An Iterative Incremental Learning Algorithm for Complex-Valued Hopfield Associative Memory

Size: px
Start display at page:

Download "An Iterative Incremental Learning Algorithm for Complex-Valued Hopfield Associative Memory"

Transcription

1 An Iterative Incremental Learning Algorithm for Complex-Value Hopfiel Associative Memory aoki Masuyama (B) an Chu Kiong Loo Faculty of Computer Science an Information Technology, University of Malaya, Kuala Lumpur, Malaysia Abstract. This paper iscusses a complex-value Hopfiel associative memory with an iterative incremental learning algorithm. The mathematical proofs erive that the weight matrix is approximate as a weight matrix by the complex-value pseuo inverse algorithm. Furthermore, the minimum number of iterations for the learning sequence is efine with maintaining the network stability. From the result of simulation experiment in terms of memory capacity an noise tolerance, the propose moel has the superior ability than the moel with a complexvalue pseuo inverse learning algorithm. Keywors: Associative memory Complex-value moel Incremental learning 1 Introuction In the past ecaes, numerous types of Artificial Intelligence moels have been propose in the fiel of computer science in orer to realize the humanlike abilities base on the analysis an moeling of essential functions of a biological neuron an its complicate networks in a computer. It has been note that one of the interesting an challenging subjects is the imitation of memory function of the human brain. In the past ecaes, several types of artificial associative memory moels an its improvements have introuce such as Hopfiel Associative Memory (HAM) [7], an Bi-/Multi-irectional Associative Memory (BAM, MAM) [6,11]. However, the majority of moels are limite as offline an one-shot learning rules. Storkey an Valabregue [14] propose an incremental learning algorithm for HAM base on the Hebb/Anti-Hebb learning. Chartier an Boukaoum [3] also propose an analyze the moel with a self-convergent iterative learning rule base on the Hebb/anti-Hebb approach, an a nonlinear output function Dieerich an Opper [4] propose a Wirow-Hoff type learning. However, the convergence of these moels is quite slow when the memory patterns are correlate. The local iterative learning, on the other han, which is propose by Blatt an Vergini [2] can be ealt with above kin of problems. c Springer International Publishing AG 2016 A. Hirose et al. (Es.): ICOIP 2016, Part IV, LCS 9950, pp , DOI: /

2 424. Masuyama an C.K. Loo Moreover, this moel is able to efine the minimum number of learning iterations with maintaining a network stability. In regar as events in the real worl, information representation using binary or bipolar state is insufficient. Jankowski et al. [9] have introuce complex-value Hopfiel Associative Memory (CHAM) with neurons processing a complex-value iscrete activation function. Conventionally, numerous stuies that improve complex-value moels are introuce base on the improvements for real-value moels. Lee [13] applie a complex-value projection matrix to CHAM (PInvCHAM) an analyze the stability of the moel by using energy function. The learning algorithm of these moels, however, are characterize by a batch learning. Isokawa et al. [8] analyze the stability of complex-value Hopfiel moel with from a local iterative learning scheme viewpoint though the learning algorithm is Hebb learning base. In this paper, we introuce a local iterative incremental learning with CHAM base on Blatt an Vergini learning algorithm [2]. Here, we shall call the propose moel as BVCHAM. The noteworthy features of BVCHAM are escribe as follows; (i) the resultant of weight matrix in BVCHAM is approximate to the projection matrix operation. The network is able to store the patterns though the number of store patterns p is larger than the number of neurons (It is known that the memory capacity is limite as p<with a projection matrix learning moel.), an (ii) the learning algorithm is guarantee to calculate a weight matrix within a finite number of iterations with keeping a network stability. The paper is ivie as follows; Sect. 2 escribes the ynamics of BVCHAM. Section 3 presents the network stability analysis for BVCHAM. In Sect. 4, it will be presente simulation experiments of BVCHAM in terms of the memory capacity an noise tolerance comparing with PinvCHAM. Concluing remarks are presente in Sect Dynamics of a Local Iterative Learning for CHAM This section presents the ynamics of a propose moel, we shall call as BVCHAM. Let us suppose that the moel stores complex-value funamental memory vectors X p, where X p =[x p 1,xp 2,...,xp ]T, enotes the number of neurons, an p enotes the number of patterns. The components x p i are efine as follows; x p i exp [j2πn/q]q 1 n=0, i =1, 2,..., (1) where q enotes a quantization value on the complex value unit circle. Here, supposing a new pattern X l stores to the network by upating the weight matrix W (l 1) that alreay has (l 1) patterns embee. X (l) is presente n l times to the network as follows; n l W (l) = W (l 1) + ΔW (l) (2) =1

3 An Iterative Incremental Learning Algorithm for Complex-Value HAM 425 where, ΔW is efine as a following; ΔW (l) = k 1 ( x l )( ) i h i x l j h j /. (3) The local fiel h i which changes ( 1) times is performe as a following; [ ] h i = j=1 ( 1 W (l 1) ij + r=1 W (l) r ) ij x l j. (4) Similar with Eq. (4), the local fiel h j is efine. Here, the minimum number of iterations n l can be efine as a following; n l log k [/ (π/q T ) 2] (5) where, a parameter k, calle memory coefficient, is a real number that belongs to the interval 0 <k 4, an a parameter T is set between 0 T < π/q.it allows to perform in orer to achieve aligne local fiels with values of at least T [2]. q enotes a quantization value on the complex unit circle, which is escribe in a following part. The iterative weight upate is performe until satisfying the criterion as T>error ɛ, namely; ( ) T>ɛ= arg hi. (6) i=1 In summary, the process of weight upate is escribe as Algorithm 1. For the association process, the self-connections eliminate weight matrix W is utilize. On the other han, the weight matrix W which is calculate by Algorithm 1 is applie to the further incremental learning process. X l i Algorithm 1. An algorithm for a weight matrix W (l) Require: weight matrix W (l 1), funamental memory vector X l, error parameter T,memorycoefficient k Ensure: weight matrix W (l) if l =1then Initialize W as a zero matrix en if Set =1 Calculate an error ɛ using Eq. (6) while n l an ɛ>t o Calculate a weight matrix W (l) using Eqs. (2) an (3) Calculate an error ɛ using Eq. (6) Set +1 en while The activation function is a complex projection function that operates on each component of the state vector as a following; { Z exp(j2πn/q), If arg exp(j2πn/q)} <π/qan Z 0 φ(z) = (7) previous state, If Z = 0

4 426. Masuyama an C.K. Loo where, arg(α) enotes the phase angle of α which is taken to range over ( π, π). q enotes a quantization value on the complex unit circle, n takes an integer. We utilize a iscrete complex unit circle moel to etermine recalle signals. Thus, the ynamics of network is summarize as follows; h (t) = W X (t) (8) ( ) X (t+1) = φ h (t) (9) The stationary conitions for the recalle memory vector are escribe as a following; ( ) h 0 arg X p < π q. (10) 3 etwork Stability Analysis In this section, base on Blatt an Vergini algorithm [2], the conitions of network stability in BVCHAM will be iscusse, an it will be erive a criterion for the number of iterations n l to guarantee the stability of X l. Here, Dirac notation in C is utilize for simplifying the representation of proofs. Thus, Eqs. (3) an (4) can be escribe as follows; ΔW l = k 1 Xl h X l h (11) [ ] 1 h = W (l 1) + X l (12) r=1 ΔW l r here, it satisfies X l h = X l h. First of all, the changes of weight connection when a new memory vector is repeate to the network is analyze. Here, ΔW (l) (1 ) is efine as a following; r=1 ΔW (l) r = Q (l) E (l 1) X l X l E (l 1) (13) where, E (l) = I W (l) (14) here, I enotes an ientity matrix which has same imension with W (l). It assumes that Eq. (13) hols for -th iteration in orer to prove ( + 1)-th iteration. The ifference of weight connection between the -th an ( + 1)-th iteration with a memory vector X l an its local fiel h is expresse by Eqs. (12), (13) an (14), as follows; X l h =(1 a (l) Q (l) )E(l 1) X l (15)

5 An Iterative Incremental Learning Algorithm for Complex-Value HAM 427 where, a (l) = Xl E (l 1) X l. (16) Thechangein( + 1)-th iteration is expresse by Eqs. (11) an (15) asa following; ( ) 2 ΔW (l) +1 = k 1 a (l) Q (l) E (l 1) X l X l E (l 1). (17) Comparing with Eqs. (13) an (17), it can be regare as a proportional relation with the same operator. Thus, the following recurrence relations are obtaine; Q (l) 1 = 1 (18) Q (l) = Q(l) 1 + k 1 ( 1 a (l) Q (l) 1) 2. (19) From the Eqs. (13) an (14), Eq. (2) is represente as a following; E (l) = E (l 1) Q n (l) E (l 1) X l X l E (l 1) l. (20) Therefore, when a new memory vector is presente to the network, an operator which is proportional to the projector onto E (l 1) X l is ae to the weight connection. Accoring to Eq. (11), ΔW increases exponentially with the number of iterations. However, if the following conition is satisfie, the elements of ΔW remain finite, i.e.; 0 φ E (l) φ φ φ for all φ C. (21) In the first learning step, it maintains E (0) = I an Q (1) = 1. Furthermore, base on Cauchy Schwarz inequality, Eq. (21) is verifie for l = 1. Here, assumingthateq.(21) is vali for l. Then, the eigenvalues of E (l) take between 0 to 1. Therefore, the following conition is satisfie; E (l) φ 2 φ E (l) φ. (22) Let us suppose that a (l+1) =0,E (l) X l+1 = 0 is erive from Eqs. (16) an (22), then E (l+1) = E (l) is maintaine from Eq. (20). Thus, Eq. (21) is also satisfie for (l+1). In contrast, in case of a (l+1) 0, it is prove by the inuctive hypothesis 0 <a (l+1) 1. Furthermore, accoring to [2], following conitions are maintaine; 0 <a (l) Q (l) 1 a (l) Q (l) 1. (23) ). (24) ( k a (l) From the following part, it focuses the memorize pattern X μ (1 μ<l) an its local fiel h are able to be closer than other memorize patterns. The

6 428. Masuyama an C.K. Loo istance between X μ an h ecreases exponentially with the number of iterations. This is erive by the inuction process. First of all, the following conition is maintaine by the Eqs. (14) an (22); X μ W (l) X μ 2 X μ E (l) X μ. (25) Here, Eq. (20) is generalize as a following; E (l) = E (μ) l ν=μ+1 Q ν E (ν 1) X ν X ν E (ν 1) n ν. (26) Then, X μ multiplie on the left han sie, an X μ multiplie on the right han sie to Eq. (26), therefore; X μ E (l) X μ X μ E (μ) X μ. (27) For the Eq. (20) with a μ-th memory vector, X μ is multiplie on the left han sie, an X μ is multiplie on the right han sie, i.e.; X μ E (μ) X μ = X μ E (μ 1) X μ Q n (μ) ( X μ E (μ 1) X μ ) 2 μ. (28) Consiering with Eq. (16), Eq. (28) is escribe as a following; ( ) X μ E (μ) X μ = a (μ) 1 a (μ) Q n (μ) μ. (29) Furthermore, an a (μ) multiplie to Eq. (24) with a μ-th memory vector, i.e.; a (μ) ( 1 a (μ) Q (μ) n μ ) k nμ. (30) From Eqs. (25), (27), (29) an (30), the following conition is obtaine; X μ W (l) X μ 2 X μ E (l) X μ X μ E (μ) X μ = a (μ) ( 1 a (μ) Q (μ) n μ ) k nμ. (31) Accoring to the stability conition as Eq. (10), Eq. (31) is escribe as a following; X μ W (l) X μ 2 k nμ ( ) 2 π q T (32) where, q enotes a quantization value on the complex unit circle. The optimal stability can be controlle by the parameter T [5, 12]. In aition, the network stability is guarantee in case of T = 0. Furthermore, from Eq. (32), the minimum number of iterations n l is erive as Eq. (5).

7 An Iterative Incremental Learning Algorithm for Complex-Value HAM Simulation Experiment This section presents the simulation experiments comparing with a pseuo inverse learning moel (PInvCHAM) [1] an a propose moel (BVCHAM), in terms of memory capacity an noise tolerance. 4.1 Conition Table 1 shows the simulation conitions to evaluate the memory capacity an the noise tolerance. In this experiment, the number of pairs p is increase from 1 to 220 at intervals of 10 (p =1, 10, 20,...,220). oise tolerance is a significant property for the associative memory. Typically, noise is roughly ivie into two types in associative memory. One is the similarity of the store patterns, another is the store patterns contain noise itself. Due to the propose moel has the similar properties with a pseuo inverse learning moel, it is expecte that the propose moel is able to learn the correlate memory vectors without errors. In this paper, therefore, we consier about a latter type of noise which is containe in an initial input with 0 to 50 [%] by the salt & pepper noise. Furthermore, it is known that the ability of a complex-value associative memory is epenent upon the number of ivisions of a complex-value unit circle. Here, we set 4, 8 an 16 ivisions for this simulation. Table 1. Simulation conition. umber of pairs p : umber of neurons : 200 umber of ivisions q: 4,8,16 Data set configuration: Amplitue: 1.0, Phase: Ran 4.2 Result In Fig. 1, PInvCHAM maintains the high recall rate, especially R = 0.0. However, ue to the limitation of the pseuo inverse learning, the recall rate is suenly roppe uner the conition p. As shown in Fig. 2, ue to the weight matrix of BVCHAM can be approximate as the weight matrix by a pseuo inverse learning, the recall rate of BVCHAM shows the similar or superior results (especially in Fig. 2(a)) than PInvCHAM. Here, it focuses on the results with R =0.0 in Fig. 2. Since the weight matrix of BVCHAM is not equal to the ientity matrix at p =, BVCHAM is able to maintain the high recall rate than PInvCHAM even if the conition is uner p. From the above results, it is regare that BVCHAM has the following noteworthy avantages; although a propose learning algorithm is incremental, the ability can be comparable to a batch learning as a pseuo inverse learning algorithm, an it is able to overcome the limitation of a pseuo inverse learning algorithm that is characterize by p<.

8 430. Masuyama an C.K. Loo (a) q =4 (b)q =8 (c) q =16 Fig. 1. Results of recall ratio for a pseuo inverse learning moel. (a) q =4 (b)q =8 (c) q =16 Fig. 2. Results of recall ratio for a BV incremental learning moel. 5 Conclusion This paper introuce a local iterative incremental learning algorithm for a complex-value Hopfiel associative memory. Furthermore, we presente the network stability analysis which erive the weight matrix of BVCHAM is approximate as a weight matrix from a complex-value pseuo inverse learning algorithm, an the minimum number of iterations with maintaining a network convergence. From the result of simulation experiment in terms of memory capacity an noise tolerance, BVCHAM has the superior ability than the moels with the Hebb learning an a complex-value pseuo inverse learning algorithm. oteworthy, unlike the moel with a pseuo inverse learning algorithm, the propose moel is able to maintain the high recall rate even if the number of store patterns is larger than the number of neurons. As a future work, we will exten the propose incremental learning algorithm to hetero-association moels, such as bi/multi-irectional associative memory moels [10]. Acknowlegments. The authors woul like to acknowlege a scholarship provie by the University of Malaya (Fellowship Scheme). This research is supporte by High Impact Research UM.C/625/1/HIR/MOHE/FCSIT/10 from University of Malaya.

9 An Iterative Incremental Learning Algorithm for Complex-Value HAM 431 References 1. Albert, A.: Regression an the Moore-Penrose Inverse. Acaemic Press, ew York (1972) 2. Blatt, M.G., Vergini, E.G.: eural networks: a local learning prescription for arbitrary correlate patterns. Phys. Rev. Lett. 66(13), 1793 (1991) 3. Chartier, S., Boukaoum, M.: A biirectional heteroassociative memory for binary an grey-level patterns. IEEE Trans. eural etw. 17(2), (2006) 4. Dieerich, S., Opper, M.: Learning of correlate patterns in spin-glass networks by local learning rules. Phys. Rev. Lett. 58(9), 949 (1987) 5. Garner, E.: Optimal basins of attraction in ranomly sparse neural network moels. J. Phys. A: Math. Gen. 22(12), 1969 (1989) 6. Hagiwara, M.: Multiirectional associative memory. In: International Joint Conference on eural etworks, vol. 1, pp. 3 6 (1990) 7. Hopfiel, J.J.: eural networks an physical systems with emergent collective computational abilities. Proc. at. Aca. Sci. 79(8), (1982) 8. Isokawa, T., ishimura, H., Matsui,.: An iterative learning scheme for multistate complex-value an quaternionic Hopfiel neural networks (2009) 9. Jankowski, S., Lozowski, A., Zuraa, J.: Complex-value multistate neural associative memory. IEEE Trans. eural etw. 7(6), (1996) 10. Kobayashi, M., Yamazaki, H.: Complex-value multiirectional associative memory. Electr. Eng. Jpn. 159(1), (2007) 11. Kosko, B.: Constructing an associative memory. Byte 12(10), (1987) 12. Krauth, W., Mézar, M.: Learning algorithms with optimal stability in neural networks. J. Phys. A: Math. Gen. 20(11), L745 (1987) 13. Lee, D.L.: Improvements of complex-value Hopfiel associative memory by using generalize projection rules. IEEE Trans. eural etw. 17(5), (2006) 14. Storkey, A.J., Valabregue, R.: The basins of attraction of a new Hopfiel learning rule. eural etw. 12(6), (1999)

Slide10 Haykin Chapter 14: Neurodynamics (3rd Ed. Chapter 13)

Slide10 Haykin Chapter 14: Neurodynamics (3rd Ed. Chapter 13) Slie10 Haykin Chapter 14: Neuroynamics (3r E. Chapter 13) CPSC 636-600 Instructor: Yoonsuck Choe Spring 2012 Neural Networks with Temporal Behavior Inclusion of feeback gives temporal characteristics to

More information

A simple model for the small-strain behaviour of soils

A simple model for the small-strain behaviour of soils A simple moel for the small-strain behaviour of soils José Jorge Naer Department of Structural an Geotechnical ngineering, Polytechnic School, University of São Paulo 05508-900, São Paulo, Brazil, e-mail:

More information

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations Diophantine Approximations: Examining the Farey Process an its Metho on Proucing Best Approximations Kelly Bowen Introuction When a person hears the phrase irrational number, one oes not think of anything

More information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

Lower Bounds for the Smoothed Number of Pareto optimal Solutions Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.

More information

A Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential

A Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential Avances in Applie Mathematics an Mechanics Av. Appl. Math. Mech. Vol. 1 No. 4 pp. 573-580 DOI: 10.4208/aamm.09-m0946 August 2009 A Note on Exact Solutions to Linear Differential Equations by the Matrix

More information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments 2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor

More information

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations Optimize Schwarz Methos with the Yin-Yang Gri for Shallow Water Equations Abessama Qaouri Recherche en prévision numérique, Atmospheric Science an Technology Directorate, Environment Canaa, Dorval, Québec,

More information

Conservation laws a simple application to the telegraph equation

Conservation laws a simple application to the telegraph equation J Comput Electron 2008 7: 47 51 DOI 10.1007/s10825-008-0250-2 Conservation laws a simple application to the telegraph equation Uwe Norbrock Reinhol Kienzler Publishe online: 1 May 2008 Springer Scienceusiness

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische

More information

Quantum mechanical approaches to the virial

Quantum mechanical approaches to the virial Quantum mechanical approaches to the virial S.LeBohec Department of Physics an Astronomy, University of Utah, Salt Lae City, UT 84112, USA Date: June 30 th 2015 In this note, we approach the virial from

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

Lie symmetry and Mei conservation law of continuum system

Lie symmetry and Mei conservation law of continuum system Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive

More information

Qubit channels that achieve capacity with two states

Qubit channels that achieve capacity with two states Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March

More information

Least-Squares Regression on Sparse Spaces

Least-Squares Regression on Sparse Spaces Least-Squares Regression on Sparse Spaces Yuri Grinberg, Mahi Milani Far, Joelle Pineau School of Computer Science McGill University Montreal, Canaa {ygrinb,mmilan1,jpineau}@cs.mcgill.ca 1 Introuction

More information

A Second Time Dimension, Hidden in Plain Sight

A Second Time Dimension, Hidden in Plain Sight A Secon Time Dimension, Hien in Plain Sight Brett A Collins. In this paper I postulate the existence of a secon time imension, making five imensions, three space imensions an two time imensions. I will

More information

IPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy

IPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy IPA Derivatives for Make-to-Stock Prouction-Inventory Systems With Backorers Uner the (Rr) Policy Yihong Fan a Benamin Melame b Yao Zhao c Yorai Wari Abstract This paper aresses Infinitesimal Perturbation

More information

Agmon Kolmogorov Inequalities on l 2 (Z d )

Agmon Kolmogorov Inequalities on l 2 (Z d ) Journal of Mathematics Research; Vol. 6, No. ; 04 ISSN 96-9795 E-ISSN 96-9809 Publishe by Canaian Center of Science an Eucation Agmon Kolmogorov Inequalities on l (Z ) Arman Sahovic Mathematics Department,

More information

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013 Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing

More information

On the number of isolated eigenvalues of a pair of particles in a quantum wire

On the number of isolated eigenvalues of a pair of particles in a quantum wire On the number of isolate eigenvalues of a pair of particles in a quantum wire arxiv:1812.11804v1 [math-ph] 31 Dec 2018 Joachim Kerner 1 Department of Mathematics an Computer Science FernUniversität in

More information

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21 Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting

More information

Chapter 2 Lagrangian Modeling

Chapter 2 Lagrangian Modeling Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie

More information

Multi-robot Formation Control Using Reinforcement Learning Method

Multi-robot Formation Control Using Reinforcement Learning Method Multi-robot Formation Control Using Reinforcement Learning Metho Guoyu Zuo, Jiatong Han, an Guansheng Han School of Electronic Information & Control Engineering, Beijing University of Technology, Beijing

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

u t v t v t c a u t b a v t u t v t b a

u t v t v t c a u t b a v t u t v t b a Nonlinear Dynamical Systems In orer to iscuss nonlinear ynamical systems, we must first consier linear ynamical systems. Linear ynamical systems are just systems of linear equations like we have been stuying

More information

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control 19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior

More information

One-dimensional I test and direction vector I test with array references by induction variable

One-dimensional I test and direction vector I test with array references by induction variable Int. J. High Performance Computing an Networking, Vol. 3, No. 4, 2005 219 One-imensional I test an irection vector I test with array references by inuction variable Minyi Guo School of Computer Science

More information

Schrödinger s equation.

Schrödinger s equation. Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of

More information

Estimation of the Maximum Domination Value in Multi-Dimensional Data Sets

Estimation of the Maximum Domination Value in Multi-Dimensional Data Sets Proceeings of the 4th East-European Conference on Avances in Databases an Information Systems ADBIS) 200 Estimation of the Maximum Domination Value in Multi-Dimensional Data Sets Eleftherios Tiakas, Apostolos.

More information

ELEC3114 Control Systems 1

ELEC3114 Control Systems 1 ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.

More information

Situation awareness of power system based on static voltage security region

Situation awareness of power system based on static voltage security region The 6th International Conference on Renewable Power Generation (RPG) 19 20 October 2017 Situation awareness of power system base on static voltage security region Fei Xiao, Zi-Qing Jiang, Qian Ai, Ran

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

1 Heisenberg Representation

1 Heisenberg Representation 1 Heisenberg Representation What we have been ealing with so far is calle the Schröinger representation. In this representation, operators are constants an all the time epenence is carrie by the states.

More information

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d A new proof of the sharpness of the phase transition for Bernoulli percolation on Z Hugo Duminil-Copin an Vincent Tassion October 8, 205 Abstract We provie a new proof of the sharpness of the phase transition

More information

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k A Proof of Lemma 2 B Proof of Lemma 3 Proof: Since the support of LL istributions is R, two such istributions are equivalent absolutely continuous with respect to each other an the ivergence is well-efine

More information

Combinatorica 9(1)(1989) A New Lower Bound for Snake-in-the-Box Codes. Jerzy Wojciechowski. AMS subject classification 1980: 05 C 35, 94 B 25

Combinatorica 9(1)(1989) A New Lower Bound for Snake-in-the-Box Codes. Jerzy Wojciechowski. AMS subject classification 1980: 05 C 35, 94 B 25 Combinatorica 9(1)(1989)91 99 A New Lower Boun for Snake-in-the-Box Coes Jerzy Wojciechowski Department of Pure Mathematics an Mathematical Statistics, University of Cambrige, 16 Mill Lane, Cambrige, CB2

More information

Euler equations for multiple integrals

Euler equations for multiple integrals Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................

More information

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS Mauro Boccaoro Magnus Egerstet Paolo Valigi Yorai Wari {boccaoro,valigi}@iei.unipg.it Dipartimento i Ingegneria Elettronica

More information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

Iterated Point-Line Configurations Grow Doubly-Exponentially

Iterated Point-Line Configurations Grow Doubly-Exponentially Iterate Point-Line Configurations Grow Doubly-Exponentially Joshua Cooper an Mark Walters July 9, 008 Abstract Begin with a set of four points in the real plane in general position. A to this collection

More information

Discrete Operators in Canonical Domains

Discrete Operators in Canonical Domains Discrete Operators in Canonical Domains VLADIMIR VASILYEV Belgoro National Research University Chair of Differential Equations Stuencheskaya 14/1, 308007 Belgoro RUSSIA vlaimir.b.vasilyev@gmail.com Abstract:

More information

SYSTEMS OF DIFFERENTIAL EQUATIONS, EULER S FORMULA. where L is some constant, usually called the Lipschitz constant. An example is

SYSTEMS OF DIFFERENTIAL EQUATIONS, EULER S FORMULA. where L is some constant, usually called the Lipschitz constant. An example is SYSTEMS OF DIFFERENTIAL EQUATIONS, EULER S FORMULA. Uniqueness for solutions of ifferential equations. We consier the system of ifferential equations given by x = v( x), () t with a given initial conition

More information

Applications of First Order Equations

Applications of First Order Equations Applications of First Orer Equations Viscous Friction Consier a small mass that has been roppe into a thin vertical tube of viscous flui lie oil. The mass falls, ue to the force of gravity, but falls more

More information

Nonlinear Dielectric Response of Periodic Composite Materials

Nonlinear Dielectric Response of Periodic Composite Materials onlinear Dielectric Response of Perioic Composite aterials A.G. KOLPAKOV 3, Bl.95, 9 th ovember str., ovosibirsk, 639 Russia the corresponing author e-mail: agk@neic.nsk.su, algk@ngs.ru A. K.TAGATSEV Ceramics

More information

Generalized-Type Synchronization of Hyperchaotic Oscillators Using a Vector Signal

Generalized-Type Synchronization of Hyperchaotic Oscillators Using a Vector Signal Commun. Theor. Phys. (Beijing, China) 44 (25) pp. 72 78 c International Acaemic Publishers Vol. 44, No. 1, July 15, 25 Generalize-Type Synchronization of Hyperchaotic Oscillators Using a Vector Signal

More information

4. Important theorems in quantum mechanics

4. Important theorems in quantum mechanics TFY4215 Kjemisk fysikk og kvantemekanikk - Tillegg 4 1 TILLEGG 4 4. Important theorems in quantum mechanics Before attacking three-imensional potentials in the next chapter, we shall in chapter 4 of this

More information

arxiv:physics/ v2 [physics.ed-ph] 23 Sep 2003

arxiv:physics/ v2 [physics.ed-ph] 23 Sep 2003 Mass reistribution in variable mass systems Célia A. e Sousa an Vítor H. Rorigues Departamento e Física a Universiae e Coimbra, P-3004-516 Coimbra, Portugal arxiv:physics/0211075v2 [physics.e-ph] 23 Sep

More information

IERCU. Institute of Economic Research, Chuo University 50th Anniversary Special Issues. Discussion Paper No.210

IERCU. Institute of Economic Research, Chuo University 50th Anniversary Special Issues. Discussion Paper No.210 IERCU Institute of Economic Research, Chuo University 50th Anniversary Special Issues Discussion Paper No.210 Discrete an Continuous Dynamics in Nonlinear Monopolies Akio Matsumoto Chuo University Ferenc

More information

Sturm-Liouville Theory

Sturm-Liouville Theory LECTURE 5 Sturm-Liouville Theory In the three preceing lectures I emonstrate the utility of Fourier series in solving PDE/BVPs. As we ll now see, Fourier series are just the tip of the iceberg of the theory

More information

Physics 5153 Classical Mechanics. The Virial Theorem and The Poisson Bracket-1

Physics 5153 Classical Mechanics. The Virial Theorem and The Poisson Bracket-1 Physics 5153 Classical Mechanics The Virial Theorem an The Poisson Bracket 1 Introuction In this lecture we will consier two applications of the Hamiltonian. The first, the Virial Theorem, applies to systems

More information

Abstract A nonlinear partial differential equation of the following form is considered:

Abstract A nonlinear partial differential equation of the following form is considered: M P E J Mathematical Physics Electronic Journal ISSN 86-6655 Volume 2, 26 Paper 5 Receive: May 3, 25, Revise: Sep, 26, Accepte: Oct 6, 26 Eitor: C.E. Wayne A Nonlinear Heat Equation with Temperature-Depenent

More information

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University

More information

Approximate reduction of dynamic systems

Approximate reduction of dynamic systems Systems & Control Letters 57 2008 538 545 www.elsevier.com/locate/sysconle Approximate reuction of ynamic systems Paulo Tabuaa a,, Aaron D. Ames b, Agung Julius c, George J. Pappas c a Department of Electrical

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

Chapter 6: Energy-Momentum Tensors

Chapter 6: Energy-Momentum Tensors 49 Chapter 6: Energy-Momentum Tensors This chapter outlines the general theory of energy an momentum conservation in terms of energy-momentum tensors, then applies these ieas to the case of Bohm's moel.

More information

Acute sets in Euclidean spaces

Acute sets in Euclidean spaces Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y Ph195a lecture notes, 1/3/01 Density operators for spin- 1 ensembles So far in our iscussion of spin- 1 systems, we have restricte our attention to the case of pure states an Hamiltonian evolution. Toay

More information

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS MARK SCHACHNER Abstract. When consiere as an algebraic space, the set of arithmetic functions equippe with the operations of pointwise aition an

More information

Adaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements

Adaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements Aaptive Gain-Scheule H Control of Linear Parameter-Varying Systems with ime-delaye Elements Yoshihiko Miyasato he Institute of Statistical Mathematics 4-6-7 Minami-Azabu, Minato-ku, okyo 6-8569, Japan

More information

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7. Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency

More information

Monotonicity for excited random walk in high dimensions

Monotonicity for excited random walk in high dimensions Monotonicity for excite ranom walk in high imensions Remco van er Hofsta Mark Holmes March, 2009 Abstract We prove that the rift θ, β) for excite ranom walk in imension is monotone in the excitement parameter

More information

The Press-Schechter mass function

The Press-Schechter mass function The Press-Schechter mass function To state the obvious: It is important to relate our theories to what we can observe. We have looke at linear perturbation theory, an we have consiere a simple moel for

More information

Existence of equilibria in articulated bearings in presence of cavity

Existence of equilibria in articulated bearings in presence of cavity J. Math. Anal. Appl. 335 2007) 841 859 www.elsevier.com/locate/jmaa Existence of equilibria in articulate bearings in presence of cavity G. Buscaglia a, I. Ciuperca b, I. Hafii c,m.jai c, a Centro Atómico

More information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching Time Optimization in Discretized Hybrid Dynamical Systems Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set

More information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

Tractability results for weighted Banach spaces of smooth functions

Tractability results for weighted Banach spaces of smooth functions Tractability results for weighte Banach spaces of smooth functions Markus Weimar Mathematisches Institut, Universität Jena Ernst-Abbe-Platz 2, 07740 Jena, Germany email: markus.weimar@uni-jena.e March

More information

Sensors & Transducers 2015 by IFSA Publishing, S. L.

Sensors & Transducers 2015 by IFSA Publishing, S. L. Sensors & Transucers, Vol. 184, Issue 1, January 15, pp. 53-59 Sensors & Transucers 15 by IFSA Publishing, S. L. http://www.sensorsportal.com Non-invasive an Locally Resolve Measurement of Soun Velocity

More information

arxiv: v1 [cond-mat.stat-mech] 9 Jan 2012

arxiv: v1 [cond-mat.stat-mech] 9 Jan 2012 arxiv:1201.1836v1 [con-mat.stat-mech] 9 Jan 2012 Externally riven one-imensional Ising moel Amir Aghamohammai a 1, Cina Aghamohammai b 2, & Mohamma Khorrami a 3 a Department of Physics, Alzahra University,

More information

Equilibrium in Queues Under Unknown Service Times and Service Value

Equilibrium in Queues Under Unknown Service Times and Service Value University of Pennsylvania ScholarlyCommons Finance Papers Wharton Faculty Research 1-2014 Equilibrium in Queues Uner Unknown Service Times an Service Value Laurens Debo Senthil K. Veeraraghavan University

More information

GLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS

GLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS Electronic Journal of Differential Equations, Vol. 015 015), No. 99, pp. 1 14. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu GLOBAL SOLUTIONS FOR D COUPLED

More information

A note on the Mooney-Rivlin material model

A note on the Mooney-Rivlin material model A note on the Mooney-Rivlin material moel I-Shih Liu Instituto e Matemática Universiae Feeral o Rio e Janeiro 2945-97, Rio e Janeiro, Brasil Abstract In finite elasticity, the Mooney-Rivlin material moel

More information

Proof of SPNs as Mixture of Trees

Proof of SPNs as Mixture of Trees A Proof of SPNs as Mixture of Trees Theorem 1. If T is an inuce SPN from a complete an ecomposable SPN S, then T is a tree that is complete an ecomposable. Proof. Argue by contraiction that T is not a

More information

arxiv:hep-th/ v1 3 Feb 1993

arxiv:hep-th/ v1 3 Feb 1993 NBI-HE-9-89 PAR LPTHE 9-49 FTUAM 9-44 November 99 Matrix moel calculations beyon the spherical limit arxiv:hep-th/93004v 3 Feb 993 J. Ambjørn The Niels Bohr Institute Blegamsvej 7, DK-00 Copenhagen Ø,

More information

arxiv: v5 [cs.lg] 28 Mar 2017

arxiv: v5 [cs.lg] 28 Mar 2017 Equilibrium Propagation: Briging the Gap Between Energy-Base Moels an Backpropagation Benjamin Scellier an Yoshua Bengio * Université e Montréal, Montreal Institute for Learning Algorithms March 3, 217

More information

Level Construction of Decision Trees in a Partition-based Framework for Classification

Level Construction of Decision Trees in a Partition-based Framework for Classification Level Construction of Decision Trees in a Partition-base Framework for Classification Y.Y. Yao, Y. Zhao an J.T. Yao Department of Computer Science, University of Regina Regina, Saskatchewan, Canaa S4S

More information

Influence of weight initialization on multilayer perceptron performance

Influence of weight initialization on multilayer perceptron performance Influence of weight initialization on multilayer perceptron performance M. Karouia (1,2) T. Denœux (1) R. Lengellé (1) (1) Université e Compiègne U.R.A. CNRS 817 Heuiasyc BP 649 - F-66 Compiègne ceex -

More information

Energy behaviour of the Boris method for charged-particle dynamics

Energy behaviour of the Boris method for charged-particle dynamics Version of 25 April 218 Energy behaviour of the Boris metho for charge-particle ynamics Ernst Hairer 1, Christian Lubich 2 Abstract The Boris algorithm is a wiely use numerical integrator for the motion

More information

Attribute Reduction and Information Granularity *

Attribute Reduction and Information Granularity * ttribute Reuction an nformation Granularity * Li-hong Wang School of Computer Engineering an Science, Shanghai University, Shanghai, 200072, P.R.C School of Computer Science an Technology, Yantai University,

More information

Variational principle for limit cycles of the Rayleigh van der Pol equation

Variational principle for limit cycles of the Rayleigh van der Pol equation PHYICAL REVIEW E VOLUME 59, NUMBER 5 MAY 999 Variational principle for limit cycles of the Rayleigh van er Pol equation R. D. Benguria an M. C. Depassier Faculta e Física, Pontificia Universia Católica

More information

A study on ant colony systems with fuzzy pheromone dispersion

A study on ant colony systems with fuzzy pheromone dispersion A stuy on ant colony systems with fuzzy pheromone ispersion Louis Gacogne LIP6 104, Av. Kenney, 75016 Paris, France gacogne@lip6.fr Sanra Sanri IIIA/CSIC Campus UAB, 08193 Bellaterra, Spain sanri@iiia.csic.es

More information

Markov Chains in Continuous Time

Markov Chains in Continuous Time Chapter 23 Markov Chains in Continuous Time Previously we looke at Markov chains, where the transitions betweenstatesoccurreatspecifietime- steps. That it, we mae time (a continuous variable) avance in

More information

On a limit theorem for non-stationary branching processes.

On a limit theorem for non-stationary branching processes. On a limit theorem for non-stationary branching processes. TETSUYA HATTORI an HIROSHI WATANABE 0. Introuction. The purpose of this paper is to give a limit theorem for a certain class of iscrete-time multi-type

More information

Strength Analysis of CFRP Composite Material Considering Multiple Fracture Modes

Strength Analysis of CFRP Composite Material Considering Multiple Fracture Modes 5--XXXX Strength Analysis of CFRP Composite Material Consiering Multiple Fracture Moes Author, co-author (Do NOT enter this information. It will be pulle from participant tab in MyTechZone) Affiliation

More information

Periods of quadratic twists of elliptic curves

Periods of quadratic twists of elliptic curves Perios of quaratic twists of elliptic curves Vivek Pal with an appenix by Amo Agashe Abstract In this paper we prove a relation between the perio of an elliptic curve an the perio of its real an imaginary

More information

PHYS 414 Problem Set 2: Turtles all the way down

PHYS 414 Problem Set 2: Turtles all the way down PHYS 414 Problem Set 2: Turtles all the way own This problem set explores the common structure of ynamical theories in statistical physics as you pass from one length an time scale to another. Brownian

More information

State-Space Model for a Multi-Machine System

State-Space Model for a Multi-Machine System State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal

More information

Lower bounds on Locality Sensitive Hashing

Lower bounds on Locality Sensitive Hashing Lower bouns on Locality Sensitive Hashing Rajeev Motwani Assaf Naor Rina Panigrahy Abstract Given a metric space (X, X ), c 1, r > 0, an p, q [0, 1], a istribution over mappings H : X N is calle a (r,

More information

Improving Estimation Accuracy in Nonrandomized Response Questioning Methods by Multiple Answers

Improving Estimation Accuracy in Nonrandomized Response Questioning Methods by Multiple Answers International Journal of Statistics an Probability; Vol 6, No 5; September 207 ISSN 927-7032 E-ISSN 927-7040 Publishe by Canaian Center of Science an Eucation Improving Estimation Accuracy in Nonranomize

More information

Gravitation as the result of the reintegration of migrated electrons and positrons to their atomic nuclei. Osvaldo Domann

Gravitation as the result of the reintegration of migrated electrons and positrons to their atomic nuclei. Osvaldo Domann Gravitation as the result of the reintegration of migrate electrons an positrons to their atomic nuclei. Osvalo Domann oomann@yahoo.com (This paper is an extract of [6] liste in section Bibliography.)

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

The canonical controllers and regular interconnection

The canonical controllers and regular interconnection Systems & Control Letters ( www.elsevier.com/locate/sysconle The canonical controllers an regular interconnection A.A. Julius a,, J.C. Willems b, M.N. Belur c, H.L. Trentelman a Department of Applie Mathematics,

More information

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Course Project for CDS 05 - Geometric Mechanics John M. Carson III California Institute of Technology June

More information

Multi-component bi-hamiltonian Dirac integrable equations

Multi-component bi-hamiltonian Dirac integrable equations Chaos, Solitons an Fractals 9 (009) 8 8 www.elsevier.com/locate/chaos Multi-component bi-hamiltonian Dirac integrable equations Wen-Xiu Ma * Department of Mathematics an Statistics, University of South

More information

Chapter 2 Derivatives

Chapter 2 Derivatives Chapter Derivatives Section. An Intuitive Introuction to Derivatives Consier a function: Slope function: Derivative, f ' For each, the slope of f is the height of f ' Where f has a horizontal tangent line,

More information

G4003 Advanced Mechanics 1. We already saw that if q is a cyclic variable, the associated conjugate momentum is conserved, L = const.

G4003 Advanced Mechanics 1. We already saw that if q is a cyclic variable, the associated conjugate momentum is conserved, L = const. G4003 Avance Mechanics 1 The Noether theorem We alreay saw that if q is a cyclic variable, the associate conjugate momentum is conserve, q = 0 p q = const. (1) This is the simplest incarnation of Noether

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

Separation of Variables

Separation of Variables Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical

More information

Witt#5: Around the integrality criterion 9.93 [version 1.1 (21 April 2013), not completed, not proofread]

Witt#5: Around the integrality criterion 9.93 [version 1.1 (21 April 2013), not completed, not proofread] Witt vectors. Part 1 Michiel Hazewinkel Sienotes by Darij Grinberg Witt#5: Aroun the integrality criterion 9.93 [version 1.1 21 April 2013, not complete, not proofrea In [1, section 9.93, Hazewinkel states

More information