Physics, Modeling, and Simulation of the Optical Response of Layers of Semiconductor Nano-Objects. O. Voskoboynikov

Size: px
Start display at page:

Download "Physics, Modeling, and Simulation of the Optical Response of Layers of Semiconductor Nano-Objects. O. Voskoboynikov"

Transcription

1 hyscs Modlg ad Sulato of th Optcal Rspos of Lays of Scoducto Nao-Objcts O. Vosoboyov Dpatt of lctocs gg ad Isttut of lctocs Natoal Chao Tug Uvsty Hschu Tawa Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

2 Outl Itoducto. Why do w sulat th optcs of systs of scoducto ao-objcts? Scoductos th ao-scal. Scoducto ao-objcts Mtaatals ad scoducto ao-objcts Quatu foato ad scoducto ao-objcts Sulato statgy Scoducto ao-objcts. Idvdual ad collctv sposs Mult-Scal Hybd Appoach Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos ffctv Haltoa ad daagtc spos Mappg thod Optcal spos fo systs of scoducto ao-objcts Ba ad dssd polazablty of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts Mast quato Ipltato of th statgy Gal flow daga of th appoach pltato Lays of bddd quatu gs Lays of bddd quatu dot olculs. Magto-llpsoty Th dsoal aays of scoducto ao-objcts Coclusv Ras Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

3 Itoducto Moo's Law: Th ub of tasstos o a chp doubls about vy two yas wda.og A hoto/aul Saua Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

4 Itoducto Th ao - scal s a qualtatvly w scal wh atals popts dpd o sz ad shap as wll as coposto ad dff sgfcatly fo th sa popts th bul Nao-scc ss to udstad ths w popts. Nao-tchology ss to dvlop systs ad stuctus that xhbt ovl popts ad fuctos du to th ao-scal sz Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 4

5 Itoducto Nao-aadg: NANO MANS QUANTUM tyg to fd a coput sulato of physcs ss to to b a xcllt poga to follow out ad I ot happy wth all th aalyss that go wth just th classcal thoy bcaus NATUR ISN T CLASSICAL dat ad f you wat to a a sulato of atu you d btt MAK IT QUANTUM MCHANICAL ad golly t s a wodful pobl bcaus t dos t loo so asy. Rchad Fya Itatoal Joual of Thotcal hyscs Vol. p Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 5

6 Itoducto Scoductos th ao-scal. Scoducto ao-objcts Rlvat lgths scal - Ma f path th quatu Hall g - Ma f path hgh oblty scoductos at T< 4 K - - d Bogl wavlgth scoductos. - d Bogl wavlgth tals dstac btw atos Coft of th lcto oto at last o spatal dso affcts th gy lvls ad th dsty of stats Dt Bbg. Scoducto Naostuctus. Spg 8 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 6

7 Itoducto Scoductos th ao-scal. Scoducto ao-objcts Th-dsoal STM ag of a ucovd IAs quatu dot gow o GaAs. STM ctu Gally lcto Spctoscopy Goup Ftz-Hab-Isttut Bl Atoc soluto STM ag of a stac of slf assbld quatu dots 5x5.. M. Koaad t al. hysca 7 56 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 7

8 Itoducto Scoductos th ao-scal. Scoducto ao-objcts Advacs th fabcato of scoducto ao-stuctus hav allowd us to costuct ao-scal systs wth a wd ag of gots ~5 Slf assbld latal IAs/GaAs Quatu Dot Molcul G. Mũoz-Matutao t al. RB Slf assbld IAs/GaS Quatu Rgs J.M. Gasa at al. 997 Slf assbld vtcal Quatu Dot Molcul M. Bay t al. Scc 9 45 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 8

9 Itoducto Mtaatals ad scoducto ao-objcts Atos Bul Mtaatal ad fo bddd SNOs Bul covtoal atal SNO Quatu wll Quatu w Quatu Dots Quatu Dot Molculs Quatu Dot osts Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa Quatu Rgs tc. Doubl Quatu Rgs 9

10 Itoducto Mtaatals ad scoducto ao-objcts ffctv Mda Dscpto aft V. Vslago966 ablty I A R I A R Mtals < > = No Tassso I A R Covtoal > > = + I A T R ttvty T NRIM < < = - Fts > < = No Tassso Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

11 Itoducto Mtaatals ad scoducto ao-objcts Ngatv factg th Sll s low: Wh < aft V. Vslago 968- ad J.B. dy : hyscs Covtoal Appoxato xact Sll s law Doppl ffct Chov ffct s s s s f ad Fsl Foulas z s cos cos cos cos s z z cos z cos z cos cos O could a w typs of tassso ls flts ad coupls tc. Ad - tly w possblts thos w ca t cogz today Rflcto coffct fo oal cdc o a tfac No flcto codto Bwst law cos ta cos z z z z z z z cos z z ta z cos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

12 Th sufac plaso soac at th sufac fo lctc ad agtc copots lads to a aplfcato of th vasct wavs: ; ; a taatal tfac c c c c y x y x z y x y x z z z Th wavlgth stcto o soluto fo wavs J. B. dy RL a atal - a a taatal - a Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa Itoducto Mtaatals ad scoducto ao-objcts

13 Itoducto Mtaatals ad scoducto ao-objcts fct Ls J. dy Souc NRIM = =- Iag a << Lght Cloa J.B. dy Cotpoay hyscs : J.B.dy D. Schug ad D. R. Sth Scc Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa NRIM Objct

14 Itoducto Mtaatals ad scoducto ao-objcts Most popula ad dct way s to aag a du whch xhbt th lctc Dud ad agtc Lotz dspso latos p ; pm pm I I M R R Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 4

15 Itoducto Mtaatals ad scoducto ao-objcts Fst pltatos Sth D. R. t al. hys. Rv. Ltt R. A. Shlby Scc 9 77 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 5

16 Itoducto Mtaatals ad scoducto ao-objcts Uaxal Mtaatal bult fo IAs/GaAs ao-gs. Ut cll dso: al <<. s-polazd lght / ; 5 5 xx ε yy ; zz xx μ yy ; zz ffctv pttvty ad pablty of th syst. Ral pats of xx ad xx O. Vosoboyov t al. Mcolctocs Joual xx xx yy yy zz zz M M Hz Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 6

17 Itoducto Mtaatals ad scoducto ao-objcts D photoc-taatal stuctus C. M. Sououls ad M. Wg Natu photocs 5 5 Doubl-fsht wth sval lays Mtaatal fabcatd though stacd lctoba lthogaphy Mtaatal ad usg dct-las wtg ad lctoplatg Hypbolc taatalad by lctoplatg hxagoal-hol-aay tplats Mtal dlctc layd taatal Mtaatal fabcatd usg ba pojcto lthogaphy Vsbl gatv-dx taatal basd o a coaxal dsg Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa Mtaatal stuctu aabl to dct las wtg Mtaatal ad usg lag-aa slfassbly All-dlctc gatvdx taatal coposd of two sts of hgh-factv-dx dlctc sphs aagd o a splcubc lattc 7

18 8 zz yy xx zz yy xx ; ε Th Maxwll wav quato fo th lctc fld -copot xp [t-] o-sotopc da Fsl s quato fo th oal ods ε c y z zz y z x z z y z x xx x y z x y x z y xx c c c Uaxal Mda: Hypbolc taatals. Idft dx taatals Itoducto Mtaatals ad scoducto ao-objcts Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

19 Itoducto Mtaatals ad scoducto ao-objcts Fsl s quato fo th oal ods x zz y z xx c xx c oday od OM xx c xtaoday od OM x zz y z xx c xx zz xx zz llpsodal Hypbolc Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 9

20 Itoducto Mtaatals ad scoducto ao-objcts Th optcal so-fqucy sufacs = fo xtaoday ods: z z z x y x y x y llpsodal Mtaatal: xx zz > Typ Hypbolc Mtatatal zz < ; xx > Typ Hypbolc Mtatatal zz > ; xx < Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

21 Itoducto Mtaatals ad scoducto ao-objcts hotoc dsty of stats DOS d dv z d d z d z y x llpsodal Mtaatal x y x y dv c xx zz d Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa Hypbolc Mtatatal :Optcal Topologcal Tasto dv ax ~ ax d DOS

22 Itoducto. Mtaatals ad scoducto ao-objcts Hypbolc taatals o of th ost uusual classs of lctoagtc taatals. Thy dsplay hypbolc o dft dspso whch ogats fo o of th pcpal copots of th lctc o agtc ffctv tso havg th oppost sg to th oth two pcpal copots. Such asotopc stuctud atals xhbt dstctv popts cludg stog hact of spotaous sso dvgg dsty of stats gatv facto ad hacd suplsg ffcts. A. odduby I. Iosh. Blov ad Y. Kvsha Natu photocs Sup dcay volvg hgh- stats of quatu tts wh placd o a typ HMM substat: x d x c 8 a N. S. Hash t al. Scc 6 5 a xx zz d c x y ; d Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

23 Itoducto Mtaatals ad scoducto ao-objcts p xx xx I z z p x z z ; c xx xx zz zz N. S. Hash t al. Scc 6 5 xx Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

24 Itoducto Mtaatals ad scoducto ao-objcts xx zz Mtaatal stuctu cosstg of altatg lays of slv 9 ad ttau doxd TO cospodg to a 9% fll facto of slv Th tasto fo llptcal to hypbolc dspso occus at 6 N. S. Hash t al. Scc 6 5 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 4

25 Itoducto Mtaatals ad scoducto ao-objcts T-solvd photoluscc data fo QDs dpostd o th taatal cotol sapl ad glass substat at 65 6 ad 65 Lft of th QDs as a fucto of wavlgth o taatal cotol sapl ad glass substat N. S. Hash t al. Scc 6 5 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 5

26 - Qubts: -lvl quatu systs - Quatu as: Supposto: taglt Bll's bass: - Qubts a xtly dlcat ;. 6 Itoducto Quatu foato ad scoducto ao-objcts Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

27 σ S ; ; z y x s xp cos - lcto sp s a atual qubt 7 Bloch Sph Itoducto Quatu foato ad scoducto ao-objcts Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

28 Itoducto. Quatu foato ad scoducto ao-objcts - Iso-sp s a atual qubt: Doubl Dot syst Quatu Dot Molcul UD U LD L Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 8

29 9 V dv S y x B l D B C B B z y x B Sgl Quatu Dot Itoducto Quatu foato ad scoducto ao-objcts Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

30 Itoducto. Quatu foato ad scoducto ao-objcts Vtcal Quatu Dot Molcul Sytcal Asytcal B Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

31 Itoducto Quatu foato ad scoducto ao-objcts Vtcal IAs/GaAs Quatu Dot Molcul L = 5 U = 9.5 h L = h U = 4 d = O. Vosoboyov RB 78 8 Two lowst lctoc stats l s Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

32 s l s l f N s l s l s l f B M B M Magtzato agtc ot of th syst wh Magtc suscptblty Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa Itoducto Quatu foato ad scoducto ao-objcts

33 Itoducto Quatu foato ad scoducto ao-objcts Daagtc Qubt Vtcal Quatu Dot Molcul O. Vosoboyov ad C. M. J. Wjs JCTN 7 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

34 4 Quatu Gat cotol Vtcal Quatu Dot Molcul z y x Z Y X Ĥ Η Η X X Itoducto Quatu foato ad scoducto ao-objcts Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

35 Itoducto Quatu foato ad scoducto ao-objcts Th potac of scalablty: Factog of a 4-bt tg ub a asoabl t w d 8 9 physcal qubts Massvly paalll opato ca b achvd by a optcal dsg Quatu dots a plaa optcal cocavty fo th bass of th QuDOS hadwa platfo N. Cody Jos RX 7 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 5

36 Sulato statgy Scoducto ao-objcts. Idvdual ad collctv sposs Statc Idvdual Rspos: polazato la appoxato d SNO d α B SNO α B B Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 6

37 Absopto sso Sulato statgy Scoducto ao-objcts. Idvdual ad collctv sposs Dyac Idvdual Rspos: lght absopto - sso out xctos LD Lass lastc scattg No-pola hotoc Cystals Dyac polazato Actv Mataatals Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 7

38 Sulato statgy Scoducto ao-objcts. Idvdual ad collctv sposs Collctv lctoagtc Rspos I R p s = ta T llpsoty : ost sstv la optcal tchqu Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 8

39 Sulato statgy Mult-Scal Hybd Appoach ASY ffctv Mda Mthod Bud cotuous Lays NOT SO ASY MS Hybd Mthod Bud Lays of SNOs a Taspat Matx Cotus Mda Dsct SNO Cotus Mdu Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 9

40 Sulato statgy Mult-Scal Hybd Appoach To buld up fo th botto fo >> a > d systs Nao Scal Dsct Maco Scal Hybd Maco Scal Cotus Quatu Mchacs of SNO: lcto s gy vlop Fuctos F olazablty of SNO: Dyac α ad Statc α S Itacto quatos: Lays of Dsct Dpols of Stgth d bddd to Cotus Dlctc Matx Rot Flds: R. Optcs Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 4

41 Quatu thoy of D scoducto ao-objcts Mdu ffctv xta pottal V xta SNO Π V cystal g σb Π σv V = Π A B 4 c B A B cystal xta - Boh agto ; Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 4

42 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos H p p p thod th bul 4 c V p σ V cystal = cystal ; Bloch typ soluto Ψ = xp u Bloch typ p Schödg quato H H u = u H π π 4 c σ V cystal ; Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 4

43 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Th fst Bllou zo fo a FCC ad zc bld stuctu lctos Hols Bad Stuctu bul GaAs Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 4

44 44 No-dgat ptubato thoy to th p quato fo a solatd bad a = ; u u : u u u u ' ' ' π π Zcbld ad daod cystals = ad o sp-obt tacto: Oly two bads c ad v lctoc ffctv ass : j j j j j j p p ; ; v c g v c p j g p j u p u Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

45 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Oly two bads c ad v Lght hol ffctv ass : lh j p g j p ~ V g ~ 5 V lh Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 45

46 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Th stadad stat odg fo zcbld ad daod g g Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 46

47 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Mo accuat dscpto o bad paats to b cludd: u C u u Obtal j j Syty u /;+/ S u /;-/ S u /;+/ X Y - g g u 4 /; +/ Z X Y - g u 5 /;-/ Z X Y - g u 6 /;-/ X Y - g u 7 /;/ - g - Z u 8 /; -/ Z X Y - g X Y Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 47

48 48 g z g z g g z g z g z z z C C C H No zo atx lts: x y Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

49 49 Ka s soluto: ffctv asss fo th solutos xpaso a = : ; g g g g g SO g lh hh g g 4 4 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

50 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Bac to -hoogous stuctus ad flds Mdu ffctv xta pottal V xta SNO Π V cystal g σb Π σv V = Π A B 4 c B A cystal xta ; Most coo choc - vlop fucto appoxato to pst wav fuctos ts of th Bloch fuctos u = F u Ψ Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 5

51 5 bul bul a V H H vlop fucto quato th bul a F u F a u xp xp vlop fucto appoxato Ad Lt a vcty of = So: bul a u H xp b bul F u F b u b a u H xp F u F V u Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

52 Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos vlop fucto quato fo lctos a solatd bad b b b * * V F F Mo gal j=xyz j j j V F F V F F Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 5

53 T 8p p p 8 8 F... F F F;F F H cof a S K 8 8 V H H H H H S R S Q U V Q S R S V U S Q Q S R V U R S S Q R V S R R Q S V Q S R S Q U V U V V V U V U U V V A A H * * * * * * * * * * * * * * * * K Ktc pat aul pat Sta pat = =c v y x z y x z y x y x z y x z y x v z y x c A D D D V D U D D D S D D D D R D D D Q D D D D D D 6 A C. yo RB ; plus agtc fld zo pat 5 ght-bad appoxato Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

54 s s q u v q s s v u s q q p s v u s s q p v s q p s v q s s q p u v u v v v u v u u v v v * v * * * * * * * * * * * * * c * * c S a a a a H σ J σ H BB. 4 4 ; sp fo atx sp sp fo atx sp J σ j j j j zz yy xx y x z yz xz xy yy xx yy xx zz w w w D v D u d s d b b q p 6 a v Dvatvs of th local dsplacts statg fo th tfacs th tfac at d d d d yz xz xy xyxy zz xx zz xx yy xx xxyy zz yy xx xxxx a a a a a a wth C C C d F ; δf ; : zo - fld V p z y x 4 xy zx yz 54 ght-bad appoxato. Sta zo ad aul Quatu thoy of D scoducto ao-objcts K thod ad vlop fuctos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

55 If w focus o th cas of th lctos hols w ca obta a ffctv Haltoa fo o copot vlop fucto Mult-bad Schödg quato ojcto oto lcto hol subspac Fouldy-Wouthuys tasfoato ffctv Haltoa fo lctoc vlop fucto wth sp-obt tacto W H H W V H H Ψ Ψ Ψ Ψ h h h h V H H. Ĥ Ĥ A B A Π Π Π σ B σ Π Π g V V V BIA B pzo sta cof d Aada Slva t al. 997 Schäps t al. 998 Vosoboyov t al. s s Π σ Π Π σ Π Sp dpdt bouday codtos 55 Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

56 aats of th thoy fo lctos. g sta cof g sta cof g sta cof g sta cof g sta cof V V g V V V V V V V V 56 Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

57 Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos ffctv Haltoa fo lctoc vlop fucto two bad sp splt Ka Haltoa L. M. Thu ad O. Vosoboyov RB Π A Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 57

58 58 ffctv Haltoa fo hol vlop fuctos fou-bad Luttg-Koh Haltoa { } - st of th Luttg paats * * * * I H h h V R S R S S R S R. hz h h hz h S R hy hx h hy hx h h A Π Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

59 Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos lctoc stats two copot spo vlop fucto F F F S S Ĥ F F F F Hol stats fou copot spo vlop fucto Chalty: = Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 59

60 Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos xctoc ffcts xctoc Haltoa Th G s fucto of th osso quato xctoc vlop wav fucto xctoc tasto gs Coffcts xctoc pstato dt G h g h g x j Gj a j j x [ G ] h a [ h h ] x j j Wh: G j J z J ' z F [ l V F J z ; J ' h; h' ' l' z ' V ] J z ; J ' h; h' F z J h ' z d F J ' h' z ' *COMSOL Multphyscs FM solvs Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 6

61 6 z B B Magtc fld dpdt ts th Haltoa: B y x B g S S L L B S L ; ; 8 H Magtc fld as a ptubato lads to: y x B g g B B 8 ' ' ' S L B S L B paaagtc daagtc O: j j B V V g q q S B A p A p H Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

62 Gaug-og dpdt dfto: Π Π H h h h h h V A Π h h q B A B A * d h h h Gaug-og dpdt daagtc coffct B z: 8 B h h h h ρ ρ y x ρ B A 6 Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

63 Quatu thoy of D scoducto ao-objcts ffctv Haltoa ad daagtc spos Quatu Dot Atfcal ato Idal so-scal g O-dsoal loop >5 yas of th Ahaoov-Boh ffct Quatu Rg B B B B l C B Dl B l ; l B l F S B Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa h Sgatu of th AB ffct ~ S B h ;

64 Quatu thoy of D scoducto ao-objcts Mappg thod Flow daga of th appg pocdu Fo a ao-objct of coplx goty paats to ap V ; g ; ; ; ; C j;l 4 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 64

65 Quatu thoy of D scoducto ao-objcts Mappg thod hoto sso lcto Mcoscopy M Coss-sctoal tassso lcto coscopy XTM Atoc Foc Mcoscopy AFM Klv ob Foc Mcoscopy KFM Coss-sctoal scag tul Mcoscopy XSTM xapl: IAs/GaAs ao-g XSTM. Offas t al. AL Nao objct s goty pofl h x y ffctv lctoc hol s coft pottal x hxy y Vff [ x y z h x y] V ax outsd Vff V sd V V lctoc C ax bad offst Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 65

66 66 Cappd wobbld IxGa x As/GaAs x slf-assbld quatu g. xapl of th hght pofl - hxy. ; R y x R y x h y x y x h h y x h R y x R y x R y x R R h y x y x h h y x h M M Quatu thoy of D scoducto ao-objcts Mappg thod Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

67 osto dpdt coductg bad offst: 4 Δ a y x h z T a z s T V h h Tx = tahx h = hout h 67 Utlss appg fucto V M Mappd paats... ; ; ; ; ; ; M M M M M M V M V M M M M M M M V out out out g out g h out out out g g g aats of th thoy... ; ; ; ; ; ; h h h g g V Quatu thoy of D scoducto ao-objcts Mappg thod Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

68 Quatu thoy of D scoducto ao-objcts Mappg thod Stad IAs sd gias =.84 V Δ IAs =.9 V IAs =.44 ₀ hias =.74 g hias =. ad IAs = 5. GaAs atx outsd ggaas =.5 V Δ GaAs =.4 V GaAs =.67 ₀ hgaas =.5 g hgaas =.6 ad = GaAs =. ojctos of th lcto V ad hol V h coft pottals o th xrz pla wth th actual gy gap btw O. Vosoboyov t al. RB Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 68

69 Quatu thoy of D scoducto ao-objcts Mappg thod C. Ka t al. AL V V x z Vtcal IAs/GaAs Quatu Dot Molcul ojctos of th lcto V coft pottals o th xz pla Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 69

70 Optcal spos fo systs of scoducto ao-objcts Ba ad dssd polazablty of scoducto ao-objcts Mda d SNO Icog lght ba: Th dpol stgth Dsct Dpol Appoxato d V SNO d th la thoy fo th spos fuctos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 7

71 Optcal spos fo systs of scoducto ao-objcts Ba ad dssd polazablty of scoducto ao-objcts α Dsct Dpol Appoxato >> a > d fo SNOs Vosoboyov t al. RB 5-9 olazablty Tso B ω Statc pat = α Mda SNO S B + α D Dyac pat ω Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa d Dpol stgth Bul optcal atx lt Ba xcss bddd polazablty B f d α B A Appld lctc fld vlop fucto Ovlap tgal * T x h h x Fqucy dpdt facto f x 7

72 Optcal spos fo systs of scoducto ao-objcts Ba ad dssd polazablty of scoducto ao-objcts d α B A Actual Local fld Spatal avag SNO calculatd th thoy d α D L xtal ot fld asud xpts Ba polazablty A = L + td bdd Dssd polazablty Local fld x th cas of a sgl SNO lctoagtc tasf tso dpolazato Accodg to th dftos: α α B D t Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 7

73 Optcal spos fo systs of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts Syst of bddd SNOs th la DDA Th local fld at th posto of th th dpol = fjd j L X + Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 7

74 Optcal spos fo systs of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts d D ε so ε T j ε j f j G xp Δ Itcllula tasf tso Dyadc G Fucto Δ T j T I I j j j j 4 Δ j Δ j j j ; j ; j c I a statc ag: >>a > >d I fa wav ag >> >>a >d I T xp Δ G j T j j G I j ; 4 Δ 4 Δ T j j j Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 74

75 Optcal spos fo systs of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts. Mast quato Th syst s Mast quato T R R T G T X T G T d R Th syst s collctv spos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa d d j t T wh T j t Dj j d O Xj j f j d f t s j 6 c Xj j t α B j I Bj α D Dso: N Lotz adato dapg 75

76 Optcal spos fo systs of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts. Mast quato Rflcto ad tassso R = F d wh z T = F d wh z X T Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 76

77 Optcal spos fo systs of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts. Mast quato Fo a sgl bddd SNO solv: Spatal avag calculatd SNO Fo th bouday codtos Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 77

78 Optcal spos fo systs of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts. Mast quato Two-dsoal squa lattc a lay of SNOs of th lattc paat a L : th Vlg s soluto J. Vlg hysca th Vlg s ot tplaa tasf tso z z Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 78

79 Optcal spos fo systs of scoducto ao-objcts lctoagtc tacto btw scoducto ao-objcts. Mast quato Th flcto sp ad tassso t sp coffcts flctac R sp tasttac T sp ad absobac A sp of th lay R A s p s p s p ; R T T s p s p p s = ta Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 79

80 Ipltato of th statgy Gal flow daga of th appoach pltato Scal of a Idvdual Nao-Objct Scal of Maco-Systs of Nao-Objcts Laplac quato Statc xcss olazablts S α S D α B Slf Itacto Tso S t Shödg quato H h F h h F h Tasto gs ad Ovlap Itgals x Ψ Ψ Φ l h l Ovall bddd Ba olazablty α S B Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa Mult-Dpol Itacto quato Mast quato C R T abs j T j d G j G Optcs :.g. Fsl's X Absopto 4 d l * l coffcts coss d } d N l d scto Id d l X α Dl * 8 d * l

81 Ipltato of th statgy Lays of bddd quatu gs Tasto gs of th IAs/GaAs dots ad gs R = O. Vosoboyov t al. RB ; C. M. J. Wjs t al. RB ; pssc 78 6 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 8

82 Ipltato of th statgy Lays of bddd quatu gs llpsoty fo =6 ad = 5 V o bddd a L =8 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 8

83 Ipltato of th statgy Lays of bddd quatu gs llpsoty fo =6 = 5 V ad a L = 8 ; Dashd- o bddd Sold -bddd Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 8

84 Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty Ka t al. AL p lays of IAs QD's flctos ŝ ΔR 6 5 xpt ΔR Th Mthod Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 84

85 Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty B B Lag Dot lctoc bad Sall Dot Hol bad B B B C B B Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 85

86 Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa L. M. Thu ad O. Vosoboyov RB ; hysca

87 Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty B * T x h h f Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 87

88 Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 88

89 8 - dg 8 - dg dg dg Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty Icdc of = 6º = V ttdot dstac - ; N = c - B z Bz Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 89

90 Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty Icdc of = 6º = V ttdot dstac - ; N = c - B z Bz Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 9

91 Ipltato of th statgy Lays of bddd quatu dot olculs. Magto-llpsoty Icdc of = 6º ttdot dstac - ; N = c - Ap BT V BT V = V = 5 V Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 9

92 Ipltato of th statgy Th dsoal aays of scoducto ao-objcts Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

93 Ipltato of th statgy Th dsoal aays of scoducto ao-objcts opagato Matx Appoach Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa ad tatvly apply to + lays 9

94 Ipltato of th statgy Th dsoal aays of scoducto ao-objcts Rflctac of quatu dot ultlayd stuctus ad 5 lays as fucto o th optcal tasto gy ad agl of cdc d dstac btw lays L. M. Thu ad O. Vosoboyov JCS 45 7 Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa

95 Ipltato of th statgy Th dsoal aays of scoducto ao-objcts Scal of a Idvdual Nao-Objct Scal of Maco-Systs of Nao-Objcts Laplac quato Shödg quato H F h h h F h ffctv Clausus-Mossott suscptblty I D Statc xcss Tasto gs ad olazablts Ovlap Itgals S l Fh F α S l D α ffctv pttvty B χ QDM N α N α D Slf Itacto Tso S t Ovall bddd Ba olazablty α S B ε I χ QDM Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa L. M. Thu ad O. Vosoboyov AI Cof. oc

96 R xx / I xx / Ipltato of th statgy Th dsoal aays of scoducto ao-objcts Itdot dstac - ; N =.6 6 c - ; B z xx yy zz Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 96

97 R xx / I xx / Ipltato of th statgy Th dsoal aays of scoducto ao-objcts Itdot dstac - ; N =.6 6 c - ; B z Itatoal Woshop o Modlg ad Sulato of Scoducto Naostuctus ad gy Nao-Dvcs 4/7/5 Tohou Uvsty Sda Japa 97

98 Coclusv Ras Mult-scal hybd thod s a w labl ad posg appoach to sulatos of optcal popts of scoducto ao-stuctud taatals Th thod cobs dsct ad cotuu dscptos th ao ad aco scals Th thod allows us to oto coht apulatos of lctoc quatu stats scoducto ao-objcts by th covtoal optcal tchqus Ou calculato sults claly suggst asuabl valus fo chags of th ffctv pttvty of D aays of SNOs. 98

99 Tha You! 99

Today s topics. How did we solve the H atom problem? CMF Office Hours

Today s topics. How did we solve the H atom problem? CMF Office Hours CMF Offc ous Wd. Nov. 4 oo-p Mo. Nov. 9 oo-p Mo. Nov. 6-3p Wd. Nov. 8 :30-3:30 p Wd. Dc. 5 oo-p F. Dc. 7 4:30-5:30 Mo. Dc. 0 oo-p Wd. Dc. 4:30-5:30 p ouly xa o Th. Dc. 3 Today s topcs Bf vw of slctd sults

More information

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines Ogs of Quatu Thoy Masuts of sso of lght (EM adato) fo (H) atos foud dsct ls 5 4 Abl to ft to followg ss psso ν R λ c λwavlgth, νfqucy, cspd lght RRydbg Costat (~09,7677.58c - ),,, +, +,..g.,,.6, 0.6, (Lya

More information

In the name of Allah Proton Electromagnetic Form Factors

In the name of Allah Proton Electromagnetic Form Factors I th a of Allah Poto Elctoagtc o actos By : Maj Hazav Pof A.A.Rajab Shahoo Uvsty of Tchology Atoc o acto: W cos th tactos of lcto bas wth atos assu to b th gou stats. Th ct lcto ay gt scatt lastcally wth

More information

Control Systems. Lecture 8 Root Locus. Root Locus. Plant. Controller. Sensor

Control Systems. Lecture 8 Root Locus. Root Locus. Plant. Controller. Sensor Cotol Syt ctu 8 Root ocu Clacal Cotol Pof. Eugo Schut hgh Uvty Root ocu Cotoll Plat R E C U Y - H C D So Y C C R C H Wtg th loo ga a w a ttd tackg th clod-loo ol a ga va Clacal Cotol Pof. Eugo Schut hgh

More information

Homework 1: Solutions

Homework 1: Solutions Howo : Solutos No-a Fals supposto tst but passs scal tst lthouh -f th ta as slowss [S /V] vs t th appaac of laty alty th path alo whch slowss s to b tat to obta tavl ts ps o th ol paat S o V as a cosquc

More information

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom Today s topic Sttig up th Hydog Ato pobl Hydog ato pobl & Agula Motu Objctiv: to solv Schödig quatio. st Stp: to dfi th pottial fuctio Schatic of Hydog Ato Coulob s aw - Z 4ε 4ε fo H ato Nuclus Z What

More information

Handout 7. Properties of Bloch States and Electron Statistics in Energy Bands

Handout 7. Properties of Bloch States and Electron Statistics in Energy Bands Hdout 7 Popts of Bloch Stts d Elcto Sttstcs Eg Bds I ths lctu ou wll l: Popts of Bloch fuctos Podc boud codtos fo Bloch fuctos Dst of stts -spc Elcto occupto sttstcs g bds ECE 407 Spg 009 Fh R Coll Uvst

More information

Chapter 6. pn-junction diode: I-V characteristics

Chapter 6. pn-junction diode: I-V characteristics Chatr 6. -jucto dod: -V charactrstcs Tocs: stady stat rsos of th jucto dod udr ald d.c. voltag. ucto udr bas qualtatv dscusso dal dod quato Dvatos from th dal dod Charg-cotrol aroach Prof. Yo-S M Elctroc

More information

Phys Nov. 3, 2017 Today s Topics. Continue Chapter 2: Electromagnetic Theory, Photons, and Light Reading for Next Time

Phys Nov. 3, 2017 Today s Topics. Continue Chapter 2: Electromagnetic Theory, Photons, and Light Reading for Next Time Phys 31. No. 3, 17 Today s Topcs Cou Chap : lcomagc Thoy, Phoos, ad Lgh Radg fo Nx Tm 1 By Wdsday: Radg hs Wk Fsh Fowls Ch. (.3.11 Polazao Thoy, Jos Macs, Fsl uaos ad Bws s Agl Homwok hs Wk Chap Homwok

More information

Lecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t

Lecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t Cla ot fo EE6318/Phy 6383 Spg 001 Th doumt fo tutoal u oly ad may ot b opd o dtbutd outd of EE6318/Phy 6383 tu 7 Dffuo Ou flud quato that w dvlopd bfo a: f ( )+ v v m + v v M m v f P+ q E+ v B 13 1 4 34

More information

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform NANO 70-Nots Chapt -Diactd bams Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio. Idal cystals a iiit this, so th will b som iiitis lii about. Usually, th iiit quatity oly ists

More information

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures Chpt Rcpocl Lttc A mpott cocpt o lyzg podc stuctus Rsos o toducg cpocl lttc Thoy o cystl dcto o x-ys, utos, d lctos. Wh th dcto mxmum? Wht s th tsty? Abstct study o uctos wth th podcty o Bvs lttc Fou tsomto.

More information

Development of indirect EFBEM for radiating noise analysis including underwater problems

Development of indirect EFBEM for radiating noise analysis including underwater problems csnk 03 It. J. Naval cht. Oca E. 03 5:39~403 http://dx.do.o/0.478/ijnoe-03-04 Dvlopmt of dct EFBEM fo adat os aalyss clud udwat poblms Hyu-Wu Kwo Su-Yoo Ho ad J-Hu So 3 Rsach Isttut of Ma Systms E RIMSE

More information

6.012 Electronic Devices and Circuits Formula Sheet for Final Exam, Fall q = 1.6x10 19 Coul III IV V = x10 14 o. = 3.

6.012 Electronic Devices and Circuits Formula Sheet for Final Exam, Fall q = 1.6x10 19 Coul III IV V = x10 14 o. = 3. 6.0 Elctc Dvcs ad Ccuts ula Sht f al Exa, all 003 Paat Valus: Pdc Tabl: q.6x0 9 Cul III IV V 8.854 x0 4 /c,,s.7,,so 3.9 B C N 0 S /c, SO 3.5 x0 3 /c Al S P [S@R.T] 0 0 c 3 Ga G As /q 0.05 V ; ( /q) l0

More information

Handout 30. Optical Processes in Solids and the Dielectric Constant

Handout 30. Optical Processes in Solids and the Dielectric Constant Haut Otal Sl a th Dlt Ctat I th ltu yu wll la: La ut Ka-Kg lat Dlt tat l Itba a Itaba tbut t th lt tat l C 47 Sg 9 Faha Raa Cll Uty Chag Dl, Dl Mt, a lazat Dty A hag l t a gat a a t hag aat by ta: Q Q

More information

SIMULTANEOUS METHODS FOR FINDING ALL ZEROS OF A POLYNOMIAL

SIMULTANEOUS METHODS FOR FINDING ALL ZEROS OF A POLYNOMIAL Joual of athmatcal Sccs: Advacs ad Applcatos Volum, 05, ags 5-8 SIULTANEUS ETHDS FR FINDING ALL ZERS F A LYNIAL JUN-SE SNG ollg of dc Yos Uvsty Soul Rpublc of Koa -mal: usopsog@yos.ac. Abstact Th pupos

More information

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane.

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane. CBSE CBSE SET- SECTION. Gv tht d W d to fd 7 7 Hc, 7 7 7. Lt,. W ow tht.. Thus,. Cosd th vcto quto of th pl.. z. - + z = - + z = Thus th Cts quto of th pl s - + z = Lt d th dstc tw th pot,, - to th pl.

More information

The real E-k diagram of Si is more complicated (indirect semiconductor). The bottom of E C and top of E V appear for different values of k.

The real E-k diagram of Si is more complicated (indirect semiconductor). The bottom of E C and top of E V appear for different values of k. Modr Smcoductor Dvcs for Itgratd rcuts haptr. lctros ad Hols Smcoductors or a bad ctrd at k=0, th -k rlatoshp ar th mmum s usually parabolc: m = k * m* d / dk d / dk gatv gatv ffctv mass Wdr small d /

More information

Course 10 Shading. 1. Basic Concepts: Radiance: the light energy. Light Source:

Course 10 Shading. 1. Basic Concepts: Radiance: the light energy. Light Source: Cour 0 Shadg Cour 0 Shadg. Bac Coct: Lght Sourc: adac: th lght rg radatd from a ut ara of lght ourc or urfac a ut old agl. Sold agl: $ # r f lght ourc a ot ourc th ut ara omttd abov dfto. llumato: lght

More information

k of the incident wave) will be greater t is too small to satisfy the required kinematics boundary condition, (19)

k of the incident wave) will be greater t is too small to satisfy the required kinematics boundary condition, (19) TOTAL INTRNAL RFLTION Kmacs pops Sc h vcos a coplaa, l s cosd h cd pla cocds wh h X pla; hc 0. y y y osd h cas whch h lgh s cd fom h mdum of hgh dx of faco >. Fo cd agls ga ha h ccal agl s 1 ( /, h hooal

More information

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential Istumtatio o Chaactizatio o Naomatials (v). Cystal Pottial Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio om cystal. Idal cystals a iiit this, so th will b som iiitis lii

More information

Noise in electronic components.

Noise in electronic components. No lto opot5098, JDS No lto opot Th PN juto Th ut thouh a PN juto ha fou opot t: two ffuo ut (hol fo th paa to th aa a lto th oppot to) a thal at oty ha a (hol fo th aa to th paa a lto th oppot to, laka

More information

Ch. 6 Free Electron Fermi Gas

Ch. 6 Free Electron Fermi Gas Ch. 6 lcto i Gas Coductio lctos i a tal ov fl without scattig b io cos so it ca b cosidd as if walitactig o f paticls followig idiac statistics. hfo th coductio lctos a fqutl calld as f lcto i gas. Coductio

More information

VISUALIZATION OF TRIVARIATE NURBS VOLUMES

VISUALIZATION OF TRIVARIATE NURBS VOLUMES ISUALIZATIO OF TRIARIATE URS OLUMES SAMUELČÍK Mat SK Abstact. I ths pap fcs patca st f f-f bcts a ts sazat. W xt appach f g cs a sfacs a ppa taat s bas z a -sp xpsss. O a ga s t saz g paatc s. Th sazat

More information

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find BSE SMLE ER SOLUTONS LSS-X MTHS SET- BSE SETON Gv tht d W d to fd 7 7 Hc, 7 7 7 Lt, W ow tht Thus, osd th vcto quto of th pl z - + z = - + z = Thus th ts quto of th pl s - + z = Lt d th dstc tw th pot,,

More information

International Journal of Advanced Scientific Research and Management, Volume 3 Issue 11, Nov

International Journal of Advanced Scientific Research and Management, Volume 3 Issue 11, Nov 199 Algothm ad Matlab Pogam fo Softwa Rlablty Gowth Modl Basd o Wbull Od Statstcs Dstbuto Akladswa Svasa Vswaatha 1 ad Saavth Rama 2 1 Mathmatcs, Saaatha Collg of Egg, Tchy, Taml Nadu, Ida Abstact I ths

More information

Ch. 8: Electron Levels In Periodic Potential

Ch. 8: Electron Levels In Periodic Potential C. 8: Elto Lvls I Pod Pottal Wat a t oss of a pod pottal o t fo of t wav ftos sptv of t xat fo of t pottal ad sptv of wt t atal s a odto o a slato? s t fftv olto pottal. Blo s To: T gstats of t o-lto altoa

More information

CPT-Frames for PT-symmetric Hamiltonians

CPT-Frames for PT-symmetric Hamiltonians -a fo P-ytc Haltoa Hua-X Cao Zh-Hua Guo Zhg-L Ch Collg of athatc ad Ifoato Scc Shaax Noal Uvty X'a 76 Cha al: caohx@uduc Abtact: P-ytc quatu chac a altatv foulato of quatu chac whch th athatcal axo of

More information

Part I- Wave Reflection and Transmission at Normal Incident. Part II- Wave Reflection and Transmission at Oblique Incident

Part I- Wave Reflection and Transmission at Normal Incident. Part II- Wave Reflection and Transmission at Oblique Incident Apl 6, 3 Uboudd Mda Gudd Mda Chap 7 Chap 8 3 mls 3 o 3 M F bad Lgh wavs md by h su Pa I- Wav Rlo ad Tasmsso a Nomal Id Pa II- Wav Rlo ad Tasmsso a Oblqu Id Pa III- Gal Rlao Bw ad Wavguds ad Cavy Rsoao

More information

Statistical Thermodynamics Essential Concepts. (Boltzmann Population, Partition Functions, Entropy, Enthalpy, Free Energy) - lecture 5 -

Statistical Thermodynamics Essential Concepts. (Boltzmann Population, Partition Functions, Entropy, Enthalpy, Free Energy) - lecture 5 - Statstcal Thrmodyamcs sstal Cocpts (Boltzma Populato, Partto Fuctos, tropy, thalpy, Fr rgy) - lctur 5 - uatum mchacs of atoms ad molculs STATISTICAL MCHANICS ulbrum Proprts: Thrmodyamcs MACROSCOPIC Proprts

More information

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r.

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r. Statcs Th cotact btw a mapulato ad ts vomt sults tactv ocs ad momts at th mapulato/vomt tac. Statcs ams at aalyzg th latoshp btw th actuato dv tous ad th sultat oc ad momt appld at th mapulato dpot wh

More information

Department of Mathematics and Statistics Indian Institute of Technology Kanpur MSO202A/MSO202 Assignment 3 Solutions Introduction To Complex Analysis

Department of Mathematics and Statistics Indian Institute of Technology Kanpur MSO202A/MSO202 Assignment 3 Solutions Introduction To Complex Analysis Dpartmt of Mathmatcs ad Statstcs Ida Isttut of Tchology Kapur MSOA/MSO Assgmt 3 Solutos Itroducto To omplx Aalyss Th problms markd (T) d a xplct dscusso th tutoral class. Othr problms ar for hacd practc..

More information

Magnetic effects and the peculiarity of the electron spin in Atoms

Magnetic effects and the peculiarity of the electron spin in Atoms Magtic ffcts ad t pculiaity of t lcto spi i Atos Pit Za Hdik otz Nobl Piz 90 Otto t Nobl 9 Wolfgag Pauli Nobl 95 ctu Nots tuctu of Matt: Atos ad Molculs; W. Ubacs T obital agula otu of a lcto i obit iclassical

More information

Computational Material Chemistry. Kaito Takahashi Institute of Atomic and Molecular Sciences,

Computational Material Chemistry. Kaito Takahashi Institute of Atomic and Molecular Sciences, Coputatoal ateal Chesty Kato Takahash sttute of Atoc ad olecula Sceces kt@gate.sca.edu.tw A Udestad the basc theoy behd quatu chesty calculato Lea ug quatu chesty poga Udestad what the output s sayg Get

More information

IFYFM002 Further Maths Appendix C Formula Booklet

IFYFM002 Further Maths Appendix C Formula Booklet Ittol Foudto Y (IFY) IFYFM00 Futh Mths Appd C Fomul Booklt Rltd Documts: IFY Futh Mthmtcs Syllbus 07/8 Cotts Mthmtcs Fomul L Equtos d Mtcs... Qudtc Equtos d Rmd Thom... Boml Epsos, Squcs d Ss... Idcs,

More information

The tight-binding method

The tight-binding method Th tight-idig thod Wa ottial aoach: tat lcto a a ga of aly f coductio lcto. ow aout iulato? ow aout d-lcto? d Tight-idig thod: gad a olid a a collctio of wa itactig utal ato. Ovla of atoic wav fuctio i

More information

Compact Tripple U-Shaped Slot Loaded Circular Disk Patch Antenna for Bluetooth and WLAN Application

Compact Tripple U-Shaped Slot Loaded Circular Disk Patch Antenna for Bluetooth and WLAN Application 9 VOL.6, NO., MACH Compact ppl U-Shapd Slot Loadd Ccula Dsk Patch Ata fo Blutooth ad WLAN Applcato J. A. Asa, Auag Msha, N. P. Yadav, P. Sgh, B.. Vshvakama Dpatmt of Elctocs & Commucato Uvsty of Allahabad,

More information

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch Solid stat physics Lctu 3: chmical bonding Pof. D. U. Pitsch Elcton chag dnsity distibution fom -ay diffaction data F kp ik dk h k l i Fi H p H; H hkl V a h k l Elctonic chag dnsity of silicon Valnc chag

More information

A study on Ricci soliton in S -manifolds.

A study on Ricci soliton in S -manifolds. IO Joual of Mathmatc IO-JM -IN: 78-578 p-in: 9-765 olum Iu I Ja - Fb 07 PP - wwwojoualo K dyavath ad Bawad Dpatmt of Mathmatc Kuvmpu vtyhaaahatta - 577 5 hmoa Kaataa Ida Abtact: I th pap w tudy m ymmtc

More information

ALPHABET. 0Letter Practice

ALPHABET. 0Letter Practice ALPHABET 0Ltt Pat Ltt Pat - Aa A A A A a a a Cl A s A a a A A Cl a s A a k Aa a Cut ut th ltt s a glu thm th ght st. Catal A Las a 2014 Lau Thms.msthmsstasus.m a a A a A A Ltt Pat - B B B B B Cl B s m

More information

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles ENGG 03 Tutoial Systms ad Cotol 9 Apil Laig Obctivs Z tasfom Complx pols Fdbac cotol systms Ac: MIT OCW 60, 6003 Diffc Equatios Cosid th systm pstd by th followig diffc quatio y[ ] x[ ] (5y[ ] 3y[ ]) wh

More information

The Hydrogen Atom. Chapter 7

The Hydrogen Atom. Chapter 7 Th Hyog Ato Chapt 7 Hyog ato Th vy fist pobl that Schöig hislf tackl with his w wav quatio Poucig th oh s gy lvls a o! lctic pottial gy still plays a ol i a subatoic lvl btw poto a lcto V 4 Schöig q. fo

More information

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables Sogklaaka J. Sc. Tchol. 4 () 4-48 Ma. -. 8 Ogal tcl Nw bouds o Posso aomato to th dstbuto of a sum of gatv bomal adom vaabls * Kat Taabola Datmt of Mathmatcs Faculty of Scc Buaha Uvsty Muag Chobu 3 Thalad

More information

Estimating the Variance in a Simulation Study of Balanced Two Stage Predictors of Realized Random Cluster Means Ed Stanek

Estimating the Variance in a Simulation Study of Balanced Two Stage Predictors of Realized Random Cluster Means Ed Stanek Etatg th Varac a Sulato Study of Balacd Two Stag Prdctor of Ralzd Rado Clutr Ma Ed Stak Itroducto W dcrb a pla to tat th varac copot a ulato tudy N ( µ µ W df th varac of th clutr paratr a ug th N ulatd

More information

Numerical Method: Finite difference scheme

Numerical Method: Finite difference scheme Numrcal Mthod: Ft dffrc schm Taylor s srs f(x 3 f(x f '(x f ''(x f '''(x...(1! 3! f(x 3 f(x f '(x f ''(x f '''(x...(! 3! whr > 0 from (1, f(x f(x f '(x R Droppg R, f(x f(x f '(x Forward dffrcg O ( x from

More information

3. Anomalous magnetic moment

3. Anomalous magnetic moment 3. Anolos gntc ont 3.1 Mgntc ont of th lcton: Dc qton wth lcton colng to lcto-gntc t fld: D A A D ψ 0 cnoncl ont Anstz fo th solton s fo f tcl: t t Χ Φ Φ Χ 0 A 0 A Χ Φ 0 Χ Φ χ ϕ x x 4 Non-ltvstc lt: E,

More information

Nuclear Chemistry -- ANSWERS

Nuclear Chemistry -- ANSWERS Hoor Chstry Mr. Motro 5-6 Probl St Nuclar Chstry -- ANSWERS Clarly wrt aswrs o sparat shts. Show all work ad uts.. Wrt all th uclar quatos or th radoactv dcay srs o Urau-38 all th way to Lad-6. Th dcay

More information

UvA-VU Master Course: Advanced Solid State Physics

UvA-VU Master Course: Advanced Solid State Physics UvA-U Maste ouse: Advaced Sold State Pyscs otets 005: Dffacto fo peodc stuctues wee 6, Ad lectoc bad stuctue of solds wee 7, Ad Moto of electos ad taspot peoea wee 8, Ad Supecoductvty wee 9&10, RW Magets

More information

READ T H E DATE ON LABEL A blue m a r k a r o u n d this notice will call y o u r attention to y o u r LOWELL. MICHIGAN, THURSDAY, AUGUST 29.

READ T H E DATE ON LABEL A blue m a r k a r o u n d this notice will call y o u r attention to y o u r LOWELL. MICHIGAN, THURSDAY, AUGUST 29. B U D D B < / UDY UU 29 929 VU XXXV Y B 5 2 $25 25 25 U 6 B j 3 $8 D D D VD V D D V D B B % B 2 D - Q 22: 5 B 2 3 Z D 2 5 B V $ 2 52 2 $5 25 25 $ Y Y D - 8 q 2 2 6 Y U DD D D D Y!! B D V!! XU XX D x D

More information

Weights Interpreting W and lnw What is β? Some Endnotes = n!ω if we neglect the zero point energy then ( )

Weights Interpreting W and lnw What is β? Some Endnotes = n!ω if we neglect the zero point energy then ( ) Sprg Ch 35: Statstcal chacs ad Chcal Ktcs Wghts... 9 Itrprtg W ad lw... 3 What s?... 33 Lt s loo at... 34 So Edots... 35 Chaptr 3: Fudatal Prcpls of Stat ch fro a spl odl (drvato of oltza dstrbuto, also

More information

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

ELECTROMAGNETISM, NUCLEAR STRUCTURES & GRAVITATION

ELECTROMAGNETISM, NUCLEAR STRUCTURES & GRAVITATION . l & a s s Vo Flds o as l axwll a l sla () l Fld () l olasao () a Flx s () a Fld () a do () ad è s ( ). F wo Sala Flds s b dd l a s ( ) ad oool a s ( ) a oal o 4 qaos 3 aabls - w o Lal osas - oz abo Lal-Sd

More information

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109 Th fa fl calculao: Appoa a ac oluo Pa K Novb 0h 005 B-09 Oul Novb 0h 005 Pa K Iouco Appoa oluo flco fo h gou ac oluo Cocluo Pla wav fo Ic fl: pla wav k ( ) jk H ( ) λ λ ( ) Polaao fo η 0 0 Hooal polaao

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

Handout on. Crystal Symmetries and Energy Bands

Handout on. Crystal Symmetries and Energy Bands dou o Csl s d g Bds I hs lu ou wll l: Th loshp bw ss d g bds h bs of sp-ob ouplg Th loshp bw ss d g bds h ps of sp-ob ouplg C 7 pg 9 Fh Coll Uvs d g Bds gll hs oh Th sl pol ss ddo o h l slo s: Fo pl h

More information

X-ray Diffraction from Materials

X-ray Diffraction from Materials X-ay ffato fo Matal 8 Spg St Lt; Yag Mo Koo Moday ad Wdday :5~6: . X-ay ff Sattg. Thal ff Sattg d to to Vbato. Odg ad ff Sattg d to Stat plat Howo . X-ay ff Sattg ffato of x-ay: pod aay of ato Ba podty

More information

6.Optical and electronic properties of Low

6.Optical and electronic properties of Low 6.Optical and lctonic poptis of Low dinsional atials (I). Concpt of Engy Band. Bonding foation in H Molculs Lina cobination of atoic obital (LCAO) Schoding quation:(- i VionV) E find a,a s.t. E is in a

More information

Radial Distribution Function. Long-Range Corrections (1) Temperature. 3. Calculation of Equilibrium Properties. Thermodynamics Properties

Radial Distribution Function. Long-Range Corrections (1) Temperature. 3. Calculation of Equilibrium Properties. Thermodynamics Properties . Calculato o qulbrum Prorts. hrmodamc Prorts mratur, Itral rg ad Prssur Fr rg ad tro. Calculato o Damc Prorts Duso Coct hrmal Coductvt Shar scost Irard Absorto Coct k k k mratur m v Rmmbr hrmodamcs or

More information

ASYMPTOTIC AND TOLERANCE 2D-MODELLING IN ELASTODYNAMICS OF CERTAIN THIN-WALLED STRUCTURES

ASYMPTOTIC AND TOLERANCE 2D-MODELLING IN ELASTODYNAMICS OF CERTAIN THIN-WALLED STRUCTURES AYMPTOTIC AD TOLERACE D-MODELLIG I ELATODYAMIC OF CERTAI THI-WALLED TRUCTURE B. MICHALAK Cz. WOŹIAK Dpartmt of tructural Mchacs Lodz Uvrsty of Tchology Al. Poltrchk 6 90-94 Łódź Polad Th objct of aalyss

More information

The Odd Generalized Exponential Modified. Weibull Distribution

The Odd Generalized Exponential Modified. Weibull Distribution Itatoal Mathmatcal oum Vol. 6 o. 9 943-959 HIKARI td www.m-ha.com http://d.do.og/.988/m.6.6793 Th Odd Galzd Epotal Modd Wbull Dstbuto Yassm Y. Abdlall Dpatmt o Mathmatcal Statstcs Isttut o Statstcal Studs

More information

Consider two masses m 1 at x = x 1 and m 2 at x 2.

Consider two masses m 1 at x = x 1 and m 2 at x 2. Chapte 09 Syste of Patcles Cete of ass: The cete of ass of a body o a syste of bodes s the pot that oes as f all of the ass ae cocetated thee ad all exteal foces ae appled thee. Note that HRW uses co but

More information

COHERENCE SCANNING INTERFEROMETRY

COHERENCE SCANNING INTERFEROMETRY COHERENCE SCANNING INTERFEROMETRY Pt 1. Bscs, Cto Austt Sus K. Rsy PD Mc 2013 OUTLINE No cotct suc sut systs Coc sc tot Sts ISO, ASME Pt sts Vto tst Cto, ustt pocus Octv ocus optzto Scc stts w sut stts

More information

Phase diagram and frustration of decoherence in Y-shaped Josephson junction networks. D.Giuliano(Cosenza), P. Sodano(Perugia)

Phase diagram and frustration of decoherence in Y-shaped Josephson junction networks. D.Giuliano(Cosenza), P. Sodano(Perugia) Phas dagram ad frustrato of dcohrc Y-shapd Josphso jucto tworks D.GulaoCosza, P. SodaoPruga Frz, Frz, Octobr Octobr 008 008 Ma da Y-Shapd twork of Josphso jucto chas YJJN wth a magtc frustrato Ft-couplg

More information

3.4 Properties of the Stress Tensor

3.4 Properties of the Stress Tensor cto.4.4 Proprts of th trss sor.4. trss rasformato Lt th compots of th Cauchy strss tsor a coordat systm wth bas vctors b. h compots a scod coordat systm wth bas vctors j,, ar gv by th tsor trasformato

More information

SUNWAY UNIVERSITY BUSINESS SCHOOL SAMPLE FINAL EXAMINATION FOR FIN 3024 INVESTMENT MANAGEMENT

SUNWAY UNIVERSITY BUSINESS SCHOOL SAMPLE FINAL EXAMINATION FOR FIN 3024 INVESTMENT MANAGEMENT UNWA UNIVRIT BUIN HOOL AMPL FINAL AMINATION FOR FIN 34 INVTMNT MANAGMNT TION A A ALL qto th cto. Qto tha kg facg fo a ca. Th local bak ha ag to gv hm a loa fo 9% of th cot of th ca h ll pay th t cah a

More information

P a g e 5 1 of R e p o r t P B 4 / 0 9

P a g e 5 1 of R e p o r t P B 4 / 0 9 P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e

More information

The Random Phase Approximation:

The Random Phase Approximation: Th Random Phas Appoxmaton: Elctolyts, Polym Solutons and Polylctolyts I. Why chagd systms a so mpotant: thy a wat solubl. A. bology B. nvonmntally-fndly polym pocssng II. Elctolyt solutons standad dvaton

More information

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes Galaxy Photomty Fo galaxis, w masu a sufac flux, that is, th couts i ach pixl. Though calibatio, this is covtd to flux dsity i Jaskys ( Jy -6 W/m/Hz). Fo a galaxy at som distac, d, a pixl of sid D subtds

More information

Numerical Solution of Transient Thermal Stresses in a Functionally Graded Cylinder

Numerical Solution of Transient Thermal Stresses in a Functionally Graded Cylinder La d gg Mha gg Glgy al l f a hal a Fally Gadd yld IQ H KHOLO I-LMH aal gg a Jda y f ad hlgy P.O x Ibd JO al: daabh@.d. ba: - h a d h a hal a la yld ad f a fally gadd aal FGM. h yld aal dd b gadd alg h

More information

Th n nt T p n n th V ll f x Th r h l l r r h nd xpl r t n rr d nt ff t b Pr f r ll N v n d r n th r 8 l t p t, n z n l n n th n rth t rn p rt n f th v

Th n nt T p n n th V ll f x Th r h l l r r h nd xpl r t n rr d nt ff t b Pr f r ll N v n d r n th r 8 l t p t, n z n l n n th n rth t rn p rt n f th v Th n nt T p n n th V ll f x Th r h l l r r h nd xpl r t n rr d nt ff t b Pr f r ll N v n d r n th r 8 l t p t, n z n l n n th n rth t rn p rt n f th v ll f x, h v nd d pr v n t fr tf l t th f nt r n r

More information

Lecture #11. A Note of Caution

Lecture #11. A Note of Caution ctur #11 OUTE uctos rvrs brakdow dal dod aalyss» currt flow (qualtatv)» morty carrr dstrbutos Radg: Chatr 6 Srg 003 EE130 ctur 11, Sld 1 ot of Cauto Tycally, juctos C dvcs ar formd by coutr-dog. Th quatos

More information

Reliability of time dependent stress-strength system for various distributions

Reliability of time dependent stress-strength system for various distributions IOS Joural of Mathmatcs (IOS-JM ISSN: 78-578. Volum 3, Issu 6 (Sp-Oct., PP -7 www.osrjourals.org lablty of tm dpdt strss-strgth systm for varous dstrbutos N.Swath, T.S.Uma Mahswar,, Dpartmt of Mathmatcs,

More information

signal amplification; design of digital logic; memory circuits

signal amplification; design of digital logic; memory circuits hatr Th lctroc dvc that s caabl of currt ad voltag amlfcato, or ga, cojucto wth othr crcut lmts, s th trasstor, whch s a thr-trmal dvc. Th dvlomt of th slco trasstor by Bard, Bratta, ad chockly at Bll

More information

Cylon BACnet Unitary Controller (CBT) Range

Cylon BACnet Unitary Controller (CBT) Range ATASHEET Cyo BAC y Coo (CBT) Rg Th Cyo BAC y Coo (CBT) Rg g o BTL L BAC Av Appo Coo wh p 8 op, y o oog g o p. Th v h g ow o o, po ppo o g VAV ppo. BAC MS/TP F Sppo h oowg og BAC oj: A/B/AO/BO/AV/BV, A,

More information

( ) L = D e. e e. Example:

( ) L = D e. e e. Example: xapl: A Si p juctio diod av acoss sctioal aa of, a accpto coctatio of 5 0 8 c -3 o t p-sid ad a doo coctatio of 0 6 c -3 o t -sid. T lif ti of ols i -gio is 47 s ad t lif ti of lctos i t p-gio is 5 s.

More information

Lecture 1: Empirical economic relations

Lecture 1: Empirical economic relations Ecoomcs 53 Lctur : Emprcal coomc rlatos What s coomtrcs? Ecoomtrcs s masurmt of coomc rlatos. W d to kow What s a coomc rlato? How do w masur such a rlato? Dfto: A coomc rlato s a rlato btw coomc varabls.

More information

Elasticity 1. 10th April c 2003, Michael Marder

Elasticity 1. 10th April c 2003, Michael Marder Elasticity 0th Apil 003 c 003, Michal Mad Gnal Thoy of Lina Elasticity Bfo dfomation Aft dfomation Many ways to div lasticity. Cold div fom thoy of atoms and thi intactions. Howv, this appoach is not histoically

More information

Order Statistics from Exponentiated Gamma. Distribution and Associated Inference

Order Statistics from Exponentiated Gamma. Distribution and Associated Inference It J otm Mth Scc Vo 4 9 o 7-9 Od Stttc fom Eottd Gmm Dtto d Aoctd Ifc A I Shw * d R A Bo G og of Edcto PO Bo 369 Jddh 438 Sd A G og of Edcto Dtmt of mthmtc PO Bo 469 Jddh 49 Sd A Atct Od tttc fom ottd

More information

GTAP Eleventh Annual Conference, 2008 "Future of Global Economy" Helsinki

GTAP Eleventh Annual Conference, 2008 Future of Global Economy Helsinki GTAP Elvth Aual Cof, 28 "Futu of Global Eooy" lsk SAM laboato as a ultobtv austt pobl Casao Maqu Laa Pñat Dpto Aálss Eoóo Aplao Uvsa Las Palas Ga Caaa (Spa aqu@aa.ulpg.s Dolos R. Satos-Pñat Dpto Métoos

More information

A L A BA M A L A W R E V IE W

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

Previous knowlegde required. Spherical harmonics and some of their properties. Angular momentum. References. Angular momentum operators

Previous knowlegde required. Spherical harmonics and some of their properties. Angular momentum. References. Angular momentum operators // vious owg ui phica haoics a so o thi poptis Goup thoy Quatu chaics pctoscopy H. Haga 8 phica haoics Rcs Bia. iv «Iucib Tso thos A Itouctio o chists» Acaic ss D.A. c Quai.D. io «hii hysiu Appoch oécuai»

More information

The Real Hydrogen Atom

The Real Hydrogen Atom T Ra Hydog Ato ov ad i fist od gt iddt of :.6V a us tubatio toy to dti: agti ffts si-obit ad yfi -A ativisti otios Aso av ab sift du to to sfitatio. Nd QD Dia q. ad dds o H wavfutio at sou of ti fid. Vy

More information

LINEAR REGRESSION ANALYSIS

LINEAR REGRESSION ANALYSIS LINEAR REGRESSION ANALYSIS MODULE V Lecture - Correctg Model Iadequaces Through Trasformato ad Weghtg Dr. Shalabh Departmet of Mathematcs ad Statstcs Ida Isttute of Techology Kapur Aalytcal methods for

More information

ME 501A Seminar in Engineering Analysis Page 1

ME 501A Seminar in Engineering Analysis Page 1 St Ssts o Ordar Drtal Equatos Novbr 7 St Ssts o Ordar Drtal Equatos Larr Cartto Mcacal Er 5A Sar Er Aalss Novbr 7 Outl Mr Rsults Rvw last class Stablt o urcal solutos Stp sz varato or rror cotrol Multstp

More information

Jim Lambers MAT 280 Summer Semester Practice Final Exam Solution. dy + xz dz = x(t)y(t) dt. t 3 (4t 3 ) + e t2 (2t) + t 7 (3t 2 ) dt

Jim Lambers MAT 280 Summer Semester Practice Final Exam Solution. dy + xz dz = x(t)y(t) dt. t 3 (4t 3 ) + e t2 (2t) + t 7 (3t 2 ) dt Jim Lambers MAT 28 ummer emester 212-1 Practice Final Exam olution 1. Evaluate the line integral xy dx + e y dy + xz dz, where is given by r(t) t 4, t 2, t, t 1. olution From r (t) 4t, 2t, t 2, we obtain

More information

EQUATION SHEETS FOR ELEC

EQUATION SHEETS FOR ELEC QUTON SHTS FO C 47 Fbuay 7 QUTON SHTS FO C 47 Fbuay 7 hs hυ h ω ( J ) h.4 ω υ ( µ ) ( ) h h k π υ ε ( / s ) G Os (Us > x < a ) Sll s aw s s s Shal z z Shal buay (, aus ) z y y z z z Shal ls ( s sua, s

More information

Chapter 3 What make semiconductors so useful? Macroscopic properties

Chapter 3 What make semiconductors so useful? Macroscopic properties SUMMARY Chapt 3 What a scnducts s usful? Macscpc ppts - Hw d scnducts hav such a wd ang f cnductvty? vn f th sa scnduct cpund,. g. S? - Th natu f - Hw d s hav pstv Hall ffcts (p-typ), and s hav ngatv Hall

More information

Born-Oppenheimer Approximation. Kaito Takahashi

Born-Oppenheimer Approximation. Kaito Takahashi o-oppehee ppoato Kato Takahah toc Ut Fo quatu yte uch a ecto ad olecule t eae to ue ut that ft the=tomc UNT Ue a of ecto (ot kg) Ue chage of ecto (ot coulob) Ue hba fo agula oetu (ot kg - ) Ue 4pe 0 fo

More information

ELEC9721: Digital Signal Processing Theory and Applications

ELEC9721: Digital Signal Processing Theory and Applications ELEC97: Digital Sigal Pocssig Thoy ad Applicatios Tutoial ad solutios Not: som of th solutios may hav som typos. Q a Show that oth digital filts giv low hav th sam magitud spos: i [] [ ] m m i i i x c

More information

Lecture 11: Introduction to nonlinear optics I.

Lecture 11: Introduction to nonlinear optics I. Lectue : Itoducto to olea optcs I. Pet Kužel Fomulato of the olea optcs: olea polazato Classfcato of the olea pheomea Popagato of wea optc sgals stog quas-statc felds (descpto usg eomalzed lea paametes)!

More information

Measuring dielectric properties at the nanoscale using Electrostatic Force Microscopy

Measuring dielectric properties at the nanoscale using Electrostatic Force Microscopy Masug dlctc popts at th aoscal usg Elctostatc Foc Mcoscopy R. Ao, C. Rdl,,3, G. A. Schwatz 4, G. Lévêqu, A. Algía 3,4, Ph. Todjma 5, N. E. Isaloff 6, M. Ramoda 7 ad J. Colmo,3,4 IES, UMR CNRS 54, Uvsté

More information

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD II.3. DETEMINTION OF THE ELETON SPEIFI HGE Y MENS OF THE MGNETON METHOD. Wok pupos Th wok pupos is to dtin th atio btwn th absolut alu of th lcton chag and its ass, /, using a dic calld agnton. In this

More information

VIII Dynamics of Systems of Particles

VIII Dynamics of Systems of Particles VIII Dyacs of Systes of Patcles Cete of ass: Cete of ass Lea oetu of a Syste Agula oetu of a syste Ketc & Potetal Eegy of a Syste oto of Two Iteactg Bodes: The Reduced ass Collsos: o Elastc Collsos R whee:

More information

,. *â â > V>V. â ND * 828.

,. *â â > V>V. â ND * 828. BL D,. *â â > V>V Z V L. XX. J N R â J N, 828. LL BL D, D NB R H â ND T. D LL, TR ND, L ND N. * 828. n r t d n 20 2 2 0 : 0 T http: hdl.h ndl.n t 202 dp. 0 02802 68 Th N : l nd r.. N > R, L X. Fn r f,

More information

GMm. 10a-0. Satellite Motion. GMm U (r) - U (r ) how high does it go? Escape velocity. Kepler s 2nd Law ::= Areas Angular Mom. Conservation!!!!

GMm. 10a-0. Satellite Motion. GMm U (r) - U (r ) how high does it go? Escape velocity. Kepler s 2nd Law ::= Areas Angular Mom. Conservation!!!! F Satllt Moton 10a-0 U () - U ( ) 0 f ow g dos t go? scap locty Kpl s nd Law ::= Aas Angula Mo. Consaton!!!! Nwton s Unsal Law of Gaty 10a-1 M F F 1) F acts along t ln connctng t cnts of objcts Cntal Foc

More information

Ch. 22: Classical Theory of Harmonic Crystal

Ch. 22: Classical Theory of Harmonic Crystal C. : Clssl Toy o mo Cysl gl o ml moo o o os l s ld o ls o pl ollowg:. Eqlbm Pops p o ls d Islos Eqlbm sy d Cos Egs Tml Epso d lg. Tspo Pops T pd o lo Tm Fl o Wdm-Fz Lw pody Tml Cody o Islos Tsmsso o od.

More information

D. Bertsekas and R. Gallager, "Data networks." Q: What are the labels for the x-axis and y-axis of Fig. 4.2?

D. Bertsekas and R. Gallager, Data networks. Q: What are the labels for the x-axis and y-axis of Fig. 4.2? pd by J. Succ ECE 543 Octob 22 2002 Outl Slottd Aloh Dft Stblzd Slottd Aloh Uslottd Aloh Splttg Algoths Rfc D. Btsks d R. llg "Dt twoks." Rvw (Slottd Aloh): : Wht th lbls fo th x-xs d y-xs of Fg. 4.2?

More information

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9 OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at

More information

Aotomorphic Functions And Fermat s Last Theorem(4)

Aotomorphic Functions And Fermat s Last Theorem(4) otomorphc Fuctos d Frmat s Last Thorm(4) Chu-Xua Jag P. O. Box 94 Bg 00854 P. R. Cha agchuxua@sohu.com bsract 67 Frmat wrot: It s mpossbl to sparat a cub to two cubs or a bquadrat to two bquadrats or gral

More information