untitled

Size: px
Start display at page:

Download "untitled"

Transcription

1 /,

2

3

4

5

6

7 S=1/2 S=0 S=1/2

8

9

10 -

11 S// m H m H = S G

12 e + +

13

14

15

16

17

18

19

20

21

22

23

24

25

26

27

28

29

30

31 G Z (t) 1 0 t

32 G Z (t) 1 0 t

33 G Z (t) 1 0 t

34

35

36

37

38 SR

39 G Z (t) = 1/3 + (2/3)(1-2 t 2 )exp(- 2 t 2 /2) G Z (t) 1-1/3 1/3 0 3/ 3/ t

40 G Z (t) = 1/3 + (2/3)(1-2 t 2 )exp(- 2 t 2 /2) G Z (t) - 1 G Z (t) 1 1/3 1/3 0 3/ 3/ t 1/3 1/3 0 t 1/3 x -1 1/3 y 1/3 z z 1/3 G Z (t) = 1 2/3 G Z (t) = 0 0 G Z (t) 1 t

41 SR G Z (t) 1 1/3 z 0 t

42 SR G Z (t) G Z (t) G Z (t) t 0 t 0 t -1

43 SR G Z (t) G Z (t) 1 1 1/3 1/3 0 t 0 t

44 SR G Z (t) 1 G Z (t) 1 0 t 0 t

45 SR G Z (t) G Z (t) 1 1 1/3 1/3 0 t 0 t

46 25 La 2-x Sr x Cu 1-y Fe y O 4 x = y = 0.01 Raw Asymmetry (%) Time (µsec) T = 20.5 K Normalized Asymmetry La 1.85 Sr 0.15 Cu 0.90 Ni 0.10 O 4 3 K 2 K 0.3 K 20 K 5 K Time (µsec)

47 N. Nishida et al., Jpn. J. Appl. Phys. 26 (1987) L1856

48 SR LF- SR) G Z (t) G Z (t) t 0 t

49

50 SR TF- SR) T > T c G Z (t) 1 0 t -1

51 TF- SR T < T c H c1 < H < H c2 H c1 < H < H c2 vortex vortex (m*/n s ) 1/2

52 TF- SR -2 n s /m*

53

54 SR TF- SR) = ( G Z (t) t

55

56

57 < 10-9 sec sec > 10-5 sec

58

59

60

61

62

63 Bohr model E n 2 4 Z me = 2 2 8n ε h 2 4πεon h rn = 2 Zme mµ E 207 m E e o 2 µ e 2 r r e µ

64

65

66

67 RAL PSI TRIUMF KEK-MSL J-PARC Pulse beam : long relaxation of muon spins DC beam : fast muon-spin precession and fast relaxation of muon spins

68 The END

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

positron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) MeV : thermalization m psec 100 positron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) 0.5 1.5MeV : thermalization 10 100 m psec 100psec nsec E total = 2mc 2 + E e + + E e Ee+ Ee-c mc

More information

KamLAND (µ) ν e RSFP + ν e RSFP(Resonant Spin Flavor Precession) ν e RSFP 1. ν e ν µ ν e RSFP.ν e νµ ν e νe µ KamLAND νe KamLAND (ʼ4). kton-day 8.3 < E ν < 14.8 MeV candidates Φ(νe) < 37 cm - s -1 P(νe

More information

コロイド化学と界面化学

コロイド化学と界面化学 x 25 1 kg 1 kg = 1 l mmol dm -3 ----- 1000 mg CO 2 -------------------------------------250 mg Li + --------------------------------1 mg Sr 2+ -------------------- 10

More information

C 3 C-1 Ru 2 x Fe x CrSi A A, A, A, A, A Ru 2 x Fe x CrSi 1) 0.3 x 1.8 2) Ru 2 x Fe x CrSi/Pb BTK P Z 3 x = 1.7 Pb BTK P = ) S.Mizutani, S.Ishid

C 3 C-1 Ru 2 x Fe x CrSi A A, A, A, A, A Ru 2 x Fe x CrSi 1) 0.3 x 1.8 2) Ru 2 x Fe x CrSi/Pb BTK P Z 3 x = 1.7 Pb BTK P = ) S.Mizutani, S.Ishid C 3 C-1 Ru 2 x Fe x CrSi A A, A, A, A, A Ru 2 x Fe x CrSi 1).3 x 1.8 2) Ru 2 x Fe x CrSi/Pb BTK P Z 3 x = 1.7 Pb BTK P =.52 1) S.Mizutani, S.Ishida, S.Fujii and S.Asano, Mater. Tran. 47(26)25. 2) M.Hiroi,

More information

, ,

, , 41 42 73 121 121 10 122 11 122 12 131 13 131 15 10 133 16 11 133 17 12 136 18 13 141 19 14 141 20 15 146 21 16 149 22 17 149 23 174 18 24 73 19 241,301 25 20 242,301 (1) 26 21 331 27 22 241,341 28 23 242,341

More information

1. 2001 10 2 480 2003 8 1.6 5 2. 90 3. 4. 5. 5 60 6. 1 2 2 2 4 5 5 6 6 6 7 10 10 10 12 12 12 14 14 15 15 60 15 17 17 18 2001 10 2 480 2003 8 1.6 5 1 1.8 3.6 1 6.8 1.5 3 3 5 6065 70 5 1.22004 1 1 2002 4

More information

23 1 Section ( ) ( ) ( 46 ) , 238( 235,238 U) 232( 232 Th) 40( 40 K, % ) (Rn) (Ra). 7( 7 Be) 14( 14 C) 22( 22 Na) (1 ) (2 ) 1 µ 2 4

23 1 Section ( ) ( ) ( 46 ) , 238( 235,238 U) 232( 232 Th) 40( 40 K, % ) (Rn) (Ra). 7( 7 Be) 14( 14 C) 22( 22 Na) (1 ) (2 ) 1 µ 2 4 23 1 Section 1.1 1 ( ) ( ) ( 46 ) 2 3 235, 238( 235,238 U) 232( 232 Th) 40( 40 K, 0.0118% ) (Rn) (Ra). 7( 7 Be) 14( 14 C) 22( 22 Na) (1 ) (2 ) 1 µ 2 4 2 ( )2 4( 4 He) 12 3 16 12 56( 56 Fe) 4 56( 56 Ni)

More information

untitled

untitled NPO 2006( ) 11 14 ( ) (2006/12/3) 1 50% % - - (CO+H2) ( ) 6 44 1) --- 2) ( CO H2 ) 2 3 3 90 3 3 2 3 2004 ( ) 1 1 4 1 20% 5 ( ) ( ) 2 6 MAWERA ) MAWERA ( ) ( ) 7 6MW -- 175kW 8 ( ) 900 10 2 2 2 9 -- - 10

More information

d > 2 α B(y) y (5.1) s 2 = c z = x d 1+α dx ln u 1 ] 2u ψ(u) c z y 1 d 2 + α c z y t y y t- s 2 2 s 2 > d > 2 T c y T c y = T t c = T c /T 1 (3.

d > 2 α B(y) y (5.1) s 2 = c z = x d 1+α dx ln u 1 ] 2u ψ(u) c z y 1 d 2 + α c z y t y y t- s 2 2 s 2 > d > 2 T c y T c y = T t c = T c /T 1 (3. 5 S 2 tot = S 2 T (y, t) + S 2 (y) = const. Z 2 (4.22) σ 2 /4 y = y z y t = T/T 1 2 (3.9) (3.15) s 2 = A(y, t) B(y) (5.1) A(y, t) = x d 1+α dx ln u 1 ] 2u ψ(u), u = x(y + x 2 )/t s 2 T A 3T d S 2 tot S

More information

1-x x µ (+) +z µ ( ) Co 2p 3d µ = µ (+) µ ( ) W. Grange et al., PRB 58, 6298 (1998). 1.0 0.5 0.0 2 1 XMCD 0-1 -2-3x10-3 7.1 7.2 7.7 7.8 8.3 8.4 up E down ρ + (E) ρ (E) H, M µ f + f E F f + f f + f X L

More information

JAJP

JAJP Agilent 7500ce ORS ICP-MS Glenn Woods Agilent Technologies Ltd. 5500 Lakeside, Cheadle Royal Business Park Stockport UK Agilent 7500ce ICP-MS 5 7500ce (ORS) 1 ORS 7500ce ORS ICP-MS ( ) 7500 ICP-MS (27.12

More information

437“ƒ

437“ƒ et al., et al., et al., et al., et al., et al., 2 et al., et al., et al., Lancet Pharmacol Res. et al. Jpn J Cancer Res. et al. Jpn J Cancer Res. et al. Tohoku J Exp Med. et al. Jpn Circ J. et al. Cancer

More information

C: PC H19 A5 2.BUN Ohm s law

C: PC H19 A5 2.BUN Ohm s law C: PC H19 A5 2.BUN 19 8 6 3 19 3.1........................... 19 3.2 Ohm s law.................... 21 3.3.......................... 24 4 26 4.1................................. 26 4.2.................................

More information

C 3 C-1 Cu 2 (OH) 3 Cl A, B A, A, A, B, B Cu 2 (OH) 3 Cl clinoatacamite S=1/2 Heisenberg Cu 2+ T N 1 =18K T N 2 =6.5K SR T N 2 T N 1 T N 1 0T 1T 2T 3T

C 3 C-1 Cu 2 (OH) 3 Cl A, B A, A, A, B, B Cu 2 (OH) 3 Cl clinoatacamite S=1/2 Heisenberg Cu 2+ T N 1 =18K T N 2 =6.5K SR T N 2 T N 1 T N 1 0T 1T 2T 3T C 3 C-1 Cu 2 (OH) 3 Cl A, B A, A, A, B, B Cu 2 (OH) 3 Cl clinoatacamite S=1/2 Heisenberg Cu 2+ T N 1 =18K T N 2 =6.5K SR T N 2 T N 1 T N 1 0T 1T 2T 3T 4T 5T 6T C (J/K mol) 20 18 16 14 12 10 8 6 0 0 5 10

More information

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)

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) 1 9 v..1 c (216/1/7) Minoru Suzuki 1 1 9.1 9.1.1 T µ 1 (7.18) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1) E E µ = E f(e ) E µ (9.1) µ (9.2) µ 1 e β(e µ) 1 f(e )

More information

C-2 NiS A, NSRRC B, SL C, D, E, F A, B, Yen-Fa Liao B, Ku-Ding Tsuei B, C, C, D, D, E, F, A NiS 260 K V 2 O 3 MIT [1] MIT MIT NiS MIT NiS Ni 3 S 2 Ni

C-2 NiS A, NSRRC B, SL C, D, E, F A, B, Yen-Fa Liao B, Ku-Ding Tsuei B, C, C, D, D, E, F, A NiS 260 K V 2 O 3 MIT [1] MIT MIT NiS MIT NiS Ni 3 S 2 Ni M (emu/g) C 2, 8, 9, 10 C-1 Fe 3 O 4 A, SL B, NSRRC C, D, E, F A, B, B, C, Yen-Fa Liao C, Ku-Ding Tsuei C, D, D, E, F, A Fe 3 O 4 120K MIT V 2 O 3 MIT Cu-doped Fe3O4 NCs MIT [1] Fe 3 O 4 MIT Cu V 2 O 3

More information

QMI_10.dvi

QMI_10.dvi ... black body radiation black body black body radiation Gustav Kirchhoff 859 895 W. Wien O.R. Lummer cavity radiation ν ν +dν f T (ν) f T (ν)dν = 8πν2 c 3 kt dν (Rayleigh Jeans) (.) f T (ν) spectral energy

More information

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

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 1 6 6.1 (??) (P = ρ rad /3) ρ rad T 4 d(ρv ) + PdV = 0 (6.1) dρ rad ρ rad + 4 da a = 0 (6.2) dt T + da a = 0 T 1 a (6.3) ( ) n ρ m = n (m + 12 ) m v2 = n (m + 32 ) T, P = nt (6.4) (6.1) d [(nm + 32 ] )a

More information

1 d 6 L S p p p p-d d 10Dq 1 ev p-d d 70 % 1: NiO [3] a b CI c [5] NiO Ni [ 1(a)] Ni 2+ d 8 d 7 d 8 + hν d 7 + e d 7 1(b) d 7 p Ni 2+ t 3 2g t3 2g e2

1 d 6 L S p p p p-d d 10Dq 1 ev p-d d 70 % 1: NiO [3] a b CI c [5] NiO Ni [ 1(a)] Ni 2+ d 8 d 7 d 8 + hν d 7 + e d 7 1(b) d 7 p Ni 2+ t 3 2g t3 2g e2 3 3.1 3.1.1 - d s p d 3d d d d d d d 10 23 d d 1954 [1] d d 1970 I-II-VI 2 II-VI II 1:1 I III CuAlS 2 Al 3+ d 5 Fe 3+ d 5 S 3p d 6 L L [2] configuration interaction: CI d 5 1 1 d 6 L S p p p p-d d 10Dq

More information

ohpr.dvi

ohpr.dvi 2003/12/04 TASK PAF A. Fukuyama et al., Comp. Phys. Rep. 4(1986) 137 A. Fukuyama et al., Nucl. Fusion 26(1986) 151 TASK/WM MHD ψ θ ϕ ψ θ e 1 = ψ, e 2 = θ, e 3 = ϕ ϕ E = E 1 e 1 + E 2 e 2 + E 3 e 3 J :

More information

SPring-8_seminar_

SPring-8_seminar_ X 21 SPring-8 XAFS 2016 (= ) X PC cluster Synchrotron TEM-EELS XAFS / EELS HΨ k = E k Ψ k XANES/ELNES DFT ( + ) () WIEN2k, Elk, OLCAO () CASTEP, QUANTUM ESPRESSO FEFF, GNXAS, etc. Bethe-Salpeter (BSE)

More information

IS(A3) 核データ表 ( 内部転換 オージェ電子 ) No.e1 By IsoShieldJP 番号 核種核種半減期エネルギー放出割合核種番号通番数値単位 (kev) (%) 核崩壊型 娘核種 MG H β-/ce K A

IS(A3) 核データ表 ( 内部転換 オージェ電子 ) No.e1 By IsoShieldJP 番号 核種核種半減期エネルギー放出割合核種番号通番数値単位 (kev) (%) 核崩壊型 娘核種 MG H β-/ce K A IS(A3)- 284 - No.e1 核種核種半減期エネルギー放出割合核種通番数値単位 (kev) (%) 1 1 1 MG-28 20.915 H 29.08 27.0000 β-/ce K Al-28 2 1 2 MG-28 20.915 H 30.64 2.6000 β-/ce L Al-28 3 2 1 SC-44M 58.6 H 270.84 0.0828 EC/CE CA-44 4 2

More information

<4D F736F F D B B83578B6594BB2D834A836F815B82D082C88C602E646F63>

<4D F736F F D B B83578B6594BB2D834A836F815B82D082C88C602E646F63> スピントロニクスの基礎 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. http://www.morikita.co.jp/books/mid/077461 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. i 1 2 ii 3 5 4 AMR (anisotropic magnetoresistance effect) GMR (giant magnetoresistance

More information

untitled

untitled 4. NEDO NEDO 20 23-26 Grain Boundary Grain Interior.2.1.1.1-1 mm μm nm Mg Photodiode Counts 450 500 550 600 Energy Loss (ev).2 (AZ91+ 300-1 300 0.1%.1.1-1 -2 -3 (1) (2) (3) 18 19 AZ61 AZ80 ZK60 ACM522.2.1-1.2.1-1.2.1-2.2.1-2

More information

a L = Ψ éiγ c pa qaa mc ù êë ( - )- úû Ψ 1 Ψ 4 γ a a 0, 1,, 3 {γ a, γ b } η ab æi O ö æo ö β, σ = ço I α = è - ø çèσ O ø γ 0 x iβ γ i x iβα i

a L = Ψ éiγ c pa qaa mc ù êë ( - )- úû Ψ 1 Ψ 4 γ a a 0, 1,, 3 {γ a, γ b } η ab æi O ö æo ö β, σ = ço I α = è - ø çèσ O ø γ 0 x iβ γ i x iβα i 解説 4 matsuo.mamoru jaea.go.jp 4 eizi imr.tohoku.ac.jp 4 maekawa.sadamichi jaea.go.jp i ii iii i Gd Tb Dy g khz Pt ii iii Keywords vierbein 3 dreibein 4 vielbein torsion JST-ERATO 1 017 1. 1..1 a L = Ψ

More information

Microsoft Word - 00”ŒŁ\”ƒf.doc

Microsoft Word - 00”ŒŁ\”ƒf.doc 1-1 1 1-2 5S 3 1-3 5 2-1 1 2-2 3 2-3 5 2-4 7 3-1 1 3-2 3 3-3 5 3-4 7 4-1 1977 1 4-2 1987 7 4-3 17 4-4 26 1-1 1 1-2 5S 3 1-3 5 1-1 (1) (2) (3) 1. -1-1 1:15 1:10 2.. owf / 1.0 40 1.0 3.0 60 3.0 80 kg 0.25

More information

untitled

untitled 1 / 37 5-4 6.1 1 2 / 37 1 (1) FePt AuAg (2) CdSe ZnSXY 2 O 3 X X : ZnO (3) SiO 2 (4) (5) 2 1 3 / 37 1 (1) FePt AuAg (2) CdSe ZnSXY 2 O 3 X X : ZnO (3) SiO 2 (4) (5) 3 4 / 37 1Tbits/cm 2 HD FePt FePt 110nm

More information

36 th IChO : - 3 ( ) , G O O D L U C K final 1

36 th IChO : - 3 ( ) , G O O D L U C K final 1 36 th ICh - - 5 - - : - 3 ( ) - 169 - -, - - - - - - - G D L U C K final 1 1 1.01 2 e 4.00 3 Li 6.94 4 Be 9.01 5 B 10.81 6 C 12.01 7 N 14.01 8 16.00 9 F 19.00 10 Ne 20.18 11 Na 22.99 12 Mg 24.31 Periodic

More information

Microsoft PowerPoint - summer_school_for_web_ver2.pptx

Microsoft PowerPoint - summer_school_for_web_ver2.pptx スピン流で観る物理現象 大阪大学大学院理学研究科物理学専攻 新見康洋 スピントロニクスとは スピン エレクトロニクス メモリ産業と深くつなが ている メモリ産業と深くつながっている スピン ハードディスクドライブの読み取りヘッド N 電荷 -e スピンの流れ ピ の流れ スピン流 S 巨大磁気抵抗効果 ((GMR)) from http://en.wikipedia.org/wiki/disk_readand-write_head

More information

CH 2 CH CH 2 CH CH 2 CH CH 2 CH 2 COONa CH 2 N CH 2 COONa O Co 2+ O CO CH 2 CH N 2 CH 2 CO 9 Change in Ionic Form of IDA resin with h ph CH 2 NH + COO

CH 2 CH CH 2 CH CH 2 CH CH 2 CH 2 COONa CH 2 N CH 2 COONa O Co 2+ O CO CH 2 CH N 2 CH 2 CO 9 Change in Ionic Form of IDA resin with h ph CH 2 NH + COO CH 2 CH CH 2 CH CH 2 CH CH 2 CH 2 COONa CH 2 N CH 2 COONa O Co 2+ O CO CH 2 CH N 2 CH 2 CO 9 Change in Ionic Form of IDA resin with h ph CH 2 NH + COOH COOH COOH COO - CH 2 NH + + CH 2 NH COO - COO - COO

More information

X線分析の進歩36 別刷

X線分析の進歩36 別刷 X X X-Ray Fluorescence Analysis on Environmental Standard Reference Materials with a Dry Battery X-Ray Generator Hideshi ISHII, Hiroya MIYAUCHI, Tadashi HIOKI and Jun KAWAI Copyright The Discussion Group

More information

2009 Aida et al. Caries Res 2006;40 2000 100 % 78.7 88.0 96.6 98.8 98.8 98.8 100.0 100.0 100 75 69.4 50 75.3 74.8 73.3 73.1 73.0 72.4 71.8 71.7 51.7 40.2 69.4 68.8 73.6 25 22.3 32.8 21.9 22.9 22.1

More information

untitled

untitled , Kaoru ARIYAMA 10 17N, Na, Mg,Al,Si,P,S,Cl,K,Ca,Fe,Cu,Zn,Se,Br,Rb Sr 14r2 0.9617 Tricholoma matsutake,,, JAS ICP-OESICP-MS 2ICP-OES ICP-MS,, Tricholoma matsutake -24- 1 7 2006 70 13 8 5 2,, 2007,, 10

More information

Mott散乱によるParity対称性の破れを検証

Mott散乱によるParity対称性の破れを検証 Mott Parity P2 Mott target Mott Parity Parity Γ = 1 0 0 0 0 1 0 0 0 0 1 0 0 0 0 1 t P P ),,, ( 3 2 1 0 1 γ γ γ γ γ γ ν ν µ µ = = Γ 1 : : : Γ P P P P x x P ν ν µ µ vector axial vector ν ν µ µ γ γ Γ ν γ

More information

Outline I. Introduction: II. Pr 2 Ir 2 O 7 Like-charge attraction III.

Outline I. Introduction: II. Pr 2 Ir 2 O 7 Like-charge attraction III. Masafumi Udagawa Dept. of Physics, Gakushuin University Mar. 8, 16 @ in Gakushuin University Reference M. U., L. D. C. Jaubert, C. Castelnovo and R. Moessner, arxiv:1603.02872 Outline I. Introduction:

More information

PowerPoint プレゼンテーション

PowerPoint プレゼンテーション 2004 3 3 2 3 4 5 6 7 8 9 10 T. Ito, A. Yamamoto, et al., J. Chem. Soc., Chem. Commun., 136 (1974) J. Chem. Soc., Dalton Trans., 1783 (1974) J. Chem. Soc., Dalton Trans., 1398 (1975) 11 T.Ito, A. Yamamoto,

More information

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

C el = 3 2 Nk B (2.14) c el = 3k B C el = 3 2 Nk B I ino@hiroshima-u.ac.jp 217 11 14 4 4.1 2 2.4 C el = 3 2 Nk B (2.14) c el = 3k B 2 3 3.15 C el = 3 2 Nk B 3.15 39 2 1925 (Wolfgang Pauli) (Pauli exclusion principle) T E = p2 2m p T N 4 Pauli Sommerfeld

More information

1 1 H Li Be Na M g B A l C S i N P O S F He N Cl A e K Ca S c T i V C Mn Fe Co Ni Cu Zn Ga Ge As Se B K Rb S Y Z Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb T e

1 1 H Li Be Na M g B A l C S i N P O S F He N Cl A e K Ca S c T i V C Mn Fe Co Ni Cu Zn Ga Ge As Se B K Rb S Y Z Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb T e No. 1 1 1 H Li Be Na M g B A l C S i N P O S F He N Cl A e K Ca S c T i V C Mn Fe Co Ni Cu Zn Ga Ge As Se B K Rb S Y Z Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb T e I X e Cs Ba F Ra Hf Ta W Re Os I Rf Db Sg Bh

More information

D-2 Co(S,Se) 2 A A, A, A Co(S 1 x Se x ) 2 S Se x.5 [1] CoS 2 Co(S 1 x Se x ) 2 SQUID FC-7 FC-77 1:1 CoS 2 S Se [1]H. Wada et al, Phys. Rev. B 74 (26)

D-2 Co(S,Se) 2 A A, A, A Co(S 1 x Se x ) 2 S Se x.5 [1] CoS 2 Co(S 1 x Se x ) 2 SQUID FC-7 FC-77 1:1 CoS 2 S Se [1]H. Wada et al, Phys. Rev. B 74 (26) D 3 D-1 Fe/Cr GMR A, B, C A, A, A, A, B, B, C, C, C Fe/Cr (Giant magnetoresistance:gmr) Fe Cr GMR, GMR [Fe(2 )/Cr(8 )] 2 3MeV C 4+ 1 15 /cm 2 GMR GPa P 2. GPa, -3 T B 3 T, T=, 77.4K Fig.1 [Fe(2 )/Cr(8

More information

W 1983 W ± Z cm 10 cm 50 MeV TAC - ADC ADC [ (µs)] = [] (2.08 ± 0.36) 10 6 s 3 χ µ + µ 8 = (1.20 ± 0.1) 10 5 (Ge

W 1983 W ± Z cm 10 cm 50 MeV TAC - ADC ADC [ (µs)] = [] (2.08 ± 0.36) 10 6 s 3 χ µ + µ 8 = (1.20 ± 0.1) 10 5 (Ge 22 2 24 W 1983 W ± Z 0 3 10 cm 10 cm 50 MeV TAC - ADC 65000 18 ADC [ (µs)] = 0.0207[] 0.0151 (2.08 ± 0.36) 10 6 s 3 χ 2 2 1 20 µ + µ 8 = (1.20 ± 0.1) 10 5 (GeV) 2 G µ ( hc) 3 1 1 7 1.1.............................

More information

[Ver. 0.2] 1 2 3 4 5 6 7 1 1.1 1.2 1.3 1.4 1.5 1 1.1 1 1.2 1. (elasticity) 2. (plasticity) 3. (strength) 4. 5. (toughness) 6. 1 1.2 1. (elasticity) } 1 1.2 2. (plasticity), 1 1.2 3. (strength) a < b F

More information

TOP URL 1

TOP URL   1 TOP URL http://amonphys.web.fc.com/ 1 19 3 19.1................... 3 19.............................. 4 19.3............................... 6 19.4.............................. 8 19.5.............................

More information

( 2001MB062) Zachary Fisk Thomas Maurice Rice Hans Rudolf Ott MgB Y 2 C 3 18K 11K Ca EuB 6 CaB 6 CaB 2 C 2 MgB 2 Y 2 C 3 1 NED

( 2001MB062) Zachary Fisk Thomas Maurice Rice Hans Rudolf Ott MgB Y 2 C 3 18K 11K Ca EuB 6 CaB 6 CaB 2 C 2 MgB 2 Y 2 C 3 1 NED ( 2001MB062) Zachary Fisk Thomas Maurice Rice Hans Rudolf Ott 2001 4 2004 3 1 MgB 2 3 2 3 Y 2 C 3 18K 11K Ca EuB 6 CaB 6 CaB 2 C 2 MgB 2 Y 2 C 3 1 NEDO 2 MgB 2 2001 1 MgB 2 NEDO MgB 2 σ π MgB 2 [1] MgB

More information

03J_sources.key

03J_sources.key Radiation Detection & Measurement (1) (2) (3) (4)1 MeV ( ) 10 9 m 10 7 m 10 10 m < 10 18 m X 10 15 m 10 15 m ......... (isotope)...... (isotone)......... (isobar) 1 1 1 0 1 2 1 2 3 99.985% 0.015% ~0% E

More information

産衛誌57-4たより.indb

産衛誌57-4たより.indb A89 26 7 1 9 4 33 1 87 A90 24 A91 23 ACOH2014 A92 4 1 2 3 4 5 6 7 A93 A94 A95 A96 A97 A98 A99 A100 A101 27 8 1 9 A102 4 33 A103 A104 26 3 140 27 1 A105 27 A106 A107 A108 A109 A110 A111 A112 A113 et al

More information

4‐E ) キュリー温度を利用した消磁:熱消磁

4‐E ) キュリー温度を利用した消磁:熱消磁 ( ) () x C x = T T c T T c 4D ) ) Fe Ni Fe Fe Ni (Fe Fe Fe Fe Fe 462 Fe76 Ni36 4E ) ) (Fe) 463 4F ) ) ( ) Fe HeNe 17 Fe Fe Fe HeNe 464 Ni Ni Ni HeNe 465 466 (2) Al PtO 2 (liq) 467 4G ) Al 468 Al ( 468

More information

rcnp01may-2

rcnp01may-2 E22 RCP Ring-Cyclotron 97 953 K beam K-atom HF X K, +,K + e,e K + -spectroscopy OK U U I= First-order -exchange - coupling I= U LS U LS Meson-exchange model /5/ I= Symmetric LS Anti-symmetric LS ( σ Λ

More information

取扱説明書[L704i]

取扱説明書[L704i] 231 N b N b A N b A N N P 232 N N b b K Q P M I b C c C 233 DC I d I M M M C I I C C I C C 234 M I C M J C J C D J C C H D C DC I b I 235 M b 1 3 7 9 F E 5 b J b c b c d e c b d e M H M I 236 J M J M I

More information

natMg+86Krの反応による生成核からのβ線の測定とGEANTによるシミュレーションとの比較

natMg+86Krの反応による生成核からのβ線の測定とGEANTによるシミュレーションとの比較 nat Mg+ 86 Kr の反応による生成核からの β 線の測定と GEANT によるシミュレーションとの比較 田尻邦彦倉健一朗 下田研究室 目次 実験の目的 nat Mg+ 86 Kr 生成核からの β 線の測定 @RCNP 実験方法 実験結果 GEANT によるシミュレーション 解析 結果 まとめ 今後の課題 実験の目的 偏極した中性子過剰 Na アイソトープの β-γ-γ 同時測定実験を TRIUMF

More information

Al アルミニウム Cu 銅 Fe 鉄 Ni ニ

Al アルミニウム Cu 銅 Fe 鉄 Ni ニ Al アルミニウム 30000 30000 30000 26000 26000 26000 28000 Cu 銅 140000 140000 140000 110000 110000 110000 130000 Fe 鉄 86000 87000 88000 140000 140000 140000 110000 Ni ニッケル 13000 13000 14000 23000 23000 23000

More information

PDF

PDF 1 1 1 1-1 1 1-9 1-3 1-1 13-17 -3 6-4 6 3 3-1 35 3-37 3-3 38 4 4-1 39 4- Fe C TEM 41 4-3 C TEM 44 4-4 Fe TEM 46 4-5 5 4-6 5 5 51 6 5 1 1-1 1991 1,1 multiwall nanotube 1993 singlewall nanotube ( 1,) sp 7.4eV

More information

2008/02/18 08:40-10:10, 12:50-14:20 14:30-16:00, 16:10-17:40,

2008/02/18 08:40-10:10, 12:50-14:20 14:30-16:00, 16:10-17:40, 008/0/18 08:40-10:10, 1:50-14:0 14:30-16:00, 16:10-17:40, 1pt A 1911 Leiden Heike Kammelingh-Onnes H.Kammelingh Onnes 1907 He 1 4. K H H c T c T H c Hg:40 mt, Pb:80 mt, Sn:30 mt 100 mt I c H c H c H

More information

untitled

untitled SPring-8 RFgun JASRI/SPring-8 6..7 Contents.. 3.. 5. 6. 7. 8. . 3 cavity γ E A = er 3 πε γ vb r B = v E c r c A B A ( ) F = e E + v B A A A A B dp e( v B+ E) = = m d dt dt ( γ v) dv e ( ) dt v B E v E

More information

...1 (1)... 1 (2) ) )... 1 (3)... 1 (4) ) )... 2 (5)... 3 (6)... 3 (7) ) )... 4 (8)... 4 (9)... 4 (10) (1

...1 (1)... 1 (2) ) )... 1 (3)... 1 (4) ) )... 2 (5)... 3 (6)... 3 (7) ) )... 4 (8)... 4 (9)... 4 (10) (1 ...1 (1)... 1 (2)... 1 1)... 1 2)... 1 (3)... 1 (4)... 1 1)... 1 2)... 2 (5)... 3 (6)... 3 (7)... 4 1)... 4 2)... 4 (8)... 4 (9)... 4 (10)... 4...5 (1)... 5 1)... 5 2)... 5 (2)... 5 1)... 5 2)... 5 3)...

More information

²ÄÀÑʬΥ»¶ÈóÀþ·¿¥·¥å¥ì¡¼¥Ç¥£¥ó¥¬¡¼ÊýÄø¼°¤ÎÁ²¶á²òÀÏ Asymptotic analysis for the integrable discrete nonlinear Schrödinger equation

²ÄÀÑʬΥ»¶ÈóÀþ·¿¥·¥å¥ì¡¼¥Ç¥£¥ó¥¬¡¼ÊýÄø¼°¤ÎÁ²¶á²òÀÏ  Asymptotic analysis for the integrable discrete nonlinear Schrödinger equation Asymptotic analysis for the integrable discrete nonlinear Schrödinger equation ( ) ( ) 2016 12 17 1. Schrödinger focusing NLS iu t + u xx +2 u 2 u = 0 u(x, t) =2ηe 2iξx 4i(ξ2 η 2 )t+i(ψ 0 +π/2) sech(2ηx

More information

Λ (Λ ) Λ (Ge) Hyperball γ ΛN J-PARC Λ dead time J-PARC flash ADC 1 dead time ( ) 1 µsec 3

Λ (Λ ) Λ (Ge) Hyperball γ ΛN J-PARC Λ dead time J-PARC flash ADC 1 dead time ( ) 1 µsec 3 19 Λ (Λ ) Λ (Ge) Hyperball γ ΛN J-PARC Λ dead time J-PARC flash ADC 1 dead time ( ) 1 µsec 3 1 1 1.1 γ ΛN................. 1 1.2 KEK J-PARC................................ 2 1.2.1 J-PARC....................................

More information

τ p ω πτ p ω π τ p (t) = 2 2 t 2 exp(i t)exp 8 2 S(,t) = s( ) (t )d d 2 E x dz 2 = 2 E x z E x = E 0 e z, = + j = 1 2 0 tan = 0, v = c r 10 11 Horn Circulator Net Work Analyzer t H = E t E = H E t B =

More information

From Evans Application Notes

From Evans Application Notes 3 From Evans Application Notes http://www.eaglabs.com From Evans Application Notes http://www.eaglabs.com XPS AES ISS SSIMS ATR-IR 1-10keV µ 1 V() r = kx 2 = 2π µν x mm 1 2 µ= m + m 1 2 1 k ν = OSC 2

More information

2016select追加小冊子_0704出稿0706修正.indd

2016select追加小冊子_0704出稿0706修正.indd -JPN3 -JPN3 -G1 -G1 -G3 -OP -OP -OP -G3 -G3 -G3 -G3 -G3 -L -L -G1 -JPN1 -OP -G3 -OP -JPN2 -G3 -JPN1 -G3 -G3 -L-L -L -L -G3 -L -L -G2 -L -G3 -G1 -G2 -G2 -G3 -L -G1 -G2 -G3 -G1 -G3 -L -L -L -G3 -G3 -L -G1

More information

2 1 7 - TALK ABOUT 21 μ TALK ABOUT 21 Ag As Se 2. 2. 2. Ag As Se 1 2 3 4 5 6 7 8 9 1 1 2 3 4 5 6 7 8 9 1 1 2 3 4 5 6 7 8 9 1 Sb Ga Te 2. Sb 2. Ga 2. Te 1 2 3 4 5 6 7 8 9 1 1 2 3 4 5 6 7 8 9 1 1 2 3 4

More information

42 3 u = (37) MeV/c 2 (3.4) [1] u amu m p m n [1] m H [2] m p = (4) MeV/c 2 = (13) u m n = (4) MeV/c 2 =

42 3 u = (37) MeV/c 2 (3.4) [1] u amu m p m n [1] m H [2] m p = (4) MeV/c 2 = (13) u m n = (4) MeV/c 2 = 3 3.1 3.1.1 kg m s J = kg m 2 s 2 MeV MeV [1] 1MeV=1 6 ev = 1.62 176 462 (63) 1 13 J (3.1) [1] 1MeV/c 2 =1.782 661 731 (7) 1 3 kg (3.2) c =1 MeV (atomic mass unit) 12 C u = 1 12 M(12 C) (3.3) 41 42 3 u

More information

橡H141(成人モニタリング12年まとめ)表紙・目次・

橡H141(成人モニタリング12年まとめ)表紙・目次・ 2 12 C NO2SPM C 10 1 V25 NOx 1 10836 NOx 0.767ppm 13860 NOx 0.703ppm (3) 33562 NOx 0.710ppm (4) 33432 NOx 0.800ppm (5) 15392 NOx 0.611ppm (6) 9263 NOx 0.508ppm (7) 8165 NOx 0.284ppm - 1 - (8) 10866 NOx

More information

1 1 2 2 3 3 RBS 3 K-factor 3 5 8 Bragg 15 ERDA 21 ERDA 21 ERDA 21 31 31 33 RUMP 38 42 42 42 42 42 42 4 45 45 Ti 45 Ti 61 Ti 63 Ti 67 Ti 84 i Ti 86 V 90 V 99 V 101 V 105 V 114 V 116 121 Ti 121 Ti 123 V

More information

高知工科大学電子 光システム工学科

高知工科大学電子 光システム工学科 卒業研究報告 題 目 量子力学に基づいた水素分子の分子軌道法的取り扱いと Hamiltonian 近似法 指導教員 山本哲也 報告者 山中昭徳 平成 14 年 月 5 日 高知工科大学電子 光システム工学科. 3. 4.1 4. 4.3 4.5 6.6 8.7 10.8 11.9 1.10 1 3. 13 3.113 3. 13 3.3 13 3.4 14 3.5 15 3.6 15 3.7 17

More information

1).1-5) - 9 -

1).1-5) - 9 - - 8 - 1).1-5) - 9 - ε = ε xx 0 0 0 ε xx 0 0 0 ε xx (.1 ) z z 1 z ε = ε xx ε x y 0 - ε x y ε xx 0 0 0 ε zz (. ) 3 xy ) ε xx, ε zz» ε x y (.3 ) ε ij = ε ij ^ (.4 ) 6) xx, xy ε xx = ε xx + i ε xx ε xy = ε

More information

橡kenkyuhoukoku8.PDF

橡kenkyuhoukoku8.PDF 10-1- -2- 11 21 10 5 12 1 10 0 5 3-3- -4-10 75 3 10 10 75 100 10 75 5 10 (1) (2) -5- (3) -6- (4) 27 11.290 291-7- (5) 1 1-8- 1 (6) 51 (7) -9- (1) (2) -10- (3) -11- (4) -12- -13- (5) (6) (7) (1) (2) -14-

More information

30

30 3 ............................................2 2...........................................2....................................2.2...................................2.3..............................

More information

untitled

untitled 1. Web21 2001 4 2. Web21 2001 4 3. Web21 2001 4 4. Web21 2001 4 5. BCS Web21 2001 6 6. Web21 2001 6 7. Web21 2001 8 8. - Web21 2001 10 9. 9-1. Web21 2001 10 9-2. d Web21 2001 12 9-3. Web21 2001 12 1. T

More information

02

02 Q A Ax Pb Ni Cd Hg Al Q A Q A Q A 1 2 3 2 0 1 2 3 4 5 6 7 0 1 2 3 4 5 6 7 8 0 0 1 2 3 4 1 0 1 2 Q A ng/ml 4500 D H E A 4000 3500 3000 2500 2000 DHEA-S - S 1500 1000 500 0 10 15 20 25 30 35 40 45

More information

税関分析25 年の進歩

税関分析25 年の進歩 25 1 25 40 27 25 27 32 25 CeEDTA 10) 11 1) Fe Al Zn EDTA 2) 12) n IR400 2N BT EDTA 14) e 15) 16) 17) 18) 3) Zn Cu 4) Mn 5) 6) 7) 8) 9 13) 2 24) X 56),57) 58) 25) 59) 60) X 61) X X 26) X 27),28),29) 62)

More information

( ) ) AGD 2) 7) 1

( ) ) AGD 2) 7) 1 ( 9 5 6 ) ) AGD ) 7) S. ψ (r, t) ψ(r, t) (r, t) Ĥ ψ(r, t) = e iĥt/ħ ψ(r, )e iĥt/ħ ˆn(r, t) = ψ (r, t)ψ(r, t) () : ψ(r, t)ψ (r, t) ψ (r, t)ψ(r, t) = δ(r r ) () ψ(r, t)ψ(r, t) ψ(r, t)ψ(r, t) = (3) ψ (r,

More information

¼§À�ÍýÏÀ – Ê×ÎòÅŻҼ§À�¤È¥¹¥Ô¥ó¤æ¤é¤®

¼§À�ÍýÏÀ – Ê×ÎòÅŻҼ§À�¤È¥¹¥Ô¥ó¤æ¤é¤® email: takahash@sci.u-hyogo.ac.jp Spring semester, 2012 Outline 1. 2 / 26 Introduction : (d ) : 4f 1970 ZrZn 2, MnSi, Ni 3 Al, Sc 3 In Stoner-Wohlfarth Moriya-Kawabata (1973) 3 / 26 Properties of Weak

More information

70の法則

70の法則 70 70 1 / 27 70 1 2 3 4 5 6 2 / 27 70 70 70 X r % = 70 2 r r r 10 72 70 72 70 : 1, 2, 5, 7, 10, 14, 35, 70 72 : 1, 2, 3, 4, 6, 8, 9, 12, 18, 24, 36, 72 3 / 27 r = 10 70 r = 10 70 1 : X, X 10 = ( X + X

More information

2 6 8 10 12 14 18 20 22 24 26 29 32 34 36 1 40 42 44 39 47 48 50 52 54 56 58 60 62 64 68 70 72 74 76 78 80 67 83 84 86 88 90 92 94 96 97 98 100 102 103 104 106 110 112 114 116 118 120 122 124 126 128 130

More information

E-2 A, B, C A, A, B, A, C m-cresol (NEAT) Rh S m-cresol m-cresol m-cresol x x x ,Rh N N N N H H n Polyaniline emeraldine base E-3 II

E-2 A, B, C A, A, B, A, C m-cresol (NEAT) Rh S m-cresol m-cresol m-cresol x x x ,Rh N N N N H H n Polyaniline emeraldine base E-3 II E 7, 8, 9 E-1 A, B B A, A, A,, [Novoselov, et al., Science 306, 666, (2004)].,,,.,,,.,. (t a, t b, t c ), [PRB.74, 033413, (2006)],.,, t b /t a t c /t a 0.5., [Ni, etal., ACS, Nano2, 2301, (2008)],, [Zhou

More information