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S221266781300018X | Amodel are proposed for modeling data-centric Web services which are powered by relational databases and interact with users according to logical formulas specifying input constraints, control-flow constraints and state/output/action rules. The Linear Temporal First-Order Logic (LTL-FO) formulas over inputs, states, outputs and actions are used to express the properties to be verified.We have proven that automatic verification of LTL-FO properties of data-centric Web services under input-bounded constraints is decidable by reducing Web services to data-centric Web applications. Thus, we can verify Web service specifications using existing verifier designed for Web applications. | [
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S000926141301539X | In this Letter we revisit the Chesnavich model Hamiltonian [37] in the light of recent developments in TST. For barrierless systems such as ion–molecule reactions, the concepts of OTS and TTS can be clearly formulated in terms of well defined phase space geometrical objects. (For work on the phase space description of OTS, see Refs. [38–40].) The first goal of the present article is the identification of these notions with well defined phase space dividing surfaces attached to NHIMs. The second and main goal is an elucidation of the roaming phenomenon in the context of the Chesnavich model Hamiltonian. The associated potential function, possessing many features associated with a realistic molecular PES, leads to dynamics which clearly reveal the origins of the roaming effect. Based on our trajectory simulations, we show how the identification of the TTS and OTS DSs with periodic orbit dividing surfaces (PODS) provides the natural framework for analysis of the roaming mechanism. | [
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S0009261412013838 | Experimental studies of the dynamics of individual carbon atoms in graphene have been empowered by the recent progress in aberration-corrected transmission electron microscopy (AC-TEM) capable of sub-Ångstrom resolution. The examples include AC-TEM observations of the formation and annealing of Stone–Wales defects [1], edge reconstruction [2,3] and formation of a large hole in graphene sheet from a single vacancy defect [3]. The AC-TEM has been also exploited in visualization in real time of the process of self-assembly of graphene nanoribbons from molecular precursors [4,5] and formation of nanometre size hollow protrusion on the nanotube sidewall [6]. Based on AC-TEM observations of transformation of small finite graphene flake into fullerene, a new ‘top-down’ mechanism for the formation of fullerene under the electron beam radiation has been proposed [7]. The critical step in the proposed ‘top-down’ mechanism of the fullerene formation is creation of vacancies in small graphene flake as a result of knock-on damage by electrons of the imaging electron beam (e-beam). The subsequent formation of pentagons at the vacancy sites near the edge reduces the number of dangling bonds and triggers the curving process of graphene flake into a closed fullerene structure [7]. Thus, dynamic behaviour of vacancies near graphene edge plays a crucial role in explaining mechanisms of the e-beam assisted self-assembly and structural transformations in graphene-like structures. | [
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S0927025612000249 | The need for power generation industry to improve the thermal efficiency of power plant has led to the development of 9–12% Cr martensitic steels. The development of and research on P91 steels started since late 1970s and early 1990s, respectively [1]. The work has focussed on their creep strengths due to its intended application at high temperature. Recently, the introduction of more cyclic operation of power plant has introduced the possibility of fatigue problems. Bore cracking due to the effects of varying steam warming has been reported [2]. The temperature cycling causes thermal gradients between the inside and outside of components and this can cause cyclic stress levels to be of concerns. Recently, research on thermal–mechanical analysis of P91 has been carried out including the characterisation of the cyclic behaviour of the material using the two-layer and unified visco-plasticity models [3,4]. | [
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S003238610900086X | We deal with the intensity scattered by a random mixture of deuterated/hydrogenated PE chains. The algorithm used by us to evaluate the Kratky plots by sets of parallel polymer stems is very simplified. We checked it to be adequate in the reciprocal coordinate range under investigation [0<q(=4πsinθ/λ)≤0.25Å−1] comparing the results with more precise calculations. The scattering centres are identified with pseudo-atoms repeating after a constant distance of 1.27Å along straight lines coinciding with the stem axes, 100 scattering centres being placed on each stem; the scattering by atoms belonging to chain folds is neglected. The parallel stem axes are disposed according to a hexagonal setting – a rough approximation to the monoclinic, pseudo-hexagonal structure of PE – and the scattering centres have the same axial coordinates in all the stems. Defining an integer i going from 1 to the total number ns·100 of scattering centres, we have (q<1) [9](1A)q2·I(q)=C·(bH−bD)2∑i=1ns·100∑j=1ns·1004πqsin(q·dij)dij;dij2=Δij2+(zj−zi)2;q=2πsinθλwhere bH, bD respectively are the scattering lengths of hydrogen and deuterium, dij is the distance between C atoms, 2θ is the diffraction angle and λ the wavelength. The i-th C atom coordinate along the stem axis is zi and Δij is the distance between the stem axes where the atoms i and j belong. For all the stems we have the same set of zi coordinates. The sum in Eq. (1A) is extended to all the stems of the crystalline domain, see Figs. 2 and 10 for examples. | [
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S0009261415000974 | Within the range of temperatures chosen, alanine dipeptide exhibits very simple behaviour. This result is due to the relatively small number of physically relevant minima (seven were characterised using this force field and solvent model) and the larger potential energy spacing between the global minimum and higher energy minima. Indeed, cross-overs in the approximate global free energy minimum for this system (where the free energy of the second-lowest potential energy minimum becomes lower than that of the global potential energy minimum) in the harmonic approximation would occur at 1170K. In general, the harmonic prediction for the crossover temperature between two minima is(4)kBTxo=V1−V2ln((o2ν¯2κ)/(o1ν¯1κ)),from Eq. (3), which clearly illustrates the balance between potential energy and well entropy. | [
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S2212671612000704 | The load of beam pumping unit is changeable, which is often in a state of light load. Reducing a certain voltage can improve the power factor and efficiency of the beam pumping unit when in light load .We can change the voltage by changing the thyristor trigger angle. It is complex and unacceptable to analyze the change of the cycles of the load overall. So we can divide the load of the whole cycle into several equal parts, each can be thought of as a constant load. The most optimal voltage for the current load can be calculated by genetic algorithm. When each load is in the most optimal voltage, we can get the whole optimal voltage changeable rule. Then it produces the result of energy saving. | [
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S2212667812000664 | According to the shortcomings of long time and big errors about the moving plate recognition system, we present the moving plate recognition algorithm based on principal component analysis(PCA) color extraction. On the basis of the analysis of moving plate recognition system's basic principles, it introduces the basic principles and calculation steps about PCA extraction algorithm, and discusses the feasibility of applying the algorithm to PRS in the paper. The experimental results show that the algorithm has the advantages of faster speed and higher accuracy of recognition. The algorithm provides a new thought for the research on the moving plate recognition algorithm. | [
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S0031920113001222 | Seismic tomography is a powerful tool to investigate the deep structure under the volcanoes. With the recently rapid development of Chinese provincial seismic networks (Zheng et al., 2009, 2010) and some portable seismic arrays (Hetland et al., 2004; Duan et al., 2009; Lei et al., 2012b) around the volcanoes, it has become possible to image the detailed 3-D velocity structure under some of these volcanoes, where seismic stations are densely spaced. In this overview, we synthesize the results from the deep seismic images of the upper mantle under the Changbaishan, Tengchong, Hainan volcanoes as well as the Datong volcano (Fig. 1). We also evaluate the advantages of recently updated seismic tomographic techniques for deriving potential information. This work updates a previous review of Zhao and Liu (2010) on this topic, with more detailed synthesis of all the available information. | [
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S0021999113005603 | After all micro elements reach a relaxed steady-state, measurements are obtained using a cumulative averaging technique to reduce noise. Each micro element is divided into spatially-oriented bins in the y-direction in order to resolve the velocity and shear-stress profiles. Velocity in each bin is measured using the Cumulative Averaging Method (CAM) [24], while the stress tensor field is measured using the Irving–Kirkwood relationship [25]. A least-squares polynomial fit to the data is performed, which helps reduce noise further. The fit produces a continuous function that avoids stability issues arising from supplying highly fluctuating data to the macro solver. A least-squares fit is applied to an Nth order polynomial for the velocity profile in the core region, and an Mth order polynomial for the velocity profile in the constrained region:(16)〈ui,core〉=∑k=1Nbk,iyi′(N−k),for 0⩽yi′⩽hcore, and(17)〈ui,cs〉=∑k=1Mck,iyi″(M−k),for 0⩽yi″⩽hcs, where bk,i and ck,i are the coefficients of the polynomials used in the core micro region and constrained region respectively. An estimate of the new slip velocity uB for input to the macro solution (6) is taken directly from the compressed wall micro-element solution (16), at yi′=0. | [
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S2212667814001440 | In this paper, we present a tele-operated mobile robot system for old age surveillance. The robot operates in autonomous mode in which the robots navigates in the environment and search for unusual situation of elderly people. If a patient is lying on the floor, the robot informs the user. The user switches the control mode from autonomous to haptic based user control. In the autonomous mode, the robot utilizes the visual sensor and landmarks to monitor the entire environment. The robot is equipped microphone, speaker and monitor making it possible to communicate with the user in remote place. In addition, the robot utilizes the vital sensors to check the patient's condition. The preliminary surveillance experiments show a good performance. | [
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S2212667814000124 | Based on expectation-maximization algorithm, parameter estimation was proposed for data-driven nonlinear models in this work. On this basis, particle filters were used to approximately calculate integrals, deriving EM algorithm based on particle filter. And the effectiveness of using the proposed algorithm for the soft sensor of COx content in tail gas of PX oxidation side reactions was verified through simulation results. | [
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S0166218X1300348X | Max-linear programs have been used to describe optimisation problems for multiprocessor interactive systems. In some instances the variables used in this model are required to be integer; however, no method seems to exist for finding integer solutions to max-linear programs.For a generic class of matrices, we show that integer solutions to two-sided max-linear systems and programs can be found in polynomial time. For general matrices, we adapt the existing methods for finding real solutions to obtain algorithms for finding integer solutions. | [
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S0375960115004120 | Another remarkable feature of the quantum field treatment can be revealed from the investigation of the vacuum state. For a classical field, vacuum is realized by simply setting the potential to zero resulting in an unaltered, free evolution of the particle's plane wave (|ψI〉=|ψIII〉=|k0〉). In the quantized treatment, vacuum is represented by an initial Fock state |n0=0〉 which still interacts with the particle and yields as final state |ΨIII〉 behind the field region(19)|ΨI〉=|k0〉⊗|0〉⇒|ΨIII〉=∑n=0∞t0n|k−n〉⊗|n〉 with a photon exchange probability(20)P0,n=|t0n|2=1n!e−Λ2Λ2n The particle thus transfers energy to the vacuum field leading to a Poissonian distributed final photon number. Let's consider, for example, a superconducting resonant circuit as source of the field. The magnetic field along the axis of a properly shaped coil is well approximated by the rectangular form. A particle with a magnetic dipole moment passing through the coil then interacts with the circuit and excites it with a measurable loss of kinetic energy even if the circuit is initially uncharged and there is classically no field it can couple to. The phenomenon that vacuum in quantum field theory does not mean to “no influence” as known from Casimir forces or Lamb shift is clearly visible here as well. | [
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S0010938X15300512 | Anodizing processes are widely used for protecting aluminium alloys against corrosion [1]. The resultant films are composed of amorphous alumina and consist of a relatively thick, porous, outer region and a thinner, non-porous, inner region [2,3]. The porous region contains the major pores of the film, which extend from the film surface to the barrier layer. Near the film surface, shorter, incipient pores are also present, whose growth stopped in the early stages of anodizing. The diameter of the major pores and the thickness of the inner, barrier region are dependent on the potential applied during anodizing, with typical proportionalities of ∼1nmV−1 [3,4]. Studies of ionic migration in barrier-type and porous anodic alumina films have usually found a transport number of O2− ions of ∼0.6 [5,6]. During the formation of porous films, the outward migrating Al3+ ions, constituting the remainder of the ionic current, are ejected to the electrolyte at the pore bases [7]. The electronic current in the barrier region is generally considered to be negligible. The thickness of the barrier region, which is relatively constant during the growth of a film under either a constant potential or constant current density, is maintained by a balance between growth of the barrier layer by continued oxidation of the aluminium substrate and thinning of the barrier layer by either field-assisted dissolution of the alumina at the pore bases [8] or field-assisted flow of alumina from the barrier layer to the pore walls [9–13]. The pores may be widened toward the film surface by chemical dissolution to an extent dependent on the anodizing conditions. | [
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S0370269304008858 | The reason to investigate the BFKL and DGLAP equations in the case of supersymmetric theories is based on a common belief, that the high symmetry may significantly simplify the structure of these equations. Indeed, it was found in the leading logarithmic approximation (LLA) [10], that the so-called quasi-partonic operators in N=1 SYM are unified in supermultiplets with anomalous dimensions obtained from universal anomalous dimensions γuni(j) by shifting its arguments by an integer number. Further, the anomalous dimension matrices for twist-2 operators are fixed by the superconformal invariance [10]. Calculations in the maximally extended N=4 SYM, where the coupling constant is not renormalized, give even more remarkable results. Namely, it turns out, that here all twist-2 operators enter in the same multiplet, their anomalous dimension matrix is fixed completely by the super-conformal invariance and its universal anomalous dimension in LLA is proportional to Ψ(j−1)−Ψ(1), which means, that the evolution equations for the matrix elements of quasi-partonic operators in the multicolor limit Nc→∞ are equivalent to the Schrödinger equation for an integrable Heisenberg spin model [11,12]. In QCD the integrability remains only in a small sector of the quasi-partonic operators [13]. In the case of N=4 SYM the equations for other sets of operators are also integrable [14–16]. Evolution equations for quasi-partonic operators are written in an explicitly super-conformal form in Ref. [17]. | [
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S2212671612002351 | In this paper, a novel position estimation method of prism was proposed for single-lens stereovision system. The prism with multi faces was considered as a single optical system composed of some refractive planes. A transformation matrix which can express the relationship between an object point and its image by the refraction of prism was derived based on geometrical optics, and a mathematical model was introduced which can denote the position of prism with arbitrary faces only by 7 parameters. This model can extend the application of single-lens stereovision system using prism to a more widely area. Experimentation results are presented to prove the effectiveness and robustness of our proposed model. | [
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S1071581916300854 | We have developed a systematic, quantified understanding of a specific problem: the design of mobile-friendly unique identifiers. But our results also apply to the design of other text-based services. There has been a trend toward bespoke and adaptive keyboards (e.g., Dunlop and Levine, 2012; Karrenbauer and Oulasvirta, 2014; Leiva et al., 2015; Wiseman et al., 2013). More often than not, though, input devices are a fixed constraint in the design of a service. Most users are typing on the keyboard that came with their phone. Those keyboards have advantages, limitations and quirks. The mode-switching that most touchscreen keyboards require to reach numbers and capital letters is at the root of design improvements we propose in this paper. When designing services, it is vital to be aware of the fixed constraints of a system and to then focus on the aspects of a service's design that can be controlled. Making changes to input data in this way is a cheap, quick and easy way to improve user experience. | [
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S0003491615000433 | Nuclear theory devoted major efforts since 4 decades to describe thermalization in nuclear reactions, predominantly using semi-classical methods [13,14,10], in line with similar problems in quantum liquids [15,16]. There were attempts to develop improved molecular dynamics methods combining quantum features with a semi classical treatment of dynamical correlations [17,18]. Still, no clear-cut quantum approach is readily available yet, in spite of numerous formal attempts [19,20,10]. The field of clusters and nano structures is far younger but fast developing in relation to the ongoing developments of lasers and imaging techniques. Semiclassical approaches were also considered in the field to include some dynamical corrections [21,22] and could qualitatively describe dynamical processes. But such approaches are bound to simple metals with sufficiently delocalized wave functions, and thus smooth potentials justifying semiclassical approximations. The case of organic systems, in particular the much celebrated C60 [4,23], cannot be treated this way. Semi classical, and even classical approaches, can be used at very high excitations such as delivered by very intense laser pulses [2]. In such cases the system is blown up and details of its quantum mechanical features do not matter anymore. But for less violent scenarios, quantum shell effects cannot be ignored. | [
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S0895611116300684 | In the case of PSR applied to vessels, preservation of high curvature and branches (concavities) demands a high value of the d parameter, resulting in models with high number of polygons. To cope with this problem, Wu et al. (2013) evaluates a variant of PSR (in that work referred to as scale-adaptive [SA]), which includes curvature-dependent polygonization (e.g. increasing/decreasing the size of triangles according to the local curvature) (Wu et al., 2010). In Wu et al. (2013), other methods including MC (without smoothing and decimation) are evaluated with application to vessel modeling. The authors, point at SA as a suitable method for reconstruction of vessels with applications to surgery planning. The methods evaluated by Wu et al. (2013) could be also compared with another set of techniques (known as model-based methods) (Preim and Oeltze, 2008), widely used in the context of vessel modeling for surgery planning. | [
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S0098300413002720 | Artificial Neural Networks (ANN) have been widely used in science and engineering problems. They attempt to model the ability of biological nervous systems to recognize patterns and objects. ANN basic architecture consists of networks of primitive functions capable of receiving multiple weighted inputs that are evaluated in terms of their success at discriminating the classes in Τa. Different types of primitive functions and network configurations result in varying models (Hastie et al., 2009; Rojas, 1996). During training network connection weights are adjusted if the separation of inputs and predefined classes incurs an error. Convergence proceeds until the reduction in error between iterations reaches a decay threshold (Kotsiantis, 2007; Rojas, 1996). We use feed-forward networks with a single hidden layer of nodes, a so called Multi-Layer Perceptron (MLP) (Venables and Ripley, 2002), and select one of two possible parameters: size, the number nodes in the hidden layer. | [
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S0098300412001793 | MINERAL (MINeral ERror AnaLysis) is a new MATLAB® based program that provides mineral formula recalculations combined with the associated propagation of the analytical uncertainties. Methods are based on the work of Giamarita and Day (1990). However, additional features have been added to provide users with greater flexibility in data reporting. Many programs exist to recalculate wt% data into formula unit cations. Some generalized programs can be used to recalculate the formula of multiple minerals e.g. CALCMIN (Brandelik, 2009) and HYPER-FORM (De Bjerg et al., 1992). Other programs are mineral specific e.g. AMPH CLASS (Esawi, 2004) and PROBE AMPH (Tindle and Webb, 1994) for the recalculation of amphibole analyses; ILMAT (Lepage, 2003) for the recalculation of magnetite and ilmenite; and PX-NOM (Sturm, 2002) for the recalculation of pyroxene analyses. MINERAL provides a rapid method for the recalculation of multiple common minerals. However, its strength lies in the fact that is the first tool to incorporate the associated uncertainty propagation calculations. As these are performed concurrently with the standard recalculations, no additional time is needed to perform uncertainty propagation. While an understanding of the underlying calculations is strongly recommended, MINERAL is designed to allow users with little or no experience operating MATLAB® and/or performing mineral formula recalculations and uncertainty propagation to undertake both with ease. | [
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S0377025714001931 | Tack is an important property of a PSA as it quantifies its ability to form instantly a bond when brought into contact with a surface. The final adhesion and cohesive strength of the bond are influenced by numerous factors including the surface energies of the adhesive and substrate, dwell time, contact pressure, mechanical properties of the adhesive, as well as environmental conditions such as temperature and humidity [8]. Therefore, tack is important in many applications where an instant bond is required, however it is equally important when a ‘clean’ separation of the initially bonded surfaces is desirable. Many different methods for measuring the tack have been devised with the four main ones being the rolling ball, loop tack, quick stick and probe tack tests [9]. Each has its own advantages and disadvantages and the specific testing method should be selected based on the particular application. | [
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"type_": "Process"
},
{
"id": "T27",
"start": 1015,
"end": 1050,
"type": 0,
"type_": "Material"
},
{
"id": "T28",
"start": 1081,
"end": 1119,
"type": 2,
"type_": "Task"
},
{
"id": "T29",
"start": 1124,
"end": 1159,
"type": 2,
"type_": "Task"
},
{
"id": "T30",
"start": 1198,
"end": 1202,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T1",
"arg2": "T2",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T2",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
}
] |
Dataset Card for ScienceIE
Dataset Summary
ScienceIE is a dataset for the SemEval task of extracting key phrases and relations between them from scientific documents. A corpus for the task was built from ScienceDirect open access publications and was available freely for participants, without the need to sign a copyright agreement. Each data instance consists of one paragraph of text, drawn from a scientific paper. Publications were provided in plain text, in addition to xml format, which included the full text of the publication as well as additional metadata. 500 paragraphs from journal articles evenly distributed among the domains Computer Science, Material Sciences and Physics were selected. The training data part of the corpus consists of 350 documents, 50 for development and 100 for testing. This is similar to the pilot task described in Section 5, for which 144 articles were used for training, 40 for development and for 100 testing.
There are three subtasks:
- Subtask (A): Identification of keyphrases
- Given a scientific publication, the goal of this task is to identify all the keyphrases in the document.
- Subtask (B): Classification of identified keyphrases
- In this task, each keyphrase needs to be labelled by one of three types: (i) PROCESS, (ii) TASK, and (iii) MATERIAL.
- PROCESS: Keyphrases relating to some scientific model, algorithm or process should be labelled by PROCESS.
- TASK: Keyphrases those denote the application, end goal, problem, task should be labelled by TASK.
- MATERIAL: MATERIAL keyphrases identify the resources used in the paper.
- In this task, each keyphrase needs to be labelled by one of three types: (i) PROCESS, (ii) TASK, and (iii) MATERIAL.
- Subtask (C): Extraction of relationships between two identified keyphrases
- Every pair of keyphrases need to be labelled by one of three types: (i) HYPONYM-OF, (ii) SYNONYM-OF, and (iii) NONE.
- HYPONYM-OF: The relationship between two keyphrases A and B is HYPONYM-OF if semantic field of A is included within that of B. One example is Red HYPONYM-OF Color.
- SYNONYM-OF: The relationship between two keyphrases A and B is SYNONYM-OF if they both denote the same semantic field, for example Machine Learning SYNONYM-OF ML.
- Every pair of keyphrases need to be labelled by one of three types: (i) HYPONYM-OF, (ii) SYNONYM-OF, and (iii) NONE.
Note: The default config science_ie
converts the original .txt & .ann files to a dictionary format that is easier to use.
For every other configuration the documents were split into sentences using spaCy, resulting in a 2388, 400, 838 split. The id
consists of the document id and the example index within the document separated by an underscore, e.g. S0375960115004120_1
. This should enable you to reconstruct the documents from the sentences.
Supported Tasks and Leaderboards
- Tasks: Key phrase extraction and relation extraction in scientific documents
- Leaderboards: https://competitions.codalab.org/competitions/15898
Languages
The language in the dataset is English.
Dataset Structure
Data Instances
science_ie
An example of "train" looks as follows:
{
"id": "S221266781300018X",
"text": "Amodel are proposed for modeling data-centric Web services which are powered by relational databases and interact with users according to logical formulas specifying input constraints, control-flow constraints and state/output/action rules. The Linear Temporal First-Order Logic (LTL-FO) formulas over inputs, states, outputs and actions are used to express the properties to be verified.We have proven that automatic verification of LTL-FO properties of data-centric Web services under input-bounded constraints is decidable by reducing Web services to data-centric Web applications. Thus, we can verify Web service specifications using existing verifier designed for Web applications.",
"keyphrases": [
{
"id": "T1", "start": 24, "end": 58, "type": 2, "type_": "Task"
},
...,
{"id": "T3", "start": 245, "end": 278, "type": 1, "type_": "Process"},
{"id": "T4", "start": 280, "end": 286, "type": 1, "type_": "Process"},
...
],
"relations": [
{"arg1": "T4", "arg2": "T3", "relation": 1, "relation_": "Synonym-of"},
{"arg1": "T3", "arg2": "T4", "relation": 1, "relation_": "Synonym-of"}
]
}
subtask_a
An example of "train" looks as follows:
{
"id": "S0375960115004120_1",
"tokens": ["Another", "remarkable", "feature", "of", "the", "quantum", "field", "treatment", "can", "be", "revealed", "from", "the", "investigation", "of", "the", "vacuum", "state", "."],
"tags": [0, 0, 0, 0, 0, 1, 2, 2, 0, 0, 0, 0, 0, 0, 0, 0, 1, 2, 0]
}
subtask_b
An example of "train" looks as follows:
{
"id": "S0375960115004120_2",
"tokens": ["For", "a", "classical", "field", ",", "vacuum", "is", "realized", "by", "simply", "setting", "the", "potential", "to", "zero", "resulting", "in", "an", "unaltered", ",", "free", "evolution", "of", "the", "particle", "'s", "plane", "wave", "(", "|ψI〉=|ψIII〉=|k0", "〉", ")", "."],
"tags": [0, 0, 0, 0, 0, 1, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 0, 0, 0, 0, 0]
}
subtask_c
An example of "train" looks as follows:
{
"id": "S0375960115004120_3",
"tokens": ["In", "the", "quantized", "treatment", ",", "vacuum", "is", "represented", "by", "an", "initial", "Fock", "state", "|n0=0", "〉", "which", "still", "interacts", "with", "the", "particle", "and", "yields", "as", "final", "state", "|ΨIII", "〉", "behind", "the", "field", "region(19)|ΨI〉=|k0〉⊗|0〉⇒|ΨIII〉=∑n=0∞t0n|k−n〉⊗|n", "〉", "with", "a", "photon", "exchange", "probability(20)P0,n=|t0n|2=1n!e−Λ2Λ2n", "The", "particle", "thus", "transfers", "energy", "to", "the", "vacuum", "field", "leading", "to", "a", "Poissonian", "distributed", "final", "photon", "number", "."],
"tags": [[0, 0, ...], [0, 0, ...], ...]
}
Note: The tag sequence consists of vectors for each token, that encode what the relationship between that token and every other token in the sequence is for the first token in each key phrase.
ner
An example of "train" looks as follows:
{
"id": "S0375960115004120_4",
"tokens": ["Let", "'s", "consider", ",", "for", "example", ",", "a", "superconducting", "resonant", "circuit", "as", "source", "of", "the", "field", "."],
"tags": [0, 0, 0, 0, 0, 0, 0, 0, 1, 2, 2, 0, 0, 0, 0, 0, 0]
}
re
An example of "train" looks as follows:
{
"id": "S0375960115004120_5",
"tokens": ["In", "the", "quantized", "treatment", ",", "vacuum", "is", "represented", "by", "an", "initial", "Fock", "state", "|n0=0", "〉", "which", "still", "interacts", "with", "the", "particle", "and", "yields", "as", "final", "state", "|ΨIII", "〉", "behind", "the", "field", "region(19)|ΨI〉=|k0〉⊗|0〉⇒|ΨIII〉=∑n=0∞t0n|k−n〉⊗|n", "〉", "with", "a", "photon", "exchange", "probability(20)P0,n=|t0n|2=1n!e−Λ2Λ2n", "The", "particle", "thus", "transfers", "energy", "to", "the", "vacuum", "field", "leading", "to", "a", "Poissonian", "distributed", "final", "photon", "number", "."],
"arg1_start": 2,
"arg1_end": 4,
"arg1_type": "Task",
"arg2_start": 5,
"arg2_end": 6,
"arg2_type": "Material",
"relation": 0
}
Data Fields
science_ie
id
: the instance id of this document, astring
feature.text
: the text of this document, astring
feature.keyphrases
: the list of keyphrases of this document, alist
ofdict
.id
: the instance id of this keyphrase, astring
feature.start
: the character offset start of this keyphrase, anint
feature.end
: the character offset end of this keyphrase, exclusive, anint
feature.type
: the key phrase type of this keyphrase, a classification label.type_
: the key phrase type of this keyphrase, astring
feature.
relations
: the list of relations of this document, alist
ofdict
.arg1
: the instance id of the first keyphrase, astring
feature.arg2
: the instance id of the second keyphrase, astring
feature.relation
: the relation label of this instance, a classification label.relation_
: the relation label of this instance, astring
feature.
Keyphrase types:
{"O": 0, "Material": 1, "Process": 2, "Task": 3}
Relation types:
{"O": 0, "Synonym-of": 1, "Hyponym-of": 2}
subtask_a
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: the list of tags of this sentence marking a token as being outside, at the beginning, or inside a key phrase, alist
of classification labels.
{"O": 0, "B": 1, "I": 2}
subtask_b
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: the list of tags of this sentence marking a token as being outside a key phrase, or being part of a material, process or task, alist
of classification labels.
{"O": 0, "M": 1, "P": 2, "T": 3}
subtask_c
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: a vector for each token, that encodes what the relationship between that token and every other token in the sequence is for the first token in each key phrase, alist
of alist
of a classification label.
{"O": 0, "S": 1, "H": 2}
ner
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: the list of ner tags of this sentence, alist
of classification labels.
{"O": 0, "B-Material": 1, "I-Material": 2, "B-Process": 3, "I-Process": 4, "B-Task": 5, "I-Task": 6}
re
id
: the instance id of this sentence, astring
feature.token
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.arg1_start
: the 0-based index of the start token of the relation arg1 mention, anìnt
feature.arg1_end
: the 0-based index of the end token of the relation arg1 mention, exclusive, anìnt
feature.arg1_type
: the key phrase type of the end token of the relation arg1 mention, astring
feature.arg2_start
: the 0-based index of the start token of the relation arg2 mention, anìnt
feature.arg2_end
: the 0-based index of the end token of the relation arg2 mention, exclusive, anìnt
feature.arg2_type
: the key phrase type of the relation arg2 mention, astring
feature.relation
: the relation label of this instance, a classification label.
{"O": 0, "Synonym-of": 1, "Hyponym-of": 2}
Data Splits
Train | Dev | Test | |
---|---|---|---|
science_ie | 350 | 50 | 100 |
subtask_a | 2388 | 400 | 838 |
subtask_b | 2388 | 400 | 838 |
subtask_c | 2388 | 400 | 838 |
ner | 2388 | 400 | 838 |
re | 24558 | 4838 | 6618 |
Dataset Creation
Curation Rationale
Source Data
Initial Data Collection and Normalization
Who are the source language producers?
Annotations
Annotation process
Who are the annotators?
Personal and Sensitive Information
Considerations for Using the Data
Social Impact of Dataset
Discussion of Biases
Other Known Limitations
Additional Information
Dataset Curators
Licensing Information
Citation Information
@article{DBLP:journals/corr/AugensteinDRVM17,
author = {Isabelle Augenstein and
Mrinal Das and
Sebastian Riedel and
Lakshmi Vikraman and
Andrew McCallum},
title = {SemEval 2017 Task 10: ScienceIE - Extracting Keyphrases and Relations
from Scientific Publications},
journal = {CoRR},
volume = {abs/1704.02853},
year = {2017},
url = {http://arxiv.org/abs/1704.02853},
eprinttype = {arXiv},
eprint = {1704.02853},
timestamp = {Mon, 13 Aug 2018 16:46:36 +0200},
biburl = {https://dblp.org/rec/journals/corr/AugensteinDRVM17.bib},
bibsource = {dblp computer science bibliography, https://dblp.org}
}
Contributions
Thanks to @phucdev for adding this dataset.
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