Ultrahigh Frequency Generation in GaAs-type. Two-Valley Semiconductors

Similar documents
Physics 232 Exam I Feb. 14, 2005

Physics 232 Exam I Feb. 13, 2006

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of

BINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k =

Generalized Fibonacci-Type Sequence and its Properties

Week 8 Lecture 3: Problems 49, 50 Fourier analysis Courseware pp (don t look at French very confusing look in the Courseware instead)

F.Y. Diploma : Sem. II [CE/CR/CS] Applied Mathematics

The sphere of radius a has the geographical form. r (,)=(acoscos,acossin,asin) T =(p(u)cos v, p(u)sin v,q(u) ) T.

TEST-12 TOPIC : SHM and WAVES

ONE RANDOM VARIABLE F ( ) [ ] x P X x x x 3

Lecture 3 summary. C4 Lecture 3 - Jim Libby 1

Duration Notes 1. To motivate this measure, observe that the duration may also be expressed as. a a T a

EE757 Numerical Techniques in Electromagnetics Lecture 9

Suggested Solution for Pure Mathematics 2011 By Y.K. Ng (last update: 8/4/2011) Paper I. (b) (c)

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt.

The Complete Graph: Eigenvalues, Trigonometrical Unit-Equations with associated t-complete-eigen Sequences, Ratios, Sums and Diagrams

Physics 232 Exam II Mar. 28, 2005

Existence Of Solutions For Nonlinear Fractional Differential Equation With Integral Boundary Conditions

Chapter 1 Electromagnetic Field Theory

E&CE 476 Antenna and Wireless Systems Final Examination

ANALYSIS OF THERMOELASTIC DISC WITH RADIATION CONDITIONS ON THE CURVED SURFACES

Mathematical Statistics

1. Six acceleration vectors are shown for the car whose velocity vector is directed forward. For each acceleration vector describe in words the

). So the estimators mainly considered here are linear

MOSFET device models and conventions

Review for the Midterm Exam.

ANSWER KEY PHYSICS. Workdone X

D zone schemes

A new approach to Kudryashov s method for solving some nonlinear physical models

NEIGHBOURHOODS OF A CERTAIN SUBCLASS OF STARLIKE FUNCTIONS. P. Thirupathi Reddy. E. mail:

SUMMATION OF INFINITE SERIES REVISITED

LIPSCHITZ ESTIMATES FOR MULTILINEAR COMMUTATOR OF MARCINKIEWICZ OPERATOR

Outline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem

Relation (12.1) states that if two points belong to the convex subset Ω then all the points on the connecting line also belong to Ω.

rad / sec min rev 60sec. 2* rad / sec s

Multi-Electron Atoms-Helium

T h e C S E T I P r o j e c t

S, we call the base curve and the director curve. The straight lines

Wave Propagation in Rectangular Waveguide Filled with Anisotropic Metamaterial

Reinforcement Learning

Calculus BC 2015 Scoring Guidelines


On the k-lucas Numbers of Arithmetic Indexes

0 otherwise. sin( nx)sin( kx) 0 otherwise. cos( nx) sin( kx) dx 0 for all integers n, k.

Inverse Thermoelastic Problem of Semi-Infinite Circular Beam

Physics 235 Final Examination December 4, 2006 Solutions

Some algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER

Supplementary Information

BINOMIAL THEOREM SOLUTION. 1. (D) n. = (C 0 + C 1 x +C 2 x C n x n ) (1+ x+ x 2 +.)

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

African Journal of Science and Technology (AJST) Science and Engineering Series Vol. 4, No. 2, pp GENERALISED DELETION DESIGNS

Transient Solution of the M/M/C 1 Queue with Additional C 2 Servers for Longer Queues and Balking

e t dt e t dt = lim e t dt T (1 e T ) = 1

DERIVING THE DEMAND CURVE ASSUMING THAT THE MARGINAL UTILITY FUNCTIONS ARE LINEAR

Math 2414 Homework Set 7 Solutions 10 Points

2.Decision Theory of Dependence

Journal of Engineering Science and Technology Review 6 (1) (2013) Research Article

RESPONSE OF A RECTANGULAR PLATE TO BASE EXCITATION Revision E W( )

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.

Department of Mathematics. Birla Institute of Technology, Mesra, Ranchi MA 2201(Advanced Engg. Mathematics) Session: Tutorial Sheet No.

PHYSICS 102. Intro PHYSICS-ELECTROMAGNETISM

() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration

Cameras and World Geometry

Graphing Review Part 3: Polynomials

Extension of Hardy Inequality on Weighted Sequence Spaces

Technical Vibration - text 2 - forced vibration, rotational vibration

Fourier Series and Applications

HOMEWORK 6 - INTEGRATION. READING: Read the following parts from the Calculus Biographies that I have given (online supplement of our textbook):

Schrödinger Equation Via Laplace-Beltrami Operator

ME 141. Engineering Mechanics

x a y n + b = 1 0<b a, n > 0 (1.1) x 1 - a y = b 0<b a, n > 0 (1.1') b n sin 2 + cos 2 = 1 x n = = cos 2 6 Superellipse (Lamé curve)

ALGEBRA II CHAPTER 7 NOTES. Name

S n. = n. Sum of first n terms of an A. P is

f(bx) dx = f dx = dx l dx f(0) log b x a + l log b a 2ɛ log b a.

C(p, ) 13 N. Nuclear reactions generate energy create new isotopes and elements. Notation for stellar rates: p 12

Applications of force vibration. Rotating unbalance Base excitation Vibration measurement devices

Statistical Optics and Free Electron Lasers

PROGRESSION AND SERIES

«A first lesson on Mathematical Induction»

Spectrum of The Direct Sum of Operators. 1. Introduction

Comparison between Fourier and Corrected Fourier Series Methods

IJRET: International Journal of Research in Engineering and Technology eissn: pissn:

EE757 Numerical Techniques in Electromagnetics Lecture 8

Parameter Estimation and Hypothesis Testing of Two Negative Binomial Distribution Population with Missing Data

Rotations.

The Non-Truncated Bulk Arrival Queue M x /M/1 with Reneging, Balking, State-Dependent and an Additional Server for Longer Queues

42. (20 pts) Use Fermat s Principle to prove the law of reflection. 0 x c

[ 20 ] 1. Inequality exists only between two real numbers (not complex numbers). 2. If a be any real number then one and only one of there hold.

LECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1.

On Almost Increasing Sequences For Generalized Absolute Summability

By the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences

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

Available online at J. Math. Comput. Sci. 2 (2012), No. 4, ISSN:

UNIT V: Z-TRANSFORMS AND DIFFERENCE EQUATIONS. Dr. V. Valliammal Department of Applied Mathematics Sri Venkateswara College of Engineering

ELECTROPHORESIS IN STRUCTURED COLLOIDS

ECE Microwave Engineering. Fall Prof. David R. Jackson Dept. of ECE. Notes 10. Waveguides Part 7: Transverse Equivalent Network (TEN)

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation.

1 Notes on Little s Law (l = λw)

4.8 Improper Integrals

Name: Period: Date: 2.1 Rules of Exponents

Transcription:

Adv. Sudies Theo. Phys. Vol. 3 9 o. 8 93-98 lhigh Fequecy Geeio i GAs-ype Two-Vlley Seicoducos.. sov. K. Gsiov A. Z. Phov d A.. eiel Bu Se ivesiy 3 Z. Khlilov s. Az 48 Bu ciy- Physicl siue o he Azebij iol Acdey o Scieces 33. Jvid ve. Az 43 Bu ciy Azebij Yüzücü Yil ivesiy Fculy o Scieces d As 658 V-Tuey ideiel@yhoo.co Absc is heoeiclly show h i GAs -ype wo-vlley seicoducos i he cei ievl o eel geic ield usble wve is ppeed. The equecy d icee o his wve e deeied. The pliude d equecy o he oscillios e clculed.. oducio The cue oscillios i eel elecic ield i GAs -ype wo-vlley seicoducos o he is ie e sudied by Gu [6]. O he bsis o his eec he eegy geeos wee cosuced. The eegy diio o supehigh 9 equecy ~ ) occus he cei vlue o he dc elecic ield. The ciicl vlues o elecic ield which he eegy diio begis e oud i y wos icludig []. The Gu eec echis e ivesiged i [ 8]. The uhos o hese wos poi ou h i GAs d P wih icesig o he eel elecic ield he chge cies wih slle eegies e pssed io high lyig eegy bd. Bu he low - equecies ge hese chge cies pss o he ioized ps i he bd gp.

94.. sov. K. Gsiov A. Z. Phov d A.. eiel. lhigh Fequecy Geeio i GAs-ype wo-wlley Seicoducos Whe he ube o he chge cies eceeds y cei giude sple coduciviy is decesed d egive dieeil coduciviy es plce: d d ) d is cue desiy d is iesiy o eel ield. A egive vlues o coduciviy d < ) he elecic ield i cysl becoes o-uio shply - epessed es o elecic ield i.e. "dois" e oed. This cicusce es heoeicl cosideio o poble diicul becuse o olie ie depedece o pliude. ll heoeicl wos he Gu eec is ivesiged e heshold i.e. e siio poi o d. Moeove i he pevious wos geic ield iluece o he cue oscillios is o ivesiged boh i lie d olie ppoiios. he give wo he olie heoy o he Gu eec he pesece o eel sog geic ield > whee is he obiliy c is he c ligh velociy d is he eel geic ield iesiy. oe es io ccou h ie o siio o lowe obiliy ses is egligible sll d he cue cie coceio i i vlley deceses ivesely popoiol o y degee o elecic ield he ube o ioized doos does e los o chge d he cue oscillios occu oly becuse o he eleco siio o he uppe eegy ses. A obiliy i he uppe eegeic se i GAs uch less h o i cel vlley 3 s / s ) [ 3 8]. The cie ube i he lowe vlley will be equl o y p o he ull cie ube ). ) hee ) ) whee he ol cie coceio is he obiliy e d >> >> d is elecic ield vlue coespoded o heshold. A pee is ided o epeie [3]. A cue desiy i he GAs ype copouds cosis o wo ps:

lhigh equecy geeio 95 3) whee d e he cue desiies i he is d secod vlleys. he bsece o he eel ields he cie coceios i he vlleys e << d <<. The o ol cue we hve [ ] [ ] e e e e 4) Coside he ollowig geoey [ ] [ ] e e e e i h e he ui vecos) oig ) ) o eq. ) we ge o cue desiy o lie equio [ ] h h h d e 5) ee c > oe-diesiol cse we hve 6) Wih ig io ccou 4) o c wie he equio 5) i he o: Φ T << 7) Applyig he Bogolyubov Miopolsy ehod i is esy o id he cue oscillio pliude i he is ppoiio [4 5 7]

96.. sov. K. Gsiov A. Z. Phov d A.. eiel β ψ ψ π π si Φ d d d 8) 8 ψ << θ ψ 9) wee θ - phse he we id o 6) e β ) whee is he iiil pliude X β y e he cysl diesios i he d y diecios coespodigly ϕ 3 ) ) 9 ϕ y. is see o 9) h ϕ is icesed wih icese o he eel geic ield d heshold is decesed. Wih begiig o he eegy geeio cysl psses io he usble codiio d o cei giude o he wve is popged i he cysl. The equecies o his wve c be ided o lie ppoiio o equio ) ) ) ) ) y y )

lhigh equecy geeio 97 whee. X ollows o he soluios o he equio ) h whe he geic ield vlues chge i he ievl < < whee ; ) ) h wve equecy deceses wih icesig. The e ) wve icee γ is decesed wih icesig. Thus chgig eel geic ield oe c guide wve popgio. Accodig o he epeiel d [6] o he cie coceio 3 s he isbiliy egie whe diio is occued he geic ield is chged i he ievl < <. ) eeeces. B.K. idley. Poc. Phys.8 954 963.. B.K. idley T.B. Wis. Poc. Phys. Soc. 78 93 963. 3. B..vidov Joul o Theoeicl d peiel Physics) JTP 7 69 937 4...Gsov.K.Gsiov "Vuey eusoychivos v dvudolii polupovodi" 5. Gsov. Thiov B.A Gsıov.K. Cue Oscillios d Geeio o egy i Coducig Meils Wih Fllig Cue-Volge Chceisic. TP-6 3d. eiol Coeece o Techicl Physicl i Powe gieeig. My 9-3 6 A Tuey. p.586-587.

98.. sov. K. Gsiov A. Z. Phov d A.. eiel 6.. B. Gu. o boo Poc.. Co. Phys. Seicoducos Kyoo 966. p.55. 7...Bogolyubov Yu.A.Miopolsy "Asipoichesiye eody v eoii elieyi olebiy" 8..W. gel G.F. Que Ts.. B 4966 eceived: July 8