e3Pt3i0.3Pt3i0 · 2020. 11. 2. · z.IE l eRecED.Cefze3Pt3i0.3Pt3i0e3Pt3iO henz3 3P Rele e cosczo...

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z.IE l eRecED.Cefz e3Pt3iO henz3 e3Pt3i0.3Pt3i0 3 P Rele e cosczo feel e costa costa I So for 30 E f Iz t 21h cos 8 o O E n t t E CBO Cso O IT E 6 It Iii ni Shaded region has cosho O 7T and the unshaded region I 6 has cosczo LO f G I grows as 171 70 with cosc30 O Ift l decays as 121 30 with CBC 303 0

Transcript of e3Pt3i0.3Pt3i0 · 2020. 11. 2. · z.IE l eRecED.Cefze3Pt3i0.3Pt3i0e3Pt3iO henz3 3P Rele e cosczo...

  • z.IE l eRecED.Cefz e3Pt3iO henz3e3Pt3i0.3Pt3i03PRele e cosczo feel e costacosta

    ISo for 30E f Iz t 21h cos 8 o

    O E n t t E CBOCso OIT E6 It

    Iii niShaded region has cosho O

    7T and the unshaded regionI6 has cosczo LO

    fG I grows as 171 70 with cosc30 OIft l decays as 121 30 with CBC303 0

  • y I 1 h CBCIfcz oscillates if cos 03 0

    The asymptotic behavior willnot change if we consider Pcz7esince there is an R 0 and C o sit for all El RI.tt ns1PCz3l E C 121 where n degCPFor any fixed 0if cos3070

    limeIPA est 7 figg f EP eeoso lime

    e'Pasospz eeti0 p pp o P

    if cos30 so

    fing IPA e l E Liff c een.eeosoc.ligyee3Poso nIo

    as Iipm Paso np D since ouzo sotoo

    if cos30 0 then le I L and lim le't Past limpest p12120 12136So the grow or decaybehavior is roughly unchanged except in the

    interface where oscillation occurs

    2 2 D or as E w o is an essential

    singularity since as 171 70 Hal is neither boundedor simply go to hence 2 P is neither a removable

    singularity nor a pole hence 2 0 is an essential singularity

    2 fez On E faz has

  • Zeros 2 1 2 3poles Z Z 2 D

    each of them has order 1

    Near 2 L we have Taylor expansion

    let u Z l then

    flatus taffeta u 1 atu 2 u l UU 2 a Hutu'tU 212112W J y city inu 2 1 ut

    2ut U2

    Near 2 P use w Yz and expand around w othose fits i E IFw

    To I w l 3W l12W t DIwc I 2W1th 2 t

    FI Find the winding number around 0 for the followingcurve

    a f f C C unit circle fc z3 EZus r fez HII7 45

  • Solin the winding number is

    a ner or if two dw dzwEfcc

    numberof zeros of food inside Cof poles of f inside c

    3 O 3since the roots are 7 0 2 IFL

    2 her o zero of polding of f in C2 2 0

    Ht For any point 2 ED away from the poles we havea small disk DECZ that is freefrompoles ZiZz 3

    2a

  • polesZeo

    El Zz Zz f23 3

    Dada i

    Then for any Z E DIZ such that12 Znl E A Enlant

    Then Ifczyl E En TEY E T En tant kAgAnd If't't'll E EE Tain e IT A CD

    Hence f is holomorphic in a neighborhood Dscz of Lfor any E ID I Zi Zz iZn

    gleio joiI y Let Flo Z be a functionon 0,212 X D then by Thur5.2 in Ch2 we know

    fat f dei z f et.fi ei0idoOoJo HO Z do

    is a holomorphic function on D

    Similarly view FcQZ as a function on0,21T x IC DT is hot'c in Z continuous in

    both variables hence fit is also holk on 14213

    Let C Eff 1gal then for any121 1 we haveg

  • f glfczsltfswyp.IT nteuIIuI e o as so

    2 and CD The story goes as follows

    we first consider 8th Z for ZEC ItuNEIL

    then forn 30 fez

    HIEIO 121 I

    mo fcHeo

    zn 12171

    In general for ZOE G we have the difference ofthe two boundary values from inside and outside being ga7 fcr.to Liff fcr.to gtfo

    This is clear if gas is a finite linear combinationof Z got Az En't Ar Zn't AN 2nThis is also true more generally for any gotsmooth function on C or even just continuous function