scholarly journals Algebraic hull of maximal measurable cocycles of surface groups into Hermitian Lie groups

Author(s):  
A. Savini

AbstractFollowing the work of Burger, Iozzi and Wienhard for representations, in this paper we introduce the notion of maximal measurable cocycles of a surface group. More precisely, let $$\mathbf {G}$$ G be a semisimple algebraic $${\mathbb {R}}$$ R -group such that $$G=\mathbf {G}({\mathbb {R}})^{\circ }$$ G = G ( R ) ∘ is of Hermitian type. If $$\Gamma \le L$$ Γ ≤ L is a torsion-free lattice of a finite connected covering of $$\mathrm{PU}(1,1)$$ PU ( 1 , 1 ) , given a standard Borel probability $$\Gamma $$ Γ -space $$(\Omega ,\mu _\Omega )$$ ( Ω , μ Ω ) , we introduce the notion of Toledo invariant for a measurable cocycle $$\sigma :\Gamma \times \Omega \rightarrow G$$ σ : Γ × Ω → G . The Toledo invariant remains unchanged along G-cohomology classes and its absolute value is bounded by the rank of G. This allows to define maximal measurable cocycles. We show that the algebraic hull $$\mathbf {H}$$ H of a maximal cocycle $$\sigma $$ σ is reductive and the centralizer of $$H=\mathbf {H}({\mathbb {R}})^{\circ }$$ H = H ( R ) ∘ is compact. If additionally $$\sigma $$ σ admits a boundary map, then H is of tube type and $$\sigma $$ σ is cohomologous to a cocycle stabilizing a unique maximal tube type subdomain. This result is analogous to the one obtained for representations. In the particular case $$G=\mathrm{PU}(n,1)$$ G = PU ( n , 1 ) maximality is sufficient to prove that $$\sigma $$ σ is cohomologous to a cocycle preserving a complex geodesic. We conclude with some remarks about boundary maps of maximal Zariski dense cocycles.

Author(s):  
F. Sarti ◽  
A. Savini

AbstractLet $$\Gamma $$ Γ be a torsion-free lattice of $$PU (p,1)$$ P U ( p , 1 ) with $$p \ge 2$$ p ≥ 2 and let $$(X,\mu _X)$$ ( X , μ X ) be an ergodic standard Borel probability $$\Gamma $$ Γ -space. We prove that any maximal Zariski dense measurable cocycle $$\sigma : \Gamma \times X \longrightarrow SU (m,n)$$ σ : Γ × X ⟶ S U ( m , n ) is cohomologous to a cocycle associated to a representation of $$PU (p,1)$$ P U ( p , 1 ) into $$SU (m,n)$$ S U ( m , n ) , with $$1 \le m \le n$$ 1 ≤ m ≤ n . The proof follows the line of Zimmer’ Superrigidity Theorem and requires the existence of a boundary map, that we prove in a much more general setting. As a consequence of our result, there cannot exist maximal measurable cocycles with the above properties when $$1< m < n$$ 1 < m < n .


Geophysics ◽  
2003 ◽  
Vol 68 (4) ◽  
pp. 1380-1388 ◽  
Author(s):  
Changsoo Shin ◽  
Seungwon Ko ◽  
Wonsik Kim ◽  
Dong‐Joo Min ◽  
Dongwoo Yang ◽  
...  

We present a new, fast 3D traveltime calculation algorithm that employs existing frequency‐domain wave‐equation downward‐continuation software. By modifying such software to solve for a few complex (rather than real) frequencies, we are able to calculate not only the first arrival and the approximately most energetic traveltimes at each depth point but also their corresponding amplitudes. We compute traveltimes by either taking the logarithm of displacements obtained by the one‐way wave equation at a frequency or calculating derivatives of displacements numerically. Amplitudes are estimated from absolute value of the displacement at a frequency. By using the one‐way downgoing wave equation, we also circumvent generating traveltimes corresponding to near‐surface upcoming head waves not often needed in migration. We compare the traveltimes computed by our algorithm with those obtained by picking the most energetic arrivals from finite‐difference solutions of the one‐way wave equation, and show that our traveltime calculation method yields traveltimes comparable to solutions of the one‐way wave equation. We illustrate the accuracy of our traveltime algorithm by migrating the 2D IFP Marmousi and the 3D SEG/EAGE salt models.


2011 ◽  
Vol 3 (2) ◽  
pp. 56-63
Author(s):  
Rimantas Belevičius ◽  
Darius Mačiūnas ◽  
Dmitrij Šešok

The aim of the article is to report a technology for the optimization of grillage-type foundations seeking for the least possible reactive forces in the piles for a given number of piles and in the absolute value of the bending moments when connecting beams of the grillage. Mathematically, this seems to be the global optimization problem possessing a large number of local minima points. Both goals can be achieved choosing appropriate pile positions under connecting beams; however, these two problems contradict to each other and lead to diff erent schemes for pile placement. Therefore, we suggest using a compromise objective function (to be minimized) that consists of the largest reactive force arising in all piles and that occurring in the absolute value of the bending moment when connecting beams, both with the given weights. Bending moments are calculated at three points of each beam. The design parameters of the problem are positions of the piles. The feasible space of design parameters is determined by two constraints. First, during the optimization process, piles can move only along connecting beams. Therefore, the two-dimensional grillage is “unfolded” to the one-dimensional construct, and supports are allowed to range through this space freely. Second, the minimum allowable distance between two adjacent piles is introduced due to the specific capacities of a pile driver. Also, due to some considerations into the scheme of pile placement, the designer sometimes may introduce immovable supports (usually at the corners of the grillage) that do not participate in the optimization process and always retain their positions. However, such supports hinder to achieve a global solution to a problem and are not treated in this paper. The initial data for the problem are as follows: a geometrical scheme of the grillage, the given number of piles, a cross-section and material data on connecting beams, the minimum possible distance between adjacent supports and loading data given in the form of concentrated loads or trapezoidal distributed loadings. The results of the solution are the required positions of piles. This solution can serve as a pilot project for more detailed design. The entire optimization problem is solved in two steps. First, the grillage is transformed into the one-dimensional construct and the optimizer decides about a routine solution (i.e. the positions of piles in this construct). Second, backward transformation returns pile positions into the two-dimensional grillage and the “black-box” finite element program returns the corresponding objective function value. On the basis of this value, the optimizer predicts new positions of piles etc. The finite element program idealizes connecting beams as beam elements and piles – as mesh nodes of the finite element with a given boundary conditions in the form of vertical and rotational stiff ness. Since the problem may have several tens of design parameters, the only choice for optimization algorithms is using stochastic optimization algorithms. In our case, we use the original elitist real-number genetic algorithm and launch the program sufficient number of times in order to exclude large scattering of results. Three numerical examples are presented for the optimization of 10-pile grillage: when optimizing purely the largest reactive force, purely the largest in the absolute value of the bending moment and both parameters with equal weights.


2010 ◽  
Vol 172 (1) ◽  
pp. 517-566 ◽  
Author(s):  
Marc Burger ◽  
Alessandra Iozzi ◽  
Anna Wienhard

2014 ◽  
Vol 48 (1) ◽  
Author(s):  
Riaan Rheeder

God did not create once and then put an end to it. Testimony from Scripture shows that God continuously establishes or creates new things. Humans can therefore expect to always see and experience new things in creation. With this pattern of reasoning, one can anticipate that the human being as image of God will continuously establish new things in history. Although nature has value, it does not have absolute value and therefore it can be synthesised responsibly. The thought that humans are stewards of God is no longer adequate to, theologically put into words, the relationship human beings have with nature. New biotechnological developments ask for different answers from Scripture. Several ethicists are of the opinion that the theological construction of humans and created co-creators can help found the relationship of the human being to nature. Humans developed as God’s image evolutionary. On the one hand, this means humans themselves are a product of nature. On the other hand, the fact that humans are the image of God is also an ethical call that humans, like God, have to develop and create new things throughout history. Synthetic biology can be evaluated as technology that is possible, because humans are the image of God. However, it should, without a doubt, be executed responsibly.Sintetiese biologie eties geëvalueer: Die skeppende God en medeskeppende mens. God het nie net eenmaal geskep en daar gestop nie. Uit Skrifgetuienisse kan afgelei word dat God voortdurend nuwe dinge tot stand bring of skep. Daarom kan die mens verwag om gedurig nuwe dinge in die skepping te sien en te beleef. Hiermee saam kan verwag word dat die mens as beeld van God voortdurend nuwe dinge in die geskiedenis tot stand sal bring. Alhoewel die natuur waarde het, het dit nie absolute waarde nie en kan dus verantwoordelik gesintetiseer word. Die gedagte dat die mens rentmeester van God is, is nie meer voldoende om die mens se verhouding tot die natuur teologies te verwoord nie. Nuwe biotegnologiese ontwikkelinge vra na ander antwoorde vanuit die Skrif. Verskeie etici is van mening dat die teologiese konstruksie van die mens as geskepte medeskepper kan help om die mens se verhouding tot die natuur te begrond. Die mens het deur ’n evolusionêre proses tot God se beeld ontwikkel. Aan die een kant beteken dit dat die mens self ’n produk van die natuur is. Aan die ander kant is beeldskap ook ’n etiese oproep dat die mens, soos God, nuwe dinge in die geskiedenis moet ontwikkel en skep. Sintetiese biologie kan gesien word as tegnologie wat moontlik is omdat die mens na die beeld van God geskape is. Sonder twyfel moet sintetiese biologie egter verantwoordelik beoefen word.


1954 ◽  
Vol 21 (3) ◽  
pp. 291-293
Author(s):  
G. A. Zizicas

Abstract A nomogram constructed exclusively by means of straight lines is presented, giving the ratio of the octahedral to the maximum shearing stresses for all possible stress distributions in terms of the nondimensional ratios of the two principal stresses to the one of maximum absolute value. The physical interpretation of the nomogram is discussed. It is shown that states of stress with constant ratio of octahedral to maximum shearing stress are represented by straight lines. To such lines are found to correspond fixed values of the deviatoric parameter μ = 2 S 2 - S 1 - S 3 S 1 - S 3 in agreement with a recent observation by Novozhilov. The values of μ are given directly by the nomogram.


PMLA ◽  
1988 ◽  
Vol 103 (5) ◽  
pp. 739-748 ◽  
Author(s):  
Stanley Fish

WHEN members of an institution debate, it may seem that they are arguing about fundamental principles, but it is more often the case that the truly fundamental principle is the one that makes possible the terms of the disagreement and is therefore not in dispute at all. I am thinking in particular of the arguments recently marshaled for and against blind submission to the journal of the Modern Language Association. Blind submission is the practice whereby an author's name is not revealed to the reviewer who evaluates his or her work. It is an attempt, as William Schaefer explained in the MLA Newsletter, “to ensure that in making their evaluations readers are not influenced by factors other than the intrinsic merits of the article” (4). In his report to the members, Schaefer, then executive director of the association, declared that he himself was opposed to blind submission because the impersonality of the practice would erode the humanistic values that are supposedly at the heart of our enterprise. Predictably, Schaefer's statement provoked a lively exchange in which the lines of battle were firmly, and, as I will argue, narrowly, drawn. On the one hand those who agreed with Schaefer feared that a policy of anonymous review would involve a surrender “to the spurious notions about objectivity and absolute value that … scientists and social scientists banter about”; on the other hand those whose primary concern was with the fairness of the procedure believed that “[j]ustice should be blind” (“Correspondence” 4). Each side concedes the force of the opposing argument—the proponents of anonymous review admit that impersonality brings its dangers, and the defenders of the status quo acknowledge that it is important to prevent “extraneous considerations” from interfering with the identification of true merit (5).


1990 ◽  
Vol 05 (13) ◽  
pp. 2677-2686 ◽  
Author(s):  
RAYMOND K. SHELINE ◽  
P. C. SOOD

The inverted odd-even staggering of the differential radii of the Eu isotopes from neutron number 88 through 93, and the Kπ = 5/2± parity doublets with magnetic moments tending towards the hybridized limit and with connecting enhanced El transitions in l55 Eu and 153 Eu suggest the existence of intrinsic reflection asymmetry in the ground state of the Eu isotopes. The average splitting energy between 3 parity doublets in 155 Eu is 63.8 keV, while it is 97.4 keV for the one parity doublet in 153 Eu . Decoupling parameters of the Kπ = 1/2± parity doublet bands in l55 Eu have opposite signs but are approaching the same absolute value as expected for intrinsic reflection asymmetric nuclei. However, the presence of the 3/2 [411] bands with octupole vibrations ~530 keV above also implies the coexistence of reflection symmetric spectra in the low energy regions of both 155 Eu and 153 Eu .


Author(s):  
Rakesh Yadav ◽  
Ellen Meeks ◽  
Graham Goldin ◽  
Stefano Orsino

A methodology has been developed for coupling the one-dimensional (1D) solution of flow inside the nonpermeable channels with the 3D outer flow in shell and tube type of configurations. In the proposed reacting channel, the 1D channels have detailed reactions while the outer 3D flow can be reactive or nonreactive. The channels are discretized into 1D grid points and a parabolic solver is used to solve the species transport and energy equations inside the channels. Since the walls of the channels are nonpermeable, the two zones are coupled only through the heat transfer. The current approach is tested and validated for a series of problems with increasing complexities. The predictions of the channel model (CM) are compared with 3D modeling of the channels and experimental data. The CM predictions are in excellent agreement with the fully resolved (FR) model with much less computational cost. The discussed methodology is useful for applications such as fuel reformers, hydrocarbon cracking furnaces, heat exchangers, etc.


Author(s):  
S. Tapatee ◽  
B. S. Kedukodi ◽  
S. Juglal ◽  
P. K. Harikrishnan ◽  
S. P. Kuncham

AbstractThe notion of a matrix nearring over an arbitrary nearring was introduced by (Meldrum and Walt Arch. Math. 47(4): 312–319, 1986). In this paper, we define the notions such as weakly $$\tau$$ τ -prime $$(\tau =0,c,3,e)$$ ( τ = 0 , c , 3 , e ) ideals of an N-group G,  which are the generalization of the classes of $$\tau$$ τ -prime ideals of G, and provide suitable examples to distinguish between the two classes. We extend the concept to obtain the one-one correspondence between weakly $$\tau$$ τ -prime ideals $$(\tau =0,c,3,e)$$ ( τ = 0 , c , 3 , e ) of N-group (over itself) and those of $$M_n(N)$$ M n ( N ) -group $$N^{n}$$ N n , where $$M_n(N)$$ M n ( N ) is the matrix nearring over the nearring N. Further, we prove the correspondence between weakly 2-absorbing ideals of these classes.


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