This document provides an introduction and overview of nonparametric predictive regression for modeling nonlinear and time-varying effects. It summarizes the following key points:
1) Nonparametric predictive regression is proposed to model relationships that may change over time using orthogonal series estimation and local smoothing.
2) A two-step estimation procedure is used, with orthogonal series estimation in the first step to reduce bias, followed by local smoothing in the second step.
3) Asymptotic properties of the estimators are derived, showing they are consistent and asymptotically normal under certain conditions, whether the predictors are stationary or nonstationary.
The document discusses dual gravitons in AdS4/CFT3 and proposes that the holographic Cotton tensor can play the role of the dual operator to the metric in the boundary CFT.
The Cotton tensor is a symmetric, traceless and conserved tensor that can be constructed from the linearized metric. It is the stress-energy tensor of gravitational Chern-Simons theory. The document proposes that the Cotton tensor and stress-energy tensor form a dual pair under the holographic duality, with the Cotton tensor acting as the operator corresponding to fluctuations of the metric in the bulk. This is motivated by properties of gravitational instantons and self-dual solutions in AdS.
Supersymmetric Q-balls and boson stars in (d + 1) dimensions - Jena Talk Mar ...Jurgen Riedel
This document summarizes research on supersymmetric Q-balls and boson stars in (d+1) dimensions. It discusses solitons in nonlinear field theories and properties of topological and non-topological solitons. Derrick's theorem restricting soliton solutions in more than one dimension is covered. The document presents a model of Q-balls and boson stars using a complex scalar field with a conserved Noether charge. Equations for the metric, scalar field, charge, and mass are given. Graphs show properties of Q-balls in Minkowski and anti-de Sitter spacetimes, including the maximum angular velocity as a function of dimension and cosmological constant.
Supersymmetric Q-balls and boson stars in (d + 1) dimensionsJurgen Riedel
This document summarizes research on supersymmetric Q-balls and boson stars in (d+1) dimensions. The researchers set up a model to support boson star solutions as well as Q-ball solutions in the limit without back reaction. They studied solutions with a gauge-mediated SUSY potential in d+1 dimensions. They investigated stability conditions of the solutions and differences from the standard Φ6-potential ansatz. Their results included expressions for charge and mass of the solutions, existence conditions, profiles of scalar fields, and properties of excited Q-balls.
The document summarizes two models:
1. The Lo-Zivot Threshold Cointegration Model, which uses a threshold vector error correction model (TVECM) to analyze the dynamic adjustment of cointegrated time series variables to their long-run equilibrium. It allows for nonlinear and asymmetric adjustment speeds.
2. A bivariate vector error correction model (VECM) and band-threshold vector error correction model (BAND-TVECM) that extend the VECM to allow for nonlinear and discontinuous adjustments to long-run equilibrium across multiple regimes defined by thresholds on a variable. This captures asymmetric adjustment speeds and dynamic behavior.
The BAND-TVECM allows modeling of
Research Inventy : International Journal of Engineering and Scienceinventy
Research Inventy : International Journal of Engineering and Science is published by the group of young academic and industrial researchers with 12 Issues per year. It is an online as well as print version open access journal that provides rapid publication (monthly) of articles in all areas of the subject such as: civil, mechanical, chemical, electronic and computer engineering as well as production and information technology. The Journal welcomes the submission of manuscripts that meet the general criteria of significance and scientific excellence. Papers will be published by rapid process within 20 days after acceptance and peer review process takes only 7 days. All articles published in Research Inventy will be peer-reviewed.
On Twisted Paraproducts and some other Multilinear Singular IntegralsVjekoslavKovac1
Presentation.
9th International Conference on Harmonic Analysis and Partial Differential Equations, El Escorial, June 12, 2012.
The 24th International Conference on Operator Theory, Timisoara, July 3, 2012.
Dual Gravitons in AdS4/CFT3 and the Holographic Cotton TensorSebastian De Haro
This document summarizes research on dual gravitons in AdS4/CFT3 and the holographic Cotton tensor. Key points:
- In AdS4/CFT3, both modes of the graviton are normalizable, allowing duality to interchange the boundary metric g(0) and stress tensor T.
- The Cotton tensor C, which maps a metric to its stress tensor, plays a special role as the "holographic Cotton tensor".
- There is a duality symmetry of the bulk equations of motion under which the linearized metric fluctuations ḣ and Cotton tensor of the dual metric C(ḣ) are interchanged.
- This relates the
The document discusses dual gravitons in AdS4/CFT3 and proposes that the holographic Cotton tensor can play the role of the dual operator to the metric in the boundary CFT.
The Cotton tensor is a symmetric, traceless and conserved tensor that can be constructed from the linearized metric. It is the stress-energy tensor of gravitational Chern-Simons theory. The document proposes that the Cotton tensor and stress-energy tensor form a dual pair under the holographic duality, with the Cotton tensor acting as the operator corresponding to fluctuations of the metric in the bulk. This is motivated by properties of gravitational instantons and self-dual solutions in AdS.
Supersymmetric Q-balls and boson stars in (d + 1) dimensions - Jena Talk Mar ...Jurgen Riedel
This document summarizes research on supersymmetric Q-balls and boson stars in (d+1) dimensions. It discusses solitons in nonlinear field theories and properties of topological and non-topological solitons. Derrick's theorem restricting soliton solutions in more than one dimension is covered. The document presents a model of Q-balls and boson stars using a complex scalar field with a conserved Noether charge. Equations for the metric, scalar field, charge, and mass are given. Graphs show properties of Q-balls in Minkowski and anti-de Sitter spacetimes, including the maximum angular velocity as a function of dimension and cosmological constant.
Supersymmetric Q-balls and boson stars in (d + 1) dimensionsJurgen Riedel
This document summarizes research on supersymmetric Q-balls and boson stars in (d+1) dimensions. The researchers set up a model to support boson star solutions as well as Q-ball solutions in the limit without back reaction. They studied solutions with a gauge-mediated SUSY potential in d+1 dimensions. They investigated stability conditions of the solutions and differences from the standard Φ6-potential ansatz. Their results included expressions for charge and mass of the solutions, existence conditions, profiles of scalar fields, and properties of excited Q-balls.
The document summarizes two models:
1. The Lo-Zivot Threshold Cointegration Model, which uses a threshold vector error correction model (TVECM) to analyze the dynamic adjustment of cointegrated time series variables to their long-run equilibrium. It allows for nonlinear and asymmetric adjustment speeds.
2. A bivariate vector error correction model (VECM) and band-threshold vector error correction model (BAND-TVECM) that extend the VECM to allow for nonlinear and discontinuous adjustments to long-run equilibrium across multiple regimes defined by thresholds on a variable. This captures asymmetric adjustment speeds and dynamic behavior.
The BAND-TVECM allows modeling of
Research Inventy : International Journal of Engineering and Scienceinventy
Research Inventy : International Journal of Engineering and Science is published by the group of young academic and industrial researchers with 12 Issues per year. It is an online as well as print version open access journal that provides rapid publication (monthly) of articles in all areas of the subject such as: civil, mechanical, chemical, electronic and computer engineering as well as production and information technology. The Journal welcomes the submission of manuscripts that meet the general criteria of significance and scientific excellence. Papers will be published by rapid process within 20 days after acceptance and peer review process takes only 7 days. All articles published in Research Inventy will be peer-reviewed.
On Twisted Paraproducts and some other Multilinear Singular IntegralsVjekoslavKovac1
Presentation.
9th International Conference on Harmonic Analysis and Partial Differential Equations, El Escorial, June 12, 2012.
The 24th International Conference on Operator Theory, Timisoara, July 3, 2012.
Dual Gravitons in AdS4/CFT3 and the Holographic Cotton TensorSebastian De Haro
This document summarizes research on dual gravitons in AdS4/CFT3 and the holographic Cotton tensor. Key points:
- In AdS4/CFT3, both modes of the graviton are normalizable, allowing duality to interchange the boundary metric g(0) and stress tensor T.
- The Cotton tensor C, which maps a metric to its stress tensor, plays a special role as the "holographic Cotton tensor".
- There is a duality symmetry of the bulk equations of motion under which the linearized metric fluctuations ḣ and Cotton tensor of the dual metric C(ḣ) are interchanged.
- This relates the
A T(1)-type theorem for entangled multilinear Calderon-Zygmund operatorsVjekoslavKovac1
This document summarizes a talk given by Vjekoslav Kovač at a joint mathematics conference. The talk concerned establishing T(1)-type theorems for entangled multilinear Calderón-Zygmund operators. Specifically, Kovač discussed studying multilinear singular integral forms where the functions partially share variables, known as an "entangled structure." He outlined establishing generalized modulation invariance and Lp estimates for such operators. The talk motivated further studying related problems involving bilinear ergodic averages and forms with more complex graph structures. Kovač specialized his techniques to bipartite graphs, multilinear Calderón-Zygmund kernels, and "perfect" dyadic models.
Tales on two commuting transformations or flowsVjekoslavKovac1
1) The document summarizes recent work on ergodic averages and flows for commuting transformations. It discusses convergence results for single and double linear ergodic averages in L2 and almost everywhere, as well as providing norm estimates to quantify the rate of convergence.
2) It also considers double polynomial ergodic averages and provides proofs for almost everywhere convergence in the continuous-time setting. Open problems remain for the discrete-time case.
3) An ergodic-martingale paraproduct is introduced, motivated by an open question from 1950. Convergence in Lp norm is shown, while almost everywhere convergence remains open.
Many areas of machine learning and data mining focus on point estimates of key parameters. In transportation, however, the inherent variance, and, critically, the need to understand the limits of that variance and the impact it may have, have long been understood to be important. Indeed, variance and other risk measures that capture the cost of the spread around the mean, are critical factors in understanding how people act. Thus they are critical for prediction, as well as for purposes of long term planning, where controlling risk may be equally important to controlling the mean (the point estimate).
There has been tremendous progress on large scale optimization techniques to enable the solution of large scale machine learning and data analytics problems. Stochastic Gradient Descent and its variants is probably the most-used large-scale optimization technique for learning. This has not yet seen an impact on the problem of statistical inference — namely, obtaining distributional information that might allow us to control the variance and hence the risk of certain solutions.
The document provides an introduction to the gamma function Γ(x). Some key points:
1) The gamma function was introduced by Euler to generalize the factorial to non-integer values. It is defined by definite integrals and satisfies the functional equation Γ(x+1)=xΓ(x).
2) The gamma function can be defined for both positive and negative real values, except for negative integers where it has simple poles. It is related to important constants like Euler's constant.
3) The gamma function satisfies important formulas like the duplication formula, multiplication formula, and complement/reflection formula. Stirling's formula approximates the gamma function for large integer values.
Trilinear embedding for divergence-form operatorsVjekoslavKovac1
The document discusses a trilinear embedding theorem for divergence-form operators with complex coefficients. It proves that if matrices A, B, C are appropriately p,q,r-elliptic, then there is a bound on the integral of the product of the gradients of the semigroups associated with the operators. The proof uses a Bellman function technique and shows the relationship to the concept of p-ellipticity. It generalizes previous work on bilinear embeddings to the trilinear case.
This document discusses multilinear twisted paraproducts, which are generalizations of classical paraproduct operators to higher dimensions. It begins by reviewing classical paraproducts on the real line and their generalization to higher dimensions using dyadic squares. It then discusses complications that arise, such as twisted paraproducts. The document presents a unified framework for studying such operators using bipartite graphs and selections of vertices. It proves a main boundedness result and discusses special cases like classical dyadic paraproducts and dyadic twisted paraproducts. It introduces tools like Bellman functions and calculus of finite differences to analyze estimates for paraproduct-like operators on finite trees of dyadic squares.
This document summarizes research on norm-variation estimates for ergodic bilinear and multiple averages. It begins by motivating the study of ergodic averages and their convergence properties. Previous results are discussed that provide pointwise convergence and norm estimates for certain cases. The document then presents new norm-variation estimates obtained by the authors for bilinear and multiple ergodic averages over general measure-preserving systems. These estimates bound the number of jumps in the L2 norm as the averages converge. Finally, analogous results are discussed for bilinear averages on R2 and Z2, linking the estimates to established bounds for singular integrals.
This document discusses unconditionally stable finite-difference time-domain (FDTD) methods for solving Maxwell's equations numerically. It outlines FDTD algorithms such as Yee's method from 1966 which discretize the equations on a staggered grid. It also discusses the von Neumann stability analysis and compares implicit Crank-Nicolson and alternating-direction implicit methods to conventional explicit FDTD methods. The document notes the advantages of unconditionally stable methods but also mentions potential disadvantages.
The document describes the error correction model (ECM) version of Granger causality testing for determining the causal relationship between two non-stationary time series variables. It involves first testing for cointegration between the variables using the Johansen test or Engle-Granger approach. If cointegrated, the ECM version estimates an error correction model and performs Granger causality tests to examine short-run, long-run, and strong causality. The procedure and hypotheses for each test are provided along with the method for calculating the relevant F-statistics.
11.generalized and subset integrated autoregressive moving average bilinear t...Alexander Decker
This document proposes generalized integrated autoregressive moving average bilinear (GBL) time series models and subset generalized integrated autoregressive moving average bilinear (GSBL) models to achieve stationary for all nonlinear time series. It presents the models' formulations and discusses their properties including stationary, convergence, and parameter estimation. An algorithm is provided to fit the one-dimensional models. The generalized models are applied to Wolfer sunspot numbers and the GBL model is found to perform better than the GSBL model.
The document provides tables summarizing common transform pairs for the continuous-time Fourier transform, continuous-time pulsation Fourier transform, z-transform, discrete-time Fourier transform, and Laplace transform. It includes the transform, its properties, examples, and regions of convergence for each transform. The tables are intended to provide a handy reference for engineers and students working with various transformation pairs and properties.
Simple Comparison of Convergence of GeneralIterations and Effect of Variation...Komal Goyal
The document compares the convergence of Jungck-Ishikawa and Jungck-Noor iterative procedures for solving nonlinear equations. It presents 4 examples showing that the two procedures compute solutions in the same number of iterations when the parameters α, β, and γ are equal. Graphs demonstrate the effect of varying these parameters and the initial value x0 on the number of iterations needed for convergence. Both procedures consistently converge for the examples presented.
1. The document provides definitions and identities relating to theoretical computer science topics like asymptotic analysis, series, recurrences, and discrete structures.
2. It includes definitions for big O, Omega, and Theta notation used to describe the asymptotic behavior of functions.
3. Recurrences, like the master method, are presented for analyzing the runtime of divide-and-conquer algorithms.
4. Discrete structures like combinations, Stirling numbers, and trees are also covered, along with their properties and relationships.
Scattering theory analogues of several classical estimates in Fourier analysisVjekoslavKovac1
This document summarizes some classical estimates in Fourier analysis and their analogues in nonlinear Fourier analysis. It discusses Carleson's theorem on convergence of Fourier series and Fourier transforms, Hausdorff-Young inequalities bounding Lp norms, and results on lacunary trigonometric series and products. Open questions are presented about extending these classical estimates to the nonlinear setting of the SU(1,1) Fourier transform and lacunary SU(1,1) trigonometric products.
11.vibration characteristics of non homogeneous visco-elastic square plateAlexander Decker
This document presents research on the vibration characteristics of a non-homogeneous visco-elastic square plate with variations in thickness and temperature. A mathematical model is developed to analyze the effects of thermal gradients and taper parameters on the fundamental frequencies of the plate. The frequencies of the first two vibration modes are calculated for different values of the parameters using MATLAB. The results show that the frequencies decrease with increasing thermal gradient but increase with rising taper constants. The study aims to provide engineers and researchers a theoretical model to analyze thermally induced vibrations in non-homogeneous plates.
Vibration characteristics of non homogeneous visco-elastic square plateAlexander Decker
This document presents a mathematical model to analyze the vibration characteristics of a non-homogeneous visco-elastic square plate with variations in thickness and temperature. Rayleigh-Ritz method is used to derive the frequency equation for a plate with thickness tapering parabolically in one direction and temperature varying linearly in one direction and parabolically in another. Computational analysis using MATLAB calculates the fundamental frequencies for the first two vibration modes under varying thermal gradient and taper parameters. The results show that the frequency decreases with increasing thermal gradient or thickness tapering for both vibration modes.
Ban berfungsi untuk menopang beban kendaraan, mendorong dan memperlambat kendaraan, membelokkan kendaraan, serta memberikan kenyamanan saat mengemudi. Untuk itu, ban dibuat dari komponen utama seperti tread, casing, dan bead yang disusun secara radial atau bias."
Bahan ini memberikan informasi tentang bagaimana konstruksi dari mobil-mobil atau kendaraan hybrid yang sedang d kembangkan saat sekarang ini, semoga bisa bermanfaat.
Modul ini membahas tentang melepas, memasang, dan menyetel roda pada kendaraan. Terdiri atas empat kegiatan belajar yaitu mengidentifikasi jenis roda, melepas roda, pemeriksaan roda, dan memasang roda. Setelah mempelajari modul ini, peserta diharapkan mampu melepas, memasang, dan menyetel roda secara efektif, efisien, dan aman.
A T(1)-type theorem for entangled multilinear Calderon-Zygmund operatorsVjekoslavKovac1
This document summarizes a talk given by Vjekoslav Kovač at a joint mathematics conference. The talk concerned establishing T(1)-type theorems for entangled multilinear Calderón-Zygmund operators. Specifically, Kovač discussed studying multilinear singular integral forms where the functions partially share variables, known as an "entangled structure." He outlined establishing generalized modulation invariance and Lp estimates for such operators. The talk motivated further studying related problems involving bilinear ergodic averages and forms with more complex graph structures. Kovač specialized his techniques to bipartite graphs, multilinear Calderón-Zygmund kernels, and "perfect" dyadic models.
Tales on two commuting transformations or flowsVjekoslavKovac1
1) The document summarizes recent work on ergodic averages and flows for commuting transformations. It discusses convergence results for single and double linear ergodic averages in L2 and almost everywhere, as well as providing norm estimates to quantify the rate of convergence.
2) It also considers double polynomial ergodic averages and provides proofs for almost everywhere convergence in the continuous-time setting. Open problems remain for the discrete-time case.
3) An ergodic-martingale paraproduct is introduced, motivated by an open question from 1950. Convergence in Lp norm is shown, while almost everywhere convergence remains open.
Many areas of machine learning and data mining focus on point estimates of key parameters. In transportation, however, the inherent variance, and, critically, the need to understand the limits of that variance and the impact it may have, have long been understood to be important. Indeed, variance and other risk measures that capture the cost of the spread around the mean, are critical factors in understanding how people act. Thus they are critical for prediction, as well as for purposes of long term planning, where controlling risk may be equally important to controlling the mean (the point estimate).
There has been tremendous progress on large scale optimization techniques to enable the solution of large scale machine learning and data analytics problems. Stochastic Gradient Descent and its variants is probably the most-used large-scale optimization technique for learning. This has not yet seen an impact on the problem of statistical inference — namely, obtaining distributional information that might allow us to control the variance and hence the risk of certain solutions.
The document provides an introduction to the gamma function Γ(x). Some key points:
1) The gamma function was introduced by Euler to generalize the factorial to non-integer values. It is defined by definite integrals and satisfies the functional equation Γ(x+1)=xΓ(x).
2) The gamma function can be defined for both positive and negative real values, except for negative integers where it has simple poles. It is related to important constants like Euler's constant.
3) The gamma function satisfies important formulas like the duplication formula, multiplication formula, and complement/reflection formula. Stirling's formula approximates the gamma function for large integer values.
Trilinear embedding for divergence-form operatorsVjekoslavKovac1
The document discusses a trilinear embedding theorem for divergence-form operators with complex coefficients. It proves that if matrices A, B, C are appropriately p,q,r-elliptic, then there is a bound on the integral of the product of the gradients of the semigroups associated with the operators. The proof uses a Bellman function technique and shows the relationship to the concept of p-ellipticity. It generalizes previous work on bilinear embeddings to the trilinear case.
This document discusses multilinear twisted paraproducts, which are generalizations of classical paraproduct operators to higher dimensions. It begins by reviewing classical paraproducts on the real line and their generalization to higher dimensions using dyadic squares. It then discusses complications that arise, such as twisted paraproducts. The document presents a unified framework for studying such operators using bipartite graphs and selections of vertices. It proves a main boundedness result and discusses special cases like classical dyadic paraproducts and dyadic twisted paraproducts. It introduces tools like Bellman functions and calculus of finite differences to analyze estimates for paraproduct-like operators on finite trees of dyadic squares.
This document summarizes research on norm-variation estimates for ergodic bilinear and multiple averages. It begins by motivating the study of ergodic averages and their convergence properties. Previous results are discussed that provide pointwise convergence and norm estimates for certain cases. The document then presents new norm-variation estimates obtained by the authors for bilinear and multiple ergodic averages over general measure-preserving systems. These estimates bound the number of jumps in the L2 norm as the averages converge. Finally, analogous results are discussed for bilinear averages on R2 and Z2, linking the estimates to established bounds for singular integrals.
This document discusses unconditionally stable finite-difference time-domain (FDTD) methods for solving Maxwell's equations numerically. It outlines FDTD algorithms such as Yee's method from 1966 which discretize the equations on a staggered grid. It also discusses the von Neumann stability analysis and compares implicit Crank-Nicolson and alternating-direction implicit methods to conventional explicit FDTD methods. The document notes the advantages of unconditionally stable methods but also mentions potential disadvantages.
The document describes the error correction model (ECM) version of Granger causality testing for determining the causal relationship between two non-stationary time series variables. It involves first testing for cointegration between the variables using the Johansen test or Engle-Granger approach. If cointegrated, the ECM version estimates an error correction model and performs Granger causality tests to examine short-run, long-run, and strong causality. The procedure and hypotheses for each test are provided along with the method for calculating the relevant F-statistics.
11.generalized and subset integrated autoregressive moving average bilinear t...Alexander Decker
This document proposes generalized integrated autoregressive moving average bilinear (GBL) time series models and subset generalized integrated autoregressive moving average bilinear (GSBL) models to achieve stationary for all nonlinear time series. It presents the models' formulations and discusses their properties including stationary, convergence, and parameter estimation. An algorithm is provided to fit the one-dimensional models. The generalized models are applied to Wolfer sunspot numbers and the GBL model is found to perform better than the GSBL model.
The document provides tables summarizing common transform pairs for the continuous-time Fourier transform, continuous-time pulsation Fourier transform, z-transform, discrete-time Fourier transform, and Laplace transform. It includes the transform, its properties, examples, and regions of convergence for each transform. The tables are intended to provide a handy reference for engineers and students working with various transformation pairs and properties.
Simple Comparison of Convergence of GeneralIterations and Effect of Variation...Komal Goyal
The document compares the convergence of Jungck-Ishikawa and Jungck-Noor iterative procedures for solving nonlinear equations. It presents 4 examples showing that the two procedures compute solutions in the same number of iterations when the parameters α, β, and γ are equal. Graphs demonstrate the effect of varying these parameters and the initial value x0 on the number of iterations needed for convergence. Both procedures consistently converge for the examples presented.
1. The document provides definitions and identities relating to theoretical computer science topics like asymptotic analysis, series, recurrences, and discrete structures.
2. It includes definitions for big O, Omega, and Theta notation used to describe the asymptotic behavior of functions.
3. Recurrences, like the master method, are presented for analyzing the runtime of divide-and-conquer algorithms.
4. Discrete structures like combinations, Stirling numbers, and trees are also covered, along with their properties and relationships.
Scattering theory analogues of several classical estimates in Fourier analysisVjekoslavKovac1
This document summarizes some classical estimates in Fourier analysis and their analogues in nonlinear Fourier analysis. It discusses Carleson's theorem on convergence of Fourier series and Fourier transforms, Hausdorff-Young inequalities bounding Lp norms, and results on lacunary trigonometric series and products. Open questions are presented about extending these classical estimates to the nonlinear setting of the SU(1,1) Fourier transform and lacunary SU(1,1) trigonometric products.
11.vibration characteristics of non homogeneous visco-elastic square plateAlexander Decker
This document presents research on the vibration characteristics of a non-homogeneous visco-elastic square plate with variations in thickness and temperature. A mathematical model is developed to analyze the effects of thermal gradients and taper parameters on the fundamental frequencies of the plate. The frequencies of the first two vibration modes are calculated for different values of the parameters using MATLAB. The results show that the frequencies decrease with increasing thermal gradient but increase with rising taper constants. The study aims to provide engineers and researchers a theoretical model to analyze thermally induced vibrations in non-homogeneous plates.
Vibration characteristics of non homogeneous visco-elastic square plateAlexander Decker
This document presents a mathematical model to analyze the vibration characteristics of a non-homogeneous visco-elastic square plate with variations in thickness and temperature. Rayleigh-Ritz method is used to derive the frequency equation for a plate with thickness tapering parabolically in one direction and temperature varying linearly in one direction and parabolically in another. Computational analysis using MATLAB calculates the fundamental frequencies for the first two vibration modes under varying thermal gradient and taper parameters. The results show that the frequency decreases with increasing thermal gradient or thickness tapering for both vibration modes.
Ban berfungsi untuk menopang beban kendaraan, mendorong dan memperlambat kendaraan, membelokkan kendaraan, serta memberikan kenyamanan saat mengemudi. Untuk itu, ban dibuat dari komponen utama seperti tread, casing, dan bead yang disusun secara radial atau bias."
Bahan ini memberikan informasi tentang bagaimana konstruksi dari mobil-mobil atau kendaraan hybrid yang sedang d kembangkan saat sekarang ini, semoga bisa bermanfaat.
Modul ini membahas tentang melepas, memasang, dan menyetel roda pada kendaraan. Terdiri atas empat kegiatan belajar yaitu mengidentifikasi jenis roda, melepas roda, pemeriksaan roda, dan memasang roda. Setelah mempelajari modul ini, peserta diharapkan mampu melepas, memasang, dan menyetel roda secara efektif, efisien, dan aman.
Modul teknologi sepeda motor (oto225 01)- sistem pengapian oleh beni setya nu...Ahmad Faozi
Modul ini membahas tentang memeriksa, merawat, memperbaiki, dan menyetel sistem pengapian konvensional dan elektronik pada sepeda motor. Modul ini terdiri atas dua kegiatan belajar yang membahas tentang sistem pengapian konvensional dan elektronik sepeda motor. Setelah mempelajari modul ini, mahasiswa diharapkan mampu memeriksa, merawat, memperbaiki, dan menyetel sistem pengapian sepeda motor.
1. Sistem manajemen mesin Toyota mulai menggunakan EFI pada 1979 dan sejak itu terus mengembangkan fitur diagnostik dan kontrol emisi.
2. Sistem ini menggunakan sensor untuk mengontrol injeksi bahan bakar, waktu pengapian, kecepatan idel, EGR, dan emisi lainnya melalui ECU.
3. ECU terhubung ke aktuator seperti injektor, katup pengapian, ISC valve, dan EGR valve untuk mengontrol kiner
Modul ini membahas sistem transmisi otomatis jenis CVT pada sepeda motor. Terdiri dari pengenalan komponen CVT seperti primary pulley, secondary pulley, v-belt, dan final gear. Juga dijelaskan prinsip kerja CVT yang mengubah rasio putaran menggunakan perubahan diameter pulley sesuai kecepatan mesin. Modul ini bertujuan membantu siswa memahami sistem transmisi otomatis CVT.
Pemeliharaan servise sistem kemudi bab 1 dan 2Purwadi ae
Dokumen tersebut membahas tentang konstruksi dan cara kerja sistem kemudi pada kendaraan. Sistem kemudi berfungsi untuk mengatur arah roda depan sesuai dengan keinginan pengemudi dengan memutar roda kemudi. Ada dua jenis sistem kemudi, yaitu manual dan power steering. Dokumen juga menjelaskan komponen-komponen utama sistem kemudi seperti roda kemudi, poros utama, gigi kemudi, lengan penghubung, serta
RPP SMK Pemeliharaan Sasis dan Pemindah Tenaga Kendaraan Ringan Kelas XIIDiva Pendidikan
Rencana pelaksanaan pembelajaran mata pelajaran Pemeliharaan Sasis dan Pemindah Tenaga Kendaraan Ringan membahas tentang roda dan ban selama 10 pertemuan. Materi pembelajaran meliputi pengertian, tipe, dan kode spesifikasi roda dan ban, prosedur perawatan dan perbaikan, serta praktik melepas, memasang, dan membalans roda dan ban.
Cálculo ii howard anton - capítulo 16 [tópicos do cálculo vetorial]Henrique Covatti
This document contains a chapter from a textbook on vector calculus. It includes 33 multi-part exercises involving concepts like divergence, curl, line integrals, and parameterizing curves. The exercises provide calculations and proofs related to vector fields and vector operations in three dimensions.
(1) The document discusses various topics in geometry including lines, circles, triangles, and coordinate geometry. Key concepts discussed include the centroid, orthocentre, and circumcentre of a triangle as well as equations of lines and circles.
(2) Formulas are provided for distances between points and lines, parallel lines, perpendiculars from points to lines, and images of points in lines. Theorems regarding secants and intercepts made by circles on lines are also summarized.
(3) Standard notations used for circles are defined, such as representing the value of the equation of a circle at a point (x1, y1) as S1. Special cases of circles like those touching or passing through
This document defines and provides examples of different types of curves in the complex plane. It begins by defining functions and graphs of functions. It then introduces curves as continuous functions from the real interval [0,1] to the complex plane. Examples are provided of both closed curves where the endpoints are equal, forming loops, and open curves where the endpoints differ. Closed curve examples include the unit circle, Rhodonea cosine/sine curves, the cardioid, double folium, limacon of Pascal, and crooked egg. Open curve examples include a line segment, parabola, cosine/sine curves, and the Archimedean spiral.
This document provides examples and explanations of vector-valued functions and the calculus of vector-valued functions. Some key points covered include:
- Examples of vector-valued functions and their domains.
- Limits of vector-valued functions, including using L'Hopital's rule.
- Derivatives of vector-valued functions and evaluating them at specific values.
- Finding parametric equations of tangent lines to vector-valued functions.
The document contains over 40 examples of vector-valued functions and calculations involving limits, derivatives, and tangent lines of vector-valued functions.
International Journal of Engineering Research and Applications (IJERA) is an open access online peer reviewed international journal that publishes research and review articles in the fields of Computer Science, Neural Networks, Electrical Engineering, Software Engineering, Information Technology, Mechanical Engineering, Chemical Engineering, Plastic Engineering, Food Technology, Textile Engineering, Nano Technology & science, Power Electronics, Electronics & Communication Engineering, Computational mathematics, Image processing, Civil Engineering, Structural Engineering, Environmental Engineering, VLSI Testing & Low Power VLSI Design etc.
Updates provided to the D-STOP Business Advisory Council at the 2017 Symposium and Board Meeting: https://ctr.utexas.edu/2018/04/12/d-stop-2017-symposium-archive/
Solution Manual Image Processing for Engineers by Yagle and Ulabyspaceradar35
This is a sample from "Sample for Solution Manual Image Processing for Engineers by Yagle and Ulaby".
Full Complete Solutions are available too.
I can send full complete Solution Manual for anyone who contact me on E. M ail.
This document presents the solution to quadruple Fourier series equations involving heat polynomials. Quadruple series equations are useful for solving four-part boundary value problems in fields like electrostatics and elasticity. The document considers two sets of quadruple series equations, the first kind and second kind, involving heat polynomials of the first and second kind. The solutions are obtained by reducing the problems to simultaneous Fredholm integral equations of the second kind. The specific equations considered and the steps to solve them using operator theory are presented.
The purpose of this note is to elaborate in how far a 4 factor affine model can generate an incomplete bond market together with the flexibility of a 3 factor flexible affine cascade structure model.
This document summarizes techniques for approximating marginal likelihoods and Bayes factors, which are important quantities in Bayesian inference. It discusses Geyer's 1994 logistic regression approach, links to bridge sampling, and how mixtures can be used as importance sampling proposals. Specifically, it shows how optimizing the logistic pseudo-likelihood relates to the bridge sampling optimal estimator. It also discusses non-parametric maximum likelihood estimation based on simulations.
This document defines and provides examples of curves and parametrized curves. It discusses regular and unit-speed curves. The key points are:
i) A parametrized curve is a continuous function from an interval to Rn. Examples of parametrized curves include ellipses, parabolas, and helices.
ii) A regular curve is one where the derivative of the parametrization is never zero. A unit-speed curve has a derivative of constant length 1.
iii) The arc-length of a curve is defined as the integral of the derivative of the parametrization. Any reparametrization of a regular curve is also regular. A curve has a unit-
1. The document discusses stochastic approximations for mortality projection models like the Lee-Carter (LC) and Cairns-Blake-Dowd (CBD) models.
2. It presents comonotonic approximations that provide conservative estimates of survival probabilities and numbers of survivors in a portfolio, avoiding complex simulations.
3. Numerical results show the conservative comonotonic approximations are close to the true values, providing useful tools for practitioners.
The document provides information on various integration techniques including the midpoint rule, trapezoidal rule, Simpson's rule, integration by parts, trigonometric substitutions, and applications of integrals such as finding the area between curves, arc length, surface area of revolution, and volume of revolution. It also covers integrals of common functions, properties of integrals, and techniques for parametric and polar coordinates.
This document discusses Fourier analysis and periodic functions. It defines periodic functions and introduces Fourier series representation of periodic functions as the sum of sinusoidal components. The key points are:
1) A periodic function can be represented by an infinite series of sinusoids of harmonically related frequencies, known as Fourier series representation.
2) The coefficients of the Fourier series (a0, an, bn) can be calculated from the integrals of the function over one period.
3) Periodic functions may exhibit odd symmetry, even symmetry, or half-wave symmetry, which determines which coefficients (an or bn) are zero.
4) Examples demonstrate the Fourier analysis of specific periodic waveforms, such as a
The convenience yield implied by quadratic volatility smiles presentation [...yigalbt
This document discusses the implied convenience yield from quadratic volatility smiles in options. It presents formulas to calculate the implied convenience yield for illiquid options based on using liquid at-the-money options as hedging instruments. The formulas depend on observable market parameters like volatility and are meant to provide a simple way to compute the implied convenience yield without historical data assumptions. However, the model relies on several undefined expressions and economic assumptions that are not fully clear.
This document contains exercises and solutions for line integrals from a chapter on the topic. It includes 6 exercises evaluating line integrals over various curves defined parametrically or through equations. It also contains exercises using Green's Theorem and evaluating line integrals for conservative vector fields. The solutions provide the parametrizations needed to set up and evaluate the line integrals.
This document discusses various methods for approximating marginal likelihoods and Bayes factors, including:
1. Geyer's 1994 logistic regression approach for approximating marginal likelihoods using importance sampling.
2. Bridge sampling and its connection to Geyer's approach. Optimal bridge sampling requires knowledge of unknown normalizing constants.
3. Using mixtures of importance distributions and the target distribution as proposals to estimate marginal likelihoods through Rao-Blackwellization. This connects to bridge sampling estimates.
4. The document discusses various methods for approximating marginal likelihoods and comparing hypotheses using Bayes factors. It outlines the historical development and connections between different approximation techniques.
Theta θ(g,x) and pi π(g,x) polynomials of hexagonal trapezoid system tb,aijcsa
A counting polynomial, called Omega Ω(G,x), was proposed by Diudea. It is defined on the ground of
“opposite edge strips” ops. Theta Θ(G,x) and Pi Π(G,x) polynomials can also be calculated by ops
counting. In this paper we compute these counting polynomials for a family of Benzenoid graphs that called
Hexagonal trapezoid system Tb,a.
This is the entrance exam paper for ISI MSQE Entrance Exam for the year 2008. Much more information on the ISI MSQE Entrance Exam and ISI MSQE Entrance preparation help available on http://crackdse.com
2. Introduction
Nonlinear effects and time-varying effects exist widely in
financial markets.
Capital asset pricing model (CAPM)
Blume, M. (1975) suggested that beta coefficients change
over time
Fabozzi, F.J. Francis, J.C. (1978) revealed that many
stocks’ beta coefficients move randomly through time
rather than remain stable
Relationship between the electricity demand and other
variables such as the income, the real price of electricity and
temperature.
Chang, Y., Martinez-Chombo, E., (2003) found that this
relationship may change over time.
Yt = β(t) Xt + t , (1.1)
2 / 36
3. Introduction
Most variables in financial industry are nonstationary.
Granger, C.W.J. (1981) and Engle, R.F., Granger, C.W.J.
(1987) introduced cointegration models in 1990s.
Cointegrating parameters are constant.
Yt = γ(zt ) Xt + t (1.2)
Cai et al. (2009) considered (1.2)
The local linear estimation
A single value of bandwidth could not make the estimation
optimal in the sense of minimizing the asymptotic mean
square error
A two-step estimation procedure
Xiao,Z. (2009) considered (1.2)
Focused on inference procedures for both parameter
instability and the hypothesis of cointegration
3 / 36
4. Introduction
Application with models (1.1)-(1.2)
y: stock price of Morgan Stanley
x: S&P 500
z: log "difference" of 5 year daily Treasury bond yield rate
and 6 month daily Treasury bill yield rate
residual of linear regression model
y∗
: log of 5 year daily Treasury bond yield rate
x∗
: log of 6 month daily Treasury bill yield rate
4 / 36
5. 2004 2008 2012
−70−50−30
time
β0
2004 2008 2012
0.0400.0500.060
time
β1
−0.4 −0.2 0.0 0.2
−30−1001020
z
γ0
−0.4 −0.2 0.0 0.2
0.0050.0150.025 z
γ1
Figure: Top two functions are estimated from model (1.1), bottom two
functions are estimated from model (1.2)
5 / 36
6. 2004 2006 2008 2010 2012 2014 2016
−15−50510
time
Estimatedresidualfrommodel1.1
2004 2006 2008 2010 2012 2014 2016
−2001030
time
Estimatedresidualfrommodel1.2
Figure: Top picture shows the residual from model (1.1), bottom
picture shows the residual from model (1.2)
6 / 36
7. Introduction
Which model is better? Which effect is true? Do these two
effects exist in the relationship between the predictors and
response?
yi = β0(ti) + γ0(zi) + {β1(ti) + γ1(zi)}xi + εi. (1.3)
We fit model (1.3) with real data and compare the goodness of
fit with models (1.1) and (1.2) in last Chapter .
7 / 36
8. Our model
For i = 1, . . . , n,
yi = β0(ti) + γ0(zi) + {β1(ti) + γ1(zi)} xi + εi, (2.1)
where
β0(ti): 1 × 1 function, γ0(zi): 1 × 1 function
β1(ti): p × 1 functions, γ1(zi): p × 1 functions
xi: p × 1, vector, either I(0) or I(1)
ti: i/n, scalar
zi: scalar, I(0)
εi: E[εi|xi, zi] = 0, E[ε2
i |xi, zi] = δ2, a strictly α-mixing
stationary process
Assume that E[γ0(zi)] = E[γ1(zi)] = 0.
8 / 36
9. Step 1: Orthogonal series estimation
Let {pκ(·), κ = 1, 2, . . .} be a standard orthogonal basis for
smooth functions on [−1, 1] and satisfy that
1
−1 pκ(x)dx = 0,
and
1
−1
pk (x)pj(x) dx =
1 if k = j;
0 otherwise.
Pκ(t, z) = [1, p1(t), . . . , pκ(t), p1(z), . . . , pκ(z)]
Θκb = (θ0,b, θ11,b, . . . , θ1κ,b, θ21,b, . . . , θ2κ,b) for b = 0, 1, . . . , p
Pκ (t, z)Θκ0 is a series approximation to β0(t) + γ0(z),
Pκ (t, z)Θκd is a series approximation to the dth component of
β1(t) + γ1(z) for d = 1, . . . , p.
9 / 36
10. Step 1: Orthogonal series estimation
Our orthogonal series estimator of β0(t) + γ0(z) and the dth
component β1d (t) + γ1d (z) of β1(t) + γ1(z) are respectively
defined as
˜β0(t) + ˜γ0(z) = Pκ (t, z)ˆΘκ0 and ˜β1d (t) + ˜γ1d (z) = Pκ (t, z)ˆΘκd
where
(ˆΘκ0, ˆΘκd ) = arg min
Θκj
n
i=1
yi−Pκ (ti, zi)Θκ0−
p
d=1
Θκd Pκ(ti, zi)xi,d
2
(3.1)
where xi,d is the dth component of xi.
10 / 36
11. Step 1: Orthogonal series estimation
B = Θκ0, Θκ1, Θκ2, . . . , Θκp]
ˆB = ˆΘκ0, ˆΘκ1, ˆΘκ2, . . . , ˆΘκp
Ai =
Pκ(ti, zi) , Pκ(ti, zi) xi,1, Pκ(ti, zi) xi,2, . . . , Pκ(ti, zi) xi,p]
Pκ(t) = 1, p1(t), . . . , pκ(t) , Pκ(z) = p1(z), . . . , pκ(z) ,
Θκbt = (θ0,b, θ11,b, . . . , θ1κ,b) ,
Θκbz = (θ21,b, . . . , θ2κ,b) for b = 0, 1, · · · p
ˆΘκbt = (ˆθ0,b, ˆθ11,b, . . . , ˆθ1κ,b) ,
ˆΘκbz = (ˆθ21,b, . . . , ˆθ2κ,b) for b = 0, 1, · · · p
Equation 3.1 can be written as
ˆB = arg min
Θκj
n
i=1
yi − Ai B
2
, (3.2)
Solution: ˆB = n
AiA
−1 n
yiAi . 11 / 36
12. Step 1: Orthogonal series estimation
It can be easily check that Pκ(t, z) = [Pκ(t) , Pκ(z) ]
Θκb = [Θκbt , Θκbz]
ˆΘκb = [ˆΘκbt , ˆΘκbz]
˜β0(ti) = Pκ (ti)ˆΘκ0t
˜β1d (ti) = Pκ (ti)ˆΘκdt , ˜β1(ti) xi = p
d=1 Pκ (ti)ˆΘκdt xi,d
˜γ0(zi) = Pκ (zi)ˆΘκ0z
˜γ1d (zi) = Pκ (zi)ˆΘκdz, ˜γ1(zi) xi = p
d=1 Pκ (zi)ˆΘκdzxi,d
Centralize ˜γ0(z) and ˜γ1(z): ˜γ∗
b(z) = ˜γb(z) − E˜γb(z) ,
˜β∗
b(t) = ˜βb(t) + E˜γb(z).
˜γ∗
b(z) and ˜β∗
b(t) are first-step estimators.
The orthogonal series estimators are used to ensure that the
biases of first-step estimators converge to zero rapidly.
12 / 36
13. Step 2: Local smoother
Taylor’s expansion for any ti in the neighborhood of t,
βk (ti) ≈ βk (t) + βk (t)(ti − t) ≡ ak + bk (ti − t) k = 0, 1
and for any zi in the neighborhood of z,
γk (zi) ≈ γk (z) + γk (z)(zi − z) ≡ ck + dk (zi − z) k = 0, 1
In the second step, we minimize
n
i=1
[yi − ˜β∗
0(ti)−˜γ∗
0(zi)− ˜β∗
1(ti) xi −{c1+d1(zi −z)} xi]2
Kh1
(zi −z)
(3.3)
and get the minimizer ˆc1 which estimates γ1(z) denoted by
ˆγ1(z), where Kh1
(·) = 1
h1
K( ·
h1
).
13 / 36
14. Step 2: Local smoother
Similarly, we minimize
n
i=1
[yi − ˜β∗
0(ti)−˜γ∗
0(zi)−˜γ∗
1(zi) xi −{a1+b1(ti −t)} xi]2
Kh2
(ti −t),
(3.4)
n
i=1
[yi −˜γ∗
0(zi)− ˜β∗
1(ti) xi −˜γ∗
1(zi) xi −{a0+b0(ti −t)}]2
Kh0
(ti −t),
(3.5)
and
n
i=1
[yi − ˜β∗
0(ti)− ˜β∗
1(ti) xi −˜γ∗
1(zi) xi −{c0+d0(zi −z)}]2
Kh4
(zi −z),
(3.6)
get minimizer ˆa0, ˆa1 and ˆc0 which estimates β0(t), β1(t) and
γ0(z) denoted by ˆβ0(t), ˆβ1(t) and ˆγ0(z).
14 / 36
15. Step 2: Local smoother
Wih1
(z) = (1, zi −z
h1
) ⊗ xi
A∗ = n
i=1 Wih1
(z) Wih1
(z)Kh1
(zi − z)
B∗ = n
i=1[yi − ˜β∗
0(ti) − ˜γ∗
0(zi) − ˜β∗
1(ti) xi]Wih1
(z) Kh1
(zi − z)
Take the first derivative of equation 3.3
ˆc1
h1
ˆd1
= [A∗]−1B∗
Similarly ˆa0, ˆc0 and ˆa1 could be easily determined.
15 / 36
16. Asymptotics when xi is stationary
Theorem 1
Under conditions (A1) ∼ (A9),
√
nh1[ ˆγ1(z) − γ1(z) −
h2
1
2 µ2(K)γ
(2)
1 (z){1 + op(1)}]
d
→
N{0, fz(z)−1δ2S−1ν0(K)}
Theorem 2
Under conditions (A1) ∼ (A9),
√
nh2[ˆβ1(t) − β1(t) −
h2
2
2 µ2(K)β
(2)
1 (t){1 + op(1)}]
d
→
N{0, δ2S−1
0 ν0(K)}
16 / 36
17. Asymptotics when xi is stationary
Theorem 3
Under conditions (A1) ∼ (A9),
√
nh4[ ˆγ0(z) − γ0(z) −
h2
4
2 µ2(K)γ
(2)
0 (z){1 + op(1)}]
d
→
N{0, fz(z)−1δ2ν0(K)}
Theorem 4
Under conditions (A1) ∼ (A9),
√
nh0[ˆβ0(t)−β0(t)−
h2
0
2 µ2(K)β
(2)
0 (t){1+op(1)}]
d
→ N{0, δ2ν0(K)}
17 / 36
18. Asymptotics when xi is nonstationary
xi = xi−1 + δi = x0 + i
s=1 δs(i ≥ 1), where δs is an I(0)
process with mean zero and variance Ωδ.
x[nr]
√
n
=
xi
√
n
=
x0
√
n
+
1
√
n
i
s=1
δs =
x0
√
n
+
1
√
n
[nr]
s=1
δs (4.1)
where r = i/n and [x] denotes the integer part of x, see Cai et
al. (2009).
Under some regularity conditions, Donsker’s theorem leads to
x[nr]
√
n
=⇒ Wδ(r) as n −→ ∞ (4.2)
where Wδ(·) is a p-dimensional Brownian motion on [0, 1] with
covariance matrix Σδ.
18 / 36
19. Asymptotics when xi is nonstationary
For any Borel measurable and totally Lebesgue integrable
function Γ(·), one has
1
n
n
i=1
Γ(x[nr])
√
n
d
−→
1
0
Γ(Wδ(s))ds as n −→ ∞ (4.3)
where
d
−→ denotes the convergence in distribution, so that, for
= 1, 2,
1
n
n
i=1
(
x[nr]
√
n
)⊗ d
−→
1
0
Wδ(s)⊗
ds ≡ Wδ, as n −→ ∞ (4.4)
see Theorem 1.2 in Berkes, I., Horváth, L. (2006) and Cai et al.
(2009)
19 / 36
20. Asymptotics when xi is nonstationary
Theorem 5
Under conditions (B1),(B2)(i),(B3) ∼(B8)
n
√
h1[ ˆγ1(z) − γ1(z) −
h2
1
2 µ2(K)γ
(2)
1 (z){1 + op(1)}]
d
→ MN Σδ(z)
where MN(Σδ(z)) is a mixed normal distribution with mean zero
and conditional covariance matrix given by
Σδ(z) = δ2ν0(K)W−1
δ,2 /fz(z)
Here, a mixed normal distribution is defined as follows.
Conditional on the random variable that appears at the
asymptotic variance, the estimator has an asymptotic normal
distribution
20 / 36
21. Asymptotics when xi is nonstationary
Theorem 6
Under conditions (B1),(B2)(ii),(B3) ∼(B8)
n
√
h2[ˆβ1(t) − β1(t) −
h2
2
2 µ2(K)β
(2)
1 (t){1 + op(1)}]
d
→ MN Σδ(t)
where MN(Σδ(t)) is a mixed normal distribution with mean zero
and conditional covariance matrix given by
Σδ(t) = δ2ν0(K)W−1
δ,2
Theorem 7
Under conditions (B1),(B2)(iii),(B3) ∼(B8),
√
nh0[ˆβ0(t)−β0(t)−
h2
0
2 µ2(K)β
(2)
0 (t){1+op(1)}]
d
→ N{0, δ2ν0(K)}
Theorem 8
Under conditions (B1),(B2)(iv),(B3) ∼(B8),
√
nh4[ˆγ0(z) − γ0(z) −
h2
4
2 µ2(K)γ
(2)
0 (z){1 + op(1)}]
d
→
N{0, f−1
z (z)δ2ν0(K)}
21 / 36
22. Simulation
B-spline
κ = 8
Standard normal kernel
We consider the following model
yi = β0(ti)+γ0(zi)+(β1(ti)+γ1(zi))xi,1+(β2(ti)+γ2(zi))xi,2+εi
= e3ti
+ 20ti + (0.5z3
i − 1.5z2
i − 0.5zi + 8)
+(−40t2
i −20ti+1.5z2
i −7.5zi−8)xi,1+(e4ti
+2ti+3z2
i −6zi−16)xi,2+εi
(5.1)
where γ0(zi) = 0.5z3
i − 1.5z2
i − 0.5zi + 8,
γ1(zi) = 1.5z2
i − 7.5zi − 8 and γ2(zi) = 3z2
i − 6zi − 16. p = 2.
ε ∼ N(0, 0.25), zi = 0.3zi−1 + Ui and Ui ∼ Uniform (−4, 4)
Eγ0(zi) = Eγ1(zi) = Eγ2(zi) = 0.
22 / 36
23. Simulation with stationary xi
x1,1 = x1,2 = 0
xi,1 = 0.9xi−1,1 + δ1i
δ1i ∼ t(3)
xi,2 = 0.6xi−1,2 + δ2i
δ2i ∼ t(7)
y is generated from above model (5.1)
x1, x2 and y all are stationary.
10 grid points for β functions and 40 grid points for γ functions
500 simulations at each grid point
Simulation results are shown in Figure 3 for n = 100.
Simulation results are shown in Figure 4 for n = 400.
23 / 36
24. 0.0 0.2 0.4 0.6 0.8 1.0
01030
t
β0
−4 −2 0 2 4
−50−30−1010
z
γ0
0.0 0.2 0.4 0.6 0.8 1.0
−60−200
t
β1
−4 −2 0 2 4
−2002040
z
γ1
0.0 0.2 0.4 0.6 0.8 1.0
0204060
t
β2
−4 −2 0 2 4
−200204060
z
γ2
Figure: Estimated function β and γ, their mediums and 95%
pointwise confidence intervals for Model 5.1 when x is stationary and
n = 100 24 / 36
25. 0.0 0.2 0.4 0.6 0.8 1.0
01030
t
β0
−4 −2 0 2 4
−50−30−1010
z
γ0
0.0 0.2 0.4 0.6 0.8 1.0
−60−200
t
β1
−4 −2 0 2 4
−2002040
z
γ1
0.0 0.2 0.4 0.6 0.8 1.0
0204060
t
β2
−4 −2 0 2 4
−200204060
z
γ2
Figure: Estimated function β and γ, their mediums and 95%
pointwise confidence intervals for Model 5.1 when x is stationary and
n = 400 25 / 36
26. Simulation with nonstationary xi
x1,1 = x1,2 = 0
xi,1 = xi−1,1 + δ1i
δ1i ∼ t(3)
xi,2 = xi−1,2 + δ2i
δ2i ∼ t(7)
y is generated from above model (5.1)
x1, x2 and y all are nonstationary, xi and yi are cointegration.
10 grid points for β functions and 40 grid points for γ functions
500 simulations at each grid point
Simulation results are shown in Figure 5 for n = 100.
Simulation results are shown in Figure 6 for n = 400.
26 / 36
27. 0.0 0.2 0.4 0.6 0.8 1.0
01030
t
β0
−4 −2 0 2 4
−50−30−1010
z
γ0
0.0 0.2 0.4 0.6 0.8 1.0
−60−200
t
β1
−4 −2 0 2 4
−2002040
z
γ1
0.0 0.2 0.4 0.6 0.8 1.0
0204060
t
β2
−4 −2 0 2 4
−200204060
z
γ2
Figure: Estimated function β and γ, their mediums and 95%
pointwise confidence intervals for Model 5.1 when x is nonstationary
and n = 100 27 / 36
28. 0.0 0.2 0.4 0.6 0.8 1.0
01030
t
β0
−4 −2 0 2 4
−50−30−1010
z
γ0
0.0 0.2 0.4 0.6 0.8 1.0
−60−200
t
β1
−4 −2 0 2 4
−2002040
z
γ1
0.0 0.2 0.4 0.6 0.8 1.0
0204060
t
β2
−4 −2 0 2 4
−200204060
z
γ2
Figure: Estimated function β and γ, their mediums and 95%
pointwise confidence intervals for Model 5.1 when x is nonstationary
and n = 400 28 / 36
29. Real example
5 year daily Treasury bond yield rate
6 month daily Treasury bill yield rate
Stock price of Morgan Stanley and price of S&P500
All data are from the Jan. 2nd, 2003 to Dec. 31st, 2015. The
sample size is 3249.
Stock price of Morgan Stanley and price of S&P500 are
nonstationary
Log "difference" of 5 year daily Treasury bond yield rate and 6
month daily Treasury bill yield rate is stationary
yi = β0(ti−1) + γ0(zi−1) + (β1(ti−1) + γ1(zi−1))xi−1 + i. (6.1)
z: log "difference" of 5 year daily Treasury bond yield rate and 6
month daily Treasury bill yield rate
y: stock price of Morgan Stanley x: price of S&P500.
29 / 36
30. ADF Test Statistic P VALUE
Stock price of Morgan Stanley -0.5896 0.4284
Price of S&P500 1.3095 0.9522
log "difference" of Treasury yield rate -3.3093 < 0.01
Table: ADF test for stock price of Morgan Stanley, price of S&P500
and log "difference" of 5 year daily Treasury bond yield rate and 6
month daily Treasury bill yield rate
30 / 36
31. 2004 2008 2012
−100−60−200
time
β0
2004 2008 2012
0.020.060.10
time
β1
−0.4 −0.2 0.0 0.2
−20−10010
yield rate
γ0
−0.4 −0.2 0.0 0.2
−0.0100.0000.010 yield rate
γ1
Figure: Estimated functions from model 6.1
31 / 36
32. Real example
Variance of the residual model 1.1 model 1.2 model 6.1
13.380 68.504 5.859
Table: variance of the residual in each model
32 / 36
33. 2004 2006 2008 2010 2012 2014 2016
0204060
time
price
2004 2006 2008 2010 2012 2014
0.020.060.10
time
functionofcoefficient
Figure: Estimated stock price and function of coefficient from model
6.1
33 / 36
34. Real example: one step forecast
Split sample into two parts: training sample, the first 3000 data
and testing sample, the remaining 249 data.
Define one step forecast ˆyj for y at time j as following:
ˆyj = ˆβ0(tj−1) + ˆγ1(zj−1) + ( ˆβ1(tj−1) + ˆγ1(zj−1))xj−1 (6.2)
where j from 3001 to 3249 and ˆβ0, ˆγ0
ˆβ1 and ˆγ1 are estimated
by the proposed two-step estimation method using only the
data from 1 to j − 1
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35. 2004 2006 2008 2010 2012 2014 2016
0102030405060
x
yscale
Figure: ˆy and One step forecast (6.2)
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