Spin(calori)tronics = spin+heat+electronics
|
|
- Britney May
- 5 years ago
- Views:
Transcription
1 Spi(calori)troic = pi+hat+lctroic Grrit aur Sdai 仙台 Populatio:.046 illio Grrit E.W. aur Grrit aur Tohoku Uivrity ( 東北 学 ) Udrgraduat,094 Potgraduat 7,704 itratioal tudt,346 ctur DC Magtolctroic i. dfiitio ii. quatu chaic of pi iii. chag ad agti iv. pi traport i pi valv v. pi trafr torqu AC Magtolctroic 3 Spi Caloritroic Dfiitio Elctroic: Spitroic: Spi caloritroic: Cotrol of charg currt i all circuit ad dvic Gratio, dtctio, ad cotrol of charg ad pi currt Charg, pi, rgy ad tropy currt Elctroic i traport of charg Oh aw j V A V Gl V GV A R A G V E j E A A P V R G S h Grrit E.W. aur iar rpo of hat ad a traport: Fourir/Fick aw
2 Spi i agular otu Magtic ot i pi v Grrit E.W. aur M Ka & Schr 969 d r M V r v claical gyroagtic ratio Magtic dipol i a agtic fild Macropi U M T M Ergy Torqu d dt F d M M dt M - d dt T M dm d T M dt dt adau-ifhit quatio F M Forc piig top i gravity fild agtic ot i agtic fild Wolgag Pauli ad Nil ohr Elctro pi ad quatu chaic Wolfgag Pauli, yi, S 0 0 Tipp top Wikipdia 0 S 3
3 Elctro pi vctor oprator σ μg g ohr agto σ g 0 0 i 0 σ,, Pauli atric 0 i 0 0 ˆ g 0 0 H μ H 0 Rotatio i quatu chaic ˆ f f R d f, y f d, y dy f d dy y i f y fd ˆ d f y y (, y,0) d yd y y dy y d Fiit rotatio: li d ˆ i R ˆ li d log li log li ˆ i ˆ i logr li d ˆ ˆ R i ˆ Rotatio i quatu chaic Rotatio of a tat by a agl aroud a ai with uit vctor : R Rotatio oprator: ˆ R p i ˆ / Elctro pi: ˆ σ ˆ R y With co,i,0, R, 0 grat all poibl pi tat. Eapl: R, 0 ˆ R i σ / Spi o th loch phr R 0 / i y / 0 0, 0! 0 Chck: co i i co Spi-up tat i -dirctio i obtaid by rotatio about y-ai with.,0,0 0 R, 0 May-body probl ditiguihability ad Pauli cluio Prutatio atiytry:, 0 r, r r, r r, r 0 r r Two lctro caot b i th a tat or at th a pi ad otu coordiat. P r r r r,,, chag hol r r 3
4 Echag itractio rducd Coulob rpulio du to chag hol E Coul C r r M icrad kitic rgy by lctro cofit du to Hibrg ucrtaity rlatio p / p E ki M M r C avrag ditac btw lctro lctro ffctiv a Th pi-paralll (=frroagtic) tat i favorabl wh th kitic rgy cot du to Pauli pricipl i allr tha th Coulob rgy gai, i.. wh M * ad/or r ar larg. Thi rgy gai i calld chag itractio. Stor tallic frroagt : chag(-corrlatio) pottial that rflct th rgy plittig btw ajory ad iority pi tat. E F p F p F p y p Spi-dpdt diti, Fri Halftallic ota, frroagt ad obiliti Ab iitio bad tructur calculatio FCC-Co Hud rul ad uprchag F 3+, M + :3d 5 ad S=5/ uprchag: atifrroagtic couplig through filld hll Zwirycki, Xia, t al. (008) Yttriu ro Gart Y 3 (3+) F (3+) (F (3+) O 4 (-) ) 3 A.R. Chakhouradia - ot foud i atur - 80 ato/priitiv uit cll - frriagtic iulator - Curi tpratur 550 K - Gilbrt dapig ~0-5 4
5 ilayr ad pi valv Prpdicular aotructur crytalli aorphou MgO CoF Oid MgO tul barrir o th atoic cal TEM iag of a full dvic Appl. Phy. tt. 95, 39 (009) J. Appl. Phy. 05, (009) atral aotructur Spi-dpdt itrfac traiivity Atta 50 Py Cu pi valv Co Cu va W Co graph pi valv ajority iority Spi accuulatio ad pi currt F N c F N F pi valv d N d D f N d D f pi-flip diffuio lgth diffuio cotat pi-flip rlaatio ti V V V V 5
6 F N F pi valv F N F pi valv d d V V V V F N F pi valv: o-colliar d Slocwki torqu i half tal Noral / HMF / / logitudial pi currt travr pi currt = torqu = / /?????? N V V N = ubr of icoig chal Switchig by pi trafr Switchig by pi trafr 6
ECEN 5005 Crystals, Nanocrystals and Device Applications Class 14 Group Theory For Crystals
ECEN 5005 Cryta Naocryta ad Dvic Appicatio Ca 14 Group Thory For Cryta Spi Aguar Motu Quatu Stat of Hydrog-ik Ato Sig Ectro Cryta Fid Thory Fu Rotatio Group 1 Spi Aguar Motu Spi itriic aguar otu of ctro
More informationMagnetic 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 informationCh. 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 information1985 AP Calculus BC: Section I
985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b
More informationToday 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 informationSolid State Device Fundamentals
8 Biasd - Juctio Solid Stat Dvic Fudamtals 8. Biasd - Juctio ENS 345 Lctur Cours by Aladr M. Zaitsv aladr.zaitsv@csi.cuy.du Tl: 718 98 81 4N101b Dartmt of Egirig Scic ad Physics Biasig uiolar smicoductor
More informationAnalysis of a Finite Quantum Well
alysis of a Fiit Quatu Wll Ira Ka Dpt. of lctrical ad lctroic girig Jssor Scic & Tcology Uivrsity (JSTU) Jssor-748, Baglads ika94@uottawa.ca Or ikr_c@yaoo.co Joural of lctrical girig T Istitutio of girs,
More informationSession : Plasmas in Equilibrium
Sssio : Plasmas i Equilibrium Ioizatio ad Coductio i a High-prssur Plasma A ormal gas at T < 3000 K is a good lctrical isulator, bcaus thr ar almost o fr lctros i it. For prssurs > 0.1 atm, collisio amog
More informationLecture contents. Transport, scattering Generation/recombination. E c. E t. E v. NNSE508 / NENG452 Lecture #13. Band-to-band recombination
Lctur cotts Trasort, scattrig Gratio/rcobiatio E E c E t E v Bad-to-bad rcobiatio Tra-assistd (SRH) rcobiatio ad gratio Augr rcobiatio Elctro trasort: Gral cosidratios How fr carrirs ract o xtral lctric
More informationSpin(calori)tronics = spin+heat+electronics
Heat = (ergy ー Work) pi(calori)troic = pi+heat+electroic errit Bauer errit.w. Bauer "CD orced Covectio Heat ik " by Iofil Lecture DC Magetoelectroic 2 AC Magetoelectroic 3 pi Caloritroic i. Theroelectric
More informationNarayana IIT Academy
INDIA Sc: LT-IIT-SPARK Dat: 9--8 6_P Max.Mars: 86 KEY SHEET PHYSIS A 5 D 6 7 A,B 8 B,D 9 A,B A,,D A,B, A,B B, A,B 5 A 6 D 7 8 A HEMISTRY 9 A B D B B 5 A,B,,D 6 A,,D 7 B,,D 8 A,B,,D 9 A,B, A,B, A,B,,D A,B,
More informationReview Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2
MATHEMATIS --RE Itgral alculus Marti Huard Witr 9 Rviw Erciss. Evaluat usig th dfiitio of th dfiit itgral as a Rima Sum. Dos th aswr rprst a ara? a ( d b ( d c ( ( d d ( d. Fid f ( usig th Fudamtal Thorm
More informationcoulombs or esu charge. It s mass is about 1/1837 times the mass of hydrogen atom. Thus mass of electron is
1 ATOMIC STRUCTURE Fudamtal Particls: Mai Fudamtal Particl : (a) Elctro: It is a fudamtal particl of a atom which carris a uit gativ charg. It was discovrd by J.J. Thomso (1897) from th studis carrid out
More informationLECTURE 13 Filling the bands. Occupancy of Available Energy Levels
LUR 3 illig th bads Occupacy o Availabl rgy Lvls W hav dtrmid ad a dsity o stats. W also d a way o dtrmiig i a stat is illd or ot at a giv tmpratur. h distributio o th rgis o a larg umbr o particls ad
More informationELG3150 Assignment 3
ELG350 Aigmt 3 Aigmt 3: E5.7; P5.6; P5.6; P5.9; AP5.; DP5.4 E5.7 A cotrol ytm for poitioig th had of a floppy dik driv ha th clodloop trafr fuctio 0.33( + 0.8) T ( ) ( + 0.6)( + 4 + 5) Plot th pol ad zro
More informationOutline. Ionizing Radiation. Introduction. Ionizing radiation
Outli Ioizig Radiatio Chaptr F.A. Attix, Itroductio to Radiological Physics ad Radiatio Dosimtry Radiological physics ad radiatio dosimtry Typs ad sourcs of ioizig radiatio Dscriptio of ioizig radiatio
More informationTHz intervalence band antipolaritons
THz itrvalc bad atipolaritos FARAGAI, Iuwa A ad PEREIRA, Mauro Availabl from Shffild Hallam Uivrsity Rsarch Archiv (SHURA) at: http://shura.shu.ac.uk/8488/ This documt
More informationMONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx
MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of
More informationThe 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 information8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions
Solutios for HW 8 Captr 5 Cocptual Qustios 5.. θ dcrass. As t crystal is coprssd, t spacig d btw t plas of atos dcrass. For t first ordr diffractio =. T Bragg coditio is = d so as d dcrass, ust icras for
More informationDigital Signal Processing, Fall 2006
Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti
More informationLecture contents. Semiconductor statistics. NNSE508 / NENG452 Lecture #12
Ltur otts Sioutor statistis S58 / G45 Ltur # illig th pty bas: Distributio futio ltro otratio at th rgy (Dsity of stats) (istributio futio): ( ) ( ) f ( ) Pauli lusio Priipl: o two ltros (frios) a hav
More informationc z c z c z c z c c c c a a c A P( a ) a c a z c x z R j z z, z z z z I
. Quatu Spi States State Vectors c c i Ier Products: * * c c oralied. orthogoal c c c c c c * * i ii Probability that a particle i state ca be foud i state. c. States i S -basis y i i Geeral States. c
More informationMagnetic Moment of the Proton
SB/F/35.3-2 Magtic Mot of th Proto G. Gozálz-Martí*, I.Taboada Dpartato d Física, Uivrsidad Sió Bolívar, Apartado 89, Caracas 18-A, Vzula. ad J. Gozálz Physics Dpartt, Northatr Uivrsity, Bosto, U.S.A.
More informationCombined effects of Hall current and rotation on free convection MHD flow in a porous channel
Idia Joural of Pur & Applid Physics Vol. 47, Sptbr 009, pp. 67-63 Cobid ffcts of Hall currt ad rotatio o fr covctio MHD flow i a porous chal K D Sigh & Raksh Kuar Dpartt of Mathatics (ICDEOL, H P Uivrsy,
More informationECE 340 Lecture 38 : MOS Capacitor I Class Outline:
ECE 34 Lctur 38 : MOS Capacitor I Class Outli: Idal MOS Capacitor higs you should ow wh you lav Ky Qustios What ar th diffrt ias rgios i MOS capacitors? What do th lctric fild ad lctrostatic pottial loo
More informationFermi Gas. separation
ri Gas Distiguishabl Idistiguishabl Classical dgrat dd o dsity. If th wavlgth siilar to th saratio tha dgrat ri gas articl h saratio largr traturs hav sallr wavlgth d tightr ackig for dgracy
More informationIdeal crystal : Regulary ordered point masses connected via harmonic springs
Statistical thrmodyamics of crystals Mooatomic crystal Idal crystal : Rgulary ordrd poit masss coctd via harmoic sprigs Itratomic itractios Rprstd by th lattic forc-costat quivalt atom positios miima o
More informationLectur 22. RF and Microwave Circuit Design Γ-Plane and Smith Chart Analysis. ECE 303 Fall 2005 Farhan Rana Cornell University
ctur RF ad Micrwav Circuit Dig -Pla ad Smith Chart Aalyi I thi lctur yu will lar: -pla ad Smith Chart Stub tuig Quartr-Wav trafrmr ECE 33 Fall 5 Farha Raa Crll Uivrity V V Impdac Trafrmati i Tramii i ω
More information1 of 42. Abbreviated title: [SAP-SVT-Nmsm-g & 137] - Updated on 31 July, 09. Shankar V.Narayanan
1 of 4 ONE EQUATION ad FOUR Subatomic Particls ad thir FOUR Itractios icludig (g &17) factors with Spac Vortx Thory (A No matrial shll modl) (Part 1 of ) (Th cotts of this txt ar th sam as i Subatomic
More informationCircular Array of Tapered Nylon Rod Antennas: A Computational Study
tratioal Joural of Elctroics ad Commuicatio Egirig. SSN 974-266 Volum 4, Numbr (2), pp.3-38 tratioal Rsarch Publicatio Hous http://www.irphous.com Circular Array of Taprd Nylo Rod Atas: A Computatioal
More informationS- AND P-POLARIZED REFLECTIVITIES OF EXPLOSIVELY DRIVEN STRONGLY NON-IDEAL XENON PLASMA
S- AND P-POLARIZED REFLECTIVITIES OF EXPLOSIVELY DRIVEN STRONGLY NON-IDEAL XENON PLASMA Zaporozhts Yu.B.*, Mitsv V.B., Gryazov V.K., Riholz H., Röpk G. 3, Fortov V.E. 4 Istitut of Problms of Chmical Physics
More information10. Excitons in Bulk and Two-dimensional Semiconductors
Excitos i Bulk ad Two-dimsioal Smicoductors Th Wair modl drivd i th prvious chaptr provids a simpl framwork for th iclusio of xcitos i th optical proprtis of smicoductors I this chaptr w will valuat th
More informationTerahertz band-gap in InAs/GaSb type II superlattices
Trart Scic ad Tcology, ISSN 1941-7411 Vol.1, No 4, Dcmbr 008 Trart bad-gap i IAs/GaSb typ II suprlattics L.L. Li 1, W. Xu 1, 3, Z. Zg 1, ad Y.L. Si 1 Ky Laboratory of Matrials Pysics, Istitut of Solid
More informationEstimating 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( ) 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 information1 of 46. Abbreviated title: [SAP-SVT-Nmsm-g & 137] - Updated on 07 Oct, 09. Shankar V.Narayanan
1 of 46 Subatomic Particls ad thir FOUR Itractios icludig (g &17) (p&) factors with Spac Vortx Thory (A No matrial shll modl) (Part 1 of ) (Th cotts of this txt ar th sam as i ONE EQUATION ad FOUR Subatomic
More informationChapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1
Chatr Fiv Mor Dimsios 51 Th Sac R W ar ow rard to mov o to sacs of dimsio gratr tha thr Ths sacs ar a straightforward gralizatio of our Euclida sac of thr dimsios Lt b a ositiv itgr Th -dimsioal Euclida
More informationEE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors
3 Lightwav Dvics Lctur 3: Basic Smicoductor Physics ad Optical Procsss Istructor: Mig C. Wu Uivrsity of Califoria, Brly lctrical girig ad Computr Scics Dpt. 3 Lctur 3- Optical Proprtis of Smicoductors
More informationTopological Insulators in 2D and 3D
Topological Isulators i D ad 3D 0. Elctric polarizatio, Chr Numbr, Itgr Quatum Hall Effct I. Graph - Halda modl - Tim rvrsal symmtry ad Kramrs thorm II. D quatum spi Hall isulator - Z topological ivariat
More informationIII.5. THE THERMISTOR
III.5. H HRMISOR 1. Wor uros o cc t law dscribig t tratur ddc of t lctrical rsistac of sicoductor atrials ad to valuat tir ga.. ory Quatu caics stats tat isolatd icrosysts (lctros, olculs, ios) av oly
More informationTransport electronique
rasport lctroiqu Josph P. Hras Dpartt o Mchaical ad Arospac girig Dpartt o Physics h Ohio Stat Uirsity, Colubus, Ohio 4, USA Hras.@osu.du s ots sot aglais, ais j parlrai racais i accts, i cdills Rrcs:
More informationP 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 informationPH4210 Statistical Mechanics
PH4 Statistical Mchaics Probl Sht Aswrs Dostrat that tropy, as giv by th Boltza xprssio S = l Ω, is a xtsiv proprty Th bst way to do this is to argu clarly that Ω is ultiplicativ W ust prov that if o syst
More informationChapter 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 informationScattering Parameters. Scattering Parameters
Motivatio cattrig Paramtrs Difficult to implmt op ad short circuit coditios i high frqucis masurmts du to parasitic s ad Cs Pottial stability problms for activ dvics wh masurd i oopratig coditios Difficult
More informationJoule-Lenz Energy of Quantum Electron Transitions Compared with the Electromagnetic Emission of Energy
Joural of Modr Physics, 06, 7, 440-448 Publishd Oli August 06 i SciRs http://wwwscirporg/joural/jmp http://dxdoiorg/0436/jmp0673 Joul-Lz Ergy of Quatum Elctro Trasitios Compard with th Elctromagtic Emissio
More information1. Brillouin zones of rectangular lattice. Make a plot of the first two Brillouin zones of a primitive rectangular two-dimensional lattice with axes
Chap9 練 Brilloui oe of rectagular lattice Mae a plot of the firt two Brilloui oe of a priitive rectagular two-dieioal lattice with axe a b=3a Brilloui oe rectagular lattice A two-dieioal etal ha oe ato
More informationBipolar Junction Transistors
ipolar Juctio Trasistors ipolar juctio trasistors (JT) ar activ 3-trmial dvics with aras of applicatios: amplifirs, switch tc. high-powr circuits high-spd logic circuits for high-spd computrs. JT structur:
More informationWeights 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 informationRÉSONATEURS NANOMÉCANIQUES DANS LE RÉGIME QUANTIQUE NANOMECHANICAL RESONATORS IN QUANTUM REGIME
Chair d Physiqu Mésoscopiqu Michl Dvort Aé 01, 15 ai - 19 ju RÉSONATEURS NANOMÉCANIQUES DANS LE RÉGIME QUANTIQUE NANOMECHANICAL RESONATORS IN QUANTUM REGIME Cquiè lço / Fifth lctur This Collg d Frac docut
More informationDTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1
DTFT Proprtis Exampl - Dtrmi th DTFT Y of y α µ, α < Lt x α µ, α < W ca thrfor writ y x x From Tabl 3., th DTFT of x is giv by ω X ω α ω Copyright, S. K. Mitra Copyright, S. K. Mitra DTFT Proprtis DTFT
More informationPURE MATHEMATICS A-LEVEL PAPER 1
-AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio
More information5. Quantum Nature of the Nano-world ( Fundamental of. Quantum mechanics)
5. Quatu Nature of the Nao-world Fudaetal of What is the defiitio of aoaterials?? Quatu echaics i Origial: quatu size effect where the electroic properties of solids are altered with great reductios i
More informationThe 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 informationSuperfluid Liquid Helium
Surfluid Liquid Hlium:Bo liquid ad urfluidity Ladau thory: two fluid modl Bo-iti Codatio ad urfluid ODLRO, otaou ymmtry brakig, macrocoic wafuctio Gro-Pitakii GP quatio Fyma ictur Rfrc: Thory of quatum
More informationChapter 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 informationChp6. pn Junction Diode: I-V Characteristics I
147 C6. uctio Diod: I-V Caractristics I 6.1. THE IDEAL DIODE EQUATION 6.1.1. Qualitativ Drivatio 148 Figur rfrc: Smicoductor Dvic Fudamtals Robrt F. Pirrt, Addiso-Wsly Publicig Comay 149 Figur 6.1 juctio
More informationThe Phase Probability for Some Excited Binomial States
Egypt. J. Sl., Vl. 5, N., 3 Th Pha Prbability fr S Excitd Biial Stat. Darwih Faculty f Educati, Suz Caal Uivrity at Al-Arih, Egypt. I thi papr, th pha prprti i Pgg-Bartt frali ar cidrd. Th pha ditributi
More informationTime : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120
Tim : hr. Tst Papr 8 D 4//5 Bch - R Marks : SINGLE CORRECT CHOICE TYPE [4, ]. If th compl umbr z sisfis th coditio z 3, th th last valu of z is qual to : z (A) 5/3 (B) 8/3 (C) /3 (D) o of ths 5 4. Th itgral,
More informationWashington State University
he 3 Ktics ad Ractor Dsig Sprg, 00 Washgto Stat Uivrsity Dpartmt of hmical Egrg Richard L. Zollars Exam # You will hav o hour (60 muts) to complt this xam which cosists of four (4) problms. You may us
More informationNumerical study of the lattice vacancy effects on the quantum transport of four-terminal graphene nanodevice
Idia Joural of Pur & Applid Physics Vol. 52, Octobr 2014, pp. 678-683 Numrical study of th lattic vacacy ffcts o th quatum trasport of four-trmial graph aodvic A Jafari*, M Ghoraviss, M R Hathzadh & R
More informationPPS (Pottial Path Spac) i y i l j Vij (2) H x PP (Pottial Path ra) (gravity-typ masur) i i i j1 cij (1) D j j c ij ij 4)7) 8), 9) D j V ij j i 198 1)1
1 2 3 1 (68-8552 4 11) E-mail: taimoto@ss.tottori-u.ac.jp 2 (68-8552 4 11) 3 (657-851 1-1) Ky Words: accssibility, public trasportatio plaig, rural aras, tim allocatio, spac-tim prism 197 Hady ad Nimir
More informationDerivation of a Predictor of Combination #1 and the MSE for a Predictor of a Position in Two Stage Sampling with Response Error.
Drivatio of a Prdictor of Cobiatio # ad th SE for a Prdictor of a Positio i Two Stag Saplig with Rspos Error troductio Ed Stak W driv th prdictor ad its SE of a prdictor for a rado fuctio corrspodig to
More informationThe state space model needs 5 parameters, so it is not as convenient to use in this control study.
Trasfer fuctio for of the odel G θ K ω 2 θ / v θ / v ( s) = = 2 2 vi s + 2ζωs + ω The followig slides detail a derivatio of this aalog eter odel both as state space odel ad trasfer fuctio (TF) as show
More informationChapter At each point (x, y) on the curve, y satisfies the condition
Chaptr 6. At ach poit (, y) o th curv, y satisfis th coditio d y 6; th li y = 5 is tagt to th curv at th poit whr =. I Erciss -6, valuat th itgral ivolvig si ad cosi.. cos si. si 5 cos 5. si cos 5. cos
More informationConsider serial transmission. In Proakis notation, we receive
5..3 Dciio-Dirctd Pha Trackig [P 6..4] 5.-1 Trackr commoly work o radom data igal (plu oi), o th kow-igal modl do ot apply. W till kow much about th tructur o th igal, though, ad w ca xploit it. Coidr
More informationPhysics 2D Lecture Slides Lecture 14: Feb 3 rd 2004
Bria Wcht, th TA is back! Pl. giv all rgrad rqusts to him Quiz 4 is This Friday Physics D Lctur Slids Lctur 14: Fb 3 rd 004 Vivk Sharma UCSD Physics Whr ar th lctros isid th atom? Early Thought: Plum puddig
More informationMechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter
Time Respose & Frequecy Respose d -Order Dyamic System -Pole, Low-Pass, Active Filter R 4 R 7 C 5 e i R 1 C R 3 - + R 6 - + e out Assigmet: Perform a Complete Dyamic System Ivestigatio of the Two-Pole,
More informationControl 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 informationES.182A Topic 40 Notes Jeremy Orloff
ES.182A opic 4 Notes Jeremy Orloff 4 Flux: ormal form of Gree s theorem Gree s theorem i flux form is formally equivalet to our previous versio where the lie itegral was iterpreted as work. Here we will
More informationln x = n e = 20 (nearest integer)
H JC Prlim Solutios 6 a + b y a + b / / dy a b 3/ d dy a b at, d Giv quatio of ormal at is y dy ad y wh. d a b () (,) is o th curv a+ b () y.9958 Qustio Solvig () ad (), w hav a, b. Qustio d.77 d d d.77
More informationELEC 372 LECTURE NOTES, WEEK 4 Dr. Amir G. Aghdam Concordia University
ELEC 37 LECTURE NOTES, WEE 4 Dr Amir G Aghdam Cocordia Uiverity Part of thee ote are adapted from the material i the followig referece: Moder Cotrol Sytem by Richard C Dorf ad Robert H Bihop, Pretice Hall
More informationChapter (8) Estimation and Confedence Intervals Examples
Chaptr (8) Estimatio ad Cofdc Itrvals Exampls Typs of stimatio: i. Poit stimatio: Exampl (1): Cosidr th sampl obsrvatios, 17,3,5,1,18,6,16,10 8 X i i1 17 3 5 118 6 16 10 116 X 14.5 8 8 8 14.5 is a poit
More informationExercises for lectures 23 Discrete systems
Exrciss for lcturs 3 Discrt systms Michal Šbk Automatické říí 06 30-4-7 Stat-Spac a Iput-Output scriptios Automatické říí - Kybrtika a robotika Mols a trasfrs i CSTbx >> F=[ ; 3 4]; G=[ ;]; H=[ ]; J=0;
More informationDiscrete Fourier Transform (DFT)
Discrt Fourir Trasorm DFT Major: All Egirig Majors Authors: Duc guy http://umricalmthods.g.us.du umrical Mthods or STEM udrgraduats 8/3/29 http://umricalmthods.g.us.du Discrt Fourir Trasorm Rcalld th xpotial
More informationQuasi-Supercontinuum Interband Lasing Characteristics of Quantum Dot Nanostructures
USOD 008 ottiha UK Quasi-Suprcotiuu Itrbad Lasi Charactristics of Quatu Dot aostructurs C. L. a Y. Wa H. S. Di B. S. Ooi Ctr for Optica choois ad Dpartt of ctrica ad Coputr iri Lhih Uivrsity Bthh Psyvaia
More informationWBJEE Answer Keys by Aakash Institute, Kolkata Centre
WBJEE - 7 Aswer Keys by, Kolkata Cetre MATHEMATICS Q.No. B A C B A C A B 3 D C B B 4 B C D D 5 D A B B 6 C D B B 7 B C C A 8 B B A A 9 A * B D C C B B D A A D B B C B 3 A D D D 4 C B A A 5 C B B B 6 C
More informationLithium-Ion battery State of Charge estimation with a Kalman Filter based on a electrochemical model
thium-o battry Stat of Charg timatio with a Kalma Filtr bad o a lctrochmical modl Domico Di Domico, Giovai Figo ad a Stfaopoulou btract thium-io battry i th cor of w plug-i hybrid-lctrical vhicl PHEV a
More informationMILLIKAN OIL DROP EXPERIMENT
11 Oct 18 Millika.1 MILLIKAN OIL DROP EXPERIMENT This xprimt is dsigd to show th quatizatio of lctric charg ad allow dtrmiatio of th lmtary charg,. As i Millika s origial xprimt, oil drops ar sprayd ito
More informationNote: Torque is prop. to current Stationary voltage is prop. to speed
DC Mach Cotrol Mathmatcal modl. Armatr ad orq f m m a m m r a a a a a dt d ψ ψ ψ ω Not: orq prop. to crrt Statoary voltag prop. to pd Mathmatcal modl. Fld magtato f f f f d f dt a f ψ m m f f m fλ h torq
More informationConditions for equilibrium (both translational and rotational): 0 and 0
Leon : Equilibriu, Newton econd law, Rolling, Angular Moentu (Section 8.3- Lat tie we began dicuing rotational dynaic. We howed that the rotational inertia depend on the hape o the object and the location
More informationu t u 0 ( 7) Intuitively, the maximum principles can be explained by the following observation. Recall
Oct. Heat Equatio M aximum priciple I thi lecture we will dicu the maximum priciple ad uiquee of olutio for the heat equatio.. Maximum priciple. The heat equatio alo ejoy maximum priciple a the Laplace
More informationLecture contents. Density of states Distribution function Statistic of carriers. Intrinsic Extrinsic with no compensation Compensation
Ltur otts Dsity of stats Distributio futio Statisti of arrirs Itrisi trisi with o ompsatio ompsatio S 68 Ltur #7 Dsity of stats Problm: alulat umbr of stats pr uit rgy pr uit volum V() Larg 3D bo (L is
More informationKISS: A Bit Too Simple. Greg Rose
KI: A Bit Too impl Grg Ros ggr@qualcomm.com Outli KI radom umbr grator ubgrators Efficit attack N KI ad attack oclusio PAGE 2 O approach to PRNG scurity "A radom umbr grator is lik sx: Wh it's good, its
More informationComparisons of the Variance of Predictors with PPS sampling (update of c04ed26.doc) Ed Stanek
Coparo o th Varac o Prdctor wth PPS aplg (updat o c04d6doc Ed Sta troducto W copar prdctor o a PSU a or total bad o PPS aplg Th tratgy to ollow that o Sta ad Sgr (JASA, 004 whr w xpr th prdctor a a lar
More informationPhysics 324, Fall Dirac Notation. These notes were produced by David Kaplan for Phys. 324 in Autumn 2001.
Physics 324, Fall 2002 Dirac Notatio These otes were produced by David Kapla for Phys. 324 i Autum 2001. 1 Vectors 1.1 Ier product Recall from liear algebra: we ca represet a vector V as a colum vector;
More informationResonant Spin Hall Effect in Two Dimensional Electron Gas
Reoat Spi Hall Effect i Two Dimeioal Electro Ga Dr. Shu-Qig She Departmet of Phic The Uiverit of Hog Kog December / 4 4 Beijig Collaborator (o pi Hall effect) Profeor Michael Ma (Uiverit of Ciciatti) Profeor
More informationPartition Functions and Ideal Gases
Partitio Fuctios ad Idal Gass PFIG- You v lard about partitio fuctios ad som uss ow w ll xplor tm i mor dpt usig idal moatomic diatomic ad polyatomic gass! for w start rmmbr: Q( N ( N! N Wat ar N ad? W
More informationCourse 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(c) Write, but do not evaluate, an integral expression for the volume of the solid generated when R is
Calculus BC Fial Review Name: Revised 7 EXAM Date: Tuesday, May 9 Remiders:. Put ew batteries i your calculator. Make sure your calculator is i RADIAN mode.. Get a good ight s sleep. Eat breakfast. Brig:
More information2D DSP Basics: Systems Stability, 2D Sampling
- Digital Iage Processig ad Copressio D DSP Basics: Systes Stability D Saplig Stability ty Syste is stable if a bouded iput always results i a bouded output BIBO For LSI syste a sufficiet coditio for stability:
More informationNarayana IIT Academy
-0-8_Sr. IIT_IZ_Ph-I_JEE-ADV_New Model-_P_GTA-9_Key&Sol s Narayaa IIT Academy INDIA Sec: Sr.IIT_IZ GTA-9 Date: -0-8 Time: 0:00 PM to 05:00 PM NEW Model-(P) Ma Marks: 64 KEY & SLUTINS MATHS AB ABC 3 AB
More informationSupplementary Information
Suppleetary Iforatio -Breakdow of cotiuu fracture echaics at the aoscale- Takahiro Shiada,,* Keji Ouchi, Yuu Chihara, ad Takayuki Kitaura Departet of echaical Egieerig ad Sciece, Kyoto Uiversity, Nishikyo-ku,
More informationELECTROMAGNETIC FIELD COUPLING TO ARBITRARY WIRE CONFIGURATIONS BURIED IN A LOSSY GROUND: A REVIEW OF ANTENNA MODEL AND TRANSMISSION LINE APPROACH
D. Poljak t al., It. J. Comp. Mth. ad Exp. Ma., Vol., No. (3) 4 63 ELECTROMAGNETIC FIELD COUPLING TO ARBITRARY WIRE CONFIGURATIONS BURIED IN A LOSSY GROUND: A REVIEW OF ANTENNA MODEL AND TRANSMISSION LINE
More informationFluid Physics 8.292J/12.330J % (1)
Fluid Physics 89J/133J Problem Set 5 Solutios 1 Cosider the flow of a Euler fluid i the x directio give by for y > d U = U y 1 d for y d U + y 1 d for y < This flow does ot vary i x or i z Determie the
More informationA =A +VA, A =d A, A =A (r r'). Within the Coulomb gauge, the transverse vector potential associated to spatially uniform, time-independent
PHYSICAL REVIEW A VOLUME 45, NUMBER 9 1 MAY 199 Calculatio of molcular magtic proprtis withi th Ladau gaug M. B.Frraro ad T. E. Hrr Dpartamto d F&sica, Facultad d Cicias Exactas y Naturals, Uivrsidad d
More informationCalculus Revision A2 Level
alculus Rvision A Lvl Tabl of drivativs a n sin cos tan d an sc n cos sin Fro AS * NB sc cos sc cos hain rul othrwis known as th function of a function or coposit rul. d d Eapl (i) (ii) Obtain th drivativ
More informationCPU Frequency Tuning for Optimizing the Energy. David Brayford 1
CPU Frqucy Tuig or Optimizig th Ergy to Solutio. David Brayord Brayord@lrz.d 1 Cost o Larg HPC Systms Computr Hardwar HPC systm, cabls, data archivig systm tc. Buildig Th availability ad pric o ral stat.
More informationElectromagnetic radiation and steady states of hydrogen atom
Elctromagtic radiatio ad stady stats of hydrog atom Jiaomig Luo Egirig Rsarch Ctr i Biomatrials, Sichua Uivrsity, 9# Wagjiag Road, Chgdu, Chia, 610064 Abstract. Elctromagtic phoma i hydrog atom ar cotrolld
More information