untitled

Size: px
Start display at page:

Download "untitled"

Transcription

1 大学加速器施設一覧 大学加速器連携協議会

2

3

4 URL

5 1 YU-AMS 2 3 CYRIC GeV BST 7 t-acts 8 9 UTTAC 10 GHMC 11 FEL-TUS 12 LEBRA MALT 15

6 HIT NUANS 21 SR KU-FEL 27 QSEC 28 FFAG RCNP 31 32

7 SDH-2 37 HSRC FFAG 40 UVSOR-III 41 KEK J-PARC 42 KEK SuperKEKB 43 KEK LINAC 44 KEK PF 45 KEK PF-AR 46 KEK ATF 47 KEK LUCX 48

8 YU-AMS 2 9 UTTAC 10 MALT 15 HIT NUANS 21 QSEC

9 5SDH t-acts 8 LEBRA KEK LINAC 44

10 KEK ATF 47 KEK LUCX 48 CYRIC 4 24 FFAG 29 RCNP 31 FFAG 40 KEK J-PARC 42 3 GHMC GeV BST 7

11 FEL-TUS 12 SR 22 KU-FEL 27 HSRC 38 UVSOR-III 41 KEK PF 45 KEK PF-AR KEK SuperKEKB 43

12 , MeV 36 μa A 10 m 2/3 π π mm mrad R F RF 2,856 MHz Duty % 50 pulse/s 3.4 μs / m 3 Normal/Maximum Resolution Δ E/E % : Peak E π mm mrad : 2 1,127 m m 2 71 kw / 20/30 2, MeV- 100 μa-50 pulse/s

13 YU-AMS AMS , SDH-1, NEC AMS C, 13 C, 14 C 0.5 MV 400 μa MC-SNICS II 60 kev π mm mrad B ρ 0.5 MeV Δ E/E: % 400 m 2 2 kw / 200/10 1,000 MC-SNICS 2 4

14 C 6+ RFQ + IH - DTL Hz 4 MeV/u 430 MeV/u FODO nm mm ma ma 63 m m RF MHz RF MV h at ma h at ma 3D

15 CYRIC , AVF 1999 H Xe K kv 10 pps 3 μa ECR 14 GHz, 10 GHz, 2.4 GHz 1.64 Tesla 396,000 AT RF 2 1/4 λ RF MHz MeV n/cm m ,000 kw / 200/50 1,800 HM12 PET

16 kw 60 MeV RI MeV 120 μ A 130 ma 20 m S-band 80 π mm mrad RF 2 RF 2,856 MHz Duty 0.1 % 300 pulse/s 3 μs / 8 / 1 m Resolution Δ E/E % : 10 Peak E π mm mrad m kw / 126 / MeV linac %

17 GeV BST 100 MeV m S BST , MeV 0.6 μa 60 ma 15 m + α α RF 1 RF 2,856 MHz Duty pulse/s 3 μs / 2 / 3 m Resolution Δ E/E % : 1.0 % ε π mm mrad : m kw 1,300 RF t-acts

18 1.3 GeV BST GeV , Hz 0.09 GeV 1.3 GeV : double-bend, 4 cell 140 nm 0.06 % 25 mm 40 ma 50 m 3 m RF 500 MHz RF 0.2 MV 0.3 h at 20 ma GeV BM GeV BM5 Duty 60 % 160 or GeV 1.0 GeV linac

19 t-acts MeV 3 m S MeV 0.6 μa 60 ma 15 m + α α RF 1 RF 2,856 MHz Duty pulse/s 3 μs / 1 / 3 m Resolution Δ E/E % : 1.0 % ε π mm mrad : m kw / 22/

20 , H, D, He 4.5 MV 3,000 μa 0.4 μm mm kev π mm mrad B ρ MeV Δ E/E: 10-5 % : 25 25m 2 6 kw / 30 1,000 3

21 UTTAC MV 6 MV 2 Experimental Room A6 A5 A7 A4 A3 A2 A1 Positron annihilation 1 MV Tandetron Mossbauer spectrometer Experiment preparation room Polarized Ion Source (PIS) Beam transport Vertical line Machine shop S1 L5 55º Accelerator Room L4 AMS L3 S2 S5 L2 L1 MC-SNICSs S3 S4 6 MV tandem 90º 40º 105º 10 m SF 6 storage tank , SDH-2 National Electrostatics Corp. 6 MV Pelletron tandem 2016 p, d, p d He, 6.5 MV p 3 μa : 50 μa 10.5 m 2.74 m 20,865 kg Cs SNICS II Cs MC-SNICS 2 RF Alphatross AMS 65 kev 9.5 π mm mrad B ρ 1.5 T 1.27 ME/Z 2 = 176 amu MeV RP + TMP MeV Δ E/E : 10-4 % General Ionex Corp. 1 MV Tandetron p, He, 1.1 MV 3 μa Cs Model860 / 20 kev MeV ΔE/E: 10-4 % AMS m m 2 Tandetron 12 Pelletron 4 Tandetron / 102 / UD Pelletron tandem 6 MV Pelletron tandem

22 GHMC RF-KO , C 6+ 4 MeV/u 400 MeV/u 1.1s 1.44 ena 4.32 ena 63.3 m BM T, 20 deg QF6 QD6 SF3 SD3 RF MHz 2 kw 15 Normal/Maximum Resolution Δ E/E % : 1.5 Peak E π mm mrad : MeV/u 10 GHz ECR C eua RFQ + APF IH-DTL 6 π mm mrad RF 200 MHz Duty 0.02 % 0.3 pulse/s 58 μs / 2 / m 65 m 2 4 3,200 kw / 20 / 2 930

23 FEL-TUS S-band , MeV 1.5 μa 50 ma RF RF 2,856 MHz 5 pulse/s 6.8 μs / 1 / 3 m m 2 1 kw / 6/ KEK Time resolved temperature measurement of polymer surface irradiated by mid-ir free electron laser, M. Araki, T. Chiba, T. Oyama, T. Imai, and K. Tsukiyama, Nucl. Instr. Meth. in Phys. Res. B 405, Picosecond pulsed infrared laser tuned to amide I band dissociates polyglutamine fibrils in cells, T. Kawasaki, G. Ohori, T. Chiba, K. Tsukiyama and K. Nakamura, Lasers Med. Sci., 31, Isomerization and dissociation of 2,3-dihydrofuran 2,3-DHF induced by infrared free electron laser, M. Matsubara, F. Osada, M. Nakajima, T. Imai, K. Nishimura, T. Oyama and K. Tsukiyama, J. Photochem. Photobiol. A, 322,

24 LEBRA B MeV X , MeV 25 μa 100 ma 20 m DC 100 kv 10 π mm mrad R F 30 MW 2 RF 2,856 MHz Duty % 12.5 pulse/s 20 μs / 4 m 3 Normal/Maximum Resolution Δ E/E % : 2 % 6 % THz μm 4 34 kev X 500 m 2 THz, X 1 port, FEL 9 port 40 kw / 20/2 1,500 KEK PV 3030 KEK

25 L 18 L ML , 22, 18 MeV 10 μ A 1 A 20 m 90 kv 100 π mm mrad R F RF 2,856 MHz Duty % 50 pulse/s 1 μs / 30 / m Normal/Maximum Resolution Δ E/E % : 1 % Peak E π mm mrad : 35 MeV 100 π mm mrad m 2 10 m 150 kw / L, 18 L 35 L 18 L

26 MALT hmatsu@um.u-tokyo.ac.jp MV AMS NRAERDA ,000 5 UD 1993 H +, Be 3+, C 4+, N 2+, Al 3+, Cl 6+, I 5+, etc. 5.0 MV 1 μa Cs DC, 75 kev 7 π mm mrad B ρ 1.9 T m TP, Cryo-P, IP 1-30 MeV Δ E/E - % - m 2 5 RBS, ERDA, AMS, NRA, PIXE - kw / - 5,000

27 HIT HIT / 2012 / 1984 C W / P O 1.7 / 3.75 MV 200 μ A@Si / - RF / PIG - kev - π mm mrad B ρ IP, TMP, RP - MeV Δ E/E: - % 300 / 200 m kw / 70 /

28 nhagura@tcu.ac.jp MV PIG PIXE/RBS MAS MV 3 μa PIG 20 kev π mm mrad B ρ 3.4 MeV Δ E/E: % m 2 kw /

29 kev , MV 1,000 μa 1.8 m 2 m 2 m 200 kev π mm mrad B ρ MeV Δ E/E: % 60 m 2 kw / 20 6,000

30 BNL Gun RF ,000 LINAC 2001 Max. 6 MeV 50 na 500 A 10 cm 3 π mm mrad R F RF 2,856 MHz Duty % Max. 25 pulse/s s 1 μs / 1.5 / 10 cm Normal/Maximum Resolution Δ E/E % : 1 Peak E π mm mrad : 3 π mm mrad 2 X THz 100 m 2 1 kw / 25 6,000

31 AMS 14 C 5 14 C ,440 HVE model 4130-AMS MV C- 30 μa 1,120 x 510 cm 2 HVE model-846b 12 C-, 13 C-, 14 C kev π mm mrad B ρ 1.24 T, 50 cm MeV Δ E/E 6 x 10-4 % 14 C/ 12 C 14 C 160 m 2 14 C/ 13 C/ 12 C 1 48 kw / 20/ C 1, C

32 NUANS - j.html MV 15,000 μa 7.5 m ECR kev π mm mrad B ρ MeV Δ E/E % m 2 2 kw /

33 SR , mm 300 ma ma 314 m 0.5 m RF 191 MHz RF 0.1 MV 75 h at 200 ma h at ma 10 Hz 0.15 GeV GeV 1,600 nm 0.78

34 KSR RF 2,857 MHz Duty % 15 pulse/s 0.1 μs / 3 / 3 m Normal/Maximum Resolution Δ E/E % : Peak E π mm mrad : MeV 0.15 μa 100 ma 15 m 100 kv Y-796 Eimac π mm mrad R F m 2 1 kw / 0 0

35 LSR RF MHz Duty % 1 pulse/s 50 μs / 2 / 4 m Normal/Maximum Resolution Δ E/E % : Peak E π mm mrad : RFQ, DTL MeV 1 na 20 μa 8 m 50 kev π mm mrad R F 2 75 m 2 1 kw / 0 0

36 m m RF MHz RF 20 kv h at ma h at ma MeV khz MeV MeV : triple bend achromatic nm mm 100 ma ma 200 m 2 1 kw / 0 0

37 m 1.05 m RF Hz RF V h at h at 2 ma ma Mg+ Mg p:1.61 MHz Mg : khz P : 7 MeV Mg : 40 kv P : 7 MeV Mg : 40 kv QF-BM-QD nm mm 0.6 μa ma 225 m 2 1 kw / 0 0

38 KU-FEL < > 2,856 MHz < 4.5 > 8.4 MeV 7.8 μs 3 μc < > 2.9 m MeV 6.5 μs 700 nc < 1.6 > 4.6 MeV 1 4 < 1 nc 2 < > 3.6 ~ 23 μm 1 30 mj 2 μs < 1 ps 100 m 2 1 / 3 / 6 300

39 QSEC VI MV 10 μa MeV VE MV 20 μa MeV MV 1 μa Li Cs MeV 6 SDH-2 NEC MV 1 μa RF-Rb Cs MeV RI

40 FFAG KUCA ADS 150 MeV Hz GeV GeV Radial sector FFAG 15,000 nm 0.7 % 6,000 mm ma ma m 90 m RF MHz RF MV h at ma h at ma

41 kw L 1.3 GHz X X RI , Applied Radiation MeV 330 μa 6 A EIMAC YU-156 RF 1.30 GHz Duty % pulse/s pulse/s : ns μs 1 st sec. 2.5 m 2 nd sec. 1.8 m 2 X m m-tof m m m-tof, 12 m -TOF, 22 m -TOF, 150 kw / 639/ , RI

42 RCNP AVF ,000 6,000 AVF AVF 1973, Ring 1991 p, d, 3 He, 4 He, max. AVF 60, Ring 500 kv max. AVF 5, Ring 1.1 μa AVF L10 m W7 m H4 m Ring ϕ 15 m H5 m SC-ECR 18 GHz NEOMAFIOS 10 GHz 2.45 GHz ECR 2.45 GHz 15 Q kev AVF 10 Ring 2 π mm mrad Bρ AVF 1.7, Ring 2.9 Tm RP, TMP, DP, Cryo-pump AVF p 5-80 MeV, max. 35 MeV/n, Ring MeV, max. 100 MeV/n Δ E/E 0.01 % AVF 3,000 4,000 m 2 AVF 7 Ring 8 kw / 50 / 400 5,000 6,000

43 FEL ,000 Duty 0.06 % 30/60 pulse/s 5/10 μs / 39 / 3 m Normal/Maximum Resolution Δ E/E % 3 1 Peak E π mm mrad : THz L MeV 7.2 μa 15 A 480 μa 2 A 20 m 3 π mm mrad RF 1.3 GHz 268 m kw / 820/980 2, MeV 30 nc 20 ps 60 pps 30 MeV 15 A 8 ns 60 pps 15 MeV 2 A 8 μs 30 pps

44 C kev 600 kev 500 μa 2 m 50 m 2 1 / 5

45 C PIXE RBS μm m 2 1 / μm 2012 H He 0.95 MV 1 μa 2 m RF 950 kev

46 C m 2 3 / MeV 15 MeV 30 μa 300 ma 2 m Y-796 RF S 60 pulse/s 3 ns 4 μs

47 , m 2 4 / ,300 5 SDH p, He 1.7 MV p 0.4 μa SNICS II, Alphatros 6.0 kev Δ E/E 0.01 %

48 5SDH-2 RI RBS, ERDA, NRA PIXE ,300 5 SDH p, d, He, C, Cu, Ag, Au 1.7 MV 1 μa 4 m SNICS-2, Alphatross DC 25 kev 6-8 π mm mrad B ρ 1.6 T TMP MeV Δ E/E% 170 m kw / 40 1,300

49 HSRC , Hz 150 MeV 700 MeV ODOFOBOFODO 400 nm mm 350 ma - ma m 0.87 m RF MHz RF 0.2 MV 10 h at 200 ma - h at - ma T 40 mm 1 2,354.2 mm 57 mm mm 0.41 T APPLE-II 1 1,845 mm 78 mm mm 0.86 T 0.59 T 0.50 T X

50 NEC 8UDH 2014 p, d, α, 8 MV μa 14 m 1 MC-SNICS 2 RF Alphatross 70 kev B ρ 1.4 Tm m kw / 25 / MV 8 MV

51 FFAG FFAG FFAG 150 MeV FFAG μa 10 m AVF PIG 10 kev 125 MeV FFAG 1,500 kw 150 MeV

52 UVSOR mkatoh@ims.ac.jp , Hz 0.75 GeV 0.75 GeV Extended DB 17.5 nm ps 500 ma 100 ma 53.2 m 2.2 m RF 90.1 MHz RF 120 kv 300 ma Top-up 40 ma Top-up Number of magnets 8 Magnetic length m Bending radius 2.2 m Bending angle 45 deg Pole gap 55.2 mm Pole width 140 mm Apple - 1 Apple

53 KEK J-PARC KEK JAEA K 2 2 Rapid Cycling Synchrotron RCS, Main Ring Synchrotron MR 3 GeV 30 GeV KEK&JAEA KEK 41 KEK 12 KEK 14 4 KEK 2 6,000 H Linac RCS&MR 400 MeV RCS 3 GeV MR 3 GeV RCS 30 GeV MR FX RCS FX&SX MR 250 m Linac m RCS m MR) 25 Hz Linac&RCS, 0.4 Hz MR-FX, 0.2 Hz MR-SX 1 MW RCS, 750 kw MR MLF, MD, NU MLF 23 Neutron, 4 muon HD K1.8/BR, K1.1/BR, K0, Hi-momentum BL, COMET NU T2K 60,000 kw 200 / MLF 500 kw HD 44 kw NU 470 kw

54 KEK SuperKEKB ,016 m 7 GeV 4 GeV B CP KEKB 1994 KEKB 1998 SuperKEKB 2010 SuperKEKB / 7 GeV / 4 GeV 7 GeV / 4 GeV 8 x 10E35 cm -2 s π cell 4.6 / 3.2 nm 0.30 / 0.27 mm 6.4 / E-4 5 / 6 mm 2,600 / 3,600 ma 3,016 m RF MHz RF 15 MV / 10 MV Belle II collaboration Belle II KEKB hourglass 0.3 mm 83 mrad

55 KEK LINAC x m 7 GeV 4 GeV SuperKEKB 2.5 GeV PF 6.5 GeV PF-AR , ,000 MeV 3,500 MeV 1 μa 1 ka 600 m RF RF 2 10 π mm mrad RF 60 RF 2,856 MHz Duty % 50 pulse/s 1 μs / 230 / 1.9 m Normal/Maximum Resolution Δ E/E % : Peak E π mm mrad : ,000 m 2 6 4,000 kw / 10 48

56 KEK PF GeV X , Hz 2.5 GeV 2.5 GeV FODO 34.6 nm mm 450 ma ma 187 m 8.66 m RF MHz RF 1.7 MV 20 h at 450 ma 8 h at 450 ma Name u L Gy Ky c B cm m cm kev Bend 4 3.5E+14 SGU# E+17 U# E+18 U# E+16 SGU# E+17 MPW#05-W E+16 U# E+17 VW# E+14 SGU# E+16 U#16-1 & E+17 SGU# E+17 R#19B E+17 U# E+16 PF 2.5 GeV GeV PF-AR 5 1 2

57 KEK PF-AR GeV X , Hz 6.5 GeV 6.5 GeV FODO 293 nm mm 60 ma 377 m 23.2 m RF MHz RF 17 MV 15 h at 50 ma Name u L Gy Ky c B cm m cm kev Bend E+13 EMPW#N E+15 E01-W U#NE E+15 U#NW E+15 U#NW E+15 U#NW E+15 U#NW E+15 PF 2.5 GeV GeV PF-AR 5 1 2

58 KEK ATF x KEK Accelerator Test Facility, ATF ILC 1992 DR 2008 ATF DR 2010 ATF , m RF S 2,856 MHz + 2, MHz Hz 1.3 GeV 20 / 2.8 ns 0.8 μa 5 π mm mrad m 1.3 GeV :FOBO Combined Bend 1/0.01 / nm 10 ms 5 mrad 60 ns flat-top 300 ns 6 mm RF 714 MHz RF 0.7 MV Touchek Lifetime 80 s ATF2 1.3 GeV Single 150 ns ns ns nm 6,000 m 2 2,300 kw / 30 C-band BPM 25 nm 1 µm

59 KEK LUCX x KEK Laser Undulator Compact X-Ray Source:LUCX 24 MeV 1 MW λ 1064 nm10 kev X THz , MeV 1.9 μa 215 ma 13 m RF 5-8 π mm mrad R F S-band 2 NEG RF 2,856 MHz Duty % pulse/s 4 μs / 12 / 0.68 m Normal/Maximum Resolution Δ E/E % 0.2 / RMS 2/ Peak-to-Peak Peak E π mm mrad : kev m kw / 4 /

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

Microsoft PowerPoint - 島田美帆.ppt

Microsoft PowerPoint - 島田美帆.ppt コンパクト ERL におけるバンチ圧縮の可能性に関して 分子科学研究所,UVSOR 島田美帆日本原子力研究開発機構,JAEA 羽島良一 Outline Beam dynamics studies for the 5 GeV ERL 規格化エミッタンス 0.1 mm mrad を維持する周回部の設計 Towards user experiment at the compact ERL Short bunch

More information

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

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 63 3 Section 3.1 g 3.1 3.1: : 64 3 g=9.85 m/s 2 g=9.791 m/s 2 36, km ( ) 1 () 2 () 3 9.8 m/s 2 3.2 3.2: : a) b) 5 15 4 1 1. 1 3 14. 1 3 kg/m 3 2 3.3 1 3 5.8 1 3 kg/m 3 3 2.65 1 3 kg/m 3 4 6 m 3.1. 65 5

More information

Canvas-tr01(title).cv3

Canvas-tr01(title).cv3 Working Group DaiMaJin DaiRittaikaku Multiparticle Jiki-Bunnsekiki Samurai7 Superconducting Analyser for Multi particles from RadioIsotope Beams with 7Tm of bending power (γ,n) softgdr, GDR non resonant

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

X線散乱と放射光科学

X線散乱と放射光科学 8 X II 305 8.1..................................... 305 8.1.1................. 305 8.1.2.................................... 307................................... 307............................ 308.........................

More information

Neutron yield M.R. Hawkesworth, Neutron Radiography: Equipment and Methods, Atomic Energy Review 15, No. 2, , n µc -1 = n/(µa s) ~10 12 n

Neutron yield M.R. Hawkesworth, Neutron Radiography: Equipment and Methods, Atomic Energy Review 15, No. 2, , n µc -1 = n/(µa s) ~10 12 n Cross Section 7MeV Proton Linac AFRD, LBL (courtesy of Jani Reionen) LINAC SYSTEMS Applied Pulsed Power Plasma Target D+D reaction driven by LASER Neutron yield M.R. Hawkesworth, Neutron Radiography: Equipment

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

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

Table 1: Basic parameter set. Aperture values indicate the radius. δ is relative momentum deviation. Parameter Value Unit Initial emittance 10 mm.mrad

Table 1: Basic parameter set. Aperture values indicate the radius. δ is relative momentum deviation. Parameter Value Unit Initial emittance 10 mm.mrad SuperKEKB EMITTANCE GROWTH BY MISALIGNMENTS AND JITTERS IN SUPERKEKB INJECTOR LINAC Y. Seimiya, M. Satoh, T. Suwada, T. Higo, Y. Enomoto, F. Miyahara, K. Furukawa High Energy Accelerator Research Organization

More information

Undulator.dvi

Undulator.dvi X X 1 1 2 Free Electron Laser: FEL 2.1 2 2 3 SACLA 4 SACLA [1]-[6] [7] 1: S N λ [9] XFEL OHO 13 X [8] 2 2.1 2(a) (c) z y y (a) S N 90 λ u 4 [10, 11] Halbach (b) 2: (a) (b) (c) (c) 1 2 [11] B y = n=1 B

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

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

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 . 4cm 6 cm 4cm cm 8 cm λ()=a [kg/m] A 4cm A 4cm cm h h Y a G.38h a b () y = h.38h G b h X () S() = π() a,b, h,π V = ρ M = ρv G = M h S() 3 d a,b, h 4 G = 5 h a b a b = 6 ω() s v m θ() m v () θ() ω() dθ()

More information

1 2 2 (Dielecrics) Maxwell ( ) D H

1 2 2 (Dielecrics) Maxwell ( ) D H 2003.02.13 1 2 2 (Dielecrics) 4 2.1... 4 2.2... 5 2.3... 6 2.4... 6 3 Maxwell ( ) 9 3.1... 9 3.2 D H... 11 3.3... 13 4 14 4.1... 14 4.2... 14 4.3... 17 4.4... 19 5 22 6 THz 24 6.1... 24 6.2... 25 7 26

More information

OHO.dvi

OHO.dvi 1 Coil D-shaped electrodes ( [1] ) Vacuum chamber Ion source Oscillator 1.1 m e v B F = evb (1) r m v2 = evb r v = erb (2) m r T = 2πr v = 2πm (3) eb v

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

Μ粒子電子転換事象探索実験による世界最高感度での 荷電LFV探索 第3回機構シンポジューム 2009年5月11日 素粒子原子核研究所 三原 智

Μ粒子電子転換事象探索実験による世界最高感度での 荷電LFV探索  第3回機構シンポジューム 2009年5月11日 素粒子原子核研究所 三原 智 µ COMET LFV esys clfv (Charged Lepton Flavor Violation) J-PARC µ COMET ( ) ( ) ( ) ( ) B ( ) B ( ) B ( ) B ( ) B ( ) B ( ) B 2016 J- PARC µ KEK 3 3 3 3 3 3 3 3 3 3 3 clfv clfv clfv clfv clfv clfv clfv

More information

4_Laser.dvi

4_Laser.dvi 1 1905 A.Einstein 1917 A.Einstein 1954 C.H.Townes MASER Microwave Amplification by Stimulated Emission of Radiation 23.9 GHz 1.26 cm 1960 T.H.Maiman LASER Light Amplification by Stimulated Emissin of Radiation

More information

news

news ETL NEWS 1999.9 ETL NEWS 1999.11 Establishment of an Evaluation Technique for Laser Pulse Timing Fluctuations Optoelectronics Division Hidemi Tsuchida e-mail:tsuchida@etl.go.jp A new technique has been

More information

untitled

untitled BELLE TOP 12 1 3 2 BELLE 4 2.1 BELLE........................... 4 2.1.1......................... 4 2.1.2 B B........................ 7 2.1.3 B CP............... 8 2.2 BELLE...................... 9 2.3

More information

µµ InGaAs/GaAs PIN InGaAs PbS/PbSe InSb InAs/InSb MCT (HgCdTe)

µµ InGaAs/GaAs PIN InGaAs PbS/PbSe InSb InAs/InSb MCT (HgCdTe) 1001 µµ 1.... 2 2.... 7 3.... 9 4. InGaAs/GaAs PIN... 10 5. InGaAs... 17 6. PbS/PbSe... 18 7. InSb... 22 8. InAs/InSb... 23 9. MCT (HgCdTe)... 25 10.... 28 11.... 29 12. (Si)... 30 13.... 33 14.... 37

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

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

環境報告2008ダイジェスト版

環境報告2008ダイジェスト版 2008 KEK Environmental Report 2008 2008 http://www.kek.jp/kankyou/pdf/kankyohoukokusho2008.pdf Inter-University Research Institute Corporation High Energy Accelerator Research Organization CO 2 CO 2 2007

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

cm λ λ = h/p p ( ) λ = cm E pc [ev] 2.2 quark lepton u d c s t b e 1 3e electric charge e color charge red blue green qq

cm λ λ = h/p p ( ) λ = cm E pc [ev] 2.2 quark lepton u d c s t b e 1 3e electric charge e color charge red blue green qq 2007 2007 7 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 1 2007 2 4 5 6 6 2 2.1 1: KEK Web page 1 1 1 10 16 cm λ λ = h/p p ( ) λ = 10 16 cm E pc [ev] 2.2 quark lepton 2 2.2.1 u d c s t b + 2 3 e 1 3e electric charge

More information

(e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ,µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) [ ] [ ] [ ] ν e ν µ ν τ e µ τ, e R,µ R,τ R (2.1a

(e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ,µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) [ ] [ ] [ ] ν e ν µ ν τ e µ τ, e R,µ R,τ R (2.1a 1 2 2.1 (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ,µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) [ ] [ ] [ ] ν e ν µ ν τ e µ τ, e R,µ R,τ R (2.1a) L ( ) ) * 2) W Z 1/2 ( - ) d u + e + ν e 1 1 0 0

More information

J-PARC October 14-15, 2005 KEK

J-PARC October 14-15, 2005 KEK J-PARC October 14-15, 2005 KEK 目次 ミューオン 電子転換過程の紹介 MECO実験 PRISM/PRIME実験 @J-PARC まとめ GIM-like mixing! µ! e W e 3 SUSY-GUT Large top Yukawa couplings result in sizable off-diagonal components in a slepton

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

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

EGunGPU

EGunGPU Super Computing in Accelerator simulations - Electron Gun simulation using GPGPU - K. Ohmi, KEK-Accel Accelerator Physics seminar 2009.11.19 Super computers in KEK HITACHI SR11000 POWER5 16 24GB 16 134GFlops,

More information

V(x) m e V 0 cos x π x π V(x) = x < π, x > π V 0 (i) x = 0 (V(x) V 0 (1 x 2 /2)) n n d 2 f dξ 2ξ d f 2 dξ + 2n f = 0 H n (ξ) (ii) H

V(x) m e V 0 cos x π x π V(x) = x < π, x > π V 0 (i) x = 0 (V(x) V 0 (1 x 2 /2)) n n d 2 f dξ 2ξ d f 2 dξ + 2n f = 0 H n (ξ) (ii) H 199 1 1 199 1 1. Vx) m e V cos x π x π Vx) = x < π, x > π V i) x = Vx) V 1 x /)) n n d f dξ ξ d f dξ + n f = H n ξ) ii) H n ξ) = 1) n expξ ) dn dξ n exp ξ )) H n ξ)h m ξ) exp ξ )dξ = π n n!δ n,m x = Vx)

More information

COE

COE COE COOL05 MD @ @ @ @ n ν x, y 2 2 International Workshop on Beam Cooling and Related Topics ( COOL05) General Topics Overview. S-LSR Report from Lab Report from Lab Electron Cooling Muon Cooling

More information

c 2009 i

c 2009 i I 2009 c 2009 i 0 1 0.0................................... 1 0.1.............................. 3 0.2.............................. 5 1 7 1.1................................. 7 1.2..............................

More information

加速器の基本概念 V : 高周波加速の基礎

加速器の基本概念  V : 高周波加速の基礎 .... V : KEK koji.takata@kek.jp http://research.kek.jp/people/takata/home.html 2015 2015 4 16 1 2 (1) 3 (2) 4 5 6 ERL: Energy Recovery Linac LCLS: Linac Coherent Light Source LC : µ-µ Koji Takata (KEK)

More information

main.dvi

main.dvi MICE Sci-Fi 2 15 3 7 1 1 5 1.1 MICE(Muon Ionization Cooling Experiment)............. 5 1.1.1........................... 5 1.1.2............................... 7 1.1.3 MICE.......................... 10

More information

i

i 009 I 1 8 5 i 0 1 0.1..................................... 1 0.................................................. 1 0.3................................. 0.4........................................... 3

More information

橡実験IIINMR.PDF

橡実験IIINMR.PDF (NMR) 0 (NMR) 2µH hω ω 1 h 2 1 1-1 NMR NMR h I µ = γµ N 1-2 1 H 19 F Ne µ = Neh 2mc ( 1) N 2 ( ) I =1/2 I =3/2 I z =+1/2 I z = 1/2 γh H>0 2µH H=0 µh I z =+3/2 I z =+1/2 I z = 1/2 I z = 3/2 γh H>0 2µH H=0

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

放射線化学, 92, 39 (2011)

放射線化学, 92, 39 (2011) V. M. S. V. 1 Contents of the lecture note by Prof. V. M. Byakov and Dr. S. V. Stepanov (Institute of Theoretical and Experimental Physics, Russia) are described in a series of articles. The first article

More information

2

2 Rb Rb Rb :10256010 2 3 1 5 1.1....................................... 5 1.2............................................. 5 1.3........................................ 6 2 7 2.1.........................................

More information

AN6591FJM

AN6591FJM IC AN6591FJM PHS, PLL IC AN6591FJMPHSIF PLL IC QFN (Quad flat non-leaded PKG) (0.63) 34 44 R0.30 6.20±0.10 (6.00) 33 23 1 11 (0.63) 22 12 3-C 0.50 (6.00) 6.20±0.10 0.20±0.10 0.80 max Unit : mm, PLL,, APC

More information

(Blackbody Radiation) (Stefan-Boltzmann s Law) (Wien s Displacement Law)

(Blackbody Radiation) (Stefan-Boltzmann s Law) (Wien s Displacement Law) ( ) ( ) 2002.11 1 1 1.1 (Blackbody Radiation).............................. 1 1.2 (Stefan-Boltzmann s Law)................ 1 1.3 (Wien s Displacement Law)....................... 2 1.4 (Kirchhoff s Law)...........................

More information

J-PARC E15 K K-pp Missing mass Invariant mass K - 3 He Formation K - pp cluster neutron Mode to decay charged particles p Λ π - Decay p Decay E15 dete

J-PARC E15 K K-pp Missing mass Invariant mass K - 3 He Formation K - pp cluster neutron Mode to decay charged particles p Λ π - Decay p Decay E15 dete J-PARC E15 (TGEM-TPC) TGEM M1 ( ) J-PARC E15 TPC TGEM TGEM J-PARC E15 K K-pp Missing mass Invariant mass K - 3 He Formation K - pp cluster neutron Mode to decay charged particles p Λ π - Decay p Decay

More information

元素分析

元素分析 : このマークが付してある著作物は 第三者が有する著作物ですので 同著作物の再使用 同著作物の二次的著作物の創作等については 著作権者より直接使用許諾を得る必要があります (PET) 1 18 1 18 H 2 13 14 15 16 17 He 1 2 Li Be B C N O F Ne 3 4 5 6 7 8 9 10 Na Mg 3 4 5 6 7 8 9 10 11 12 Al Si P

More information

http://www.ike-dyn.ritsumei.ac.jp/ hyoo/wave.html 1 1, 5 3 1.1 1..................................... 3 1.2 5.1................................... 4 1.3.......................... 5 1.4 5.2, 5.3....................

More information

untitled

untitled MPPC 18 2 16 MPPC(Multi Pixel Photon Counter), MPPC T2K MPPC T2K (HPK) CPTA, MPPC T2K p,π T2K > 5 10 5 < 1MHz > 15% 200p.e. MIP 5p.e. p/π MPPC HPK MPPC 2 1 MPPC 5 1.1...................................

More information

ohpr.dvi

ohpr.dvi 2003-08-04 1984 VP-1001 CPU, 250 MFLOPS, 128 MB 2004ASCI Purple (LLNL)64 CPU 197, 100 TFLOPS, 50 TB, 4.5 MW PC 2 CPU 16, 4 GFLOPS, 32 GB, 3.2 kw 20028 CPU 640, 40 TFLOPS, 10 TB, 10 MW (ASCI: Accelerated

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

ファインフレックス ルビール

ファインフレックス ルビール 1 2 3 1300 1300 4 1300 1300-5 - 6 7 8 9 10 11 12 15 16 17 18 19 20 21 22 23 24 25 26 27 -N -Z -Z -Z -Z -T TM TM TM D TM H RF H RF LD LD RF MD MD UD HD RF RF RF H H RM 1 TOMBO No. 5100/5200/5300 JIS A /

More information

Drift Chamber

Drift Chamber Quench Gas Drift Chamber 23 25 1 2 5 2.1 Drift Chamber.............................................. 5 2.2.............................................. 6 2.2.1..............................................

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

( ) ,

( ) , II 2007 4 0. 0 1 0 2 ( ) 0 3 1 2 3 4, - 5 6 7 1 1 1 1 1) 2) 3) 4) ( ) () H 2.79 10 10 He 2.72 10 9 C 1.01 10 7 N 3.13 10 6 O 2.38 10 7 Ne 3.44 10 6 Mg 1.076 10 6 Si 1 10 6 S 5.15 10 5 Ar 1.01 10 5 Fe 9.00

More information

Bethe-Bloch Bethe-Bloch (stopping range) Bethe-Bloch FNAL (Fermi National Accelerator Laboratory) - (SciBooNE ) SciBooNE Bethe-Bloch FNAL - (SciBooNE

Bethe-Bloch Bethe-Bloch (stopping range) Bethe-Bloch FNAL (Fermi National Accelerator Laboratory) - (SciBooNE ) SciBooNE Bethe-Bloch FNAL - (SciBooNE 21 2 27 Bethe-Bloch Bethe-Bloch (stopping range) Bethe-Bloch FNAL (Fermi National Accelerator Laboratory) - (SciBooNE ) SciBooNE Bethe-Bloch FNAL - (SciBooNE ) Bethe-Bloch 1 0.1..............................

More information

修士論文

修士論文 SAW 14 2 M3622 i 1 1 1-1 1 1-2 2 1-3 2 2 3 2-1 3 2-2 5 2-3 7 2-3-1 7 2-3-2 2-3-3 SAW 12 3 13 3-1 13 3-2 14 4 SAW 19 4-1 19 4-2 21 4-2-1 21 4-2-2 22 4-3 24 4-4 35 5 SAW 36 5-1 Wedge 36 5-1-1 SAW 36 5-1-2

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

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

0.1 IEC 60598 1,000 IEC 60598-2 1,000V CIE 11.2 IEC 60598-2 IEC 60598-1 - 1 - IEC IEC 0.2 IEC 60598-1 IEC 60598-1 IEC ISO IEC 60061-2 IEC 60061-3 IEC 60065 1969 1995 1969 1995 1985 IEC 60068-2-63 1991

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

Note.tex 2008/09/19( )

Note.tex 2008/09/19( ) 1 20 9 19 2 1 5 1.1........................ 5 1.2............................. 8 2 9 2.1............................. 9 2.2.............................. 10 3 13 3.1.............................. 13 3.2..................................

More information

PS2701-1, PS2701-2, PS DS

PS2701-1, PS2701-2, PS DS Photocoupler SOP NEPOC PS2701-1, PS2701-2, PS2701-4 GaAs LED IC BV = 3 7 Vr.m.s. SOP tr = 3 µs TYP., tf = 5 µs TYP. 1 PS2701-1-E3, E4, F3, F4 UL No. E72422 (S) VDE0884 IC PS2701-1 4 SOP PS2701-2 8 SOP

More information

OPA134/2134/4134('98.03)

OPA134/2134/4134('98.03) OPA OPA OPA OPA OPA OPA OPA OPA OPA TM µ Ω ± ± ± ± + OPA OPA OPA Offset Trim Offset Trim Out A V+ Out A Out D In +In V+ Output In A +In A A B Out B In B In A +In A A D In D +In D V NC V +In B V+ V +In

More information

untitled

untitled --- = ---- 16 Z 8 0 8 8 0 Big Bang 8 8 s-process 50 r-process 8 50 N r-process s-process Hydrogen 71% Helium 8% Others 1.9% Heay 4-4% lements(>ni p-process (γ process? r-process s-process Big Bang H,He

More information

dr-timing-furukawa4.pptx[読み取り専用]

dr-timing-furukawa4.pptx[読み取り専用] < kazuro.furukawa @ kek.jp > 1 2 Remote controlled automatic pattern arbitrator" Manual pattern generator" Recent typical operation. ~37Hz for KEKB LER (3.5GeV e+) ~12.5Hz for KEKB HER (8GeV e ) ~0.5Hz

More information

09_organal2

09_organal2 4. (1) (a) I = 1/2 (I = 1/2) I 0 p ( ), n () I = 0 (p + n) I = (1/2, 3/2, 5/2 ) p ( ), n () I = (1, 2, 3 ) (b) (m) (I = 1/2) m = +1/2, 1/2 (I = 1/2) m = +1/2, 1/2 I m = +I, +(I 1), +(I 2) (I 1), I ( )

More information

pc725v0nszxf_j

pc725v0nszxf_j PC725NSZXF PC725NSZXF PC725NSZXF PC725 DE file PC725 Date Jun. 3. 25 SHARP Corporation PC725NSZXF 2 6 5 2 3 4 Anode Cathode NC Emitter 3 4 5 Collector 6 Base PC725NSZXF PC725YSZXF.6 ±.2.2 ±.3 SHARP "S"

More information

4 2 Rutherford 89 Rydberg λ = R ( n 2 ) n 2 n = n +,n +2, n = Lyman n =2 Balmer n =3 Paschen R Rydberg R = cm 896 Zeeman Zeeman Zeeman Lorentz

4 2 Rutherford 89 Rydberg λ = R ( n 2 ) n 2 n = n +,n +2, n = Lyman n =2 Balmer n =3 Paschen R Rydberg R = cm 896 Zeeman Zeeman Zeeman Lorentz 2 Rutherford 2. Rutherford N. Bohr Rutherford 859 Kirchhoff Bunsen 86 Maxwell Maxwell 885 Balmer λ Balmer λ = 364.56 n 2 n 2 4 Lyman, Paschen 3 nm, n =3, 4, 5, 4 2 Rutherford 89 Rydberg λ = R ( n 2 ) n

More information

untitled

untitled ( ) c a sin b c b c a cos a c b c a tan b a b cos sin a c b c a ccos b csin (4) Ma k Mg a (Gal) g(98gal) (Gal) a max (K-E) kh Zck.85.6. 4 Ma g a k a g k D τ f c + σ tanφ σ 3 3 /A τ f3 S S τ A σ /A σ /A

More information

untitled

untitled N0 N8 N0 N8 N0 * 49MeV/nuceon β 0.3c γ Hgh Z Target Pb Equvaent Photon Method 0 d σ dωde σ π γ γ π E 3 γ [!! ] dnπ σ dω π γ Eγ c h C.A.Bertuan and G.Baur Phys.Rep.63,99 988. J.D. Jackson Cassca Eectrodynamcs

More information

( ), ( ), ( ) (KEK),,, (KEK) 14 10 KEK i 1 1 2 1 3 1 4 3 5 3 5.1................................................ 3 5.2............................................. 5 5.2.1..............................................

More information

Donald Carl J. Choi, β ( )

Donald Carl J. Choi, β ( ) :: α β γ 200612296 20 10 17 1 3 2 α 3 2.1................................... 3 2.2................................... 4 2.3....................................... 6 2.4.......................................

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

Electron Ion Collider と ILC-N 宮地義之 山形大学

Electron Ion Collider と ILC-N 宮地義之 山形大学 Electron Ion Collider と ILC-N 宮地義之 山形大学 ILC-N ILC-N Ee Ee == 250, 250, 500 500 GeV GeV Fixed Fixed target: target: p, p, d, d, A A 33-34 cm-2 LL ~~ 10 1033-34 cm-2 ss-1-1 s s == 22, 22, 32 32 GeV GeV

More information

i 1 40 ii Grid Dip Meter 3 10kc 1000Mc Grid Dip Meter (RF) Q Grid Dip Meter Grid Dip Meter GDM Grid Dip Meter i ii 1. Grid Dip Meter 1 1.1................... 1 1.2............... 2 1.3............... 5

More information

Microsoft Word - 章末問題

Microsoft Word - 章末問題 1906 R n m 1 = =1 1 R R= 8h ICP s p s HeNeArXe 1 ns 1 1 1 1 1 17 NaCl 1.3 nm 10nm 3s CuAuAg NaCl CaF - - HeNeAr 1.7(b) 2 2 2d = a + a = 2a d = 2a 2 1 1 N = 8 + 6 = 4 8 2 4 4 2a 3 4 π N πr 3 3 4 ρ = = =

More information

1 Visible spectroscopy for student Spectrometer and optical spectrum phys/ishikawa/class/index.html

1 Visible spectroscopy for student Spectrometer and optical spectrum   phys/ishikawa/class/index.html 1 Visible spectroscopy for student Spectrometer and optical spectrum http://www.sci.u-hyogo.ac.jp/material/photo phys/ishikawa/class/index.html 1 2 2 2 2.1................................................

More information

S I. dy fx x fx y fx + C 3 C vt dy fx 4 x, y dy yt gt + Ct + C dt v e kt xt v e kt + C k x v k + C C xt v k 3 r r + dr e kt S Sr πr dt d v } dt k e kt

S I. dy fx x fx y fx + C 3 C vt dy fx 4 x, y dy yt gt + Ct + C dt v e kt xt v e kt + C k x v k + C C xt v k 3 r r + dr e kt S Sr πr dt d v } dt k e kt S I. x yx y y, y,. F x, y, y, y,, y n http://ayapin.film.s.dendai.ac.jp/~matuda n /TeX/lecture.html PDF PS yx.................................... 3.3.................... 9.4................5..............

More information

(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

(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 1 1 1.1 1.) T D = T = D = kn 1. 1.4) F W = F = W/ = kn/ = 15 kn 1. 1.9) R = W 1 + W = 6 + 5 = 11 N. 1.9) W b W 1 a = a = W /W 1 )b = 5/6) = 5 cm 1.4 AB AC P 1, P x, y x, y y x 1.4.) P sin 6 + P 1 sin 45

More information

Gauss Gauss ɛ 0 E ds = Q (1) xy σ (x, y, z) (2) a ρ(x, y, z) = x 2 + y 2 (r, θ, φ) (1) xy A Gauss ɛ 0 E ds = ɛ 0 EA Q = ρa ɛ 0 EA = ρea E = (ρ/ɛ 0 )e

Gauss Gauss ɛ 0 E ds = Q (1) xy σ (x, y, z) (2) a ρ(x, y, z) = x 2 + y 2 (r, θ, φ) (1) xy A Gauss ɛ 0 E ds = ɛ 0 EA Q = ρa ɛ 0 EA = ρea E = (ρ/ɛ 0 )e 7 -a 7 -a February 4, 2007 1. 2. 3. 4. 1. 2. 3. 1 Gauss Gauss ɛ 0 E ds = Q (1) xy σ (x, y, z) (2) a ρ(x, y, z) = x 2 + y 2 (r, θ, φ) (1) xy A Gauss ɛ 0 E ds = ɛ 0 EA Q = ρa ɛ 0 EA = ρea E = (ρ/ɛ 0 )e z

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

PowerPoint プレゼンテーション

PowerPoint プレゼンテーション 極短周期アンジュレータの設置に最適化した小型電子蓄積リングの設計 DESIGN STUDY OF SMALL ELECTRON STORAGE RING FOR INSTALLATION OF VERY SHORT PERIOD UNDULATORS 大熊春夫 A), B), 山本樹 C), D) Haruo Ohkuma A), B), Shigeru Yamamoto C), D) A) 高輝度光科学研究センター

More information

(1)3 (2)4 (3) (1)25 8sec 1mm 25 8sec 1mm 27 64sec 1mm 29 64sec 1mm 31 (2)33 8sec 1mm 33 64

(1)3 (2)4 (3) (1)25 8sec 1mm 25 8sec 1mm 27 64sec 1mm 29 64sec 1mm 31 (2)33 8sec 1mm 33 64 1 1.1 3 (1)3 (2)4 (3)4 1.2 5 1.2.1 5 1.2.2 10 1.3 11 1.4 21 1.5 24 1.6 25 (1)25 8sec 1mm 25 8sec 1mm 27 64sec 1mm 29 64sec 1mm 31 (2)33 8sec 1mm 33 64sec 1mm 34 35 (3)36 8sec 160 36 64sec 160 37 (4)38

More information

( ) Note (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ, µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) 3 * 2) [ ] [ ] [ ] ν e ν µ ν τ e

( ) Note (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ, µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) 3 * 2) [ ] [ ] [ ] ν e ν µ ν τ e ( ) Note 3 19 12 13 8 8.1 (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ, µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) 3 * 2) [ ] [ ] [ ] ν e ν µ ν τ e µ τ, e R, µ R, τ R (1a) L ( ) ) * 3) W Z 1/2 ( - )

More information

空気の屈折率変調を光学的に検出する超指向性マイクロホン

空気の屈折率変調を光学的に検出する超指向性マイクロホン 23 2 1M36268 2 2 4 5 6 7 8 13 15 2 21 2 23 2 2 3 32 34 38 38 54 57 62 63 1-1 ( 1) ( 2) 1-1 a ( sinθ ) 2J D ( θ ) = 1 (1-1) kaka sinθ ( 3) 1-2 1 Back face hole Amplifier Diaphragm Equiphase wave surface

More information

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

( ) ( 40 )+( 60 ) Schrödinger 3. (a) (b) (c)   yoshioka/education-09.html pdf 1 2009 1 ( ) ( 40 )+( 60 ) 1 1. 2. Schrödinger 3. (a) (b) (c) http://goofy.phys.nara-wu.ac.jp/ yoshioka/education-09.html pdf 1 1. ( photon) ν λ = c ν (c = 3.0 108 /m : ) ɛ = hν (1) p = hν/c = h/λ (2) h

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

2章.doc

2章.doc C 2 H 4 N 2 O 2 LPG LIF 13 2.1 2.1.1 2.1 2.2 115mm70mm 727cm 3 Hand Pump Injector Driver Computer Constant Volume Chamber Injector Piezo-electronic transducer Fan Spark Plug Temperature Indicator C 2 H

More information

1516-機器センサ_J.indb

1516-機器センサ_J.indb 機器用センサ Grid-EYE Grid-EYE Grid-EYE Grid-EYE Grid-EYE 着座検知 扉開閉 洗濯機の水位検知 電子レンジ PS-A 微圧タイプ 水位検知 Grid-EYE 温度計測 位置検知 熱 軸GF 赤外線アレイセンサ Grid-EYE 設計 仕様について予告なく変更する場合があります ご購入及びご使用前に当社の技術仕様書などをお求め願い それらに基づいて購入及び使用していただきますようお願いします

More information

mthesis.dvi

mthesis.dvi Study of multiple electron transfer processes to Highly charged ions with microcapillary targets : 96941 2001/01/19 1 5 1.1... 5 1.2... 6 1.2.1... 6 1.2.2 Classical over barrier(cob)... 7 1.2.3... 8 1.3...

More information

B 1 B.1.......................... 1 B.1.1................. 1 B.1.2................. 2 B.2........................... 5 B.2.1.......................... 5 B.2.2.................. 6 B.2.3..................

More information

= hυ = h c λ υ λ (ev) = 1240 λ W=NE = Nhc λ W= N 2 10-16 λ / / Φe = dqe dt J/s Φ = km Φe(λ)v(λ)dλ THBV3_0101JA Qe = Φedt (W s) Q = Φdt lm s Ee = dφe ds E = dφ ds Φ Φ THBV3_0102JA Me = dφe ds M = dφ ds

More information

untitled

untitled 5522A 30 2 ( 5522A 5 10 ) tcal ±5 (tcal 5522A ) 7 5 12 Ω ±1 /... 2, 30... 5... IEEE-488(GPIB), RS-232... 0 50 (tcal)... 15 35... -20 70 ; 0 1.09999 A 1.1 A 2.99999 A 50 50 30 90 1 2... tcal +5 1 90 ( 1

More information

<90CE90EC88E290D55F955C8E862E656336>

<90CE90EC88E290D55F955C8E862E656336> 5 5 9 9 7 7 5 5 6 6 7 7 8 8 9 9 8 8 8 8 79 79 78 78 76 76 77 77 7 7 6 7 7 5 68 68 67 67 66 66 65 65 6 6 6 6 6 6 6 6 6 6 59 59 58 58 57 57 56 56 55 55 5 5 8 8 5 5 9 9 9 8 7 9 9 8 8 7 7 6 6 5 5 5 5 69 69

More information

最新耐震構造解析 ( 第 3 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 3 版 1 刷発行時のものです.

最新耐震構造解析 ( 第 3 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 3 版 1 刷発行時のものです. 最新耐震構造解析 ( 第 3 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. http://www.morikita.co.jp/books/mid/052093 このサンプルページの内容は, 第 3 版 1 刷発行時のものです. i 3 10 3 2000 2007 26 8 2 SI SI 20 1996 2000 SI 15 3 ii 1 56 6

More information

CRA3689A

CRA3689A AVIC-DRZ90 AVIC-DRZ80 2 3 4 5 66 7 88 9 10 10 10 11 12 13 14 15 1 1 0 OPEN ANGLE REMOTE WIDE SET UP AVIC-DRZ90 SOURCE OFF AV CONTROL MIC 2 16 17 1 2 0 0 1 AVIC-DRZ90 2 3 4 OPEN ANGLE REMOTE SOURCE OFF

More information