Mutually Independent Hamiltonian Cycles of Pancake Networks
|
|
- Avice Marsh
- 5 years ago
- Views:
Transcription
1 Mutually Indpndnt Hamiltonian Cycls of Pancak Ntworks Chng-Kuan Lin Dpartmnt of Mathmatics National Cntral Univrsity, Chung-Li, Taiwan 00, R O C discipl@ms0urlcomtw Hua-Min Huang Dpartmnt of Mathmatics National Cntral Univrsity, Chung-Li, Taiwan 00, R O C huang@mathncudutw Jimmy J M Tan Dpartmnt of Computr Scinc National Chiao Tung Univrsity, Hsinchu, Taiwan 00, R O C jmtan@cisnctudutw Lih-Hsing Hsu Information Enginring Dpartmnt Ta Hwa Institut of Tchnology, Hsinchu, Taiwan 07, R O C lhhsu@cisnctudutw Abstract A hamiltonian cycl C of G is dscribd as u, u,,u n(g), u to mphasiz th ordr of nods in C Thus, u is th bginning nod and u i is th i-th nod in C Two hamiltonian cycls of G bginning at a nod x, C = u, u,, u n(g), u and C = v, v,, v n(g), v, ar indpndnt if x = u = v, and u i v i for vry i n(g) A st of hamiltonian cycls {C, C,,C k } of G ar mutually indpndnt if any two diffrnt hamiltonian cycls ar indpndnt Th mutually indpndnt hamiltonicity of graph G, IHC(G), is th maximum intgr k such that for any nod u of G thr xist k-mutually indpndnt hamiltonian cycls of G starting at u In this papr, w ar going to study IHC(G) for th n-dimnsional pancak graph W will prov that IHC(P ) = and IHC( ) = n if n Introduction An intrconnction ntwork conncts th procssors of paralll computrs Its architctur can b rprsntd as a graph in which th nods corrspond to procssors and th dgs corrspond to connctions Hnc, w us graphs and ntworks intrchangably Thr ar many mutually conflicting rquirmnts in dsigning th topology for computr ntworks Akrs and Krishnamurthy [] proposd a family of intrsting intrconnction ntworks, th n-dimnsional pancak graph Thy showd that th pancak graphs ar nod transitiv Hung t al [7] studid th hamiltonian connctivity on th faulty pancak graphs Th mbdding of cycls and trs into th pancak graphs whr discussd in [,, 7, 8] Gats and Papadimitriou [5] studid th diamtr of th pancak graphs Up to now, w do not know th xact valu of th diamtr of th pancak graphs [6] For a graph dfinitions and notation w follow [] G = (V, E) is a graph if V is a finit st and E is a subst of {(u, v) (u, v) is an unordrd pair of V } W say that V is th nod st and E is th dg st W us n(g) to dnot V Lt S b a subst of V Th subgraph of G inducd by S, G[S], is th graph with V (G[S]) = S and E(G[S]) = {(x, y) (x, y) E(G) and x, y S} W us G S to dnot th subgraph of G inducd by V S Two nods u and v ar adjacnt if (u, v) is an dg of G Th st of nighbors of u, dnot by N G (u), is {v (u, v) E} Th dgr d G (u) of a nod u of G is th numbr of dgs incidnt with u Th minimum dgr of G, writtn δ(g),
2 is min{d G (x) x V } A path is a squnc of nods rprsntd by v 0, v,,v k with no rpatd nod and (v i, v i+ ) is an dg of G for all 0 i k W us Q(i) to dnot th i-th nod v i of Q = v, v,,v k W also writ th path v 0, v,, v k as v 0,,v i, Q, v j,, v k, whr Q is a path form v i to v j A path is a hamiltonian path if it contains all nods of G A graph G is hamiltonian connctd if thr xists a hamiltonian path joining any two distinct nods of G A cycl is a path with at last thr nods such that th first nod is th sam as th last on A hamiltonian cycl of G is a cycl that travrss vry nod of G A graph is hamiltonian if it has a hamiltonian cycl A hamiltonian cycl C of graph G is dscribd as u, u,,u n(g), u to mphasiz th ordr of nods in C Thus, u is th bginning nod and u i is th i-th nod in C Two hamiltonian cycls of G bginning at a nod x, C = u, u,, u n(g), u and C = v, v,, v n(g), v, ar indpndnt if x = u = v, and u i v i for vry i n(g) A st of hamiltonian cycls {C, C,,C k } of G ar mutually indpndnt if any two diffrnt hamiltonian cycls ar indpndnt Th mutually indpndnt hamiltonianicity of graph G, IHC(G), is th maximum intgr k such that for any nod u of G thr xist k-mutually indpndnt hamiltonian cycls of G starting at u Obviously, IHC(G) δ(g) if G is a hamiltonian graph Th concpt of mutually indpndnt hamiltonian cycls can b applid in a lot of aras Considr th following scnario In Christmas, w hav a holiday of 0 days A tour agncy will organiz a 0-day tour to Italy Suppos that thr will b a lot of popl joining this tour Howvr, th maximum numbr of popl stay in ach local ara is limitd, say 00 popl, for th sak of hotl contract On trivial solution is on th First-Com-First-Srv basis So only 00 popl can attnd this tour (Not that w can not schdul th tour in a piplind mannr bcaus th holiday priod is fixd) Nonthlss, w obsrv that a tour is lik a hamiltonian cycl basd on a graph, in which a nod is dnotd as a hotl and any two nods ar joind with an dg if th associatd two hotls can b travld in a rasonabl tim Thrfor, w can organiz all th diffrnt subgraphs, i ach subgraph has its own tour In this way, w do not allow two subgroups stay in th sam ara during th sam tim priod In othr words, any two diffrnt tours ar indd indpndnt hamiltonian cycls Suppos that thr ar 0-mutually indpndnt hamiltonian cycls Thn w may allow 000 popl to visit Italy on Christmas vacation For this rason, w would lik to find th maximum numbr of mutually indpndnt hamiltonian cycls Such applications ar usful for task schduling and rsourc placmnt, which ar also important for complir optimization to xploit paralllism In this papr, w study mutually indpndnt hamiltonian cycls of pancak graph In th following sction, w giv th dfinition of th pancak graphs and rviw som of th prvious work usd in this papr In sction, w prov that IHC(P ) = and IHC( ) = n if n Th pancak graphs Lt n b a positiv intgr W us n to dnot th st {,,, n} Th n-dimnsional pancak graph, dnotd by, is a graph with th nod st V ( ) = {u u u n u i n and u i u j for i j} Th adjacncy is dfind as follows: u u u i u n is adjacnt to v v v i v n through an dg of dimnsion i with i n if v j = u i j+ for all j i and v j = u j for all i < j n W will us boldfac to dnot a nod of Hnc, u,u,,u n dnot a squnc of nods in In particular, dnots th nod n Th pancak graphs P, P, and P ar illustratd in Figur P P a b P b Figur : Th pancak graphs P, P, and P By dfinition, is an (n )-rgular graph with n! nods Morovr, it is nod transitiv [] Lt u = u u u n b an arbitrary nod of W us (u) i to dnot th i-th componnt u i of u, and us {i} to dnot th i-th subgraph of inducd by thos nods u with (u) n = i Thn can b dcomposd into n nod disjoint subgraphs {i} for all i n such that ach {i} is isomorphic to Thus, th pancak graph a
3 can b constructd rcursivly Lt H n, w us Pn H to dnot th subgraph of inducd by i H V ( {i} ) For i j n, w us {i,j} to dnot th subgraph of inducd by thos nods u with (u) n = i and (u) n = j Obviously, {i,j} {j,i} and {i,j} is isomorphic to By dfinition, thr is xactly on nighbor v of u such that u and v ar adjacnt through an i-dimnsional dg with i n W us (u) i to dnot th uniqu i-nighbor of u W hav ((u) i ) i = u and (u) n {(u)} For i, j n and i j, w us E i,j to dnot th st of dgs btwn {i} and {j} Lmma Lt i, j n with i j and n Thn E i,j n = (n )! Lmma Lt u and v b two distinct nods of with d(u,v) Thn (u) (v) Thorm [7] Suppos that F is a subst of V ( ) with F n and n Thn F is hamiltonian connctd Thorm Lt {a, a,,a r } b a subst of n for som positiv intgr r n with n 5 Assum that u and v ar two distinct nods of with u and v {ar} Thn thr is a hamiltonian path H = u = x, H,y,x, H,y,,x r, H r,y r = v of r i= {ai} joining u to v such that x = u, P {a} n y r = v, and H i is a hamiltonian path of P {ai} n joining x i to y i for vry i r Proof W st x as u and st that y r as v W know that {ai} is isomorphic to for vry i r By Thorm, this statmnt holds for r = Thus, w assum that r By Lmma, En ai,ai+ = (n )! 6 for vry i r W choos (y i,x i+ ) E ai,ai+ for vry i r with y x and x r y r By Thorm, thr is a hamiltonian path H i of {ai} joining x i to y i for vry i r Thn H = u = x, H,y,x, H,y,,x r, H r,y r = v forms a dsird path S Figur for illustration on { a} u=x { a } x { ar} x r H H y H y r y r =v Figur : Illustration for Thorm on IHC( ) Lmma Lt k n with n, and lt x b a nod of Thr is a hamiltonian path P of {x} joining th nod (x) n to som nod v with (v) = k Proof Suppos that n = Sinc P is nod transitiv, w may assum that x = Th rquird paths of P {} ar listd blow: k = ()()()()()()()() ()()()()()()()() ()()()()()()() k = ()()()()()()()() ()()()()()()()() ()()()()()()() k = ()()()()()()()() ()()()()()()()() ()()()()()()() k = ()()()()()()()() ()()()()()()()() ()()()()()()() With Thorm, w can find th rquird hamiltonian path in for vry n 5 Lmma Lt a, b n with a b and n, and lt x b a nod of Thr is a hamiltonian path P of {x} joining a nod u with (u) = a to a nod v with (v) = b Proof Suppos that n = Sinc P is nod transitiv, w may assum that x = Without loss of gnrality, w may assum that a < b W hav a and b Th rquird paths of P {} ar listd blow: ()()()()()()()() ()()()()()()()() ()()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()()() With Thorm, w can find th rquird hamiltonian path on for vry n 5 Lmma 5 Lt n, and a, b n with a b Assum that x and y ar two adjacnt nods of Thr is a hamiltonian path P of {x,y} joining a nod u with (u) = a to a nod v with (v) = b
4 Proof Sinc is nod transitiv, w may assum that x = and y = () i for som i {,,, n} Without loss of gnrality, w assum that a < b Thus, a n and b W prov this lmma by induction on n For n =, th rquird paths of P {, () i } ar listd blow: y = ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() y = ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() y = ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() ()()()()()()()() ()()()()()()()() ()()()()()() Suppos that this lmma is tru for P k for vry k < n W hav th following cass: Cas y = () i for som i and i n, i y {n} Lt c n {a} By induction, thr is a hamiltonian path R of {n} {, () i } joining a nod u with (u) = a to a nod z with (z) = c W choos a nod v in n {c} with (v) = b By Thorm, thr is a hamiltonian path H of n joining th nod (z) n to v Thn u, R,z, (z) n, H,v forms th dsird path Cas y = () n, i y {} Lt c n {, a} and d n {, b, c} By Lmma, thr is a hamiltonian path R of {n} {} joining a nod u with (u) = a to a nod w with (w) = c Again, thr is a hamiltonian path H of {} {() n } joining a nod z with (z) = d to a nod v with (v) = b By Thorm, thr is a hamiltonian path Q of n {} joining th nod (w) n to th nod (z) n Thn u, R,w, (w) n, Q, (z) n,z, H,v forms th dsird path Lmma 6 Lt a, b n with n Assum that x is a nod of, and x and x ar two distinct nighbors of x Thr is a hamiltonian path P of {x,x,x } joining a nod u with (u) = a to a nod v with (v) = b Proof Sinc is nod transitiv, w may assum that x = Morovr, w assum that x = () i and x = () j for som i, j n {} with i < j Without loss of gnrality, w assum that a < b Thus, a n and b W prov this lmma by induction on n For n =, th rquird paths of P {, () i, () j } ar listd blow: x = and x = ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() x = and x = ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()()
5 x = and x = ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() x = and x = ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() ()()()()()()() Suppos that this lmma is tru for P k for vry k < n W hav th following cass: Cas j n, i x {n} and x {n} Lt c n {, a} By induction, thr is a hamiltonian path R of {n} {,x,x } joining a nod u with (u) = a to a nod z with (z) = c W choos a nod v in {} with (v) = b By Thorm, thr is a hamiltonian path H of n joining th nod (z) n to v W st P = u, R,z, (z) n, H,v, Thn P forms th dsird path Cas j = n, i x {n} and x {} Lt c n {, a} and d n {, b, c} By Lmma 5, thr is a hamiltonian path R of {n} {,x } joining a nod u with (u) = a to a nod z with (z) = c By Lmma, thr is a hamiltonian path H of {} {x } joining a nod w with (w) = d to a nod v with (v) = b By Thorm, thr is a hamiltonian Q of n {} joining th nod (z) n to th nod (w) n W st P = u, R,z, (z) n, Q, (w) n,w, H,v, Thn P forms th dsird path Our main rsult for th pancak graph is statd in th following thorm Thorm IHC(P ) = and IHC( ) = n if n Proof It is asy to s that P is isomorphic to a cycl with six nods, so IHC(P ) = is (n )-rgular graph, it is clar that IHC( ) n Sinc is nod transitiv, w only nd to show that thr xist (n )-mutually indpndnt hamiltonian cycls of starting form th nod For n =, w prov that IHC(P ) by listing th rquird hamiltonian cycls as following: ()()()()()()()()() C ()()()()()()()()() ()()()()()()() ()()()()()()()()() C ()()()()()()()()() ()()()()()()() ()()()()()()()()() C ()()()()()()()()() ()()()()()()() Lt n 5 Lt B b th (n ) n matrix with { i + j if i + j n, b i,j = i + j n + if n < i + j Mor prcisly, n n 5 n B = n n n n It is not hard to s that (b i,, b i,,, b i,n ) forms a prmutation of {,,, n} for vry i with i n Morovr, b i,j b i,j for any i < i n and j n In othr words, B forms a latin rctangl with ntris in {,,, n} W construct {C, C,, C n } as follows: () k = By Lmma, thr is a hamiltonian path H of {b,n} {} joining a nod x with x () n and (x) = n to th nod () n By Thorm, thr is a hamiltonian path H of n t= {b,t} joining th nod () n to th nod (x) n with H (i+(j )(n )!) {b,j } for vry i (n )! and for vry j n W st C =, () n, H, (x) n,x, H, () n, () k = By Lmma 5, thr is a hamiltonian path Q of {b,n } {, () } joining a nod y with (y) = n to a nod z with (z) = By Thorm, thr is a hamiltonian Q of n t= {b,t} joining th nod (() ) n to th nod (y) n such that Q (i + (j )(n )!) {b,j } for vry i (n )! and for vry j n By Thorm, thr is a hamiltonian path Q of {b,n} joining th nod (z) n to th nod () n W st C =, (), (() ) n, Q, (y) n,y, Q,z, (z) n, Q, () n, () k n By Lmma 6, thr is a hamiltonian path R k of P {b k,n k+} n {, () k, () k } joining a nod w k with (w k ) = n to a nod v k with (v k ) = By Thorm, thr is a hamiltonian path R k of n k t= P {b k,t} n joining th
6 nod (() k ) n to th nod (w k ) n such that R k (i + (j )(n )!) P {b k,j} n for vry i (n )! and for vry j n k Again, thr is a hamiltonian path R k of n t=n k+ P {b k,t} n joining th nod (v k ) n to th nod (() k ) n such that R k(i+(j )(n )!) P {b k,n k+j+} n for vry i (n )! and for vry j k W st C k =, () k, (() k ) n, R k, (w k) n,w k, R k,v k, (v k ) n, R k, (() k ) n, () k, Thn {C, C,, C n } forms a st of (n )-mutually indpndnt hamiltonian cycls of starting from th nod Exampl: W illustrat th proof of Thorm with n = 5 as follows: W st 5 B = Thn w construct {C, C, C, C } as follows: () k = By Lmma, thr is a hamiltonian path H of P {b,5} 5 {} joining a nod x with x () and (x) = to th nod () By Thorm, thr is a hamiltonian path H of t= P {b,t} 5 joining th nod () 5 to th nod (x) 5 with H (i + (j )) P {b,j} 5 for vry i and for vry j W st C =, () 5, H, (x) 5,x, H, (), () k = By Lmma 5, thr is a hamiltonian path Q of P {b,} 5 {, () } joining a nod y with (y) = to a nod z with (z) = By Thorm, thr is a hamiltonian Q of t= P {b,t} 5 joining th nod (() ) 5 to th nod (y) 5 such that Q (i + (j )) P {b,j} 5 for vry i and for vry j By Thorm, thr is a hamiltonian path Q of P {b,5} 5 joining th nod (z) 5 to th nod () 5 W st C =, (), (() ) 5, Q, (y) 5,y, Q,z, (z) 5, Q, () 5, C C C C ( ) ( ) ( ) { } ( ) 5 H { } (() ) 5 { } (() ) 5 { } (() ) 5 Q R R 5 6 ( w) 5 6 { } { } { } { 5} { } { } 7 { 5} w - { (, ),( ) } R v 9 ( w) 5 { } ( v) { } - { (, ) } { 5} w 5 - {, ( ), () } R v 7 ( y ) 5 { } ( v) 5 { } 7 { 5} y Q z ( x ) 5 { } { } x { } () z 5 { } - H Q R R ( ( ) ) 5 ( ( ) ) 5 ( ) 0 ( ) Figur : Illustration for Thorm on ( ) ( ) () k By Lmma 6, thr is a hamiltonian path R k of P {b k,6 k} 5 {, () k, () k } joining a nod w k with (w k ) = to a nod v k with (v k ) = By Thorm, thr is a hamiltonian path R k of 5 k t= P {b k,t} 5 joining th nod (() k ) 5 to th nod (w k ) 5 such that R k(i + (j )) P {b k,j} 5 for vry i and for vry j 5 k Again, thr is a hamiltonian path R k of 5 t=7 k P {b k,t} 5 joining th nod (v k ) 5 to th nod (() k ) 5 such that R k(i + (j )) P {b k,6 k+j } 5 for vry i and for vry j k W st C k =, () k, (() k ) 5, R k, (w k) 5,w k, R k,v k, (v k ) 5, R k, (() k ) 5, () k, Thn {C, C, C, C } forms a st of -mutually indpndnt hamiltonian cycls of starting from th nod S Figur for illustration Rfrncs [] S B Akrs and B Krishnamurthy, A groupthortic modl for symmtric intrconnction ntworks, IEEE Transactions on Computrs, Vol 8, pp , 989 [] J A Bondy and U S R Murty, Graph Thory with Applications, North Holland, Nw York, 980 [] K Day and A Tripathi, A comparativ study of topological proprtis, IEEE Transactions on Paralll and Distributd Systms, Vol 5, pp 8, 99 [] W C Fang and C C Hsu, On th faulttolrant mbdding of complt binary tr in th pancak graph intrconnction ntwork, Information Scincs, Vol 6, pp 9 0, 000 [5] W H Gats and C H Papadimitriou, Bounds for sorting by prfix rvrsal, Discrt Mathmatics, Vol 7, pp 7 57, 979 [6] M H Hydari and I H Sudborough, On th diamtr of th pancak ntwork, Journal of Algorithms, Vol 5, pp 67 9, 997 [7] C N Hung, H C Hsu, K Y Liang, and LH Hsu, Ring mbdding in faulty pancak graphs, Information Procssing Lttrs, Vol 86, pp 7 75, 00
7 [8] A Kanvsky and C Fng, On th mbdding of cycls in pancak graphs, Paralll Computing, Vol, pp 9 96, 995
Week 3: Connected Subgraphs
Wk 3: Connctd Subgraphs Sptmbr 19, 2016 1 Connctd Graphs Path, Distanc: A path from a vrtx x to a vrtx y in a graph G is rfrrd to an xy-path. Lt X, Y V (G). An (X, Y )-path is an xy-path with x X and y
More informationThe Equitable Dominating Graph
Intrnational Journal of Enginring Rsarch and Tchnology. ISSN 0974-3154 Volum 8, Numbr 1 (015), pp. 35-4 Intrnational Rsarch Publication Hous http://www.irphous.com Th Equitabl Dominating Graph P.N. Vinay
More informationIntroduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013
18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:
More informationcycle that does not cross any edges (including its own), then it has at least
W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th
More informationBINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES. 1. Statement of results
BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim and n a positiv intgr, lt ν p (n dnot th xponnt of p in n, and u p (n n/p νp(n th unit part of n. If α
More informationOn spanning trees and cycles of multicolored point sets with few intersections
On spanning trs and cycls of multicolord point sts with fw intrsctions M. Kano, C. Mrino, and J. Urrutia April, 00 Abstract Lt P 1,..., P k b a collction of disjoint point sts in R in gnral position. W
More informationSquare of Hamilton cycle in a random graph
Squar of Hamilton cycl in a random graph Andrzj Dudk Alan Friz Jun 28, 2016 Abstract W show that p = n is a sharp thrshold for th random graph G n,p to contain th squar of a Hamilton cycl. This improvs
More informationConstruction of asymmetric orthogonal arrays of strength three via a replacement method
isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy
More informationSection 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation.
MAT 444 H Barclo Spring 004 Homwork 6 Solutions Sction 6 Lt H b a subgroup of a group G Thn H oprats on G by lft multiplication Dscrib th orbits for this opration Th orbits of G ar th right costs of H
More information(Upside-Down o Direct Rotation) β - Numbers
Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg
More informationInternational Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN
Intrnational Journal of Scintific & Enginring Rsarch, Volum 6, Issu 7, July-25 64 ISSN 2229-558 HARATERISTIS OF EDGE UTSET MATRIX OF PETERSON GRAPH WITH ALGEBRAI GRAPH THEORY Dr. G. Nirmala M. Murugan
More informationFinding low cost TSP and 2-matching solutions using certain half integer subtour vertices
Finding low cost TSP and 2-matching solutions using crtain half intgr subtour vrtics Sylvia Boyd and Robrt Carr Novmbr 996 Introduction Givn th complt graph K n = (V, E) on n nods with dg costs c R E,
More informationStrongly Connected Components
Strongly Connctd Componnts Lt G = (V, E) b a dirctd graph Writ if thr is a path from to in G Writ if and is an quivalnc rlation: implis and implis s quivalnc classs ar calld th strongly connctd componnts
More informationBINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES
BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim (implicit in notation and n a positiv intgr, lt ν(n dnot th xponnt of p in n, and U(n n/p ν(n, th unit
More informationDerangements and Applications
2 3 47 6 23 Journal of Intgr Squncs, Vol. 6 (2003), Articl 03..2 Drangmnts and Applications Mhdi Hassani Dpartmnt of Mathmatics Institut for Advancd Studis in Basic Scincs Zanjan, Iran mhassani@iasbs.ac.ir
More informationThe Matrix Exponential
Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!
More informationSOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH.
SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. K VASUDEVAN, K. SWATHY AND K. MANIKANDAN 1 Dpartmnt of Mathmatics, Prsidncy Collg, Chnnai-05, India. E-Mail:vasu k dvan@yahoo.com. 2,
More informationThe Matrix Exponential
Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!
More informationBasic Polyhedral theory
Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist
More informationCombinatorial Networks Week 1, March 11-12
1 Nots on March 11 Combinatorial Ntwors W 1, March 11-1 11 Th Pigonhol Principl Th Pigonhol Principl If n objcts ar placd in hols, whr n >, thr xists a box with mor than on objcts 11 Thorm Givn a simpl
More informationCOUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM
COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM Jim Brown Dpartmnt of Mathmatical Scincs, Clmson Univrsity, Clmson, SC 9634, USA jimlb@g.clmson.du Robrt Cass Dpartmnt of Mathmatics,
More informationLimiting value of higher Mahler measure
Limiting valu of highr Mahlr masur Arunabha Biswas a, Chris Monico a, a Dpartmnt of Mathmatics & Statistics, Txas Tch Univrsity, Lubbock, TX 7949, USA Abstract W considr th k-highr Mahlr masur m k P )
More informationSearching Linked Lists. Perfect Skip List. Building a Skip List. Skip List Analysis (1) Assume the list is sorted, but is stored in a linked list.
3 3 4 8 6 3 3 4 8 6 3 3 4 8 6 () (d) 3 Sarching Linkd Lists Sarching Linkd Lists Sarching Linkd Lists ssum th list is sortd, but is stord in a linkd list. an w us binary sarch? omparisons? Work? What if
More informationCS 361 Meeting 12 10/3/18
CS 36 Mting 2 /3/8 Announcmnts. Homwork 4 is du Friday. If Friday is Mountain Day, homwork should b turnd in at my offic or th dpartmnt offic bfor 4. 2. Homwork 5 will b availabl ovr th wknd. 3. Our midtrm
More informationSome Results on E - Cordial Graphs
Intrnational Journal of Mathmatics Trnds and Tchnology Volum 7 Numbr 2 March 24 Som Rsults on E - Cordial Graphs S.Vnkatsh, Jamal Salah 2, G.Sthuraman 3 Corrsponding author, Dpartmnt of Basic Scincs, Collg
More informationA Polynomial-Time Approximation Scheme for the Minimum-Connected Dominating Set in Ad Hoc Wireless Networks
A Polynomial-Tim Approximation Schm for th Minimum-Connctd Dominating St in Ad Hoc Wirlss Ntworks Xiuzhn Chng Dpartmnt of Computr Scinc, Gorg Washington Univrsity, Washington, DC 20052 Xiao Huang 3M Cntr,
More information10. The Discrete-Time Fourier Transform (DTFT)
Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w
More informationAddition of angular momentum
Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th
More information1 Isoparametric Concept
UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric
More informationSupplementary Materials
6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic
More informationDeift/Zhou Steepest descent, Part I
Lctur 9 Dift/Zhou Stpst dscnt, Part I W now focus on th cas of orthogonal polynomials for th wight w(x) = NV (x), V (x) = t x2 2 + x4 4. Sinc th wight dpnds on th paramtr N N w will writ π n,n, a n,n,
More informationAddition of angular momentum
Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat
More informationSCHUR S THEOREM REU SUMMER 2005
SCHUR S THEOREM REU SUMMER 2005 1. Combinatorial aroach Prhas th first rsult in th subjct blongs to I. Schur and dats back to 1916. On of his motivation was to study th local vrsion of th famous quation
More informationApproximation and Inapproximation for The Influence Maximization Problem in Social Networks under Deterministic Linear Threshold Model
20 3st Intrnational Confrnc on Distributd Computing Systms Workshops Approximation and Inapproximation for Th Influnc Maximization Problm in Social Ntworks undr Dtrministic Linar Thrshold Modl Zaixin Lu,
More informationSECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.
SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain
More informationCOMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.
C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH
More informationMulticoloured Hamilton cycles and perfect matchings in pseudo-random graphs
Multicolourd Hamilton cycls and prfct matchings in psudo-random graphs Danila Kühn Dryk Osthus Abstract Givn 0 < p < 1, w prov that a psudo-random graph G with dg dnsity p and sufficintly larg ordr has
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1
More informationRecall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1
Chaptr 11 Th singular sris Rcall that by Thorms 10 and 104 togthr provid us th stimat 9 4 n 2 111 Rn = SnΓ 2 + on2, whr th singular sris Sn was dfind in Chaptr 10 as Sn = q=1 Sq q 9, with Sq = 1 a q gcda,q=1
More informationCramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter
WHEN THE CRAMÉR-RAO INEQUALITY PROVIDES NO INFORMATION STEVEN J. MILLER Abstract. W invstigat a on-paramtr family of probability dnsitis (rlatd to th Parto distribution, which dscribs many natural phnomna)
More informationSome remarks on Kurepa s left factorial
Som rmarks on Kurpa s lft factorial arxiv:math/0410477v1 [math.nt] 21 Oct 2004 Brnd C. Kllnr Abstract W stablish a connction btwn th subfactorial function S(n) and th lft factorial function of Kurpa K(n).
More informationComputing and Communications -- Network Coding
89 90 98 00 Computing and Communications -- Ntwork Coding Dr. Zhiyong Chn Institut of Wirlss Communications Tchnology Shanghai Jiao Tong Univrsity China Lctur 5- Nov. 05 0 Classical Information Thory Sourc
More information1 Minimum Cut Problem
CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms
More informationarxiv: v2 [cs.dm] 17 May 2018
Inhritanc of Convxity for th P min -Rstrictd Gam arxiv:708.0675v [cs.dm] 7 May 08 A. Skoda July 6, 08 Abstract W considr rstrictd gams on wightd graphs associatd with minimum partitions. W rplac in th
More informationOn the irreducibility of some polynomials in two variables
ACTA ARITHMETICA LXXXII.3 (1997) On th irrducibility of som polynomials in two variabls by B. Brindza and Á. Pintér (Dbrcn) To th mmory of Paul Erdős Lt f(x) and g(y ) b polynomials with intgral cofficints
More informationFigure 1: Closed surface, surface with boundary, or not a surface?
QUESTION 1 (10 marks) Two o th topological spacs shown in Figur 1 ar closd suracs, two ar suracs with boundary, and two ar not suracs. Dtrmin which is which. You ar not rquird to justiy your answr, but,
More informationNEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA
NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals
More informationLINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM
Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL
More informationThe second condition says that a node α of the tree has exactly n children if the arity of its label is n.
CS 6110 S14 Hanout 2 Proof of Conflunc 27 January 2014 In this supplmntary lctur w prov that th λ-calculus is conflunt. This is rsult is u to lonzo Church (1903 1995) an J. arkly Rossr (1907 1989) an is
More informationDirect Approach for Discrete Systems One-Dimensional Elements
CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:
More informationLecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.
Lctur 2: Discrt-Tim Signals & Systms Rza Mohammadkhani, Digital Signal Procssing, 2015 Univrsity of Kurdistan ng.uok.ac.ir/mohammadkhani 1 Signal Dfinition and Exampls 2 Signal: any physical quantity that
More informationPropositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018
Propositional Logic Combinatorial Problm Solving (CPS) Albrt Olivras Enric Rodríguz-Carbonll May 17, 2018 Ovrviw of th sssion Dfinition of Propositional Logic Gnral Concpts in Logic Rduction to SAT CNFs
More informationOn Grids in Topological Graphs
On Grids in Topological Graphs Eyal Ackrman Dpartmnt of Computr Scinc Fri Univrsität Brlin Takustr. 9, 14195 Brlin, Grmany yal@inf.fu-brlin.d Jacob Fox Dpartmnt of Mathmatics Princton Univrsity Princton,
More informationANALYSIS IN THE FREQUENCY DOMAIN
ANALYSIS IN THE FREQUENCY DOMAIN SPECTRAL DENSITY Dfinition Th spctral dnsit of a S.S.P. t also calld th spctrum of t is dfind as: + { γ }. jτ γ τ F τ τ In othr words, of th covarianc function. is dfind
More informationFourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.
Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform
More informationA Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes
Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical
More informationHardy-Littlewood Conjecture and Exceptional real Zero. JinHua Fei. ChangLing Company of Electronic Technology Baoji Shannxi P.R.
Hardy-Littlwood Conjctur and Excptional ral Zro JinHua Fi ChangLing Company of Elctronic Tchnology Baoji Shannxi P.R.China E-mail: fijinhuayoujian@msn.com Abstract. In this papr, w assum that Hardy-Littlwood
More informationSlide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS
Slid DIGITAL SIGAL PROCESSIG UIT I DISCRETE TIME SIGALS AD SYSTEM Slid Rviw of discrt-tim signals & systms Signal:- A signal is dfind as any physical quantity that varis with tim, spac or any othr indpndnt
More informationQuasi-Classical States of the Simple Harmonic Oscillator
Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats
More information3 Finite Element Parametric Geometry
3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,
More informationA Propagating Wave Packet Group Velocity Dispersion
Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to
More informationON THE DISTRIBUTION OF THE ELLIPTIC SUBSET SUM GENERATOR OF PSEUDORANDOM NUMBERS
INTEGERS: ELECTRONIC JOURNAL OF COMBINATORIAL NUMBER THEORY 8 2008, #A3 ON THE DISTRIBUTION OF THE ELLIPTIC SUBSET SUM GENERATOR OF PSEUDORANDOM NUMBERS Edwin D. El-Mahassni Dpartmnt of Computing, Macquari
More informationDivision of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.
Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions
More informationu 3 = u 3 (x 1, x 2, x 3 )
Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.
More informationExponential inequalities and the law of the iterated logarithm in the unbounded forecasting game
Ann Inst Stat Math (01 64:615 63 DOI 101007/s10463-010-03-5 Exponntial inqualitis and th law of th itratd logarithm in th unboundd forcasting gam Shin-ichiro Takazawa Rcivd: 14 Dcmbr 009 / Rvisd: 5 Octobr
More informationChapter 6 Folding. Folding
Chaptr 6 Folding Wintr 1 Mokhtar Abolaz Folding Th folding transformation is usd to systmatically dtrmin th control circuits in DSP architctur whr multipl algorithm oprations ar tim-multiplxd to a singl
More informationApplication of Vague Soft Sets in students evaluation
Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt
More informationCLONES IN 3-CONNECTED FRAME MATROIDS
CLONES IN 3-CONNECTED FRAME MATROIDS JAKAYLA ROBBINS, DANIEL SLILATY, AND XIANGQIAN ZHOU Abstract. W dtrmin th structur o clonal classs o 3-connctd ram matroids in trms o th structur o biasd graphs. Robbins
More informationMutually Independent Hamiltonian Paths in Star Networks
Mutually Independent Hamiltonian Paths in Star Networks Cheng-Kuan Lin a, Hua-Min Huang a, Lih-Hsing Hsu b,, and Sheng Bau c, a Department of Mathematics National Central University, Chung-Li, Taiwan b
More informationCategory Theory Approach to Fusion of Wavelet-Based Features
Catgory Thory Approach to Fusion of Wavlt-Basd Faturs Scott A. DLoach Air Forc Institut of Tchnology Dpartmnt of Elctrical and Computr Enginring Wright-Pattrson AFB, Ohio 45433 Scott.DLoach@afit.af.mil
More information1 N N(θ;d 1...d l ;N) 1 q l = o(1)
NORMALITY OF NUMBERS GENERATED BY THE VALUES OF ENTIRE FUNCTIONS MANFRED G. MADRITSCH, JÖRG M. THUSWALDNER, AND ROBERT F. TICHY Abstract. W show that th numbr gnratd by th q-ary intgr part of an ntir function
More informationGeneral Caching Is Hard: Even with Small Pages
Algorithmica manuscript No. (will b insrtd by th ditor) Gnral Caching Is Hard: Evn with Small Pags Luká² Folwarczný Ji í Sgall August 1, 2016 Abstract Caching (also known as paging) is a classical problm
More informationOn the number of pairs of positive integers x,y H such that x 2 +y 2 +1, x 2 +y 2 +2 are square-free
arxiv:90.04838v [math.nt] 5 Jan 09 On th numbr of pairs of positiv intgrs x,y H such that x +y +, x +y + ar squar-fr S. I. Dimitrov Abstract In th prsnt papr w show that thr xist infinitly many conscutiv
More informationTOPIC 5: INTEGRATION
TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function
More informationSpectral Synthesis in the Heisenberg Group
Intrnational Journal of Mathmatical Analysis Vol. 13, 19, no. 1, 1-5 HIKARI Ltd, www.m-hikari.com https://doi.org/1.1988/ijma.19.81179 Spctral Synthsis in th Hisnbrg Group Yitzhak Wit Dpartmnt of Mathmatics,
More informationTwo Products Manufacturer s Production Decisions with Carbon Constraint
Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint
More informationON RIGHT(LEFT) DUO PO-SEMIGROUPS. S. K. Lee and K. Y. Park
Kangwon-Kyungki Math. Jour. 11 (2003), No. 2, pp. 147 153 ON RIGHT(LEFT) DUO PO-SEMIGROUPS S. K. L and K. Y. Park Abstract. W invstigat som proprtis on right(rsp. lft) duo po-smigroups. 1. Introduction
More informationOuterplanar graphs and Delaunay triangulations
CCCG 011, Toronto ON, August 10 1, 011 Outrplanar graphs and Dlaunay triangulations Ashraful Alam Igor Rivin Ilana Strinu Abstract Ovr 0 yars ago, Dillncourt [1] showd that all outrplanar graphs can b
More informationSearch sequence databases 3 10/25/2016
Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an
More informationThat is, we start with a general matrix: And end with a simpler matrix:
DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss
More informationGEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia
GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES Eduard N. Klnov* Rostov-on-Don, Russia Th articl considrs phnomnal gomtry figurs bing th carrirs of valu spctra for th pairs of th rmaining additiv
More informationSymmetric centrosymmetric matrix vector multiplication
Linar Algbra and its Applications 320 (2000) 193 198 www.lsvir.com/locat/laa Symmtric cntrosymmtric matrix vctor multiplication A. Mlman 1 Dpartmnt of Mathmatics, Univrsity of San Francisco, San Francisco,
More informationAbstract Interpretation: concrete and abstract semantics
Abstract Intrprtation: concrt and abstract smantics Concrt smantics W considr a vry tiny languag that manags arithmtic oprations on intgrs valus. Th (concrt) smantics of th languags cab b dfind by th funzcion
More informationObjective Mathematics
x. Lt 'P' b a point on th curv y and tangnt x drawn at P to th curv has gratst slop in magnitud, thn point 'P' is,, (0, 0),. Th quation of common tangnt to th curvs y = 6 x x and xy = x + is : x y = 8
More informationA. Limits and Horizontal Asymptotes ( ) f x f x. f x. x "±# ( ).
A. Limits and Horizontal Asymptots What you ar finding: You can b askd to find lim x "a H.A.) problm is asking you find lim x "# and lim x "$#. or lim x "±#. Typically, a horizontal asymptot algbraically,
More informationECE602 Exam 1 April 5, You must show ALL of your work for full credit.
ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b
More informationChapter 10. The singular integral Introducing S(n) and J(n)
Chaptr Th singular intgral Our aim in this chaptr is to rplac th functions S (n) and J (n) by mor convnint xprssions; ths will b calld th singular sris S(n) and th singular intgral J(n). This will b don
More informationREPRESENTATIONS OF LIE GROUPS AND LIE ALGEBRAS
REPRESENTATIONS OF LIE GROUPS AND LIE ALGEBRAS JIAQI JIANG Abstract. This papr studis th rlationship btwn rprsntations of a Li group and rprsntations of its Li algbra. W will mak th corrspondnc in two
More informationON A CONJECTURE OF RYSElt AND MINC
MA THEMATICS ON A CONJECTURE OF RYSElt AND MINC BY ALBERT NIJE~HUIS*) AND HERBERT S. WILF *) (Communicatd at th mting of January 31, 1970) 1. Introduction Lt A b an n x n matrix of zros and ons, and suppos
More informationUNTYPED LAMBDA CALCULUS (II)
1 UNTYPED LAMBDA CALCULUS (II) RECALL: CALL-BY-VALUE O.S. Basic rul Sarch ruls: (\x.) v [v/x] 1 1 1 1 v v CALL-BY-VALUE EVALUATION EXAMPLE (\x. x x) (\y. y) x x [\y. y / x] = (\y. y) (\y. y) y [\y. y /
More informationCPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming
CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of
More informationSeparating principles below Ramsey s Theorem for Pairs
Sparating principls blow Ramsy s Thorm for Pairs Manul Lrman, Rd Solomon, Hnry Towsnr Fbruary 4, 2013 1 Introduction In rcnt yars, thr has bn a substantial amount of work in rvrs mathmatics concrning natural
More informationStochastic Submodular Maximization
Stochastic Submodular Maximization Arash Asadpour, Hamid Nazrzadh, and Amin Sabri Stanford Univrsity, Stanford, CA. {asadpour,hamidnz,sabri}@stanford.du Abstract. W study stochastic submodular maximization
More informationEquidistribution and Weyl s criterion
Euidistribution and Wyl s critrion by Brad Hannigan-Daly W introduc th ida of a sunc of numbrs bing uidistributd (mod ), and w stat and prov a thorm of Hrmann Wyl which charactrizs such suncs. W also discuss
More informationHomogeneous Constant Matrix Systems, Part I
39 Homognous Constant Matrix Systms, Part I Finally, w can start discussing mthods for solving a vry important class of diffrntial quation systms of diffrntial quations: homognous constant matrix systms
More informationMATHEMATICS (B) 2 log (D) ( 1) = where z =
MATHEMATICS SECTION- I STRAIGHT OBJECTIVE TYPE This sction contains 9 multipl choic qustions numbrd to 9. Each qustion has choic (A), (B), (C) and (D), out of which ONLY-ONE is corrct. Lt I d + +, J +
More informationMATRIX FACTORIZATIONS OVER PROJECTIVE SCHEMES
MATRIX FACTORIZATIONS OVER PROJECTIVE SCHEMES JESSE BURKE AND MARK E. WALKER Abstract. W study matrix factorizations of locally fr cohrnt shavs on a schm. For a schm that is projctiv ovr an affin schm,
More informationDynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *
17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High
More informationINCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS. xy 1 (mod p), (x, y) I (j)
INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS T D BROWNING AND A HAYNES Abstract W invstigat th solubility of th congrunc xy (mod ), whr is a rim and x, y ar rstrictd to li
More informationInternational Journal of Foundations of Computer Science c World Scientic Publishing Company Searching a Pseudo 3-Sided Solid Orthoconvex Grid ANTONIO
Intrnational Journal of Foundations of Computr Scinc c World Scintic Publishing Company Sarching a Psudo 3-Sidd Solid Orthoconvx Grid ANTONIOS SYMVONIS Bassr Dpartmnt of Computr Scinc, Univrsity of Sydny
More information