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Characterizing Subsurface Environments Using Borehole Magnetic Gradiometry. [PDF]
Asgharzadeh MF +3 more
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Capturing carbon monoxide-Accessing bis(boryl)ketones through direct B-B bond carbonylation. [PDF]
Beck E +4 more
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Numerical Calculations of Electric Response Properties Using the Bubbles and Cube Framework. [PDF]
Solala E +3 more
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Mathematical Notes of the Academy of Sciences of the USSR, 1984
In the present paper the author introduces the concept of almost slender modules, which is very useful for studying the Cartesian products of modules over a Dedekind domain. The ring R is called slender [see \textit{E. L. Lady}, Pac. J. Math. 49, 397-406 (1973; Zbl 0274.16015)] if for every homomorphism \(f: \prod^{\infty}_{i=1}A_ i\to R\), where ...
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In the present paper the author introduces the concept of almost slender modules, which is very useful for studying the Cartesian products of modules over a Dedekind domain. The ring R is called slender [see \textit{E. L. Lady}, Pac. J. Math. 49, 397-406 (1973; Zbl 0274.16015)] if for every homomorphism \(f: \prod^{\infty}_{i=1}A_ i\to R\), where ...
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1970
When we say in analytic geometry that a point has co-ordinates (x, y), the order in which x and y occur, in the symbol (x, y), is important: (1, 2) ≠ (2, 1). For this reason we call (x, y) an ordered pair. Moreover, x and y come from sets; in this case x, y ∈ R. This idea can be generalizedf as follows. Let 𝒰 be a universe.
H. B. Griffiths, Peter Hilton
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When we say in analytic geometry that a point has co-ordinates (x, y), the order in which x and y occur, in the symbol (x, y), is important: (1, 2) ≠ (2, 1). For this reason we call (x, y) an ordered pair. Moreover, x and y come from sets; in this case x, y ∈ R. This idea can be generalizedf as follows. Let 𝒰 be a universe.
H. B. Griffiths, Peter Hilton
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On the Discrepancy for Cartesian Products
Journal of the London Mathematical Society, 2000We prove that the discrepancy for the family of Cartesian products \(B_1\times B_2\subseteq \mathbb{R}^4\), where \(B_1\) and \(B_2\) are circular discs in the plane, is \(O(n^{1/4+\varepsilon})\) for an arbitrarily small constant \(\varepsilon>0\), i.e. essentially the same as that for discs in the plane.
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American Journal of Mathematics, 1969
0. Introduction. Let as be an arc in the interior In of the n-cell In and let X be the quotient space I"/ac obtained by shrinking a to a point. According to Kwun and Raymond [4], X X 12 is an (n + 2)-cell. The crucial tool in their proof is the result of Andrews-Curtis that, under the above conditions, In/a X R1 is homeomorphic to In XR1.
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0. Introduction. Let as be an arc in the interior In of the n-cell In and let X be the quotient space I"/ac obtained by shrinking a to a point. According to Kwun and Raymond [4], X X 12 is an (n + 2)-cell. The crucial tool in their proof is the result of Andrews-Curtis that, under the above conditions, In/a X R1 is homeomorphic to In XR1.
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