Distance dependence of fluorescence resonance energy transfer

Size: px
Start display at page:

Download "Distance dependence of fluorescence resonance energy transfer"

Transcription

1 J hm Sc, Vol, o 5, Sptmbr 009, pp Indn cdmy of Scncs stnc dpndnc of fluorscnc rsonnc nry trnsfr R S SWTHI nd K L SEBSTI prtmnt of Inornc nd Physcl hmstry, Indn Insttut of Scnc, Bnlor ml: ls@pcscrntn bstrct vtons from th usul R 6 dpndnc of th rt of fluorscnc rsonnc nry trnsfr (FRET on th dstnc btwn th donor nd th ccptor hv bn common scnro n th rcnt tms In ths ppr, w prsnt crtcl nlyss of th dstnc dpndnc of FRET, nd try to llustrt th non-r 6 typ bhvour of th rt for th cs of trnsfr from locld lctronc xctton on th donor, dy molcul to thr dffrnt nry ccptors wth dlocld lctronc xcttons nmly, rphn, two-dmnsonl smconductn sht nd th cs of such smconductn sht rolld to obtn nnotub W us smpl nlytc modls to undrstnd th dstnc dpndnc n ch cs Kywords FRET; rphn; nnotub; tht-bndn modl Introducton Rsonnc nry trnsfr s th procss of nonrdtv trnsfr of nry from n xctd stt donor to round stt ccptor Th rsonnc condton mpls tht th msson spctrum of th donor hs to hv snfcnt ovrlp wth th bsorpton spctrum of th ccptor Whn th donor s fluorscnt spcs, th procss s clld fluorscnc rsonnc nry trnsfr (FRET ccptor my or my not b fluorscnt In FRET, th rt of nry trnsfr follows n R 6 dpndnc whr R s th dstnc btwn th donor nd th ccptor Th rt of nry trnsfr cn b vlutd usn th Frm oldn rul of tm-dpndnt untum mchncs: π = ρ ρ Ψ Ψ H Ψ Ψ, f v u v u I v u v u v u δ ( E E E E ( nd rfr to th donor nd th ccptor rspctvly Th ntl stt of th donor s n xctd stt dnotd s Ψ v, wth n nry E v Th donor s ntlly n n xctd stt wth n lctron tht ws sttn n th molculr orbtl ψ promotd to th orbtl ψ Intlly, th ccptor s n th round stt, nd ftr th nry trnsfr, n dctd to th mmory of th lt Profssor S K Rnrjn For corrspondnc lctron whch ws sttn n th molculr orbtl ψ s promotd to ψ In th bov procss, thr r chns n th vbrtonl stts of both th donor nd th ccptor Th vbrtonl unt r dnotd by ν, ν, u nd u ρ v nd ρ u r th ntl dstrbutons of th donor n th xctd stt nd th ccptor n th round stt rspctvly H s th prt of th Hmltonn rsponsbl for th nry trnsfr nd s oulombc n ntur, s no othr ntrcton s possbl f th ovrlp btwn th orbtls of th donor nd th ccptor s smll (whch s usully th cs Wthn th dbtc pproxmton, th mtrx lmnt my thn b wrttn s 3 v u HI v u Ψ Ψ Ψ Ψ ψ ψ ψ ψ vu r = v u ( ( ( (, ( whr ε s th prmttvty of th mdum sprtn th donor nd th ccptor s rsult of th oulombc ntrcton, n lctron n th donor ts d-xctd, wth th smultnous xctton of n lctron of th ccptor lctn th nuclr poston dpndnc of th mtrx lmnt r ψ ( ψ ( ψ ( ψ ( 777

2 778 R S Swth nd K L Sbstn nd pproxmtn t by ts vlu vlutd t th ulbrum postons of th nucl s = ( drψ r rψ ( r r ψ ( ψ ( ψ ( ψ ( r ψ ( ψ ( ψ ( ψ ( ˆR s th unt vctor n th drcton of th vctor R connctn th cntrs of chr of th two spcs u to th dpolr pproxmton of (4, th rt of trnsfr hs n R 6 dpndnc Förstr 3 ws th frst to nlys ths procss thortclly nd h rrvd t th follown xprsson for th rottonlly vrd rt: lds to = v u HI v u Ψ Ψ Ψ Ψ v v u u r ψ ( ψ ( ψ ( ψ ( ot tht th ntrl r ψ ( ψ ( ψ ( ψ ( (3 (w shll from now onwrds nlct th subscrpt s just th lctrosttc ntrcton btwn th trnston dnsts ψ ( ψ ( nd ψ ( ψ ( For lr ntrprtcl sprtons, ths ntrcton my b pproxmtd s th ntrcton btwn th corrspondn trnston dpols Ths s nown s th dpolr pproxmton Wthn ths pproxmton, r ψ ( ψ ( ψ ( ψ ( 3 ˆˆ RR =, 3 R (4 whr, r th trnston dpols of th donor nd th ccptor rspctvly nd r dfnd by nd = ( drψ r rψ ( r, 6 R0 =, τ 0 R (5 whr τ 0 s th lftm of th donor n th bsnc of th ccptor nd R 0 s th wll-nown Förstr rdus 4 Snc th xprmntl dmonstrton of FRET s usful spctroscopc rulr by Stryr nd Hulnd, 5 t hs bn usd xtnsvly for undrstndn th conformtonl dynmcs of bolocl molculs l protns, R, tc Whn th donor nd th ccptor r two dy molculs, FRET s found to b ffctv n th rn 0 Å 00 Å Enry trnsfr provds n ddtonl dxctton pthwy for th donor thrby ldn to dcrs n th lftm of th xctd donor n prsnc of th ccptor comprd to tht n th bsnc of th ccptor ftr bout 00 Å, n FRET, th xctd donor dcys ccordn to ts nturl lftm, rthr thn by nry trnsfr Whn thr th donor or th ccptor or both r xtndd systms wth dlocld chr dnsts, brdown of th dpolr pproxmton lds to dvtons from th usul R 6 dpndnc In vw of th rcnt studs ldn to non-r 6 dpndncs of th rt of nry trnsfr, w nlys th procss of nry trnsfr from dy molcul, whch hs locld xctton to thr dffrnt ccptors wth dlocld xcttons: rphn, two-dmnsonl smconductn sht nd lon smconductn nnotub W prsnt crtcl nlyss of th dstnc dpndnc of th rt n ll th css Th ppr s ornd s follows: n th scond scton, w prsnt nrl formlsm for vlutn th rt for th cs of trnsfr from locld donor to dlocld ccptors Thrd, fourth nd ffth sctons dl wth trnsfr to rphn, two-dmnsonl smconductn sht nd lon smconductn nnotub rspctvly In th sxth scton, w prsnt nrl dscusson of th non-r 6 bhvour of th rt for vrous systms

3 stnc dpndnc of RET 779 Rsonnc nry trnsfr from locld donor to ccptors wth dlocld lctron dnsts W consdr th procss of rsonnc nry trnsfr from locld donor, nmly dy molcul to ccptors wth dlocld chr dnsts Th mtrx lmnt for ntrcton s vn by U d d ψ ψ ψ r r r ψ r r r r r ( ( ( ( = (6 Th orbtls ψ ( r nd ψ ( r on th ccptor r xtndd n spc (n comprson wth th dstnc of th donor from th ccptor In such stuton, w cn thn of th ntrcton btwn th donor nd th ccptor s tht btwn th trnston dpol of th donor, loctd t th cntr of chr vn by = ( drψ r rψ ( r nd th trnston chr dnsty ψ ( r ψ ( r of th ccptor Thrfor, th mtrx lmnt for ntrcton bcoms U = Φ, (7 whr Φ s th lctrosttc potntl t th pont r (th poston of th donor du to th chr dnsty ψ ( r ψ ( r W shll thn of th ccptor s hvn prodcty, s rsult of whch th stts r chrctrsd by th wv vctor s rsult of nry trnsfr from th donor, n lctron n n nry lvl wth wv vctor s xctd to lvl wth wv vctor f For th trnsfr of n nry Ω from th donor to th ccptor, th rt s vn by: π U E E ( Ω=, δ ( Ω f f f (8 W dfn f =, whr s th momntum trnsfrrd to th ccptor Th rt cn thrfor b wrttn s: π U E E ( Ω=, δ ( Ω (9 Th trnston dnsty vn by ψ ( r ψ ( r = ψ ( r ψ ( r thn hs prodcty wth wv vctor If on dopts th smplst possbl pproxmton, th lctrosttc potntl t pont outsd such chr dstrbuton s functon only of U, = U( (ths s not tru for rphn nd crbon nnotubs Thrfor, th rt cn b wrttn s π U F whr ( Ω= ( (, (0 F( = δ ( E E Ω ( Th dstnc dpndnc of th rt of nry trnsfr s thrfor ovrnd by th functonl forms of th ntrcton nry, U( nd F( W us th nrl formlsm vn bov to undrstnd th procss of nry trnsfr from locld donor to th follown nry ccptors: rphn, twodmnsonl smconductn sht nd th cs of such smconductn sht rolld to obtn nnotub 3 Rsonnc nry trnsfr from dy to rphn W now consdr th procss of nry trnsfr from fluorscnt dy to rphn (s fur 6,7 W us th tht-bndn modl for rphn 8 Th wv functons for rphn r ψ s χ ( r s ( r=, δ s B χ ( r sb B B ( whr th sn holds for th vlnc bnd (π bnd nd th sn holds for th conducton bnd (π bnd nd B rfr to th two crbon toms of th unt cll of rphn s th numbr of toms of ch typ n th lttc χs r th p tomc orbtl wv functons of th crbon toms of th lttc Th phs fctor δ s dfnd by th follown rlton: δ H B ( =, H ( B (3

4 780 R S Swth nd K L Sbstn whr / 3 / 3 x x H ( = t[ cos( /] (4 B In th bov uton, t s th hoppn ntrl nd = l 3 Th nrs of th bnds r vn by E = t[ 4cos( /cos( 3 / y / y 4cos ( /], (5 whr th sn s for th conducton bnd nd th sn s for th vlnc bnd Th vlnc nd th conducton bnds mt t th K-ponts r th K- ponts, 9 th nry dsprson bcoms 3 E = t = vf, (6 whr = x y Whn th donor, fluorscnt dy molcul s xctd, n lctron from n occupd orbtl s xctd to n unoccupd orbtl W consdr th x y trnston dpol momnt of th dy, = ˆ ˆ ˆ x yj to b ntrctn wth th lctrons of rphn s rsult of such n ntrcton, th dy rturns bc to ts round stt nd n lctron n rphn s xctd Exctton of n lctron from ψ ( r to ψ ( r lds to trnston chr dnsty vn by ρ ψ ψ (= r ( ( r r ( δ δ ( s χ r s χ ( r s, (7 whr th summton s ovr crbon toms of thr typ n th lttc Furthr, w hv nlctd th product of χs whch blon to dffrnt toms of th lttc, s thy r nlbl Th lctrosttc potntl du to such trnston dnsty s vn by ρ( r Φ r r (8 r r (= d 4 πε Snc th dnsty χ ( r s χ( r s s locld nr th th tom, w cn us th multpol xpnson to clcult ts lctrosttc potntl t th pont r Th lowst ordr trm s th monopol trm ldn to s ( δ δ (= Φ r 8 πε r s (9 For smll vlus of (=, th sum n th bov uton my b rplcd by n ntrl so tht s ( δ δ (= Φ r d, 8πε s r s u (0 whr u s th r of th unt cll of rphn Th two-dmnsonl ntrl wrttn bov cn b vlutd to t Fur schmtc of th rphn lttc nd th donor dy Th poston vctors nvolvd n th nlyss r lso shown ( δ δ X Φ(= r, ( 4ε whr w hv usd r = (X,, wth X bn prlll to th pln of rphn s th r of th

5 stnc dpndnc of RET 78 rphn lttc W vlut th ntrcton nry usn (7 nd fnd t to b ( δ δ = ( ˆ ˆ U X, 4ε ( whr ˆ = / s th unt vctor n th drcton of nd ˆ s th unt vctor n th drcton Th sur of th ntrcton nry s U = [ cos( ϕ ϕ ] 8ε ˆ ( ˆ (3 W now us (9 to obtn th follown xprsson for th rt of trnsfr: π G whr ˆ ( Ω= ( ˆ (, 4ε (4 G( = [ cos( ϕ ϕ ] δ( E E Ω (5 ot tht th xtr trm n G( comprd to F( dfnd n ( s du to th phs fctor n th wv functons of rphn W frst vlut G( W now us (6 for th nry lvls of rphn, rplc th sum ovr by n ntrl to t π cosψ ψ 0 0 ψ G( = d d 4π cos f δ[ v ( cos ψ Ω] (6 Th bov ntrl cn b vlutd xctly 0 to obtn Θ( Ω v G( = 8 π ( Ω f vf (7 W now substtut th bov rsult nto (4, rplc th sum ovr by n ntrl to t π ( Ω= d dθ[ μ 64πhε 0 0 v f vf θ ( Ω ( μxcosθ μysn θ ] ( Ω (8 Th ntrl ovr θ cn b sly prformd to t ( Ω = ( μ x μy μ 64hε Ω/ v f 0 3 d ( Ω vf (9 For lr vlus of, only vlus of /( contrbut to th bov ntrl In such cs, w cn nlct v f n comprson wth ( Ω, nd xtnd th uppr lmt of th ntrl n (9 to nfnty, to t μx μy μ 4 3π ( ( Ω= (30 56Ωh ε Th bov xprsson for rt cn b rwrttn s sn cos 4 3π ( μ θ μ θ ( Ω=, (3 56Ωh ε whr = nd θ s th nl tht ms wth th -xs W now prform n vrn ovr ll possbl ornttons of th donor trnston dpol momnt to t μ 4 π ( Ω = (3 64Ωh ε Thrfor, th rt of nry trnsfr hs powr lw dpndnc [(dstnc 4 ] for lr vlus of 4 Rsonnc nry trnsfr from dy to two-dmnsonl smconductn sht W now consdr th procss of nry trnsfr from dy molcul to th lctrons confnd to two-dmnsonl smconductn sht W ssum

6 78 R S Swth nd K L Sbstn tht thr s bnd p ε nd th nry lvls bov nd blow th p r vn by E ε = m (33 Th sn s for th conducton bnd nd th sn s for th vlnc bnd s two-dmnsonl wv vctor W hv ssumd th ffctv mss m to b th sm for stts bov nd blow th bnd p Th corrspondn wv functons r ψ (= r ( r R, (34 R χ = whr th sn s for th conducton bnd nd th sn s for th vlnc bnd R dnots th poston of th th tom n th sht s th totl numbr of toms of th sht χ (r R l nd χ (r R dnot th locld orbtls on th th tom tht contrbut to th conducton nd th vlnc bnds rspctvly Wth th bov, xctton of n lctron from ψ ( r to ψ ( r lds to trnston chr dnsty vn by ( = r ( ( r r ρ ψ ψ (35 ( R χ r R χ ( r R, = whr w hv nlctd th product of χs whch blon to dffrnt toms of th lttc, s thy r nlbl Th lctrosttc potntl du to such trnston dnsty s vn by ρ( r Φ r r (36 r r (= d 4 πε Snc th dnsty χ ( r R χ ( r R s locld nr th th tom, w cn us th multpol xpnson to clcult ts lctrosttc potntl t th pont r Th monopol trm of th multpol xpnson vs ro snc th two orbtls χ nd χ r orthoonl Thrfor, th lowst ordr non-ro trm s dpolr n ntur nd on ts whr = dr χ ( r R ( r R χ ( r R s th trnston dpol for th χ χ trnston For smll vlus of (=, th sum n th bov uton my b rplcd by n ntrl so tht R Φ(= r r d, 4 πε R (38 r R u whr u s th r of th unt cll of th twodmnsonl lttc W consdr tht th unt cll of th lttc contns on tom such tht = u, whr s th r of th sht Th twodmnsonl ntrl wrttn bov cn b vlutd to t X Φ(= r r, (39 ε whr w hv usd r =( X,, wth X bn prlll to th pln of th sht Th bov uton cn b smplfd to obtn (= ( ˆ ˆ X Φ r (40 ε W now us (7 to t ˆ = ( ˆ ( ˆ ˆ U, ε X (4 whr s th trnston dpol momnt of th dy vn by = ˆ ˆ ˆ x y j ot tht U s functon only of Thrfor, w substtut (4 nto (0 to t th rt of trnsfr vn by π ( Ω= ( ˆ ˆ ε ˆ ( ˆ F( (4 W now vlut F( usn (33 nd ( to t Φ(= r, 4 πε r R r = R (37 m m F( = Θ ( Ω ε π (43

7 stnc dpndnc of RET 783 W now substtut ths bc nto (4 nd rplc th sum ovr by n ntrl to obtn th follown xprsson for th rt: 3 m 3 ε 0 m ( Ω= d Θ ( Ω 6π ε π 0 ˆ ˆ d ( ˆ ˆ θ ( (44 Th two-dmnsonl vctor s xprssd n ts polr coordnts nd θ For lr, only smll vlus of r mportnt Thn, m m Θ ( Ω ε ( =, Θ Ω ε f Ω > ε For such stuton, th ntrl ovr cn b xctly vlutd to obtn th follown xprsson for th rt 3 m ( Ω= π ε π ˆ ˆ d θ ( ˆ ( ˆ (45 0 Th ntrl ovr θ cn now b prformd to t n xprsson nvolvn th componnts of th dpol momnts, nd W thn prform n vrn ovr ll possbl ornttons of th donor dpol, ldn to th follown xprsson for th rt: m ( Ω = 64 πε 3 4 vry lon tubul of rdus (whch s of nnodmnsons nd lnth L ( (s fur W dopt th smplst possbl dscrpton for th lctrons of th tubul W ssum tht w hv smconductn nnotub, hvn structur smlr to th boron ntrd nnotub, wth bnd p ε (s fur 3 Th cs of crbon nnotub s ntrstn nd s dscussd n sprt publcton Th stts bov nd blow th bnd p my b chrctrd by th momntum prlll to th xs of th tub, whch w dnot by nd th nulr momntum bout th tub xs, whch s untd (nulr momntum bn ul to m, wth m = 0,,, 3 W t th lctron wv functons to b ψ ( ρ, φ, = χ ( r R m ϕ, m = Th suprscrpts n ψ, m( ρ, φ, dnot stts bov ( or blow ( th p χ (r R nd χ (r R dnot th locld orbtls on th th lttc st tht contrbut to th conducton nd th vlnc bnds rspctvly s th numbr of lttc sts of th tubul W t th nrs of th stts to b vn by 4 ε =, m m m ε m, (48 whr m s th ffctv mss Wth th bov, xctton of n lctron from ψ, m( r to ψ, m ( r f f lds to trnston chr dnsty vn by ( x y f Ω> μ μ μ μ ε (46 =0 f Ω <, (47 ε whr w hv usd = nd ˆ = ˆ ˆ x yj Th rt of trnsfr n ths cs too hs (dstnc 4 dpndnc 5 Rsonnc nry trnsfr from dy to lon tubul W now consdr th procss of nry trnsfr from dy molcul to th lctrons confnd to Fur schmtc of th trnston dpol momnt of th donor dy nd th tub

8 784 R S Swth nd K L Sbstn whr u s th surfc r of th unt cll of th cylndrcl surfc W consdr tht th unt cll of th lttc contns on tom ldn to = u, whr s th surfc r of th lon cylndr W now us th follown multpol xpnson for th /r R trm n cylndrcl coordnts: 5 = d r R π m = m ( ϕ ϕ ( Fur 3 schmtc of th on-dmnsonl nry bnds of th nnotub shown th untum numbrs lon th utorl drcton, th nry p nd th mount of nry trnsfrrd f, mf, m ρ( r= ψ ( r ψ ( r m ϕ ( χ r R χ ( r R, = (49 whr w hv put f =, m f = m m nd nlctd th product of χs whch blon to dffrnt sts of th lttc, s thy r nlbl (, ϕ, r th cylndrcl polr coordnts of R Th lctrosttc potntl du to such trnston dnsty s vn by ρ( r Φ r r (50 r r (= d 4 πε Snc th dnsty χ ( r R χ ( r R s locld nr th th tom, on cn wrt th potntl s Φ(= r, r R r = m ϕ (5 whr = drχ ( r R( r R χ ( r R s th trnston dpol for th χ χ trnston For smll vlus of, th sum n th bov uton my b rplcd by n ntrl so tht m ϕ Φ(= r r d, R r R u (5 I ( K ( d R, (53 m m whr w hv usd r =dcosϕˆ dsnϕˆj ˆ nd R = cos ˆ sn ˆ ˆ ϕ ϕj On substtutn ths bc nto (5 nd vlutn th subsunt ntrls, on ts m (= I ( [ m ϕ Φ r K m ( d ] ε r (54 W now us μ = ˆ μρρ μϕϕˆ μ ˆ to obtn mϕ Φ(= r I m ( ε ρ ( K m ( m ( d K d m ϕ K m ( d d (55 W now vlut th ntrcton nry usn (7 nd t s vn by mϕ U = I m ( ε K m ( d K m ( d ρ ρ d d m ( ϕ ρ ϕ ρ ( ρ ρ d, m m ϕ ρ ϕ ϕ K m ( d d d m ( ϕ ϕ d (56

9 stnc dpndnc of RET 785 whr w hv usd μ = ˆ ˆ μρρ μϕϕ μ ˆ W now vlut F( usn ( W us th nry lvls from (48 to obtn th follown uton for F(: Lm F( = d π δ m ( m m m ( m ( Ω ε On vlutn th ntrl, w obtn Lm F ( = π { m } 4 m ( Ω ε {( m m m } (57 (58 Th nulr brcts ovr m ndct tht th summton ncluds thos vlus of m for whch th untty wthn th sur root trm s postv For smll vlus of momntum trnsfr (whch dtrmn th lon dstnc bhvour, w cn nlct th trm n comprson wth Ω ε 4 m ( {( m m m } Wth ths condton, Lm F ( π 4 m( Ω ε { m } {( m m m } (59 Substtutn (59 nto (0 nd rplcn th sum ovr by n ntrl vs ( Ω= Lm 3 π { m }, m {( m m m } 4 m ( Ω ε d U (, (60 whr U( s vn by (56 To vlut th ntrl ovr, w chn th vrbl of ntrton to t dfnd by t = d nd subsuntly us th symptotc form of I m vn by I m t d, m t t d d Γ ( m Th ntrl ovr t cn now b sly vlutd for vrous vlus of m Th ldn ordr trm n th xprsson for th rt corrsponds to th cs whn m = 0 W frst vlut th ntrl ovr t for such cs nd thn vr ovr ll possbl ornttons of th donor trnston dpol momnt to t th follown xprsson for th rt: 3 m (33μ 7 μ ρ ( Ω= π ε d { m } μ m m ( Ω ε, (6 whr w hv usd = Thrfor, th ldn ordr trm n th xprsson for th rt hs (dstnc 5 dpndnc 6 scusson In th rcnt tms, vrty of mtrls l polymrs, 6 nnoprtcls, 7 untum wlls, 8 untum dots, untum wrs, 9 mtl surfcs 0 tc hv bn usd s nry donors/ccptors nd thy hv ld to dvtons from th R 6 dpndnc Whn th nry trnsfr occurs from locld xctton on th donor to locld xctton on th ccptor, th dpolr pproxmton wors nd thrfor on hs n R 6 dpndnc On th contrry, f th nry trnsfr procss nvolvs n xtndd lctronc systm whr th xcttons r dlocld l n th cs of polymrs, untum wrs, untum wlls, th dpolr pproxmton s not vld nd on cn hv dvtons from th R 6

10 786 R S Swth nd K L Sbstn rts non-r 6 dpndnc s of rt ntrst du to th nd for dvlopn nnoscopc rulrs, tht cn msur dstncs wll byond 00 Å hnc t l hv thortclly nlysd th procss of dcy of n xctd molcul fluorscn nr mtllc flm Thy found d 3 dpndnc of th rt of nry trnsfr on th dstnc btwn th molcul nd th mtl for vry thc flms But, for th cs of thn mtllc flms, thy found d 4 dpndnc mpon t l xprmntlly studd th procss of lctronc xctton nry trnsfr from pyrn to snl crystl mtl surfc nd found d 3 dpndnc of th rt d 4 dpndnc hs lso bn obsrvd for th dcy of bctyl bov slvr surfc 0 Furthr, Prsson nd Ln 3 studd th procss of nry trnsfr from vbrtn dpol to th conducton lctrons of mtl Thy fnd tht th nry trnsfr to th surfc mods of th mtl lds to d 4 dpndnc of th rt on th dstnc, whl th trnsfr to th bul mods lds to d 3 dpndnc For th cs of nry trnsfr to th surfc plsmon mods of flt mtl surfc from proxml dpolr mttr, 4 urtc dstnc dpndnc hs bn rportd Th bov dpndncs cn b sly undrstood In FRET, th trnsfr occurs from ro-dmnsonl donor to ro-dmnsonl ccptor ldn to n R 6 dpndnc For th cs of trnsfr to th bul mods of th mtl, th ccptor xcttons r n thr-dmnsons Thrfor, on hs d 3 dpndnc Whn th trnsfr occurs to th ccptors whr th xcttons r confnd to two dmnsons, on hs d 4 dpndnc Lyo 5 hs studd th procss of xctonc nry trnsfr from nrrow untum wr to wd untum wr Th rt of trnsfr ws found to hv d 4 dpndnc for ntrmdt vlus of d nd d 5 dpndnc n th symptotc lmt for lr vlus of d H hs lso nlysd th cs of trnsfr from nrrow untum wr to unform rry of dntcl prlll wd untum wrs nd found d 4 dpndnc n such cs Vry rcntly, Govorov t l 9 rportd study of th procss of xctton nry trnsfr from nnoprtcl to nnowr Whn th rdus of th nnoprtcl s smll comprd to th dstnc btwn th nnoprtcl nd th nnowr, th xcttons n nnoprtcls cn b consdrd locld nd hnc dpolr For lr nnoprtclnnowr dstncs, thy fnd d 5 dpndnc of th rt on th dstnc Snc th ccptor xcttons r confnd to on-dmnson, th rt hs d 5 dpndnc Enry trnsfr from n nornc untum wll to n ornc polyfluorn flm hs bn found to occur 6 du to th oulombc coupln btwn th Mott Wnnr xctons on th untum wll to th Frnl xctons on th polymr Th rt ws found to hv d dpndnc Smlr dstnc dpndnc hs bn found rlr for th cs of lctronc xctton nry trnsfr from polyfluorn to ttrphnyl porphyrn 6 Hll t l 7 hv lso rportd smlr dstnc dpndnc for th cs of nry trnsfr btwn two fluorscnt polymrs tht r rown s lyrd structurs Snc th xcttons n polymr flms nd untum wlls r dlocld ovr two-dmnsons, th rt hs d dpndnc Th procss of nry trnsfr from untum wll 8 to monolyr of smconductor nnocrystls ws rportd rcntly Th xprmnts rvld vry hh ffcncs of nry trnsfr nd th procss ws ttrctv for us n vrty of tchnolocl pplctons l LEs, lsrs, tc Kos t l 8 hv studd ths procss thortclly ssumn tht th s of th untum dot nd th wdth of th untum wll r smll n comprson wth th dstnc btwn thm Thy consdrd two typs of xctd stts n th untum dots s rsult of trnsfr, nmly uscontnuum of hh nry stts nd dscrt low nry stts For th cs of trnsfr to uscontnuum of stts, thy fnd d 4 dpndnc of th rt, whl for xctton to dscrt low nry stts, thy fnd n xponntl dpndnc rnovch t l 9 hv consdrd th procss of nry trnsfr from n nornc untum wll to n ornc lyr nd found n xponntl dstnc dpndnc In ll th bov css, thr th donor or th ccptor or both wr xtndd systms wth dlocld chr dnsts Thrfor, brdown of th dpolr pproxmton to th rt ld to dvtons from th usul R 6 dpndnc Strous t l 30 hv studd th procss of nry trnsfr from th dy fluorscn to 4 nm dmtr old nnoprtcl oubl-strndd molculs of vrous lnths wr usd to fx th dstncs btwn th donor nd th ccptor Surprsnly, thouh th dstncs btwn th donor nd th ccptor r much lrr thn th dmnsons of th donor nd th ccptor, thy fnd d 4 dpndnc of th rt Thy rfr to ths procss s nnoprtcl surfc nry trnsfr (SET nd th rn of

11 stnc dpndnc of RET 787 dstncs tht cn b msurd usn SET s mor thn doubl tht of th trdtonl FRET xprmnts Thrfor, t s ntrstn to s why th dstnc dpndnc n SET s d 4 But, thortcl clcultons for such systm consdrn th trnsfr to th plsmons nd th lctron-hol pr xcttons of th nnoprtcl prdomnntly fnd n R 6 dpndnc 3,3 7 onclusons W hv studd th dstnc dpndnc of th procss of rsonnc nry trnsfr from locld donor, dy molcul to vrous typs of nry ccptors-rphn, two-dmnsonl smconductn sht nd smconductn nnotub usn smpl nlytc modls For th cs of trnsfr to rphn nd two-dmnsonl smconductn sht of lctronc chr dnsty, w fnd (dstnc 4 dpndnc For th cs of trnsfr to smconductn nnotub, w fnd (dstnc 5 dpndnc W hop tht smpl nlytc modls of nry trnsfr prsntd hr cn ld to ntrstn physcl nshts nto th procss of rsonnc nry trnsfr cnowldmnts R S Swth cnowlds ouncl of Scntfc nd Industrl Rsrch (SIR, Ind nd Brstol Myrs Subb Fllowshp for fnncl support Rfrncs Lowc J R 006 Prncpls of fluorscnc spctroscopy (w Yor: Sprnr My V nd Kuhn O 000 hr nd nry trnsfr dynmcs n molculr systms (Wly-VH 3 Förstr T 948 nn Phys 55 4 Vlur B 00 Molculr fluorscnc (w Yor: Wly-VH 5 Stryr L nd Hulnd R P 967 Proc tl cd Sc US Swth R S nd Sbstn K L 008 J hm Phys Swth R S nd Sbstn K L 009 J hm Phys Wllc P R 947 Phys Rv Ktsnlson M I 007 Mtr Tody Shun Knnth W K 986 Phys Rv B Mruls V, Muyumn E E nd Gdu E 008 Phys Rv B Swth R S nd Sbstn K L (unpublshd 3 Blsss nd Gumbs G 006 Phys Rv B Gumbs G nd Blsss 005 Phys Rv B Jcson J 975 lsscl lctrodynmcs (w Yor: Wly Estrn Lmtd 6 Won K F, Bch B nd Rossy P J 004 J Phys hm Sönnchsn, Rnhrd B M, Lphrdt J nd lvstos P 005 t Botchnol chrmnn M, Ptrus M, Kos S, Smth L, Kols nd Klmov V I 004 tur Mrtn P L H nd Govorov O 008 Phys Rv B lvstos P, Vldc H nd Hrrs B 985 J hm Phys 8 54 hnc R R, Proc nd Slby R 978 dv hm Phys 37 mpon, Gllo R, Hrrs B, Robot H J nd Whtmor P M 980 hm Phys Ltt Prsson B J nd Ln 98 Phys Rv B Lrn I, Stocmn M I, chrmnn M nd Klmov V I 004 Phys Rv B69 403(R 5 Lyo S K 006 Phys Rv B Itsos G, Hlots G, Louds P G, Lupton J, Brrds P, lvs E, Prr S, Wtson I M, wson M, Fldmnn J, Murry R nd Brdly 007 Phys Rv B Hll J, Hrot S Y, Worsfold O, Rchrdson T H nd Fox M 004 Phys Rv B (R 8 Kos S, chrmnn M, Klmov V I nd Smth L 005 Phys Rv B rnovch V M, Bso M, L Rocc G nd Bssn F 998 J Phys: ondns Mttr Yun S, Jvr, Jnnns T, Fshr M, Hr S, Ptrson S, Hopns B, Rch O nd Strous G F 005 J m hm Soc Swth R S nd Sbstn K L 007 J hm Phys Bhowmc S, Sn S, Shnoy V B nd Bch B 006 J hm Phys 5 80

Rate of Molecular Exchange Through the Membranes of Ionic Liquid Filled. Polymersomes Dispersed in Water

Rate of Molecular Exchange Through the Membranes of Ionic Liquid Filled. Polymersomes Dispersed in Water Supportng Informton for: Rt of Molculr Exchng hrough th Mmrns of Ionc Lqud Flld olymrsoms Dsprsd n Wtr Soonyong So nd mothy. Lodg *,, Dprtmnt of Chmcl Engnrng & Mtrls Scnc nd Dprtmnt of Chmstry, Unvrsty

More information

A general N-dimensional vector consists of N values. They can be arranged as a column or a row and can be real or complex.

A general N-dimensional vector consists of N values. They can be arranged as a column or a row and can be real or complex. Lnr lgr Vctors gnrl -dmnsonl ctor conssts of lus h cn rrngd s column or row nd cn rl or compl Rcll -dmnsonl ctor cn rprsnt poston, loct, or cclrton Lt & k,, unt ctors long,, & rspctl nd lt k h th componnts

More information

(A) the function is an eigenfunction with eigenvalue Physical Chemistry (I) First Quiz

(A) the function is an eigenfunction with eigenvalue Physical Chemistry (I) First Quiz 96- Physcl Chmstry (I) Frst Quz lctron rst mss m 9.9 - klogrm, Plnck constnt h 6.66-4 oul scon Sp of lght c. 8 m/s, lctron volt V.6-9 oul. Th functon F() C[cos()+sn()] s n gnfuncton of /. Th gnvlu s (A)

More information

h Summary Chapter 7.

h Summary Chapter 7. Summry Chptr 7. In Chptr 7 w dscussd byond th fr lctron modl of chptr 6. In prtculrly w focusd on th nflunc of th prodc potntl of th on cors on th nrgy lvl dgrm of th outr lctrons of th toms. It wll hlp

More information

Fundamentals of Continuum Mechanics. Seoul National University Graphics & Media Lab

Fundamentals of Continuum Mechanics. Seoul National University Graphics & Media Lab Fndmntls of Contnm Mchncs Sol Ntonl Unvrsty Grphcs & Md Lb Th Rodmp of Contnm Mchncs Strss Trnsformton Strn Trnsformton Strss Tnsor Strn T + T ++ T Strss-Strn Rltonshp Strn Enrgy FEM Formlton Lt s Stdy

More information

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation Lctur Rlc nutrnos mpratur at nutrno dcoupln and today Effctv dnracy factor Nutrno mass lmts Saha quaton Physcal Cosmoloy Lnt 005 Rlc Nutrnos Nutrnos ar wakly ntractn partcls (lptons),,,,,,, typcal ractons

More information

Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:

Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture: Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin

More information

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9 Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:

More information

The Hyperelastic material is examined in this section.

The Hyperelastic material is examined in this section. 4. Hyprlastcty h Hyprlastc matral s xad n ths scton. 4..1 Consttutv Equatons h rat of chang of ntrnal nrgy W pr unt rfrnc volum s gvn by th strss powr, whch can b xprssd n a numbr of dffrnt ways (s 3.7.6):

More information

INTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)

INTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x) Chptr 7 INTEGRALS 7. Ovrviw 7.. Lt d d F () f (). Thn, w writ f ( ) d F () + C. Ths intgrls r clld indfinit intgrls or gnrl intgrls, C is clld constnt of intgrtion. All ths intgrls diffr y constnt. 7..

More information

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari snbrg Modl Sad Mohammad Mahd Sadrnhaad Survsor: Prof. bdollah Langar bstract: n ths rsarch w tr to calculat analtcall gnvalus and gnvctors of fnt chan wth ½-sn artcls snbrg modl. W drov gnfuctons for closd

More information

1.9 Cartesian Tensors

1.9 Cartesian Tensors Scton.9.9 Crtsn nsors s th th ctor, hghr ordr) tnsor s mthmtc obct hch rprsnts mny physc phnomn nd hch xsts ndpndnty of ny coordnt systm. In ht foos, Crtsn coordnt systm s sd to dscrb tnsors..9. Crtsn

More information

UNIT # 08 (PART - I)

UNIT # 08 (PART - I) . r. d[h d[h.5 7.5 mol L S d[o d[so UNIT # 8 (PRT - I CHEMICL INETICS EXERCISE # 6. d[ x [ x [ x. r [X[C ' [X [[B r '[ [B [C. r [NO [Cl. d[so d[h.5 5 mol L S d[nh d[nh. 5. 6. r [ [B r [x [y r' [x [y r'

More information

Magnetic field dependence of electrical transport properties in acceptor doped bismuth

Magnetic field dependence of electrical transport properties in acceptor doped bismuth IOSR Journl of Appld Physcs (IOSR-JAP) -ISS: 78-486.Volum 7, Issu Vr. III (Mr. - Apr. 5), PP -6 www.osrjournls.org Mgntc fld dpndnc of lctrcl trnsport proprts n ccptor dopd bsmuth Kjl Krshn Dy Dprtmnt

More information

Errata for Second Edition, First Printing

Errata for Second Edition, First Printing Errt for Scond Edition, First Printing pg 68, lin 1: z=.67 should b z=.44 pg 1: Eqution (.63) should rd B( R) = x= R = θ ( x R) p( x) R 1 x= [1 G( x)] = θp( R) + ( θ R)[1 G( R)] pg 15, problm 6: dmnd of

More information

Preview. Graph. Graph. Graph. Graph Representation. Graph Representation 12/3/2018. Graph Graph Representation Graph Search Algorithms

Preview. Graph. Graph. Graph. Graph Representation. Graph Representation 12/3/2018. Graph Graph Representation Graph Search Algorithms /3/0 Prvw Grph Grph Rprsntton Grph Srch Algorthms Brdth Frst Srch Corrctnss of BFS Dpth Frst Srch Mnmum Spnnng Tr Kruskl s lgorthm Grph Drctd grph (or dgrph) G = (V, E) V: St of vrt (nod) E: St of dgs

More information

Errata for Second Edition, First Printing

Errata for Second Edition, First Printing Errt for Scond Edition, First Printing pg 68, lin 1: z=.67 should b z=.44 pg 71: Eqution (.3) should rd B( R) = θ R 1 x= [1 G( x)] pg 1: Eqution (.63) should rd B( R) = x= R = θ ( x R) p( x) R 1 x= [1

More information

8. Linear Contracts under Risk Neutrality

8. Linear Contracts under Risk Neutrality 8. Lnr Contrcts undr Rsk Nutrlty Lnr contrcts r th smplst form of contrcts nd thy r vry populr n pplctons. Thy offr smpl ncntv mchnsm. Exmpls of lnr contrcts r mny: contrctul jont vnturs, quty jont vnturs,

More information

, between the vertical lines x a and x b. Given a demand curve, having price as a function of quantity, p f (x) at height k is the curve f ( x,

, between the vertical lines x a and x b. Given a demand curve, having price as a function of quantity, p f (x) at height k is the curve f ( x, Clculus for Businss nd Socil Scincs - Prof D Yun Finl Em Rviw vrsion 5/9/7 Chck wbsit for ny postd typos nd updts Pls rport ny typos This rviw sht contins summris of nw topics only (This rviw sht dos hv

More information

ERDOS-SMARANDACHE NUMBERS. Sabin Tabirca* Tatiana Tabirca**

ERDOS-SMARANDACHE NUMBERS. Sabin Tabirca* Tatiana Tabirca** ERDO-MARANDACHE NUMBER b Tbrc* Tt Tbrc** *Trslv Uvrsty of Brsov, Computr cc Dprtmt **Uvrsty of Mchstr, Computr cc Dprtmt Th strtg pot of ths rtcl s rprstd by rct work of Fch []. Bsd o two symptotc rsults

More information

Quantum Mechanics & Spectroscopy Prof. Jason Goodpaster. Problem Set #2 ANSWER KEY (5 questions, 10 points)

Quantum Mechanics & Spectroscopy Prof. Jason Goodpaster. Problem Set #2 ANSWER KEY (5 questions, 10 points) Chm 5 Problm St # ANSWER KEY 5 qustios, poits Qutum Mchics & Spctroscopy Prof. Jso Goodpstr Du ridy, b. 6 S th lst pgs for possibly usful costts, qutios d itgrls. Ths will lso b icludd o our futur ms..

More information

Hydrogen Atom and One Electron Ions

Hydrogen Atom and One Electron Ions Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial

More information

TOPIC 5: INTEGRATION

TOPIC 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 information

Instructions for Section 1

Instructions for Section 1 Instructions for Sction 1 Choos th rspons tht is corrct for th qustion. A corrct nswr scors 1, n incorrct nswr scors 0. Mrks will not b dductd for incorrct nswrs. You should ttmpt vry qustion. No mrks

More information

Minimum Spanning Trees

Minimum Spanning Trees Mnmum Spnnng Trs Spnnng Tr A tr (.., connctd, cyclc grph) whch contns ll th vrtcs of th grph Mnmum Spnnng Tr Spnnng tr wth th mnmum sum of wghts 1 1 Spnnng forst If grph s not connctd, thn thr s spnnng

More information

Chem 104A, Fall 2016, Midterm 1 Key

Chem 104A, Fall 2016, Midterm 1 Key hm 104A, ll 2016, Mitrm 1 Ky 1) onstruct microstt tl for p 4 configurtion. Pls numrt th ms n ml for ch lctron in ch microstt in th tl. (Us th formt ml m s. Tht is spin -½ lctron in n s oritl woul writtn

More information

Grand Canonical Ensemble

Grand Canonical Ensemble Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls

More information

Integration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals

Integration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion

More information

CHAPTER 33: PARTICLE PHYSICS

CHAPTER 33: PARTICLE PHYSICS Collg Physcs Studnt s Manual Chaptr 33 CHAPTER 33: PARTICLE PHYSICS 33. THE FOUR BASIC FORCES 4. (a) Fnd th rato of th strngths of th wak and lctromagntc forcs undr ordnary crcumstancs. (b) What dos that

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 2: Derivation of Ideal MHD Equation

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 2: Derivation of Ideal MHD Equation .65, MHD Thory of Fuson Systms Prof. Frdbrg Lctur : Drvton of Idl MHD Equton Rvw of th Drvton of th Momnt Equton. Strtng Pont: Boltzmnn Equton for lctrons, ons nd Mxwll Equtons. Momnts of Boltzmnn Equton:

More information

ELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware

ELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware LG 43 Lctur #6 Mrk Mirtnik, Ph.D. Prfssr Th Univrsity f Dlwr mil: mirtni@c.udl.du Wv Prpgtin nd Plritin TM: Trnsvrs lctrmgntic Wvs A md is prticulr fild cnfigurtin. Fr givn lctrmgntic bundry vlu prblm,

More information

Linear Algebra Existence of the determinant. Expansion according to a row.

Linear Algebra Existence of the determinant. Expansion according to a row. Lir Algbr 2270 1 Existc of th dtrmit. Expsio ccordig to row. W dfi th dtrmit for 1 1 mtrics s dt([]) = (1) It is sy chck tht it stisfis D1)-D3). For y othr w dfi th dtrmit s follows. Assumig th dtrmit

More information

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization THE UNIVERSITY OF MARYLAND COLLEGE PARK, MARYLAND Economcs 600: August, 007 Dynamc Part: Problm St 5 Problms on Dffrntal Equatons and Contnuous Tm Optmzaton Quston Solv th followng two dffrntal quatons.

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS

MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS VSRT MEMO #05 MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS 01886 Fbrury 3, 009 Tlphon: 781-981-507 Fx: 781-981-0590 To: VSRT Group From: Aln E.E. Rogrs Subjct: Simplifid

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn.

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn. Modul 10 Addtonal Topcs 10.1 Lctur 1 Prambl: Dtrmnng whthr a gvn ntgr s prm or compost s known as prmalty tstng. Thr ar prmalty tsts whch mrly tll us whthr a gvn ntgr s prm or not, wthout gvng us th factors

More information

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören ME 522 PINCIPLES OF OBOTICS FIST MIDTEM EXAMINATION April 9, 202 Nm Lst Nm M. Kml Özgörn 2 4 60 40 40 0 80 250 USEFUL FOMULAS cos( ) cos cos sin sin sin( ) sin cos cos sin sin y/ r, cos x/ r, r 0 tn 2(

More information

Multi-Section Coupled Line Couplers

Multi-Section Coupled Line Couplers /0/009 MultiSction Coupld Lin Couplrs /8 Multi-Sction Coupld Lin Couplrs W cn dd multipl coupld lins in sris to incrs couplr ndwidth. Figur 7.5 (p. 6) An N-sction coupld lin l W typiclly dsign th couplr

More information

A Note on Estimability in Linear Models

A Note on Estimability in Linear Models Intrnatonal Journal of Statstcs and Applcatons 2014, 4(4): 212-216 DOI: 10.5923/j.statstcs.20140404.06 A Not on Estmablty n Lnar Modls S. O. Adymo 1,*, F. N. Nwob 2 1 Dpartmnt of Mathmatcs and Statstcs,

More information

The University of Sydney MATH 2009

The University of Sydney MATH 2009 T Unvrsty o Syny MATH 2009 APH THEOY Tutorl 7 Solutons 2004 1. Lt t sonnt plnr rp sown. Drw ts ul, n t ul o t ul ( ). Sow tt s sonnt plnr rp, tn s onnt. Du tt ( ) s not somorp to. ( ) A onnt rp s on n

More information

Special Random Variables: Part 1

Special Random Variables: Part 1 Spcl Rndom Vrbls: Prt Dscrt Rndom Vrbls Brnoull Rndom Vrbl (wth prmtr p) Th rndom vrbl x dnots th succss from trl. Th probblty mss functon of th rndom vrbl X s gvn by p X () p X () p p ( E[X ]p Th momnt

More information

Folding of Regular CW-Complexes

Folding of Regular CW-Complexes Ald Mathmatcal Scncs, Vol. 6,, no. 83, 437-446 Foldng of Rgular CW-Comlxs E. M. El-Kholy and S N. Daoud,3. Dartmnt of Mathmatcs, Faculty of Scnc Tanta Unvrsty,Tanta,Egyt. Dartmnt of Mathmatcs, Faculty

More information

The Angular Momenta Dipole Moments and Gyromagnetic Ratios of the Electron and the Proton

The Angular Momenta Dipole Moments and Gyromagnetic Ratios of the Electron and the Proton Journl of Modrn hysics, 014, 5, 154-157 ublishd Onlin August 014 in SciRs. htt://www.scir.org/journl/jm htt://dx.doi.org/.436/jm.014.51415 Th Angulr Momnt Diol Momnts nd Gyromgntic Rtios of th Elctron

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

I. The Connection between Spectroscopy and Quantum Mechanics

I. The Connection between Spectroscopy and Quantum Mechanics I. Th Connction twn Spctroscopy nd Quntum Mchnics On of th postults of quntum mchnics: Th stt of systm is fully dscrid y its wvfunction, Ψ( r1, r,..., t) whr r 1, r, tc. r th coordints of th constitunt

More information

Elliptical motion, gravity, etc

Elliptical motion, gravity, etc FW Physics 130 G:\130 lctur\ch 13 Elliticl motion.docx g 1 of 7 11/3/010; 6:40 PM; Lst rintd 11/3/010 6:40:00 PM Fig. 1 Elliticl motion, grvity, tc minor xis mjor xis F 1 =A F =B C - D, mjor nd minor xs

More information

Convergence Theorems for Two Iterative Methods. A stationary iterative method for solving the linear system: (1.1)

Convergence Theorems for Two Iterative Methods. A stationary iterative method for solving the linear system: (1.1) Conrgnc Thors for Two Itrt Mthods A sttonry trt thod for solng th lnr syst: Ax = b (.) ploys n trton trx B nd constnt ctor c so tht for gn strtng stt x of x for = 2... x Bx c + = +. (.2) For such n trton

More information

Limits Indeterminate Forms and L Hospital s Rule

Limits Indeterminate Forms and L Hospital s Rule Limits Indtrmint Forms nd L Hospitl s Rul I Indtrmint Form o th Tp W hv prviousl studid its with th indtrmint orm s shown in th ollowin mpls: Empl : Empl : tn [Not: W us th ivn it ] Empl : 8 h 8 [Not:

More information

ELECTRONIC SUPPLEMENTARY INFORMATION

ELECTRONIC SUPPLEMENTARY INFORMATION Elctronc Supplmntry Mtrl (ESI) or Polymr Cmstry. Ts ournl s T Royl Socty o Cmstry 2015 ELECTRONIC SUPPLEMENTARY INFORMATION Poly(lyln tcont)s An ntrstn clss o polystrs wt proclly loct xo-cn oul ons suscptl

More information

Review - Probabilistic Classification

Review - Probabilistic Classification Mmoral Unvrsty of wfoundland Pattrn Rcognton Lctur 8 May 5, 6 http://www.ngr.mun.ca/~charlsr Offc Hours: Tusdays Thursdays 8:3-9:3 PM E- (untl furthr notc) Gvn lablld sampls { ɛc,,,..., } {. Estmat Rvw

More information

Fractions. Mathletics Instant Workbooks. Simplify. Copyright

Fractions. Mathletics Instant Workbooks. Simplify. Copyright Frctons Stunt Book - Srs H- Smplfy + Mthltcs Instnt Workbooks Copyrht Frctons Stunt Book - Srs H Contnts Topcs Topc - Equvlnt frctons Topc - Smplfyn frctons Topc - Propr frctons, mpropr frctons n mx numbrs

More information

b.) v d =? Example 2 l = 50 m, D = 1.0 mm, E = 6 V, " = 1.72 #10 $8 % & m, and r = 0.5 % a.) R =? c.) V ab =? a.) R eq =?

b.) v d =? Example 2 l = 50 m, D = 1.0 mm, E = 6 V,  = 1.72 #10 $8 % & m, and r = 0.5 % a.) R =? c.) V ab =? a.) R eq =? xmpl : An 8-gug oppr wr hs nomnl mtr o. mm. Ths wr rrs onstnt urrnt o.67 A to W lmp. Th nsty o r ltrons s 8.5 x 8 ltrons pr u mtr. Fn th mgntu o. th urrnt nsty. th rt vloty xmpl D. mm,.67 A, n N 8.5" 8

More information

In which direction do compass needles always align? Why?

In which direction do compass needles always align? Why? AQA Trloy Unt 6.7 Mntsm n Eltromntsm - Hr 1 Complt t p ll: Mnt or s typ o or n t s stronst t t o t mnt. Tr r two typs o mnt pol: n. Wrt wt woul ppn twn t pols n o t mnt ntrtons low: Drw t mnt l lns on

More information

Chapter 16. 1) is a particular point on the graph of the function. 1. y, where x y 1

Chapter 16. 1) is a particular point on the graph of the function. 1. y, where x y 1 Prctic qustions W now tht th prmtr p is dirctl rltd to th mplitud; thrfor, w cn find tht p. cos d [ sin ] sin sin Not: Evn though ou might not now how to find th prmtr in prt, it is lws dvisl to procd

More information

Quasi-Classical States of the Simple Harmonic Oscillator

Quasi-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 information

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density [NWP.19] Radal Cataphorss n Hg-Ar Fluorscnt Lamp schargs at Hgh Powr nsty Y. Aura, G. A. Bonvallt, J. E. Lawlr Unv. of Wsconsn-Madson, Physcs pt. ABSTRACT Radal cataphorss s a procss n whch th lowr onzaton

More information

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d)

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d) Ερωτήσεις και ασκησεις Κεφ 0 (για μόρια ΠΑΡΑΔΟΣΗ 9//06 Th coffcnt A of th van r Waals ntracton s: (a A r r / ( r r ( (c a a a a A r r / ( r r ( a a a a A r r / ( r r a a a a A r r / ( r r 4 a a a a 0 Th

More information

CIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7

CIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7 CIVL / -D Boundr Vlu Prolms - Rctngulr Elmnts / RECANGULAR ELEMENS - In som pplictions, it m mor dsirl to us n lmntl rprsnttion of th domin tht hs four sids, ithr rctngulr or qudriltrl in shp. Considr

More information

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces C465/865, 26-3, Lctur 7, 2 th Sp., 26 lctrochmcal qulbrum lctromotv Forc Rlaton btwn chmcal and lctrc drvng forcs lctrochmcal systm at constant T and p: consdr G Consdr lctrochmcal racton (nvolvng transfr

More information

Outlier-tolerant parameter estimation

Outlier-tolerant parameter estimation Outlr-tolrant paramtr stmaton Baysan thods n physcs statstcs machn larnng and sgnal procssng (SS 003 Frdrch Fraundorfr fraunfr@cg.tu-graz.ac.at Computr Graphcs and Vson Graz Unvrsty of Tchnology Outln

More information

Jones vector & matrices

Jones vector & matrices Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o

More information

CONTINUITY AND DIFFERENTIABILITY

CONTINUITY AND DIFFERENTIABILITY MCD CONTINUITY AND DIFFERENTIABILITY NCERT Solvd mpls upto th sction 5 (Introduction) nd 5 (Continuity) : Empl : Chck th continuity of th function f givn by f() = + t = Empl : Emin whthr th function f

More information

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m hy3: Gnral hyscs III 4/0/008 haptr Worksht lctrc Flds: onsdr a fxd pont charg of 0 µ (q ) q = 0 µ d = 0 a What s th agntud and drcton of th lctrc fld at a pont, a dstanc of 0? q = = 8x0 ˆ o d ˆ 6 N ( )

More information

Wave Phenomena Physics 15c

Wave Phenomena Physics 15c Wv hnon hyscs 5c cur 4 Coupl Oscllors! H& con 4. Wh W D s T " u forc oscllon " olv h quon of oon wh frcon n foun h sy-s soluon " Oscllon bcos lr nr h rsonnc frquncy " hs chns fro 0 π/ π s h frquncy ncrss

More information

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP ISAHP 00, Bal, Indonsa, August -9, 00 COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP Chkako MIYAKE, Kkch OHSAWA, Masahro KITO, and Masaak SHINOHARA Dpartmnt of Mathmatcal Informaton Engnrng

More information

, each of which is a tree, and whose roots r 1. , respectively, are children of r. Data Structures & File Management

, each of which is a tree, and whose roots r 1. , respectively, are children of r. Data Structures & File Management nrl tr T is init st o on or mor nos suh tht thr is on sint no r, ll th root o T, n th rminin nos r prtition into n isjoint susts T, T,, T n, h o whih is tr, n whos roots r, r,, r n, rsptivly, r hilrn o

More information

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D Comp 35 Introducton to Machn Larnng and Data Mnng Fall 204 rofssor: Ron Khardon Mxtur Modls Motvatd by soft k-mans w dvlopd a gnratv modl for clustrng. Assum thr ar k clustrs Clustrs ar not rqurd to hav

More information

8-node quadrilateral element. Numerical integration

8-node quadrilateral element. Numerical integration Fnt Elmnt Mthod lctur nots _nod quadrlatral lmnt Pag of 0 -nod quadrlatral lmnt. Numrcal ntgraton h tchnqu usd for th formulaton of th lnar trangl can b formall tndd to construct quadrlatral lmnts as wll

More information

Chapter 6 Student Lecture Notes 6-1

Chapter 6 Student Lecture Notes 6-1 Chaptr 6 Studnt Lctur Nots 6-1 Chaptr Goals QM353: Busnss Statstcs Chaptr 6 Goodnss-of-Ft Tsts and Contngncy Analyss Aftr compltng ths chaptr, you should b abl to: Us th ch-squar goodnss-of-ft tst to dtrmn

More information

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added 4.3, 4.4 Phas Equlbrum Dtrmn th slops of th f lns Rlat p and at qulbrum btwn two phass ts consdr th Gbbs functon dg η + V Appls to a homognous systm An opn systm whr a nw phas may form or a nw componnt

More information

22 t b r 2, 20 h r, th xp t d bl n nd t fr th b rd r t t. f r r z r t l n l th h r t rl T l t n b rd n n l h d, nd n nh rd f pp t t f r n. H v v d n f

22 t b r 2, 20 h r, th xp t d bl n nd t fr th b rd r t t. f r r z r t l n l th h r t rl T l t n b rd n n l h d, nd n nh rd f pp t t f r n. H v v d n f n r t d n 20 2 : 6 T P bl D n, l d t z d http:.h th tr t. r pd l 22 t b r 2, 20 h r, th xp t d bl n nd t fr th b rd r t t. f r r z r t l n l th h r t rl T l t n b rd n n l h d, nd n nh rd f pp t t f r

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION CHAPTER 7d. DIFFERENTIATION AND INTEGRATION A. J. Clark School o Engnrng Dpartmnt o Cvl and Envronmntal Engnrng by Dr. Ibrahm A. Assakka Sprng ENCE - Computaton Mthods n Cvl Engnrng II Dpartmnt o Cvl and

More information

ψ ij has the eigenvalue

ψ ij has the eigenvalue Moller Plesset Perturbton Theory In Moller-Plesset (MP) perturbton theory one tes the unperturbed Hmltonn for n tom or molecule s the sum of the one prtcle Foc opertors H F() where the egenfunctons of

More information

FSA. CmSc 365 Theory of Computation. Finite State Automata and Regular Expressions (Chapter 2, Section 2.3) ALPHABET operations: U, concatenation, *

FSA. CmSc 365 Theory of Computation. Finite State Automata and Regular Expressions (Chapter 2, Section 2.3) ALPHABET operations: U, concatenation, * CmSc 365 Thory of Computtion Finit Stt Automt nd Rgulr Exprssions (Chptr 2, Sction 2.3) ALPHABET oprtions: U, conctntion, * otin otin Strings Form Rgulr xprssions dscri Closd undr U, conctntion nd * (if

More information

Ch 1.2: Solutions of Some Differential Equations

Ch 1.2: Solutions of Some Differential Equations Ch 1.2: Solutions of Som Diffrntil Equtions Rcll th fr fll nd owl/mic diffrntil qutions: v 9.8.2v, p.5 p 45 Ths qutions hv th gnrl form y' = y - b W cn us mthods of clculus to solv diffrntil qutions of

More information

Optical Bistability in a Two-State Dissipative Medium Inside a Fabry-Perot Cavity

Optical Bistability in a Two-State Dissipative Medium Inside a Fabry-Perot Cavity Egypt. J. olds, Vol. 3, No., 7 63 Optcl stblty n Two-tt Dssptv Mdum nsd bry-prot vty M. M. EL-Ncklwy, A.. Hssn, A. T. Mtr nd H. A. Hf. Physcs Dprtmnt, culty of cnc, Hlwn Unvrsty, Hlwn, ro, Egypt. n ths

More information

5/1/2018. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees

5/1/2018. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees. Huffman Coding Trees /1/018 W usully no strns y ssnn -lnt os to ll rtrs n t lpt (or mpl, 8-t on n ASCII). Howvr, rnt rtrs our wt rnt rquns, w n sv mmory n ru trnsmttl tm y usn vrl-lnt non. T s to ssn sortr os to rtrs tt our

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

ECE COMBINATIONAL BUILDING BLOCKS - INVEST 13 DECODERS AND ENCODERS

ECE COMBINATIONAL BUILDING BLOCKS - INVEST 13 DECODERS AND ENCODERS C 24 - COMBINATIONAL BUILDING BLOCKS - INVST 3 DCODS AND NCODS FALL 23 AP FLZ To o "wll" on this invstition you must not only t th riht nswrs ut must lso o nt, omplt n onis writups tht mk ovious wht h

More information

n r t d n :4 T P bl D n, l d t z d th tr t. r pd l

n r t d n :4 T P bl D n, l d t z d   th tr t. r pd l n r t d n 20 20 :4 T P bl D n, l d t z d http:.h th tr t. r pd l 2 0 x pt n f t v t, f f d, b th n nd th P r n h h, th r h v n t b n p d f r nt r. Th t v v d pr n, h v r, p n th pl v t r, d b p t r b R

More information

Magnetic Suspension System Control Using Jacobian and Input State Linearisation. D. Giaouris, J.W. Finch

Magnetic Suspension System Control Using Jacobian and Input State Linearisation. D. Giaouris, J.W. Finch Mntc Sspnson Systm Control Usn Jcobn n Inpt Stt nrston D. Gors J.W. Fnch School o Elctrcl Elctronc & Comptr Ennrn Unvrsty o Nwcstl pon Tyn Nwcstl pon Tyn NE 7RU UK mls: Dmn.Gors@ncl.c. j.w.nch@ncl.c. BSTRCT

More information

Status and Development of KAERI Atomic Database

Status and Development of KAERI Atomic Database nd Mting o th tomic nd Molculr Dt Cntrs Sttus nd Dvlopmnt o KERI tomic Dtbs D.-H. Kwon Nuclr Dt Cntr Kor tomic Enrgy Rsrch Institut 4 Sptmbr 013 Outlin History Ovrviw Rcnt ctivitis Futur Plns Summry &

More information

Minimum Spanning Trees

Minimum Spanning Trees Minimum Spnning Trs Minimum Spnning Trs Problm A town hs st of houss nd st of rods A rod conncts nd only houss A rod conncting houss u nd v hs rpir cost w(u, v) Gol: Rpir nough (nd no mor) rods such tht:

More information

Basic Electrical Engineering for Welding [ ] --- Introduction ---

Basic Electrical Engineering for Welding [ ] --- Introduction --- Basc Elctrcal Engnrng for Wldng [] --- Introducton --- akayosh OHJI Profssor Ertus, Osaka Unrsty Dr. of Engnrng VIUAL WELD CO.,LD t-ohj@alc.co.jp OK 15 Ex. Basc A.C. crcut h fgurs n A-group show thr typcal

More information

1. Stefan-Boltzmann law states that the power emitted per unit area of the surface of a black

1. Stefan-Boltzmann law states that the power emitted per unit area of the surface of a black Stf-Boltzm lw stts tht th powr mttd pr ut r of th surfc of blck body s proportol to th fourth powr of th bsolut tmprtur: 4 S T whr T s th bsolut tmprtur d th Stf-Boltzm costt= 5 4 k B 3 5c h ( Clcult 5

More information

JEE-2017 : Advanced Paper 2 Answers and Explanations

JEE-2017 : Advanced Paper 2 Answers and Explanations DE 9 JEE-07 : Advancd Papr Answrs and Explanatons Physcs hmstry Mathmatcs 0 A, B, 9 A 8 B, 7 B 6 B, D B 0 D 9, D 8 D 7 A, B, D A 0 A,, D 9 8 * A A, B A B, D 0 B 9 A, D 5 D A, B A,B,,D A 50 A, 6 5 A D B

More information

Definition of vector and tensor. 1. Vector Calculus and Index Notation. Vector. Special symbols: Kronecker delta. Symbolic and Index notation

Definition of vector and tensor. 1. Vector Calculus and Index Notation. Vector. Special symbols: Kronecker delta. Symbolic and Index notation Dfnton of vctor nd tnsor. Vctor Clculus nd Indx Notton Crtsn nsor only Pnton s Chp. Vctor nd ordr tnsor v = c v, v = c v = c c, = c c k l kl kl k l m physcl vrbl, sm symbolc form! Cn b gnrlzd to hghr ordr

More information

4 4 N v b r t, 20 xpr n f th ll f th p p l t n p pr d. H ndr d nd th nd f t v L th n n f th pr v n f V ln, r dn nd l r thr n nt pr n, h r th ff r d nd

4 4 N v b r t, 20 xpr n f th ll f th p p l t n p pr d. H ndr d nd th nd f t v L th n n f th pr v n f V ln, r dn nd l r thr n nt pr n, h r th ff r d nd n r t d n 20 20 0 : 0 T P bl D n, l d t z d http:.h th tr t. r pd l 4 4 N v b r t, 20 xpr n f th ll f th p p l t n p pr d. H ndr d nd th nd f t v L th n n f th pr v n f V ln, r dn nd l r thr n nt pr n,

More information

Having a glimpse of some of the possibilities for solutions of linear systems, we move to methods of finding these solutions. The basic idea we shall

Having a glimpse of some of the possibilities for solutions of linear systems, we move to methods of finding these solutions. The basic idea we shall Hvn lps o so o t posslts or solutons o lnr systs, w ov to tos o nn ts solutons. T s w sll us s to try to sply t syst y lntn so o t vrls n so ts qutons. Tus, w rr to t to s lnton. T prry oprton nvolv s

More information

ELECTRON-MUON SCATTERING

ELECTRON-MUON SCATTERING ELECTRON-MUON SCATTERING ABSTRACT Th lctron charg is considrd to b distributd or xtndd in spac. Th diffrntial of th lctron charg is st qual to a function of lctron charg coordinats multiplid by a four-dimnsional

More information

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time.

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time. Elctroncphalography EEG Dynamc Causal Modllng for M/EEG ampltud μv tm ms tral typ 1 tm channls channls tral typ 2 C. Phllps, Cntr d Rchrchs du Cyclotron, ULg, Blgum Basd on slds from: S. Kbl M/EEG analyss

More information

46 D b r 4, 20 : p t n f r n b P l h tr p, pl t z r f r n. nd n th t n t d f t n th tr ht r t b f l n t, nd th ff r n b ttl t th r p rf l pp n nt n th

46 D b r 4, 20 : p t n f r n b P l h tr p, pl t z r f r n. nd n th t n t d f t n th tr ht r t b f l n t, nd th ff r n b ttl t th r p rf l pp n nt n th n r t d n 20 0 : T P bl D n, l d t z d http:.h th tr t. r pd l 46 D b r 4, 20 : p t n f r n b P l h tr p, pl t z r f r n. nd n th t n t d f t n th tr ht r t b f l n t, nd th ff r n b ttl t th r p rf l

More information

Development of a Heat Transfer Model for the Integrated Façade Heating

Development of a Heat Transfer Model for the Integrated Façade Heating Dvlopmnt of Ht rnsfr Modl for th Intgrtd Fçd Htng Dvd E. Clrdg Phd P.E Xngyng Gong Dvd H. Archr PhD Profssor Grdut tudnt Profssor Enrgy ystms bortory Cntr for Buldng Prformnc nd Dgnostcs Dprtmnt of Mchncl

More information

KOHN LUTTINGER SUPERCONDUCTIVITY IN GRAPHENE

KOHN LUTTINGER SUPERCONDUCTIVITY IN GRAPHENE KOHN LUTTINGER SUPERCONDUCTIITY IN GRAPHENE J. Gonzálz Instituto d Estructur d l Mtri, CSIC, Spin Is it possibl to hv suprconducting instbility in grphn (by suitbl doping)? Thr hv bn lrdy svrl proposls

More information

Dennis Bricker, 2001 Dept of Industrial Engineering The University of Iowa. MDP: Taxi page 1

Dennis Bricker, 2001 Dept of Industrial Engineering The University of Iowa. MDP: Taxi page 1 Denns Brcker, 2001 Dept of Industrl Engneerng The Unversty of Iow MDP: Tx pge 1 A tx serves three djcent towns: A, B, nd C. Ech tme the tx dschrges pssenger, the drver must choose from three possble ctons:

More information

te Finance (4th Edition), July 2017.

te Finance (4th Edition), July 2017. Appndx Chaptr. Tchncal Background Gnral Mathmatcal and Statstcal Background Fndng a bas: 3 2 = 9 3 = 9 1 /2 x a = b x = b 1/a A powr of 1 / 2 s also quvalnt to th squar root opraton. Fndng an xponnt: 3

More information

ON THE COMPLEXITY OF K-STEP AND K-HOP DOMINATING SETS IN GRAPHS

ON THE COMPLEXITY OF K-STEP AND K-HOP DOMINATING SETS IN GRAPHS MATEMATICA MONTISNIRI Vol XL (2017) MATEMATICS ON TE COMPLEXITY OF K-STEP AN K-OP OMINATIN SETS IN RAPS M FARAI JALALVAN AN N JAFARI RA partmnt of Mathmatcs Shahrood Unrsty of Tchnology Shahrood Iran Emals:

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information