A High-Rate MSR Code With Polynomial Sub-Packetization Level

Size: px
Start display at page:

Download "A High-Rate MSR Code With Polynomial Sub-Packetization Level"

Transcription

1 A High-Rae MSR Code Wih Polynomial Sub-Packeizaion Level Birenjih Sasidharan, Gaurav Kumar Agarwal, and P Vijay Kumar Deparmen of Elecrical Communicaion Engineering, Indian Insiue of Science, Bangalore biren, agarwal, vijay@eceiiscernein arxiv: v1 [csit] 27 Jan 2015 Absrac We presen a high-rae (n,k,d = n 1)-MSR code wih a sub-packeizaion level ha is polynomial in he dimension k of he code While polynomial sub-packeizaion level was achieved earlier for vecor MDS codes ha repair sysemaic nodes opimally, no such MSR code consrucion is known In he low-rae regime (i e, raes less han one-half), MSR code consrucions wih a linear sub-packeizaion level are available Bu in he high-rae regime (i e, raes greaer han one-half), he known MSR code consrucions required a sub-packeizaion level ha is exponenial in k In he presen paper, we consruc an MSR code for d = n 1 wih a fixed rae R = 1, 2, achieveing a sub-packeizaion level α = O(k ) The code allows help-by-ransfer repair, i e, no compuaions are needed a he helper nodes during repair of a failed node Index Terms Disribued sorage, regeneraing codes, subpackeizaion, msr I INTRODUCTION In a disribued sorage sysem, he daa file comprising of B daa symbols drawn from a finie field F q, is encoded using an error-correcing code of block lengh n and he code symbols are sored in n nodes of he sorage nework A naive sraegy aimed a achieving resilience agains node failures is o sore muliple replicas of he same daa Given he massive amoun of daa being sored, sophisicaed codes such as Reed- Solomon (RS) codes wih low sorage overhead are being employed in pracice However, he amoun of daa download required o repair a single node-failure is quie large for he RS codes The framework of regeneraing codes was inroduced in [1] o address his problem In an (n, k, d)-regeneraing code, a file comprised of B symbols from a finie field F q is encoded ino a se of nα coded symbols and hen sored across n nodes in he nework wih each node soring α coded symbols The parameer α is ermed as he sub-packeizaion level of he code A daa collecor can download he daa by connecing o any k nodes In he even of node failure, node repair is accomplished by having he replacemen node connec o any d nodes and download β α symbols from each node wih α dβ < B The quaniy dβ is ermed he repair bandwidh Here one makes a disincion beween funcional and exac repair By funcional repair (FR), i is mean ha a failed node will be replaced by a new node This research is suppored in par by he Naional Science Foundaion under Gran No and in par by he join UGC-ISF Research Gran No 1676/14 Birenjih Sasidharan would like o acknowledge he suppor of TCS Research Scholar Programme Fellowship such ha he resuling nework coninues o saisfy he daa collecion and node-repair properies defining a regeneraing code An alernaive o funcion repair is exac repair (ER) under which one demands ha he replacemen node sore precisely he same conen as he failed node A cu-se bound based on nework-coding conceps, ells us ha given a code parameer se (n,k,d), he maximum possible size of a daa file under FR, is upper bounded [1] by k B min{α,(d l+1)β} (1) l=1 The above bound is igh since he exisence of codes achieving his bound has been esablished using nework-coding argumens relaed o mulicasing For fixed values of (n,k,d,b), he bound in (1) characerizes a radeoff beween α and β, referred o as he Sorage-Repair Bandwidh radeoff The wo exremal poins in he radeoff are respecively, he minimumsorage regeneraing (MSR) and minimum bandwidh regeneraing (MBR) poins which correspond o he poins a which he sorage and repair bandwidh are respecively minimized A MBR poin, we have ( ) k α = dβ, B = kα β, (2) 2 and a MSR poin, we have α = (d k +1)β, B = kα (3) I is proved ha MSR and MBR poins are achievable by ER codes as well The focus of he curren paper is on ER MSR codes and for convenience we simply refer o hem as MSR codes A MSR Codes The MSR codes can be considered as codes over a vecor alphabef q α wih dimensionk Since hey olerae any(n k) node-erasures, and hey have a file size ofb = kα, MSR codes are Maximum-Disance-Separable (MDS) codes over he vecor alphabe F q α The combinaion of hese wo properies is herefore called he MDS propery of MSR codes On he oher hand, MSR codes in addiion o being vecor MDS codes can repair a failed node wih he leas possible repair bandwidh The consrucion of MSR codes is a well-sudied problem in lieraure In [2], a framework o consruc MSR codes is provided for d 2k 2 In [3], high-rae MSR codes wih

2 parameers (n,k = n 2,d = n 1) are consruced using Hadamard designs In [4], high-rae MSR codes, known as zigzag codes, are consruced for d = n 1; here efficien node-repair is guaraneed only in he case of sysemaic nodes This was subsequenly exended o include he repair of pariy nodes as well in [5] A consrucion for MSR codes wih d = n 1 2k 1 using echniques of inerference alignmen is presened in [6] and [7] In [8], auhors showed he exisence of MSR codes for any value of (n,k,d) B Our Approach On Sub-packeizaion and Conribuions A parameer of ineres for MSR codes is he amoun of sub-packeizaion (α) required for a given value of (n, k, d) The MSR consrucions known as zigzag codes ha allow arbirarily high raes required a sub-packeizaion level ha is exponenial in k Laer in [9], a vecor MDS codes ha repair sysemaic nodes was consruced achieving α = r k r+1 where r := n k Recenly in [10], anoher vecor MDS code ha repairs sysemaic nodes opimally was proposed saisfying an addiional propery known as access-opimaliy The consrucion required α = r k r In [11], auhors derived a lower bound on he sub-packeizaion in erms of k, and r as given below: 2log 2 α(log ( r α+1)+1 k r 1) Earlier in [12], auhors consruced a vecor MDS code wih rae R = 2 3, requiring an α ha is polynomial in k They could also achieve polynomial α for any fixed rae in he regime 2 3 R 1 However, hese codes were also limied by he fac ha opimal repair was feasible for sysemaic codes alone Quie similar o he approach in [12], we also resric our focus o he family of MSR codes wih a fixed rae R = 1, 2 I is worhwhile o remark a his poin ha he family of Produc-Marix MSR codes [2] wih rae resriced by R 1 2 required only a linear sub-packeizaion level In he presen paper, we consruc a (n,k,d = n 1)-MSR code wih a fixed rae R = 1 where 2 is an ineger parameer The code will have α = ( k ) To he bes of our knowledge, hese are he firs MSR consrucions ha achieve a sub-packeizaion level ha is polynomial in k These codes are help-by-ransfer codes, by which we mean ha he helper nodes need no do any compuaion during he repair of a failed node II MSR CODE CONSTRUCTION FOR RATE= 1 In his secion, we provide he consrucion for MSR codes wih a rae, R = 1 for some posiive ineger The consrucion is described for a paricular example of = 3, and subsequenly generalized A Code Consrucion for R = 2 3 We have an auxiliary parameer q = p m for some prime p, and m a posiive ineger 1 Then he code has parameers n = 3q, k = 2q, d = (n 1), α = q 3 1 The auxiliary parameer akes values from a finie-field, hough i is sufficien o work wih a finie-ring This does no cause any lack of generaliy in he principles used for he consrucion A codeword of an MSR code can be reaed as an array of size (α n) We firs inroduce an indexing for he rows and columns (nodes and columns are ofen used inerchangeably) of he codeword array Le F q = {0,1,,q 1} denoe a finie field of size q, and a 2-uple (i,θ),i {1,2,3}, θ F q is used o index he columns The rows are indexed by elemens (x,y,z) from F 3 q where x,y,z F q Thus C(x,y,z;(i,θ)) represens one code symbol from he codeword array a he inersecion of he row (x,y,z) and he node (i,θ) In order o describe he code, we firs inroduce he following noaion n a 1 a 2 a n := c i a i, c i 0, i [n] (4) i=1 o denoe a linear combinaion involving each of he scalars in {a 1,a 2,,a n } wih non-zero coefficiens The noaion is oblivious o he paricular choice of non-zero coefficiens in he linear combinaion The code is described by q 4 pariycheck consrains Throughou his paper, he symbol is used wih a differen meaning The erms wihin a are no conneced by he binary operaor +, bu by he operaor as defined in (4) For every (x,y,z) F 3 q, C(x,y,z;(1,θ)) C(x,y,z;(2,θ)) C(x,y,z;(3,θ)) = 0, (5) C(x,y,z;(1,x)) C(x,y,z;(2,y)) C(x,y,z ;(3,z)) C(x,y,z;(1,θ)) C(x,y,z;(2,θ)) C(x,y,z;(3,θ)) = 0, F q (6) The pariy-check consrain in (5) is referred o as he rowpariy, and he ha in (6) is referred o as he -pariy I can be observed ha he firs hree erms in he -pariy equaions are enries ha do no belong o he(x, y, z)-row These enries are referred o as he shifed enries Wha remains is he idenificaion of coefficiens in hese pariy-check consrains so ha he MDS propery holds Insead of consrucing hese coefficiens explicily, we will show in Sec II-A2 ha such coefficiens indeed exis in a sufficienly large field Therefore, he descripion of he code is complee wih (5), (6) In he zigzag code [4], pariy symbols are caegorized ino wo ypes, namely row-pariies and zigzag pariies The row pariies are made up of message symbols from he same row of he codeword array Bu he zigzag pariies are made up of message symbols belonging o various rows such ha one message symbol is picked per column In our consrucion also, every pariy-check consrain corresponding o 0 involves shifed enries ha do no belong o he row under consideraion In his manner, our consrucion is of a similar flavor as ha in [4] Bu he major difference of our consrucion from he zigzag consrucion lies in he symmery

3 of he pariy-check consrains I also differs in he fac ha wo symbols of he same column can be involved in he same pariy-check consrain in he case of 0 Such an approach was earlier adoped in [10] 1) Opimal Repair of a Failed Node : Wihou loss of generaliy, assume ha he node (1,θ 0 ) failed We download symbols belonging he rows Γ = {(θ 0,y,z) y,z F q } Clearly Γ = q 2 Thus we have {C(θ 0,y,z;(i,θ)) i = 1,2,3,θ θ 0,y,z F q } The rows are seleced such ha x = θ 0, because he firs coordinae of he index of he node is 1 If he firs coordinae had been 2 or 3, we would have fixed y = θ 0 or z = θ 0 respecively All he code symbols C(θ 0,y,z;(1,θ 0 )), y,z F q are repaired using he row-pariies Hence we have all he symbols belonging o rows in Γ from all he n nodes Nex, le us wrie he equaion for -pariy, F q corresponding o an arbirary row (θ 0,y,z) H C(θ 0,y,z;(1,θ 0 )) C(θ 0,y,z;(2,y)) C(θ 0,y,z ;(3,z)) C(θ 0,y,z;(1,θ)) C(θ 0,y,z;(2,θ)) C(θ 0,y,z;(3,θ)) = 0 (7) Excep he erm C(θ 0,y,z;(1,θ 0 )), all oher symbols involved in (7) are known o us Thus C(θ 0,y,z;(1,θ 0 )) can be repaired for all choices of y,z By making use of all he -pariies, we can hus repair all he remaining symbols in he node (1,θ 0 ) The oal number of symbols downloaded per node is β = q 2 = q3 q = α d k +1, and hus he repair is bandwidh-opimal 2) The MDS Propery: In his secion, we will show ha we can find an assignmen of coefficiens o he row-pariies and -pariies such ha he code saisfies he MDS propery We sar wih saing a useful fac Lemma 21: Le H be a ((n k) n)-pariy-check marix of a linear code C If S [n], S = (n k) is such ha rank(h S ) = (n k), hen i is possible o decode every codeword of C accessing symbols belonging o locaionss c = [n]\s Based on he pariy-consrains in (5), (6), we will deermine he srucure of he pariy-check marix H Firs, we vecorize he codeword array node-by-node so ha he firs α = q 3 columns of H represen he firs node, he second q 3 columns represen he second node and so on The group of q 3 columns associaed wih a node is referred o as a hick column The pariy-check marix hus obained will be of size (q 4 3q 4 ) wih n hick columns each conainingαhin columns In order o describe he suppor and hereby he srucure of H, we will for a momen assume ha all he coefficiens are se o 1 This marix is denoed by H s, and is given by H s = J +E, where he marices J and E are given in (8) and (9) The equaion (8) also illusraes he fac ha he rows of J can be decomposed ino blocks of size q 3, each corresponding o pariy-check consrains wih a fixed The firs se of q 3 pariy-check consrains correspond o row-pariies possibly associaed wih = 0 In (8), (9), I q 3,0 q 3 respecively represen ideniy and allzero marix of size q 3 q 3 The marices {E i δ,θ i {1,2,3},δ F q,θ F q } are made up of 1s and zeros, and represen he shifed enries of he corresponding -pariies The marices J,E and hence H are block marices of size (q 3q) where each block is a square marix of size q 3 We will show ha he MDS propery can be ensured by assigning suiable coefficiens o locaions idenified by he suppor of H s Our mehod is quie similar o he mehod used in [10] By 21, i is sufficien ha H resriced o any (n k) = q hick columns has a rank equal o qα = q 4 Le us assign an indeerminae c o all he locaions deermined by he suppor of E Now consider he square submarix H D obained by resricing H o D [n], D = (n k) hick columns If we assume ha all he coefficiens of J are fixed, he deerminan of H D will be a polynomial in he indeerminae c Le us denoe his polynomial by p D (c) In he following lemma, we prove ha p D (c) can be made a non-zero polynomial for every choice of D [n], D = n k Lemma 22: There exiss an assignmen of coefficiens o J such ha p D (c) is a non-zero polynomial for every choice of D [n], D = n k Proof: Consider a [3q, 2q]-RS code and is pariy-check marix H mds of size (q 3q) Clearly a (q q)-marix obained by resricing H mds o any q columns has full rank Le A B denoe he Kronecker produc of marices A and B If we se J o J 0, J 0 = H mds I q 3, (10) hen we mus have p D (0) evaluaing o a non-zero value for every choice of D [n], D = n k Hence p D (c) mus be a non-zero polynomial for every valid choice of D Henceforh, we assume ha he coefficiens of he polynomials p D (c) are fixed by he coefficiens of J as deermined by Lemma 22 By he srucure of E, i is clear ha Nex, consider he polynomial p(c) = deg(p D (c)) q 4 q 3 (11) D [n], D =k p D (c) (12) Clearly p(c) is no idenically zero, and is degree is upper bounded by ( n k) q 3 (q 1) Hence i is sufficien ha we find an non-zero assignmen c 0 0 for c such ha p(c 0 ) 0 By Combinaorial Nullsellansaz [13], his is possible if we choose he field size greaer han ( n k) q 3 (q 1)+1 Thus we have proved he following heorem Theorem 23: There exiss an assignmen for he coefficiens in he pariy-check consrains in (5), (6) such ha he code described in II-A is an MSR code

4 E = J = = 0 = 1 = q 1 0 q 3 0 q 3 0 q 3 0 q 3 0 q 3 0 q 3 E1,1 1 E1,q 1 E1,1 2 E1,q 2 E1,1 3 E1,q 3 (8) (9) E 1 q 1,1 E 1 q 1,q E 2 q 1,1 E 2 q 1,q E 3 q 1,1 E 3 q 1,q Using he consan c 0 guaraneed in he proof of Thm 23, and J 0 in (10), he pariy-check marix H of he MSR code akes he form H = J 0 +c 0 E (13) B Code Consrucion for R = 1, 2 The principle of he consrucion is elucidaed in he las secion compleely, and he generalizaion o he case of rae R = 1, 2 is sraighforward For an auxiliary parameer q = p m for some prime p, and m a posiive ineger, he code consrucion has parameers n = q, k = ( 1)q, d = (n 1), α = q A 2-uple (i,θ),i {1,2,,}, θ F q is used o index he columns The rows are indexed by elemens (x 1,x 2,,x ) from F q where x j F q Thus C(x 1,x 2,,x ;(i,θ)) represens one code symbol from he codeword array a he inersecion of he row (x 1,x 2,,x ) and he node (i,θ) The code is described by q +1 pariy-check consrains For every x = (x 1,x 2,,x ) F q, C(x;(1,θ)) C(x;(2,θ)) C(x;(2,θ)) C(x;(,θ)) = 0, F q (15) The pariy-check consrain in (14) is referred o as he rowpariy, and he ha in (15) is referred o as he -pariy As in he special case of = 3 described in Sec II-A, he firs erms in he -pariy equaions are enries ha do no belong o he (x 1,x 2,,x )-row These enries are referred o as he shifed enries Exisence of coefficiens for pariy-check equaions ha ensure MDS propery follows in he same line as ha in Sec II-A2 Wha remains is o presen a repair sraegy ha is bandwidh-opimal 1) Opimal Repair of a Failed Node : Assume ha he node(i 0,θ 0 ) failed We download symbols belonging he rows Γ = {x x j F q, j i 0, x i0 = θ 0 } Clearly Γ = q 1 Thus we have {C(x;(i,θ)) (i,θ) (i 0,θ 0 ),x Γ} All he code symbols C(x;(i 0,θ 0 )), x Γ are repaired using he row-pariies Then we have all he symbols belonging o rows in Γ from all he n nodes Nex, le us wrie he equaion for -pariy, F q corresponding o an arbirary row x Γ C(x 1,x 2,,x ;(1,x 1 )) C(x 1,,x i0,,x ;(i 0,θ 0 )) C(x 1,x 2,,x ;(,x )) C(x;(j,θ)) = 0,j [] (16) Excep he erm C(x 1,,x i0,,x ;(i 0,θ 0 )), all oher symbols involved in (16) are known o us By varying, we can hus repair all he remaining symbols in he node (i 0,θ 0 ) C(x;(,θ)) = 0, (14) The oal number of symbols downloaded per node is β = q 1 = q α = C(x 1,x 2,,x ;(1,x 1 )) C(x 1,x 2,,x ;(2,x 2 )) q d k +1, C(x 1,x 2,,x ;(,x )) and hus he repair is bandwidh-opimal C(x;(1,θ)) REFERENCES [1] A Dimakis, P Godfrey, Y Wu, M Wainwrigh, and K Ramchandran, Nework coding for disribued sorage sysems, IEEE Trans Inf Theory, vol 56, no 9, pp , Sep 2010 [2] K V Rashmi, N B Shah, and P V Kumar, Opimal Exac- Regeneraing Codes for Disribued Sorage a he MSR and MBR Poins via a Produc-Marix Consrucion, IEEE Trans Inf Theory, vol 57, no 8, pp , Aug 2011 [3] D Papailiopoulos, A Dimakis, and V Cadambe, Repair Opimal Erasure Codes hrough Hadamard Designs, IEEE Trans Inf Theory, vol 59, no 5, pp , 2013 [4] I Tamo, Z Wang, and J Bruck, Zigzag codes: MDS array codes wih opimal rebuilding, IEEE Trans Inform Theory, vol 59, no 3, pp , 2013

5 [5] Wang, Z and Tamo, I and Bruck, J, On Codes for Opimal Rebuilding Access, in Proc IEEE 47h Annual Alleron Conference on Communicaion, Conrol, and Compuing, 2009, pp [6] C Suh and K Ramchandran, Exac-repair MDS code consrucion using inerference alignmen, IEEE Trans Inf Theory, vol 57, no 3, pp , 2011 [7] N B Shah, K V Rashmi, P V Kumar, and K Ramchandran, Inerference Alignmen in Regeneraing Codes for Disribued Sorage: Necessiy and Code Consrucions, IEEE Trans Inf Theory, vol 58, no 4, pp , Apr 2012 [8] V Cadambe, S A Jafar, H Maleki, K Ramchandran, and C Suh, Asympoic inerference alignmen for opimal repair of mds codes in disribued sorage, IEEE Trans Inf Theory, vol 59, no 5, pp , 2013 [9] Z Wang, I Tamo, and J Bruck, Long MDS codes for opimal repair bandwidh, in Proc IEEE Inernaional Symposium on Informaion Theory, ISIT, 2012, pp [10] G K Agarwal, B Sasidharan, and P V Kumar, An alernae consrucion of an access-opimal regeneraing code wih opimal subpackeizaion level, in Naional Conference on Communicaion (NCC), 2015 [11] S Goparaju, I Tamo, and A R Calderbank, An improved subpackeizaion bound for minimum sorage regeneraing codes, IEEE Trans on Inf Theory, vol 60, no 5, pp , 2014 [12] V R Cadambe, C Huang, J Li, and S Mehrora, Polynomial lengh MDS codes wih opimal repair in disribued sorage, in Conference Record of he Fory Fifh Asilomar Conference on Signals, Sysems and Compuers ACSCC 2011, pp [13] N Alon, Combinaorial Nullsellensaz, Combinaorics, Probabiliy and Compuing, 1999

Progress on High-rate MSR Codes: Enabling Arbitrary Number of Helper Nodes

Progress on High-rate MSR Codes: Enabling Arbitrary Number of Helper Nodes Progress on High-rate MSR Codes: Enabling Arbitrary Number of Helper Nodes Ankit Singh Rawat CS Department Carnegie Mellon University Pittsburgh, PA 523 Email: asrawat@andrewcmuedu O Ozan Koyluoglu Department

More information

Staircase Codes for Secret Sharing with Optimal Communication and Read Overheads

Staircase Codes for Secret Sharing with Optimal Communication and Read Overheads Saircase Codes for Secre Sharing wih Opimal Communicaion and Read Overheads Rawad Biar, Salim El Rouayheb ECE Deparmen, IIT, Chicago rbiar@hawkiiedu, salim@iiedu Absrac We sudy he communicaion efficien

More information

Some Ramsey results for the n-cube

Some Ramsey results for the n-cube Some Ramsey resuls for he n-cube Ron Graham Universiy of California, San Diego Jozsef Solymosi Universiy of Briish Columbia, Vancouver, Canada Absrac In his noe we esablish a Ramsey-ype resul for cerain

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

We just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n

We just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n Lecure 3 - Kövari-Sós-Turán Theorem Jacques Versraëe jacques@ucsd.edu We jus finished he Erdős-Sone Theorem, and ex(n, F ) ( /(χ(f ) )) ( n 2). So we have asympoics when χ(f ) 3 bu no when χ(f ) = 2 i.e.

More information

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal

More information

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN Inernaional Journal of Scienific & Engineering Research, Volume 4, Issue 10, Ocober-2013 900 FUZZY MEAN RESIDUAL LIFE ORDERING OF FUZZY RANDOM VARIABLES J. EARNEST LAZARUS PIRIYAKUMAR 1, A. YAMUNA 2 1.

More information

5. Stochastic processes (1)

5. Stochastic processes (1) Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly

More information

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004 ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform

More information

ERROR LOCATING CODES AND EXTENDED HAMMING CODE. Pankaj Kumar Das. 1. Introduction and preliminaries

ERROR LOCATING CODES AND EXTENDED HAMMING CODE. Pankaj Kumar Das. 1. Introduction and preliminaries MATEMATIČKI VESNIK MATEMATIQKI VESNIK 70, 1 (2018), 89 94 March 2018 research paper originalni nauqni rad ERROR LOCATING CODES AND EXTENDED HAMMING CODE Pankaj Kumar Das Absrac. Error-locaing codes, firs

More information

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT Inerna J Mah & Mah Sci Vol 4, No 7 000) 48 49 S0670000970 Hindawi Publishing Corp GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT RUMEN L MISHKOV Received

More information

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning

More information

Optimal Paired Choice Block Designs. Supplementary Material

Optimal Paired Choice Block Designs. Supplementary Material Saisica Sinica: Supplemen Opimal Paired Choice Block Designs Rakhi Singh 1, Ashish Das 2 and Feng-Shun Chai 3 1 IITB-Monash Research Academy, Mumbai, India 2 Indian Insiue of Technology Bombay, Mumbai,

More information

CHAPTER 2 Signals And Spectra

CHAPTER 2 Signals And Spectra CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par

More information

Stability and Bifurcation in a Neural Network Model with Two Delays

Stability and Bifurcation in a Neural Network Model with Two Delays Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

More information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS

A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS A DELAY-DEPENDENT STABILITY CRITERIA FOR T-S FUZZY SYSTEM WITH TIME-DELAYS Xinping Guan ;1 Fenglei Li Cailian Chen Insiue of Elecrical Engineering, Yanshan Universiy, Qinhuangdao, 066004, China. Deparmen

More information

Optimality Conditions for Unconstrained Problems

Optimality Conditions for Unconstrained Problems 62 CHAPTER 6 Opimaliy Condiions for Unconsrained Problems 1 Unconsrained Opimizaion 11 Exisence Consider he problem of minimizing he funcion f : R n R where f is coninuous on all of R n : P min f(x) x

More information

Rate Regions for Coherent and Noncoherent Multisource Network Error Correction

Rate Regions for Coherent and Noncoherent Multisource Network Error Correction Rae Regions for Coheren and Noncoheren Mulisource Nework Error Correcion Svilana Vyerenko, Tracey Ho, Michelle Effros California Insiue of Technology Email: {svilana,ho,effros}@calech.edu Joerg Kliewer

More information

Robotics I. April 11, The kinematics of a 3R spatial robot is specified by the Denavit-Hartenberg parameters in Tab. 1.

Robotics I. April 11, The kinematics of a 3R spatial robot is specified by the Denavit-Hartenberg parameters in Tab. 1. Roboics I April 11, 017 Exercise 1 he kinemaics of a 3R spaial robo is specified by he Denavi-Harenberg parameers in ab 1 i α i d i a i θ i 1 π/ L 1 0 1 0 0 L 3 0 0 L 3 3 able 1: able of DH parameers of

More information

SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F. Trench. SIAM J. Matrix Anal. Appl. 11 (1990),

SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F. Trench. SIAM J. Matrix Anal. Appl. 11 (1990), SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F Trench SIAM J Marix Anal Appl 11 (1990), 601-611 Absrac Le T n = ( i j ) n i,j=1 (n 3) be a real symmeric

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

More information

Ordinary Differential Equations

Ordinary Differential Equations Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a

More information

Random Walk with Anti-Correlated Steps

Random Walk with Anti-Correlated Steps Random Walk wih Ani-Correlaed Seps John Noga Dirk Wagner 2 Absrac We conjecure he expeced value of random walks wih ani-correlaed seps o be exacly. We suppor his conjecure wih 2 plausibiliy argumens and

More information

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions Muli-Period Sochasic Models: Opimali of (s, S) Polic for -Convex Objecive Funcions Consider a seing similar o he N-sage newsvendor problem excep ha now here is a fixed re-ordering cos (> 0) for each (re-)order.

More information

Chapter 6. Systems of First Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh

More information

Error Correction and Partial Information Rewriting for Flash Memories

Error Correction and Partial Information Rewriting for Flash Memories Error Correcion and Parial Informaion Rewriing for Flash Memories Yue Li, Anxiao (Andrew) Jiang, and Jehoshua Bruck Texas A&M Universiy, College Saion, TX 7783, USA California Insiue of Technology, Pasadena,

More information

Modal identification of structures from roving input data by means of maximum likelihood estimation of the state space model

Modal identification of structures from roving input data by means of maximum likelihood estimation of the state space model Modal idenificaion of srucures from roving inpu daa by means of maximum likelihood esimaion of he sae space model J. Cara, J. Juan, E. Alarcón Absrac The usual way o perform a forced vibraion es is o fix

More information

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature On Measuring Pro-Poor Growh 1. On Various Ways of Measuring Pro-Poor Growh: A Shor eview of he Lieraure During he pas en years or so here have been various suggesions concerning he way one should check

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A

More information

BBP-type formulas, in general bases, for arctangents of real numbers

BBP-type formulas, in general bases, for arctangents of real numbers Noes on Number Theory and Discree Mahemaics Vol. 19, 13, No. 3, 33 54 BBP-ype formulas, in general bases, for arcangens of real numbers Kunle Adegoke 1 and Olawanle Layeni 2 1 Deparmen of Physics, Obafemi

More information

The Storage vs Repair Bandwidth Trade-off for Multiple Failures in Clustered Storage Networks

The Storage vs Repair Bandwidth Trade-off for Multiple Failures in Clustered Storage Networks Daa Collecion The Sorage vs Repair Bandwidh Trade-off for Muliple Failures in Clusered Sorage Neworks Vialy Abdrashiov, N. Prakash and Muriel Médard Research Laboraory of Elecronics, MIT, USA. Email: {vi,

More information

A Primal-Dual Type Algorithm with the O(1/t) Convergence Rate for Large Scale Constrained Convex Programs

A Primal-Dual Type Algorithm with the O(1/t) Convergence Rate for Large Scale Constrained Convex Programs PROC. IEEE CONFERENCE ON DECISION AND CONTROL, 06 A Primal-Dual Type Algorihm wih he O(/) Convergence Rae for Large Scale Consrained Convex Programs Hao Yu and Michael J. Neely Absrac This paper considers

More information

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION MATH 28A, SUMME 2009, FINAL EXAM SOLUTION BENJAMIN JOHNSON () (8 poins) [Lagrange Inerpolaion] (a) (4 poins) Le f be a funcion defined a some real numbers x 0,..., x n. Give a defining equaion for he Lagrange

More information

Signal and System (Chapter 3. Continuous-Time Systems)

Signal and System (Chapter 3. Continuous-Time Systems) Signal and Sysem (Chaper 3. Coninuous-Time Sysems) Prof. Kwang-Chun Ho kwangho@hansung.ac.kr Tel: 0-760-453 Fax:0-760-4435 1 Dep. Elecronics and Informaion Eng. 1 Nodes, Branches, Loops A nework wih b

More information

Undetermined coefficients for local fractional differential equations

Undetermined coefficients for local fractional differential equations Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani

More information

Robust estimation based on the first- and third-moment restrictions of the power transformation model

Robust estimation based on the first- and third-moment restrictions of the power transformation model h Inernaional Congress on Modelling and Simulaion, Adelaide, Ausralia, 6 December 3 www.mssanz.org.au/modsim3 Robus esimaion based on he firs- and hird-momen resricions of he power ransformaion Nawaa,

More information

Macroeconomic Theory Ph.D. Qualifying Examination Fall 2005 ANSWER EACH PART IN A SEPARATE BLUE BOOK. PART ONE: ANSWER IN BOOK 1 WEIGHT 1/3

Macroeconomic Theory Ph.D. Qualifying Examination Fall 2005 ANSWER EACH PART IN A SEPARATE BLUE BOOK. PART ONE: ANSWER IN BOOK 1 WEIGHT 1/3 Macroeconomic Theory Ph.D. Qualifying Examinaion Fall 2005 Comprehensive Examinaion UCLA Dep. of Economics You have 4 hours o complee he exam. There are hree pars o he exam. Answer all pars. Each par has

More information

Let us start with a two dimensional case. We consider a vector ( x,

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

Families with no matchings of size s

Families with no matchings of size s Families wih no machings of size s Peer Franl Andrey Kupavsii Absrac Le 2, s 2 be posiive inegers. Le be an n-elemen se, n s. Subses of 2 are called families. If F ( ), hen i is called - uniform. Wha is

More information

A New Perturbative Approach in Nonlinear Singularity Analysis

A New Perturbative Approach in Nonlinear Singularity Analysis Journal of Mahemaics and Saisics 7 (: 49-54, ISSN 549-644 Science Publicaions A New Perurbaive Approach in Nonlinear Singulariy Analysis Ta-Leung Yee Deparmen of Mahemaics and Informaion Technology, The

More information

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013 IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher

More information

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-SPACE MODELLING. A mass balance across the tank gives: B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing

More information

GMM - Generalized Method of Moments

GMM - Generalized Method of Moments GMM - Generalized Mehod of Momens Conens GMM esimaion, shor inroducion 2 GMM inuiion: Maching momens 2 3 General overview of GMM esimaion. 3 3. Weighing marix...........................................

More information

Lecture Notes 2. The Hilbert Space Approach to Time Series

Lecture Notes 2. The Hilbert Space Approach to Time Series Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship

More information

12: AUTOREGRESSIVE AND MOVING AVERAGE PROCESSES IN DISCRETE TIME. Σ j =

12: AUTOREGRESSIVE AND MOVING AVERAGE PROCESSES IN DISCRETE TIME. Σ j = 1: AUTOREGRESSIVE AND MOVING AVERAGE PROCESSES IN DISCRETE TIME Moving Averages Recall ha a whie noise process is a series { } = having variance σ. The whie noise process has specral densiy f (λ) = of

More information

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems. Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial

More information

arxiv: v1 [math.gm] 4 Nov 2018

arxiv: v1 [math.gm] 4 Nov 2018 Unpredicable Soluions of Linear Differenial Equaions Mara Akhme 1,, Mehme Onur Fen 2, Madina Tleubergenova 3,4, Akylbek Zhamanshin 3,4 1 Deparmen of Mahemaics, Middle Eas Technical Universiy, 06800, Ankara,

More information

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details! MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his

More information

Final Spring 2007

Final Spring 2007 .615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o

More information

Expert Advice for Amateurs

Expert Advice for Amateurs Exper Advice for Amaeurs Ernes K. Lai Online Appendix - Exisence of Equilibria The analysis in his secion is performed under more general payoff funcions. Wihou aking an explici form, he payoffs of he

More information

Math 315: Linear Algebra Solutions to Assignment 6

Math 315: Linear Algebra Solutions to Assignment 6 Mah 35: Linear Algebra s o Assignmen 6 # Which of he following ses of vecors are bases for R 2? {2,, 3, }, {4,, 7, 8}, {,,, 3}, {3, 9, 4, 2}. Explain your answer. To generae he whole R 2, wo linearly independen

More information

Spring Ammar Abu-Hudrouss Islamic University Gaza

Spring Ammar Abu-Hudrouss Islamic University Gaza Chaper 7 Reed-Solomon Code Spring 9 Ammar Abu-Hudrouss Islamic Universiy Gaza ١ Inroducion A Reed Solomon code is a special case of a BCH code in which he lengh of he code is one less han he size of he

More information

Echocardiography Project and Finite Fourier Series

Echocardiography Project and Finite Fourier Series Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every

More information

The General Linear Test in the Ridge Regression

The General Linear Test in the Ridge Regression ommunicaions for Saisical Applicaions Mehods 2014, Vol. 21, No. 4, 297 307 DOI: hp://dx.doi.org/10.5351/sam.2014.21.4.297 Prin ISSN 2287-7843 / Online ISSN 2383-4757 The General Linear Tes in he Ridge

More information

Christos Papadimitriou & Luca Trevisan November 22, 2016

Christos Papadimitriou & Luca Trevisan November 22, 2016 U.C. Bereley CS170: Algorihms Handou LN-11-22 Chrisos Papadimiriou & Luca Trevisan November 22, 2016 Sreaming algorihms In his lecure and he nex one we sudy memory-efficien algorihms ha process a sream

More information

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance. 1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard

More information

Technical Report Doc ID: TR March-2013 (Last revision: 23-February-2016) On formulating quadratic functions in optimization models.

Technical Report Doc ID: TR March-2013 (Last revision: 23-February-2016) On formulating quadratic functions in optimization models. Technical Repor Doc ID: TR--203 06-March-203 (Las revision: 23-Februar-206) On formulaing quadraic funcions in opimizaion models. Auhor: Erling D. Andersen Convex quadraic consrains quie frequenl appear

More information

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

More information

) were both constant and we brought them from under the integral.

) were both constant and we brought them from under the integral. YIELD-PER-RECRUIT (coninued The yield-per-recrui model applies o a cohor, bu we saw in he Age Disribuions lecure ha he properies of a cohor do no apply in general o a collecion of cohors, which is wha

More information

0.1 MAXIMUM LIKELIHOOD ESTIMATION EXPLAINED

0.1 MAXIMUM LIKELIHOOD ESTIMATION EXPLAINED 0.1 MAXIMUM LIKELIHOOD ESTIMATIO EXPLAIED Maximum likelihood esimaion is a bes-fi saisical mehod for he esimaion of he values of he parameers of a sysem, based on a se of observaions of a random variable

More information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

Lie Derivatives operator vector field flow push back Lie derivative of

Lie Derivatives operator vector field flow push back Lie derivative of Lie Derivaives The Lie derivaive is a mehod of compuing he direcional derivaive of a vecor field wih respec o anoher vecor field We already know how o make sense of a direcional derivaive of real valued

More information

THE MATRIX-TREE THEOREM

THE MATRIX-TREE THEOREM THE MATRIX-TREE THEOREM 1 The Marix-Tree Theorem. The Marix-Tree Theorem is a formula for he number of spanning rees of a graph in erms of he deerminan of a cerain marix. We begin wih he necessary graph-heoreical

More information

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS Elecronic Journal of Differenial Equaions, Vol. 217 217, No. 118, pp. 1 14. ISSN: 172-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS

More information

Anonymity in Shared Symmetric Key Primitives

Anonymity in Shared Symmetric Key Primitives Anonymiy in Shared Symmeric Key Primiives Gregory M. Zaverucha and Douglas R. Sinson David R. Cherion School of Compuer Science Universiy of Waerloo Waerloo ON, N2L 3G1, Canada {gzaveruc, dsinson}@uwaerloo.ca

More information

Pade and Laguerre Approximations Applied. to the Active Queue Management Model. of Internet Protocol

Pade and Laguerre Approximations Applied. to the Active Queue Management Model. of Internet Protocol Applied Mahemaical Sciences, Vol. 7, 013, no. 16, 663-673 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/10.1988/ams.013.39499 Pade and Laguerre Approximaions Applied o he Acive Queue Managemen Model of Inerne

More information

Update Efficient Codes for Error Correction

Update Efficient Codes for Error Correction Updae Efficien Codes for Error Correcion Arya Mazumdar and Gregory W. Wornell Dep. EECS, MIT, Cambridge, MA 02139 email: {aryam, gww}@mi.edu Venka Chandar MIT Lincoln Laboraory, Lexingon, MA 02420 Email:

More information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,

More information

Logic in computer science

Logic in computer science Logic in compuer science Logic plays an imporan role in compuer science Logic is ofen called he calculus of compuer science Logic plays a similar role in compuer science o ha played by calculus in he physical

More information

Games Against Nature

Games Against Nature Advanced Course in Machine Learning Spring 2010 Games Agains Naure Handous are joinly prepared by Shie Mannor and Shai Shalev-Shwarz In he previous lecures we alked abou expers in differen seups and analyzed

More information

Sections 2.2 & 2.3 Limit of a Function and Limit Laws

Sections 2.2 & 2.3 Limit of a Function and Limit Laws Mah 80 www.imeodare.com Secions. &. Limi of a Funcion and Limi Laws In secion. we saw how is arise when we wan o find he angen o a curve or he velociy of an objec. Now we urn our aenion o is in general

More information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions

More information

Optimal Server Assignment in Multi-Server

Optimal Server Assignment in Multi-Server Opimal Server Assignmen in Muli-Server 1 Queueing Sysems wih Random Conneciviies Hassan Halabian, Suden Member, IEEE, Ioannis Lambadaris, Member, IEEE, arxiv:1112.1178v2 [mah.oc] 21 Jun 2013 Yannis Viniois,

More information

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive

More information

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance

More information

Retrieval Models. Boolean and Vector Space Retrieval Models. Common Preprocessing Steps. Boolean Model. Boolean Retrieval Model

Retrieval Models. Boolean and Vector Space Retrieval Models. Common Preprocessing Steps. Boolean Model. Boolean Retrieval Model 1 Boolean and Vecor Space Rerieval Models Many slides in his secion are adaped from Prof. Joydeep Ghosh (UT ECE) who in urn adaped hem from Prof. Dik Lee (Univ. of Science and Tech, Hong Kong) Rerieval

More information

Optimal Exact-Regenerating Codes for Distributed Storage at the MSR and MBR Points via a Product-Matrix Construction

Optimal Exact-Regenerating Codes for Distributed Storage at the MSR and MBR Points via a Product-Matrix Construction Optimal Exact-Regenerating Codes for Distributed Storage at the MSR and MBR Points via a Product-Matrix Construction K V Rashmi, Nihar B Shah, and P Vijay Kumar, Fellow, IEEE Abstract Regenerating codes

More information

On Boundedness of Q-Learning Iterates for Stochastic Shortest Path Problems

On Boundedness of Q-Learning Iterates for Stochastic Shortest Path Problems MATHEMATICS OF OPERATIONS RESEARCH Vol. 38, No. 2, May 2013, pp. 209 227 ISSN 0364-765X (prin) ISSN 1526-5471 (online) hp://dx.doi.org/10.1287/moor.1120.0562 2013 INFORMS On Boundedness of Q-Learning Ieraes

More information

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon 3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of

More information

Mathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation

Mathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation Mahcad Lecure #8 In-class Workshee Curve Fiing and Inerpolaion A he end of his lecure, you will be able o: explain he difference beween curve fiing and inerpolaion decide wheher curve fiing or inerpolaion

More information

1 Review of Zero-Sum Games

1 Review of Zero-Sum Games COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any

More information

Energy Storage Benchmark Problems

Energy Storage Benchmark Problems Energy Sorage Benchmark Problems Daniel F. Salas 1,3, Warren B. Powell 2,3 1 Deparmen of Chemical & Biological Engineering 2 Deparmen of Operaions Research & Financial Engineering 3 Princeon Laboraory

More information

Decentralized Stochastic Control with Partial History Sharing: A Common Information Approach

Decentralized Stochastic Control with Partial History Sharing: A Common Information Approach 1 Decenralized Sochasic Conrol wih Parial Hisory Sharing: A Common Informaion Approach Ashuosh Nayyar, Adiya Mahajan and Demoshenis Tenekezis arxiv:1209.1695v1 [cs.sy] 8 Sep 2012 Absrac A general model

More information