main.dvi

Size: px
Start display at page:

Download "main.dvi"

Transcription

1 CeF 3

2 KEK E391a KL 0 π0 νν E391a CeF (l =2) (l =3)

3 Data taking system(daq) Gain Run A 64 A A.2 KEK-T B 67 72

4 KEK E391a (KEK) 12GeV (KEK-PS) KL 0 π0 νν (KEK-PS E391a) 2003 KL 0 π0 νν KL K 0 L π 0 νν KL 0 π0 νν CP KL 0 CP = 1 π 0 νν π 0 νν π 0 CP = 1 νν CP =+1 νν π 0 l KL 0 0 l =1 π 0 νν CP = (+1)( 1)( 1) l=1 =+1 KL 0 π0 νν CP KL 0 π0 νν flavor GIM 1 [1] 1.1 Feynman Diagram KL 0 πνν V ij CKM [2, 3] 2 B(K 0 L π 0 νν) =6k 1 (Im(V td V ts)) 2 X 2 (x t ) k 1 = τ(k L) τ(k + ) B(K+ π 0 e + ν e ) Vus4π 2 2 sin θ W m t top quark M W W boson X(x t ) x t =(m t /M W ) 2 X(x t )= x t 8 α 2 ( xt +2 x t 1 + 3x ) t 6 (x t 1) 2 lnx t 1 Glashow-Iliopoulos-Maiani 2 Cabibbo-Kobayashi-Maskawa

5 1 4 s t W Z d s W Z d W s t d W l 1.1: Diagram of K 0 L π0 νν [4] CKM Wolfenstein parameterization[5] V ud V us V ub V CKM = V cd V cs V cb V td V ts V tb 1 λ 2 /2 λ Aλ 3 (ρ iη) λ 1 λ 2 /2 Aλ 2 Aλ 3 (1 ρ iη) Aλ 2 1 B(KL 0 π0 νν) = η 2 A 4 X 2 (x t ) η 2 A 4 xt 1.18 (m t 150GeV /c 2 ) A 1, λ 0.2, KL 0 π0 νν CP η K L 0 π0 νν E391a 12.9GeV/c EP2 4 o K0 K0 10m

6 1 5 6m 2GeV/c K 0 K 0 2mm radian Detector Detector KL 0 Barrel End-cap End-cap ( CeF 3 CsI) KL 0 π0 νν π 0 2γ 2γ End-cap 2 γ π 0 End-cap π 0 γ π 0 KL 0 π0 P T KL 0 π0 νν γ π 0 νν π 0 KL 0 π0 νν π 0 γ K 0 L γγ(b.r. = (5.92 ± 0.15) 10 4 ) K 0 L π0 π 0 (B.R. = (9.36 ± 0.20) 10 4 ) K 0 L π0 π 0 π 0 (B.R. = (2.112 ± 0.027) 10 1 ) Back ground 3 End-cap K 0 L γγ End-cap γ main 2γ reconstruct π 0 P T selection cut P T selection cut KL 0 π0 π 0 KL 0 π0 π 0 π 0 KL 0 π0 νν 1. End-cap 100MeV γ 2. P T > 120MeV/c KL 0 π0 νν [6, 7]( [8] ) E391a KL 0 Detector K0 L 3 K 0 L π 0 π 0 K 0 L π 0 π 0 π 0

7 1 6 Back ground End-cap ΔE/E =( ) 2.5 E[GeV ] E[GeV ] 2. Barrel γ inefficiency γ γ γ High rate radiation length 1980 CERN Crystal Clear Collaboration 1 E391a E391a

8 : KEK E391a

9 CERN KEK PET [9] (Radiation length) γ X 0 d Z X 0 X 0 1 d Z(Z +1) Z (NaI 100%) 4-5 (cm) 2.8 (ns) 5 fast,30 slow 1.68 (nm) 310 fast,340 slow (%/ ) 0.05 (dyn/cm 2 ) (g/cm 3 ) 6.16 (dyn/cm 2 ) (cm) 1.7 (/ ) : 1 Positron Emission Tomography %

10 : (nm) (%) ( 1.5) NaI CsI ( / ) ( / )

11 γ [11][13] ( 1.5) NaI CsI(pure) Z γ 2.2 [10][12]

12 2 11 CeF 3 BaF 2 BGO CsF CsI(pure) PWO NaI(Tl) GSO (g/cm 3 ) Radiation length(cm) Dacay time(ns) short , long > [ms] Emission peak(nm) short long > Light yield NaI(Tl) Radiation hardness(rad) >10 8 quartz slow cost UV-glass slow cost PMT PMT slow comp slow comp 2.2:

13 CeF 3 CeF ( ) Ce 5d 4f 4 Ce 3+ γ (STE) 2.2 (1) (2) Ce 3+ (3) [11][16] Conduction Band 5d(Ce) photon photon photon (1) (2) (3) 4f(Ce) Valence Band 2p(F) Core Level 5p(Ce) excitation transitions emission transitions non-radiative transitions 2.2: CeF 3 4 V k F V k F

14 KEK-E391a collaboration 2.3 No.1 (004) No.2 No1 No.2 No.3 (300) ( ) 2.3: No1 No3 13%

15 2 14 KEK E391a 5 ( ) ( ) : KEK OKEN CERN Crystal clear collaboration KEK E391a Crystal Clear Collaboration E391a [10] 5 Bridgeman-stockberger

16 rad KEK E391a KEK E391a E391a CeF 3 CsI(pure) BaF 2 BGO NaI(Tl) : rad rad Co γ rad hr rad 1.06 sec 10 3 rad 10.6 sec 10 4 rad sec 10 5 rad sec 10 6 rad sec

17 : 220

18 : 3.3: γ

19 φ 15mm u : 3.4 : : d u : 3.6 : : d u : 3.8 : CF034 : d : 6 60 Co 10 3 rad 10 6 rad rad rad 10 4 rad 1 2

20 : u 10 X rad X 3.5: d

21 : u 10 X rad X 3.7: d

22 : u 10 X rad X 3.9: d

23 ( 3.4,3.5) ( 3.8,3.9) ( ) 10 6 rad 14-15% CF % 2.4 [10] u 10 6 rad 500nm 15% 310,340nm 10% 10 6 rad

24 CERN Crystal Clear Collaboration 5ns 30ns [9, 12, 14, 15, 16] KEK Private communication 200ns 310nm 340nm 480nm KEK E391a KEK E391a nm d 310nm 5 10% u (0.02%) d u d 4.1: SPC

25 : Sample ( ) 270nm [17] 60 Co 60 Co 1.173MeV 1.33MeV 2 γ γ γ 1 CAMAC TDC 1 1 TDC : Time to Digital Converter CAMAC start pulse stop pulse 500ns 150μsec clear 3μsec

26 : Start counter (HAMAMATSU H2431 A.1 ) 2.5cm 60 Co Start counter (OKEN 6262A ) 5mm Start counter TDC Stop counter (HAMAMATSU H1161 A.1 ) 60 Co β γ

27 cm Stop counter 60 Co γ Start counter 3000V Stop counter 2400V AVR 2 3m BNC ( B) Stop counter 4.5 Logic 4.3 Start counter Stop counter Divider START COUNTER H2431 DIV Delay CLOCK DISC DISC GDG GDG Delay COIN 1 DISC F i/o GDG COIN TDC 1 TDC 2 START CLEAR ADC 1 GATE CLEAR ADC 2 GATE CLEAR STOP COUNTER H1161 DIV COIN 2 GDG GDG INT REG COIN SCALER Delay DISC GDG Delay OUT REG 4.3: 2 1 Delay ADC 2 Stop counter ADC Discriminator Start counter 2 ADC : Analogue to Digital Converter Start counter ADC 100μsec clear 3μsec Stop counter Lecroy (2249A) 150μsec clear 3μsec

28 mV Stop counter Discriminator 10mV Discriminator Coin 1 Start PMT Stop PMT 430ns Coin 2 Start PMT 400ns Stop PMT 4.4: Coincidence 2 GDG coincidence TDC Start Stop coincidence coincidence Start Stop 1 coincidence 4.3 Start Stop coincidence Coin1 latch GDG OR (F i/o) latch Coin1 veto OR Start counter ADC TDC GDG ADC Interrupt register Interrupt register LAM(look at me) ADC TDC output register ADC TDC clear latch Interrupt register 500μsec output register latch 3 GDG : Gate Delay Generator NIM

29 4 28 5μsec ADC TDC clear Coin2 Stop counter ADC Coin1 latch Coin2 veto Coin1 Coin1 Start counter Stop counter Stop counter Coin2 Stop counter 4.5 Start ADC Stop ADC 2 ADC Start stop 260nsec

30 4 29 H photon histgram 4.5: Stop counter(h1161) ADC

31 [17] F (t) = l a j exp( t/τ j )+bkg (4.1) j=1 a j t 4 τ j bkg l 2 3 l =2 l =3 3 TDC TDC 200 (4.1) bkg (l =2) CERN Crystal clear collaboration Decay time ( ) 3 5ns 30ns E391a 324ch 1200ch 114ns ch N TDC 1ch 129.5psec (ns) (ns) χ 2 /ndf d 3.85± ± u 2.35± ± d 3.17± ± u 3.02± ± : 4 TDC 5 CERN PAW

32 4 31 TDC 2ch d TDC 2ch u TDC 2ch d TDC 2ch u 4.6: 2

33 4 32 H1161 ( ) (4.1) F (t) a1 exp( t/τ 1 ) dt F (t) dt 100(%) d d 310nm d 5 10% 2.4 (%) (%) d( ) u( ) d( ) u( ) : (l =3) 30ns 2 345ns 2 (4.1) (l =3) TDC ch( 345ns) (4.1) i 4.5 ai exp( t/τ i ) dt F (t) dt 100(%) 6 (p.37)

34 (ns) 2 (ns) 3 (ns) χ 2 /ndf d 3.37± ± ± u 2.15± ± ± d 2.81± ± ± u 2.69± ± ± : 1 (%) 2 (%) 3 (%) d( ) u( ) d( ) u( ) : nm nm nm A.J. Wojtowicz [21] 310nm 340nm 370nm 50ns (ns) (ns) χ 2 /ndf 340nm (μs) nm : 2

35 4 34 TDC 2ch d TDC 2ch u TDC 2ch d TDC 2ch u 4.7:

36 4 35 filter none filter 300nm filter 340nm filter 370nm 4.8:

37 4 36 TDC 2ch S76-UV34(340nm) TDC 2ch S76-L37(370nm) 4.9:

38 ns 2 30ns CERN Stop counter 1ns ns 1ns % KEK private communication ns 2 χ TDC 340ns μs χ 2 (2 ) χ 2 (3 ) d u d u : χ 2 340nm 18μs 370nm 622ns τ 340nm 30ns 10% Stop counter

39 d % 6.7% E391a KL 0 480kHz[18]

40 [19, 20] (KEK) T1 0.4GeV/c 2.0GeV/c ( π ) : T1

41 KEK T1 12GeV 23 o (Q) (D) Q-Q-D-D 2.0GeV/c e + π + π 5.1 D : TOF 1 3.8m 2GeV/c TOF 20 β> P electron > 17.84MeV/c π P π > 4.87GeV/c T1 2GeV/c TOF TOF 1 Time Of Flight

42 mm 1spill CeF PHOTONIS XP2978( A.2) 200nm fused silica (KE-103 ) nm 80% 5.3: mm GeV 1spill

43 : No5 5.5: (nm) (%) ) 3 330mm 19.5X 0 100% 80 TSE3033( ) 9 π ( ) HV BNC 15m

44 Logic 5.6 S1 S TOF start counter(right) TOF start counter(left) Trigger counter 1 TOF stop counter(right) TOF stop counter(left) Trigger counter 2 Trigger counter 3 Cerenkov counter 1 Cerenkov counter 2 S1R S1L S2 S3R S3L S4 S5 C1 C2 Divider 2 ADC Discriminator TOF Discriminator Mean timer 3 3dB 2 Cerenkov counter(c1 C2) (0.5 2GeV/C) C1 C2 C1 C2 π C1 C2 TOF Start counter S1 TOF Stop counter(s2) TOF π NIM

45 5 44 CeF3 1 Delay CeF3 2 Delay CeF3 3 Delay CeF3 4 Delay CeF3 5 Delay CeF3 6 Delay CeF3 7 Delay CeF3 8 Delay CeF3 9 Delay S3L Clock Mean timer S3R Hadron trigger ADC gate width:220ns S2 S4 S5 veto Switch A B C Master trigger veto TDC gate Interrupt register C1 start LATCH stop C2 Electron trigger Out put register S1L Mean timer S1R 5.6: TDC

46 5 45 TDC 5.7: TDC 1.5GeV/c π +

47 Data taking system(daq) CAMAC Linux PC [24] TOF 9 ADC TDC 18ch 36ch veto 96ch GeV/c π 300mm S mm S5 π MIP 4 3 deposit No.5 Gain 8 Gain 9 calibration 5.9 ADC Run 300mm PMT PMT PMT 5.8: 4 Minimum Ionizing Particle.

48 5 47 CeF3 9 CeF3 8 CeF3 7 CeF3 6 CeF3 5 CeF3 4 CeF3 3 CeF3 2 CeF : ADC deposit energy Gaussian fit No.5 8 mean No.5 mean (C i ) Gain PMT No. C i PMT No. C i PMT No. C i :

49 5 48 CeF3 9 CeF3 8 CeF3 7 CeF3 6 CeF3 5 CeF3 4 CeF3 3 CeF3 2 CeF :

50 Gain Gain (Gain) A No.5 No.5 KEK 1120V N 5.11 NIM clock generator TTL (width 25ns) clock generator NIM GDG qvt qvt qvt 1ch pC( ) rate 2 HV Filter Signal Out PMT 5.11: (1120V) 5.12 (LED) LED μ σ N

51 : Gauss fit mean 99ch 252.6ch σ E = σ N = 1 (5.1) N N p.e. = 1 ( σ E )2 (5.2) 5.12 N σ (ch) mean 252.6(ch) E =( ) ( ) (E) 153.6ch 38.66pC N (5.2) N p.e =( )2 = (p.e) e = = 38.66pC = e

52 V 1200V Gain Gain 5.13 (V) Gain G(V ) G(V )= V 4.42 (5.3) Gain (1300V) (1120V) ±5.7% 1120V Gain Gain curve % Gain Gain curve

53 : CeF 3 No.5 Gain 5.14: (V)

54 Run 0.5GeV/c 1GeV/c 1.5GeV/c (Linearity) 3. 2GeV/c 10spill 1 (GeV/c) /spill 1.0 1/spill /spill 2.0 <0.1/spill 1GeV/c ADC ADC-2 ADC-4 6 S E = 9 C i (ADC i P i ) i=1 C i Gain 5.1 ADC i i ADC P i ADC GeV/c 9

55 5 54 ADC-9 ADC-8 ADC-7 ADC-6 ADC-5 ADC-4 ADC-3 ADC-2 ADC : 1GeV/c ADC 5.3 deposit ADC ADC Gauss fit m σ f(x) = 1 ( ) (x m) 2 exp 2πσ 2σ 2 (5.4) 5.17 σ E = a E(GeV ) + b (5.5)

56 5 55 a b σ E = (3.7 ± 0.3) 102 E(GeV ) + (6.3 ± 31.0) 10 4 (5.6)

57 5 56 SUM 5.16: GeV/c ADC

58 5 57 Energy resolution Injection Energy(GeV) 5.17: (GeV)

59 5 58 Linearity 2.2 ADC 5.18 ADC ADC σ ADC channel Injection energy(gev) 5.18: CeF 3 (GeV) ADC

60 Gain (5.3) 1120V ADC 1ch 0.263pC 3. ADC channel q 4. q PMT Gain q 5. N p.e. q / e Attenuator 3dB db = 20 ln V out V in (5.7) V in = e 3 20 Vout =1.162 V out ADC ADC 1.16 Divider 2 ADC MeV N p.e. = x (GeV) (5.8) 1MeV 970

61 5 60 Np.e Injection energy(gev) 5.19: (GeV)

62 GeV/c 1.0GeV/c 1.5GeV/c E391a deposit 1MeV 970 σ E = (3.7 ± 0.3) 102 E(GeV ) + (6.3 ± 31.0)

63 Co γ 10 6 rad 10 6 rad 10% 6.2 3ns 30ns 340nm 30ns 6.3 π E σ = (3.7±0.3) 102 +(6.3±31.0) 10 4 E(GeV )

64 6 63 deposit 1MeV ns TDC

65 64 A A.1 H2431 H nm 10% 25% H V H V [22] H2431 TOF(Time of flight) start trigger A.1 Rise Transit T.T.S. Tube Time Time Typ. Name Typ. Typ. FWHM (ns) (ns) (ns) H H A.1: H1161 stop trigger 1.1ns 1 1ns H1161 A.1 A.2 KEK-T466 PHOTONIS ( PHILIPS) XP2978 factor ( ) A.2

66 A 65 A.1: (ma/w) 1 1/8 fused silica 1800V 1.9ns A.2: XP2978

67 A 66 A.2 [23] (%) = 124 (ma/w ) λ(nm) A nm 0.83% 22.0% (310nm 20% 340nm 22%) A.2: (ma/w)

68 67 B slow ( ) S76-UV30 S76-UV30 S76-UV34 S76-L37 S76-L39 S76-L42 300nm, 340nm, 370nm, 390nm, 420nm B.1: S76-UV30

69 B 68 B.2: S76-UV34 B.3: S76-l37

70 B 69 B.4: S76-l39 B.5: S76-l42

71 70 [1] S.L. Glashow and J. Iliopoulos and L. Maiani, Phys. Rev. D2,1285(1970) [2] N. Cabibbo, Phys. Rev. Lett. 10,531 [3] M. Kobayashi and T. Maskawa, Prog. Theor. Phys. 49,652(1973) [4] T. Inami and C.S. Lim, Prog. Theor. Phys 65,297(1981), 65,1772(1981) [5] L. Wolfenstein, Phys. Rev. Lett. 51,1945(1983) [6] W.J. Marciano and Z. Parsa, Phys. Rev. D53, R1(1996) [7] G. Buchalla and A.J. Buras, Phys. Rev. D54, 6782(1996) [8] A. Alavi-Harati et al., Phys. Rev. D61, (2000) [9] D.F. Anderson, FERMILAB-Pub (1989) 169 [10] Proceedings of the Workshop on Scintillating Crystals(KEK,1997) [11] CeF 3 (2000) [12] D.F. Anderson, Nucl. and Meth A287 (1990) [13] F. ( ) ( 1991) [14] T.Inagaki, et al., Nucl. Instr. and Meth A443 (2000) [15] IEEE Transactions on Nuclear Science, Vol.36, No.1 (1989) [16] E. Auffray,et al., Nucl. Instr. and Meth A383 (1996) [17] D.V.O Connor, D. Phillips ( 1988) [18] T. Inagaki et al, KEK Internal Proposal of an Experiment at the KEK 12GeV Proton Synchrotron Measurement of the K 0 L π0 νν

72 B 71 [19] E. Auffray, et al., CERN-PPE (1994) [20] E. Auffray, et al., CERN-PPE (1995) [21] IEEE Transactions on Nuclear Science, Vol.39, No.4 (1992) [22] (1998) [23] PHOTONIS PMT Catalogue(1999), Photomultiplier tubes [24] 8GeV (1999)

73 72 M1 4

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

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

2005 4 18 3 31 1 1 8 1.1.................................. 8 1.2............................... 8 1.3.......................... 8 1.4.............................. 9 1.5.............................. 9

More information

25 3 4

25 3 4 25 3 4 1 µ e + ν e +ν µ µ + e + +ν e + ν µ e e + TAC START STOP START veto START (2.04 ± 0.18)µs 1/2 STOP (2.09 ± 0.11)µs 1/8 G F /( c) 3 (1.21±0.09) 5 /GeV 2 (1.19±0.05) 5 /GeV 2 Weinberg θ W sin θ W

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

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

Muon Muon Muon lif

Muon Muon Muon lif 2005 2005 3 23 1 2 2 2 2.1 Muon.......................................... 2 2.2 Muon........................... 2 2.3................................. 3 2.4 Muon life time.........................................

More information

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

1 1 (proton, p) (neutron, n) (uud), (udd) u ( ) d ( ) u d ( ) 1: 2: /2 1 0 ( ) ( 2) 0 (γ) 0 (g) ( fm) W Z 0 0 β( )

1 1 (proton, p) (neutron, n) (uud), (udd) u ( ) d ( ) u d ( ) 1: 2: /2 1 0 ( ) ( 2) 0 (γ) 0 (g) ( fm) W Z 0 0 β( ) ( ) TA 2234 oda@phys.kyushu-u.ac.jp TA (M1) 2161 sumi@epp.phys.kyushu-u.ac.jp TA (M1) 2161 takada@epp.phys.kyushu-u.ac.jp TA (M1) 2254 tanaka@epp.phys.kyushu-u.ac.jp µ ( ) 1 2 1.1...............................................

More information

[ ] [ ] [ ] [ ] [ ] [ ] ADC

[ ] [ ] [ ] [ ] [ ] [ ] ADC [ ] [ ] [ ] [ ] [ ] [ ] ADC BS1 m1 PMT m2 BS2 PMT1 PMT ADC PMT2 α PMT α α = n ω n n Pn TMath::Poisson(x,[0]) 0.35 0.3 0.25 0.2 0.15 λ 1.5 ω n 2 = ( α 2 ) n n! e α 2 α 2 = λ = λn n! e λ Poisson Pn 0.1

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

24 10 10 1 2 1.1............................ 2 2 3 3 8 3.1............................ 8 3.2............................ 8 3.3.............................. 11 3.4........................ 12 3.5.........................

More information

thesis.dvi

thesis.dvi 3 17 03SA210A 2005 3 1 introduction 1 1.1 Positronium............ 1 1.2 Positronium....................... 4 1.2.1 moderation....................... 5 1.2.2..................... 6 1.2.3...................

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

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

1/2 ( ) 1 * 1 2/3 *2 up charm top -1/3 down strange bottom 6 (ν e, ν µ, ν τ ) -1 (e) (µ) (τ) 6 ( 2 ) 6 6 I II III u d ν e e c s ν µ µ t b ν τ τ (2a) (

1/2 ( ) 1 * 1 2/3 *2 up charm top -1/3 down strange bottom 6 (ν e, ν µ, ν τ ) -1 (e) (µ) (τ) 6 ( 2 ) 6 6 I II III u d ν e e c s ν µ µ t b ν τ τ (2a) ( August 26, 2005 1 1 1.1...................................... 1 1.2......................... 4 1.3....................... 5 1.4.............. 7 1.5.................... 8 1.6 GIM..........................

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

29 1 29 1 K O TO (J-PARC E14 ) BHCV K O TO J-PARC K L π ν ν BHCV BHCV K L π ν ν BHCV 99.5% BHCV CF 4 MWPC BHCV 99.8% BHCV 2 1 K O TO 4 1.1........................................ 4 1.2 K L π ν ν................................

More information

PET. PET, PET., PET 1, TPC 3.,. TPC,,.

PET. PET, PET., PET 1, TPC 3.,. TPC,,. PET TPC 21 2 9 PET. PET, PET., PET 1, TPC 3.,. TPC,,. 1 6 2 PET 7 2.1........................... 7 2.1.1 PET..................... 7 2.1.2.......................... 10 2.2..............................

More information

1 3 1.1 PET..................................... 3 1.1.1......................................... 3 1.1.2 PET................................. 4 1.2..

1 3 1.1 PET..................................... 3 1.1.1......................................... 3 1.1.2 PET................................. 4 1.2.. 21 PET 06S2037G 2010 3 1 3 1.1 PET..................................... 3 1.1.1......................................... 3 1.1.2 PET................................. 4 1.2........................................

More information

,,..,. 1

,,..,. 1 016 9 3 6 0 016 1 0 1 10 1 1 17 1..,,..,. 1 1 c = h = G = ε 0 = 1. 1.1 L L T V 1.1. T, V. d dt L q i L q i = 0 1.. q i t L q i, q i, t L ϕ, ϕ, x µ x µ 1.3. ϕ x µ, L. S, L, L S = Ld 4 x 1.4 = Ld 3 xdt 1.5

More information

SPECT(Single Photon Emission Computer Tomography ) SPECT FWHM 3 4mm [] MPPC SPECT MPPC LSO 6mm 67.5 photo electron 78% kev γ 4.6 photo electron SPECT

SPECT(Single Photon Emission Computer Tomography ) SPECT FWHM 3 4mm [] MPPC SPECT MPPC LSO 6mm 67.5 photo electron 78% kev γ 4.6 photo electron SPECT 3 SPECT SJ SPECT(Single Photon Emission Computer Tomography ) SPECT FWHM 3 4mm [] MPPC SPECT MPPC LSO 6mm 67.5 photo electron 78% kev γ 4.6 photo electron SPECT 9ch MPPC array 3 3 9 3 3 9.mm(sigma) . SPECT..................................................................3............

More information

soturon.dvi

soturon.dvi Stopped Muon 94S2003J 11 3 10 1 2 2 3 2.1 Muon : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 3 2.2 : : : : : : : : 4 2.3 : : : : : : : : : : : : : 6 3 7 3.1 : : : : : : : : : : : : : : : :

More information

CdTe γ 02cb059e :

CdTe γ 02cb059e : CdTe γ 02cb059e : 2006 5 2 i 1 1 1.1............................................ 1 1.2............................................. 2 1.3............................................. 2 2 3 2.1....................................

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

2004 A1 10 4 1 2 2 3 2.1................................................ 3 2.2............................................. 4 2.3.................................................. 5 2.3.1.......................

More information

nenmatsu5c19_web.key

nenmatsu5c19_web.key KL π ± e νe + e - (Ke3ee) Ke3ee ν e + e - Ke3 K 0 γ e + π - Ke3 KL ; 40.67(%) Ke3ee K 0 ν γ e + π - Ke3 KL ; 40.67(%) Me + e - 10 4 10 3 10 2 : MC Ke3γ : data K L real γ e detector matter e e 10 1 0 0.02

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

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

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 ±

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 ± 7 7. ( ) SU() SU() 9 ( MeV) p 98.8 π + π 0 n 99.57 9.57 97.4 497.70 δm m 0.4%.% 0.% 0.8% π 9.57 4.96 Σ + Σ 0 Σ 89.6 9.46 K + K 0 49.67 (7.) p p = αp + βn, n n = γp + δn (7.a) [ ] p ψ ψ = Uψ, U = n [ α

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

π + e + ν e

π + e + ν e π + e + ν e 2 2013 2 5 π + e + ν e π + µ + ν µ R = Γ(π + e + ν e )/Γ(π + µ + ν µ ) 0.1% PIENU 2009 TRIUMF R 0.01% 10 R 0.1% 1000TeV PIENU 0.1% 1980 TRIUMF π + e + ν e π + µ + ν µ KEK COPPER 500MHz Flash

More information

LLG-R8.Nisus.pdf

LLG-R8.Nisus.pdf d M d t = γ M H + α M d M d t M γ [ 1/ ( Oe sec) ] α γ γ = gµ B h g g µ B h / π γ g = γ = 1.76 10 [ 7 1/ ( Oe sec) ] α α = λ γ λ λ λ α γ α α H α = γ H ω ω H α α H K K H K / M 1 1 > 0 α 1 M > 0 γ α γ =

More information

LHC ALICE (QGP) QGP QGP QGP QGP ω ϕ J/ψ ALICE s = ev + J/ψ

LHC ALICE (QGP) QGP QGP QGP QGP ω ϕ J/ψ ALICE s = ev + J/ψ 8 + J/ψ ALICE B597 : : : 9 LHC ALICE (QGP) QGP QGP QGP QGP ω ϕ J/ψ ALICE s = ev + J/ψ 6..................................... 6. (QGP)..................... 6.................................... 6.4..............................

More information

3 1 4 1.1......................... 4 1.1.1....................... 4 1.1.2.................. 4 1.1.3 Coulomb potential.............. 5 1.2.............

3 1 4 1.1......................... 4 1.1.1....................... 4 1.1.2.................. 4 1.1.3 Coulomb potential.............. 5 1.2............. Fe muonic atom X 25 5 21 3 1 4 1.1......................... 4 1.1.1....................... 4 1.1.2.................. 4 1.1.3 Coulomb potential.............. 5 1.2.......................... 6 1.2.1...................

More information

untitled

untitled masato@icrr.u-tokyo.ac.jp 996 Start 997 998 999 000 00 00 003 004 005 006 007 008 SK-I Accident Partial Reconstruction SK-II Full reconstruction ( SK-III ( ),46 (40%) 5,8 (9%),9 (40%) 5MeV 7MeV 4MeV(plan)

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

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

3-2 PET ( : CYRIC ) ( 0 ) (3-1 ) PET PET [min] 11 C 13 N 15 O 18 F 68 Ga [MeV] [mm] [MeV]

3-2 PET ( : CYRIC ) ( 0 ) (3-1 ) PET PET [min] 11 C 13 N 15 O 18 F 68 Ga [MeV] [mm] [MeV] 3 PET 3-1 PET 3-1-1 PET PET 1-1 X CT MRI(Magnetic Resonance Imaging) X CT MRI PET 3-1 PET [1] H1 D2 11 C-doxepin 11 C-raclopride PET H1 D2 3-2 PET 0 0 H1 D2 3-1 PET 3-2 PET ( : CYRIC ) ( 0 ) 3-1-2 (3-1

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

1 12 CP 12.1 SU(2) U(1) U(1) W ±,Z [ ] [ ] [ ] u c t d s b [ ] [ ] [ ] ν e ν µ ν τ e µ τ (12.1a) (12.1b) u d u d +W u s +W s u (udd) (Λ = uds)

1 12 CP 12.1 SU(2) U(1) U(1) W ±,Z [ ] [ ] [ ] u c t d s b [ ] [ ] [ ] ν e ν µ ν τ e µ τ (12.1a) (12.1b) u d u d +W u s +W s u (udd) (Λ = uds) 1 1 CP 1.1 SU() U(1) U(1) W ±,Z 1 [ ] [ ] [ ] u c t d s b [ ] [ ] [ ] ν e ν µ ν τ e µ τ (1.1a) (1.1b) u d u d +W u s +W s u (udd) (Λ = uds) n + e + ν e d u +W u + e + ν e (1.a) Λ + e + ν e s u +W u + e

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

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

miyazaki_mthesis.pdf

miyazaki_mthesis.pdf 23 1 25 i,. 2,.. 1, 5σ, 60%.,.,. ii,.,...,..,..,,,..,. pick-off,,.,...,.,..,,, Khaw K. Siang,,,,,..,,,,,,,,..,... iii ii 1 1 1.1... 1 1.2... 2 1.3... 4 1.4... 7 1.4.1... 7 1.4.2... 8 1.5... 11 1.5.1...

More information

main.dvi

main.dvi SGC - 48 208X Y Z Z 2006 1930 β Z 2006! 1 2 3 Z 1930 SGC -12, 2001 5 6 http://www.saiensu.co.jp/support.htm http://www.shinshu-u.ac.jp/ haru/ xy.z :-P 3 4 2006 3 ii 1 1 1.1... 1 1.2 1930... 1 1.3 1930...

More information

- γ 1929 γ - SI γ 137 Cs 662 kev γ NaI active target NaI γ NaI 2 NaI γ NaI(Tl) γ 2 NaI γ γ γ

- γ 1929 γ - SI γ 137 Cs 662 kev γ NaI active target NaI γ NaI 2 NaI γ NaI(Tl) γ 2 NaI γ γ γ - 28 2 15 - γ 1929 γ - SI γ 137 Cs 662 kev γ NaI active target NaI γ NaI 2 NaI γ NaI(Tl) γ 2 NaI γ γ 10 3 4 γ 1 3 2 γ 5 2.1..................................... 5 2.1.1.................... 5 2.1.2..............................

More information

LEPS

LEPS LEPS2 2016 2 17 LEPS2 SPring-8 γ 3 GeV γ 10 Mcps LEPS2 7 120 LEPS Λ(1405) LEPS2 LEPS2 Silicon Strip Detector (SSD) SSD 100 µm 512 ch 6 cm 3 x y 2 SSD 6 3072 ch APV25-s1 APVDAQ VME APV25-s1 SSD 128 ch

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

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

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

pdf

pdf http://www.ns.kogakuin.ac.jp/~ft13389/lecture/physics1a2b/ pdf I 1 1 1.1 ( ) 1. 30 m µm 2. 20 cm km 3. 10 m 2 cm 2 4. 5 cm 3 km 3 5. 1 6. 1 7. 1 1.2 ( ) 1. 1 m + 10 cm 2. 1 hr + 6400 sec 3. 3.0 10 5 kg

More information

500 6 LHC ALICE ( 25 ) µsec MeV QGP

500 6 LHC ALICE ( 25 ) µsec MeV QGP 5 6 LHC ALICE shigaki@hiroshima-u.ac.jp chujo.tatsuya.fw@u.tsukuba.ac.jp gunji@cns.s.u-tokyo.ac.jp 3 ( 5 ) 5. µsec MeV QGP 98 RHIC QGP CERN LHC. LHC ALICE LHC p+p RHIC QGP ALICE 3 5 36 3, [, ] ALICE [,

More information

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 (

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 ( 9 1. (Ti:Al 2 O 3 ) (DCM) (Cr:Al 2 O 3 ) (Cr:BeAl 2 O 4 ) 2. 2.1 Ĥ ψ n (r) ω n Schrödinger Ĥ ψ n (r) = ω n ψ n (r), (1) ω i ψ (r, t) = [Ĥ + Ĥint (t)] ψ (r, t), (2) Ĥ int (t) = eˆxe cos ωt ˆdE cos ωt, (3)

More information

untitled

untitled BELLE B J/ψ + K 12 1 1 2 BELLE 3 2.1 BELLE... 3 2.1.1 CP... 3 2.1.2 CKM... 4 2.1.3... 6 2.1.4 B CP... 8 2.2 KEKB... 13 2.3 BELLE... 16 2.3.1 SVD... 19 2.3.2 CDC.................. 2 2.3.3 ACC... 21 2.3.4

More information

Sample function Re random process Flutter, Galloping, etc. ensemble (mean value) N 1 µ = lim xk( t1) N k = 1 N autocorrelation function N 1 R( t1, t1

Sample function Re random process Flutter, Galloping, etc. ensemble (mean value) N 1 µ = lim xk( t1) N k = 1 N autocorrelation function N 1 R( t1, t1 Sample function Re random process Flutter, Galloping, etc. ensemble (mean value) µ = lim xk( k = autocorrelation function R( t, t + τ) = lim ( ) ( + τ) xk t xk t k = V p o o R p o, o V S M R realization

More information

( ) ) ) ) 5) 1 J = σe 2 6) ) 9) 1955 Statistical-Mechanical Theory of Irreversible Processes )

( ) ) ) ) 5) 1 J = σe 2 6) ) 9) 1955 Statistical-Mechanical Theory of Irreversible Processes ) ( 3 7 4 ) 2 2 ) 8 2 954 2) 955 3) 5) J = σe 2 6) 955 7) 9) 955 Statistical-Mechanical Theory of Irreversible Processes 957 ) 3 4 2 A B H (t) = Ae iωt B(t) = B(ω)e iωt B(ω) = [ Φ R (ω) Φ R () ] iω Φ R (t)

More information

201711grade1ouyou.pdf

201711grade1ouyou.pdf 2017 11 26 1 2 52 3 12 13 22 23 32 33 42 3 5 3 4 90 5 6 A 1 2 Web Web 3 4 1 2... 5 6 7 7 44 8 9 1 2 3 1 p p >2 2 A 1 2 0.6 0.4 0.52... (a) 0.6 0.4...... B 1 2 0.8-0.2 0.52..... (b) 0.6 0.52.... 1 A B 2

More information

BESS Introduction Detector BESS (BESS-TeVspectrometer) Experimetns Data analysis (1) (2) Results Summary

BESS Introduction Detector BESS (BESS-TeVspectrometer) Experimetns Data analysis (1) (2) Results Summary Measurements of Galactic and Atmospheric Cosmic-Ray Absolute Fluxes BESS Introduction Detector BESS (BESS-TeVspectrometer) Experimetns Data analysis (1) (2) Results Summary Introduction 90% 9% 100~10 6

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

ATLAS 2011/3/25-26

ATLAS 2011/3/25-26 ATLAS 2011/3/25-26 2 LHC (Large Hadron Collider)/ATLAS LHC - CERN - s=7 TeV ATLAS - LHC 1 Higgs 44 m 44m 22m 7000t 22 m 3 SCT( ) SCT(SemiConductor Tracker) - - 100 fb -1 SCT 3 SCT( ) R eta=1.0 eta=1.5

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

/ Christopher Essex Radiation and the Violation of Bilinearity in the Thermodynamics of Irreversible Processes, Planet.Space Sci.32 (1984) 1035 Radiat

/ Christopher Essex Radiation and the Violation of Bilinearity in the Thermodynamics of Irreversible Processes, Planet.Space Sci.32 (1984) 1035 Radiat / Christopher Essex Radiation and the Violation of Bilinearity in the Thermodynamics of Irreversible Processes, Planet.Space Sci.32 (1984) 1035 Radiation and the Continuing Failure of the Bilinear Formalism,

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

Part () () Γ Part ,

Part () () Γ Part , Contents a 6 6 6 6 6 6 6 7 7. 8.. 8.. 8.3. 8 Part. 9. 9.. 9.. 3. 3.. 3.. 3 4. 5 4.. 5 4.. 9 4.3. 3 Part. 6 5. () 6 5.. () 7 5.. 9 5.3. Γ 3 6. 3 6.. 3 6.. 3 6.3. 33 Part 3. 34 7. 34 7.. 34 7.. 34 8. 35

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

NEBULA 09M

NEBULA 09M NEBULA 9M1119 3 18 NEBULA( NEutron Detection system for Breakup of Unstable Nuclei with Large Acceptance ) SAMURAI NEBULA 18mm(H) 36mm(V) 1m ±1 ±5 48mm 1 41% (SAMURAI) (γ,n) 1 NEBULA Abstract NEBULA( NEutron

More information

keisoku01.dvi

keisoku01.dvi 2.,, Mon, 2006, 401, SAGA, JAPAN Dept. of Mechanical Engineering, Saga Univ., JAPAN 4 Mon, 2006, 401, SAGA, JAPAN Dept. of Mechanical Engineering, Saga Univ., JAPAN 5 Mon, 2006, 401, SAGA, JAPAN Dept.

More information

陽電子科学 第4号 (2015) 3-8

陽電子科学 第4号 (2015) 3-8 4 (2015) 3 8 Japanese Positron Science Society Positron annihilation age momentum correlation (AMOC) measurement Abstract: Positron annihilation Age-MOmentum Correlation (AMOC) measurement is the coincidence

More information

The Physics of Atmospheres CAPTER :

The Physics of Atmospheres CAPTER : The Physics of Atmospheres CAPTER 4 1 4 2 41 : 2 42 14 43 17 44 25 45 27 46 3 47 31 48 32 49 34 41 35 411 36 maintex 23/11/28 The Physics of Atmospheres CAPTER 4 2 4 41 : 2 1 σ 2 (21) (22) k I = I exp(

More information

K E N Z U 2012 7 16 HP M. 1 1 4 1.1 3.......................... 4 1.2................................... 4 1.2.1..................................... 4 1.2.2.................................... 5................................

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

18 2 20 Abstract Spin of the proton is 1. The proton is composed of three valence quarks, sea quarks 2 and gluons. The gluon mediates strong interaction between quarks. The proton spin is the sum of spin

More information

NaI(Tl) CsI(Tl) GSO(Ce) LaBr 3 (Ce) γ Photo Multiplier Tube PMT PIN PIN Photo Diode PIN PD Avalanche Photo Diode APD MPPC Multi-Pixel Photon Counter L

NaI(Tl) CsI(Tl) GSO(Ce) LaBr 3 (Ce) γ Photo Multiplier Tube PMT PIN PIN Photo Diode PIN PD Avalanche Photo Diode APD MPPC Multi-Pixel Photon Counter L 19 P6 γ 2 3 27 NaI(Tl) CsI(Tl) GSO(Ce) LaBr 3 (Ce) γ Photo Multiplier Tube PMT PIN PIN Photo Diode PIN PD Avalanche Photo Diode APD MPPC Multi-Pixel Photon Counter LaBr 3 (Ce) PMT 662keV 2.9% CsI(Tl) 7.1%

More information

05Mar2001_tune.dvi

05Mar2001_tune.dvi 2001 3 5 COD 1 1.1 u d2 u + ku =0 (1) dt2 u = a exp(pt) (2) p = ± k (3) k>0k = ω 2 exp(±iωt) (4) k

More information

m(ẍ + γẋ + ω 0 x) = ee (2.118) e iωt P(ω) = χ(ω)e = ex = e2 E(ω) m ω0 2 ω2 iωγ (2.119) Z N ϵ(ω) ϵ 0 = 1 + Ne2 m j f j ω 2 j ω2 iωγ j (2.120)

m(ẍ + γẋ + ω 0 x) = ee (2.118) e iωt P(ω) = χ(ω)e = ex = e2 E(ω) m ω0 2 ω2 iωγ (2.119) Z N ϵ(ω) ϵ 0 = 1 + Ne2 m j f j ω 2 j ω2 iωγ j (2.120) 2.6 2.6.1 mẍ + γẋ + ω 0 x) = ee 2.118) e iωt Pω) = χω)e = ex = e2 Eω) m ω0 2 ω2 iωγ 2.119) Z N ϵω) ϵ 0 = 1 + Ne2 m j f j ω 2 j ω2 iωγ j 2.120) Z ω ω j γ j f j f j f j sum j f j = Z 2.120 ω ω j, γ ϵω) ϵ

More information

untitled

untitled D nucleation 3 3D nucleation Glucose isomerase 10 V / nm s -1 5 0 0 5 10 C - C e / mg ml -1 kinetics µ R K kt kinetics kinetics kinetics r β π µ π r a r s + a s : β: µ πβ µ β s c s c a a r, & exp exp

More information

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 +

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 + 2.6 2.6.1 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 + Ne2 m j f j ω 2 j ω2 iωγ j (2.121) Z ω ω j γ j f j

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

PowerPoint Presentation

PowerPoint Presentation / 2008/04/04 Ferran Salleras 1 2 40Gb/s 40Gb/s PC QD PC: QD: e.g. PCQD PC/QD 3 CP-ON SP T CP-OFF PC/QD-SMZ T ~ps, 40Gb/s ~100fJ T CP-ON CP-OFF 500µm500µm Photonic Crystal SMZ K. Tajima, JJAP, 1993. Control

More information

19 σ = P/A o σ B Maximum tensile strength σ % 0.2% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional

19 σ = P/A o σ B Maximum tensile strength σ % 0.2% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional 19 σ = P/A o σ B Maximum tensile strength σ 0. 0.% 0.% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional limit ε p = 0.% ε e = σ 0. /E plastic strain ε = ε e

More information

Abstruct CANGAROO-III (PhotoMultiplier Tube PMT PMT ) PMT PMT R3479 ND 1 PMT 10 ( 90 ) Woomera PMT PMT (Light Guide LG) LG 0.944±0.023 PMT (4 ch) PMT

Abstruct CANGAROO-III (PhotoMultiplier Tube PMT PMT ) PMT PMT R3479 ND 1 PMT 10 ( 90 ) Woomera PMT PMT (Light Guide LG) LG 0.944±0.023 PMT (4 ch) PMT CANGAROOIII January 16, 2009 Abstruct CANGAROO-III (PhotoMultiplier Tube PMT PMT ) PMT PMT R3479 ND 1 PMT 10 ( 90 ) Woomera PMT PMT (Light Guide LG) LG 0.944±0.023 PMT (4 ch) PMT R8900U (HPKK) R8900U Bialkali

More information

反D中間子と核子のエキゾチックな 束縛状態と散乱状態の解析

反D中間子と核子のエキゾチックな   束縛状態と散乱状態の解析 .... D 1 in collaboration with 1, 2, 1 RCNP 1, KEK 2 . Exotic hadron qqq q q Θ + Λ(1405) etc. uudd s? KN quasi-bound state? . D(B)-N bound state { { D D0 ( cu) B = D ( cd), B = + ( bu) B 0 ( bd) D(B)-N

More information

0.1 I I : 0.2 I

0.1 I I : 0.2 I 1, 14 12 4 1 : 1 436 (445-6585), E-mail : sxiida@sci.toyama-u.ac.jp 0.1 I I 1. 2. 3. + 10 11 4. 12 1: 0.2 I + 0.3 2 1 109 1 14 3,4 0.6 ( 10 10, 2 11 10, 12/6( ) 3 12 4, 4 14 4 ) 0.6.1 I 1. 2. 3. 0.4 (1)

More information

) ] [ h m x + y + + V x) φ = Eφ 1) z E = i h t 13) x << 1) N n n= = N N + 1) 14) N n n= = N N + 1)N + 1) 6 15) N n 3 n= = 1 4 N N + 1) 16) N n 4

) ] [ h m x + y + + V x) φ = Eφ 1) z E = i h t 13) x << 1) N n n= = N N + 1) 14) N n n= = N N + 1)N + 1) 6 15) N n 3 n= = 1 4 N N + 1) 16) N n 4 1. k λ ν ω T v p v g k = π λ ω = πν = π T v p = λν = ω k v g = dω dk 1) ) 3) 4). p = hk = h λ 5) E = hν = hω 6) h = h π 7) h =6.6618 1 34 J sec) hc=197.3 MeV fm = 197.3 kev pm= 197.3 ev nm = 1.97 1 3 ev

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

306 [7] GeV TeV PAMELA 100 GeV PAMELA AMS GeV [8] TeV [9] PAMELA[10] AMS BESS-Polar 95 [11]AMS 1.3 AMS AMS rigidity TOFTime Of Flight TRDE

306 [7] GeV TeV PAMELA 100 GeV PAMELA AMS GeV [8] TeV [9] PAMELA[10] AMS BESS-Polar 95 [11]AMS 1.3 AMS AMS rigidity TOFTime Of Flight TRDE 305 Alpha Magnetic Spectrometer (AMS) Sadakazu.Haino@cern.ch 2013 2 28 1 AMS 1.1 AMS AMS 60 600 1976 LEP L3 LEP GeV TeV 2011 5 AMS ISS ISS 2020 20 BESS [2] HEAT[3] AMS PAMELA [4] Fermi [5] 10 GeV 100 GeV

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

006 11 8 0 3 1 5 1.1..................... 5 1......................... 6 1.3.................... 6 1.4.................. 8 1.5................... 8 1.6................... 10 1.6.1......................

More information

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.

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. 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. http://www.morikita.co.jp/books/mid/009192 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. i 2 t 1. 2. 3 2 3. 6 4. 7 5. n 2 ν 6. 2 7. 2003 ii 2 2013 10 iii 1987

More information

数学の基礎訓練I

数学の基礎訓練I I 9 6 13 1 1 1.1............... 1 1................ 1 1.3.................... 1.4............... 1.4.1.............. 1.4................. 3 1.4.3........... 3 1.4.4.. 3 1.5.......... 3 1.5.1..............

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

MOSFET 6-2 CMOS 6-2 TTL Transistor Transistor Logic ECL Emitter Coupled Logic I2L Integrated

MOSFET 6-2 CMOS 6-2 TTL Transistor Transistor Logic ECL Emitter Coupled Logic I2L Integrated 1 -- 7 6 2011 11 1 6-1 MOSFET 6-2 CMOS 6-2 TTL Transistor Transistor Logic ECL Emitter Coupled Logic I2L Integrated Injection Logic 6-3 CMOS CMOS NAND NOR CMOS 6-4 6-5 6-1 6-2 CMOS 6-3 6-4 6-5 c 2011 1/(33)

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

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

TeV b,c,τ KEK/ ) ICEPP

TeV b,c,τ KEK/ ) ICEPP TeV b,c,τ KEK/ ) ICEPP 2 TeV TeV ~1930 ~1970 ~2010 LHC TeV LHC TeV LHC TeV CKM K FCNC K CP violation c b, τ B-B t B CP violation interplay 6 Super B Factory Super KEKB LoI (hep-ex/0406071) SLAC Super B

More information