Polynomials. 1 What is a polynomial? John Stalker

Size: px
Start display at page:

Download "Polynomials. 1 What is a polynomial? John Stalker"

Transcription

1 Polynomals John Stalker What s a polynomal? If you thnk you already know what a polynomal s then skp ths secton. Just be aware that I consstently wrte thngs lke p = c z j =0 nstead of p(z) = c z. =0 You can regard ths smply as an eccentrcty, or as an abbrevaton. So you re stll readng? Well, as t turns out, you probably don t don t know what a polynomal s. If you contnue readng then you wll fnd out, possbly after beng confused brefly, but t won t make any dfference as far as ths module s concerned, so feel free to skp ahead. A polynomal s a sequence of numbers 2, ndexed by the non-negatve ntegers, only Copyrght 207 Really, a unvarate polynomal, probably more famlar to you as a polynomal n one varable. 2 What sort of numbers are allowed? Certanly ratonals, reals or complex numbers are allowed. For much of what follows, ntegers would work as well, not for everythng. If you know abstract algebra then my assumpton s smply that elements of the fntely many of whose elements are non-zero. A non-zero polynomal has a last ndex for whch the correspondng element s non-zero, and ths s called the degree of the polynomal. Polynomals of degree zero have a sngle non-zero element, the one wth ndex zero, and we dentfy them wth ths element. We defne addton of polynomals as you would expect: the k th element of p + q s the sum of the k th elements of p and q. (α 0, α, α 2,...) + (β 0, β, β 2,...) = (α 0 + β 0, α + β, α 2 + β 2,...). Multplcaton by a number s also defned as you would expect: the k th element of αp s α tmes the k th element of p. α(β 0, β, β 2,...) = (αβ 0, αβ, αβ 2,...) Multplcaton s not however defned n the way you mght expect. The k th element of pq s defned to be the sum of the products of the th element of p and the j th element of q, the sum beng taken over all pars (, ) such that + = k. There are only fntely many such pars, so there s no problem n defnng ths sum. (α 0, α, α 2,...)(β 0, β, β 2,...) = (α 0 β 0, α 0 β + α β 0, α 0 β 2 + α β + α 2 β 0,...). Later t wll be conve- sequence belong to a feld. nent to assume more.

2 Ths defnton s consstent wth our earler dentfcaton of polynomals of degree zero wth numbers and our defnton of the product of a number and a polynomal. It s not mmedately obvous that the usual commutatve, assocatve and dstrbutve laws hold for polynomals, but they do. There s a specal polynomal, whch we call z, wth zeroes for all elements except the element wth ndex, whch s a : z = (0,, 0, 0, ) Because of the way multplcaton s defned, z k has all elements zero except for the k th, whch s. We can therefore wrte (α 0, α, α 2,...) = α 0 + α z + α 2 z 2 +. The sum s, despte appearances, fnte, snce we can stop after the z d term, where d s the degree of the polynomal. From now on we wll never wrte polynomals explctly as sequences and wll nstead always wrte them as a sum of coeffcents tmes powers of z. Normally these are wrtten wth the powers lsted n descendng order. That s purely a matter of conventon, but we wll follow that conventon from now on. Why do we not defne just defne polynomals as functons of the form d =0 α z j? After all, that s the motvaton behnd our defntons of addton and multplcaton, whch were so chosen that and (p + q)(z) = p(z) + q(z) (pq)(z) = p(z)q(z) for any choce of Z for whch they make sense. There are a few reasons why defnng polynomals as functons s problematc. It s not obvous whether dfferent sequences of coeffcents can gve rse to the same functon. If the sequence α 0, α, α 2... sn t unquely determned by the functon d =0 α z j then t doesn t make sense to defne the degree to be d, the constant term to be α 0, the leadng term to be α d, etc. For real or complex polynomals t s possble to show that the sequence of coeffcents s unquely determned by the values of the correspondng functon, but ths requres work, and that work s avoded by adoptng the defnton of a polynomal as a sequence of coeffcents. Another reason to avod the functonal defnton s that we want to be flexble n our choce of Z. We want to allow not just numbers as arguments to the functon but also square matrces. More generally we may want to allow Z to be an endomorphsm of a vector space, possbly nfnte dmensonal. In general we want to mantan the opton of takng t to be anythng whch can meanngfully be added, rased to powers and multpled by numbers. If p s a functon then we are forced to choose ts doman, and f we later change ths doman we could concevable dscover that polynomal denttes proved earler wth a dfferent choce are no longer vald. Wth the sequence defnton we can be sure that any denttes proved for polynomals wll also hold for the correspondng functons, no matter what choce of doman we make. A further reason s the we want our results to apply n more exotc contexts, lke 2

3 fnte felds. That s rrelevant to our applcatons n ths module, but mportant n other areas of mathematcs, lke number theory or algebrac geometry. If our coeffcents belong to a fnte feld and the doman s the same fnte feld then t s no longer true that the functon determnes the coeffcents unquely. Then many thngs start to go wrong f we ve dentfed polynomals wth functons. It s no longer true, for example that the product of non-zero polynomals s non-zero. Z 2 + Z = (Z + )Z = 0, for example, for all Z n the feld wth two elements, even though nether Z nor Z + s dentcally zero. Ths doesn t happen f we defne polynomals as sequences. In that case z 2 + z s the sequence (0,,, 0, 0,...), whch s non-zero. 2 Matrces Computatonally t s often convenent to us matrces to perform polynomal calculatons. The central observaton whch makes ths work s essental trval. It s just that z d α z. = ( α d α α 0 ) =0 z. Polynomals of degree at most d are thus just row vectors tmes the fxed column vector z d. x = z. The coeffcents of the polynomal are the entres of the row vector. Because of the way matrx multplcaton s defned, f we multply x from the rght by a matrx A nstead of a column vector c then we get a column vector whose entres are polynomals, wth each entry havng coeffcents gven by the correspondng row of A. Dvson We can dvde polynomals n much the same way we dvde ntegers. For example, to dvde z 5 + z + z 2 + z + by z 2 z + we frst dvde the leadng terms, z 5 /z 2 = z. It follows that z tmes z 2 z + equals z 5 + x 4 + z + z 2 + z + plus terms of lower order: z 5 + z 4 + z + z 2 + z + = z (z 2 z + ) + 2z 4 + z 2 + z +. Dvdng the leadng term of 2z 4 + z 2 + z + by that of z 2 z + gves 2z 2, and 2z 4 + z 2 + z + = 2z 2 (z 2 z + ) + 2z z 2 + z +. Dvdng leadng terms agan gves 2z and 2z z 2 + z + = 2z(z 2 z + ) + z 2 z +. Dvdng one fnal tme gves and It follows that z 2 z + = (z 2 z + ). z 5 + z 4 + z + z 2 + z + = (z + 2z 2 + 2z + )(z 2 z + ).

4 In general we expect to get a remander, of course, just as we do when dvdng ntegers. Here we ddn t, because z 2 z + happens to be a factor of z 5 + z 4 + z + z 2 + z +. The remander wll always be of lower order than the dvsor. There s an alternate way to do ths calculaton, whch doesn t have an analogue for ntegers. We solve ya = c where A = and Ths gves c = ( ). y = ( ). To see why ths works, multply both sdes of the equaton ya = c from the rght by the row vector z 5 z 4 z z 2, z as descrbed n the precedng paragraph. Ths sn t really an alternate method. It s n fact a repackagng of the prevous method. The steps n dvson correspond exactly to the steps n Gaussan elmnaton. The arthmetc s the same, but we don t need to wrte the powers of z everywhere. In general we can dvde a polynomal p of degree d by a polynomal p 2 of degree d 2, wth d d 2, obtanng a quotent q of degree d d 2 and a remander r of degree less than d 2 : p = p 2 q + r. We can always perform ths dvson usng matrx algebra. We form a (d + ) (d + ) matrx A whose th row, for d d 2 + and j th column, for j d + s coeffcent of z d j+ n z d d 2 + p 2. The frst d d 2 + rows are thus shfted versons of the coeffcents of p 2, always wth the leadng coeffcent on the man dagonal. The fnal d 2 rows are the same as the correspondng rows of the dentty matrx. We form a row vector c whose entres are the coeffcents of p. The soluton to the equaton ya = c s then a row vector y whose frst d d 2 + entres are to coeffcents of the quotent q and whose last d 2 rows are the coeffcents of the remander r. Ths works because ya = c f and only f yax = cx where x s a row vector whose entres are decreasng powers of z and the equaton yax = cx s just p = p 2 q + r n matrx form. The equaton ya = c s solvable because A s upper trangular and ts dagonal entres are non-zero, so t s nvertble. For a further example, let s dvde z 4 +2z + z 2 + 4z + 4 by 6z 2 + 7z A = , c = ( ), 4

5 The soluton to ya = c s so y = ( ), 26 z 4 + 2z + z 2 + 4z + 4 ( = 6 z z + 25 ) (6z 2 + 7z + 8 ) z , as you can check drectly. 4 GCDs, Resultants, etc. Once we know how to dvde polynomals we can carry over many famlar notons from ntegers, lke least common multples and greatest common dvsors. We can fnd the greatest common dvsor by repeated dvson, just as n the case of ntegers. It follows from ths constructon that f r s the greatest common dvsor of p and q then r = sp + tq for some polynomals s and t wth the degree of s less than the degree of q and the degree of t less than the degree of p. As an example, suppose Dvdng, p = z, q = z 2 + z +. z 2 + z + = (z + 2)(z ) + Really, a greatest common dvsor, unless we normalse them, for example by choosng the leadng coeffcent to be. so we get a remander of, whch s the least common denomnator. From the calculaton t follows that = (z 2 + z + ) + ( z 2)(z ). Normally we have to dvde more than once. For example, wth we have so Then so p = z 2 + z +, q = z 2 + z 2 + z + = (z 2 + ) + z, z = (z 2 + z + ) + ( )(z 2 + ). z 2 + z + = (z + )z +, = (z 2 + z + ) + ( z )z = z(z 2 + z + ) + (z + )(z 2 + ). Polynomals whose greatest common dvsor s constant, as n the examples above, are called relatvely prme. Suppose p and q are relatvely prme and let d p and d q be ther degrees. Then ρ = up + vq. for some polynomals u and v. Suppose the degree of r s less than d p + d q then r = ru ρ p + rv ρ q 5

6 Dvde ru/ρ by q, ru ρ = wq + s where the degree of s s less than d q. Then where r = sp + tq t = rv ρ q wp. The degree of t must be less than d p because otherwse the rght hand sde of the equaton r = sp + tq would have hgher degree than the left hand sde. In ths way we see the p and q are relatvely prme f and only f the equaton r = sp + tq s solvable for s and t for any r, the degrees beng less than d q, d p and d q +d r, respectvely. The equaton r = sp + tq can be wrtten n matrx form c = ya where y s a row vector consstng of the coeffcents of s followed by those of t, c s a row vector consstng of the coeffcents of r, and A s a matrx consstng of shfted versons of p and q. More precsely, the th entry of c s the coeffcent of z dp+dq n c, the th entry of y s the coeffcent of z dq of s for d q and s the coeffcent of z dp+dq n t for d q + d p + d q, and the entry n the th row j th column of A s the coeffcent of z dp+dq j n z dq p for d q s the coeffcent of z dp+dq j d q + d p + d q. For example, the equaton n z dpdq q for = z(z 2 + z + ) + (z + )(z 2 + ) n matrx from s c = ya where and c = ( ), y = ( 0 ), 0 0 A = The precedng consderatons lead us to the concluson that p and q are relatvely prme f and only f A s nvertble. The happens f and only f the determnant of A s non-zero. Ths determnant has a name. It s called the resultant of the polynomals p and q. A partcularly mportant case s the resultant of p and p, where p and p are related by p = α z, =0 d p = ( + )α + z. =0 In ths case the resultant of p and p s known as the dscrmnant of p. If p looks famlar, n the case of real or complex polynomals ths s the dervatve of p. The defnton makes sense n general though. 4 4 There s however one werd thng whch can happen for felds of non-zero characterstc: the dervatve of a non-constant polynomal may be zero. 6

7 A polynomal wth no non-constant factors of lower degree s called rreducble. 5 If a polynomal s not rreducble then t must have a factor of lower degree. We can repeatedly dvde out such factors untl we are left wth an rreducble polynomal. The process must termnate after fntely many steps, snce the degree s reduced wth each dvson. Ths sounds smple enough, but ths procedure s, unlke absolutely everythng else n ths set of notes, not constructve. In any case, we can, at least n theory, factor any monc 6 polynomal nto a product of powers of dstnct rreducble monc factors. Ths factorsaton s unque. Both the statement and proof here mrror those for postve ntegers. 7 5 Partal Fractons Suppose p = m = p e where each p s rreducble and p and p j are relatvely prme for j,.e. ther greatest common dvsor s constant. Let d be the degree of p. Defne q,j,k = z d k p e j l l, 5 Snce the termnology for polynomals otherwse mrrors that for ntegers t would have been better to call such polynomals prme rather than rreducble. 6 Monc means wth leadng coeffcent. 7 Ths ncludes the fact that factorng, whle easy n prncple, may be hard n practce. At least we hope t s hard, so much of modern cryptography reles on the dffculty of factorng large ntegers. so that or, equvalently, z d k p = p j q,j,k q,j,k p = zd k p j for all m, j < e, k d. The degree of p s m d = d e, = whch s just the number of polynomals q,j,k. We form a d d matrx A as follows. Each row wll correspond to one of the q,j,k and each column to a power z d l of z. We order the rows by ncreasng values of, then by ncreasng values of j wth that, and by ncreasng values of k wthn that. We order the columns by ncreasng values of l, n other words by decreasng powers of z. So each row represents a polynomal and each column a power of z. The entry n that row and column s then the coeffcent of that power of z n that polynomal. Another way of sayng ths s that Ax = b, where x s the column vector consstng of decreasng powers of z, as before, and b s the column vector whose entres are the polynomals q,j,k. For example, z 4 z z + = (z ) 2 (z 2 + z + ), so the correspondng p, e, q,j,k and A are p = z, e = 2, p 2 = z 2 + z +, e 2 =, 7

8 and q,, = z, q,2, = z 2 + z +, q 2,, = z 2z 2 + z, q 2,,2 = z 2 2z +, A = Multplyng A from the rght by a column vector x = gves the column vector z z 2 z q,, q b = Ax =,2, q 2,,. q 2,,2 If we re workng over the complex numbers then we can factor any polynomal nto lnear factors. For example, ( z 4 z z + = (z ) 2 z ) ( 2 z + 2 ), 2 so p = z, e = 2, p 2 = z , e2 =, p = z + 2 2, e =, q,, = z, q,2, = z 2 + z +, ( q 2,, = z ) z 2 q,, = z + z + 2 2, ( 2 2 ) z 2 z , and A = We return now to the general case. Consder the equaton ya = c. Snce A has a row for each polynomal q,j,k and a column for each power z d we have an entry n y correspondng to each q,j,k and an entry n c correspondng to each z d. A polynomal s zero f and only f all ts coeffcents are, so ya = c f and only f.e. f yax = cx, m e d η,j,k q,j,k = γ d l z d l = j= k= l= where η,j,k s the entry of y n the poston correspondng to q,j,k and γ d l s the entry n c n the poston correspondng to z d l. Defnng the polynomals r and s,j by r = γ d l z d l l= 8

9 and s,j = d k= η,j,k z d k, the equaton above becomes r = m e = j= s,j p e j l l. Ths equaton n polynomals s equvalent to the equaton r p = m e = j= s,j p j, for ratonal functons, where the polynomals r and s,j are defned by In other words, solvng ya = c s equvalent to computng the partal fracton decomposton of the ratonal functon r/p. Can ths equaton be solved for all column vectors c? Snce A s a square matrx we know from elementary lnear algebra that ether ts range s everythng or ts null space s nonzero. So to show that ths equaton s solvable for all c t suffces to show that there s no non-zero y such that ya = 0. In terms of polynomals, we want to show that f m e = j= s,j p e j l l = 0 then s,j = 0 for all and j. Assume otherwse. Then there s a last value of for whch there s a non-zero s,j and for ths value of there s a last j for whch s,j. But then all the other summands above are dvsble by p e j+ l l. Snce 0 s also dvsble by ths we fnd that s,j p e j l l s dvsble by the same factor. Dvdng by, we then fnd that p e j s,j l l s dvsble by p. None of the p l are dvsble by p, so s,j s dvsble by p. But s,j s of degree at most d, so t must then be zero, contrary to our assumpton. So our assumpton that there s a non-zero s,j n the expanson m e = j= s,j p e j l l = 0 cannot be correct. The matrx A therefore has non-zero null space and hence full range. We conclude that for any polynomal r of degree lower than d there are unque polynomals s,j of degree less than d such that r p = m e = j= s,j p j. Thus the partal fracton expanson of a proper ratonal functon exsts and s unque. Furthermore t can be found explctly by matrx arthmetc. Of course f we have an mproper ratonal functon t/p then we can fnd the quotent and remander t = pq + r 9

10 and obtan an expanson t p = q + m e = j= s,j p j, smlar to the prevous one, but wth an extra polynomal summand. As an example, we compute the partal fracton expanson of the ratonal functon z 4 z z +. The results wll be dfferent dependng on whether we re workng over the real or complex numbers. Over the reals, we have, as we found before, A = Its nverse s 2 A = Our numerator s, whch s represented by the column vector c = ( ), so we need to compute y = ca = ( ). Our partal fracton expanson s then z 4 z z +. = (z ) + (z ) 2 + z + z 2 + z +. Over the complex numbers we have A = , A = , and y = ( ). The partal fracton expanson s therefore z 4 z z + = z + (z ) z z In theory complex numbers are smpler to deal wth because all polynomals factor completely but they are often harder to deal wth n practce, as n ths example. 6 The CRT A useful result n elementary number theory s the Chnese Remander Theorem, whch allows us to solve smultaneous congruences. There s a smlar result for polynomals, whch we can now prove. Suppose, as n the prevous secton, that p = m = p e 0

11 where each p s monc rreducble and p and p j are relatvely prme for j, and that d be the degree of p. For any set of polynomals r k of degree less than d k e k there s a polynomal t of degree less than d such that t r k (mod p e k k ). To see ths let s,j,k be the unque soluton to r k = m e = j= s,j,k p e j l l, whch we know exsts because of the prevous secton. Then e j= for k, so s,j,k p e j l l 0 (mod p e k k ) r k t k (mod p e k k ). where t k = We note that e k j= s k,j,k p e k j k l k l. t k 0 (mod l ) for l k. Also the degree of t k s less than d, so m m e k t = t k = s,j, p e j k= = j= s the polynomal we re seekng. l l.

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens THE CHINESE REMAINDER THEOREM KEITH CONRAD We should thank the Chnese for ther wonderful remander theorem. Glenn Stevens 1. Introducton The Chnese remander theorem says we can unquely solve any par of

More information

a b a In case b 0, a being divisible by b is the same as to say that

a b a In case b 0, a being divisible by b is the same as to say that Secton 6.2 Dvsblty among the ntegers An nteger a ε s dvsble by b ε f there s an nteger c ε such that a = bc. Note that s dvsble by any nteger b, snce = b. On the other hand, a s dvsble by only f a = :

More information

Foundations of Arithmetic

Foundations of Arithmetic Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an

More information

Example: (13320, 22140) =? Solution #1: The divisors of are 1, 2, 3, 4, 5, 6, 9, 10, 12, 15, 18, 20, 27, 30, 36, 41,

Example: (13320, 22140) =? Solution #1: The divisors of are 1, 2, 3, 4, 5, 6, 9, 10, 12, 15, 18, 20, 27, 30, 36, 41, The greatest common dvsor of two ntegers a and b (not both zero) s the largest nteger whch s a common factor of both a and b. We denote ths number by gcd(a, b), or smply (a, b) when there s no confuson

More information

Math 261 Exercise sheet 2

Math 261 Exercise sheet 2 Math 261 Exercse sheet 2 http://staff.aub.edu.lb/~nm116/teachng/2017/math261/ndex.html Verson: September 25, 2017 Answers are due for Monday 25 September, 11AM. The use of calculators s allowed. Exercse

More information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could

More information

DISCRIMINANTS AND RAMIFIED PRIMES. 1. Introduction A prime number p is said to be ramified in a number field K if the prime ideal factorization

DISCRIMINANTS AND RAMIFIED PRIMES. 1. Introduction A prime number p is said to be ramified in a number field K if the prime ideal factorization DISCRIMINANTS AND RAMIFIED PRIMES KEITH CONRAD 1. Introducton A prme number p s sad to be ramfed n a number feld K f the prme deal factorzaton (1.1) (p) = po K = p e 1 1 peg g has some e greater than 1.

More information

Difference Equations

Difference Equations Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1

More information

Complex Numbers. x = B B 2 4AC 2A. or x = x = 2 ± 4 4 (1) (5) 2 (1)

Complex Numbers. x = B B 2 4AC 2A. or x = x = 2 ± 4 4 (1) (5) 2 (1) Complex Numbers If you have not yet encountered complex numbers, you wll soon do so n the process of solvng quadratc equatons. The general quadratc equaton Ax + Bx + C 0 has solutons x B + B 4AC A For

More information

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,

More information

APPENDIX A Some Linear Algebra

APPENDIX A Some Linear Algebra APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,

More information

5 The Rational Canonical Form

5 The Rational Canonical Form 5 The Ratonal Canoncal Form Here p s a monc rreducble factor of the mnmum polynomal m T and s not necessarly of degree one Let F p denote the feld constructed earler n the course, consstng of all matrces

More information

Section 3.6 Complex Zeros

Section 3.6 Complex Zeros 04 Chapter Secton 6 Comple Zeros When fndng the zeros of polynomals, at some pont you're faced wth the problem Whle there are clearly no real numbers that are solutons to ths equaton, leavng thngs there

More information

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

COMPLEX NUMBERS AND QUADRATIC EQUATIONS COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not

More information

PRIMES 2015 reading project: Problem set #3

PRIMES 2015 reading project: Problem set #3 PRIMES 2015 readng project: Problem set #3 page 1 PRIMES 2015 readng project: Problem set #3 posted 31 May 2015, to be submtted around 15 June 2015 Darj Grnberg The purpose of ths problem set s to replace

More information

Lecture 5 Decoding Binary BCH Codes

Lecture 5 Decoding Binary BCH Codes Lecture 5 Decodng Bnary BCH Codes In ths class, we wll ntroduce dfferent methods for decodng BCH codes 51 Decodng the [15, 7, 5] 2 -BCH Code Consder the [15, 7, 5] 2 -code C we ntroduced n the last lecture

More information

Errors for Linear Systems

Errors for Linear Systems Errors for Lnear Systems When we solve a lnear system Ax b we often do not know A and b exactly, but have only approxmatons  and ˆb avalable. Then the best thng we can do s to solve ˆx ˆb exactly whch

More information

LECTURE V. 1. More on the Chinese Remainder Theorem We begin by recalling this theorem, proven in the preceeding lecture.

LECTURE V. 1. More on the Chinese Remainder Theorem We begin by recalling this theorem, proven in the preceeding lecture. LECTURE V EDWIN SPARK 1. More on the Chnese Remander Theorem We begn by recallng ths theorem, proven n the preceedng lecture. Theorem 1.1 (Chnese Remander Theorem). Let R be a rng wth deals I 1, I 2,...,

More information

SL n (F ) Equals its Own Derived Group

SL n (F ) Equals its Own Derived Group Internatonal Journal of Algebra, Vol. 2, 2008, no. 12, 585-594 SL n (F ) Equals ts Own Derved Group Jorge Macel BMCC-The Cty Unversty of New York, CUNY 199 Chambers street, New York, NY 10007, USA macel@cms.nyu.edu

More information

Polynomials. 1 More properties of polynomials

Polynomials. 1 More properties of polynomials Polynomals 1 More propertes of polynomals Recall that, for R a commutatve rng wth unty (as wth all rngs n ths course unless otherwse noted), we defne R[x] to be the set of expressons n =0 a x, where a

More information

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0 MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector

More information

FINITELY-GENERATED MODULES OVER A PRINCIPAL IDEAL DOMAIN

FINITELY-GENERATED MODULES OVER A PRINCIPAL IDEAL DOMAIN FINITELY-GENERTED MODULES OVER PRINCIPL IDEL DOMIN EMMNUEL KOWLSKI Throughout ths note, s a prncpal deal doman. We recall the classfcaton theorem: Theorem 1. Let M be a fntely-generated -module. (1) There

More information

Problem Do any of the following determine homomorphisms from GL n (C) to GL n (C)?

Problem Do any of the following determine homomorphisms from GL n (C) to GL n (C)? Homework 8 solutons. Problem 16.1. Whch of the followng defne homomomorphsms from C\{0} to C\{0}? Answer. a) f 1 : z z Yes, f 1 s a homomorphsm. We have that z s the complex conjugate of z. If z 1,z 2

More information

Formulas for the Determinant

Formulas for the Determinant page 224 224 CHAPTER 3 Determnants e t te t e 2t 38 A = e t 2te t e 2t e t te t 2e 2t 39 If 123 A = 345, 456 compute the matrx product A adj(a) What can you conclude about det(a)? For Problems 40 43, use

More information

An Introduction to Morita Theory

An Introduction to Morita Theory An Introducton to Morta Theory Matt Booth October 2015 Nov. 2017: made a few revsons. Thanks to Nng Shan for catchng a typo. My man reference for these notes was Chapter II of Bass s book Algebrac K-Theory

More information

Problem Solving in Math (Math 43900) Fall 2013

Problem Solving in Math (Math 43900) Fall 2013 Problem Solvng n Math (Math 43900) Fall 2013 Week four (September 17) solutons Instructor: Davd Galvn 1. Let a and b be two nteger for whch a b s dvsble by 3. Prove that a 3 b 3 s dvsble by 9. Soluton:

More information

2.3 Nilpotent endomorphisms

2.3 Nilpotent endomorphisms s a block dagonal matrx, wth A Mat dm U (C) In fact, we can assume that B = B 1 B k, wth B an ordered bass of U, and that A = [f U ] B, where f U : U U s the restrcton of f to U 40 23 Nlpotent endomorphsms

More information

THE SUMMATION NOTATION Ʃ

THE SUMMATION NOTATION Ʃ Sngle Subscrpt otaton THE SUMMATIO OTATIO Ʃ Most of the calculatons we perform n statstcs are repettve operatons on lsts of numbers. For example, we compute the sum of a set of numbers, or the sum of the

More information

8.6 The Complex Number System

8.6 The Complex Number System 8.6 The Complex Number System Earler n the chapter, we mentoned that we cannot have a negatve under a square root, snce the square of any postve or negatve number s always postve. In ths secton we want

More information

Affine transformations and convexity

Affine transformations and convexity Affne transformatons and convexty The purpose of ths document s to prove some basc propertes of affne transformatons nvolvng convex sets. Here are a few onlne references for background nformaton: http://math.ucr.edu/

More information

The Ramanujan-Nagell Theorem: Understanding the Proof By Spencer De Chenne

The Ramanujan-Nagell Theorem: Understanding the Proof By Spencer De Chenne The Ramanujan-Nagell Theorem: Understandng the Proof By Spencer De Chenne 1 Introducton The Ramanujan-Nagell Theorem, frst proposed as a conjecture by Srnvasa Ramanujan n 1943 and later proven by Trygve

More information

where a is any ideal of R. Lemma 5.4. Let R be a ring. Then X = Spec R is a topological space Moreover the open sets

where a is any ideal of R. Lemma 5.4. Let R be a ring. Then X = Spec R is a topological space Moreover the open sets 5. Schemes To defne schemes, just as wth algebrac varetes, the dea s to frst defne what an affne scheme s, and then realse an arbtrary scheme, as somethng whch s locally an affne scheme. The defnton of

More information

Bernoulli Numbers and Polynomials

Bernoulli Numbers and Polynomials Bernoull Numbers and Polynomals T. Muthukumar tmk@tk.ac.n 17 Jun 2014 The sum of frst n natural numbers 1, 2, 3,..., n s n n(n + 1 S 1 (n := m = = n2 2 2 + n 2. Ths formula can be derved by notng that

More information

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons

More information

12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA. 4. Tensor product

12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA. 4. Tensor product 12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA Here s an outlne of what I dd: (1) categorcal defnton (2) constructon (3) lst of basc propertes (4) dstrbutve property (5) rght exactness (6) localzaton

More information

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law: CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

2 More examples with details

2 More examples with details Physcs 129b Lecture 3 Caltech, 01/15/19 2 More examples wth detals 2.3 The permutaton group n = 4 S 4 contans 4! = 24 elements. One s the dentty e. Sx of them are exchange of two objects (, j) ( to j and

More information

9 Characteristic classes

9 Characteristic classes THEODORE VORONOV DIFFERENTIAL GEOMETRY. Sprng 2009 [under constructon] 9 Characterstc classes 9.1 The frst Chern class of a lne bundle Consder a complex vector bundle E B of rank p. We shall construct

More information

Structure and Drive Paul A. Jensen Copyright July 20, 2003

Structure and Drive Paul A. Jensen Copyright July 20, 2003 Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.

More information

= z 20 z n. (k 20) + 4 z k = 4

= z 20 z n. (k 20) + 4 z k = 4 Problem Set #7 solutons 7.2.. (a Fnd the coeffcent of z k n (z + z 5 + z 6 + z 7 + 5, k 20. We use the known seres expanson ( n+l ( z l l z n below: (z + z 5 + z 6 + z 7 + 5 (z 5 ( + z + z 2 + z + 5 5

More information

Digital Signal Processing

Digital Signal Processing Dgtal Sgnal Processng Dscrete-tme System Analyss Manar Mohasen Offce: F8 Emal: manar.subh@ut.ac.r School of IT Engneerng Revew of Precedent Class Contnuous Sgnal The value of the sgnal s avalable over

More information

MMA and GCMMA two methods for nonlinear optimization

MMA and GCMMA two methods for nonlinear optimization MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons

More information

18.781: Solution to Practice Questions for Final Exam

18.781: Solution to Practice Questions for Final Exam 18.781: Soluton to Practce Questons for Fnal Exam 1. Fnd three solutons n postve ntegers of x 6y = 1 by frst calculatng the contnued fracton expanson of 6. Soluton: We have 1 6=[, ] 6 6+ =[, ] 1 =[,, ]=[,,

More information

First day August 1, Problems and Solutions

First day August 1, Problems and Solutions FOURTH INTERNATIONAL COMPETITION FOR UNIVERSITY STUDENTS IN MATHEMATICS July 30 August 4, 997, Plovdv, BULGARIA Frst day August, 997 Problems and Solutons Problem. Let {ε n } n= be a sequence of postve

More information

Some Consequences. Example of Extended Euclidean Algorithm. The Fundamental Theorem of Arithmetic, II. Characterizing the GCD and LCM

Some Consequences. Example of Extended Euclidean Algorithm. The Fundamental Theorem of Arithmetic, II. Characterizing the GCD and LCM Example of Extended Eucldean Algorthm Recall that gcd(84, 33) = gcd(33, 18) = gcd(18, 15) = gcd(15, 3) = gcd(3, 0) = 3 We work backwards to wrte 3 as a lnear combnaton of 84 and 33: 3 = 18 15 [Now 3 s

More information

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1 C/CS/Phy9 Problem Set 3 Solutons Out: Oct, 8 Suppose you have two qubts n some arbtrary entangled state ψ You apply the teleportaton protocol to each of the qubts separately What s the resultng state obtaned

More information

ALGEBRA HW 7 CLAY SHONKWILER

ALGEBRA HW 7 CLAY SHONKWILER ALGEBRA HW 7 CLAY SHONKWILER 1 Whch of the followng rngs R are dscrete valuaton rngs? For those that are, fnd the fracton feld K = frac R, the resdue feld k = R/m (where m) s the maxmal deal), and a unformzer

More information

where a is any ideal of R. Lemma Let R be a ring. Then X = Spec R is a topological space. Moreover the open sets

where a is any ideal of R. Lemma Let R be a ring. Then X = Spec R is a topological space. Moreover the open sets 11. Schemes To defne schemes, just as wth algebrac varetes, the dea s to frst defne what an affne scheme s, and then realse an arbtrary scheme, as somethng whch s locally an affne scheme. The defnton of

More information

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP C O L L O Q U I U M M A T H E M A T I C U M VOL. 80 1999 NO. 1 FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP BY FLORIAN K A I N R A T H (GRAZ) Abstract. Let H be a Krull monod wth nfnte class

More information

Kernel Methods and SVMs Extension

Kernel Methods and SVMs Extension Kernel Methods and SVMs Extenson The purpose of ths document s to revew materal covered n Machne Learnng 1 Supervsed Learnng regardng support vector machnes (SVMs). Ths document also provdes a general

More information

Attacks on RSA The Rabin Cryptosystem Semantic Security of RSA Cryptology, Tuesday, February 27th, 2007 Nils Andersen. Complexity Theoretic Reduction

Attacks on RSA The Rabin Cryptosystem Semantic Security of RSA Cryptology, Tuesday, February 27th, 2007 Nils Andersen. Complexity Theoretic Reduction Attacks on RSA The Rabn Cryptosystem Semantc Securty of RSA Cryptology, Tuesday, February 27th, 2007 Nls Andersen Square Roots modulo n Complexty Theoretc Reducton Factorng Algorthms Pollard s p 1 Pollard

More information

332600_08_1.qxp 4/17/08 11:29 AM Page 481

332600_08_1.qxp 4/17/08 11:29 AM Page 481 336_8_.qxp 4/7/8 :9 AM Page 48 8 Complex Vector Spaces 8. Complex Numbers 8. Conjugates and Dvson of Complex Numbers 8.3 Polar Form and DeMovre s Theorem 8.4 Complex Vector Spaces and Inner Products 8.5

More information

Lecture 3. Ax x i a i. i i

Lecture 3. Ax x i a i. i i 18.409 The Behavor of Algorthms n Practce 2/14/2 Lecturer: Dan Spelman Lecture 3 Scrbe: Arvnd Sankar 1 Largest sngular value In order to bound the condton number, we need an upper bound on the largest

More information

Lecture 4: Universal Hash Functions/Streaming Cont d

Lecture 4: Universal Hash Functions/Streaming Cont d CSE 5: Desgn and Analyss of Algorthms I Sprng 06 Lecture 4: Unversal Hash Functons/Streamng Cont d Lecturer: Shayan Oves Gharan Aprl 6th Scrbe: Jacob Schreber Dsclamer: These notes have not been subjected

More information

Linear Approximation with Regularization and Moving Least Squares

Linear Approximation with Regularization and Moving Least Squares Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...

More information

NOTES ON SIMPLIFICATION OF MATRICES

NOTES ON SIMPLIFICATION OF MATRICES NOTES ON SIMPLIFICATION OF MATRICES JONATHAN LUK These notes dscuss how to smplfy an (n n) matrx In partcular, we expand on some of the materal from the textbook (wth some repetton) Part of the exposton

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

Lecture Notes Introduction to Cluster Algebra

Lecture Notes Introduction to Cluster Algebra Lecture Notes Introducton to Cluster Algebra Ivan C.H. Ip Updated: Ma 7, 2017 3 Defnton and Examples of Cluster algebra 3.1 Quvers We frst revst the noton of a quver. Defnton 3.1. A quver s a fnte orented

More information

Exercises. 18 Algorithms

Exercises. 18 Algorithms 18 Algorthms Exercses 0.1. In each of the followng stuatons, ndcate whether f = O(g), or f = Ω(g), or both (n whch case f = Θ(g)). f(n) g(n) (a) n 100 n 200 (b) n 1/2 n 2/3 (c) 100n + log n n + (log n)

More information

Restricted Lie Algebras. Jared Warner

Restricted Lie Algebras. Jared Warner Restrcted Le Algebras Jared Warner 1. Defntons and Examples Defnton 1.1. Let k be a feld of characterstc p. A restrcted Le algebra (g, ( ) [p] ) s a Le algebra g over k and a map ( ) [p] : g g called

More information

Notes on Frequency Estimation in Data Streams

Notes on Frequency Estimation in Data Streams Notes on Frequency Estmaton n Data Streams In (one of) the data streamng model(s), the data s a sequence of arrvals a 1, a 2,..., a m of the form a j = (, v) where s the dentty of the tem and belongs to

More information

MEM 255 Introduction to Control Systems Review: Basics of Linear Algebra

MEM 255 Introduction to Control Systems Review: Basics of Linear Algebra MEM 255 Introducton to Control Systems Revew: Bascs of Lnear Algebra Harry G. Kwatny Department of Mechancal Engneerng & Mechancs Drexel Unversty Outlne Vectors Matrces MATLAB Advanced Topcs Vectors A

More information

REDUCTION MODULO p. We will prove the reduction modulo p theorem in the general form as given by exercise 4.12, p. 143, of [1].

REDUCTION MODULO p. We will prove the reduction modulo p theorem in the general form as given by exercise 4.12, p. 143, of [1]. REDUCTION MODULO p. IAN KIMING We wll prove the reducton modulo p theorem n the general form as gven by exercse 4.12, p. 143, of [1]. We consder an ellptc curve E defned over Q and gven by a Weerstraß

More information

Workshop: Approximating energies and wave functions Quantum aspects of physical chemistry

Workshop: Approximating energies and wave functions Quantum aspects of physical chemistry Workshop: Approxmatng energes and wave functons Quantum aspects of physcal chemstry http://quantum.bu.edu/pltl/6/6.pdf Last updated Thursday, November 7, 25 7:9:5-5: Copyrght 25 Dan Dll (dan@bu.edu) Department

More information

The Order Relation and Trace Inequalities for. Hermitian Operators

The Order Relation and Trace Inequalities for. Hermitian Operators Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence

More information

1 GSW Iterative Techniques for y = Ax

1 GSW Iterative Techniques for y = Ax 1 for y = A I m gong to cheat here. here are a lot of teratve technques that can be used to solve the general case of a set of smultaneous equatons (wrtten n the matr form as y = A), but ths chapter sn

More information

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

From Biot-Savart Law to Divergence of B (1)

From Biot-Savart Law to Divergence of B (1) From Bot-Savart Law to Dvergence of B (1) Let s prove that Bot-Savart gves us B (r ) = 0 for an arbtrary current densty. Frst take the dvergence of both sdes of Bot-Savart. The dervatve s wth respect to

More information

MTH 819 Algebra I S13. Homework 1/ Solutions. 1 if p n b and p n+1 b 0 otherwise ) = 0 if p q or n m. W i = rw i

MTH 819 Algebra I S13. Homework 1/ Solutions. 1 if p n b and p n+1 b 0 otherwise ) = 0 if p q or n m. W i = rw i MTH 819 Algebra I S13 Homework 1/ Solutons Defnton A. Let R be PID and V a untary R-module. Let p be a prme n R and n Z +. Then d p,n (V) = dm R/Rp p n 1 Ann V (p n )/p n Ann V (p n+1 ) Note here that

More information

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2 Salmon: Lectures on partal dfferental equatons 5. Classfcaton of second-order equatons There are general methods for classfyng hgher-order partal dfferental equatons. One s very general (applyng even to

More information

The Geometry of Logit and Probit

The Geometry of Logit and Probit The Geometry of Logt and Probt Ths short note s meant as a supplement to Chapters and 3 of Spatal Models of Parlamentary Votng and the notaton and reference to fgures n the text below s to those two chapters.

More information

1 Matrix representations of canonical matrices

1 Matrix representations of canonical matrices 1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:

More information

Quantum Mechanics for Scientists and Engineers. David Miller

Quantum Mechanics for Scientists and Engineers. David Miller Quantum Mechancs for Scentsts and Engneers Davd Mller Types of lnear operators Types of lnear operators Blnear expanson of operators Blnear expanson of lnear operators We know that we can expand functons

More information

MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS

MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS These are nformal notes whch cover some of the materal whch s not n the course book. The man purpose s to gve a number of nontrval examples

More information

Density matrix. c α (t)φ α (q)

Density matrix. c α (t)φ α (q) Densty matrx Note: ths s supplementary materal. I strongly recommend that you read t for your own nterest. I beleve t wll help wth understandng the quantum ensembles, but t s not necessary to know t n

More information

Outline and Reading. Dynamic Programming. Dynamic Programming revealed. Computing Fibonacci. The General Dynamic Programming Technique

Outline and Reading. Dynamic Programming. Dynamic Programming revealed. Computing Fibonacci. The General Dynamic Programming Technique Outlne and Readng Dynamc Programmng The General Technque ( 5.3.2) -1 Knapsac Problem ( 5.3.3) Matrx Chan-Product ( 5.3.1) Dynamc Programmng verson 1.4 1 Dynamc Programmng verson 1.4 2 Dynamc Programmng

More information

12. The Hamilton-Jacobi Equation Michael Fowler

12. The Hamilton-Jacobi Equation Michael Fowler 1. The Hamlton-Jacob Equaton Mchael Fowler Back to Confguraton Space We ve establshed that the acton, regarded as a functon of ts coordnate endponts and tme, satsfes ( ) ( ) S q, t / t+ H qpt,, = 0, and

More information

Week 2. This week, we covered operations on sets and cardinality.

Week 2. This week, we covered operations on sets and cardinality. Week 2 Ths week, we covered operatons on sets and cardnalty. Defnton 0.1 (Correspondence). A correspondence between two sets A and B s a set S contaned n A B = {(a, b) a A, b B}. A correspondence from

More information

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also

More information

Math 594. Solutions 1

Math 594. Solutions 1 Math 594. Solutons 1 1. Let V and W be fnte-dmensonal vector spaces over a feld F. Let G = GL(V ) and H = GL(W ) be the assocated general lnear groups. Let X denote the vector space Hom F (V, W ) of lnear

More information

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016 U.C. Berkeley CS94: Spectral Methods and Expanders Handout 8 Luca Trevsan February 7, 06 Lecture 8: Spectral Algorthms Wrap-up In whch we talk about even more generalzatons of Cheeger s nequaltes, and

More information

Week 5: Neural Networks

Week 5: Neural Networks Week 5: Neural Networks Instructor: Sergey Levne Neural Networks Summary In the prevous lecture, we saw how we can construct neural networks by extendng logstc regresson. Neural networks consst of multple

More information

Poisson brackets and canonical transformations

Poisson brackets and canonical transformations rof O B Wrght Mechancs Notes osson brackets and canoncal transformatons osson Brackets Consder an arbtrary functon f f ( qp t) df f f f q p q p t But q p p where ( qp ) pq q df f f f p q q p t In order

More information

763622S ADVANCED QUANTUM MECHANICS Solution Set 1 Spring c n a n. c n 2 = 1.

763622S ADVANCED QUANTUM MECHANICS Solution Set 1 Spring c n a n. c n 2 = 1. 7636S ADVANCED QUANTUM MECHANICS Soluton Set 1 Sprng 013 1 Warm-up Show that the egenvalues of a Hermtan operator  are real and that the egenkets correspondng to dfferent egenvalues are orthogonal (b)

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

Lecture 2: Gram-Schmidt Vectors and the LLL Algorithm

Lecture 2: Gram-Schmidt Vectors and the LLL Algorithm NYU, Fall 2016 Lattces Mn Course Lecture 2: Gram-Schmdt Vectors and the LLL Algorthm Lecturer: Noah Stephens-Davdowtz 2.1 The Shortest Vector Problem In our last lecture, we consdered short solutons to

More information

MULTIPLICATIVE FUNCTIONS: A REWRITE OF ANDREWS CHAPTER 6

MULTIPLICATIVE FUNCTIONS: A REWRITE OF ANDREWS CHAPTER 6 MULTIPLICATIVE FUNCTIONS: A REWRITE OF ANDREWS CHAPTER 6 In these notes we offer a rewrte of Andrews Chapter 6. Our am s to replace some of the messer arguments n Andrews. To acheve ths, we need to change

More information

Homework Notes Week 7

Homework Notes Week 7 Homework Notes Week 7 Math 4 Sprng 4 #4 (a Complete the proof n example 5 that s an nner product (the Frobenus nner product on M n n (F In the example propertes (a and (d have already been verfed so we

More information

More metrics on cartesian products

More metrics on cartesian products More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of

More information

The internal structure of natural numbers and one method for the definition of large prime numbers

The internal structure of natural numbers and one method for the definition of large prime numbers The nternal structure of natural numbers and one method for the defnton of large prme numbers Emmanul Manousos APM Insttute for the Advancement of Physcs and Mathematcs 3 Poulou str. 53 Athens Greece Abstract

More information

Limited Dependent Variables

Limited Dependent Variables Lmted Dependent Varables. What f the left-hand sde varable s not a contnuous thng spread from mnus nfnty to plus nfnty? That s, gven a model = f (, β, ε, where a. s bounded below at zero, such as wages

More information

The KMO Method for Solving Non-homogenous, m th Order Differential Equations

The KMO Method for Solving Non-homogenous, m th Order Differential Equations The KMO Method for Solvng Non-homogenous, m th Order Dfferental Equatons Davd Krohn Danel Marño-Johnson John Paul Ouyang March 14, 2013 Abstract Ths paper shows a smple tabular procedure for fndng the

More information

Problem Set 9 Solutions

Problem Set 9 Solutions Desgn and Analyss of Algorthms May 4, 2015 Massachusetts Insttute of Technology 6.046J/18.410J Profs. Erk Demane, Srn Devadas, and Nancy Lynch Problem Set 9 Solutons Problem Set 9 Solutons Ths problem

More information

STAT 309: MATHEMATICAL COMPUTATIONS I FALL 2018 LECTURE 16

STAT 309: MATHEMATICAL COMPUTATIONS I FALL 2018 LECTURE 16 STAT 39: MATHEMATICAL COMPUTATIONS I FALL 218 LECTURE 16 1 why teratve methods f we have a lnear system Ax = b where A s very, very large but s ether sparse or structured (eg, banded, Toepltz, banded plus

More information

Solutions to Problem Set 6

Solutions to Problem Set 6 Solutons to Problem Set 6 Problem 6. (Resdue theory) a) Problem 4.7.7 Boas. n ths problem we wll solve ths ntegral: x sn x x + 4x + 5 dx: To solve ths usng the resdue theorem, we study ths complex ntegral:

More information

On quasiperfect numbers

On quasiperfect numbers Notes on Number Theory and Dscrete Mathematcs Prnt ISSN 1310 5132, Onlne ISSN 2367 8275 Vol. 23, 2017, No. 3, 73 78 On quasperfect numbers V. Sva Rama Prasad 1 and C. Suntha 2 1 Nalla Malla Reddy Engneerng

More information

Linear Algebra and its Applications

Linear Algebra and its Applications Lnear Algebra and ts Applcatons 4 (00) 5 56 Contents lsts avalable at ScenceDrect Lnear Algebra and ts Applcatons journal homepage: wwwelsevercom/locate/laa Notes on Hlbert and Cauchy matrces Mroslav Fedler

More information

ALGEBRA MID-TERM. 1 Suppose I is a principal ideal of the integral domain R. Prove that the R-module I R I has no non-zero torsion elements.

ALGEBRA MID-TERM. 1 Suppose I is a principal ideal of the integral domain R. Prove that the R-module I R I has no non-zero torsion elements. ALGEBRA MID-TERM CLAY SHONKWILER 1 Suppose I s a prncpal deal of the ntegral doman R. Prove that the R-module I R I has no non-zero torson elements. Proof. Note, frst, that f I R I has no non-zero torson

More information