Temporal Difference Methods and Approximate Monte Carlo Linear Algebra

Size: px
Start display at page:

Download "Temporal Difference Methods and Approximate Monte Carlo Linear Algebra"

Transcription

1 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon empal Dfference Mehod and Appromae Mone Carlo Lnear Algebra Dmr P. Bereka Deparmen Elecrcal Engneerng and Compuer Scence Maachue Inue echnology RL Wkhop, Llle 8

2 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Focu Appromae oluon lnear equaon (, where ( A b, A n n, b R n by olvng he proeced equaon y Π (y Π proecon on a ubpace ba funcon (wh repec o ome nm h he Galerkn appromaon approach, bu mulaon play a cenral and non-radonal role. We conder very large n. Sarng pon: Appromae DP/Bellman equaon/polcy evaluaon A : encode he chan rucure, b : co vec hen y Π (y he equaon olved by D mehod [D(λ, LSD(λ, LSPE(λ] We generalze o he cae where A arbrary, ubec only o I ΠA : nverble (on wk wh H. Yu - paper avalable from our web e

3 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Benef and Challenge Generalzaon A hgher perpecve f D mehod n appromae DP Movae mprovemen n varou area: Eplaon ue Auomac generaon feaure bound Smplfed convergence analy An eenon o a va new area applcaon here are many lnear yem huge dmenon n pracce Dealng wh le rucure Lack conracon Abence a chan Ill-condonng

4 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Oulne Proeced Equaon Appromaon he Appromae DP Cone he General Proeced Equaon Cone General LSD and LSPE-ype Alghm Fm he Alghm Choce f a Conracon Auomac Generaon Feaure Mulep Veron - λ-mehod 3 Eenon onlnear Eenon Lea Square/Bellman -ype Mehod

5 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon DP Cone/Polcy Evaluaon an Decon Problem (MDP n ae, ranon probable dependng on conrol Polcy eraon mehod; we focu on ngle polcy evaluaon Bellman equaon: A b where b: co vec A ha ranon rucure, e.g., A αp f dcouned problem, A P f average co problem

6 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Appromae Polcy Evaluaon Appromaon whn ubpace S { r R }, Φ a mar wh ba funcon a column Proeced Bellman equaon: Π(A b bound, aumng ΠA conracon wh modulu α (, α Π Long hy, arng wh D(λ (Suon, 988 Lea quare mehod are currenly me popular

7 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Lea Square Polcy Evaluaon (LSD Dae o 996 (Bradke and Baro, wh λ-eenon by Boyan ( Idea: Solve a mulaon-baed appromaon he proeced equaon he proeced Bellman equaon wren a Cr d LSD olve Ĉr ˆd, where are obaned ung mulaon Ĉ C, ˆd d Doe no need he conracon propery DP problem Mulep veron: LSD(λ whch LSD appled o he mappng (λ ( ( λ λ k k ( A (λ b (λ, k where A (λ ( λ λ k A k, b (λ λ k A k b k k

8 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Proeced Value Ieraon (PVI Value Ieraon > Proecon > Value Ieraon > Proecon... (Φ S an Squar Proecon on on S o mal Subpace S ( Φ Π Π r Condonal Mea Π Π mu be a conracon - beng a conracon no enough m machng eenal: a (Eucldean proecon nm f whch a conracon here a magcal nm: he eady-ae drbuon nm (ae are weghed by he eady-ae drbuon he chan

9 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Lea Square Polcy Evaluaon (LSPE Π Subpace S Π Subpace S ( Π Subpace S Proecon on S mal ( Π θ Condonal Subpace S Proecon on Emaon S θ Condonal Emaon mal Π Π noe wh noe wh θ Condonal Emaon mal θ Condonal Emaon mal k k k k noe wh k k k k k k k k noe wh f (z z f (z z PVI LSPE Z PVI Z o ξ (May UeLSPE Q oy Π Subpace S Proecon on S Subpace S Proecon on S ( foy ( Π opue P A Q Z (z z o ξ (May Ue Q o Probably o ξ (May fzprobably (z z Π Condonal θ Emaon ( Subpace S Emaon Proecon ( Π Subpace SonProecon on SPmal θ Condonal on S(mal Π Subpace Sranmed Proecon S oy Recever Sgnal Regon ranmed oy Recever Regon o P A osgnal P P A Probably noe wh Probably noe θ Condonal Emaon mal θ Condonal wh Emaon Π mal Π " ranmed ranmed ( S Proecon on S oy Recever ranmed Recever (Sgnal Regon Π Subpace S Proecon on S Sgnal Regon Subpace ranmed noe wh oy noe wh ( Π Subpace S Proecon on S θ Condonal Emaon mal ranmed Π " f Π " f (z z... ranmed z Z k k k k Z (z noe Π wh θmal Emaon mal fz (z θzcondonal fcondonal (z z o ξ (May Ue Q f < f Probably f < Emaon f mal θ Condonal Emaon Probably Z noe wh o P P A noe wh Probably noe wh oy Recever ranmed fz (z Probably z oy Recever ranmed Sgnal Regon f ( f S Proecon on S Π < Sgnal fregon < Π f S Proecon ( Subpace on S ( ranmed Π Subpace Subpace S Proecon on S Recever ranmed oy Recever Sgnal Regon ranmed oy Sgnal Regon ranmed Π f(z Π Probably f (z Π fz z Z (z Z z ranmed Subpace S ranmed ZEmaon µ mal Subpace θ Condonal Emaon mal aθ Condonal a b A f { A} ( f ( y Π µ b A f { A} ( f (Recever y Π µsgnal,sµy µy y (µ, µy Regon y y (µ Condonal Emaon mal zero-m oy θ ranmed θ Condonal Emaon mal θ Condonal Emaon mal Probably noe wh noe Probably wh Probably noe wh ranmed f < f y f < f a b A f ( f ( y µ µ y (µ, µy wh a hrehold noe wh ranmed Sgnal { A} Se E par Efficennoe Froner Selecon k ( Se E oy Froner hrehold k b A f { A} f ( par y µ Sgnal µrecever (µ Selecon Efficen y y Regon, µyregon oy Recever Sgnal Regon ranmed oy Recever ranmed f < f ranmed f < f fz (z z fz (z z fz (z kz (z ranmed Seg E fzpar z Efficen (zranmed zefficen Froner Selecon hrehold α β g( H g( H f (d α βselecon g( Hhrehold Seg E fzpar Froner kh f (d g( f < f Probably Probably Probably Probably A Probably A a b Proce f { A} ( ( µy y (µregon a b Proce f { A} ( f ( y µ Poble Recever Sgnal y (µregon, µy Calculaon, µy ranmed µyobervaon Space Poble Obervaon Calculaon Poer Space Poer oy ranmed αfβoy g( y HµRecever g( HSgnal g f (d f < f α β g( H g( H f (d g Sgnal ranmed oy Recever Regon Recever b AfRecever ( fregon ( y µp ranmed a b A f { A} f ( y µ oy µy yranmed (µ, µy Sgnal Regon ranm ( µ y y (µ,µ y { A} pθ ( P(Θ oy ka P(Θ k P(Θ ( ksgnal ranmed ranmed Selecon Calculaon f hrehold Proce < Poer f Θ P(Θ f kk < Se EfSpace Efficen ranmed par Froner k ranmed Poble Obervaon Se E Space par Efficen PobleFroner Obervaon Selecon Calculaonhrehold Proce Poer. Froner Se E par Efficen hrehold k k Se E par Efficen pθ (..Froner P(Θ Selecon k hrehold P(Θ k k P(Θ Selecon p kaθp(θ ( ;fθ p ( ; θ p ( ; θ p ( ; θm p (; θ p (;pθ θm ( α.. β g( ( ; p ( ; θ p (; θ p (; θ. A ( f ( y µ µ (µ, µ b p m m y y y α β g( H g(h f (d g < f H g( H f (d g { A} f f < f f ( y µα µ. y y (µ, µyf { A} ( < f H elecon H < g f α βf g( H Hypohe g( fa(db g AΘ f (d ( ; Hypohe elecon Θ Θ Space Θ Poer.. Space β fg( f θ p( ;Obervaon θpg( ( ; θ ph (; θ ppoer (; θm.. < f m p Calculaon Poble p ( ;Obervaon θ p ( ; θ pcalculaon ( ; θm Se p (; θ par p (; θeffcen m. EProce Froner Poble Selecon hrehold k Proce bp(θ fcalculaon ( a bcalculaon ( ( Froner y µppoble ( Selecon µay A P(Θ { A} yk y (µ,kµ f ( k y µ µy y (µ, µy Space ppoble Proce Space Obervaon Proce Poer { A} ( Obervaon P(Θ A fk P(Θ Poer par fkefficen SeE hrehold Θ fs (; H p ( ; θ p ( ; θm p (; θθ p (; θm elecon Θ Θ fs (; H p ( ; θ p ( ; θm p (; θhypohe p (; θm elecon Θ Θ pθ ( Hypohe P(Θ k P(Θ k pθ ( P(Θ k P(Θ k γ.α βy µg( H g( H f (d a gb Ak f { A}Froner ( f (.. y µ Selecon µy y (µhrehold, µy a bpar A f { A} ffroner f µyselecon (, µpe ghrehold k g( y f(µ y α(βnerval ph fθ( Effcen a b Aecf { A} ( fθ( Se yrule,( µ(; a b AH µp ( ;θmeffcen θymθ(µ, (; µ(; ( ;Se (d ( ;yθpar µpyp( ; (; pp. θm y θm p ( ; ( yh ; θµepp ( ;θdecon yp θ(µ pconfdence.. g( p mµ Decon Rule Confdence nerval (;.y θθm p (; fs (; p (; θm ec { A} fs(; H p ( ;aθ ( ; θ p ( ; θm p (;...θpoble f θm.. ( f ( y µ µy y (µ, µy Obervaon p ( ; θ p ( ; θ p ( ; θm p (; θ pspace (;Space θm Poble p ( ; θ pcalculaon ( ; θ p ( ; θmproce p (; θbpoer pa (; { A} Obervaon Calculaon Proce Poer Se E par Efficen Hypohe elecon Θ Θ Se E par Efficen Froner Selecon hrehold k Hypohe elecon Θ Θ Froner Selecon hrehold k Seξ E par Efficen Froner Selecon hrehold k SeP(Θ E par Efficen Froner Selecon hrehold kh p ( k P(Θ k γ α β g( g( H f (d g Decon Rule Confdence nerval ec γ α β g( H g( H f (d g Θ v log / v log ξ / pθ ec ( P(Θ elecon k P(ΘΘ Θ Hypohe elecon Decon Θ Θ Rule Confdence nerval Hypohe k Se E par Efficen Froner Selecon hrehold k (; α θβ pg( H g( H f (dproce g fs (; ( ; θ ph( ; θfm(d.pobervaon fs (;HH pg( ( ; θ ph( ; θfm pg (;αθβ pml (; θmh g( H fα (d (;θm g( Emae ML Emae Emae Space Calculaon Poer α β g( β gg( HH p g( (demae Space Poble Obervaon Calculaon Proce Poer.Poble.. pgξ(;/ / fs (; H p ( ; θ p ( ; θm p (;vθlog θpm( ; (; ( ; θ θθpm θ..m(; pθm (; vθlog θm pθ( ; ;( ; θθm pfsp( ; θhmθpp (; p pξ(; ( ; ( pθ ( ;pθ p (; pp (; ( Proce P(Θ α kcalculaon P(Θ Proce HPoer Space Poble p ( P(Θ k P(Θ k Θ Obervaon β g( H g( fk Space Poble Obervaon Calculaon Proce Poer (d g Θ Decon Rule Confdence nerval ec Poer Poble Obervaon Calculaon Proce Poer Space Poble Obervaon Calculaon Decon Rule Confdence nerval ec p ( ; H p ( ; H pspace (; θ p ( ; H p ( ; H p ( ; θ p (; θ p (; θ Emae ML Emae m m m ( ; θm p (; θ p p ( P(Θ k P(Θ k ML pec Emae Θ Hypohe k P(Θ ΘpΘ kθdecon P(Θ Rule Confdence k nerval elecon P(Θ elecon Θ pθ (Decon P(Θ Emae nerval k P(Θ (Hypohe ( Θ k P(Θec k Rule Confdence Θ Poble Obervaon Calculaon Proce.. Poer.vlogSpace H H umber head k Θ, Obervaon Pr pθ H umber head k Θ, Obervaon Prp pθ( ; ξ p / v logh ξ / ;θθ ( ;θθ m p (; p ( θm ; H p.. ( θp; H p( ( ( ;. pp p(; θ θk P(Θ θ p. ( θθp p( ; θm p (; θ p..(; m m(; (; P(Θ p θ..m.k p ( v ;log Hξ pf ( p;h( ; p;(; Θ p( ; θm m p( ; pθ(; θ p pp(; (; Θ θpθ θ ( ; θm;mθ (; θm (; (; ( ; (; / θfsh p(; θ( ; θ pp.p( ; m θm ( ; ( ;H p ( ; θ p ( Emae ; θ p ( ;ML θm Emae p (;Θ/ θ pp(; θmθ p.. ( fs; (; p( ; θvmlog pξp(; θ θpmp(;( ;θθm p.. ( ; θ p ( ; θm p (; θ p (; θm. ( θ Emae ML Emae H H umber head k Θ,ΘObervaon Pr pθ Hypohe elecon Θ Hypohe elecon Θ Θ H H umber head k Θ, Obervaon Pr p. Emae Θ Emae ML Hypohe elecon Θ Θ Emae Hypohe elecon Θ Rule Θ Hypohe Hypohe elecon elecon ΘΘ ML Θ Emae fec Decon Confdence nerval p ( ; θ p ( ; θ p ( ; θm p (; θ p (; θm.. Decon Rule Confdence nerval fθθ p Θ p ( ec ; H p ( ; H p ( ; θm p (; θ p (; θm ( ; H p ( ; H p ( ; θm p (; θ p (; θm fhypohe p(; ( ; p pp (; (;θ θp p(;θ(; Condonal p Θ f Θ Pon Emae Analy pp f Θp Pon pfθs(; mθ (;θsh θ θemae S (; pp θ( ; mθp( (; θm θm(; ( ;H ( ; p ( p;h( ; θpm ( ; (;θpmh(; θ ( (; ;H(; ( ; pθh pθh (; θ pθ ( ; θ( ; pθ( ; ec m θpfcondonal m( ; ec mf(; S(; H m m θm pθ ( ; θ( ; p θpanaly fs (;ph ph θumber pθ(; p; H θpm ps (; (; Θ m pv m m Θ ( ; elecon / ph umber head kθ, Obervaon ΘPr p H head k Θ,pf(; Obervaon p( ;Pr plog ξθh A mulaon-baed appromaon o PVI Dae o 996 (Bereka and Ife; alo n he Bereka and kl (996 book - ued n a er applcaon LSPE: mulaon noe wh Π, {z } PVI Incremenal lke D(λ - no epze unlke D(λ Same compley/ame oluon a LSD Aympocally dencal" o LSD, bu dffer n early age Allow f a favable nal gue r ; may be an advanage n opmc/few ample appromae polcy eraon Θ f ξ / v log Θ

10 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Advanage Proeced Equaon Mehod n DP All operaon are done n low-dmenon he hgh-dmenonal vec need no be ed he proecon nm mplemened n mulaon - need no be known a pr here a proecon nm (he drbuon nm ha nduce conracon ΠA and a pr bound

11 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon General/onDP Proeced Equaon Mehod A doe no have a ranon probably rucure o chan, no conracon guaranee We may nroduce an arfcal chan f amplng/proecon Wh clever choce he chan, ΠA may be a conracon Compuable bound are avalable All operaon are done n low-dmenon he hgh-dmenonal vec need no be ed Mehod: LSD analog (doe no requre ΠA o be a conracon LSPE analog (requre ΠA o be a conracon D(λ analog (requre ΠA o be a conracon

12 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Proeced Equaon Appromaon Mehod (LSD-lke Le Π be proecon wh repec o v u ξ n ξ, where ξ R n a probably drbuon wh pove componen Eplc fm proeced equaon Π(A b n n r arg mn r a φ( r b A r R where φ( denoe he h row he mar Φ Opmaly condon/equvalen fm: n n ξ a φ( A r {z } Epeced value n ξ φ(b {z } Epeced value he wo epeced value are appromaed by mulaon

13 Proeced Equaon Appromaon noe General LSD and LSPE-ype Alghm Eenon Smulaon Mechanm o ξ (May Ue Q o P A Π Subpace S Proecon on S ( k k k k... k k k k k.k kkk k. k k k k kk k k k. k k k k(may k... Π ξ oξ ξ Ue Q o ξ (May Ue oue ξ (May Ue o ξ (May Q Ue Q Q o o ξ (May o (May Q Ue Ch o ξ (May Ue θ Condonal Emaon o A o o P A o P mal A P A P o P noe wh ( Π S SΠ o osubpace PSubpace P S S Proecon ( A Subpace Proecon on ( Π ( Π Subpace Π Proecon on S on S Proecon S ( S on S ( Π Subpace S Proec Π Π Π Π Π S Π Subpace ( on Subpace S Proecon ( kkk k fz S Π kproecon zk k k Π k(z k k θ k k k k Condonal Squar θ Condonal Emaon mal ze θ Condonal θ k Condonal θ Condonal Emaon Emaon mal Emaon mal mal o ξ (May o Ue ξ (May Ue Q θ Condonal Emaon Erro o ξ (May Ue Q o ξ (May Ue Q noe Π Π noe wh Q wh wh noe wh Probably noe wh noe o A P A noe wh o P o A P o P A θ Condonal θrecever Emaon mal Emaon oy Sgnal Regon ξ, ranmed amplng: equence {Π Proecon,...} o.e., Condonal Π,S ( ( Π accdng Subpace Proecon S Proecon S Proecon on S on S f ( Subpace S on S (Generae Π Subpace on S fsubpace Z( f z Π fz (z zπ fz(z z Z (z z Z (z ranmed wh noe wh Π f (z z relave frequency each row ξ Π Z Probably θ Condonal θ Condonal Emaon Emaon mal mal zer Probably θcondonal Emaon mal Probably θ Condonal Emaon mal Probably equence Probably amplng: Generae (,,..oy. accdng o Sgnal,,Probably Recever ( wh noe wh noe noe Recever wh noe wh oy Recever Sgnal ra oy oy Sgnal oy Recever Regon Sgnal Recever Regon Sgnal Regon ranmed Regon ranmed ranmed f < f z oy Sgnal Regon wh ranmed ome ranon mar (z zp wh frecever Z Z (z ranmed ranmed probably ranmed f ranmed f ranmed fz (z z fz (z z Z (z z fz (z z p >Probably f a, 6 Probably f Probably Probably Probably Probably a b A f ( f ( y µ µy (µ, µy f f < f yf< f < f < f f { A} franmed < ranmed f ran oy oy Recever Sgnal Recever Regon Sgnal Regon oy.e., Recever Sgnal oy Regon Recever Sgnal Regon ranmed oy Recever Sgnal Regon oy Recever Sgnal Regon ranmed f each, he relave frequency (, p ranmed Froner ranmed ranmed ranmed Se E par Effcen Selecon hrehold k ranmed ranmed amplng may be done ung a chan wh ranon mar a b A f { A} ( f ( γ α β g( H g( H f (d g Q (unrelaed o P b A fy { A} y (µ µy a b A f a b A ( f f a(b ( A yffaµ( ( µyµf ( µfy,yµ( y (µ y, µµµyy, µ y( (µ yµ y y (µ, µ f { A} { A} b f ( yµ µy < A f< { A} f f( < par f Frone f { A} f f E < fa Se Effcen Spacealo Poble Obervaon Proce- Poer amplng may be done whouacalculaon chan u ample Se E Effcen Effcen Froner EEffcen par Froner Se par Selecon Froner hrehold Selecon khrehold Selecon k Selecon hrehold k ( f Se E par Sep ome Effcen EP(Θ <drbuon Froner par fk fpar Effcen k < Froner f β g( hrehol Θ Se E Selecon row accdng o known ξp(θ (e.g., a unfm γ α H

14 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon and o ξ (May Ue Q w o ξ (May Ue Q o P A ( P Π A Subpace S Proecon on S umn o Accdn Π on ( Π Subpace S Proecon S Π k k k... mal k k k k k θk Condonal kk.k kk k k. k k Emaon k k k k k k. Acc o ξ (May Ue M oue ξ (May Ue o ξ(may (May Ue oue ξ (May Ue o ξ (May Q Q ( QCha Marko (May Π Ch ( noe Emaon wh o ξ o Q o o ξξ(may Ue Ue θ Condonal mal o P A o o A o P Π A A P P Π ( Subpace S P o P A wh ξ (May Ue Q o o osubpace PSubpace A S o Proecon ( Subpace ( Π ( Π ( Subpace Π Proecon SΠ on S on S Proecon S Condonal on S Subpace z Π S Proecon (fz(z Π on Pθ Proecon o S A Π Π Π Π Π Subpace ( ( S Π Proecon on Subpace S S Proec noe wh θ Condonal Emao Π f (z z k k k k k k k k Z ( Π Subpace S Proecon on S k k k k kk Probably θnoe Condonal Emaon o θ Condonal k θ k Condonal θ Condonal Emaon Emaon mal Emaon mal mal zero wh o (May Ue Qm θsgnal Condonal Emaon (May Ue Q ξ ξπ (May Ue Q Π Recever Π ξ o (May o Ue ξ ranmed noe wh Probably noe wh noe oy wh noe wh o Regon o P A P A noe wh P o P o A mal θ Condonal Emaon o A ranmed y Recever Sgnal Regon ranmed θ Condonal θ Emaon mal Emaon Subpace Subpace Condonal fzproecon (z Π ( Π ( ( Proecon Π S Proecon S on Sz Err on (wh SSubpace S Proecon on SProbably noe Π Subpace on S Err amplng Sae Sequence Generaon n DP. Affec: ranmed fz (z z f z Π fz (z zπ fz(z z (z Z (z f z wh noe wh Z Π Π oy Recever Probably he proecon nm θ Condonal Condonal mal zero-m m Emaon (z Probably θcondonal Probably femaon θ f fz Emaon mal Emaon Sgnal Probably θ Condonal Probably mal <oy Z ranmed Recever Regon err Probably Wheher ΠA a conracon noe wh noe wh noe wh noe wh oy Recever Sgnal Regon oy oy Recever Sgnal oy Recever Regon Sgnal Recever Regon Sgnal Regon ranmed ranmed ranm f < f Probably ranmed oy Recever Sgnal Regon f z Z (z Z (z amplng ranon Sequence Generaon nfdp. Canzbe ranmed ranmed ranmed ranmed ranmed oy Recever Sgnal Regon ranmed fz (z Affec: z fz (z z fz (z z fz (z z oally unrelaed o rowamplng. ranmed a b A f { A} ( f ( y µ µy y (µ, µy f < f Probably Probably he amplng/mulaon Probably Probably Probably Probably b A f { A} ( f ( µynoe, µf yf y < f < k Machng Se y µ f < oy (µ Recever < f f f< f famplng Sgnal f P wh A ha an effec lke n mpance E par Effcen Froner oy Recever Sgnal Recever Regon hrehold Regon ranm oy Recever Sgnal oy Regon Sgnal Regon w oy Recever Sgnal Regon Selecon ranmed ranmed oy Recever Sgnal Regon ranmed f < f ranmed ranmed ranmed E par Effcen Selecon hrehold k a b A f ( f Froner ranmed ranmed ranmed { A}

15 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon LSD-Lke Mehod Opmaly condon/equvalen fm proeced equaon n n n ξ a φ( A r ξ φ(b {z } Epeced value {z } Epeced value he wo epeced value are appromaed by row and column amplng (bach A me, we olve he lnear equaon hen r r k φ( k φ( k a «k k φ( k r p k k φ( k b k k

16 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Conder PVI LSPE-ype Mehod Π(A b,,,... Epreng he proecon a a lea quare mnmzaon, we have equvalenly r r arg mn r R (A b ξ,! n ξ φ(φ( {z } Epeced value n n ξ a φ( r b A {z } Epeced value Appromae he wo epeced value by row and column amplng r! φ( k φ( k k k φ( k ak k p k k φ( k r b k If ΠA a conracon wh repec o ome nm, r r «

17 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon f Conracon I Mu have Sum A o have hope conracon ΠA Propoon: Le ξ be he nvaran drbuon an rreducble Q uch ha A Q hen and Π are conracon mappng under any one he followng hree condon: ( F ome calar α (,, we have A αq. ( here e an nde ī uch ha aī < q ī f all,..., n. (3 here e an nde ī uch ha P n aī <. oe : Under condon ( and (, and Π are conracon mappng wh repec o he pecfc nm ξ oe : Apple o DP dcouned and ochac he pah problem

18 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon f Conracon II Mu have Sum A Propoon: Le ξ be he nvaran drbuon a Q wh no ranen ae. Aume A Q and ha I ΠA nverble. hen he mappng Π γ, where γ ( γi γ, a conracon wh repec o ξ f all γ (,. oe : Π γ and Π have he ame fed pon oe : Π need no be a conracon oe 3: Apple o average co problem (Yu and Bereka 6

19 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Back o Dcouned DP/Eplaon Here A αp, where P crepond o he polcy evaluaed and α he dcoun fac If we ake Q P f row amplng, hen ΠA a conracon We may alo ue chan Q P f row amplng, o change ξ and nduce eplaon; f eample ue Polcy R (f polcy prob. β, Polcy P (on polcy prob. β he LSD-ype alghm alway apple ( doe no requre ha ΠA be a conracon If ΠA can be hown o be a conracon, he LSPE(λ- and D(λ-ype alghm apply. In parcular, we ge convergence wh no ba f: ( F all λ [, f β α ( F all β [, f λ uffcenly large

20 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Applcaon o Dagonally Domnan Syem Conder he oluon he yem C d, where d R n and C an n n mar uch c, c c,,..., n Conver o he yem A b, where b d c ( f We have a n a o row um A c c f and c,,..., n, c Under he earler condon, ΠA a conracon.

21 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Auomac Generaon Power A a Ba Funcon Ue Φ whoe h row where g ome vec φ( `g( (Ag( (A g( Eample n he MDP cae: Ue a feaure fne hzon co A ufcaon f A a conracon and g b: he fed pon ha an epanon he fm A k b Whle (A k g( hard o generae, can be appromaed by amplng (n effec we ue noy feaure k

22 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Mulep Veron (Fed Sep and λ-mehod Replace by a mulep mappng wh he ame fed pon, e.g., k where k fed, (λ ( λ λ k k, A (λ ( λ λ k A k, k k where λ (, uch ha he nfne ere converge Movaon f λ-mehod, aumng ha pecral radu A (A Propoon: If I A nverble and (A, hen (A (λ <, λ (,, lm λ `A (λ A λ ncreae he conracon become ronger We mu have λ < /(A f a λ-mehod o apply. here are no rercon f a k-ep mehod

23 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon λ-mehod When he LSD/LSPE-ype mehod gven earler are appled o Π (λ hey yeld generalzaon o LSD(λ and LSPE(λ he fmula nvolve empal dfference, baed on he epanon (λ ( λ m (A m b A m A m m he enre analy D(λ, LSD(λ, and LSPE(λ f DP generalze ubec o he followng rercon: Egenvalue λa mu be whn he un crcle f LSD analog Addonal conracon aumpon f LSPE(λ and D(λ [.e., ΠA (λ a conracon]

24 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Fm λ-mehod I and column amplng are done ung he ame chan P. Defne w k, and f m w k,m a k k p k k a k k p k k a km km p km km Eample: Dcouned DP w k,m α m, k LSPE-ype mehod r r! φ( k φ( k φ( k λ mk w k,mk d ( m, k k mk where d ( m are he empal dfference d ( m b m w m, φ( m r φ( m r,, m

25 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Fm λ-mehod II Recurve/effcen updae f LSPE-ype mehod r r B (C r h where B B φ( φ(, h h z b, C C z `w, φ( φ(, z λw, z φ(. LSD(λ-ype mehod u r C h D(λ-ype mehod where γ he epze r r γ z d (

26 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Convergence Reul Propoon: Aume ha P rreducble, and ha λ afe λ ma a /p <, λ [,., Le r be generaed by he LSD(λ-ype alghm. hen, r r λ wh probably he ame rue f he LSPE(λ-ype alghm [aumng alo ha (A (λ ] Here r λ he oluon he proeced equaon Π (λ Smlar reul f D(λ-ype eenon, under uable (ochac appromaon-ype condon f he epze

27 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon A onlnear Equaon wh Scalar onlneare Conder he yem ( Af ( b, where f : R n R n a mappng wh calar funcon componen he fm f ( `f (,..., f n( n. Aume ha each he mappng f : R R nonepanve: f ( f (,,..., n,, R. hen f A a conracon wh repec o a weghed Eucldean nm, alo a conracon h rucure mple favable choce a chan f mulaon

28 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Opmal Soppng Le ( αpf ( b, where P rreducble ranon probably wh nvaran drbuon ξ, α (, a calar dcoun fac, and f ha componen f ( mn{c, },,..., n, where c are ome calar. hen ( he Q-fac equaon crepondng o a dcouned opmal oppng problem In h cae, ΠA a conracon wh repec o ξ [kl and Van Roy (999, who gave a Q-learnng alghm wh lnear funcon appromaon] he LSPE alghm ha been generalzed o h problem (Yu and Bereka 7; alo he 3rd Edon my DP e 7 here no good" LSD-ype alghm f h problem (he fed pon equaon o be appromaed nonlnear

29 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Lnear Lea Square/Regreon/Bellman Mehod Conder olvng he problem mn r R A b ξ o appromae he weghed lea quare oluon A b. Here A : m n mar, ξ a known probably drbuon vec, b R m, and Φ an n mar ba funcon. he oluon r (Φ A ΞAΦ Φ A Ξb, where Ξ he dagonal m m mar havng ξ along he dagonal o appromae he oluon, we replace Φ A ΞAΦ and Φ A Ξb wh mulaon-baed emae

30 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Iue n Regreon/Bellman Mehod eed o ample wo column f each row me noe Varance reducon a fm mpance amplng may be eenal Dealng wh (near ngular Φ A ΞAΦ Add a mall mulple he deny o Φ A ΞAΦ (lke a pr n a regreon eng,.e., appromae by mulaon where γ mall pove parameer Ue a promal mehod: r (Φ A ΞAΦ γi Φ A Ξb r (Φ A ΞAΦ γ I (Φ A Ξb γ r, where γ a pove parameer. h converge o he crec oluon (Φ A ΞAΦ Φ A Ξb Applcaon n nvere problem and oher area (huge dmenon - e.g., n 9, A: fully dene

31 Proeced Equaon Appromaon General LSD and LSPE-ype Alghm Eenon Concludng Remark D mehod can be naurally eended o olve lnear yem equaon In dong o, perpecve and new mehod are obaned f appromae DP he all approach very mple: Sar wh a deermnc alghm Wre n erm epeced value Appromae he epeced value by mulaon he approach apple o many lnear algebra-ype problem - beyond hoe dcued here (e.g., compung he domnan egenvalue a mar, appromang he nvaran drbuon a chan here conderable leraure and heecal wk on Mone Carlo lnear algebra mehod (arng wh von eumann he new elemen here lnear funcon appromaon and he connecon wh D mehod Ecng propec: Applcaon o lnear algebra problem huge dmenon, far beyond he DP cone

(,,, ) (,,, ). In addition, there are three other consumers, -2, -1, and 0. Consumer -2 has the utility function

(,,, ) (,,, ). In addition, there are three other consumers, -2, -1, and 0. Consumer -2 has the utility function MACROECONOMIC THEORY T J KEHOE ECON 87 SPRING 5 PROBLEM SET # Conder an overlappng generaon economy le ha n queon 5 on problem e n whch conumer lve for perod The uly funcon of he conumer born n perod,

More information

Approximate Monte Carlo Linear Algebra. Temporal Difference Methods and

Approximate Monte Carlo Linear Algebra. Temporal Difference Methods and Proeced Equan Aroan General LD and LPE-ye Algh Een eal Dfference Mehod and Aroae Me Carlo Lnear Algebra Dr P Berea Dearen Elecrcal Engneerng and Couer cence Maachue Inue echnology RL Who, Llle 8 Proeced

More information

Control Systems. Mathematical Modeling of Control Systems.

Control Systems. Mathematical Modeling of Control Systems. Conrol Syem Mahemacal Modelng of Conrol Syem chbum@eoulech.ac.kr Oulne Mahemacal model and model ype. Tranfer funcon model Syem pole and zero Chbum Lee -Seoulech Conrol Syem Mahemacal Model Model are key

More information

A Demand System for Input Factors when there are Technological Changes in Production

A Demand System for Input Factors when there are Technological Changes in Production A Demand Syem for Inpu Facor when here are Technologcal Change n Producon Movaon Due o (e.g.) echnologcal change here mgh no be a aonary relaonhp for he co hare of each npu facor. When emang demand yem

More information

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany Herarchcal Markov Normal Mxure models wh Applcaons o Fnancal Asse Reurns Appendx: Proofs of Theorems and Condonal Poseror Dsrbuons John Geweke a and Gann Amsano b a Deparmens of Economcs and Sascs, Unversy

More information

ANALYSIS AND MODELING OF HYDROLOGIC TIME SERIES. Wasserhaushalt Time Series Analysis and Stochastic Modelling Spring Semester

ANALYSIS AND MODELING OF HYDROLOGIC TIME SERIES. Wasserhaushalt Time Series Analysis and Stochastic Modelling Spring Semester ANALYSIS AND MODELING OF HYDROLOGIC TIME SERIES Waerhauhal Tme Sere Analy and Sochac Modellng Sprng Semeer 8 ANALYSIS AND MODELING OF HYDROLOGIC TIME SERIES Defnon Wha a me ere? Leraure: Sala, J.D. 99,

More information

Lecture VI Regression

Lecture VI Regression Lecure VI Regresson (Lnear Mehods for Regresson) Conens: Lnear Mehods for Regresson Leas Squares, Gauss Markov heorem Recursve Leas Squares Lecure VI: MLSC - Dr. Sehu Vjayakumar Lnear Regresson Model M

More information

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 4

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 4 CS434a/54a: Paern Recognon Prof. Olga Veksler Lecure 4 Oulne Normal Random Varable Properes Dscrmnan funcons Why Normal Random Varables? Analycally racable Works well when observaon comes form a corruped

More information

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s Ordnary Dfferenal Equaons n Neuroscence wh Malab eamples. Am - Gan undersandng of how o se up and solve ODE s Am Undersand how o se up an solve a smple eample of he Hebb rule n D Our goal a end of class

More information

Notes on the stability of dynamic systems and the use of Eigen Values.

Notes on the stability of dynamic systems and the use of Eigen Values. Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon

More information

Cooling of a hot metal forging. , dt dt

Cooling of a hot metal forging. , dt dt Tranen Conducon Uneady Analy - Lumped Thermal Capacy Model Performed when; Hea ranfer whn a yem produced a unform emperaure drbuon n he yem (mall emperaure graden). The emperaure change whn he yem condered

More information

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5 TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres

More information

Appendix H: Rarefaction and extrapolation of Hill numbers for incidence data

Appendix H: Rarefaction and extrapolation of Hill numbers for incidence data Anne Chao Ncholas J Goell C seh lzabeh L ander K Ma Rober K Colwell and Aaron M llson 03 Rarefacon and erapolaon wh ll numbers: a framewor for samplng and esmaon n speces dversy sudes cology Monographs

More information

A. Inventory model. Why are we interested in it? What do we really study in such cases.

A. Inventory model. Why are we interested in it? What do we really study in such cases. Some general yem model.. Inenory model. Why are we nereed n? Wha do we really udy n uch cae. General raegy of machng wo dmlar procee, ay, machng a fa proce wh a low one. We need an nenory or a buffer or

More information

Lecture 6: Learning for Control (Generalised Linear Regression)

Lecture 6: Learning for Control (Generalised Linear Regression) Lecure 6: Learnng for Conrol (Generalsed Lnear Regresson) Conens: Lnear Mehods for Regresson Leas Squares, Gauss Markov heorem Recursve Leas Squares Lecure 6: RLSC - Prof. Sehu Vjayakumar Lnear Regresson

More information

Robust and Accurate Cancer Classification with Gene Expression Profiling

Robust and Accurate Cancer Classification with Gene Expression Profiling Robus and Accurae Cancer Classfcaon wh Gene Expresson Proflng (Compuaonal ysems Bology, 2005) Auhor: Hafeng L, Keshu Zhang, ao Jang Oulne Background LDA (lnear dscrmnan analyss) and small sample sze problem

More information

L N O Q. l q l q. I. A General Case. l q RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY. Econ. 511b Spring 1998 C. Sims

L N O Q. l q l q. I. A General Case. l q RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY. Econ. 511b Spring 1998 C. Sims Econ. 511b Sprng 1998 C. Sm RAD AGRAGE UPERS AD RASVERSAY agrange mulpler mehod are andard fare n elemenary calculu coure, and hey play a cenral role n economc applcaon of calculu becaue hey ofen urn ou

More information

( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model

( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model BGC1: Survval and even hsory analyss Oslo, March-May 212 Monday May 7h and Tuesday May 8h The addve regresson model Ørnulf Borgan Deparmen of Mahemacs Unversy of Oslo Oulne of program: Recapulaon Counng

More information

. The geometric multiplicity is dim[ker( λi. number of linearly independent eigenvectors associated with this eigenvalue.

. The geometric multiplicity is dim[ker( λi. number of linearly independent eigenvectors associated with this eigenvalue. Lnear Algebra Lecure # Noes We connue wh he dscusson of egenvalues, egenvecors, and dagonalzably of marces We wan o know, n parcular wha condons wll assure ha a marx can be dagonalzed and wha he obsrucons

More information

Volatility Interpolation

Volatility Interpolation Volaly Inerpolaon Prelmnary Verson March 00 Jesper Andreasen and Bran Huge Danse Mares, Copenhagen wan.daddy@danseban.com brno@danseban.com Elecronc copy avalable a: hp://ssrn.com/absrac=69497 Inro Local

More information

Lecture 11: Stereo and Surface Estimation

Lecture 11: Stereo and Surface Estimation Lecure : Sereo and Surface Emaon When camera poon have been deermned, ung rucure from moon, we would lke o compue a dene urface model of he cene. In h lecure we wll udy he o called Sereo Problem, where

More information

A Nonlinear ILC Schemes for Nonlinear Dynamic Systems To Improve Convergence Speed

A Nonlinear ILC Schemes for Nonlinear Dynamic Systems To Improve Convergence Speed IJCSI Inernaonal Journal of Compuer Scence Iue, Vol. 9, Iue 3, No, ay ISSN (Onlne): 694-84 www.ijcsi.org 8 A Nonlnear ILC Scheme for Nonlnear Dynamc Syem o Improve Convergence Speed Hoen Babaee, Alreza

More information

. The geometric multiplicity is dim[ker( λi. A )], i.e. the number of linearly independent eigenvectors associated with this eigenvalue.

. The geometric multiplicity is dim[ker( λi. A )], i.e. the number of linearly independent eigenvectors associated with this eigenvalue. Mah E-b Lecure #0 Noes We connue wh he dscusson of egenvalues, egenvecors, and dagonalzably of marces We wan o know, n parcular wha condons wll assure ha a marx can be dagonalzed and wha he obsrucons are

More information

Track Properities of Normal Chain

Track Properities of Normal Chain In. J. Conemp. Mah. Scences, Vol. 8, 213, no. 4, 163-171 HIKARI Ld, www.m-har.com rac Propes of Normal Chan L Chen School of Mahemacs and Sascs, Zhengzhou Normal Unversy Zhengzhou Cy, Hennan Provnce, 4544,

More information

EEL 6266 Power System Operation and Control. Chapter 5 Unit Commitment

EEL 6266 Power System Operation and Control. Chapter 5 Unit Commitment EEL 6266 Power Sysem Operaon and Conrol Chaper 5 Un Commmen Dynamc programmng chef advanage over enumeraon schemes s he reducon n he dmensonaly of he problem n a src prory order scheme, here are only N

More information

ELEC 201 Electric Circuit Analysis I Lecture 9(a) RLC Circuits: Introduction

ELEC 201 Electric Circuit Analysis I Lecture 9(a) RLC Circuits: Introduction //6 All le courey of Dr. Gregory J. Mazzaro EE Elecrc rcu Analy I ecure 9(a) rcu: Inroucon THE ITADE, THE MIITAY OEGE OF SOUTH AOINA 7 Moulre Sree, harleon, S 949 V Sere rcu: Analog Dcoery _ 5 Ω pf eq

More information

Solution in semi infinite diffusion couples (error function analysis)

Solution in semi infinite diffusion couples (error function analysis) Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of

More information

Matrix reconstruction with the local max norm

Matrix reconstruction with the local max norm Marx reconrucon wh he local max norm Rna oygel Deparmen of Sac Sanford Unvery rnafb@anfordedu Nahan Srebro Toyoa Technologcal Inue a Chcago na@cedu Rulan Salakhudnov Dep of Sac and Dep of Compuer Scence

More information

Advanced Machine Learning & Perception

Advanced Machine Learning & Perception Advanced Machne Learnng & Percepon Insrucor: Tony Jebara SVM Feaure & Kernel Selecon SVM Eensons Feaure Selecon (Flerng and Wrappng) SVM Feaure Selecon SVM Kernel Selecon SVM Eensons Classfcaon Feaure/Kernel

More information

Dynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005

Dynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005 Dynamc Team Decson Theory EECS 558 Proec Shruvandana Sharma and Davd Shuman December 0, 005 Oulne Inroducon o Team Decson Theory Decomposon of he Dynamc Team Decson Problem Equvalence of Sac and Dynamc

More information

Fundamentals of PLLs (I)

Fundamentals of PLLs (I) Phae-Locked Loop Fundamenal of PLL (I) Chng-Yuan Yang Naonal Chung-Hng Unvery Deparmen of Elecrcal Engneerng Why phae-lock? - Jer Supreon - Frequency Synhe T T + 1 - Skew Reducon T + 2 T + 3 PLL fou =

More information

SSRG International Journal of Thermal Engineering (SSRG-IJTE) Volume 4 Issue 1 January to April 2018

SSRG International Journal of Thermal Engineering (SSRG-IJTE) Volume 4 Issue 1 January to April 2018 SSRG Inernaonal Journal of Thermal Engneerng (SSRG-IJTE) Volume 4 Iue 1 January o Aprl 18 Opmal Conrol for a Drbued Parameer Syem wh Tme-Delay, Non-Lnear Ung he Numercal Mehod. Applcaon o One- Sded Hea

More information

Cubic Bezier Homotopy Function for Solving Exponential Equations

Cubic Bezier Homotopy Function for Solving Exponential Equations Penerb Journal of Advanced Research n Compung and Applcaons ISSN (onlne: 46-97 Vol. 4, No.. Pages -8, 6 omoopy Funcon for Solvng Eponenal Equaons S. S. Raml *,,. Mohamad Nor,a, N. S. Saharzan,b and M.

More information

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy Arcle Inernaonal Journal of Modern Mahemacal Scences, 4, (): - Inernaonal Journal of Modern Mahemacal Scences Journal homepage: www.modernscenfcpress.com/journals/jmms.aspx ISSN: 66-86X Florda, USA Approxmae

More information

CHAPTER 10: LINEAR DISCRIMINATION

CHAPTER 10: LINEAR DISCRIMINATION CHAPER : LINEAR DISCRIMINAION Dscrmnan-based Classfcaon 3 In classfcaon h K classes (C,C,, C k ) We defned dscrmnan funcon g j (), j=,,,k hen gven an es eample, e chose (predced) s class label as C f g

More information

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS THE PREICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS INTROUCTION The wo dmensonal paral dfferenal equaons of second order can be used for he smulaon of compeve envronmen n busness The arcle presens he

More information

Dual Approximate Dynamic Programming for Large Scale Hydro Valleys

Dual Approximate Dynamic Programming for Large Scale Hydro Valleys Dual Approxmae Dynamc Programmng for Large Scale Hydro Valleys Perre Carpener and Jean-Phlppe Chanceler 1 ENSTA ParsTech and ENPC ParsTech CMM Workshop, January 2016 1 Jon work wh J.-C. Alas, suppored

More information

H = d d q 1 d d q N d d p 1 d d p N exp

H = d d q 1 d d q N d d p 1 d d p N exp 8333: Sacal Mechanc I roblem Se # 7 Soluon Fall 3 Canoncal Enemble Non-harmonc Ga: The Hamlonan for a ga of N non neracng parcle n a d dmenonal box ha he form H A p a The paron funcon gven by ZN T d d

More information

Multiple Failures. Diverse Routing for Maximizing Survivability. Maximum Survivability Models. Minimum-Color (SRLG) Diverse Routing

Multiple Failures. Diverse Routing for Maximizing Survivability. Maximum Survivability Models. Minimum-Color (SRLG) Diverse Routing Mulple Falure Dvere Roung for Maxmzng Survvably One-falure aumpon n prevou work Mulple falure Hard o provde 100% proecon Maxmum urvvably Maxmum Survvably Model Mnmum-Color (SRLG) Dvere Roung Each lnk ha

More information

Chapter 5 Signal-Space Analysis

Chapter 5 Signal-Space Analysis Chaper 5 Sgnal-Space Analy Sgnal pace analy provde a mahemacally elegan and hghly nghful ool for he udy of daa ranmon. 5. Inroducon o Sacal model for a genec dgal communcaon yem n eage ource: A pror probable

More information

ELIMINATION OF DOMINATED STRATEGIES AND INESSENTIAL PLAYERS

ELIMINATION OF DOMINATED STRATEGIES AND INESSENTIAL PLAYERS OPERATIONS RESEARCH AND DECISIONS No. 1 215 DOI: 1.5277/ord1513 Mamoru KANEKO 1 Shuge LIU 1 ELIMINATION OF DOMINATED STRATEGIES AND INESSENTIAL PLAYERS We udy he proce, called he IEDI proce, of eraed elmnaon

More information

CTLS 4 SNR. Multi Reference CTLS Method for Passive Localization of Radar Targets

CTLS 4 SNR. Multi Reference CTLS Method for Passive Localization of Radar Targets دا ند رعا ل» ی و ناوری ج ه ع ی و ی «ع وم 79-85 9 C 4 * Donloaded from ad.r a 9:06 +040 on Frda arch nd 09-4 - - - - (9/06/4 : 90/05/7 : ) DOA. DOA. C DOA.. C.. C SR.. C.C DOA : ul Reference C ehod for

More information

, t 1. Transitions - this one was easy, but in general the hardest part is choosing the which variables are state and control variables

, t 1. Transitions - this one was easy, but in general the hardest part is choosing the which variables are state and control variables Opmal Conrol Why Use I - verss calcls of varaons, opmal conrol More generaly More convenen wh consrans (e.g., can p consrans on he dervaves More nsghs no problem (a leas more apparen han hrogh calcls of

More information

Lecture 11 SVM cont

Lecture 11 SVM cont Lecure SVM con. 0 008 Wha we have done so far We have esalshed ha we wan o fnd a lnear decson oundary whose margn s he larges We know how o measure he margn of a lnear decson oundary Tha s: he mnmum geomerc

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Lnear Response Theory: The connecon beween QFT and expermens 3.1. Basc conceps and deas Q: ow do we measure he conducvy of a meal? A: we frs nroduce a weak elecrc feld E, and hen measure

More information

Online Supplement for Dynamic Multi-Technology. Production-Inventory Problem with Emissions Trading

Online Supplement for Dynamic Multi-Technology. Production-Inventory Problem with Emissions Trading Onlne Supplemen for Dynamc Mul-Technology Producon-Invenory Problem wh Emssons Tradng by We Zhang Zhongsheng Hua Yu Xa and Baofeng Huo Proof of Lemma For any ( qr ) Θ s easy o verfy ha he lnear programmng

More information

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS R&RATA # Vol.) 8, March FURTHER AALYSIS OF COFIDECE ITERVALS FOR LARGE CLIET/SERVER COMPUTER ETWORKS Vyacheslav Abramov School of Mahemacal Scences, Monash Unversy, Buldng 8, Level 4, Clayon Campus, Wellngon

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 31 Signal & Syem Prof. Mark Fowler Noe Se #27 C-T Syem: Laplace Tranform Power Tool for yem analyi Reading Aignmen: Secion 6.1 6.3 of Kamen and Heck 1/18 Coure Flow Diagram The arrow here how concepual

More information

Chapter 6: AC Circuits

Chapter 6: AC Circuits Chaper 6: AC Crcus Chaper 6: Oulne Phasors and he AC Seady Sae AC Crcus A sable, lnear crcu operang n he seady sae wh snusodal excaon (.e., snusodal seady sae. Complee response forced response naural response.

More information

Laplace Transformation of Linear Time-Varying Systems

Laplace Transformation of Linear Time-Varying Systems Laplace Tranformaon of Lnear Tme-Varyng Syem Shervn Erfan Reearch Cenre for Inegraed Mcroelecronc Elecrcal and Compuer Engneerng Deparmen Unvery of Wndor Wndor, Onaro N9B 3P4, Canada Aug. 4, 9 Oulne of

More information

FTCS Solution to the Heat Equation

FTCS Solution to the Heat Equation FTCS Soluon o he Hea Equaon ME 448/548 Noes Gerald Reckenwald Porland Sae Unversy Deparmen of Mechancal Engneerng gerry@pdxedu ME 448/548: FTCS Soluon o he Hea Equaon Overvew Use he forward fne d erence

More information

( ) () we define the interaction representation by the unitary transformation () = ()

( ) () we define the interaction representation by the unitary transformation () = () Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger

More information

Stochastic Maxwell Equations in Photonic Crystal Modeling and Simulations

Stochastic Maxwell Equations in Photonic Crystal Modeling and Simulations Sochasc Maxwell Equaons n Phoonc Crsal Modelng and Smulaons Hao-Mn Zhou School of Mah Georga Insue of Technolog Jon work wh: Al Adb ECE Majd Bade ECE Shu-Nee Chow Mah IPAM UCLA Aprl 14-18 2008 Parall suppored

More information

Fall 2010 Graduate Course on Dynamic Learning

Fall 2010 Graduate Course on Dynamic Learning Fall 200 Graduae Course on Dynamc Learnng Chaper 4: Parcle Flers Sepember 27, 200 Byoung-Tak Zhang School of Compuer Scence and Engneerng & Cognve Scence and Bran Scence Programs Seoul aonal Unversy hp://b.snu.ac.kr/~bzhang/

More information

Comparison of Differences between Power Means 1

Comparison of Differences between Power Means 1 In. Journal of Mah. Analyss, Vol. 7, 203, no., 5-55 Comparson of Dfferences beween Power Means Chang-An Tan, Guanghua Sh and Fe Zuo College of Mahemacs and Informaon Scence Henan Normal Unversy, 453007,

More information

u(t) Figure 1. Open loop control system

u(t) Figure 1. Open loop control system Open loop conrol v cloed loop feedbac conrol The nex wo figure preen he rucure of open loop and feedbac conrol yem Figure how an open loop conrol yem whoe funcion i o caue he oupu y o follow he reference

More information

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim Korean J. Mah. 19 (2011), No. 3, pp. 263 272 GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS Youngwoo Ahn and Kae Km Absrac. In he paper [1], an explc correspondence beween ceran

More information

by Lauren DeDieu Advisor: George Chen

by Lauren DeDieu Advisor: George Chen b Laren DeDe Advsor: George Chen Are one of he mos powerfl mehods o nmercall solve me dependen paral dfferenal eqaons PDE wh some knd of snglar shock waves & blow-p problems. Fed nmber of mesh pons Moves

More information

Outline. Probabilistic Model Learning. Probabilistic Model Learning. Probabilistic Model for Time-series Data: Hidden Markov Model

Outline. Probabilistic Model Learning. Probabilistic Model Learning. Probabilistic Model for Time-series Data: Hidden Markov Model Probablsc Model for Tme-seres Daa: Hdden Markov Model Hrosh Mamsuka Bonformacs Cener Kyoo Unversy Oulne Three Problems for probablsc models n machne learnng. Compung lkelhood 2. Learnng 3. Parsng (predcon

More information

GMM parameter estimation. Xiaoye Lu CMPS290c Final Project

GMM parameter estimation. Xiaoye Lu CMPS290c Final Project GMM paraeer esaon Xaoye Lu M290c Fnal rojec GMM nroducon Gaussan ure Model obnaon of several gaussan coponens Noaon: For each Gaussan dsrbuon:, s he ean and covarance ar. A GMM h ures(coponens): p ( 2π

More information

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION S19 A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION by Xaojun YANG a,b, Yugu YANG a*, Carlo CATTANI c, and Mngzheng ZHU b a Sae Key Laboraory for Geomechancs and Deep Underground Engneerng, Chna Unversy

More information

An introduction to Support Vector Machine

An introduction to Support Vector Machine An nroducon o Suppor Vecor Machne 報告者 : 黃立德 References: Smon Haykn, "Neural Neworks: a comprehensve foundaon, second edon, 999, Chaper 2,6 Nello Chrsann, John Shawe-Tayer, An Inroducon o Suppor Vecor Machnes,

More information

Optimal Adjustment Algorithm for p Coordinates and the Starting Point in Interior Point Methods

Optimal Adjustment Algorithm for p Coordinates and the Starting Point in Interior Point Methods Amercan Journal of Operaon Reearch 9- do:.436/aor..4 Publhed Onlne December (hp://www.scrp.org/ournal/aor) 9 Opmal Adumen Algorhm for p Coordnae and he Sarng Pon n Ineror Pon Mehod Abrac Carla T. L. S.

More information

CS286.2 Lecture 14: Quantum de Finetti Theorems II

CS286.2 Lecture 14: Quantum de Finetti Theorems II CS286.2 Lecure 14: Quanum de Fne Theorems II Scrbe: Mara Okounkova 1 Saemen of he heorem Recall he las saemen of he quanum de Fne heorem from he prevous lecure. Theorem 1 Quanum de Fne). Le ρ Dens C 2

More information

Department of Economics University of Toronto

Department of Economics University of Toronto Deparmen of Economcs Unversy of Torono ECO408F M.A. Economercs Lecure Noes on Heeroskedascy Heeroskedascy o Ths lecure nvolves lookng a modfcaons we need o make o deal wh he regresson model when some of

More information

How about the more general "linear" scalar functions of scalars (i.e., a 1st degree polynomial of the following form with a constant term )?

How about the more general linear scalar functions of scalars (i.e., a 1st degree polynomial of the following form with a constant term )? lmcd Lnear ransformaon of a vecor he deas presened here are que general hey go beyond he radonal mar-vecor ype seen n lnear algebra Furhermore, hey do no deal wh bass and are equally vald for any se of

More information

( ) [ ] MAP Decision Rule

( ) [ ] MAP Decision Rule Announcemens Bayes Decson Theory wh Normal Dsrbuons HW0 due oday HW o be assgned soon Proec descrpon posed Bomercs CSE 90 Lecure 4 CSE90, Sprng 04 CSE90, Sprng 04 Key Probables 4 ω class label X feaure

More information

Comb Filters. Comb Filters

Comb Filters. Comb Filters The smple flers dscussed so far are characered eher by a sngle passband and/or a sngle sopband There are applcaons where flers wh mulple passbands and sopbands are requred Thecomb fler s an example of

More information

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.3. COMPATIBILITY EQUATIONS Connuum Mechancs Course (MMC) - ETSECCPB - UPC Overvew Compably Condons Compably Equaons of a Poenal Vecor Feld Compably Condons for Infnesmal Srans Inegraon of he Infnesmal

More information

Multiple Regressions and Correlation Analysis

Multiple Regressions and Correlation Analysis Mulple Regreon and Correlaon Analy Chaper 4 McGraw-Hll/Irwn Copyrgh 2 y The McGraw-Hll Compane, Inc. All rgh reerved. GOALS. Decre he relaonhp eween everal ndependen varale and a dependen varale ung mulple

More information

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL Sco Wsdom, John Hershey 2, Jonahan Le Roux 2, and Shnj Waanabe 2 Deparmen o Elecrcal Engneerng, Unversy o Washngon, Seale, WA, USA

More information

Optimal Filtering for Linear Discrete-Time Systems with Single Delayed Measurement

Optimal Filtering for Linear Discrete-Time Systems with Single Delayed Measurement 378 Hong-Guo Inernaonal Zhao, Journal Huan-Shu of Conrol, Zhang, Auomaon, Cheng-Hu an Zhang, Syem, an vol. Xn-Mn 6, no. Song 3, pp. 378-385, June 28 Opmal Flerng for Lnear Dcree-me Syem h Sngle Delaye

More information

Robustness Experiments with Two Variance Components

Robustness Experiments with Two Variance Components Naonal Insue of Sandards and Technology (NIST) Informaon Technology Laboraory (ITL) Sascal Engneerng Dvson (SED) Robusness Expermens wh Two Varance Componens by Ana Ivelsse Avlés avles@ns.gov Conference

More information

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems Swss Federal Insue of Page 1 The Fne Elemen Mehod for he Analyss of Non-Lnear and Dynamc Sysems Prof. Dr. Mchael Havbro Faber Dr. Nebojsa Mojslovc Swss Federal Insue of ETH Zurch, Swzerland Mehod of Fne

More information

Graduate Macroeconomics 2 Problem set 5. - Solutions

Graduate Macroeconomics 2 Problem set 5. - Solutions Graduae Macroeconomcs 2 Problem se. - Soluons Queson 1 To answer hs queson we need he frms frs order condons and he equaon ha deermnes he number of frms n equlbrum. The frms frs order condons are: F K

More information

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas)

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas) Lecure 8: The Lalace Transform (See Secons 88- and 47 n Boas) Recall ha our bg-cure goal s he analyss of he dfferenal equaon, ax bx cx F, where we emloy varous exansons for he drvng funcon F deendng on

More information

Available online at J. Nonlinear Sci. Appl. 9 (2016), Research Article

Available online at  J. Nonlinear Sci. Appl. 9 (2016), Research Article Avalable onlne a www.jna.com J. Nonlnear Sc. Appl. 9 06, 76 756 Reearch Arcle Aympoc behavor and a poeror error emae n Sobolev pace for he generalzed overlappng doman decompoon mehod for evoluonary HJB

More information

NON-HOMOGENEOUS SEMI-MARKOV REWARD PROCESS FOR THE MANAGEMENT OF HEALTH INSURANCE MODELS.

NON-HOMOGENEOUS SEMI-MARKOV REWARD PROCESS FOR THE MANAGEMENT OF HEALTH INSURANCE MODELS. NON-HOOGENEOU EI-AKO EWA POCE FO THE ANAGEENT OF HEATH INUANCE OE. Jacque Janen CEIAF ld Paul Janon 84 e 9 6 Charlero EGIU Fax: 32735877 E-mal: ceaf@elgacom.ne and amondo anca Unverà a apenza parmeno d

More information

Existence and Uniqueness Results for Random Impulsive Integro-Differential Equation

Existence and Uniqueness Results for Random Impulsive Integro-Differential Equation Global Journal of Pure and Appled Mahemacs. ISSN 973-768 Volume 4, Number 6 (8), pp. 89-87 Research Inda Publcaons hp://www.rpublcaon.com Exsence and Unqueness Resuls for Random Impulsve Inegro-Dfferenal

More information

On One Analytic Method of. Constructing Program Controls

On One Analytic Method of. Constructing Program Controls Appled Mahemacal Scences, Vol. 9, 05, no. 8, 409-407 HIKARI Ld, www.m-hkar.com hp://dx.do.org/0.988/ams.05.54349 On One Analyc Mehod of Consrucng Program Conrols A. N. Kvko, S. V. Chsyakov and Yu. E. Balyna

More information

Lecture 2 M/G/1 queues. M/G/1-queue

Lecture 2 M/G/1 queues. M/G/1-queue Lecure M/G/ queues M/G/-queue Posson arrval process Arbrary servce me dsrbuon Sngle server To deermne he sae of he sysem a me, we mus now The number of cusomers n he sysems N() Tme ha he cusomer currenly

More information

Discrete Markov Process. Introduction. Example: Balls and Urns. Stochastic Automaton. INTRODUCTION TO Machine Learning 3rd Edition

Discrete Markov Process. Introduction. Example: Balls and Urns. Stochastic Automaton. INTRODUCTION TO Machine Learning 3rd Edition EHEM ALPAYDI he MI Press, 04 Lecure Sldes for IRODUCIO O Machne Learnng 3rd Edon alpaydn@boun.edu.r hp://www.cmpe.boun.edu.r/~ehem/ml3e Sldes from exboo resource page. Slghly eded and wh addonal examples

More information

Evaluating Topological Optimized Layout of Building Structures by Using Nodal Material Density Based Bilinear Interpolation

Evaluating Topological Optimized Layout of Building Structures by Using Nodal Material Density Based Bilinear Interpolation Evaluang opologcal Opmzed Layou of Buldng Srucure by Ung Nodal Maeral Deny Baed Blnear Inerpolaon Dongkyu Lee* 1, Jaehong Lee, Khak Lee 3 and Namhk Ahn 4 1 Aan Profeor, Deparmen of Archecural Engneerng,

More information

Normal Random Variable and its discriminant functions

Normal Random Variable and its discriminant functions Noral Rando Varable and s dscrnan funcons Oulne Noral Rando Varable Properes Dscrnan funcons Why Noral Rando Varables? Analycally racable Works well when observaon coes for a corruped snle prooype 3 The

More information

Variants of Pegasos. December 11, 2009

Variants of Pegasos. December 11, 2009 Inroducon Varans of Pegasos SooWoong Ryu bshboy@sanford.edu December, 009 Youngsoo Cho yc344@sanford.edu Developng a new SVM algorhm s ongong research opc. Among many exng SVM algorhms, we wll focus on

More information

Relative controllability of nonlinear systems with delays in control

Relative controllability of nonlinear systems with delays in control Relave conrollably o nonlnear sysems wh delays n conrol Jerzy Klamka Insue o Conrol Engneerng, Slesan Techncal Unversy, 44- Glwce, Poland. phone/ax : 48 32 37227, {jklamka}@a.polsl.glwce.pl Keywor: Conrollably.

More information

China s Model of Managing the Financial System

China s Model of Managing the Financial System Chna odel of anagng he Fnancal Syem arku K Brunnermeer chael Sockn We Xong Inerne Appendx Th nerne appendx preen proof of he propoon n he man paper Proof of Propoon A We dere he perfec nformaon equlbrum

More information

FI 3103 Quantum Physics

FI 3103 Quantum Physics /9/4 FI 33 Quanum Physcs Aleander A. Iskandar Physcs of Magnesm and Phooncs Research Grou Insu Teknolog Bandung Basc Conces n Quanum Physcs Probably and Eecaon Value Hesenberg Uncerany Prncle Wave Funcon

More information

COMPUTER SCIENCE 349A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PARTS 1, 2

COMPUTER SCIENCE 349A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PARTS 1, 2 COMPUTE SCIENCE 49A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PATS, PAT.. a Dene he erm ll-ondoned problem. b Gve an eample o a polynomal ha has ll-ondoned zeros.. Consder evaluaon o anh, where e e anh. e e

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ

More information

MANY real-world applications (e.g. production

MANY real-world applications (e.g. production Barebones Parcle Swarm for Ineger Programmng Problems Mahamed G. H. Omran, Andres Engelbrech and Ayed Salman Absrac The performance of wo recen varans of Parcle Swarm Opmzaon (PSO) when appled o Ineger

More information

Introduction to Compact Dynamical Modeling. III.1 Reducing Linear Time Invariant Systems. Luca Daniel Massachusetts Institute of Technology

Introduction to Compact Dynamical Modeling. III.1 Reducing Linear Time Invariant Systems. Luca Daniel Massachusetts Institute of Technology SF & IH Inroducon o Compac Dynamcal Modelng III. Reducng Lnear me Invaran Sysems Luca Danel Massachuses Insue of echnology Course Oulne Quck Sneak Prevew I. Assemblng Models from Physcal Problems II. Smulang

More information

F-Tests and Analysis of Variance (ANOVA) in the Simple Linear Regression Model. 1. Introduction

F-Tests and Analysis of Variance (ANOVA) in the Simple Linear Regression Model. 1. Introduction ECOOMICS 35* -- OTE 9 ECO 35* -- OTE 9 F-Tess and Analyss of Varance (AOVA n he Smple Lnear Regresson Model Inroducon The smple lnear regresson model s gven by he followng populaon regresson equaon, or

More information

Research Article A Two-Mode Mean-Field Optimal Switching Problem for the Full Balance Sheet

Research Article A Two-Mode Mean-Field Optimal Switching Problem for the Full Balance Sheet Hndaw Publhng Corporaon Inernaonal Journal of Sochac Analy Volume 14 Arcle ID 159519 16 page hp://dx.do.org/1.1155/14/159519 Reearch Arcle A wo-mode Mean-Feld Opmal Swchng Problem for he Full Balance Shee

More information

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β SARAJEVO JOURNAL OF MATHEMATICS Vol.3 (15) (2007), 137 143 SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β M. A. K. BAIG AND RAYEES AHMAD DAR Absrac. In hs paper, we propose

More information

CS 536: Machine Learning. Nonparametric Density Estimation Unsupervised Learning - Clustering

CS 536: Machine Learning. Nonparametric Density Estimation Unsupervised Learning - Clustering CS 536: Machne Learnng Nonparamerc Densy Esmaon Unsupervsed Learnng - Cluserng Fall 2005 Ahmed Elgammal Dep of Compuer Scence Rugers Unversy CS 536 Densy Esmaon - Cluserng - 1 Oulnes Densy esmaon Nonparamerc

More information

On computing differential transform of nonlinear non-autonomous functions and its applications

On computing differential transform of nonlinear non-autonomous functions and its applications On compung dfferenal ransform of nonlnear non-auonomous funcons and s applcaons Essam. R. El-Zahar, and Abdelhalm Ebad Deparmen of Mahemacs, Faculy of Scences and Humanes, Prnce Saam Bn Abdulazz Unversy,

More information

CHAPTER II AC POWER CALCULATIONS

CHAPTER II AC POWER CALCULATIONS CHAE AC OWE CACUAON Conens nroducon nsananeous and Aerage ower Effece or M alue Apparen ower Coplex ower Conseraon of AC ower ower Facor and ower Facor Correcon Maxu Aerage ower ransfer Applcaons 3 nroducon

More information

This document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore.

This document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore. Ths documen s downloaded from DR-NTU, Nanyang Technologcal Unversy Lbrary, Sngapore. Tle A smplfed verb machng algorhm for word paron n vsual speech processng( Acceped verson ) Auhor(s) Foo, Say We; Yong,

More information

Density Matrix Description of NMR BCMB/CHEM 8190

Density Matrix Description of NMR BCMB/CHEM 8190 Densy Marx Descrpon of NMR BCMBCHEM 89 Operaors n Marx Noaon If we say wh one bass se, properes vary only because of changes n he coeffcens weghng each bass se funcon x = h< Ix > - hs s how we calculae

More information