General conditions for full abstraction

2014 ◽  
Vol 26 (4) ◽  
pp. 655-657 ◽  
Author(s):  
JOACHIM PARROW

Full abstraction, i.e. that a function preserves equivalence from a source to a target, has been used extensively as a correctness criterion for mappings between models of computation. I here show that with fixed equivalences, fully abstract functions almost always exist. Also, with the function and one of the equivalences fixed the other equivalence can almost always be found.

1993 ◽  
Vol 76 (3_suppl) ◽  
pp. 1283-1286 ◽  
Author(s):  
Giovanni Bruno Vicario ◽  
Elena Zambianchi

In 1988 Greene noted, if a straight pair of obliques are drawn outside of two orthogonal lines, the segments appear to be angled slightly one relative to the other. This illusion, designated as “corner Poggendorff,” is different from the Poggendorff effect (the two obliques seem to lie on a parallel path). The results of the present experiments ( N = 76 students) suggest that the general conditions for the corner Poggendorff are similar to those for the Judd illusion.


2002 ◽  
Vol 39 (03) ◽  
pp. 650-656
Author(s):  
Ludwig Baringhaus ◽  
Rudolf Grübel

We generalize Banach's matchbox problem: demands of random size are made on one of two containers, both initially with content t, where the container is selected at random in the successive steps. Let Z t be the content of the other container at the moment when the selected container is found to be insufficient. We obtain the asymptotic distribution of Z t as t → ∞ under quite general conditions. The case of exponentially distributed demands is considered in more detail.


2019 ◽  
Vol 53 (3-4) ◽  
pp. 153-206
Author(s):  
Xian Xu

Parameterization extends higher-order processes with the capability of abstraction and application (like those in lambda-calculus). As is well-known, this extension is strict, meaning that higher-order processes equipped with parameterization are strictly more expressive than those without parameterization. This paper studies strictly higher-order processes (i.e., no name-passing) with two kinds of parameterization: one on names and the other on processes themselves. We present two main results. One is that in presence of parameterization, higher-order processes can interpret first-order (name-passing) processes in a quite elegant fashion, in contrast to the fact that higher-order processes without parameterization cannot encode first-order processes at all. We present two such encodings and analyze their properties in depth, particularly full abstraction. In the other result, we provide a simpler characterization of the standard context bisimilarity for higher-order processes with parameterization, in terms of the normal bisimilarity that stems from the well-known normal characterization for higher-order calculus. As a spinoff, we show that the bisimulation up-to context technique is sound in the higher-order setting with parameterization.


Mathematika ◽  
2019 ◽  
Vol 65 (4) ◽  
pp. 1074-1092
Author(s):  
Robert Brignall ◽  
Vít Jelínek ◽  
Jan Kynčl ◽  
David Marchant

We show that if a permutation $\unicode[STIX]{x1D70B}$ contains two intervals of length 2, where one interval is an ascent and the other a descent, then the Möbius function $\unicode[STIX]{x1D707}[1,\unicode[STIX]{x1D70B}]$ of the interval $[1,\unicode[STIX]{x1D70B}]$ is zero. As a consequence, we prove that the proportion of permutations of length $n$ with principal Möbius function equal to zero is asymptotically bounded below by $(1-1/e)^{2}\geqslant 0.3995$. This is the first result determining the value of $\unicode[STIX]{x1D707}[1,\unicode[STIX]{x1D70B}]$ for an asymptotically positive proportion of permutations $\unicode[STIX]{x1D70B}$. We further establish other general conditions on a permutation $\unicode[STIX]{x1D70B}$ that ensure $\unicode[STIX]{x1D707}[1,\unicode[STIX]{x1D70B}]=0$, including the occurrence in $\unicode[STIX]{x1D70B}$ of any interval of the form $\unicode[STIX]{x1D6FC}\oplus 1\oplus \unicode[STIX]{x1D6FD}$.


1990 ◽  
Vol 1 (2) ◽  
pp. 177-187
Author(s):  
Pedro R. Marangunic ◽  
Mirta B. Stampella

We prove that in the Stefan problem with planar, cylindrical or spherical symmetry, with vanishing heat capacity and constant boundary temperature, no mushy region can appear, even in the presence of constant volumetric heat sources, if the initial data are consistent with the presence of just two pure phases. If the boundary temperature is not constant, a mushy region may or may not appear; we find some general conditions ensuring one case or the other and we give a specific example illustrating the appearance of a mushy region.


2002 ◽  
Vol 39 (3) ◽  
pp. 650-656
Author(s):  
Ludwig Baringhaus ◽  
Rudolf Grübel

We generalize Banach's matchbox problem: demands of random size are made on one of two containers, both initially with content t, where the container is selected at random in the successive steps. Let Zt be the content of the other container at the moment when the selected container is found to be insufficient. We obtain the asymptotic distribution of Zt as t → ∞ under quite general conditions. The case of exponentially distributed demands is considered in more detail.


2021 ◽  
Vol 2021 (5) ◽  
Author(s):  
Ilja Doršner ◽  
Svjetlana Fajfer ◽  
Ajla Lejlić

Abstract We introduce a novel mechanism for the leptoquark pair production at LHC that is of a t-channel topology and is quark-quark initiated. This mechanism operates under fairly general conditions. One of them is that the two leptoquarks in question couple to the same lepton and the other one is that the fermion numbers of these two leptoquarks differ by two. The strength of the proposed mechanism provides an alternative way to the conventional processes to efficiently constrain the parameter space of the two leptoquark scenarios at LHC whenever the aforementioned conditions are met. We accordingly present one case study to outline the physics potential of this novel production mechanism.


2021 ◽  
Vol 31 ◽  
Author(s):  
JEREMY G. SIEK ◽  
PETER THIEMANN ◽  
PHILIP WADLER

Abstract C#, Dart, Pyret, Racket, TypeScript, VB: many recent languages integrate dynamic and static types via gradual typing. We systematically develop four calculi for gradual typing and the relations between them, building on and strengthening previous work. The calculi are as follows: $\lambda{B}$ , based on the blame calculus of Wadler and Findler (2009); $\lambda{C}$ , inspired by the coercion calculus of Henglein (1994); $\lambda{S}$ inspired by the space-efficient calculus of Herman, Tomb, and Flanagan (2006); and $\lambda{T}$ based on the threesome calculus of Siek and Wadler (2010). While $\lambda{B}$ and $\lambda{T}$ are little changed from previous work, $\lambda{C}$ and $\lambda{S}$ are new. Together, $\lambda{B}$ , $\lambda{C}$ , $\lambda{S}$ , and $\lambda{T}$ provide a coherent foundation for design, implementation, and optimization of gradual types. We define translations from $\lambda{B}$ to $\lambda{C}$ , from $\lambda{C}$ to $\lambda{S}$ , and from $\lambda{S}$ to $\lambda{T}$ . Much previous work lacked proofs of correctness or had weak correctness criteria; here we demonstrate the strongest correctness criterion one could hope for, that each of the translations is fully abstract. Each of the calculi reinforces the design of the others: $\lambda{C}$ has a particularly simple definition, and the subtle definition of blame safety for $\lambda{B}$ is justified by the simple definition of blame safety for $\lambda{C}$ . Our calculus $\lambda{S}$ is implementation-ready: the first space-efficient calculus that is both straightforward to implement and easy to understand. We give two applications: first, using full abstraction from $\lambda{C}$ to $\lambda{S}$ to establish an equational theory of coercions; and second, using full abstraction from $\lambda{B}$ to $\lambda{S}$ to easily establish the Fundamental Property of Casts, which required a custom bisimulation and six lemmas in earlier work.


Derrida Today ◽  
2015 ◽  
Vol 8 (2) ◽  
pp. 136-155
Author(s):  
Michal Ben-Naftali

The essay examines Scholem's letter-confession on the Hebrew language addressed to Rosenzweig from two perspectives hitherto ignored in the ongoing interpretative consideration of this document: Scholem's repression of the literary space and his consequent exclusion of madness. The essay follows several threads in Derrida's own ‘internal’ reading of the letter, and leans on other Derridean writings such as The Monolingualism of the Other, Schibboleth: For Paul Celan and ‘Cogito and the History of Madness’ in order to suggest two distinct encounters between Derrida and Scholem: In the first encounter, Scholem reads Derrida and proves to be deconstructing his own notions of secular and profane Hebrew, while fighting in vain for his sanity by clinging to liturgical practices against the grain of an ongoing ‘actualization’, politicization or else fictionalization of the sacred language. In the second encounter, it is Derrida who reads Scholem. By transforming the particular conditions of possibility of Hebrew into general conditions of possibility of every language contaminated by a theological-political tension, Derrida contributes some important insights for contemporary Hebrew speakers.


The chief part of the following investigation (Sects, i. and iii.) was undertaken with the view of discovering whether it was possible to imagine a kind of vortex motion which would impress a gyrostatic quality which the forms of vortex aggregates hitherto known do not possess. The other part (Sect, ii.) deals with the nongyrostatic vortex aggregates, the discovery of which we owe to Hill, and investigates the conditions under which two or more aggregates may be combined into one. It is shown that it is allowable to suppose one or more concentric shells of vortex aggregates to be applied over a central spherical nucleus, subject to one relation between the radii and the vorticities. In all cases the vorticities must be in opposite directions in alternate shells. The special case when the aggregates are built up of the same vortical matter is considered, and the magnitudes of the radii and the positions of the equatorial axes determined. The cases of motion in a rigid spheroidal shell and of dyad spheroidal aggregates are also considered. The chief part of the paper refers to gyrostatic aggregates. The investigation has brought to light an entirely new system of spiral vortices. The general conditions for the existence of such systems, when the motion is symmetrical about an axis, are determined in Sect, i., and are worked out in more detail for a particular case of spherical aggregate in Sect. iii. It is found that the motion in meridian planes is determined from a certain function ψ in the usual manner. The velocity along a parallel of latitude is given by v = f(ψ) / ρ where p is the distance of the point from the axis. The function ψ , however, does not depend on the differential equation of the ordinary non-spiral type, but is a solution of the equation d 2 ψ / dr 2 + 1/ r 2 d 2 ψ / dθ 2 - cot θ / r 2 dψ / dθ = ρ 2 F - f df / dψ , where F and f are both functions of ψ . The case F and fdf/dψ both uniform is briefly treated. It refers to a spiral aggregate with a central solid nucleus, and is not of great interest. The case F uniform and fee f∝ψ is treated more fully. If ≡ λψ/a where a is the radius of the aggregate ψ = A { J 2 ( λr/a )- ( r 2 /a 2 ) J 2 λ } sin 2 θ.


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