訂正目次.PDF

Similar documents
プログラム

_0212_68<5A66><4EBA><79D1>_<6821><4E86><FF08><30C8><30F3><30DC><306A><3057><FF09>.pdf

main.dvi

日本内科学会雑誌第98巻第4号

日本内科学会雑誌第97巻第7号

本文/目次(裏白)

修士論文

untitled

untitled

第86回日本感染症学会総会学術集会後抄録(I)

1 9 v.0.1 c (2016/10/07) Minoru Suzuki T µ 1 (7.108) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1)

x 3 a (mod p) ( ). a, b, m Z a b m a b (mod m) a b m 2.2 (Z/mZ). a = {x x a (mod m)} a Z m 0, 1... m 1 Z/mZ = {0, 1... m 1} a + b = a +

吸収分光.PDF

TOP URL 1

Erased_PDF.pdf

Ł\”ƒ-2005

TSP信号を用いた音響系評価の研究

Microsoft Word - 学士論文(表紙).doc

第90回日本感染症学会学術講演会抄録(I)

日本内科学会雑誌第102巻第4号

1. ( ) 1.1 t + t [m]{ü(t + t)} + [c]{ u(t + t)} + [k]{u(t + t)} = {f(t + t)} (1) m ü f c u k u 1.2 Newmark β (1) (2) ( [m] + t ) 2 [c] + β( t)2

飽和分光

O1-1 O1-2 O1-3 O1-4 O1-5 O1-6

放射線専門医認定試験(2009・20回)/HOHS‐05(基礎二次)

プログラム

r d 2r d l d (a) (b) (c) 1: I(x,t) I(x+ x,t) I(0,t) I(l,t) V in V(x,t) V(x+ x,t) V(0,t) l V(l,t) 2: 0 x x+ x 3: V in 3 V in x V (x, t) I(x, t

main.dvi

5 5.1 E 1, E 2 N 1, N 2 E tot N tot E tot = E 1 + E 2, N tot = N 1 + N 2 S 1 (E 1, N 1 ), S 2 (E 2, N 2 ) E 1, E 2 S tot = S 1 + S 2 2 S 1 E 1 = S 2 E


H 0 H = H 0 + V (t), V (t) = gµ B S α qb e e iωt i t Ψ(t) = [H 0 + V (t)]ψ(t) Φ(t) Ψ(t) = e ih0t Φ(t) H 0 e ih0t Φ(t) + ie ih0t t Φ(t) = [


W u = u(x, t) u tt = a 2 u xx, a > 0 (1) D := {(x, t) : 0 x l, t 0} u (0, t) = 0, u (l, t) = 0, t 0 (2)

4 Mindlin -Reissner 4 δ T T T εσdω= δ ubdω+ δ utd Γ Ω Ω Γ T εσ (1.1) ε σ u b t 3 σ ε. u T T T = = = { σx σ y σ z τxy τ yz τzx} { εx εy εz γ xy γ yz γ

N/m f x x L dl U 1 du = T ds pdv + fdl (2.1)

7 π L int = gψ(x)ψ(x)φ(x) + (7.4) [ ] p ψ N = n (7.5) π (π +,π 0,π ) ψ (σ, σ, σ )ψ ( A) σ τ ( L int = gψψφ g N τ ) N π * ) (7.6) π π = (π, π, π ) π ±

c 2009 i

B

No δs δs = r + δr r = δr (3) δs δs = r r = δr + u(r + δr, t) u(r, t) (4) δr = (δx, δy, δz) u i (r + δr, t) u i (r, t) = u i x j δx j (5) δs 2

医系の統計入門第 2 版 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 第 2 版 1 刷発行時のものです.

LLG-R8.Nisus.pdf

ω 0 m(ẍ + γẋ + ω0x) 2 = ee (2.118) e iωt x = e 1 m ω0 2 E(ω). (2.119) ω2 iωγ Z N P(ω) = χ(ω)e = exzn (2.120) ϵ = ϵ 0 (1 + χ) ϵ(ω) ϵ 0 = 1 +

微分積分 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 初版 1 刷発行時のものです.

Onsager SOLUTION OF THE EIGENWERT PROBLEM (O-29) V = e H A e H B λ max Z 2 Onsager (O-77) (O-82) (O-83) Kramers-Wannier 1 1 Ons

9 1. (Ti:Al 2 O 3 ) (DCM) (Cr:Al 2 O 3 ) (Cr:BeAl 2 O 4 ) Ĥ0 ψ n (r) ω n Schrödinger Ĥ 0 ψ n (r) = ω n ψ n (r), (1) ω i ψ (r, t) = [Ĥ0 + Ĥint (

Note.tex 2008/09/19( )

Z: Q: R: C: sin 6 5 ζ a, b

ohpr.dvi

基礎数学I

τ τ

振動工学に基礎

II Karel Švadlenka * [1] 1.1* 5 23 m d2 x dt 2 = cdx kx + mg dt. c, g, k, m 1.2* u = au + bv v = cu + dv v u a, b, c, d R

(1) (2) (3) (4) 1


176 B B.1: ( ) ( ) ( ) (2 2 ) ( ) ( ) ( ) (quantitative nondestructive evaluation:qnde) (1) X X X X CT(computed tomography)

II No.01 [n/2] [1]H n (x) H n (x) = ( 1) r n! r!(n 2r)! (2x)n 2r. r=0 [2]H n (x) n,, H n ( x) = ( 1) n H n (x). [3] H n (x) = ( 1) n dn x2 e dx n e x2

「国債の金利推定モデルに関する研究会」報告書

64 3 g=9.85 m/s 2 g=9.791 m/s 2 36, km ( ) 1 () 2 () m/s : : a) b) kg/m kg/m k

1. (8) (1) (x + y) + (x + y) = 0 () (x + y ) 5xy = 0 (3) (x y + 3y 3 ) (x 3 + xy ) = 0 (4) x tan y x y + x = 0 (5) x = y + x + y (6) = x + y 1 x y 3 (

untitled

pp d 2 * Hz Hz 3 10 db Wind-induced noise, Noise reduction, Microphone array, Beamforming 1

nsg02-13/ky045059301600033210

4. ϵ(ν, T ) = c 4 u(ν, T ) ϵ(ν, T ) T ν π4 Planck dx = 0 e x 1 15 U(T ) x 3 U(T ) = σt 4 Stefan-Boltzmann σ 2π5 k 4 15c 2 h 3 = W m 2 K 4 5.

1. 4cm 16 cm 4cm 20cm 18 cm L λ(x)=ax [kg/m] A x 4cm A 4cm 12 cm h h Y 0 a G 0.38h a b x r(x) x y = 1 h 0.38h G b h X x r(x) 1 S(x) = πr(x) 2 a,b, h,π

6 2 T γ T B (6.4) (6.1) [( d nm + 3 ] 2 nt B )a 3 + nt B da 3 = 0 (6.9) na 3 = T B V 3/2 = T B V γ 1 = const. or T B a 2 = const. (6.10) H 2 = 8π kc2


支持力計算法.PDF

Mathematical Logic I 12 Contents I Zorn


Evolutes and involutes of fronts Masatomo Takahashi Muroran Institute of Technology

untitled

positron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) MeV : thermalization m psec 100

( ) ( )

抄録/抄録1    (1)V

6 2 2 x y x y t P P = P t P = I P P P ( ) ( ) ,, ( ) ( ) cos θ sin θ cos θ sin θ, sin θ cos θ sin θ cos θ y x θ x θ P

( ) ( 40 )+( 60 ) Schrödinger 3. (a) (b) (c) yoshioka/education-09.html pdf 1

201711grade1ouyou.pdf

1 1.1 ( ). z = a + bi, a, b R 0 a, b 0 a 2 + b 2 0 z = a + bi = ( ) a 2 + b 2 a a 2 + b + b 2 a 2 + b i 2 r = a 2 + b 2 θ cos θ = a a 2 + b 2, sin θ =

05Mar2001_tune.dvi

1 (Berry,1975) 2-6 p (S πr 2 )p πr 2 p 2πRγ p p = 2γ R (2.5).1-1 : : : : ( ).2 α, β α, β () X S = X X α X β (.1) 1 2

(1.2) T D = 0 T = D = 30 kn 1.2 (1.4) 2F W = 0 F = W/2 = 300 kn/2 = 150 kn 1.3 (1.9) R = W 1 + W 2 = = 1100 N. (1.9) W 2 b W 1 a = 0

nsg04-28/ky208684356100043077

2 1 1 α = a + bi(a, b R) α (conjugate) α = a bi α (absolute value) α = a 2 + b 2 α (norm) N(α) = a 2 + b 2 = αα = α 2 α (spure) (trace) 1 1. a R aα =

I A A441 : April 21, 2014 Version : Kawahira, Tomoki TA (Kondo, Hirotaka ) Google

V s d d 2 d n d n 2 n R 2 n V s q n 2 n Output q 2 q Decoder 2 R 2 2R 2R 2R 2R A R R R 2R A A n A n 2R R f R (a) 0 (b) 7.4 D-A (a) (b) FET n H ON p H

,., 5., ,. 2.2,., x z. y,.,,,. du dt + α p x = 0 dw dt + α p z + g = 0 α dp dt + pγ dα dt = 0 α V dα dt = 0 (2.2.1), γ = c p /c

Mott散乱によるParity対称性の破れを検証

untitled

H.Haken Synergetics 2nd (1978)

untitled

Part () () Γ Part ,

第3章

: , 2.0, 3.0, 2.0, (%) ( 2.

gr09.dvi

C el = 3 2 Nk B (2.14) c el = 3k B C el = 3 2 Nk B


4‐E ) キュリー温度を利用した消磁:熱消磁

平成 29 年度 ( 第 39 回 ) 数学入門公開講座テキスト ( 京都大学数理解析研究所, 平成 29 ~8 年月 73 月日開催 31 日 Riemann Riemann ( ). π(x) := #{p : p x} x log x (x ) Hadamard de

Microsoft PowerPoint - 山形大高野send ppt [互換モード]

2.1: n = N/V ( ) k F = ( 3π 2 N ) 1/3 = ( 3π 2 n ) 1/3 V (2.5) [ ] a = h2 2m k2 F h2 2ma (1 27 ) (1 8 ) erg, (2.6) /k B 1 11 / K

1 Tokyo Daily Rainfall (mm) Days (mm)

Transcription:

1 1-1.SAW SAW 1 SAW RF IF SAW GHz SAW v 0 1-1.SAW SAWSurface Acoustic Wave SAW m 100ppm 5

SAW 1-1 IDTInterdigital Transducer IDT f SAW V0 IDT SAW f V0/ 1-2.SAW SAW 10MHz GHz 1.5GHz RF 1.5GHz 130MHz IF 1.5GHz 130MHz 455kHz 1-2.SAW SAW 1-3. SAW SAW SAW CampbellJones IDT FIR SAW SAW 6

2 SAW 2 IDT IF IDT 6dB TTSTriple Transit Suppression 20dB SAW SPUDT Single Phase Unidirectional Transducer [1],[ 2] 2-1.FIR SAW SAW MATLAB Signal Processing Toolbox [3] IIRInfinite Impulse Response FIRFinite Impulse Response FIR 2-1. 3 Z- 1 Ts=1/fs fs 2-1. h(nt x(nt n 1 k= 0 ( k x( nt kt y ( nt = h (2-1 10

z ( z ( z H( z Y = (2-2 2-1.FIR SAW IDT SAW V SAW Ts=/2V IDT Ts=/2V FIR FIR SAW (1 SAW SAW IDT IDT (2-1h(k (2 SAW IDT 11

SAW IDT IDT h(n 1-1 1-1 1-1 1-1 1-1 2-2.SAW IDT FIR 2 FIR SAW SAW IDT IDT 1 SAW fc Wb f=fc(wb/2wt Remez Wb WbWt/2 fs fs=fc/2 MATLAB Signal Processing Toolbox 2-3.(a 2 2-3.(a 2 2 f s f s=fs/2 f s/2(=fs/4

3 SAW 2 2.5 SAW 4 5 m-file [4] 0º,140º,25º SAW 2740mm ST 15% 0.36%ST 3 2 20 80 180ppm NSPUDT [5] MATLAB 3-1. IDT IDT 3 COM 22

23 (3-1 [6] 2 AA- 2 3 2 (3-1 2 3-1. = = = C V A A I V A A A V A A A S u u ω ζ ζ ζ θ κ ζ κ θ ( 4 ( 4 ( ( ( ( ( ( ( (3-1 11 κ : α κ κ 2 e = : β ζ ζ e = : S C : A A I V 3-1.COM

COM 4 4 κ κ 11 ζ C S COM Hybrid (La 3Ga5SiO 14COM [7] COM FEMSDA FORTRAN [8] 3-2. COM 4 COM COM : κ 11 SAW SAW κ λ1 11 κ λ 11 SAW V SAW V o κ λ = 11 V V o 1 (3-2 2π λ κ 11 : κ κ λ 1 [ α] κ λ = κ λ exp 2 (3-3 SAW 24

4 SAW 3 3-1 COM 4-1.P [10] SAW 2 4 I 1 I 2 V 1 x x 11 21 x x 22 V 2 4-1.4 4 4-1. Z Y F S 4 4 P SAW 4 4-2.(a IDT SAW 34

4-2.(b 1 2 3 4-2.(b 33 P IDT SPUDT P P P22 P23 IDT SPUDT P 9 COM V I 1 V I 2 A (0 A (L W A -(0 [P] A -(L N x=0 A (0 P 11 = A ( L P I 2P 13 P P 22 2P 23 x=l P A (0 13 P A ( L 23 P V 33 (aidt (bp 4-2.P COM [6] P (4-1 A ( = θ A ( κ A ( ζv u A ( = κa ( θu A ( ζ V I ( = 4 ζ A ( 4 ζa ( ωc V S (4-1 35

5 MATLAB 5-1. MATLAB SAW 5-1. SAW (5-1 A ( = θ A ( κ A ( ζv u A ( = κa ( θu A ( ζ V I ( = 4 ζ A ( 4 ζa ( ωc V S (5-1 1 2 (5-2 A A^ ( = c exp ( θp Γ c exp ( θp ( = Γ c exp ( θ c exp ( θ p p ξ V ξ V (5-2 ( 0 SAW A 1 2 = c = Γc exp( θpl (5-3 (5-3 SAW ( 1 2 Γ Γ exp( 2θpL = ( 1 2 1 Γ Γ exp( 2θ L U Γ = (5-4 r U p SAW 48

Γ l ( 1 2 Γ Γ exp( 2θpL = ( 1 2 1 Γ Γ exp( 2θ L U = (5-5 U p L=Np=N/2 A (1/2 A (-1/2=0 A (1/2 x=-1/2 x=1/2 5-1. MATLAB refl_coef.m 5-1. 9 23 15 COM_LGS_Y50_25 COM compara 5-2. 5-3. 5-2.(a 5-2.(b NSPUDT 5-2.(b 5-3. theta_u theta_p 49

5-2.LGS0,140,25 5-3.LGS0,140,25 50

w,c,w,f,l; % weight_idt1 IDT % H N_Na=length(dist; Na =ones(1,n_na; zeta_n=zeta_t.*dist; Cn=C.*abs(dist; % IDT IDTH siz_f = size(f,1; q11 = ones( siz_f,n_na; q = zeros(siz_f,n_na; q13 = zeros(siz_f,n_na; q21 = zeros(siz_f,n_na; q22 = ones( siz_f,n_na; q23 = zeros(siz_f,n_na; q41 = zeros(siz_f,n_na; q42 = zeros(siz_f,n_na; q43 = zeros(siz_f,n_na; for ii=1:length(na [p11,p,p13,p21,p22,p23,p31,p32,p33,delta]=p_mtrixh(1,k11,k,zeta_n(ii,phse,vsaw,cn(i i,w,f,l; [T11t,Tt,T13t,T21t,T22t,T23t,T41t,T42t,T43t]=p2h(p11,p,p13,p21,p22,p23,p31,p32,p3 3; q11(:,ii = T11t; q(:,ii = Tt; q13(:,ii = T13t; q21(:,ii = T21t; q22(:,ii = T22t; q23(:,ii = T23t; q41(:,ii = T41t; q42(:,ii = T42t; q43(:,ii = T43t; end [T11,T,T13,T21,T22,T23,T31,T32,T33] = Hmatc4(q11,q,q13,q21,q22,q23,q41,q42,q43; 5-7. m - file 5-6 MATLAB m-file MATLAB 5-7 - 1.compara COM [k11,k,arg_k,zeta_t,arg_zeta_t,phse,cs,vsaw]=compara(cryst,h,la mbda; 82

COM COM 5-3. [9] 5-1. cryst (5-3. H m 11 Al lambda m 11 SAW ( 5-2. k11 11 κ λ k 11 ( κ λ arg_k [] 11 k (2 ' 2 Zeta_t 11 ζ = ( ζ λ ( ω C S arg_zeta_t [] 11 zeta_t ( Phse [] 11 2-2=arg_karg_zeta_t Cs (F/m 11 Vsaw [m/s] 11 κ λ = κ λ exp[ 2 ] α 11 ' ζ = ζ exp[ β] 83

5-3.compara cryst 1 Quartz 34Y- ( 2 Quartz ST-25 ( NSPUDT 3 LT -1Y ( 4 LT 36Y- ( 5 LN 8Y- ( 6 LN 64Y- ( 7 LN 8Y- FEUDT( 8 LBO LBO 45-Z ( : m-filecompara.m 5-9.compara function[k11,k,arg_k,zeta_t,arg_zeta_t,phse,cs,vsaw]=compara(cryst,h,lambda; % compara COM % [k11,k,zeta_t,phse,cs,vsaw]=compara(cryst,h,lambda; % ; SAW % 23EM (1994p.101-110 % ( % cryst==1;quartz 34Y- % cryst==2;quartz ST-25 % cryst==3;lt -1Y % cryst==4;lt 36Y- % cryst==5;ln 8Y- % cryst==6;ln 64Y- % cryst==7;ln 8Y- FEUDT % cryst==8;lbo 45-Z % cryst=7 ( % % % cryst: % H : [m] % lambda:saw ( [m] % % k11: k11 % k: k = k exp(2 84

6 MATLAB SAW SAW SAW S S MATLAB 6-1. 6-1.(a 6-1.(b 0 50 50 50 2 LC SAW SPUDT TTE 116

S 2 S ai,bi i (i=1,2 b1 S b 2 = S S 11 S 21 22 a1 a 2 (6-1 S11S22 1,2 SS21 SAW S 50 Z 6 6-1.(a Z L C Z (=1/Y L C 6-1(.b 6-1. 117

SAW 6-3. LC Z1Z2 SAW S S Z F SAW Z1Z4 F F 6-3. F F' F Z S 6-2. SAW IS95.mat 5-6 w_trns.m w_trns.m IDT LGS0,140,25 6-4.(a (b without matching circuits 50 6-4.(c 6-4.(a (b with matching circuits 50 SAW TTE 6-4.(d TTS 51dB 34dB TTE 6-4.(a 119

6-4(a.ex_match ( 6-4(b.ex_match ( 0

6-4(c.ex_match ( TTS TTE 6-4(d.ex_match ( 1