Seminar Talk in 慶應数理オンラインセミナー (Keio MathSci Online Seminar) at Online
In this lecture, we introduce weakly proregular sequence by Schenzel, it is introduced to study whether there is an isomorphism between Čech cohomology and local cohomology. In [Sch03], he proved that for the Local cohomology and the Čech cohomology defined by the sequence
a
––
=
a
1
,
…
,
a
r
, there is an isomorphism between these cohomologies if and only if
a
––
is weakly proregular. We give an elementary proof of his theorem without using notions of derived category theory. This seminar is based on preprint (arXiv:2105.07652).
このセミナーでは,[Sch03] による弱副正則列 (weakly proregular
sequence) を紹介する.これは Noether 環において局所コホモロジーと Čech
コホモロジーの間に同型が存在するという定理を非 Noether 環に拡張するた
めに導入されたもので,Schenzel はこれらのコホモロジーを定義する点列
푎1, . . . , 푎푟 が弱副正則列であるとき,かつそのときに限り,これらのコホモ
ロジーの間に関手的な同型が存在することを証明した.この観点において,
上に述べた Noether 環における事実は Noether 環の任意の点列は弱副正則で
ある,という形で理解できる.Schenzel は導来圏の言葉を用いて証明を行っ
たが,本セミナーでは講演者のプレプリント [And21](arXiv:2105.07652) に
基づいて,Abel 圏の言葉のみを用いて説明する.
In this paper we consider the initial-boundary value problem for a nonlinear equation induced with respect to the mathematical models in mass production process with the one sided spring boundary condition by boundary feedback control. We establish the asymptotic behavior of solutions to this problem in time, and give an example and simulation to illustrate our results. Results of this paper are able to apply industrial parts such as a typical model widely used to represent threads, wires, magnetic tapes, belts, band saws, and so on.
This document provides an introduction to modeling fully-polarimetric phased array antennas in the electromagnetic far field. It defines the far field region and outlines simplifying assumptions used in the analysis. Maxwell's equations and their time-harmonic form are reviewed. The general form of the far field solution is presented using vector spherical harmonics. Examples of vector spherical harmonics for degrees l=0 to 3 are also provided.
Dynamical Systems Methods in Early-Universe CosmologiesIkjyot Singh Kohli
The document discusses applying dynamical systems methods to develop models of the early universe. Specifically, it discusses:
1. Applying these methods to the Einstein field equations to obtain cosmological models that are spatially homogeneous but anisotropic.
2. Describing the process of analyzing the dynamics of these models, which involves identifying invariant sets, equilibrium points, monotone functions, and bifurcations in the parameter space.
3. The importance of numerical methods in understanding the global behavior of these systems, since analytical methods are often limited to local analysis near equilibrium points.
We continue the study of the concepts of minimality and homogeneity in the fuzzy context. Concretely, we introduce two new notions of minimality in fuzzy bitopological spaces which are called minimal fuzzy open set and pairwise minimal fuzzy open set. Several relationships between such notions and a known one are given. Also, we provide results about the transformation of minimal, and pairwise minimal fuzzy open sets of a fuzzy bitopological space, via fuzzy continuous and fuzzy open mappings, and pairwise continuous and pairwise open mappings, respectively. Moreover, we present two new notions of homogeneity in the fuzzy framework. We introduce the notions of homogeneous and pairwise homogeneous fuzzy bitopological spaces. Several relationships between such notions and a known one are given. And, some connections between minimality and homogeneity are given. Finally, we show that cut bitopological spaces of a homogeneous (resp. pairwise homogeneous) fuzzy bitopological space are homogeneous (resp. pairwise homogeneous) but not conversely.
As a generalization of the concept SLH space, we introduce the concept of slightly strongly locally homogeneous (SSLH) spaces. Also, we introduce the concepts of slightly dense set as well as slightly separable space, and use them to introduce two new types of slightly countable dense homogeneous spaces. Several results, relationships, examples and counter-examples concerning these concepts are obtained.
Hopf-Bifurcation Ina Two Dimensional Nonlinear Differential EquationIJMER
This document discusses Hopf bifurcation in a two-dimensional nonlinear differential equation. It contains the following key points:
1. The paper investigates the stability of Hopf bifurcation in a two-dimensional nonlinear differential equation, finding both supercritical and subcritical Hopf bifurcation depending on parameter values.
2. The center manifold theorem and normal forms are used to study the behavior of limit cycles created or destroyed through Hopf bifurcations.
3. Hopf bifurcation refers to the creation or destruction of a periodic solution emanating from an equilibrium point as a parameter crosses a critical value. It is important for studying oscillatory behavior in nonlinear systems.
1) Stokes' theorem relates the curl of a vector field integrated over a surface S to the line integral of the vector field around the boundary curve C of the surface.
2) The document provides a proof of Stokes' theorem and gives an example of verifying it for a given vector field and surface.
3) Green's theorem relates the double integral of the curl of a vector field over a plane region R to the line integral of the vector field around the boundary curve C of the region. The theorem is demonstrated through an example.
This document summarizes research into non-supersymmetric heterotic string vacua that resemble the MSSM. The researchers sought models with 4D N=1 supersymmetry that break to N=0, containing the standard model gauge group and 3 generations of quarks and leptons. They presented an explicit tachyon-free model constructed from a set of boundary condition basis vectors without supersymmetry. This model separates the observable and hidden sectors as SO(10) and SO(16) respectively, and breaks to the standard model gauge group and additional U(1) factors. Future work aims to search for models with exponentially suppressed cosmological constants and cancellation of vacuum energy tadpoles.
In this paper we consider the initial-boundary value problem for a nonlinear equation induced with respect to the mathematical models in mass production process with the one sided spring boundary condition by boundary feedback control. We establish the asymptotic behavior of solutions to this problem in time, and give an example and simulation to illustrate our results. Results of this paper are able to apply industrial parts such as a typical model widely used to represent threads, wires, magnetic tapes, belts, band saws, and so on.
This document provides an introduction to modeling fully-polarimetric phased array antennas in the electromagnetic far field. It defines the far field region and outlines simplifying assumptions used in the analysis. Maxwell's equations and their time-harmonic form are reviewed. The general form of the far field solution is presented using vector spherical harmonics. Examples of vector spherical harmonics for degrees l=0 to 3 are also provided.
Dynamical Systems Methods in Early-Universe CosmologiesIkjyot Singh Kohli
The document discusses applying dynamical systems methods to develop models of the early universe. Specifically, it discusses:
1. Applying these methods to the Einstein field equations to obtain cosmological models that are spatially homogeneous but anisotropic.
2. Describing the process of analyzing the dynamics of these models, which involves identifying invariant sets, equilibrium points, monotone functions, and bifurcations in the parameter space.
3. The importance of numerical methods in understanding the global behavior of these systems, since analytical methods are often limited to local analysis near equilibrium points.
We continue the study of the concepts of minimality and homogeneity in the fuzzy context. Concretely, we introduce two new notions of minimality in fuzzy bitopological spaces which are called minimal fuzzy open set and pairwise minimal fuzzy open set. Several relationships between such notions and a known one are given. Also, we provide results about the transformation of minimal, and pairwise minimal fuzzy open sets of a fuzzy bitopological space, via fuzzy continuous and fuzzy open mappings, and pairwise continuous and pairwise open mappings, respectively. Moreover, we present two new notions of homogeneity in the fuzzy framework. We introduce the notions of homogeneous and pairwise homogeneous fuzzy bitopological spaces. Several relationships between such notions and a known one are given. And, some connections between minimality and homogeneity are given. Finally, we show that cut bitopological spaces of a homogeneous (resp. pairwise homogeneous) fuzzy bitopological space are homogeneous (resp. pairwise homogeneous) but not conversely.
As a generalization of the concept SLH space, we introduce the concept of slightly strongly locally homogeneous (SSLH) spaces. Also, we introduce the concepts of slightly dense set as well as slightly separable space, and use them to introduce two new types of slightly countable dense homogeneous spaces. Several results, relationships, examples and counter-examples concerning these concepts are obtained.
Hopf-Bifurcation Ina Two Dimensional Nonlinear Differential EquationIJMER
This document discusses Hopf bifurcation in a two-dimensional nonlinear differential equation. It contains the following key points:
1. The paper investigates the stability of Hopf bifurcation in a two-dimensional nonlinear differential equation, finding both supercritical and subcritical Hopf bifurcation depending on parameter values.
2. The center manifold theorem and normal forms are used to study the behavior of limit cycles created or destroyed through Hopf bifurcations.
3. Hopf bifurcation refers to the creation or destruction of a periodic solution emanating from an equilibrium point as a parameter crosses a critical value. It is important for studying oscillatory behavior in nonlinear systems.
1) Stokes' theorem relates the curl of a vector field integrated over a surface S to the line integral of the vector field around the boundary curve C of the surface.
2) The document provides a proof of Stokes' theorem and gives an example of verifying it for a given vector field and surface.
3) Green's theorem relates the double integral of the curl of a vector field over a plane region R to the line integral of the vector field around the boundary curve C of the region. The theorem is demonstrated through an example.
This document summarizes research into non-supersymmetric heterotic string vacua that resemble the MSSM. The researchers sought models with 4D N=1 supersymmetry that break to N=0, containing the standard model gauge group and 3 generations of quarks and leptons. They presented an explicit tachyon-free model constructed from a set of boundary condition basis vectors without supersymmetry. This model separates the observable and hidden sectors as SO(10) and SO(16) respectively, and breaks to the standard model gauge group and additional U(1) factors. Future work aims to search for models with exponentially suppressed cosmological constants and cancellation of vacuum energy tadpoles.
This document summarizes research into non-supersymmetric heterotic string vacua that resemble the MSSM. The researchers sought models with 4D N=1 supersymmetry that break to N=0, containing the standard model gauge group and 3 generations of quarks and leptons. They presented an explicit tachyon-free model constructed from fermionic strings using a set of boundary condition basis vectors and GGSO phases. This model separates the observable and hidden sectors but contains a mismatch between fermion and boson numbers requiring future work to cancel the vacuum energy.
Sequence Entropy and the Complexity Sequence Entropy For 𝒁𝒏ActionIJRES Journal
In this paper, we study the complexity of sequence entropy for 𝑍𝑛 actions. After that, we define 𝐶𝛼 𝐹𝛼 𝜏 , ℎ𝛼 𝐹𝛼 𝜏 and the relationships between sequence entropy and complexity sequence entropy. Finally, comparisons between sequence entropy and complexity sequence entropy have been done.
Homogeneous Components of a CDH Fuzzy SpaceIJECEIAES
We prove that fuzzy homogeneous components of a CDH fuzzy topological space (X,T) are clopen and also they are CDH topological subspaces of its 0-cut topological space (X,T0).
This document discusses quantum chaos in clean many-body systems. It begins by outlining the topic and noting that quantum chaos fits into many-body physics and statistical mechanics. It then discusses how the quantum chaos conjecture relates semiclassical physics to many-body systems. Specifically, it discusses how quantum ergodicity, decay of correlations, and Loschmidt echo relate to the integrability-breaking phase transition in spin chains. It also briefly mentions how quantum chaos appears in non-equilibrium steady states of open many-body systems.
Unit 1: Topological spaces (its definition and definition of open sets)nasserfuzt
Learning Objectives:
1. To understand the definition of topology with examples
2. To know the intersection and union of topologies
3. To understand the comparison of topologies
E. Canay and M. Eingorn
Physics of the Dark Universe 29 (2020) 100565
DOI: 10.1016/j.dark.2020.100565
https://authors.elsevier.com/a/1aydL7t6qq5DB0
https://arxiv.org/abs/2002.00437
Two distinct perturbative approaches have been recently formulated within General Relativity, arguing for the screening of gravity in the ΛCDM Universe. We compare them and show that the offered screening concepts, each characterized by its own interaction range, can peacefully coexist. Accordingly, we advance a united scheme, determining the gravitational potential at all scales, including regions of nonlinear density contrasts, by means of a simple Helmholtz equation with the effective cosmological screening length. In addition, we claim that cosmic structures may not grow at distances above this Yukawa range and confront its current value with dimensions of the largest known objects in the Universe.
1) The document discusses normal subgroups, providing examples and theorems about their properties.
2) A subgroup H of a group G is normal if aH=Ha for all a in G. Some key results are that subgroups of abelian groups and subgroups of index 2 are always normal.
3) The document provides examples of normal subgroups, such as the special linear group SLn,R being normal in the general linear group GLn,R. It also gives a counterexample to show not all groups where every subgroup is normal must be abelian.
This document provides an overview of preliminary topological concepts needed for applied mathematics. It defines topological spaces and metric spaces, and introduces key topological notions like open and closed sets, bases for topologies, convergence of sequences, accumulation points, interior and closure of sets, and dense sets. Metric spaces are shown to induce a natural topological structure, though not all topologies come from a metric. Examples are provided to illustrate various definitions and properties.
1) The document presents a new argument for proving that closed timelike curves cannot exist in physical spacetime.
2) It introduces spacetime as a four-dimensional manifold with a Lorentzian metric and performs an "ADM 3+1 split" to divide spacetime into spatial and temporal components.
3) The argument then defines what would constitute a "closed timelike curve" and proves that the coordinate shift introduced in the 3+1 split would eliminate any such curves, making spacetime globally hyperbolic without closed timelike curves.
A Probabilistic Algorithm for Computation of Polynomial Greatest Common with ...mathsjournal
- The document presents a probabilistic algorithm for computing the polynomial greatest common divisor (PGCD) with smaller factors.
- It summarizes previous work on the subresultant algorithm for computing PGCD and discusses its limitations, such as not always correctly determining the variant τ.
- The new algorithm aims to determine τ correctly in most cases when given two polynomials f(x) and g(x). It does so by adding a few steps instead of directly computing the polynomial t(x) in the relation s(x)f(x) + t(x)g(x) = r(x).
Phase locking in chains of multiple-coupled oscillatorsLiwei Ren任力偉
This document summarizes a research paper that studied phase locking in chains of oscillators with coupling beyond nearest neighbors. It introduced a model for such chains using piecewise linear coupling functions. The paper proved the existence of phase locked solutions for this model by using a homotopy method to smoothly transform the model into more realistic coupling functions. It discussed differences between models with multiple coupling versus nearest neighbor coupling only, and highlighted the importance of studying coupling beyond just the nearest neighbors seen in some biological systems.
This document discusses derivations on lattices. It begins with background definitions of lattices, distributive lattices, modular lattices, and derivations. It then introduces the notion of f(x∧y)=x∧fy for a derivation f on a lattice L. It establishes some equivalence relations using isotone derivations and extends previous results on isotone derivations for distributive lattices. Finally, it shows that the set of all isotone derivations on a modular lattice, with meet and join operations, forms a modular lattice.
This document discusses derivations on lattices. It begins with background definitions of lattices, distributive lattices, modular lattices, and derivations. It then introduces the notion of f(x⋀y) = x⋀fy for a derivation f on a lattice L. It establishes some equivalence relations using isotone derivations and extends previous results on isotone derivations for distributive lattices. Finally, it shows that the set of all isotone derivations on a modular lattice forms a modular lattice itself under the operations of meet and join.
1. The work done by a force F acting along a material path L can be calculated using the integral A = ∫_0^S F(s) ds, where s is the parameter of the path.
2. The mass of an object with non-uniform density ρ(x) along the x-axis between a and b can be found using the integral m = ∫_a^b ρ(x) dx.
3. The coordinates (xc, yc) of the centroid of a curve given in parametric form x=φ(t), y=ψ(t) between α and β can be determined using the integrals xc = ∫_α^
The document presents an axiomatic characterization of biological sequences. It defines sequences as abstract, information-bearing entities that are independent of physical implementation. Sequences are composed of parts, like regions and junctions, and the document provides a set of axioms describing the mereological relationships between sequences and their parts based on an equivalence relation over sequence tokens. The axioms are formally defined and intended to serve as a foundation for representing biological sequence data.
Stochastic Processes describe the system derived by noise.
Level of graduate students in mathematics and engineering.
Probability Theory is a prerequisite.
For comments please contact me at solo.hermelin@gmail.com.
For more presentations on different subjects visit my website at http://www.solohermelin.com.
Notes on intersection theory written for a seminar in Bonn in 2010.
Following Fulton's book the following topics are covered:
- Motivation of intersection theory
- Cones and Segre Classes
- Chern Classes
- Gauss-Bonet Formula
- Segre classes under birational morphisms
- Flat pull back
Regularisation & Auxiliary Information in OOD Detectionkirk68
Neural networks are often utilised in critical domain applications (e.g. self-driving cars, financial markets, and aerospace engineering), even though they exhibit overconfident predictions for ambiguous inputs. This deficiency demonstrates a fundamental flaw indicating that neural networks often overfit on spurious correlations. To address this problem in this work we present two objectives that improve the ability of a network to detect out-of-distribution samples and therefore avoid overconfident predictions for ambiguous inputs. We empirically demonstrate that our methods outperform the baseline and performs better than the majority of existing approaches, while still maintaining competitive with the remaining ones. Additionally, we empirically demonstrate the robustness of our approach against common corruptions showcasing the importance of regularisation and auxiliary information in out-of-distribution detection.
In tis slide, an introduction to string theory has been given. Apart from that, a simple proof of 26 dimensions of bosonic string theory is given (following Zwiebach's approach).
I explained this presentation in two parts (on my YouTube channel). Here are the links
_______________________________________________
Part 1
https://www.youtube.com/watch?v=QQA4JQ6Y-eo&list=PLDpqC3uXLZGl0cDod6g30PcjeJ4DAZWhp
_______________________________________________
Part 2
https://www.youtube.com/watch?v=vhLCtLn79jE&list=PLDpqC3uXLZGl0cDod6g30PcjeJ4DAZWhp&index=2
_______________________________________________
This document discusses orthogonal trajectories and provides examples of finding orthogonal trajectories for different families of curves. It begins by defining orthogonal trajectories as curves that intersect each other at right angles. It then provides a method for finding the differential equation that describes the orthogonal trajectories for a given family of curves. Several examples are worked out, such as finding the orthogonal trajectories of the family of parabolas with equation y = x^2. Applications to equipotential lines and electric fields and electromagnetic waves are also mentioned.
This document summarizes research into non-supersymmetric heterotic string vacua that resemble the MSSM. The researchers sought models with 4D N=1 supersymmetry that break to N=0, containing the standard model gauge group and 3 generations of quarks and leptons. They presented an explicit tachyon-free model constructed from fermionic strings using a set of boundary condition basis vectors and GGSO phases. This model separates the observable and hidden sectors but contains a mismatch between fermion and boson numbers requiring future work to cancel the vacuum energy.
Sequence Entropy and the Complexity Sequence Entropy For 𝒁𝒏ActionIJRES Journal
In this paper, we study the complexity of sequence entropy for 𝑍𝑛 actions. After that, we define 𝐶𝛼 𝐹𝛼 𝜏 , ℎ𝛼 𝐹𝛼 𝜏 and the relationships between sequence entropy and complexity sequence entropy. Finally, comparisons between sequence entropy and complexity sequence entropy have been done.
Homogeneous Components of a CDH Fuzzy SpaceIJECEIAES
We prove that fuzzy homogeneous components of a CDH fuzzy topological space (X,T) are clopen and also they are CDH topological subspaces of its 0-cut topological space (X,T0).
This document discusses quantum chaos in clean many-body systems. It begins by outlining the topic and noting that quantum chaos fits into many-body physics and statistical mechanics. It then discusses how the quantum chaos conjecture relates semiclassical physics to many-body systems. Specifically, it discusses how quantum ergodicity, decay of correlations, and Loschmidt echo relate to the integrability-breaking phase transition in spin chains. It also briefly mentions how quantum chaos appears in non-equilibrium steady states of open many-body systems.
Unit 1: Topological spaces (its definition and definition of open sets)nasserfuzt
Learning Objectives:
1. To understand the definition of topology with examples
2. To know the intersection and union of topologies
3. To understand the comparison of topologies
E. Canay and M. Eingorn
Physics of the Dark Universe 29 (2020) 100565
DOI: 10.1016/j.dark.2020.100565
https://authors.elsevier.com/a/1aydL7t6qq5DB0
https://arxiv.org/abs/2002.00437
Two distinct perturbative approaches have been recently formulated within General Relativity, arguing for the screening of gravity in the ΛCDM Universe. We compare them and show that the offered screening concepts, each characterized by its own interaction range, can peacefully coexist. Accordingly, we advance a united scheme, determining the gravitational potential at all scales, including regions of nonlinear density contrasts, by means of a simple Helmholtz equation with the effective cosmological screening length. In addition, we claim that cosmic structures may not grow at distances above this Yukawa range and confront its current value with dimensions of the largest known objects in the Universe.
1) The document discusses normal subgroups, providing examples and theorems about their properties.
2) A subgroup H of a group G is normal if aH=Ha for all a in G. Some key results are that subgroups of abelian groups and subgroups of index 2 are always normal.
3) The document provides examples of normal subgroups, such as the special linear group SLn,R being normal in the general linear group GLn,R. It also gives a counterexample to show not all groups where every subgroup is normal must be abelian.
This document provides an overview of preliminary topological concepts needed for applied mathematics. It defines topological spaces and metric spaces, and introduces key topological notions like open and closed sets, bases for topologies, convergence of sequences, accumulation points, interior and closure of sets, and dense sets. Metric spaces are shown to induce a natural topological structure, though not all topologies come from a metric. Examples are provided to illustrate various definitions and properties.
1) The document presents a new argument for proving that closed timelike curves cannot exist in physical spacetime.
2) It introduces spacetime as a four-dimensional manifold with a Lorentzian metric and performs an "ADM 3+1 split" to divide spacetime into spatial and temporal components.
3) The argument then defines what would constitute a "closed timelike curve" and proves that the coordinate shift introduced in the 3+1 split would eliminate any such curves, making spacetime globally hyperbolic without closed timelike curves.
A Probabilistic Algorithm for Computation of Polynomial Greatest Common with ...mathsjournal
- The document presents a probabilistic algorithm for computing the polynomial greatest common divisor (PGCD) with smaller factors.
- It summarizes previous work on the subresultant algorithm for computing PGCD and discusses its limitations, such as not always correctly determining the variant τ.
- The new algorithm aims to determine τ correctly in most cases when given two polynomials f(x) and g(x). It does so by adding a few steps instead of directly computing the polynomial t(x) in the relation s(x)f(x) + t(x)g(x) = r(x).
Phase locking in chains of multiple-coupled oscillatorsLiwei Ren任力偉
This document summarizes a research paper that studied phase locking in chains of oscillators with coupling beyond nearest neighbors. It introduced a model for such chains using piecewise linear coupling functions. The paper proved the existence of phase locked solutions for this model by using a homotopy method to smoothly transform the model into more realistic coupling functions. It discussed differences between models with multiple coupling versus nearest neighbor coupling only, and highlighted the importance of studying coupling beyond just the nearest neighbors seen in some biological systems.
This document discusses derivations on lattices. It begins with background definitions of lattices, distributive lattices, modular lattices, and derivations. It then introduces the notion of f(x∧y)=x∧fy for a derivation f on a lattice L. It establishes some equivalence relations using isotone derivations and extends previous results on isotone derivations for distributive lattices. Finally, it shows that the set of all isotone derivations on a modular lattice, with meet and join operations, forms a modular lattice.
This document discusses derivations on lattices. It begins with background definitions of lattices, distributive lattices, modular lattices, and derivations. It then introduces the notion of f(x⋀y) = x⋀fy for a derivation f on a lattice L. It establishes some equivalence relations using isotone derivations and extends previous results on isotone derivations for distributive lattices. Finally, it shows that the set of all isotone derivations on a modular lattice forms a modular lattice itself under the operations of meet and join.
1. The work done by a force F acting along a material path L can be calculated using the integral A = ∫_0^S F(s) ds, where s is the parameter of the path.
2. The mass of an object with non-uniform density ρ(x) along the x-axis between a and b can be found using the integral m = ∫_a^b ρ(x) dx.
3. The coordinates (xc, yc) of the centroid of a curve given in parametric form x=φ(t), y=ψ(t) between α and β can be determined using the integrals xc = ∫_α^
The document presents an axiomatic characterization of biological sequences. It defines sequences as abstract, information-bearing entities that are independent of physical implementation. Sequences are composed of parts, like regions and junctions, and the document provides a set of axioms describing the mereological relationships between sequences and their parts based on an equivalence relation over sequence tokens. The axioms are formally defined and intended to serve as a foundation for representing biological sequence data.
Stochastic Processes describe the system derived by noise.
Level of graduate students in mathematics and engineering.
Probability Theory is a prerequisite.
For comments please contact me at solo.hermelin@gmail.com.
For more presentations on different subjects visit my website at http://www.solohermelin.com.
Notes on intersection theory written for a seminar in Bonn in 2010.
Following Fulton's book the following topics are covered:
- Motivation of intersection theory
- Cones and Segre Classes
- Chern Classes
- Gauss-Bonet Formula
- Segre classes under birational morphisms
- Flat pull back
Regularisation & Auxiliary Information in OOD Detectionkirk68
Neural networks are often utilised in critical domain applications (e.g. self-driving cars, financial markets, and aerospace engineering), even though they exhibit overconfident predictions for ambiguous inputs. This deficiency demonstrates a fundamental flaw indicating that neural networks often overfit on spurious correlations. To address this problem in this work we present two objectives that improve the ability of a network to detect out-of-distribution samples and therefore avoid overconfident predictions for ambiguous inputs. We empirically demonstrate that our methods outperform the baseline and performs better than the majority of existing approaches, while still maintaining competitive with the remaining ones. Additionally, we empirically demonstrate the robustness of our approach against common corruptions showcasing the importance of regularisation and auxiliary information in out-of-distribution detection.
In tis slide, an introduction to string theory has been given. Apart from that, a simple proof of 26 dimensions of bosonic string theory is given (following Zwiebach's approach).
I explained this presentation in two parts (on my YouTube channel). Here are the links
_______________________________________________
Part 1
https://www.youtube.com/watch?v=QQA4JQ6Y-eo&list=PLDpqC3uXLZGl0cDod6g30PcjeJ4DAZWhp
_______________________________________________
Part 2
https://www.youtube.com/watch?v=vhLCtLn79jE&list=PLDpqC3uXLZGl0cDod6g30PcjeJ4DAZWhp&index=2
_______________________________________________
This document discusses orthogonal trajectories and provides examples of finding orthogonal trajectories for different families of curves. It begins by defining orthogonal trajectories as curves that intersect each other at right angles. It then provides a method for finding the differential equation that describes the orthogonal trajectories for a given family of curves. Several examples are worked out, such as finding the orthogonal trajectories of the family of parabolas with equation y = x^2. Applications to equipotential lines and electric fields and electromagnetic waves are also mentioned.
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Weakly proregular sequence and Cech, local cohomology
1. Weakly proregular sequence and Čech, local cohomology
安藤遼哉
東京理科大学理工学研究科
2021/10/13
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 1 / 29
2. Research Background
1 Research Background
2 Introduction
3 Čech cohomology and local cohomology
4 Weakly proregular sequence
5 Proof of Schenzel’s theorem
6 Reference
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 2 / 29
3. Research Background
• 可換環論,特に非 Noether 環に注目して研究をしています.可換環論は代数幾何学と歴
史的に結びつきの強い分野で(発表者も所属は代数幾何系の研究室です)
,積極的に研究
されているのは Noether 環が中心です.
FAQ
• 非 Noether 環の研究って何をしているの?
• 目的は?
• 応用は?
• …etc.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 3 / 29
4. Research Background
• Q. 非 Noether 環の研究って何をしているの?
I A. 大きく分けて,Noether 環の理論を非 Noether に拡張する研究と,非 Noether でしか起
こり得ない現象を調べる研究があります.
Hamilton and Marley (2007), Kim and Walker (2020), Miller (2008) などが CM 環,
Gorenstein 環などのホモロジカルな性質を拡張して,非 Noether 環上に一般化する研究を
行っています.
2次元以上の付値環は決して Noether 環にはなりません.
また Noether ではない環を含むような環のクラスに Krull 整域(UFD の一般化)があります
(Noether 整域が Krull 整域であることと,整閉整域であることは同値です)
.
少し古いですが,非 Noether 可換環論の話題を集めた本も出ています(Chapman and
Glaz (2000))
.
今日は Schenzel (2003) による weakly proregular sequence を紹介して,Noether 環における事
実が非 Noether 環に一般化される様子をみていきましょう.そして Schenzel の定理 (Theorem
4.1) の初頭的(?)な証明を発表者の preprint1 (arXiv:2105.07652) に基づいて紹介します.
1Accepted in Moroccan Journal of Algebra and Geometry with Applications.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 4 / 29
5. Introduction
1 Research Background
2 Introduction
3 Čech cohomology and local cohomology
4 Weakly proregular sequence
5 Proof of Schenzel’s theorem
6 Reference
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 5 / 29
6. Introduction
Various cohomologies and homologies are used in (commutative) algebra theory.
Example. 𝐴 : ring (unitary and commutative), 𝐼 : ideal of 𝐴, and 𝑀, 𝑁 ∈ Mod(𝐴).
(Mod(𝐴) : the category of 𝐴-modules, mod(𝐴) : the category of finitely generated 𝐴-modules.
)
• Ext𝑖
𝐴(𝑀, −) ...........Derived functor of Hom𝐴(𝑀, −).
• Tor𝐴
𝑖 (𝑀, −) ...........Derived functor of 𝑀 ⊗𝐴 −.
• 𝐻𝑖
𝐼 (−) ...................Derived functor of lim
−
−
→
Hom𝐴(𝐴/𝐼𝑛, −).
• 𝐻𝑖 ( 𝑓 , −) ...............Koszul homology defined by the 𝐴-linear map 𝑓 : 𝑁 → 𝐴.
• ˇ
𝐻𝑖 (𝑎, −) ................Čech cohomology defined by the sequence 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴.
• and more!
Derived functor is obtained from a right (or left) exact functor. For example, let 𝐽• be an
injective resolution of 𝑁, then Ext𝑖
(𝑀, 𝑁) B 𝐻𝑖 (Hom(𝑀, 𝐽•)).
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 6 / 29
7. Introduction
Why are cohomologies used so much?
One of the reasons for this is that ideal theoretic data can be written in a easier
form for calculation.
Definition 2.1
𝐴 : ring , 𝑀 ∈ Mod(𝐴). 𝑎 ∈ 𝐴 is called 𝑀-regular if ∀𝑥 ≠ 0 ∈ 𝑀, 𝑎𝑥 ≠ 0.
A sequence 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴 is called an 𝑀-regular sequence if;
• 𝑀/(𝑎1, . . . , 𝑎𝑟 )𝑀 ≠ 0,
• 1 ≤ ∀𝑖 ≤ 𝑟, 𝑎𝑖 is an 𝑀/(𝑎1, . . . , 𝑎𝑖−1)𝑀-regular.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 7 / 29
8. Introduction
Definition 2.2
𝐴 : Noetherian ring, 𝑀 ∈ mod(𝐴) and 𝐼 : ideal with 𝐼𝑀 ≠ 𝑀.
depth𝐼 (𝑀) B sup
𝑟 ≥ 0 ∃
𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐼, 𝑎 is an 𝑀-regular sequence.
is called an 𝐼-depth of 𝑀.
Theorem 2.3 (Rees)
Under the above notation, the length of a maximal regular sequence is constant. Also;
depth𝐼 (𝑀) = inf
𝑖 ≥ 0 Ext𝑖
(𝐴/𝐼, 𝑀) ≠ 0 .
This theorem shows that the depth of module is calculatable by using a cohomology!
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 8 / 29
9. Čech cohomology and local cohomology
1 Research Background
2 Introduction
3 Čech cohomology and local cohomology
4 Weakly proregular sequence
5 Proof of Schenzel’s theorem
6 Reference
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 9 / 29
10. Čech cohomology and local cohomology
Definition 3.1
𝐴 : ring , 𝐼 : ideal of 𝐴.
𝐻𝑖
𝐼 (−) : the right derived functor of lim
−
−
→
Hom𝐴(𝐴/𝐼𝑛, −) is called a local cohomology.
Note that there are following isomorphisms,
𝐻𝑖
𝐼 (𝑀) lim
−
−
→
Ext𝑖
(𝐴/𝐼𝑛
, 𝑀)
since taking the inductive limit is an exact functor.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 10 / 29
11. Čech cohomology and local cohomology
Definition 3.2
𝐴 : ring , 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴.
{𝑒𝑖} : the standard basis of 𝐴𝑟 .
For each 𝐼 = { 𝑗1, . . . , 𝑗𝑖} (1 ≤ 𝑗1 · · · 𝑗𝑖 ≤ 𝑟), let 𝑎𝐼 = 𝑎𝑗1 · · · 𝑎𝑗𝑖 and 𝑒𝐼 = 𝑒𝑗1 ∧ · · · ∧ 𝑒𝑗𝑖 .
𝐶•(𝑎) : the complex defined by;
𝐶𝑖
(𝑎) B
Õ
#𝐼=𝑖
𝐴𝑎𝐼 𝑒𝐼,
𝑑𝑖
: 𝐶𝑖
(𝑎) → 𝐶𝑖+1
(𝑎); 𝑒𝐼 ↦→
𝑟
Õ
𝑗=1
𝑒𝐼 ∧ 𝑒𝑗 .
It is called a Čech complex.
ˇ
𝐻𝑖 (𝑎) : the cohomology of 𝐶•(𝑎) is called a Čech cohomology.
For 𝑀 ∈ Mod(𝐴), we define 𝐶•(𝑎, 𝑀) B 𝐶•(𝑎) ⊗ 𝑀, ˇ
𝐻𝑖 (𝑎, 𝑀) B 𝐻𝑖 (𝐶•(𝑎, 𝑀)).
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 11 / 29
12. Čech cohomology and local cohomology
Theorem 3.3
𝐴 : Noetherian ring, 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴 and 𝐼 = (𝑎1, . . . , 𝑎𝑟 ). There are isomorphisms;
𝐻𝑖
𝐼 (𝑀) ˇ
𝐻𝑖
(𝑎, 𝑀)
for any 𝑀 ∈ Mod(𝐴).
What happens if we remove the Noetherian assumption? Can we extend this theorem?
This theorem was extended by Schenzel (2003) by introducing a weakly proregular
sequence.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 12 / 29
13. Weakly proregular sequence
1 Research Background
2 Introduction
3 Čech cohomology and local cohomology
4 Weakly proregular sequence
5 Proof of Schenzel’s theorem
6 Reference
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 13 / 29
14. Weakly proregular sequence
Theorem 4.1 (Schenzel)
𝐴 : ring, 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴 and 𝐼 = (𝑎1, . . . , 𝑎𝑟 ).
𝑎 is a weakly proregular sequence ⇐⇒ ∀
𝑖 ≥ 0, ∀
𝑀 ∈ Mod(𝐴), 𝐻𝑖
𝐼 (𝑀) ˇ
𝐻𝑖
(𝑎, 𝑀).
A weakly proregular sequence is defined using the Koszul complex.
Definition 4.2
𝐴 : ring , 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴. {𝑒𝑖} : the standard basis of 𝐴𝑟 .
𝐾•(𝑎) is the complex defined by ;
𝐾𝑖 (𝑎) =
𝑖
Û
𝐴𝑟
𝑑𝑖 : 𝐾𝑖 (𝑎) → 𝐾𝑖−1(𝑎); 𝑒𝐼 ↦→
𝑖
Õ
𝑘=1
(−1)𝑘+1
𝑎𝑗𝑘 𝑒𝑗1 ∧ · · · ∧ c
𝑒𝑗𝑘 ∧ · · · ∧ 𝑒𝑗𝑖 .
It is called a Koszul (chain) complex.
𝐻𝑖 (𝑎) : the homology of 𝐾•(𝑎) is called a Koszul homology.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 14 / 29
15. Weakly proregular sequence
𝑎𝑛 : the sequence defined by 𝑎𝑛
1 , . . . , 𝑎𝑛
𝑟 .
Note that by following morphisms, Koszul complexes constitute an inverse system
{𝐾•(𝑎𝑛)}𝑛≥0; 𝜑𝑚𝑛 : 𝐾𝑖 (𝑎𝑚
) → 𝐾𝑖 (𝑎𝑛
); 𝑒𝐼 ↦→ 𝑎𝑚−𝑛
𝐼 𝑒𝐼 (𝑛 ≤ 𝑚).
This induces a morphism between homologies.
Definition 4.3 (Schenzel)
𝐴 : ring , 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴.
𝑎 is called a weakly proregular sequence if
1 ≤ ∀𝑖 ≤ 𝑟, ∀𝑛 ≥ 0, ∃𝑚 ≥ 𝑛; 𝜑𝑚𝑛 : 𝐻𝑖 (𝑎𝑚) → 𝐻𝑖 (𝑎𝑛) is the zero map.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 15 / 29
16. Weakly proregular sequence
We will explain that Schenzel’s theorem (Theorem 4.1) is an extension of the Noetherian case.
Definition 4.4 (Greenlees, May)
𝐴 : ring , 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴.
𝑎 is called a proregular sequence if
1 ≤ ∀𝑖 ≤ 𝑟, ∀𝑛 0, ∃𝑚 ≥ 𝑛; ∀𝑎 ∈ 𝐴, 𝑎𝑎𝑚
𝑖 ∈ (𝑎𝑚
1 , . . . , 𝑎𝑚
𝑖−1) =⇒ 𝑎𝑎𝑚−𝑛
𝑖 ∈ (𝑎𝑛
1 , . . . , 𝑎𝑛
𝑖−1).
The following relations hold;
Regular =⇒ Proregular =⇒ Weakly proregular.
• The first implication is easy. If 𝑎 is a regular sequence, for each 𝑛 0, let 𝑚 = 𝑛.
• The second is proved by calculating a Koszul homology.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 16 / 29
17. Weakly proregular sequence
Proposition 4.5
𝐴: Noetherian ring , 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴. 𝑎 is a proregular sequence.
Proof.
Let 𝐽𝑖
𝑚 = ((𝑎𝑚
1 , . . . , 𝑎𝑚
𝑖−1) : 𝑎𝑚
𝑖 𝐴), 𝐼𝑖
𝑛,𝑚 = ((𝑎𝑛
1 , . . . , 𝑎𝑛
𝑖−1) : 𝑎𝑚−𝑛
𝑖 𝐴).
𝑎 is a proregular sequence ⇐⇒ 1 ≤ ∀
𝑖 ≤ 𝑟, ∀
𝑛 0, ∃
𝑚 ≥ 𝑛; 𝐽𝑖
𝑚 ⊂ 𝐼𝑖
𝑛,𝑚.
Fix 1 ≤ ∀𝑖 ≤ 𝑟 and omit from the notation.
Fix 𝑛, {𝐼𝑛,𝑚}𝑚≥𝑛 : ascending chain of ideals ∃𝑚0 ≥ 𝑛; ∀𝑚 ≥ 𝑚0, 𝐼𝑛,𝑚0 = 𝐼𝑛,𝑚.
Let 𝑚 B 𝑚0 + 𝑛, then ∀𝑎 ∈ 𝐽𝑚0 , 𝑎𝑎𝑚−𝑛
𝑖 = 𝑎𝑎𝑚0
𝑖 ∈ (𝑎𝑚0
1 , . . . , 𝑎𝑚0
𝑖−1) ⊂ (𝑎𝑛
1 , . . . , 𝑎𝑛
𝑖−1).
So 𝐽𝑚0 ⊂ 𝐼𝑛,𝑚0 .
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 17 / 29
18. Weakly proregular sequence
Corollary 4.6 (ICYMI : Theorem 3.3)
𝐴 : Noetherian ring, 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴 and 𝐼 = (𝑎1, . . . , 𝑎𝑟 ). There are isomorphisms;
𝐻𝑖
𝐼 (𝑀) ˇ
𝐻𝑖
(𝑎, 𝑀)
for any 𝑀 ∈ Mod(𝐴).
Another proof of Theorem 3.3.
By above proposition, 𝑎 is proregular. 𝑎 is weakly proregular.
Then according to Schenzel’s theorem, 𝐻𝑖
𝐼 (𝑀) ˇ
𝐻𝑖 (𝑎, 𝑀).
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 18 / 29
19. Proof of Schenzel’s theorem
1 Research Background
2 Introduction
3 Čech cohomology and local cohomology
4 Weakly proregular sequence
5 Proof of Schenzel’s theorem
6 Reference
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 19 / 29
20. Proof of Schenzel’s theorem
Why is a weakly proregular sequence defined by using a Koszul homology?
A Čech cohomology can be written by using a Koszul cohomology!
𝐾•(𝑎) B Hom(𝐾•(𝑎), 𝐴). For 𝑀 ∈ Mod(𝐴), 𝐾•(𝑎, 𝑀) B Hom(𝐾•(𝑎), 𝑀) = 𝐾•(𝑎) ⊗ 𝑀.
𝐾•(𝑎) : · · · 𝐾1(𝑎) 𝐾0(𝑎) 0
𝐾•(𝑎) : 0 𝐾0(𝑎) 𝐾1(𝑎) · · ·
Hom(−,𝐴)
The opposition of morphism induces an inductive system {𝐾•(𝑎𝑛)}𝑛≥0;
𝜑𝑛𝑚
: 𝐾𝑖
(𝑎𝑛
) → 𝐾𝑖
(𝑎𝑚
); (𝑒𝐼)∗
↦→ 𝑎𝑚−𝑛
𝐼 (𝑒𝐼)∗
.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 20 / 29
21. Proof of Schenzel’s theorem
Proposition 5.1
𝐴 : ring, 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴 and 𝑀 ∈ Mod(𝐴). Then;
ˇ
𝐻𝑖
(𝑎, 𝑀) lim
−
−
→
𝐻𝑖
(𝑎𝑛
, 𝑀).
Sketch of the proof.
𝜑𝑖 : 𝐾𝑖 (𝑎) → 𝐶𝑖 (𝑎); (𝑒𝐼)∗ ↦→ (1/𝑎𝐼)𝑒𝐼 is a morphism of complexes.
So we get 𝜑•
𝑛 : 𝐾•(𝑎𝑛) → 𝐶•(𝑎𝑛) = 𝐶•(𝑎). It induces 𝜑 : lim
−
−
→
𝐾•(𝑎𝑛) → 𝐶•(𝑎) and this is an
isomorphism.
· · · 𝐾•(𝑎𝑛) 𝐾•(𝑎𝑚) · · · lim
−
−
→
𝐾•(𝑎𝑛)
𝐶•(𝑎)
𝜑•
𝑛
𝜑𝑛𝑚
𝜑•
𝑚
𝜑
Then ; lim
−
−
→
𝐻𝑖 (𝑎𝑛, 𝑀) = 𝐻𝑖 (lim
−
−
→
𝐾•(𝑎𝑛) ⊗ 𝑀) 𝐻𝑖 (𝐶•(𝑎𝑛) ⊗ 𝑀) = ˇ
𝐻𝑖 (𝑎𝑛, 𝑀).
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 21 / 29
22. Proof of Schenzel’s theorem
Remark 5.2
By Proposition 5.1,
ˇ
𝐻𝑖
(𝑎, 𝑀) lim
−
−
→
𝐻𝑖
(𝑎𝑛
, 𝑀).
By the definition,
𝐻𝑖
𝐼 (𝑀) lim
−
−
→
Ext𝑖
(𝐴/𝐼𝑛
, 𝑀).
Schenzel’s theorem holds if 𝐻𝑖 (𝑎𝑛, 𝑀) Ext𝑖
(𝐴/𝐼𝑛, 𝑀), which is true when 𝑎 is a
regular sequence.
However, if 𝑎 is not regular, it may not work. So we will need to find an another way.
We will show a way to use the 𝛿-functor.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 22 / 29
23. Proof of Schenzel’s theorem
𝐴: ring , 𝐼 : ideal of 𝐴. Let Γ𝐼 (𝑀) B
𝑥 ∈ 𝑀 ∃𝑛 ≥ 0; 𝐼𝑛𝑥 = 0 .
The functor Γ𝐼 (−) connects a local cohomology and a Čech cohomology.
Lemma 5.3
𝐴 : ring, 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴, 𝐼 = (𝑎1, . . . , 𝑎𝑟 ) : ideal of 𝐴 and 𝑀 ∈ Mod(𝐴).
𝐻0
𝐼 (𝑀) Γ𝐼 (𝑀) ˇ
𝐻0
(𝑎, 𝑀).
Proof.
• First isomorphism : 𝐻0
𝐼 (𝑀) = lim
−
−
→
Hom(𝐴/𝐼𝑛, 𝑀), Hom(𝐴/𝐼𝑛, 𝑀) {𝑥 ∈ 𝑀 | 𝐼𝑛𝑥 = 0} .
• ˇ
𝐻0(𝑎, 𝑀) is the kernel of (𝑀 →
É𝑟
𝑖=1 𝑀𝑎𝑖 𝑒𝑖; 𝑥 ↦→ (𝑥/1)𝑒𝑖).
∀𝑥 ∈ ˇ
𝐻0(𝑎, 𝑀), 1 ≤ ∀𝑖 ≤ 𝑟, ∃𝑛𝑖 ≥ 0; 𝑎𝑛𝑖
𝑖 𝑥 = 0. i.e. 𝑥 ∈ Γ𝐼 (𝑀).
Similarly Γ𝐼 (𝑀) ⊂ ˇ
𝐻0(𝑎, 𝑀). ˇ
𝐻0(𝑎, 𝑀) = Γ𝐼 (𝑀) as a submodule of 𝑀.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 23 / 29
24. Proof of Schenzel’s theorem
Definition 5.4
𝒜, ℬ : Abelian categories.
𝑇• B {𝑇𝑖 : 𝒜 → ℬ}𝑖≥0 : family of additive functors.
𝑇• is called a 𝛿-functor if ;
• For each exact sequence 0 → 𝐴1 → 𝐴2 → 𝐴3 → 0 in 𝒜, ∃𝛿𝑖 : 𝑇𝑖 (𝐴3) → 𝑇𝑖+1(𝐴1);
0 𝑇0(𝐴1) 𝑇0(𝐴2) 𝑇0(𝐴3) · · · 𝑇𝑖 (𝐴1) 𝑇𝑖 (𝐴2) 𝑇𝑖 (𝐴3) · · ·
𝛿0 𝛿𝑖−1 𝛿𝑖
is exact.
• It transfers a commutative diagram to a commutative diagram.
𝛿𝑖 is called a connecting morphism.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 24 / 29
25. Proof of Schenzel’s theorem
The 𝛿-functor is a generalisation of the derived functor.
It is also useful for proving that the family of functors are form a derived functor!
Definition 5.5
𝒜, ℬ : Abelian categories, 𝐹 : 𝒜 → ℬ : additive functor.
𝐹 is called effaceable if ∀ 𝐴 ∈ 𝒜, ∃ 𝑀 ∈ 𝒜; ∃𝑢 : 𝐴 → 𝑀 : injection; 𝐹(𝑢) = 0.
Proposition 5.6
𝒜, ℬ : Abelian categories, 𝒜 has enough injectives. 𝑇• = {𝑇𝑖}𝑖≥0 : 𝛿-functor.
∀𝑖 0,𝑇𝑖 is effaceable. Then;
• 𝑇0 is left-exact.
• ∀𝑖 ≥ 0,𝑇𝑖 𝑅𝑖𝑇0 (up to unique isomorphism).
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 25 / 29
26. Proof of Schenzel’s theorem
Proposition 5.7
ˇ
𝐻•(𝑎, −) is a 𝛿-functor with ˇ
𝐻0(𝑎, −) 𝐻0
𝐼 (−).
Sketch of the proof.
0 → 𝑀1 → 𝑀2 → 𝑀3 → 0 : exact sequence of Mod(𝐴).
𝐶•(𝑎, 𝑀) = 𝐶•(𝑎) ⊗ 𝑀 and 𝐶𝑖 (𝑎) is flat. We obtain an exact sequence of
complexes by taking tensor products.
0 𝐶•(𝑎, 𝑀1) 𝐶•(𝑎, 𝑀2) 𝐶•(𝑎, 𝑀3) 0 .
So there are connecting morphisms.
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 26 / 29
27. Proof of Schenzel’s theorem
Proposition 5.8
𝐴: ring, 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴.
𝑎 is a weakly proregular seqence ⇐⇒ ˇ
𝐻•
(𝑎, −) is an effaceable 𝛿-functor.
Sketch of the proof.
It is enough to check each injective module 𝐽, ˇ
𝐻𝑖 (𝑎, 𝐽) = 0 (∀𝑖 0).
Use Proposition 5.1. i.e. ˇ
𝐻𝑖 (𝑎, 𝑀) lim
−
−
→
𝐻𝑖 (𝑎𝑛, 𝑀).
Calculate the Koszul (co)homology! (Note that 𝐻𝑖 (𝑎𝑛, 𝐽) Hom(𝐻𝑖 (𝑎𝑛), 𝐽).)
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 27 / 29
28. Proof of Schenzel’s theorem
Theorem 5.9 (ICYMI : Schenzel’s theorem)
𝐴 : ring, 𝑎 = 𝑎1, . . . , 𝑎𝑟 ∈ 𝐴 and 𝐼 = (𝑎1, . . . , 𝑎𝑟 ).
𝑎 is a weakly proregular sequence ⇐⇒ ∀
𝑖 ≥ 0, ∀
𝑀 ∈ Mod(𝐴), 𝐻𝑖
𝐼 (𝑀) ˇ
𝐻𝑖
(𝑎, 𝑀).
Elementary proof of Schenzel’s theorem. A(2021).
It is a combination of what has been said so far.
𝐻0
𝐼 (−) Γ𝐼 (𝑀) ˇ
𝐻0
(𝑎, −). (Lem. 5.3)
𝑎 is a weakly proregular sequence ⇐⇒ ˇ
𝐻•
(𝑎, −) is an effaceable 𝛿-functor. (Prop. 5.8)
𝑎 is a weakly proregular sequence ⇐⇒ ∀
𝑖 ≥ 0, ˇ
𝐻𝑖
(𝑎, −) 𝐻𝑖
𝐼 (−) = 𝑅𝑖
Γ𝐼 (−). (Prop. 5.6)
Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 28 / 29
29. Reference
Reference
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Ryoya Ando (Tokyo University of Science) Weakly proregular sequence and Čech, local cohomology 2021/10/13 29 / 29