Some properties of random staircase tableaux

Size: px
Start display at page:

Download "Some properties of random staircase tableaux"

Transcription

1 Some properties of ranom staircase tableaux Sanrine Dasse Hartaut Pawe l Hitczenko Downloae /4/7 to Reistribution subject to SIAM license or copyright; see Abstract We escribe a probabilistic approach to a relatively new combinatorial object calle staircase tableaux Our approach allows us to analyze several parameters of a ranomly chosen staircase tableau of a given size Introuction A new combinatorial structure, calle staircase tableaux, was introuce in recent work of Corteel an Williams [8, ] They are relate to the asymmetric exclusion process on an one-imensional lattice with open bounaries, the ASEP This is an important an heavily stuie particle moel in statistical mechanics we refer to [8] for some backgroun information on several versions of that moel an their applications an connections to other branches of science) The stuy of the generating function of the staircase tableau has given a formula for the steay state probability of the ASEP In the same work staircase tableaux were also use to give a combinatorial formula for the moments of the weight function of the) Askey-Wilson polynomials; for a follow up work see [7] The authors of [8] calle for further investigation of the staircase tableaux because of their combinatorial interest an their potential connection to geometry In this note, we take up that issue an stuy some basic properties of staircase tableaux More precisely, we analyze the istribution of appearances of Greek letters α, β,, an in a ranomly chosen staircase tableau of size n or on the iagonal of such tableau We refer to the next section or to [8, Section ] for the necessary efinitions an the precise meaning of these symbols The work of the first author was carrie out while she hel an ANR Gamma internship at LIPN, Université Paris Nor, uner the irection of Fréérique Bassino LIPN) an Sylvie Corteel LIAFA) She woul like to thank both of them for their guiance, the members of LIPN for their hospitality, an ANR Gamma for the support The secon author was partially supporte in part by NSA Grant #H Most of his work was one uring his stay at LIPN in July 00 He woul like to thank Fréérique Bassino LIPN) for the invitation an acknowlege the hospitality of LIPN LIAFA, Université Paris Dierot Paris 7, F-7505 Paris, France Department of Mathematics, Drexel University, Philaelphia, PA904, USA Here, we only mention that in the context of the ASEP these letters correspon to the probabilities of particles entering or leaving the lattice from either irection) Staircase tableaux are generalizations of permutation tableaux see eg [5, 9, 0, 7] an references therein for more information on these objects an their connection to a version of ASEP referre to as the partially asymmetric exclusion process; PASEP) For permutation tableaux, the authors of [5] evelope a probabilistic approach that later allowe the erivation of the limiting an even exact) istributions of various parameters of the permutation tableaux Our goal here is the same: we will evelop a probabilistic approach parallel to that of [5] that will allow us to systematically compute generating functions of various quantities associate with staircase tableaux an, as a consequence, obtain their exact or limiting istributions A few of those statements coul be also obtaine by combinatorial approach base on an involution on staircase tableaux an on transformation of the parameters uner that involution Nonetheless, asie of giving new insights, our probabilistic approach allows for a more systematic an universal analysis, an thus has a value in itself, we think As we will see below, one of the parameters we stuy, namely the number of letters α or or, equivalently, the number of letters β or ) on the iagonal of a tableau turns out to coincie with a generalization of Eulerian numbers see [0, sequence A06087]) relate to Whitney numbers of Dowling lattices It seems that the first trace of the sequence [0, sequence A06087] in the literature goes back to MacMahon s paper [8], an that fairly recently this sequence has been stuie in a wier context in [6] We refer to [0, sequences A06087, A4590, A09775] an [4,,, 4] for efinitions an further information on the numbers we mentione, an the relations between them This rather unexpecte an intriguing connection between the parameter we stuy here an the generalize Eulerian numbers has not been explaine an merits, perhaps, further stuies One consequence of our work is that the triangle of generalize Eulerian numbers [0, sequence A06087], when suitably normalize, satisfies the central limit theorem As far as we can tell this result is new although it is an easy consequence of a general Copyright 0 SIAM Unauthorize reprouction is prohibite 58

2 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see theorem of Bener []) Limit theorems for a relate sequence [0, A4590] are establishe in [4] This link may have unravele connection to geometry allue to in [8] as the sequences A06087, A4590, an A09775 from [0] all have a very strong geometrical flavor Due to space limitation, we will not give the full etails here, referring instea to the full version of the paper, now in preparation We will confine ourselves to giving a etaile escription of our approach, state our results, an inclue a sample proof to illustrate how our approach works in practice Definitions an notation Staircase tableaux We recall the following concept first introuce in [8, ]: A staircase tableau of size n is a Young iagram of shape n, n,,, ) whose boxes are fille accoring to the following rules: each box is either empty or contains one of the letters α, β,, or; no box on the iagonal is empty; all boxes in the same row an to the left of a β or a are empty; all boxes in the same column an above an α or a are empty An example of a staircase tableau of size 7 is given in Figure below β β α Figure : A staircase tableau of size 7; its top row is inexe by β, the next one by α α We enote the set of all staircase tableaux of size n by S n, n It is known that the carinality of S n is 4 n n! There are several proofs of this statement cf [7] for one of them an for references to further proofs) All these proofs are base on combinatorial approaches an we wish to mention that a probabilistic technique that we evelop in this paper may be use to provie yet another proof of that fact We present our proof in Section 4 below α Connection to ASEP Staircase or earlier permutation) tableaux were introuce an stuie in the connection with ASEP Because of the importance of this connection we briefly recall its nature The ASEP is a Markov chain on wors of size n on an alphabet A {, } consisting of two letters Each such wor represents an one-imensional lattice of length n with some sites occupie by particles represente by ), an others not represente by ) A particle can only hop to the right or the left with the probabilities u an q, respectively), provie that the ajacent site is unoccupie, or enter or quit the lattice Entering from the left right) happens with the probability α resp, ) ifthe first last) site is unoccupie Exiting to the left right) happens with the probability resp β) if the first last) site is occupie At a given time one of the n + possible locations for a move is selecte uniformly at ranom) an, if possible, a transition escribe above is performe with the given probability We refer to [,, 5] or [8] for more etaile escription an further references To escribe the connection to staircase tableaux, efine the type of a staircase tableau S of size n to be a wor of the same size on the alphabet {, } obtaine by reaing the iagonal boxes from northeast NE) to southwest SW) an writing for each α or, an for each β or Thus a type of a tableau is a possible state for the ASEP) Figure shows a tableau with its type β α α α β Figure : A staircase tableau an its type ) We also nee a weight of a tableau S To compute it, we first label the empty boxes of S with u s an q s as follows: first, we fill all the boxes to the left of a β with u s, an all the boxes to the left of a with q s Then, we fill the boxes above an α or a with u s, an the boxes above a β or a with q s When the tableau is fille, its weight, wts), is a monomial of egree nn + )/ in α, β,,, u an q, which is the prouct of labels of the boxes of S Figure shows a tableau fille with u s an q s Its weight is α β u 8 q 9 Corteel an Williams [8, ] have shown that the Copyright 0 SIAM Unauthorize reprouction is prohibite 59

3 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see u β u u α q q u α u u q q q q q u α q q u β Figure : A staircase tableau with u s an q s steay state probability that the ASEP is in state σ is Z σ α, β,,, q, u) Z n α, β,,, q, u), where Z n α, β,,, q, u) Z σ α, β,,, q, u) S of type σ S of size n wts) wts) an Further efinitions an notation We now efine some parameters that will be object of our stuy Let be a subset of the set of symbols {α, β,, } We say that a row of a staircase tableau is inexe by if the leftmost entry in that row is in For the sake of brevity we will refer to rows inexe by simply as rows Thus, for example, the number of α/ rows is the number of rows inexe by α or The tableau in Figure has two α/ rows, the secon from the top inexe by α) an the bottom inexe by ) For a given staircase tableau S S n we enote this quantity by r n S) an we occasionally will skip the subscript n if there is no risk of confusion As we will see below this parameter will play a funamental role in our approach Other parameters we will consier are: the total number of entries β or β/ for short), the total number of entries α or α/), the number of entries β/ on the iagonal of the tableau, an the number of entries α/ on the iagonal For a given tableau S S n these parameters will be enote by Δ n S), Γ n S), B n S), an A n S), respectively For a tableau in Figure they are: Δ 7 S) 5,Γ 7 S) 6,B 7 S), an A 7 S) 4 Our results may be summarize as follows: all these parameters, after suitable normalization, are asymptotically normal More precisely, if Y n is any of the statistics, r n,δ n S), Γ n S), B n S), or A n S)thenasn Y n EY n N0, ), varyn ) where N0, ) enotes the stanar normal variable an the convergence is in istribution for a precise statement see Theorem 5 below) We will also obtain the exact expressions for the expecte value an the variance of Y n in each of the five cases Furthermore, inthecaseofr n,δ n,anγ n we will obtain a simple escription of the exact istribution of Y n from which it reaily follows that they are asymptotically normal) Because of the symmetries in staircase tableaux, these five cases are not inepenent of one another In fact, it suffices to consier one of r n,δ n,γ n an either A n or B n see Remark in Section 5 for the explanation), but it is interesting to know that each of these cases can be treate by our approach inepenently of other cases Also, our results o not istinguish α from an β from an so we coul replace each pair by one symbol an use only two nontrivial entries in our tableaux However, each of them has its own interpretation in terms of ASEP an this symmetry in α/ an β/ breaks in that context For this reason we ecie to follow the same notation as in the literature on ASEP As we mentione earlier our viewpoint will be probabilistic Thus, we will equip the set S n with the uniform probability measure enote by P n That means that for each S S n we have P n S) 4 n n! As is customary we will refer to a tableau chosen accoring to that measure as a ranom tableau of size n We will enote the integration with respect to the measure P n by E n With this unerstaning, the quantities r n,δ n,γ n, B n,ana n being functions on a probability space, are ranom variables from now on referre to as statistics) an we will analyze their probabilistic properties like expecte values, variances, an exact or limiting istributions) In orer to o that we will evelop a technique that is analogous to what has been one in the case of permutation tableaux see [5] or [7]) Let us recall at this point that permutation tableaux have been use to give a combinatorial escription of a stationary istribution for the PASEP We refer to eg [9, 0, 5, 7] for the efinition, connections to PASEP, further properties an etails Just as PASEP is a particular case of ASEP, permutation tableaux of size n are in bijection with a subset of staircase tableaux of that size corresponing to the case 0 Let us recall that the approach use in [5, 7] for the permutation tableaux was to ientify a funamental parameter, trace its evolution as the size of a tableau is increase by, an then use successively conitioning to reuce the size of a tableau We refer the reaer to either [5] or [7] for more etails, here we only recall that this funamental parameter was the number of unrestricte rows in a permutation tableau, an that its conitional istribution was given by + BinU n, /) This is to Copyright 0 SIAM Unauthorize reprouction is prohibite 60

4 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see mean that if a size of permutation tableau with U n unrestricte rows was increase from n ton, then the number of unrestricte rows in this extension ha the conitional) istribution + BinU n, /) As we will see in the forthcoming section, in the case of staircase tableaux the role of a funamental parameter will be playe by the number of α/ rows Set-up To escribe our approach we nee to briefly recall the evolution process of staircase tableaux escribe in [6] Let S S n be a tableau with r n r n S) α/ rows To exten its size by, we a a new column of length n at the left en an we nee to fill it accoring to the rules If r n 0thenalln rowsofs are β/ rows an hence the top n boxes of the new column have to be empty since no entries are allowe to the left of a β/ inthesamerow Thus,ifr n 0weobtain four ifferent tableaux of size n by putting one of the four symbols in the bottom box of the new column If r n then we can either put one of the symbols α/ in the bottom corner an then we are force to leave all other boxes in that column empty), or we can put a β/ in the bottom box of the new column In that case, we nee to fill all boxes in the new column corresponing to one of the r n α/ rows Accoring to the rules, if we put an α/ in any of them, then we nee to leave all boxes above it empty, otherwise we have a complete freeom It is thus seen that any tableau of size n with r n α/ rows gives 4 rn ifferent staircase tableaux of size n Inee, if r n 0 then there are 4 extensions an if r n then there are rn )+ rn ) extensions Here, the first is from putting an α/ in the bottom box of the new column, the next is from putting a β/ in that box, the term i, i r n is from putting the first counting from bottom up in the new column) α/ in the ith row as then there are i ways of filling the earlier i boxeswithsymbols β,, or leaving them empty, an finally, the rn term comes from not putting an α/ in any of the r n rows an thus filling these r n rows with β/ s or leaving them empty Summing the above gives ) + rn + rn + rn + rn )4 rn, as claime The above iscussion may be phrase in a more probabilistic language using what Shiryaev [9, Chapter I, 8 ] refers to as ecompositions which is just a special case of conitioning with respect to σ algebra) To escribe the ecomposition of S n that we will be using, note that every tableau from S n is an extension of a unique tableau S from S n Therefore, enoting by D S the set of all tableaux from S n which are obtaine from S by the process escribe above as we just iscusse, there are 4 rn S) such tableaux), we can write S n D S, S S n where D S ) S Sn are pairwise isjoint subsets of S n We enote this ecomposition of S n by D n We will nee to be able to compute the conitional probabilities P D n ) an the conitional expectations E D n ) with respect to this ecomposition To o that, let S S n be a particular tableau with r n r n S) α/ rows an let r be the number of such rows in any of its extensions to a tableau of size n We wish to know the conitional) istribution of r Clearly, the possible values for r are r n +,r n,r n,,, 0 an we nee to know the probabilities for each of these possibilities First, Pr r n + D S )PC α/ D S ) ) 4 rn, rn where the symbol C enotes the event that we put one of the symbols in the bottom box of the new column as we exten the tableau Next, for k 0,,,r n we compute Pr r n k D S ) Since k is the number of β/ s that we put in the r n allowable ie corresponing to α/ rows of S) boxes,r r n k means that we put a β/ in the bottom box an aitional kβ/ s in the r n allowable boxes above it If we o not put an α/ in any of those k boxes, we have k r n ) k possibilities is for putting a β/ at the bottom, an the rest accounts for putting β/ s in any k of the allowable r n boxes) If we o put an α/ in one of the boxes we nee to pick k + of the allowable r n boxes, put an α/ in the topmost of them an put β/ s in the remaining k of them an at the bottom) This gives k+ r n ) k+ possibilities Thus, Pr r n k D S ) k+ r n ) k+ + rn ) k ) ) 4 rn This together with ) completely escribes the conitional istribution of r n given D n an leas, in particular, to the following basic relation: For a complex number z an n with the unerstaning that Copyright 0 SIAM Unauthorize reprouction is prohibite 6

5 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see r 0 0) ) Ez rn D n ) z + ) rn z + Since we will prove a more general statement later see a comment following 65)) we will not justify ) here We wish to comment, however, that calculations similar to those giving ) are typical for our approach In fact, the ability to compute the conitional expectations of various quantities will turn up to be one of the two main ingreients of our metho We now iscuss the secon ingreient Focus on S n, the set of all staircase tableaux of size n There are two natural probability measures on S n to consier One is the uniform measure enote by P n ) an the other is a measure obtaine from the uniform probability measure on S n by collapsing all the elements of S n that are extensions of the same element S S n We will enote the latter measure P n S) there is an apparent ambiguity of notation here, however, it isappears once we remember whether S is in S n or S n ) The relationship between these two measures on S n is straightforwar to fin: since a tableau S S n with r n α/ rows gives 4 rn tableaux in S n we have 4) P n S) 4 rn 4 rn S n 4 S n rn P n S) S n Consequently, for any ranom variable X n on S n we have E n X n E n 4 S n rn X n 4 S n 5) E n rn X n Here we have use the same convention as above; for a ranom variable X on S n, E n X enotes the expectation with respect to the uniform measure on S n while E n X enotes the expectation with respect to the measure that is inuce on S n by the uniform measure on S n The relations ) an 5) are key an will allow us to analyze the istributions of the various statistics on S n Note that 4) an 5) are true regarless of whether we know the carinalities of S n an S n or not As a matter of fact, one can use 5) to provie a yet another argument that 4 n n! We refer the reaer to the full version of the paper for the etails, here we just note that once this is known, 4) an 5) simplify to 6) an 7) respectively P n S) rn n P n S) E n X n n E n rn X n, 4 Illustration: the number of staircase tableaux To illustrate how ) an 5) work we re-erive the expression for the total number of staircase tableaux of size n Proposition 4 Let S n be the set of all staircase tableaux of size n Then 4 n n! Proof Since a tableau S of size n with r n S) α/ rows gives 4 rns) tableaux of size n +, grouping the elements of S n+ accoringly, we have: S n+ 4 rns) 4 rns) S S n S S n Now observe that S S n rns) is simply the expecte value of rn compute over the uniform probability measure on S n Therefore, S n+ 4E n rn By basic properties of the conitional expectation see eg [9, Formula 6), p 79]) the expectation on the right han sie is equal to E n E rn D n ) Using this an then ) with z we see that the right han sie above is ) rn + + 4E n E rn D n )4E n 4 S n E n ) rn 5 We now use 5) with X n 5/) rn to get S n+ 4 S n 4 S n 5 E n rn 4 S n E n 5 rn ) rn Copyright 0 SIAM Unauthorize reprouction is prohibite 6

6 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see This can be iterate an gives that S n+ is equal to S n k 4k k ) ) k+)e n kk+)+) r n k With k n this becomes S n+ S 4n n n n!e n +) r Since S 4anE n +) r n +)+ we get S n+ 4 n n ++ n! 4 n+ n +)!, which proves the statement an inepenently confirms the count of staircase tableaux 5 Main results Our technique allows us to obtain the istribution sometimes exact, sometimes only asymptotic) of the statistics iscusse above Before we state our results let us recall that if X an Y are two ranom variables not necessarily efine on the same probability space) then X Y means equality in istribution Moreover if X n ) is a sequence of ranom variables which may be efine on ifferent probability spaces) then X n X enotes the convergence in istribution That means that as n then PX n x) PX x) for all x at which the function on the right is continuous We will be ealing exclusively with the case when X is the stanar normal ranom variable, N0, ) an we recall that its istribution function is given by Φx) π x We can now state our results e t / t Theorem 5 Consier the set S n with the uniform probability measure P n The following are true: i) For every n we have r n n J k, where J k s are inepenent an J k is a ranom variable which is with probability /k) an 0 with the remaining probability In particular, n E n r n k H n ln n, varr n ) n ) k k H n H) n 4 ln n, where H n n k an H) n n k are harmonic numbers of the first an secon orer, respectively Moreover, as n, r n ln n ln n ii) For every n we have 58) Δ n N0, ) n J k ), where J k ) are as in part i) In particular, we have 59) E n Δ n n H n, 50) varδ n ) H n H) n 4, an, as n, 5) iii) For every n Δ n n + ln n ln n Γ n Δn N0, ) In particular, 58) 5) hol with Δ n replace by Γ n iv) The expecte value an the variance of the number A n of α/ on the iagonal of a ranom staircase tableau of size n are, respectively, 5) E n A n n an vara n ) n + Furthermore, for n, 5) A n n/ n/ v) For every n we have N0, ) B n An In particular, 5) an 5) hol for B n in place of A n Copyright 0 SIAM Unauthorize reprouction is prohibite 6

7 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see Remark Several statements of the above theorem may be euce from others Inee, there is an involution φ on the set of staircase tableaux of a given size This involution has the following properties: if S, T S n are such that T φs) then a) Δ n S) Γ n T )anγ n S) Δ n T ); b) B n S) A n T )ana n S) B n T ) Moreover, since any row is either inexe by α/ or contains a β/, one has c) r n S)+Δ n S) n for any S S n Thus a) an c) combine imply that any of the parts i), ii), iii) of Theorem 5 implies the other two Furthermore, b) implies that part v) of that theorem follows from iv) or vice versa) Nonetheless, as far as we know, neither any of i)-iii) nor iv) or v) were known before, an so the results presente in Theorem 5 are new Besies, we think it is it is worth emphasizing that our probabilistic approach oes provie a unifie an systematic approach that in particular allows one to prove all parts of that theorem irectly an without a nee to appeal to any further information 6 Sample proof Detaile proofs of the results given in Theorem 5 will be inclue in the full version of the paper Here, to illustrate how the technique works we will just prove one part of this theorem In orer to avoi overlap with what will be presente in the paper an also to show that each part of Theorem 5 may be obtaine irectly ie without appealing to the involution on staircase tableaux) we will prove part iii) More precisely, we will show irectly that Γ n satisfies 58) 5) of part ii) of Theorem 5 To this en, we compute the joint probability generating function E n t Γn z rn of Γ n an r n We write Γ n n g k where g k is if an α/ is inserte when the kth column to the tableau is ae an is 0 otherwise recall that there can be at most one α/ in any column) We then have n E n t Γn z rn E n t g k z rn E n t Γn t gn z rn By the funamental properties of the conitional expectation see eg [9, Formulas 6), p 79 an 7), p 80]) the quantity on the right han sie is equal to 64) E n Et Γ n t gn z rn D n ) ) E n t Γ n Et gn z rn D n ) ) To procee we nee to compute the conitional expectation Et gn z rn D n ) We let F k enote the event that as we a the nth column we put kβ/ s in the r n boxes corresponing to α/ rows of a tableau of size n that we are extening Then Et gn z rn D n ) r n k0 r n tz rn k Pg n,f k D n ) + z rn k Pg n 0,F k D n ) k0 Note that the first sum is only to r n sincethe event {g n,f rn } is impossible) Consier the secon sum The event {g n 0,F k } means that we put a β/ in the bottom box of the nth column an aitional kβ/ s in the r n rows inexe by α/ s Thus we see that the secon sum is r n k0 ) z rn k k+ rn k 4 rn z +)rn 4 rn ) rn z + As for the first sum, {g n,f 0 } means that we either put an α/ in the bottom box of the nth column or we put a β/ in that box an no β/ in the r n allowable boxes above it Splitting the probability of this event accoringly, we see that the first sum is tz rn + rn r n ) +t z rn k k+ rn k + 4 rn k0 tz z ) rn + tz r n ) z rn k+) k+ rn 4 rn k + k0 tz z ) rn tz + z rn +)rn z rn ) tz ) rn z + Combining, we obtain that 65) Et gn z rn D n ) tz + ) rn z + Note that putting t gives ) an that the above calculation oes not use anything but ) an ) so Copyright 0 SIAM Unauthorize reprouction is prohibite 64

8 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see it is a self containe proof of )) Substituting 65) into equation 64) we obtain ) rn tz + z + E n t Γn z rn E n t Γn Now using 7) with we further get E n t Γn z rn X n t Γn z + ) rn tz + z + n E n rn t Γn tz + n E n t Γn z +) rn ) rn This can be iterate an upon further iteration yiels E n t Γn z rn Since n k0 tz +k)+) n E t Γ z +n )) r n! E t Γ z +n )t) r tz +n )) + ) tz +n )) +, we finally obtain E n t Γn z rn n Putting z wegetthat n tk ) + E n t Γn k n k0 tz +k)+) n n! tz +k )) + k n k )t + ) k The kth factor on the right han sie is the probability generating function of a ranom variable I k that is with probability /k) an is 0 with the remaining probability Since the prouct correspons to aing inepenent ranom variables, we see that Γ n n But this is just what 58) states The rest follows immeiately since n n E n Γ n EI k k )n H n, I k an varγ n ) n vari k ) n k k )H n H n 4 Finally, since I k EI k are uniformly boune an variances of the partial sums go to infinity, the Lineberg s conition for the central limit theorem see eg [9, Chapter III, 4]) hols trivially, thus giving 5) References [] E A Bener Central an local limit theorems applie to asymptotic enumeration J Combin Theory Ser A, 5:9, 97 [] M Benoumhani On Whitney numbers of Dowling lattices Discrete Math, 59-):, 996 [] M Benoumhani On some numbers relate to Whitney numbers of Dowling lattices Av in Appl Math, 9):06 6, 997 [4] L Clark Limit theorems for associate Whitney numbers of Dowling lattices J Combin Math Combin Comput, 50:05, 004 [5] S Corteel an P Hitczenko Expecte values of statistics on permutation tableaux In 007 Conference on Analysis of Algorithms, AofA 07, Discrete Math Theor Comput Sci Proc, AH, pages 5 9 Assoc Discrete Math Theor Comput Sci, Nancy, 007 [6] S Corteel, D Stanton, an L Williams Enumeration of staircase tableaux, 007 Preprint [7] S Corteel, D Stanton, an R Stanley L K Williams Formulae for Askey Wilson moments an enumeration of staircase tableaux arxiv: [8] S Corteel an L K Williams Tableaux combinatorics for the asymmetric exclusion process an Askey Wilson polynomials arxiv: [9] S Corteel an L K Williams A Markov chain on permutations which projects to the PASEP Int Math Res Notes, 7, 007 Art ID rnm055, 7pp [0] S Corteel an L K Williams Tableaux combinatorics for the asymmetric exclusion process Av Appl Math,, 9:9 0, 007 [] S Corteel an L K Williams Staircase tableaux, the asymmetric exclusion process, an askey- wilson polynomials Proc Natl Aca Sci, 075): , 00 [] B Derria, E Domany, an D Mukamel An exact solution of a one imensional asymmetric exclusion process with open bounaries J Statist Phys, 69-4): , 99 [] B Derria, M R Evans, V Hakim, an V Pasquier Exact solution of a D asymmetric exclusion moel using a matrix formulation J Phys A, 67):49 57, 99 [4] T A Dowling A class of geometric lattices base on finite groups J Combinatorial Theory Ser B, 4:6 86, 97 Erratum: J Combinatorial Theory Ser B, 5:, 97) Copyright 0 SIAM Unauthorize reprouction is prohibite 65

9 Downloae /4/7 to Reistribution subject to SIAM license or copyright; see [5] E Duchi an G Schaeffer A combinatorial approach to jumping particles J Combin Theory Ser A, 0): 9, 005 [6] G R Franssens On a Number Pyrami Relate to the Binomial, Deleham, Eulerian, MacMahon an Stirling number triangles Journal of Integer Sequences, 9: Article 064, 006 [7] P Hitczenko an S Janson Asymptotic normality of statistics on permutation tableaux Contemporary Math, 50:8 04, 00 [8] P A MacMahon The ivisors of numbers Proc Lonon Math Soc, 9: 05-40, 90 [9] A N Shiryaev Probability, volume 95 of Grauate Texts in Mathematics Springer-Verlag, New York, secon eition, 996 [0] N J A Sloane The On-Line Encyclopeia of Integer Sequences, 006 wwwresearchattcom/ njas/sequences/ Copyright 0 SIAM Unauthorize reprouction is prohibite 66

ON THE ASYMPTOTIC DISTRIBUTION OF PARAMETERS IN RANDOM WEIGHTED STAIRCASE TABLEAUX

ON THE ASYMPTOTIC DISTRIBUTION OF PARAMETERS IN RANDOM WEIGHTED STAIRCASE TABLEAUX ON THE ASYMPTOTIC DISTRIBUTION OF PARAMETERS IN RANDOM WEIGHTED STAIRCASE TABLEAUX PAWE L HITCZENKO AND AMANDA PARSHALL Abstract In this paper, we study staircase tableaux, a combinatorial object introduced

More information

arxiv: v1 [math.co] 7 Apr 2009

arxiv: v1 [math.co] 7 Apr 2009 arxiv:0904v [mathco] 7 Apr 009 Asymptotic Normality of Statistics on Permutation Tableaux Pawe l Hitczenko an Svante Janson Abstract In this paper we use a probabilistic approach to erive the expressions

More information

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

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

More information

Linear First-Order Equations

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

More information

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS

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

More information

2Algebraic ONLINE PAGE PROOFS. foundations

2Algebraic ONLINE PAGE PROOFS. foundations Algebraic founations. Kick off with CAS. Algebraic skills.3 Pascal s triangle an binomial expansions.4 The binomial theorem.5 Sets of real numbers.6 Surs.7 Review . Kick off with CAS Playing lotto Using

More information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

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

More information

On the enumeration of partitions with summands in arithmetic progression

On the enumeration of partitions with summands in arithmetic progression AUSTRALASIAN JOURNAL OF COMBINATORICS Volume 8 (003), Pages 149 159 On the enumeration of partitions with summans in arithmetic progression M. A. Nyblom C. Evans Department of Mathematics an Statistics

More information

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

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

More information

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

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

More information

Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs

Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs Ashish Goel Michael Kapralov Sanjeev Khanna Abstract We consier the well-stuie problem of fining a perfect matching in -regular bipartite

More information

Permanent vs. Determinant

Permanent vs. Determinant Permanent vs. Determinant Frank Ban Introuction A major problem in theoretical computer science is the Permanent vs. Determinant problem. It asks: given an n by n matrix of ineterminates A = (a i,j ) an

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

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

More information

Math 1271 Solutions for Fall 2005 Final Exam

Math 1271 Solutions for Fall 2005 Final Exam Math 7 Solutions for Fall 5 Final Eam ) Since the equation + y = e y cannot be rearrange algebraically in orer to write y as an eplicit function of, we must instea ifferentiate this relation implicitly

More information

Separation of Variables

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

More information

Calculus of Variations

Calculus of Variations Calculus of Variations Lagrangian formalism is the main tool of theoretical classical mechanics. Calculus of Variations is a part of Mathematics which Lagrangian formalism is base on. In this section,

More information

The Exact Form and General Integrating Factors

The Exact Form and General Integrating Factors 7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily

More information

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

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

More information

The total derivative. Chapter Lagrangian and Eulerian approaches

The total derivative. Chapter Lagrangian and Eulerian approaches Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function

More information

On colour-blind distinguishing colour pallets in regular graphs

On colour-blind distinguishing colour pallets in regular graphs J Comb Optim (2014 28:348 357 DOI 10.1007/s10878-012-9556-x On colour-blin istinguishing colour pallets in regular graphs Jakub Przybyło Publishe online: 25 October 2012 The Author(s 2012. This article

More information

Ramsey numbers of some bipartite graphs versus complete graphs

Ramsey numbers of some bipartite graphs versus complete graphs Ramsey numbers of some bipartite graphs versus complete graphs Tao Jiang, Michael Salerno Miami University, Oxfor, OH 45056, USA Abstract. The Ramsey number r(h, K n ) is the smallest positive integer

More information

Chromatic number for a generalization of Cartesian product graphs

Chromatic number for a generalization of Cartesian product graphs Chromatic number for a generalization of Cartesian prouct graphs Daniel Král Douglas B. West Abstract Let G be a class of graphs. The -fol gri over G, enote G, is the family of graphs obtaine from -imensional

More information

The chromatic number of graph powers

The chromatic number of graph powers Combinatorics, Probability an Computing (19XX) 00, 000 000. c 19XX Cambrige University Press Printe in the Unite Kingom The chromatic number of graph powers N O G A A L O N 1 an B O J A N M O H A R 1 Department

More information

Discrete Mathematics

Discrete Mathematics Discrete Mathematics 309 (009) 86 869 Contents lists available at ScienceDirect Discrete Mathematics journal homepage: wwwelseviercom/locate/isc Profile vectors in the lattice of subspaces Dániel Gerbner

More information

Some Examples. Uniform motion. Poisson processes on the real line

Some Examples. Uniform motion. Poisson processes on the real line Some Examples Our immeiate goal is to see some examples of Lévy processes, an/or infinitely-ivisible laws on. Uniform motion Choose an fix a nonranom an efine X := for all (1) Then, {X } is a [nonranom]

More information

Symbolic integration with respect to the Haar measure on the unitary groups

Symbolic integration with respect to the Haar measure on the unitary groups BULLETIN OF THE POLISH ACADEMY OF SCIENCES TECHNICAL SCIENCES, Vol. 65, No., 207 DOI: 0.55/bpasts-207-0003 Symbolic integration with respect to the Haar measure on the unitary groups Z. PUCHAŁA* an J.A.

More information

05 The Continuum Limit and the Wave Equation

05 The Continuum Limit and the Wave Equation Utah State University DigitalCommons@USU Founations of Wave Phenomena Physics, Department of 1-1-2004 05 The Continuum Limit an the Wave Equation Charles G. Torre Department of Physics, Utah State University,

More information

FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS. 1. Introduction

FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS. 1. Introduction FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS ALINA BUCUR, CHANTAL DAVID, BROOKE FEIGON, MATILDE LALÍN 1 Introuction In this note, we stuy the fluctuations in the number

More information

Equilibrium in Queues Under Unknown Service Times and Service Value

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

More information

Schrödinger s equation.

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

More information

Tractability results for weighted Banach spaces of smooth functions

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

More information

Robustness and Perturbations of Minimal Bases

Robustness and Perturbations of Minimal Bases Robustness an Perturbations of Minimal Bases Paul Van Dooren an Froilán M Dopico December 9, 2016 Abstract Polynomial minimal bases of rational vector subspaces are a classical concept that plays an important

More information

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:

More information

SYNCHRONOUS SEQUENTIAL CIRCUITS

SYNCHRONOUS SEQUENTIAL CIRCUITS CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents

More information

Quantum mechanical approaches to the virial

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

More information

arxiv: v4 [math.pr] 27 Jul 2016

arxiv: v4 [math.pr] 27 Jul 2016 The Asymptotic Distribution of the Determinant of a Ranom Correlation Matrix arxiv:309768v4 mathpr] 7 Jul 06 AM Hanea a, & GF Nane b a Centre of xcellence for Biosecurity Risk Analysis, University of Melbourne,

More information

Introduction to Markov Processes

Introduction to Markov Processes Introuction to Markov Processes Connexions moule m44014 Zzis law Gustav) Meglicki, Jr Office of the VP for Information Technology Iniana University RCS: Section-2.tex,v 1.24 2012/12/21 18:03:08 gustav

More information

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy, NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which

More information

arxiv: v1 [math.mg] 10 Apr 2018

arxiv: v1 [math.mg] 10 Apr 2018 ON THE VOLUME BOUND IN THE DVORETZKY ROGERS LEMMA FERENC FODOR, MÁRTON NASZÓDI, AND TAMÁS ZARNÓCZ arxiv:1804.03444v1 [math.mg] 10 Apr 2018 Abstract. The classical Dvoretzky Rogers lemma provies a eterministic

More information

arxiv: v2 [math.st] 29 Oct 2015

arxiv: v2 [math.st] 29 Oct 2015 EXPONENTIAL RANDOM SIMPLICIAL COMPLEXES KONSTANTIN ZUEV, OR EISENBERG, AND DMITRI KRIOUKOV arxiv:1502.05032v2 [math.st] 29 Oct 2015 Abstract. Exponential ranom graph moels have attracte significant research

More information

A Note on Modular Partitions and Necklaces

A Note on Modular Partitions and Necklaces A Note on Moular Partitions an Neclaces N. J. A. Sloane, Rutgers University an The OEIS Founation Inc. South Aelaie Avenue, Highlan Par, NJ 08904, USA. Email: njasloane@gmail.com May 6, 204 Abstract Following

More information

arxiv:hep-th/ v1 3 Feb 1993

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

More information

Vectors in two dimensions

Vectors in two dimensions Vectors in two imensions Until now, we have been working in one imension only The main reason for this is to become familiar with the main physical ieas like Newton s secon law, without the aitional complication

More information

u!i = a T u = 0. Then S satisfies

u!i = a T u = 0. Then S satisfies Deterministic Conitions for Subspace Ientifiability from Incomplete Sampling Daniel L Pimentel-Alarcón, Nigel Boston, Robert D Nowak University of Wisconsin-Maison Abstract Consier an r-imensional subspace

More information

International Journal of Pure and Applied Mathematics Volume 35 No , ON PYTHAGOREAN QUADRUPLES Edray Goins 1, Alain Togbé 2

International Journal of Pure and Applied Mathematics Volume 35 No , ON PYTHAGOREAN QUADRUPLES Edray Goins 1, Alain Togbé 2 International Journal of Pure an Applie Mathematics Volume 35 No. 3 007, 365-374 ON PYTHAGOREAN QUADRUPLES Eray Goins 1, Alain Togbé 1 Department of Mathematics Purue University 150 North University Street,

More information

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

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

More information

Acute sets in Euclidean spaces

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

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

A Sketch of Menshikov s Theorem

A Sketch of Menshikov s Theorem A Sketch of Menshikov s Theorem Thomas Bao March 14, 2010 Abstract Let Λ be an infinite, locally finite oriente multi-graph with C Λ finite an strongly connecte, an let p

More information

Euler equations for multiple integrals

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

More information

. Using a multinomial model gives us the following equation for P d. , with respect to same length term sequences.

. Using a multinomial model gives us the following equation for P d. , with respect to same length term sequences. S 63 Lecture 8 2/2/26 Lecturer Lillian Lee Scribes Peter Babinski, Davi Lin Basic Language Moeling Approach I. Special ase of LM-base Approach a. Recap of Formulas an Terms b. Fixing θ? c. About that Multinomial

More information

Chapter 6: Energy-Momentum Tensors

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

More information

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

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

More information

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

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

More information

SYMMETRIC KRONECKER PRODUCTS AND SEMICLASSICAL WAVE PACKETS

SYMMETRIC KRONECKER PRODUCTS AND SEMICLASSICAL WAVE PACKETS SYMMETRIC KRONECKER PRODUCTS AND SEMICLASSICAL WAVE PACKETS GEORGE A HAGEDORN AND CAROLINE LASSER Abstract We investigate the iterate Kronecker prouct of a square matrix with itself an prove an invariance

More information

Least-Squares Regression on Sparse Spaces

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

More information

MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX

MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX J. WILLIAM HELTON, JEAN B. LASSERRE, AND MIHAI PUTINAR Abstract. We investigate an iscuss when the inverse of a multivariate truncate moment matrix

More information

Math 1B, lecture 8: Integration by parts

Math 1B, lecture 8: Integration by parts Math B, lecture 8: Integration by parts Nathan Pflueger 23 September 2 Introuction Integration by parts, similarly to integration by substitution, reverses a well-known technique of ifferentiation an explores

More information

Characterizing Real-Valued Multivariate Complex Polynomials and Their Symmetric Tensor Representations

Characterizing Real-Valued Multivariate Complex Polynomials and Their Symmetric Tensor Representations Characterizing Real-Value Multivariate Complex Polynomials an Their Symmetric Tensor Representations Bo JIANG Zhening LI Shuzhong ZHANG December 31, 2014 Abstract In this paper we stuy multivariate polynomial

More information

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control

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

More information

arxiv: v1 [math.co] 29 May 2009

arxiv: v1 [math.co] 29 May 2009 arxiv:0905.4913v1 [math.co] 29 May 2009 simple Havel-Hakimi type algorithm to realize graphical egree sequences of irecte graphs Péter L. Erős an István Miklós. Rényi Institute of Mathematics, Hungarian

More information

12.11 Laplace s Equation in Cylindrical and

12.11 Laplace s Equation in Cylindrical and SEC. 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential 593 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential One of the most important PDEs in physics an engineering

More information

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

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

More information

Integration Review. May 11, 2013

Integration Review. May 11, 2013 Integration Review May 11, 2013 Goals: Review the funamental theorem of calculus. Review u-substitution. Review integration by parts. Do lots of integration eamples. 1 Funamental Theorem of Calculus In

More information

Relatively Prime Uniform Partitions

Relatively Prime Uniform Partitions Gen. Math. Notes, Vol. 13, No., December, 01, pp.1-1 ISSN 19-7184; Copyright c ICSRS Publication, 01 www.i-csrs.org Available free online at http://www.geman.in Relatively Prime Uniform Partitions A. Davi

More information

Lecture 5. Symmetric Shearer s Lemma

Lecture 5. Symmetric Shearer s Lemma Stanfor University Spring 208 Math 233: Non-constructive methos in combinatorics Instructor: Jan Vonrák Lecture ate: January 23, 208 Original scribe: Erik Bates Lecture 5 Symmetric Shearer s Lemma Here

More information

A MARKOV CHAIN ON THE SYMMETRIC GROUP WHICH IS SCHUBERT POSITIVE?

A MARKOV CHAIN ON THE SYMMETRIC GROUP WHICH IS SCHUBERT POSITIVE? A MARKOV CHAIN ON THE SYMMETRIC GROUP WHICH IS SCHUBERT POSITIVE? THOMAS LAM AND LAUREN WILLIAMS Abstract. We study a multivariate Markov chain on the symmetric group with remarkable enumerative properties.

More information

Hyperbolic Moment Equations Using Quadrature-Based Projection Methods

Hyperbolic Moment Equations Using Quadrature-Based Projection Methods Hyperbolic Moment Equations Using Quarature-Base Projection Methos J. Koellermeier an M. Torrilhon Department of Mathematics, RWTH Aachen University, Aachen, Germany Abstract. Kinetic equations like the

More information

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu

More information

Introduction to the Vlasov-Poisson system

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

More information

Computing Derivatives

Computing Derivatives Chapter 2 Computing Derivatives 2.1 Elementary erivative rules Motivating Questions In this section, we strive to unerstan the ieas generate by the following important questions: What are alternate notations

More information

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

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

More information

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

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

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

arxiv: v2 [cond-mat.stat-mech] 11 Nov 2016

arxiv: v2 [cond-mat.stat-mech] 11 Nov 2016 Noname manuscript No. (will be inserte by the eitor) Scaling properties of the number of ranom sequential asorption iterations neee to generate saturate ranom packing arxiv:607.06668v2 [con-mat.stat-mech]

More information

Interconnected Systems of Fliess Operators

Interconnected Systems of Fliess Operators Interconnecte Systems of Fliess Operators W. Steven Gray Yaqin Li Department of Electrical an Computer Engineering Ol Dominion University Norfolk, Virginia 23529 USA Abstract Given two analytic nonlinear

More information

TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH

TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH English NUMERICAL MATHEMATICS Vol14, No1 Series A Journal of Chinese Universities Feb 2005 TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH He Ming( Λ) Michael K Ng(Ξ ) Abstract We

More information

d dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1

d dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1 Lecture 5 Some ifferentiation rules Trigonometric functions (Relevant section from Stewart, Seventh Eition: Section 3.3) You all know that sin = cos cos = sin. () But have you ever seen a erivation of

More information

Agmon Kolmogorov Inequalities on l 2 (Z d )

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

More information

1 Math 285 Homework Problem List for S2016

1 Math 285 Homework Problem List for S2016 1 Math 85 Homework Problem List for S016 Note: solutions to Lawler Problems will appear after all of the Lecture Note Solutions. 1.1 Homework 1. Due Friay, April 8, 016 Look at from lecture note exercises:

More information

New bounds on Simonyi s conjecture

New bounds on Simonyi s conjecture New bouns on Simonyi s conjecture Daniel Soltész soltesz@math.bme.hu Department of Computer Science an Information Theory, Buapest University of Technology an Economics arxiv:1510.07597v1 [math.co] 6 Oct

More information

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

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

More information

arxiv: v1 [math.co] 15 Sep 2015

arxiv: v1 [math.co] 15 Sep 2015 Circular coloring of signe graphs Yingli Kang, Eckhar Steffen arxiv:1509.04488v1 [math.co] 15 Sep 015 Abstract Let k, ( k) be two positive integers. We generalize the well stuie notions of (k, )-colorings

More information

How to Minimize Maximum Regret in Repeated Decision-Making

How to Minimize Maximum Regret in Repeated Decision-Making How to Minimize Maximum Regret in Repeate Decision-Making Karl H. Schlag July 3 2003 Economics Department, European University Institute, Via ella Piazzuola 43, 033 Florence, Italy, Tel: 0039-0-4689, email:

More information

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz A note on asymptotic formulae for one-imensional network flow problems Carlos F. Daganzo an Karen R. Smilowitz (to appear in Annals of Operations Research) Abstract This note evelops asymptotic formulae

More information

On conditional moments of high-dimensional random vectors given lower-dimensional projections

On conditional moments of high-dimensional random vectors given lower-dimensional projections Submitte to the Bernoulli arxiv:1405.2183v2 [math.st] 6 Sep 2016 On conitional moments of high-imensional ranom vectors given lower-imensional projections LUKAS STEINBERGER an HANNES LEEB Department of

More information

Proof of SPNs as Mixture of Trees

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

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

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

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

More information

On the minimum distance of elliptic curve codes

On the minimum distance of elliptic curve codes On the minimum istance of elliptic curve coes Jiyou Li Department of Mathematics Shanghai Jiao Tong University Shanghai PRChina Email: lijiyou@sjtueucn Daqing Wan Department of Mathematics University of

More information

On lower bounds for integration of multivariate permutation-invariant functions

On lower bounds for integration of multivariate permutation-invariant functions arxiv:1310.3959v1 [math.na] 15 Oct 2013 On lower bouns for integration of multivariate permutation-invariant functions Markus Weimar October 16, 2013 Abstract In this note we stuy multivariate integration

More information

arxiv: v1 [math.co] 31 Mar 2008

arxiv: v1 [math.co] 31 Mar 2008 On the maximum size of a (k,l)-sum-free subset of an abelian group arxiv:080386v1 [mathco] 31 Mar 2008 Béla Bajnok Department of Mathematics, Gettysburg College Gettysburg, PA 17325-186 USA E-mail: bbajnok@gettysburgeu

More information

Convergence of Random Walks

Convergence of Random Walks Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of

More information

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

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

More information

Similar Operators and a Functional Calculus for the First-Order Linear Differential Operator

Similar Operators and a Functional Calculus for the First-Order Linear Differential Operator Avances in Applie Mathematics, 9 47 999 Article ID aama.998.067, available online at http: www.iealibrary.com on Similar Operators an a Functional Calculus for the First-Orer Linear Differential Operator

More information

Homotopy colimits in model categories. Marc Stephan

Homotopy colimits in model categories. Marc Stephan Homotopy colimits in moel categories Marc Stephan July 13, 2009 1 Introuction In [1], Dwyer an Spalinski construct the so-calle homotopy pushout functor, motivate by the following observation. In the category

More information

TEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS. Yannick DEVILLE

TEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS. Yannick DEVILLE TEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS Yannick DEVILLE Université Paul Sabatier Laboratoire Acoustique, Métrologie, Instrumentation Bât. 3RB2, 8 Route e Narbonne,

More information

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

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

More information

Technion - Computer Science Department - M.Sc. Thesis MSC Constrained Codes for Two-Dimensional Channels.

Technion - Computer Science Department - M.Sc. Thesis MSC Constrained Codes for Two-Dimensional Channels. Technion - Computer Science Department - M.Sc. Thesis MSC-2006- - 2006 Constraine Coes for Two-Dimensional Channels Keren Censor Technion - Computer Science Department - M.Sc. Thesis MSC-2006- - 2006 Technion

More information

Conservation Laws. Chapter Conservation of Energy

Conservation Laws. Chapter Conservation of Energy 20 Chapter 3 Conservation Laws In orer to check the physical consistency of the above set of equations governing Maxwell-Lorentz electroynamics [(2.10) an (2.12) or (1.65) an (1.68)], we examine the action

More information