Lecture Y4: Computational Optics I
|
|
- Reginald Melton
- 6 years ago
- Views:
Transcription
1 Phooc ad opolcoc chologs DPMS: Advacd Maals Udsadg lgh ma acos s cucal fo w applcaos Lcu Y4: Compuaoal Opcs I lfos Ldoks Room Π, ldok@cc.uo.g hp://cmsl.maals.uo.g/ldoks Rflco ad faco Toal al flco Tappg ad gudg lgh Maal pop: dlcc fuco d of faco 3 4
2 Dffacd wavs f Dffaco ad fc Dffaco gags g Dffaco gags a usd fo wavlgh spaao 5 6 Naus dffaco gags phooc csals Sucual colo Phooc csals cholog Applcaos m lgh mapulao 7 8
3 ampls of D phooc csals ampls of D phooc csals 9 ampls of 3D phooc csals Plasmocs: acos wh aosucud mals απορρόφ ός φηση φωτό συχνότητα φωτός kodsk.wbs.com
4 Plasmocs h mddl ags Εφαρμογές πλασμονικών νανοσωματιδίων στην ιατρική a GFR cougad gold aopacls 3 Isu of Naocholog, Nohws Uvs Rc Uvs 4 Sufac plasmos Oul /M wavs Wav quaos Bouda codos Maals opcal spos Maals opcal chaaczao Numcal soluos Applcaos dsg 5 6
5 Th classcal au of lgh Oscllag lcc ad magc flds popagao spd c=3 8 m/s Tasvs wavs ppdcula o popagao dco ppdcula o ach oh Gs polazd lal polazd (.g. ad cculal polazd (.g. gh ad lf gall wo ohogoal polazaos Iaco wh maals flco, faco, absopo, fc, scag, dffaco, /M wav pops Wavlgh λ spaal podc Pod T mpoal podc Wavvco k / spaal po a Agula fquc /T mpoal po a Dspso lao k / c ( s d of faco lao bw k ad ω lao bw spac ad m lao bw momum ad g (, p k I 3D spac, k s a 3D vco lcc ad magc flds a 3D vcos polazao of wav s h lcc fld polazao 7 8 /M wav quaos /M wav quaos D Mawll s quaos D B B D Cosuv laos D P D D(, B B(, (, (, B ( M Maal pops lcc pmv ( magc pmabl ( facv d ( ( ( A opcal fqucs 9 Mawll s quaos B D D z z Comb fo o uqu quao z z z z z z z c c /( Wav soluo a pla wavs ˆ dspso lao ( kz k ( kz c ( kz k / c / c
6 Bouda codos a facs cos cos s cos cos s Cou a h bouda: s s of h paalll compos of h lcc fld s s // of h ppdcula compos of h dsplacm of h paalll compos of h magc fld // D cos cos s s of h ppdcula compos of h ducac B cos cos Rflco ad faco a a fac asvs magc (TM p polazao k k k asvs lcc (T s polazao k k k Bouda codos o k k s k s paalll compo of k cosvd k k / c momum cosvao s s Sll s law Bouda codos o flds flco ad asmsso ampluds, flcv ad asmac R, T ( / Isd maals /, c / Rflco ad asmsso fom a h flm kd kd maals chaaczao 3 a flco coags dff fo s ad p polazaos Rflco fom podc flm aas D phooc csal Bagg mo mulpl flcos sul o m flco fo som fqucs pfc mos fo lass, slcv fls, ssos, c Toal flco kd kd kd kd kd kd k / c d a omal cdc kd 3 kd kd kd kd [ (...]
7 Dlcc fuco: maal polazabl Dlcc fuco ach obal has a dff cobuo lcoc: UV ad Vsbl aomc: IR c N m d d Dv oscllao m m K d d K / m K m N m Assum hamoc oscllao m m m m Polazao dpds o umb ds of lcoc obals al P N N m Dlcc fuco D N P m N m 5 ω γ mag 6 Maals opcal chaaczao Numcal soluo Rflcac spcoscop Cosd D Mawll s quaos, z z F dffc m doma mhod (FDTD dscz spac o gds (Δ dsac bw gds llpsom Df lcc fld o gds z w wll also dscz m o m sps (Δ m bw m sps z 7 pu magc fld a half gds ad half m sps / / / / / 8 3/
8 Spac m gd D FDTD D ad 3D FDTD / / / / / / 3/ 5/ Y lac: dff sublacs fo lcc ad magc flds cal dffcs fo all fld compos Appoma Mawll s quaos b cal dffcs Assum w kow vhg fo a m ad fo a m / z z - / / / / z - z Fld upda algohm c / / / / z c z / / / / - - / / / / z h omalzao was mad / D sabl codo c z 9 3
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 informationk 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 informationChapter 3 Plane EM Waves and Lasers in Distinct Media
hap Pla Wavs a ass sc a - Nomal Icc a a Pla oucg oua a a Ic pla wav: flcv wav: Toal fl: oucg boua a s Sag wav: Zo ull of a - amum of a -λ Zo ull of a - amum of a -λ g. -pola pla wav f amplu6mvm popagas
More informationPart 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 informationThe 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 informationAnouncements. Conjugate Gradients. Steepest Descent. Outline. Steepest Descent. Steepest Descent
oucms Couga Gas Mchal Kazha (6.657) Ifomao abou h Sma (6.757) hav b pos ol: hp://www.cs.hu.u/~msha Tch Spcs: o M o Tusay afoo. o Two paps scuss ach w. o Vos fo w s caa paps u by Thusay vg. Oul Rvw of Sps
More informationSampled, Super-structured Multi-channel FBG
Faby-Po bad-pass fl Sampld Sup-sucud Mul-chal FBG λ δ L gap Bagg 4 Samplg podc supsucu of FBG gas mulpl cops chals of h fucy spos FBG pa 0 / cos/λφ spac doma Sc samplg abls a fla spcal spos FBG pa 0 /
More informationNLO Basics. Bulk Second Harmonic Generation Examples. QuartzQ ZnO bulk and nanowires Organic nanowires
NLO Bascs Bul Scod Hamoc Gao xampls QuaQ ZO bul ad aows Ogac aows Ahamoc Poals U U- P χ χ χ Io P lco pah P Wav quao : quaos Maxwlls D J H B : chags f No 4 H B J D B μ ρ ρ s. : chags f No H H B J μ μ ρ
More informationBy Joonghoe Dho. The irradiance at P is given by
CH. 9 c CH. 9 c By Joogo Do 9 Gal Coao 9. Gal Coao L co wo po ouc, S & S, mg moocomac wav o am qucy. L paao a b muc ga a. Loca am qucy. L paao a b muc ga a. Loca po obvao P a oug away om ouc o a a P wavo
More informationBoyce/DiPrima 9 th ed, Ch 7.6: Complex Eigenvalues
BocDPm 9 h d Ch 7.6: Compl Egvlus Elm Dffl Equos d Boud Vlu Poblms 9 h do b Wllm E. Boc d Rchd C. DPm 9 b Joh Wl & Sos Ic. W cosd g homogous ssm of fs od l quos wh cos l coffcs d hus h ssm c b w s ' A
More informationCharacterizing Optical Thin Films (I)
Chaaczg Opcal Th Flms (I) Physcal vapo dposo s h mos commo chqu usd o dpos opcal h lms o a lag vay o applcaos. Ths qus h ably o g a sold maal o a vapo (gasous) om, o aspo o a suac oo whch h lm s o b dposd,
More informationTrefftz method in solving the inverse problems
IP-A Ivs Poblms: vlopms ho a applcaos Fbua 9- Wasaw Pola ff mho solvg h vs poblms Ksof Gsa Klc Uvs of cholog Al.. -lca P.P.7 5-34 Klc Pola -mal: sof@gsa.pl /7 IP-A Ivs Poblms: vlopms ho a applcaos Fbua
More informationChapter 5 Transmission Lines
ap 5 ao 5- aacc of ao ao l: a o cou ca cu o uppo a M av c M o qua-m o. Fo M o a H M H a M a µ M. cu a M av av ff caacc. A M av popaa o ff lcc a paal flco a paal ao ll occu. A ob follo ul. ll la: p a β
More informationLecture 12: Introduction to nonlinear optics II.
Lcur : Iroduco o olar opcs II r Kužl ropagao of srog opc sgals propr olar ffcs Scod ordr ffcs! Thr-wav mxg has machg codo! Scod harmoc grao! Sum frqucy grao! aramrc grao Thrd ordr ffcs! Four-wav mxg! Opcal
More informationAn Analysis of a Double-layer Electromagnetic Shield for a Universal Contactless Battery Charging Platform
A Aalyss of a Doubl-lay Elcomagc Shld fo a Uvsal Coaclss Bay Chagg Plafom Absac A pad doubl-lay plaa sucu s mployd o shld h lcomagc EM fld a h boom of a uvsal chagg plafom. Th doubl-lay cosss of a lay
More informationParametric Down Conversion. Quantum optics seminar Winter 2008 Assaf Shaham
Paam Dow Covso Quaum ops sma 7774 W 8 ssaf Shaham ox Iouo Thoy of lass Sum Fquy Gao Quaum Hamloa fo PDC pplaos No la ops Cao of w fqus h sysm. Usually h w fqus hav small amplu lav o h pu fqus. Hamo Dff
More informationHandout 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 informationChapter 5 Transmission Lines
hap 5 asmsso s 5- haacscs of asmsso s asmsso l: has o coucos cay cu o suppo a M av hch s M o quas-m mo. Fo h M mo a H M H M a a M. h cu a h M av hav ff chaacscs. A M av popaas o ff lcc ma h paal flco a
More informationChap 2: Reliability and Availability Models
Chap : lably ad valably Modls lably = prob{s s fully fucog [,]} Suppos from [,] m prod, w masur ou of N compos, of whch N : # of compos oprag corrcly a m N f : # of compos whch hav fald a m rlably of h
More informationLecture 23. Multilayer Structures
Lcu Mullay Sucus In hs lcu yu wll lan: Mullay sucus Dlcc an-flcn (AR) cangs Dlcc hgh-flcn (HR) cangs Phnc Band-Gap Sucus C Fall 5 Fahan Rana Cnll Unvsy Tansmssn Ln Juncns and Dscnnus - I Tansmssn ln dscnnus
More information( i IMPACT OF LONGITUDINAL AND TRANSVERSE WAVES BY CYLINDRICAL LAYERS WERE LIQUID 2 ~ t (1)
Joal of ldscplay gg Scc ad Tchology JST ISSN: 59- Vol. Iss Novmb - IPT OF ONGITUIN N TRNSVRS WVS INRI RS WR IQUI I.I.Safaov Z.I olav.sh hmdov haa Tchologcal- Is of gg Rpblc of Uzbsa s. K. azayv 5 safaov5@mal.
More informationChapter 1 Basic Concepts
Ch Bsc Cocs oduco od: X X ε ε ε ε ε O h h foog ssuos o css ε ε ε ε ε N Co No h X Chcscs of od: cos c ddc (ucod) d s of h soss dd of h ssocd c S qusos sd: Wh f h cs of h soss o cos d dd o h ssocd s? Wh
More informationDirect current regimes in the linear electric circuits according to the relativistic circuit theory
ISSN: 63-316X (Ol OI: 1.9114/av.vol.ss1.66 Vol Iss 1 (18 Pblshd: 18-6-3 c c gms h la lcc ccs accodg o h lavsc cc ho ml Ivaov Paov 1 1 Tchcal Uvs of Vaa, pam of Thocal lccal gg ad Ismao, 91, 1 Sdsa S, Vaa,
More informationDielectric Waveguide 1
Dilctic Wavgui Total Ital Rflctio i c si c t si si t i i i c i Total Ital Rflctio i c i cos si Wh i t i si c si cos t j o cos t t o si i si bcoms pul imagia pul imagia i, al Total Ital Rflctio 3 i c i
More informationThe Linear Regression Of Weighted Segments
The Lear Regresso Of Weghed Segmes George Dael Maeescu Absrac. We proposed a regresso model where he depede varable s made o up of pos bu segmes. Ths suao correspods o he markes hroughou he da are observed
More informationGeometrical optics. Textbook: Born and Wolf (chapters 3-5) Overview:
Gomal ops Txbook: Bo a Wol aps -5 Ovvw: Elomag pla wavs om maxwll's quaos. T Ekoal quao a s vao ops a o wavlg. Rao ll's law lo Toal al lo T psm Dspso T ls Imagg as a pojv asomao. Opal ssms a ABCD max.
More informationFresnel Equations cont.
Lecure 12 Chaper 4 Fresel quaos co. Toal eral refleco ad evaesce waves Opcal properes of meals Laer: Famlar aspecs of he eraco of lgh ad maer Fresel quaos r 2 Usg Sell s law, we ca re-wre: r s s r a a
More informationExistence of Nonoscillatory Solutions for a Class of N-order Neutral Differential Systems
Vo 3 No Mod Appd Scc Exsc of Nooscaoy Souos fo a Cass of N-od Nua Dffa Sysms Zhb Ch & Apg Zhag Dpam of Ifomao Egg Hua Uvsy of Tchoogy Hua 4 Cha E-ma: chzhbb@63com Th sach s facd by Hua Povc aua sccs fud
More informationSymmetry breaking effects of toroidicity on toroidal momentum transport. Abstract
Symmy bakg ffcs of oodcy o oodal momum aso. TH/8.9 J. Wlad, R. Sg, H. Nodma,. Kaw, A.G. s ad D. Sz. Dam of Rado ad Sac Scc, Calms. vsy of Tcology ad Euaom-VR Assocao, S96 Gobug, Swd. Isu fo lasma Rsac,
More informationMethods of quantum dynamics and simulation of pump-probe spectra
Mhods of quau dacs ad sulao of pup-pob spca Chsoph M Laboao Collsos Aéas Réacvé Uvsé Paul Saba Toulous Cas Auus 008 Mhods of quau dacs ad sulao of pup-pob spca I. Ioduco Las / olcul aco -- lco / ucl spaao
More informationMECE 3320 Measurements & Instrumentation. Static and Dynamic Characteristics of Signals
MECE 330 MECE 330 Masurms & Isrumao Sac ad Damc Characrscs of Sgals Dr. Isaac Chouapall Dparm of Mchacal Egrg Uvrs of Txas Pa Amrca MECE 330 Sgal Cocps A sgal s h phscal formao abou a masurd varabl bg
More informationChapter 4. The Properties of Light 4.1 Introduction Scattering Transmission, reflection, and refraction
Chape 4. The Popees of Lgh 4.1 Ioduco Scaeg Tasmsso, efleco, ad efaco (mcoscopc) (macoscopc) Hech by YHLEE;100510; 4-1 4. Raylegh Scaeg Scaeg of sulgh Sulgh he a Goud-sae vbao of Re-emsso of lgh. oge,
More informationMathematical Model of Acceleration Stage of Magnetic Inductive Pulsed Plasma Thruster
Mahacal Modl of Acclao Sag of Magc ducv Pulsd Plasa Thus EPC--76 Psd a h d aoal Elcc Poulso Cofc, Wsbad Gay Sb 5, Haf Daas Salh ad Sgy Yuyovch so aoal Aosac Uvsy (Khav Avao su), Khav, 67, Ua, Chalova,
More informationLeast squares and motion. Nuno Vasconcelos ECE Department, UCSD
Las squars ad moo uo Vascoclos ECE Dparm UCSD Pla for oda oda w wll dscuss moo smao hs s rsg wo was moo s vr usful as a cu for rcogo sgmao comprsso c. s a gra ampl of las squars problm w wll also wrap
More informationSuperconducting nanostructures
pcodcg aoscs a: Y.V. azao Y.M. Bla: Qa aspo Cabdg Usy Pss 9. aa P.. Bagwll M.P. aa: cag Toy of Taspo fo Msoscopc pcodcos p:docs.lb.pd.dc7. Co P.. ss oc coacs: a Ts-Bd fo Msoscopc Pyscs C aclay J. Cs: pcodcg
More informationIntegrated Optical Waveguides
Su Opls Faha Raa Cll Uvs Chap 8 Ia Opal Wavus 7 Dl Slab Wavus 7 Iu: A va f ff a pal wavus a us f a u lh a hp Th s bas pal wavu s a slab wavus shw blw Th suu s uf h - Lh s u s h b al al fl a h -la fas Cla
More informationChapter 5. Long Waves
ape 5. Lo Waes Wae e s o compaed ae dep: < < L π Fom ea ae eo o s s ; amos ozoa moo z p s ; dosac pesse Dep-aeaed coseao o mass
More informationIntroduction to Laplace Transforms October 25, 2017
Iroduco o Lplc Trform Ocobr 5, 7 Iroduco o Lplc Trform Lrr ro Mchcl Egrg 5 Smr Egrg l Ocobr 5, 7 Oul Rvw l cl Wh Lplc rform fo of Lplc rform Gg rform b gro Fdg rform d vr rform from bl d horm pplco o dffrl
More informationRAKE Receiver with Adaptive Interference Cancellers for a DS-CDMA System in Multipath Fading Channels
AKE v wh Apv f Cs fo DS-CDMA Ss Muph Fg Chs JooHu Y Su M EEE JHog M EEE Shoo of E Egg Sou o Uvs Sh-og Gw-gu Sou 5-74 Ko E-: ohu@su As hs pp pv AKE v wh vs og s popos fo DS-CDMA ss uph fg hs h popos pv
More informationECE 107: Electromagnetism
ECE 07: Elcomagnsm S 8: Plan wavs Insuco: Pof. Valy Lomakn Dpamn of Elccal and Compu Engnng Unvsy of Calfona, San Dgo, CA 92093 Wav quaon Souc-f losslss Maxwll s quaons Apply cul = jωμ ε = = jωε μ = 2
More informationGauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year
Gau Thors Elmary Parcl Physcs Sro Iraco Fomoloy o Bo cadmc yar - Gau Ivarac Gau Ivarac Whr do Laraas or Hamloas com from? How do w kow ha a cra raco should dscrb a acual hyscal sysm? Why s h lcromac raco
More informationEffectofMagneticFieldonOscillatoryFlowPastParallelPlatesinaRotatingSystemwithHeatandMassTransfer
Global Joual of Scc Fo Rsach: F Mahmacs a Dcso Sccs Volum 4 Issu 4 Vso. Ya 4 yp : Doubl Bl P Rw Iaoal Rsach Joual Publsh: Global Jouals Ic. (SA Ol ISSN: 49-466 & P ISSN: 975-5896 Effc of Magc Fl o Oscllaoy
More informationOPTICAL DESIGN. FIES fibre assemblies B and C. of the. LENS-TECH AB Bo Lindberg Document name: Optical_documentation_FIES_fiber_BC_2
OPTICAL DESIGN f h FIES fb ssmbs B d C LENS-TECH AB B Ldbg 2-4-3 Dcm m: Opc_dcm_FIES_fb_BC_2 Idc Ths p s dcm f h pc dsg f h FIES fb ssmbs B d C Th mchc dsg s shw I s shw h ssmb dwg md b Ahs Uvs Fb c Th
More informationBethe-Salpeter Equation Green s Function and the Bethe-Salpeter Equation for Effective Interaction in the Ladder Approximation
Bh-Salp Equaon n s Funcon and h Bh-Salp Equaon fo Effcv Inacon n h Ladd Appoxmaon Csa A. Z. Vasconcllos Insuo d Físca-UFRS - upo: Físca d Hadons Sngl-Pacl Popagao. Dagam xpanson of popagao. W consd as
More informationLecture 14. Time Harmonic Fields
Lcu 4 Tim amic Filds I his lcu u will la: Cmpl mahmaics f im-hamic filds Mawll s quais f im-hamic filds Cmpl Pig vc C 303 Fall 007 Faha aa Cll Uivsi Tim-amic Filds ad -filds f a pla wav a (fm las lcu:
More informationdrawing issue sheet Former Royal High School - Hotel Development
H Forer oyal High chool - Hotel Developent drawing isse sheet general arrangeents drawing nber drawing title scale size L()1 ite Plan 1:1 / L()1 egent oad level proposed floor plan 1: 1 / L() ntrance level
More informationChapter 6 Stability of Finite-Difference Time-Domain (FDTD) Method with Nonlinear Lumped Elements
hap 6 Sabl of F-ff Tm-oma FT Mhod wh Nola Lumpd lms 6. Ioduo Tadoall o su umal sabl of h algohm fo a la modl h oua-fdh-lw FL o 3.5. has o b fulflld Taflov 995. I a usabl algohm h ompud ad fld ompos wll
More informationControl Systems (Lecture note #6)
6.5 Corol Sysms (Lcur o #6 Las Tm: Lar algbra rw Lar algbrac quaos soluos Paramrzao of all soluos Smlary rasformao: compao form Egalus ad gcors dagoal form bg pcur: o brach of h cours Vcor spacs marcs
More informationLecture 20. Transmission Lines: The Basics
Lcu 0 Tansmissin Lins: Th Basics n his lcu u will lan: Tansmissin lins Diffn ps f ansmissin lin sucus Tansmissin lin quains Pw flw in ansmissin lins Appndi C 303 Fall 006 Fahan Rana Cnll Univsi Guidd Wavs
More information( r) E (r) Phasor. Function of space only. Fourier series Synthesis equations. Sinusoidal EM Waves. For complex periodic signals
Inoducon Snusodal M Was.MB D Yan Pllo Snusodal M.3MB 3. Snusodal M.3MB 3. Inoducon Inoducon o o dsgn h communcaons sd of a sall? Fqunc? Oms oagaon? Oms daa a? Annnas? Dc? Gan? Wa quaons Sgnal analss Wa
More informationHeat Transfer in Unsteady Axisymmetric Rotational Flow of Oldroyd Liquid
aoal Joual of Scfc & Egg Rsach Volum, ssu 9, Smb-0 SSN 9-558 Ha Tasf Usady Axsymmc Roaoal Flow of Oldoyd Lqud A. Msha, G. S. Ray, S. Bswal Absac - Ths a dals wh h sudy of ha asf usady axsymmc oaoal flow
More informationPartial Molar Properties of solutions
Paral Molar Properes of soluos A soluo s a homogeeous mxure; ha s, a soluo s a oephase sysem wh more ha oe compoe. A homogeeous mxures of wo or more compoes he gas, lqud or sold phase The properes of a
More informationFinite Differences. Centered vs. forward/backwards. ( x) Consider the Taylor expansion of f(x+h) around x:
FD Bass C 66 Nua Mhods Phoos F Dffs Cd vs. fowad/bawads Cosd h Tao paso of f(h) aoud : h f ( h) f h f f K Fo whh w g h fowad fs dff ( h) f f f h f ( h) f f h h h O( h) Now pad boh f(h) ad f() aoud f(h/)
More informationThe Log-Gamma-Pareto Distribution
aoa Joa of Scc: Bac ad Appd Rach JSBAR SSN 37-453 P & O hp:odphp?oajoaofbacadappd ---------------------------------------------------------------------------------------------------------------------------
More informationSOME IMPUTATION METHODS IN DOUBLE SAMPLING SCHEME FOR ESTIMATION OF POPULATION MEAN
aoal Joual of Mod Egg Rsach (JMER) www.jm.com ol. ssu. Ja-F 0 pp-00-07 N: 9- OME MPUTATON METHOD N DOUBLE AMPLNG HEME FOR ETMATON OF POPULATON MEAN ABTRAT Nada gh Thaku Kalpaa adav fo Mahmacal ccs (M)
More informationOption Pricing in a Fractional Brownian Motion Environment
Opo Pcg a acoal owa Moo vom Cpa Ncula Acamy o coomc u ucha, omaa mal: cpc@yahoo.com h a: buay, Abac h pupo o h pap o oba a acoal lack-chol omula o h pc o a opo o vy [, ], a acoal lack-chol quao a a k-ual
More informationChapter 8. Diffraction
Chap 8 Dffacon Pa I Phaso Addon Thom Wha s phaso? In mul-bam nfnc, ach ansmd bam can b xpssd as... 3 N ' ' ' ' ' 4 ' ' n [ n ] d S n q q ' ' ' 3 ' ' 5 '.., h -fld of ach bam s a complx numb n n ' ' A n
More informationConvolution of Generated Random Variable from. Exponential Distribution with Stabilizer Constant
Appld Mamacal Scc Vol 9 5 o 9 78-789 HIKARI Ld wwwm-acom p://dxdoog/988/am5559 Covoluo of Gad Radom Vaabl fom Expoal Dbuo w Sablz Coa Dod Dvao Maa Lufaa Oaa ad Maa Aa Dpam of Mamac Facul of Mamac ad Naual
More informationEMA5001 Lecture 3 Steady State & Nonsteady State Diffusion - Fick s 2 nd Law & Solutions
EMA5 Lecue 3 Seady Sae & Noseady Sae ffuso - Fck s d Law & Soluos EMA 5 Physcal Popees of Maeals Zhe heg (6) 3 Noseady Sae ff Fck s d Law Seady-Sae ffuso Seady Sae Seady Sae = Equlbum? No! Smlay: Sae fuco
More informationDie Mounted Cam Unit General Description of KGSP
D Mond Cam Un Gnal Dscpon of UHav d sc ha confoms o hgh podcon ns. U,,, 0mm and 0mm a avalabl fo h monng dh. UAvalabl angl s 0 o a ncmns of 5. U IO spngs a sd. Opon of U Mc pcfcaon(-) / LU32-(h 3-M8p5
More informationCONTENTS. Hugo Reitzel, the pickles enthusiast CERTIFICATIONS JARS POUCHES & CANS SALAD DRESSING MINI-TUBES
v4. APRIL 2018. Hugo Rz, h pk hu Th of h uhd gu g ou Hugo Rz. I 1909, Ag, Sw vg, h uhd h ow op wh vo: o p up h wod of od! Ad fo ov o hudd ow, w hoo h hg b ug ou xp o o ov ou bu od o bo THE od p. W ufu
More informationChapter 8: Propagating Quantum States of Radiation
Quum Opcs f hcs Oplccs h R Cll Us Chp 8: p Quum Ss f R 8. lcmc Ms Wu I hs chp w wll cs pp quum ss f wus fs f spc. Cs h u shw lw f lcc wu. W ssum h h wu hs l lh qul h -c wll ssum l. Th lcc cs s fuc f l
More informationWARRANT VALUATION METHODS
ARRA ALUAIO MEHOD o R. aa Ph.D. FRM Mogom Ivsm cholog Ic. Fal am J 83 Pho: 6 688-8 so.saa@fools.com www.fools.com cos h cas of a Euopa sl waa ha ls h coac hol o bu a h sk pc o sha of h ulg sock. BLAK-HOLE-MERO
More informationEQUATION 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 informationCONTROL OF A SPACE ROBOT FOR CAPTURING A TUMBLING OBJECT
CONROL OF A SPACE ROBO FOR CAPURING A UMBLING OBJEC Ou Ma (), Agl Flos-Abad (), Khah Pham (2) () Dpam o Mchacal ad Aospac Egg, Nw Mxco Sa Uvsy, Las Cucs, NM 88, USA Emal: oma@msu.du, a_abad@msu.du (2)
More informationInternational Journal of Pure and Applied Sciences and Technology
I J Pu Appl Sc Tchol 8 pp 59-7 Iaoal Joual o Pu ad Appld Sccs ad Tchology ISSN 9-67 Avalabl ol a wwwopaasa Rsach Pap Tasmud Quas Ldly Dsbuo: A Galzao o h Quas Ldly Dsbuo I Elbaal ad M Elgahy * Isu o Sascal
More informationConvergence tests for the cluster DFT calculations
Covgc ss o h clus DF clculos. Covgc wh spc o bss s. s clculos o bss s covgc hv b po usg h PBE ucol o 7 os gg h-b. A s o h Guss bss ss wh csg s usss hs b us clug h -G -G** - ++G(p). A l sc o. Å h c bw h
More informationWAKEFIELD UNDULATOR RADIATION
WKEFIELD UNDULTOR RDITION. Opanasnko NSC KIPT, UKRINE MECHNISM OF WFU RDITION SPECTRL -NGULR CHRCTERISTICS MODEL OF WF UNDULTOR WKEFIELD DISTRIBUTION HRD X-RY GENERTING POSSIBILITY of EXPERIMENTL STUDY
More informationMotion Control Systems Chapter 1
Asf Šboć Kouh Ohsh Moo Cool Syss Chp Elcochcl Syss Dycs Moo Cool Syss Asf Šboć Kouh Ohsh 0 oh Wly Sos (As) P Bsc us Mchcl Syss Poso locy Foc wok Mou x F F ( xx ) p p x x W F Fx x x Kc gy Pol gy ol gy xx
More informationSuppose we have observed values t 1, t 2, t n of a random variable T.
Sppose we have obseved vales, 2, of a adom vaable T. The dsbo of T s ow o belog o a cea ype (e.g., expoeal, omal, ec.) b he veco θ ( θ, θ2, θp ) of ow paamees assocaed wh s ow (whee p s he mbe of ow paamees).
More informationOCCOQUAN RIVER CONDITION SURVEY PRINCE WILLIAM AND FAIRFAX COUNTIES, VIRGINIA CHARLES COUNTY, MARYLAND. BAY Havre De Grace INDEX OF DRAWINGS TITLE
2 3 5 t pp. pt W FFX, G t pp. k, Q l w h b pu x t v 33 wpt w 2 2 4 F.5.5 m pt m h 34 d 2 p p h flk flk 35 tmuth 36 8 4 36 3 pt F FX d W G l t l : l t dt: p hl mptm 2 32 h f,v.h tbug 3 ubm ttd b: p hl Wllmbug
More informationGet Funky this Christmas Season with the Crew from Chunky Custard
Hol Gd Chcllo Adld o Hdly Fdy d Sudy Nhs Novb Dcb 2010 7p 11.30p G Fuky hs Chss Sso wh h Cw fo Chuky Cusd Fdy Nhs $99pp Sudy Nhs $115pp Tck pc cluds: Full Chss d buff, 4.5 hou bv pck, o sop. Ts & Codos
More informationConvection in a Differentially Heated Narrow Slot By Teja Muppirala Advisor: Dr. Cho Lik Chan. University of Arizona, Spring/Summer 2002
Coco a Dffall Ha Naow Slo ja ala so: D. Co k Ca Us of zoa S/S Coco a ffall a aow slo of fl ca sla a ff s of bao o os of fl a os of slo. basc cl s a fl a o wall wll s o s cas a a fl a cool wall wll fall.
More informationThe Signal, Variable System, and Transformation: A Personal Perspective
The Sgal Varable Syem ad Traformao: A Peroal Perpecve Sherv Erfa 35 Eex Hall Faculy of Egeerg Oule Of he Talk Iroduco Mahemacal Repreeao of yem Operaor Calculu Traformao Obervao O Laplace Traform SSB A
More informationNumerical 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 information11/8/2002 CS 258 HW 2
/8/ CS 58 HW. G o a a qc of aa h < fo a I o goa o co a C cc c F ch ha F fo a I A If cc - c a co h aoa coo o ho o choo h o qc? I o g o -coa o o-coa? W ca choo h o qc o h a a h aa a. Tha f o o a h o h a:.
More informationLoad Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below.
oa Euatons Thoughout all of chapt 4, ou focus s on th machn tslf, thfo w wll only pfom a y smpl tatmnt of th ntwok n o to s a complt mol. W o that h, but alz that w wll tun to ths ssu n Chapt 9. So lt
More informationKey words: Fractional difference equation, oscillatory solutions,
OSCILLATION PROPERTIES OF SOLUTIONS OF FRACTIONAL DIFFERENCE EQUATIONS Musafa BAYRAM * ad Ayd SECER * Deparme of Compuer Egeerg, Isabul Gelsm Uversy Deparme of Mahemacal Egeerg, Yldz Techcal Uversy * Correspodg
More informationComputational Fluid Dynamics. Numerical Methods for Parabolic Equations. Numerical Methods for One-Dimensional Heat Equations
Compuaoal Flud Dyamcs p://www.d.edu/~gyggva/cfd-couse/ Compuaoal Flud Dyamcs p://www.d.edu/~gyggva/cfd-couse/ Compuaoal Flud Dyamcs Numecal Meods o Paabolc Equaos Lecue Mac 6 7 Géa Tyggvaso Compuaoal Flud
More information4/12/2018. PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105. Plan for Lecture 34: Review radiating systems
PHY 7 Eodynams 9-9:5 M MWF On 5 Pan o u : Rvw adang sysms Souon o Maxw s quaons wh sous Tm pod sous Examps //8 PHY 7 Spng 8 -- u //8 PHY 7 Spng 8 -- u Gna vw -- SI uns mosop o vauum om ( P M ): Couombs
More informationChapter 21: Connecting with a Network
Pag 319 This chap discusss how o us h BASIC-256 wokig sams. Nwokig i BASIC-256 will allow fo a simpl "sock" cocio usig TCP (Tasmissio Cool Poocol). This chap is o ma o b a full ioducio o TCP/IP sock pogammig.
More informationADAPTIVE MULTISCALE HOMOGENIZATION OF THE LATTICE DISCRETE PARTICLE MODEL FOR THE ANALYSIS OF DAMAGE AND FRACTURE IN CONCRETE
Ssl gg Gologl f ls (SG Dpm l ml gg om Shool gg ppld S s llo 6 US DT ULTSL HOOGZTO O TH LTT DSRT RTL ODL OR TH LYSS O DG D RTUR ORT Roozh Rzh w Zho Gl s SG TRL RORT o 7-/57 Smd l ol Solds Ss 7 dp ll Homogz
More informationThe Finite Difference Time Domain (FDTD) Method Discretizing Maxwell s equation in space and time
Chape 3 The Fe Dffeece Te Doa FDTD Mehod I hs chape we povde a evew of heoecal echques of FDTD ehod eploed he cue wo. Ou sulaos ae based o he well-ow fe-dffeece e-doa FDTD[] echque. The FDTD ehod s a goous
More informationSeries of New Information Divergences, Properties and Corresponding Series of Metric Spaces
Srs of Nw Iforao Dvrgcs, Proprs ad Corrspodg Srs of Mrc Spacs K.C.Ja, Praphull Chhabra Profssor, Dpar of Mahacs, Malavya Naoal Isu of Tchology, Japur (Rajasha), Ida Ph.d Scholar, Dpar of Mahacs, Malavya
More informationLuiz Leal Oak Ridge National Laboratory. of Massachusetts Institute. of Technology (MIT)
LzLl OkRdgNlLby LsPsdhNl Egg Dp f h MsshssIs f Thlgy(MIT) Csy f Lz Ll, Ok Rdg Nl Lby. Usd wh pss. NI T Idpd Tsp Eq f Φ(E,,Ωˆ ) Ωˆ. Φ + Σ Φ = dωˆ ' de'σ s (E' E, Ωˆ ' Ω)Φ(E', ',Ωˆ ) + S 4 π 0 Σ Msplsss
More informationFALL HOMEWORK NO. 6 - SOLUTION Problem 1.: Use the Storage-Indication Method to route the Input hydrograph tabulated below.
Jorge A. Ramírez HOMEWORK NO. 6 - SOLUTION Problem 1.: Use he Sorage-Idcao Mehod o roue he Ipu hydrograph abulaed below. Tme (h) Ipu Hydrograph (m 3 /s) Tme (h) Ipu Hydrograph (m 3 /s) 0 0 90 450 6 50
More informationSIMULATIUON OF SEISMIC ACTION FOR TBILISI CITY WITH LOCAL SEISMOLOGICAL PARTICULARITIES AND SITE EFFECTS
SIMULTIUON OF SEISMIC CTION FOR TBILISI CITY WITH LOCL SEISMOLOGICL PRTICULRITIES ND SITE EFFECTS Paaa REKVV ad Keeva MDIVNI Geoga Naoal ssocao fo Egeeg Sesmology ad Eahquake Egeeg Tbls Geoga ekvavapaaa@yahoo.com
More informationDr. Junchao Xia Center of Biophysics and Computational Biology. Fall /21/2016 1/23
BIO53 Bosascs Lcur 04: Cral Lm Thorm ad Thr Dsrbuos Drvd from h Normal Dsrbuo Dr. Juchao a Cr of Bophyscs ad Compuaoal Bology Fall 06 906 3 Iroduco I hs lcur w wll alk abou ma cocps as lsd blow, pcd valu
More informationAML710 CAD LECTURE 12 CUBIC SPLINE CURVES. Cubic Splines Matrix formulation Normalised cubic splines Alternate end conditions Parabolic blending
CUIC SLINE CURVES Cubc Sples Marx formulao Normalsed cubc sples Alerae ed codos arabolc bledg AML7 CAD LECTURE CUIC SLINE The ame sple comes from he physcal srume sple drafsme use o produce curves A geeral
More informationPartial Fraction Expansion
Paial Facion Expanion Whn ying o find h inv Laplac anfom o inv z anfom i i hlpfl o b abl o bak a complicad aio of wo polynomial ino fom ha a on h Laplac Tanfom o z anfom abl. W will illa h ing Laplac anfom.
More informationPlease turn in form and check to the office by Monday, December 11 th. Amazon.com. HomeGoods. American Express. Lowe s. American Girl. Macy s.
Wh d v p u h w f? B v Sp d m u v h hd, h d ju h wh u m fm b f u PTO! Sp p h M f d. If u d mh h d fm, h u h Bm f vb. Th hudd f h. W w b d hd d du Md, Dmb 11h d v bf h u Fd, Dmb 22d. F d v $100, u p f hm
More informationLeast Squares Fitting (LSQF) with a complicated function Theexampleswehavelookedatsofarhavebeenlinearintheparameters
Leas Squares Fg LSQF wh a complcaed fuco Theeampleswehavelookedasofarhavebeelearheparameers ha we have bee rg o deerme e.g. slope, ercep. For he case where he fuco s lear he parameers we ca fd a aalc soluo
More informationHandout 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 informationNikon i-line Glass Series
Nkon ln la S ln la VNTS Nkon a an vlopmn of qualy maal a alway bn la o n fo ompany opal pou. Pon ky fao. van n la noloy pn upon pon, an a Nkon xl. Nkon ln la wa vlop fo u w ln ( nm) loapy un. I lv anman
More information1 Lecture: pp
EE334 - Wavs and Phasos Lcu: pp -35 - -6 This cous aks vyhing ha you hav bn augh in physics, mah and cicuis and uss i. Easy, only nd o know 4 quaions: 4 wks on fou quaions D ρ Gauss's Law B No Monopols
More informationExponential Synchronization of the Hopfield Neural Networks with New Chaotic Strange Attractor
ITM Web of Cofeeces, 0509 (07) DOI: 0.05/ mcof/070509 ITA 07 Expoeal Sychozao of he Hopfeld Neual Newos wh New Chaoc Sage Aaco Zha-J GUI, Ka-Hua WANG* Depame of Sofwae Egeeg, Haa College of Sofwae Techology,qogha,
More informationAnalytical Investigation of Microwave Heating. Mohammad Robiul Hossan and Prashanta Dutta
Pcdgs f h ASME Iaal Mchacal Egg Cgss & Exps IMECE Nvb -8 Vacuv Bsh Cluba Caada IMECE-3 Aalycal Ivsga f Mcwav Hag Mhaad bul Hssa ad Pashaa Dua Schl f Mchacal ad Maals Egg Washg Sa Uvsy Pulla WA 9964-9 USA
More informationModern Topics in Solid-State Theory: Topological insulators and superconductors
Mor Topc ol-a Thor: Topolocal ulaor uprcoucor ra P. chr Ma-Plac-Iu für örprforchu, uar Uvrä uar Jauar 6 Topolocal ulaor uprcoucor. Topolocal b hor - Wha opolo? - H mol polacl) - hr ulaor IQH. Topolocal
More informationDynamics of Bloch Electrons 1
Dynamics of Bloch Elcons 7h Spmb 003 c 003, Michal Mad Dfiniions Dud modl Smiclassical dynamics Bloch oscillaions K P mhod Effciv mass Houson sas Zn unnling Wav pacs Anomalous vlociy Wanni Sa ladds d Haas
More informationExisting Conditions. View from Ice Rink Patio. Ice Rink Patio. Beginner Terrain and Lighting. Tubing Hill. Little Tow & Beginner Terrain
Bg T Lghg Tubg Hll Ic k P T f Bg T V f Sc Accss Nh Ll T & Bg T I Ex T Mc Bulg B f Bg T Pkg L & g Wll V f Ic k P MA S TE Bs A & Lghg Z E H E N AN ASSOCIATES, INC. ACHITECTUE PLANNING INTEIOS LANSCAPE ACHITECTUE
More information