroningenInstituto de Astrofísica e Ciências do EspaçoINAFAix Marseille UniversityUniversity of BathNiels Bohr InstituteUniversidade Federal do Rio Grande do NorteInstituto de Astrofísica de CanariasUniversity of the WitwatersrandEuropean Space AgencyNational Tsing-Hua UniversityÉcole Polytechnique Fédérale de LausanneUniversitat Autònoma de BarcelonaUniversity of TriesteINFN, Sezione di TorinoUniversidad de ValparaísoUniversidad de La LagunaNRC Herzberg Astronomy and AstrophysicsUniversity of AntwerpObservatoire de la Côte d’AzurCavendish LaboratoryUniversity of Hawai’iUniversity of KwaZulu-NatalLudwig-Maximilians-UniversitätInstituto de Astrofísica de Andalucía-CSICINAF – Istituto di Astrofisica e Planetologia SpazialiKapteyn Astronomical InstituteNational Observatory of AthensMax-Planck Institut für extraterrestrische PhysikINAF – Osservatorio Astronomico di RomaInstituto de Astrofísica de Canarias (IAC)Institut d'Astrophysique de ParisUniversidad de SalamancaInstitut de Física d’Altes Energies (IFAE)Institut Teknologi BandungSwiss Federal Institute of TechnologyINFN - Sezione di PadovaUniversità degli Studi di Urbino ’Carlo Bo’INAF-IASF MilanoUniversità di FirenzeInstitute of Space ScienceCosmic Dawn CenterInstituto de Física de CantabriaDTU SpaceINFN Sezione di LecceINFN-Sezione di BolognaUniversity of Hartford2Osservatorio Astronomico di RomaASI - Agenzia Spaziale ItalianaInfrared Processing and Analysis Center1/2(4)37353629Space Science Data CenterBarcelona Institute of Science and TechnologyCSC – IT Center for Science Ltd.Instituto de Astrofísica e Ciências do Espaço, Universidade de LisboaUniversity of Côte d’AzurSorbonne Université, CNRSUniversité Paris-SorbonneOskar Klein CentreESAC611182515211020177823133191622951424335238284375667484646148415758426351464981307940762731735553545650598067347870726860266239776544458347716932Paris Sciences et LettresDeimos Space85Université de Toulouse III - Paul Sabatier9886Centre de Física d’Altes Energies (FPAE)9911410610595Aix Marseille Université, CNRS, CNESESAC/ESA109Center for Informatics and Computation in Science and Engineering116102100Cosmic Origins10387113112Université Paris Cité, CEA, CNRS101939497107TERMA11511110896104110149131127124132128122136142126138CNRS, Institut d’Astrophysique de Paris151125139143119137145148120117141Universitas Pendidikan Indonesia13414414614011815012314713313512112913091.89.92.88.82.90.INAF Osservatorio di PadovaINAF-IASF, BolognaINFN-Sezione di Roma TreINFN-Sezione di FerraraUniversit degli Studi di FerraraUniversit Grenoble AlpesUniversit Claude Bernard Lyon 1Universit del SalentoUniversit di FerraraINAF Osservatorio Astronomico di CapodimonteMax Planck Institut fr AstronomieUniversit Lyon 1Universit de StrasbourgUniversit de LyonRuhr-University-BochumINAF Osservatorio Astrofisico di ArcetriUniversit degli Studi di TorinoUniversity of Naples “Federico II”INAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaUniversit Di BolognaIFPU Institute for fundamental physics of the UniverseINAF ` Osservatorio Astronomico di TriesteINFN Istituto Nazionale di Fisica NucleareUniversit degli Studi Roma TreINAF Osservatorio Astronomico di Brera
Recent James Webb Space Telescope (JWST) observations have revealed a population of sources with a compact morphology and a `v-shaped' continuum, namely blue at rest-frame \lambda&lt;4000A and red at longer wavelengths. The nature of these sources, called `little red dots' (LRDs), is still debated, since it is unclear if they host active galactic nuclei (AGN) and their number seems to drastically drop at z<4. We utilise the 63 deg2deg^2 covered by the quick Euclid Quick Data Release (Q1) to extend the search for LRDs to brighter magnitudes and to lower z than what has been possible with JWST to have a broader view of the evolution of this peculiar galaxy population. The selection is done by fitting the available photometric data (Euclid, Spitzer/IRAC, and ground-based griz data) with two power laws, to retrieve the rest-frame optical and UV slopes consistently over a large redshift range (i.e, z<7.6). We exclude extended objects and possible line emitters, and perform a visual inspection to remove imaging artefacts. The final selection includes 3341 LRD candidates from z=0.33 to z=3.6, with 29 detected in IRAC. Their rest-frame UV luminosity function, in contrast with previous JWST studies, shows that the number density of LRD candidates increases from high-z down to z=1.5-2.5 and decreases at even lower z. Less evolution is apparent focusing on the subsample of more robust LRD candidates having IRAC detections, which is affected by low statistics and limited by the IRAC resolution. The comparison with previous quasar UV luminosity functions shows that LRDs are not the dominant AGN population at z<4. Follow-up studies of these LRD candidates are key to confirm their nature, probe their physical properties and check for their compatibility with JWST sources, since the different spatial resolution and wavelength coverage of Euclid and JWST could select different samples of compact sources.
We perform a search for light sterile neutrinos using the data from the T2K far detector at a baseline of 295 km, with an exposure of 14.7 (7.6)$\times 10^{20}$ protons on target in neutrino (antineutrino) mode. A selection of neutral current interaction samples are also used to enhance the sensitivity to sterile mixing. No evidence of sterile neutrino mixing in the 3+1 model was found from a simultaneous fit to the charged-current muon, electron and neutral current neutrino samples. We set the most stringent limit on the sterile oscillation amplitude sin2θ24\sin^2\theta_{24} for the sterile neutrino mass splitting \Delta m^2_{41}&lt;3\times 10^{-3} eV2/c4^2/c^4.
Accurate 3D perception is essential for autonomous driving. Traditional methods often struggle with geometric ambiguity due to a lack of geometric prior. To address these challenges, we use omnidirectional depth estimation to introduce geometric prior. Based on the depth information, we propose a Sketch-Coloring framework OmniDepth-Occ. Additionally, our approach introduces a cylindrical voxel representation based on polar coordinate to better align with the radial nature of panoramic camera views. To address the lack of fisheye camera dataset in autonomous driving tasks, we also build a virtual scene dataset with six fisheye cameras, and the data volume has reached twice that of SemanticKITTI. Experimental results demonstrate that our Sketch-Coloring network significantly enhances 3D perception performance.
Recent advances in one-shot imitation learning have enabled robots to acquire new manipulation skills from a single human demonstration. While existing methods achieve strong performance on single-step tasks, they remain limited in their ability to handle long-horizon, multi-step tasks without additional model training or manual annotation. We propose a method that can be applied to this setting provided a single demonstration without additional model training or manual annotation. We evaluated our method on multi-step and single-step manipulation tasks where our method achieves an average success rate of 82.5% and 90%, respectively. Our method matches and exceeds the performance of the baselines in both these cases. We also compare the performance and computational efficiency of alternative pre-trained feature extractors within our framework.
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The six parameters of the standard Λ\LambdaCDM model have best-fit values derived from the Planck temperature power spectrum that are shifted somewhat from the best-fit values derived from WMAP data. These shifts are driven by features in the Planck temperature power spectrum at angular scales that had never before been measured to cosmic-variance level precision. We investigate these shifts to determine whether they are within the range of expectation and to understand their origin in the data. Taking our parameter set to be the optical depth of the reionized intergalactic medium τ\tau, the baryon density ωb\omega_{\rm b}, the matter density ωm\omega_{\rm m}, the angular size of the sound horizon θ\theta_*, the spectral index of the primordial power spectrum, nsn_{\rm s}, and Ase2τA_{\rm s}e^{-2\tau} (where AsA_{\rm s} is the amplitude of the primordial power spectrum), we examine the change in best-fit values between a WMAP-like large angular-scale data set (with multipole moment \ell&lt;800 in the Planck temperature power spectrum) and an all angular-scale data set (\ell&lt;2500 Planck temperature power spectrum), each with a prior on τ\tau of 0.07±0.020.07\pm0.02. We find that the shifts, in units of the 1σ\sigma expected dispersion for each parameter, are $\{\Delta \tau, \Delta A_{\rm s} e^{-2\tau}, \Delta n_{\rm s}, \Delta \omega_{\rm m}, \Delta \omega_{\rm b}, \Delta \theta_*\} = \{-1.7, -2.2, 1.2, -2.0, 1.1, 0.9\},witha, with a \chi^2$ value of 8.0. We find that this χ2\chi^2 value is exceeded in 15% of our simulated data sets, and that a parameter deviates by more than 2.2σ\sigma in 9% of simulated data sets, meaning that the shifts are not unusually large. Comparing \ell&lt;800 instead to \ell&gt;800, or splitting at a different multipole, yields similar results. We examine the \ell&lt;800 model residuals in the \ell&gt;800 power spectrum data and find that the features there... [abridged]
Language Models (LMs) excel in natural language processing tasks for English but show reduced performance in most other languages. This problem is commonly tackled by continually pre-training and fine-tuning these models for said languages. A significant issue in this process is the limited vocabulary coverage in the original model's tokenizer, leading to inadequate representation of new languages and necessitating an expansion of the tokenizer. The initialization of the embeddings corresponding to new vocabulary items presents a further challenge. Current strategies require cross-lingual embeddings and lack a solid theoretical foundation as well as comparisons with strong baselines. In this paper, we first establish theoretically that initializing within the convex hull of existing embeddings is a good initialization, followed by a novel but simple approach, Constrained Word2Vec (CW2V), which does not require cross-lingual embeddings. Our study evaluates different initialization methods for expanding RoBERTa and LLaMA 2 across four languages and five tasks. The results show that CW2V performs equally well or even better than more advanced techniques. Additionally, simpler approaches like multivariate initialization perform on par with these advanced methods indicating that efficient large-scale multilingual continued pretraining can be achieved even with simpler initialization methods. We release our code publicly (this https URL).
Clinical evidence has shown that rib-suppressed chest X-rays (CXRs) can improve the reliability of pulmonary disease diagnosis. However, previous approaches on generating rib-suppressed CXR face challenges in preserving details and eliminating rib residues. We hereby propose a GAN-based disentanglement learning framework called Rib Suppression GAN, or RSGAN, to perform rib suppression by utilizing the anatomical knowledge embedded in unpaired computed tomography (CT) images. In this approach, we employ a residual map to characterize the intensity difference between CXR and the corresponding rib-suppressed result. To predict the residual map in CXR domain, we disentangle the image into structure- and contrast-specific features and transfer the rib structural priors from digitally reconstructed radiographs (DRRs) computed by CT. Furthermore, we employ additional adaptive loss to suppress rib residue and preserve more details. We conduct extensive experiments based on 1,673 CT volumes, and four benchmarking CXR datasets, totaling over 120K images, to demonstrate that (i) our proposed RSGAN achieves superior image quality compared to the state-of-the-art rib suppression methods; (ii) combining CXR with our rib-suppressed result leads to better performance in lung disease classification and tuberculosis area detection.
The IceCube Collaboration has previously discovered a high-energy astrophysical neutrino flux using neutrino events with interaction vertices contained within the instrumented volume of the IceCube detector. We present a complementary measurement using charged current muon neutrino events where the interaction vertex can be outside this volume. As a consequence of the large muon range the effective area is significantly larger but the field of view is restricted to the Northern Hemisphere. IceCube data from 2009 through 2015 have been analyzed using a likelihood approach based on the reconstructed muon energy and zenith angle. At the highest neutrino energies between 191 TeV and 8.3 PeV a significant astrophysical contribution is observed, excluding a purely atmospheric origin of these events at 5.6σ5.6\,\sigma significance. The data are well described by an isotropic, unbroken power law flux with a normalization at 100 TeV neutrino energy of (0.900.27+0.30)×1018GeV1cm2s1sr1\left(0.90^{+0.30}_{-0.27}\right)\times10^{-18}\,\mathrm{GeV^{-1}\,cm^{-2}\,s^{-1}\,sr^{-1}} and a hard spectral index of γ=2.13±0.13\gamma=2.13\pm0.13. The observed spectrum is harder in comparison to previous IceCube analyses with lower energy thresholds which may indicate a break in the astrophysical neutrino spectrum of unknown origin. The highest energy event observed has a reconstructed muon energy of (4.5±1.2)PeV(4.5\pm1.2)\,\mathrm{PeV} which implies a probability of less than 0.005% for this event to be of atmospheric origin. Analyzing the arrival directions of all events with reconstructed muon energies above 200 TeV no correlation with known γ\gamma-ray sources was found. Using the high statistics of atmospheric neutrinos we report the currently best constraints on a prompt atmospheric muon neutrino flux originating from charmed meson decays which is below 1.061.06 in units of the flux normalization of the model in Enberg et al. (2008).
I2n01326X(C), one can construct the quotient singularitya canonical surface singularity). The geometry of such singularities is of importanceis a singleton withdimρ/Γ])is isomorphic to a particular NakajimaReplacing every edge in this graph by a pair of opposing arrows, we obtain a quiver,one can construct several Nakajima quiver varieties, whichoften turn out to be5. Sheaves onPto the subsetI={0}is thus isomorphic to the Hilbert scheme of pointsHilbfor instance, the Hilbert schemes of points onX, the equivariant Hilbert schemeNakajima quiver varieties built from the McKay quiverQin Section 1.1.- submodulesM/Γ)where/Γ]andPProposition 3.4] (see also [10, Theorem 1.3])Quot(C). Then the quotientCthem here. We also give an overview of all known (at least, to us) interpretations ofIn this paper, we will find geometric interpretations of a large class of Nakajima, indexed by a set of irreducibleΓ-isomorphic to - or, at least, be in canonical bijection with -interesting moduli spaceswith{0,...,r}./Γisquiver varieties. Those quiver varieties appearing in thispaper will always be built/M=ncarry a canonical bijectionReferences28varieties. Especially, whenn= 2, such moduli spaces can often be constructed asattached to the singularityC, weofRstackXcontainingC= Hom(ρcorrespondence [20]. Among other things, this correspondence associates a graphWhenI={i}⊂Qphism classes of framed torsion-free sheaves on anyPby the McKay correspondence [20]. We will use the McKay quiver to build severaltheMcKay quiverassociated toΓ. From this quiver, with some additional data,Given a subgroupΓ⊂SLQuot1. Introduction14. The geometry ofPdefined in [22] have become very useful in representation theory and algebraic geom-. The Quot scheme corresponding6. Connections to previous results23representations. When considering the extended action ofΓfromCprovide geometric interpretations for a class of Nakajima quiver varieties using3. Quivers and quiver algebras10, and investigate various spaces attached toX:Abstract.LetΓ∈SLa Kleinian singularity (also known as, among other names, a du Val singularity, or/Γ, and we showtoP= 1, there is also an isomorphism [8,etry, not only because they provide constructions of interesting moduli spaces, but}be the set of irreducible representations ofΓ, such thatρparametrising isomorphism classes of quotients of an equivariant rank 1 sheaf onC(C)be a finite subgroup. We introduce a classthat moduli spaces offramed sheavesonPis trivial. For ease of notation, we will identifyQ2SØREN GAMMELGAARD AND ÁDÁM GYENGEof the singular schemePnoncommutative‘partial resolutions’PX=Csults on such quiver varieties./Γ. In various papers, e.g., [27, 5, 3, 7, 8, 13, 2], suchin the minimal model program and for theoretical physics (see e.g. [19], [16]). Itthere is anorbifold Quot schemeQuot2. Preliminaries5(theMcKay graph) to the isomorphism class ofΓ, which is an affine Dynkin graph.and Nakajima quiver varieties17nongeneric.In more detail, choose a finite subgroupΓ⊂SLand1.Introduction([12]) moduli spaces offramed sheavesof/Γ. We prove that isomor-Key words and phrases.noncommutative geometry, quiver variety, McKay correspondence,Nakajima quiver varieties(see Section 1.1 for a list). These quiver varieties, firstto Nakajima quiver varieties.LetQSecond, the first author showed in [13] that there is a projective Deligne-Mumfordquiver variety.show that these surfaces generalise both[PFirst, in [8], we showed with our coauthors that for any non-emptyI⊆QIt was also shown [8, 10] thatQuotAppendix A. A comparison with a projective stack compactifyingCto the closed points of appropriate Nakajima quiver varieties. In particular, wealso because they satisfy desirable geometric properties:they are irreducible, have2020Mathematics Subject Classification.Primary 14A22; Secondary 16G20, 14E16.moduli spaces were identified with Nakajima quiver varieties; we mention two ofhave a canonical bijection of closed pointssymplectic singularities, and when smooth, they are hyperkähler.from a particular quiver (theMcKay quiver) canonically associated toΓ⊂SLSØREN GAMMELGAARD AND ÁDÁM GYENGEfor any dimension vectornof projective noncommutative surfacesPContents/Γ)is the classical Quot scheme parameterisingC[x,y]noncommutative geometry. Our results partially generalise several previous re-has long been recognised that an approach to studying them isthrough the McKay= Spec(C[xnΓ-Hilb(V), and resolutions ofX. One can often construct such spaces as quiver/Γas an open subscheme. On this stack, one can construct,C[x,y])such thatdimRR)1∗C",":
Let ΓSL2(C)\Gamma\in \mathrm{SL}_2(\mathbb{C}) be a finite subgroup. We introduce a class of projective noncommutative surfaces PI2\mathbb{P}^2_I, indexed by a set of irreducible Γ\Gamma-representations. Extending the action of Γ\Gamma from C2\mathbb{C}^2 to P2\mathbb{P}^2, we show that these surfaces generalise both [P2/Γ][\mathbb{P}^2/\Gamma] and P2/Γ\mathbb{P}^2/\Gamma. We prove that isomorphism classes of framed torsion-free sheaves on any PI2\mathbb{P}^2_I carry a canonical bijection to the closed points of appropriate Nakajima quiver varieties. In particular, we provide geometric interpretations for a class of Nakajima quiver varieties using noncommutative geometry. Our results partially generalise several previous results on such quiver varieties.
Applying deep neural networks to 3D point cloud processing has attracted increasing attention due to its advanced performance in many areas, such as AR/VR, autonomous driving, and robotics. However, as neural network models and 3D point clouds expand in size, it becomes a crucial challenge to reduce the computational and memory overhead to meet latency and energy constraints in real-world applications. Although existing approaches have proposed to reduce both computational cost and memory footprint, most of them only address the spatial redundancy in inputs, i.e. removing the redundancy of background points in 3D data. In this paper, we propose a novel post-training weight pruning scheme for 3D object detection that is (1) orthogonal to all existing point cloud sparsifying methods, which determines redundant parameters in the pretrained model that lead to minimal distortion in both locality and confidence (detection distortion); and (2) a universal plug-and-play pruning framework that works with arbitrary 3D detection model. This framework aims to minimize detection distortion of network output to maximally maintain detection precision, by identifying layer-wise sparsity based on second-order Taylor approximation of the distortion. Albeit utilizing second-order information, we introduced a lightweight scheme to efficiently acquire Hessian information, and subsequently perform dynamic programming to solve the layer-wise sparsity. Extensive experiments on KITTI, Nuscenes and ONCE datasets demonstrate that our approach is able to maintain and even boost the detection precision on pruned model under noticeable computation reduction (FLOPs). Noticeably, we achieve over 3.89x, 3.72x FLOPs reduction on CenterPoint and PVRCNN model, respectively, without mAP decrease, significantly improving the state-of-the-art.
We propose to tackle the problem of multiview 2D/3D rigid registration for intervention via a Point-Of-Interest Network for Tracking and Triangulation (POINT2\text{POINT}^2). POINT2\text{POINT}^2 learns to establish 2D point-to-point correspondences between the pre- and intra-intervention images by tracking a set of random POIs. The 3D pose of the pre-intervention volume is then estimated through a triangulation layer. In POINT2\text{POINT}^2, the unified framework of the POI tracker and the triangulation layer enables learning informative 2D features and estimating 3D pose jointly. In contrast to existing approaches, POINT2\text{POINT}^2 only requires a single forward-pass to achieve a reliable 2D/3D registration. As the POI tracker is shift-invariant, POINT2\text{POINT}^2 is more robust to the initial pose of the 3D pre-intervention image. Extensive experiments on a large-scale clinical cone-beam CT (CBCT) dataset show that the proposed POINT2\text{POINT}^2 method outperforms the existing learning-based method in terms of accuracy, robustness and running time. Furthermore, when used as an initial pose estimator, our method also improves the robustness and speed of the state-of-the-art optimization-based approaches by ten folds.
Computed tomography (CT) reconstruction from X-ray projections acquired within a limited angle range is challenging, especially when the angle range is extremely small. Both analytical and iterative models need more projections for effective modeling. Deep learning methods have gained prevalence due to their excellent reconstruction performances, but such success is mainly limited within the same dataset and does not generalize across datasets with different distributions. Hereby we propose ExtraPolationNetwork for limited-angle CT reconstruction via the introduction of a sinogram extrapolation module, which is theoretically justified. The module complements extra sinogram information and boots model generalizability. Extensive experimental results show that our reconstruction model achieves state-of-the-art performance on NIH-AAPM dataset, similar to existing approaches. More importantly, we show that using such a sinogram extrapolation module significantly improves the generalization capability of the model on unseen datasets (e.g., COVID-19 and LIDC datasets) when compared to existing approaches.
21/2(4)37353629611251510178231331916225142433523828434841425130273153503426394432F. De MoriW. ShanS. SpataroQ. P. JiS. MarcelloM. BertaniM. AblikimH. L. DaiHere's my thinking process to extract the organizations from the provided text:"If no organizations are mentioned, return "none".", M. N. Achasov9,e, S. Ahmed, X. C. Ai, O. Albayrak, M. Albrecht, D. J. Ambrose, A. Amoroso49A,49CF. F. An, Q. An46,a, J. Z. Bai, O. Bakina, R. Baldini Ferroli20A, Y. Ban, D. W. Bennett, J. V. Bennett, N. Berger, D. Bettoni21A, J. M. Bian, F. Bianchi, E. Boger23,c, I. Boyko, R. A. Briere, H. Cai, X. Cai1,aO. Cakir40A, A. Calcaterra, G. F. Cao, S. A. Cetin40B, J. Chai49C, J. F. Chang, G. Chelkov23,c,d, G. Chen, H. S. ChenJ. C. Chen, M. L. Chen, S. Chen, S. J. Chen, X. Chen, X. R. Chen, Y. B. Chen, X. K. Chu, G. Cibinetto, J. P. Dai, A. Dbeyssi, D. Dedovich, Z. Y. Deng, A. Denig, I. Denysenko, M. Destefanis, Y. Ding, C. Dong, J. Dong, L. Y. Dong, M. Y. Dong, Z. L. Dou, S. X. Du, P. F. DuanJ. Z. Fan, J. Fang, S. S. Fang, X. Fang, Y. Fang, R. Farinelli21A,21B, L. Fava49B,49C, F. Feldbauer, G. FeliciC. Q. Feng, E. Fioravanti, M. Fritsch14,22, C. D. Fu, Q. Gao, X. L. Gao, Y. Gao, Z. Gao, I. GarziaK. Goetzen, L. Gong, W. X. Gong, W. Gradl, M. Greco, M. H. Gu, Y. T. Gu, Y. H. Guan, A. Q. GuoL. B. Guo, R. P. Guo, Y. Guo, Y. P. Guo, Z. Haddadi, A. Hafner, S. Han, X. Q. Hao, F. A. Harris, K. L. HeF. H. Heinsius, T. Held, Y. K. Heng, T. Holtmann, Z. L. Hou, C. Hu, H. M. Hu, J. F. Hu, T. Hu, Y. HuG. S. Huang, J. S. Huang, X. T. Huang, X. Z. Huang, Z. L. Huang, T. Hussain, W. Ikegami Andersson, Q. Ji, X. B. Ji, X. L. Ji, L. W. Jiang, X. S. Jiang, X. Y. Jiang, J. B. Jiao, Z. Jiao, D. P. Jin, S. JinT. Johansson, A. Julin, N. Kalantar-Nayestanaki, X. L. Kang, X. S. Kang, M. Kavatsyuk, B. C. Ke, P. KieseR. Kliemt, B. Kloss, O. B. Kolcu40B,h, B. Kopf, M. Kornicer, A. Kupsc, W. K¨uhn, J. S. Lange, M. LaraP. Larin, L. Lavezzi49C,1, H. Leithoff, C. Leng, C. Li, Cheng Li, D. M. Li, F. Li, F. Y. Li, G. Li, H. B. LiH. J. Li, J. C. Li, Jin Li, K. Li, Lei Li, P. R. Li7,41, Q. Y. Li, T. Li, W. D. Li, W. G. Li, X. L. LiX. N. Li, X. Q. Li, Y. B. Li, Z. B. Li, H. Liang, Y. F. Liang, Y. T. Liang, G. R. Liao, D. X. Lin, B. LiuB. J. Liu, C. X. Liu, D. Liu, F. H. Liu, Fang Liu, Feng Liu, H. B. Liu, H. H. Liu, H. M. Liu, J. LiuJ. B. Liu, J. P. Liu, J. Y. Liu, K. Liu, K. Y. Liu, L. D. Liu, P. L. Liu, Q. Liu, S. B. Liu, X. LiuY. B. Liu, Y. Y. Liu, Z. A. Liu, Zhiqing Liu, H. Loehner, X. C. Lou1,a,g, H. J. Lu, J. G. Lu, Y. Lu, Y. P. LuC. L. Luo, M. X. Luo, T. Luo, X. L. Luo, X. R. Lyu, F. C. Ma, H. L. Ma, L. L. Ma, M. M. Ma, Q. M. MaT. Ma, X. N. Ma, X. Y. Ma, Y. M. Ma, F. E. Maas, M. Maggiora, Q. A. Malik, Y. J. Mao, Z. P. Mao, J. G. Messchendorp, G. Mezzadri21B, J. Min, T. J. Min, R. E. Mitchell, X. H. Mo, Y. J. MoC. Morales Morales, N. Yu. Muchnoi, H. Muramatsu, P. Musiol, Y. Nefedov, F. Nerling, I. B. NikolaevZ. Ning, S. Nisar, S. L. Niu, X. Y. Niu, S. L. Olsen, Q. Ouyang, S. Pacetti20B, Y. Pan, P. PatteriM. Pelizaeus, H. P. Peng, K. Peters10,i, J. Pettersson, J. L. Ping, R. G. Ping, R. Poling, V. Prasad, H. R. QiM. Qi, S. Qian, C. F. Qiao, L. Q. Qin, N. Qin, X. S. Qin, Z. H. Qin, J. F. Qiu, K. H. Rashid, C. F. RedmerM. Ripka, G. Rong, Ch. Rosner, X. D. Ruan, A. Sarantsev23,f, M. Savri´e, C. Schnier, K. Schoenning, M. Shao, C. P. Shen, P. X. Shen, X. Y. Shen, H. Y. Sheng, W. M. Song, X. Y. Song, S. Sosio, G. X. Sun, J. F. Sun, S. S. Sun, X. H. Sun, Y. J. Sun, Y. Z. Sun, Z. J. Sun, Z. T. SunC. J. Tang, X. Tang, I. Tapan40C, E. H. Thorndike, M. Tiemens, I. Uman40D, G. S. Varner, B. Wang, B. L. WangD. Wang, D. Y. Wang, K. Wang, L. L. Wang, L. S. Wang, M. Wang, P. Wang, P. L. Wang, W. WangW. P. Wang, X. F. Wang, Y. Wang, Y. D. Wang, Y. F.2. **Scan the Provided Text:** I see a long list of author names, each followed by one or more superscript numbers (e.g., `M. Ablikim^1`, `M. N. Achasov^9,e`).* The prompt states: "Given the *first section* of a research paper, looking at the area usually under the author names..."* The problem is, the *actual affiliation list* (the key for what `1` or `9` refers to) is *missing* from the provided text. The text *cuts off* after `Y. F.`.3. **Address the Missing Affiliation List:** Since the explicit mapping of numbers to institutions is not present in the provided snippet, and the prompt explicitly mentions "Look at the domain of the author emails to be sure (every organization name you return should correspond to one of the author's email domains, obviously dont return the email domains)", this implies that I *should be looking for email domains* or that the full affiliation list *should be there*.4. **Re-read the Instructions Carefully:** "Given the first section of a research paper, looking at the area usually under the author names determine which such organizations the authors are a part of.""Be careful, many times papers will have other organizations/frameworks/library names in their first page that aren't the organizations the authors are actually from!""Look at the domain of the author emails to be sure (every organization name you return should correspond to one of the author's email domains, obviously dont return the email domains).""Return only the organization names, separated by newlines, with no additional text."5. **Critically Evaluate the Current Input:** The input *only* contains author names and their superscript affiliations (numbers and letters like `e`, `c`, `d`, `a`). It *does not* contain the actual list of institutions that these numbers refer to. It also *does not* contain any author email addresses or their domains.6. **Conclusion based on missing information:** Without the actual list that defines what `1`, `9`, `e`, `a`, etc., refer to, and without author email domains, it is *impossible* to determine the organization names from the provided text. The provided text is incomplete for the task.7. **Formulate the Output:** Since the necessary information (the list of affiliations corresponding to the numbers, or author emails) is entirely absent from the provided snippet, I cannot extract any organization names. The instruction "If no organizations are mentioned, return 'none'." applies here, as no *identifiable* organization names are present in the text provided.This is a case where the input is insufficient to complete the task as described by the instructions. The presence of the numbers (`1`, `9`, etc.) clearly indicates that affiliations *should* be listed, but they are cut off. The email domain hint also implies that there *should* be emails if the affiliation list is missing or ambiguous, but there are no emails either.Therefore, the only correct answer, given the provided snippet, is "none".none1∗":
The cross sections of e+eπ+πhce^{+}e^{-}\to\pi^{+}\pi^{-}h_c at center-of-mass energies from 3.896 to 4.600 GeV are measured using data samples collected with the BESIII detector operating at the Beijing Electron Positron Collider. The cross sections are found to be of the same order of magnitude as those of e+eπ+πJ/ψe^{+}e^{-}\to\pi^{+}\pi^{-}J/\psi and e+eπ+πψ(2S)e^{+}e^{-}\to\pi^{+}\pi^{-}\psi(2S), but the line shape is inconsistent with the YY states observed in the latter two modes. Two structures are observed in the e+eπ+πhce^{+}e^{-}\to\pi^{+}\pi^{-}h_c cross sections around 4.22 and 4.39 GeV/c2c^{2}, which we call Y(4220)Y(4220) and Y(4390)Y(4390), respectively. A fit with a coherent sum of two Breit-Wigner functions results in a mass of (4218.44.5+5.5±0.9)(4218.4^{+5.5}_{-4.5}\pm0.9) MeV/c2c^{2} and a width of (66.08.3+12.3±0.4)(66.0^{+12.3}_{-8.3}\pm0.4) MeV for the Y(4220)Y(4220), and a mass of (4391.66.8+6.3±1.0)(4391.6^{+6.3}_{-6.8}\pm1.0) MeV/c2c^{2} and a width of (139.520.6+16.2±0.6)(139.5^{+16.2}_{-20.6}\pm0.6) MeV for the Y(4390)Y(4390), where the first uncertainties are statistical and the second ones systematic. The statistical significance of Y(4220)Y(4220) and Y(4390)Y(4390) is 10σ\sigma over one structure assumption.
Michigan State University logoMichigan State UniversityUniversity of MississippiUniversity of CincinnatiCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of Pittsburgh logoUniversity of PittsburghUniversity of Cambridge logoUniversity of CambridgeSLAC National Accelerator LaboratoryImperial College London logoImperial College LondonUniversity of Notre Dame logoUniversity of Notre DameUniversity of BernUniversity of Chicago logoUniversity of ChicagoUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of BonnPanjab UniversityUniversity of EdinburghIllinois Institute of TechnologyTexas A&M University logoTexas A&M UniversityJoint Institute for Nuclear ResearchYale University logoYale UniversityTata Institute of Fundamental ResearchNorthwestern University logoNorthwestern UniversityBoston University logoBoston UniversityUniversity of Texas at Austin logoUniversity of Texas at AustinUniversit‘a di Napoli Federico IILancaster UniversityUniversity of Pennsylvania logoUniversity of PennsylvaniaColorado State UniversityRice University logoRice UniversityBrookhaven National Laboratory logoBrookhaven National LaboratoryStockholm University logoStockholm UniversityLos Alamos National LaboratoryUniversity of LiverpoolUniversity of Massachusetts AmherstUniversity of RochesterFermi National Accelerator LaboratoryUniversity of SheffieldUniversity of Science and Technology BeijingKing Abdullah University of Science and TechnologyUniversity of GlasgowQueen Mary University of London logoQueen Mary University of LondonUniversity of Warwick logoUniversity of WarwickUniversit`a degli Studi di PadovaUniversidade Estadual de CampinasThe Ohio State University logoThe Ohio State UniversityUniversidade Federal do ABCWayne State UniversityUniversity of SussexUniversity of BirminghamUniversidade Federal do Rio de JaneiroThe Institute of Mathematical SciencesUniversity of South CarolinaUniversity of AntioquiaUniversity of CagliariUniversidade de AveiroUniversit`a di BolognaUniversity of Texas at ArlingtonIndian Institute of Technology GuwahatiUniversity of KansasUniversity of YorkKorea Institute of Science and TechnologyUniversidade do Estado do Rio de JaneiroUniversit`a di CataniaUniversidade Estadual PaulistaJawaharlal Nehru UniversityNational Centre for Nuclear ResearchUniversidade de Sao PauloUniversit`a di Roma TreDortmund UniversitySouth Dakota School of Mines and TechnologyUniversity of SilesiaUniversity of Hawaii, ManoaNikhef, National Institute for Subatomic Physics2Kathmandu UniversityUniversidade Federal de Sao CarlosUniversit`a di PaviaUniversite de StrasbourgUniversite de Lyon1/2(4)373529Universidad Nacional de IngenieriaTexas A&M University-KingsvilleUniversite de Paris, CNRS, Astroparticule et Cosmologie, F-75013 Paris, FranceAdiyaman UniversityUniversidad Tecnica Federico Santa MariaLaboratoire de Physique Nucleaire et de Hautes EnergiesUniversite de BordeauxLaboratoire de Physique des 2 Infinis Ir`ene Joliot-Curie6112515212072313191622951424522843668441575842464981763155598067347262397744454732Universidade Federal de GoiasChonbuk National University85Federal University of Alfenas86991141051031139397107108104110149127124126138151125139119134144150135121129130Universitat WurzburgUniversit’e Paris-Saclay, CNRS/IN2P3, IJCLab175188174159168183200172182, 9615215, 110125, 10116993, 14519391, 10919116092, 162178211155125, 6115891, 14019688, 6815620220187, 36203214, 6715421420716117716786, 1790, 18089, 71204164210177, 128128, 24157189148, 3208Sorbonne Universit\'e, CNRS-IN2P3, Laboratoire de Physique Nucl\'eaire et de Hautes EnergiesUniversit\'e de Strasbourg, CNRS, IPHC UMR7178, F-67000 Strasbourg, FranceInstitut de Recherche sur les lois Fondamentales de l’Univers, CEA, Universit\'e Paris-Saclay,Universit\'e Paris Diderot, Sorbonne Paris Cit\'eUniversit\'e de Lyon, Universit\'e Claude Bernard Lyon 1, CNRS/IN2P3, IP2I,University of Cincinnati, Clermont CollegeUniversidad Nacional de Educaci\'on Enrique Guzm\'an y ValleIFIC, CSIC-UV91.89.82.Universit´e de Paris-SaclayUniversit¨at Zu¨richUniversità di FerraraUniversita di ParmaUniversită di GenovaUniversity of Minnesota DuluthAix-Marseille Université, CNRS/IN2P3, CPPMUniversité Grenoble Alpes, CNRS, Grenoble INP, LPSC-IN2P3Universita di Roma ‘La Sapienza’Universite de Geneve“Sapienza" Università di Roma
This document presents the concept and physics case for a magnetized gaseous argon-based detector system (ND-GAr) for the Deep Underground Neutrino Experiment (DUNE) Near Detector. This detector system is required in order for DUNE to reach its full physics potential in the measurement of CP violation and in delivering precision measurements of oscillation parameters. In addition to its critical role in the long-baseline oscillation program, ND-GAr will extend the overall physics program of DUNE. The LBNF high-intensity proton beam will provide a large flux of neutrinos that is sampled by ND-GAr, enabling DUNE to discover new particles and search for new interactions and symmetries beyond those predicted in the Standard Model.
INFN Sezione di NapoliUniversity of Waterloo logoUniversity of WaterlooImperial College London logoImperial College LondonUniversity of Chicago logoUniversity of ChicagoETH Zürich logoETH ZürichTexas A&M University logoTexas A&M UniversityJoint Institute for Nuclear ResearchColumbia University logoColumbia UniversityLancaster UniversityINFN Sezione di PisaCERN logoCERNPacific Northwest National LaboratoryUniversity of Tokyo logoUniversity of TokyoGran Sasso Science InstituteUniversity of California, Davis logoUniversity of California, DavisUniversity of Massachusetts AmherstFermi National Accelerator LaboratoryUniversity of HoustonUniversity of SheffieldPrinceton University logoPrinceton UniversityShandong University logoShandong UniversityUniversity of Warwick logoUniversity of WarwickUniversidad de ZaragozaAlma Mater Studiorum - Università di BolognaUniversidade Federal do ABCUniversity of DelawareUniversità di GenovaUniversità di Milano-BicoccaPolitecnico di TorinoUniversity of SussexUniversity of BirminghamUniversity of Groningen logoUniversity of GroningenAix Marseille UniversityJagiellonian UniversityINFN, Laboratori Nazionali del Gran SassoTRIUMFRoyal Holloway, University of LondonLawrence Livermore National LaboratoryINFN, Sezione di TorinoNRC “Kurchatov Institute” – IHEPUniversity of RijekaUniversity of Hawai’iSkobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State UniversityNational Centre for Nuclear ResearchCIEMATGSSI-Gran Sasso Science InstituteTomsk Polytechnic UniversityInstitute for Nuclear Research of the Russian Academy of SciencesSNOLABLaurentian UniversityINFN-Sezione di GenovaAugustana UniversityINFN, Sezione di CataniaUniversity of SilesiaINFN-Sezione di BolognaINFN Sezione di RomaUniversità di Cagliari2INFN Laboratori Nazionali del Sud1/2(4)37353629Università di MessinaUniversità degli Studi di Sassari611182515211020177INFN Sezione di Cagliari82313Università di Sassari31916229514243352SNOLAB Institute382843756674Université de Lyon, CNRS/IN2P3, IP2I846461484157584263514649813079INFN Sezione Roma Tre407627317355535456Université Paris Cité, CNRS, Astroparticule et Cosmologie505980673478707268602662St. Petersburg Nuclear Physics Institute39776544458347716932Università di Enna Kore82.Universit di Catania1∗Universit Claude Bernard Lyon 1Universit di PisaSapienza Universit di RomaUniversit di PadovaUniversit degli Studi di Napoli Federico IIUniversit degli Studi della Campania Luigi VanvitelliUniversit Di BolognaQueens ’ UniversityUniversit degli Studi Roma TreNational Research Centre “Kurchatov Institute”
DarkSide-20k (DS-20k) is a dark matter detection experiment under construction at the Laboratori Nazionali del Gran Sasso (LNGS) in Italy. It utilises ~100 t of low radioactivity argon from an underground source (UAr) in its inner detector, with half serving as target in a dual-phase time projection chamber (TPC). The UAr cryogenics system must maintain stable thermodynamic conditions throughout the experiment's lifetime of over 10 years. Continuous removal of impurities and radon from the UAr is essential for maximising signal yield and mitigating background. We are developing an efficient and powerful cryogenics system with a gas purification loop with a target circulation rate of 1000 slpm. Central to its design is a condenser operated with liquid nitrogen which is paired with a gas heat exchanger cascade, delivering a combined cooling power of more than 8 kW. Here we present the design choices in view of the DS-20k requirements, in particular the condenser's working principle and the cooling control, and we show test results obtained with a dedicated benchmarking platform at CERN and LNGS. We find that the thermal efficiency of the recirculation loop, defined in terms of nitrogen consumption per argon flow rate, is 95 % and the pressure in the test cryostat can be maintained within ±\pm(0.1-0.2) mbar. We further detail a 5-day cool-down procedure of the test cryostat, maintaining a cooling rate typically within -2 K/h, as required for the DS-20k inner detector. Additionally, we assess the circuit's flow resistance, and the heat transfer capabilities of two heat exchanger geometries for argon phase change, used to provide gas for recirculation. We conclude by discussing how our findings influence the finalisation of the system design, including necessary modifications to meet requirements and ongoing testing activities.
The Agent Based Model community has a rich and diverse ecosystem of libraries, platforms, and applications to help modelers develop rigorous simulations. Despite this robust and diverse ecosystem, the complexity of life from microbial communities to the global ecosystem still presents substantial challenges in making reusable code that can optimize the ability of the knowledge-sharing and reproducibility. This research seeks to provide new tools to mitigate some of these challenges by offering a vision of a more holistic ecosystem that takes researchers and practitioners from the data collection through validation, with transparent, accessible, and extensible subcomponents. This proposed approach is demonstrated through two data pipelines (crop yield and synthetic population) that take users from data download through the cleaning and processing until users of have data that can be integrated into an ABM. These pipelines are built to be transparent: by walking users step by step through the process, accessible: by being skill scalable so users can leverage them without code or with code, and extensible by being freely available on the coding sharing repository GitHub to facilitate community development. Reusing code that simulates complex phenomena is a significant challenge but one that must be consistently addressed to help the community move forward. This research seeks to aid that progress by offering potential new tools extended from the already robust ecosystem to help the community collaborate more effectively internally and across disciplines.
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