thesis.dvi

Size: px
Start display at page:

Download "thesis.dvi"

Transcription

1 SA210A

2 1 introduction Positronium Positronium moderation ortho-ps Na CsI CAMAC Pulse-Height-ADC CsI CsI ortho-ps ortho-ps TDC TDC TDC A phadc CAMAC 39 B TDC CAMAC 42 i

3 1 Ps Na moderation Na PMT1 Na 2250V PMT1 Na 1950V 2000V 2050V 2100V PMT1 PMT2 Na22 co PMT1 PMT2 Na22 co energy PMT1 PMT2 Na22 co energy 2d-plot PMT1 PMT2 Na22 co allenergy PMT2 PMT3 Na22 co energy PMT2 PMT3 Na22 co energy 2d-plot phadc phadc Moderator phadc Moderator phadc Al W Moderator phadc W-powder normalize W-powder TDC t TDC TDC KeV KeV ii

4 1 introduction 1.1 Positronium 2 r e v σ 2 σ 2 = πr2 e 1 + γ γ2 + 4γ + 1 ln ( γ + γ γ ) γ + 3 γ2 1 (1) γ = 1 1 ( vc )2 (2) (1) σ 2 = πre 2 c v (3) λ 2 ρ λ 2 = σ 2 ρv = πre 2 cρ (4) λ 3 λ 3 = σ 3 ρv = 4 3 (π2 9)αr e cρ λ (5) α (1/137) 1

5 (5) 3 2 1/370 1 λ 2 (Ps) Ps (e ) (e + ) (γ ) (QED) Ps S 1 para-ps( ) 3 ortho-ps( ) S=1 (3 ) S=0 (1 ) para-ps 2 ortho-ps 3 e - e + e - e + para-ps life time 125psec ortho-ps life time 142nsec 1: Ps 2

6 Ps Ps a B (0.106nm) (6.8eV) Ps ρ Ps = 1 p Ps 8πa 3 B o Ps λ p Ps = 4σ 2 ρ Ps v = α5 m e c s 1 (6) λ o Ps = 4 3 σ 3ρ Ps v = 2(π2 9)α 6 m e c 2 9π s 1 (7) τ p Ps = 1 λ p Ps 125ps (8) τ o Ps = 1 λ o Ps 142ns (9) para-ps 125psec ortho-ps 142nsec QED ortho-ps τ ortho Ps = nsec (QED 2002) τ ortho Ps = nsec ( 2002) 3

7 1.2 Positronium ( 22 Na) ortho-ps 22 Na 0.545MeV Ps Ps moderator moderation( ) e + 22 Na positron Max energy 0.54MeV B + decay 22 Ne * excited state 22 Ne γ -ray 1.28MeV 2: Na22 4

8 1.2.1 moderation Al(-0.2eV) Cr(-1.7eV) Cu( eV) Ni(-1.1eV) Si(- 1.0eV) W(-2.54eV) ( ) Ps Ps (O 2,N 2 ) moderator Al W 1 m + e e + γ -ray e - annihilation e + γ -ray Ps release e + e - moderator powder 3: moderation 5

9 1.2.2 λ Ne σ λ = 1 σne σ σ = πr γ γ2 + 4γ + 1 ln ( γ + γ γ ) γ + 3 γ2 1 (10) (11) r 0 = α m e c 2 γ = E + m e c 2 E + α m e ( ) c 22 Na 0.545MeV pc 0.5MeV σ m e c 2 0.5MeV E + = m e c 2 + p 2 c 2 = 2 MeV (12) 2 (11) α 1 c = m/s 137 = MeV c Ne( ) (10) σ = m 2 (13) Ne = /m 3 λ = 74.30m (14) 0.5MeV 6

10 1.2.3 N 2 ( ) O 2 ( )=7:3 d d = 1.29mg/cm 3 N O 1mol N 14.01g/mol 7 O 16.00g/mol g/mol 7 3 mol g/mol mol = g/mol (15) mol Na ( mol mol) = /mol (16) Ne Ne = Na( ) = /mol 1.29mg/cm mg/mol /mol = /m 3 (17) 7

11 2 ortho-ps 22 Na e + moderation ortho-ps 3 3γ CsI Side view powder (moderator) CsI CsI e + Na22 Top view CsI 120 γ -ray CsI CsI powder 4: 8

12 Na 22 Na 22 Na Ne β MeV 0.3psec 22 Ne 1.274MeV γ 22 Ne 0.511MeV γ 0.511MeV γ β MeV γ 3 22 Na γ Ps 22 Na 5 Na22 e + 100micro m scintilator 14mm Na22 25micro m mylar 5: Na22 9

13 2.1.2 CsI CsI CsI CsI γ CAMAC Pulse-Height-ADC ADC(peak-hold Analog-to-Digital Converter) ADC CsI γ NIM ( ) 12 CAMAC 10

14 CsI 22 Na 0.511MeV γ-ray CsI PMT1 1.27MeV γ-ray phadc HV Dis DiS Discriminator GG Gate Generator ADC Gate GG 6: CsI (4cm 4cm 3cm) CsI 22 Na ADC 7 CsI 2.25kV ADC ch 7: PMT1 Na 2250V 11

15 2.25kV ch70 ch MeV γ 0.5MeV Discriminator ch700 β MeV γ 0.5MeV 1.27MeV 1.27MeV γ 8: PMT1 Na 1950V 2000V 2050V 2100V kV 2.00kV 2.05kV 2.10kV 1.28MeV γ Peak 12

16 CsI CsI CsI 22 Na 2 CsI AND γ (0.511MeV) ADC CsI 3 PMT1 PMT2 PMT1 PMT3 HV 0.511MeV HV PMT CsI γ γ CsI PMT γ -source ch0 Discriminator Discriminator A N D Gate Generator ch1 Gate CAMAC Pulse Height ADC 9: 13

17 10: PMT1 PMT2 Na22 co 10 phadc ch PMT1 PMT2 2.0kV 0.511MeV PMT1 Peak 145ch 70ch Peak =75 phadc 0.511MeV Peak 2.0kV 75ch phadc 14

18 11: PMT1 PMT2 Na22 co energy 12: PMT1 PMT2 Na22 co energy 2d-plot 15

19 11 (kev) PMT1 PMT2 511keV 350keV 511keV 12 PMT1 PMT2 511keV 511keV 350keV 350keV 511keV 350keV 350keV 511keV 16

20 13: PMT1 PMT2 Na22 co allenergy 13 2 CsI 1000keV γ 511keV 17

21 14: PMT2 PMT3 Na22 co energy 15: PMT2 PMT3 Na22 co energy 2d-plot 18

22 14 PMT2 PMT3 PMT2 PMT3 15 PMT2 PMT3 19

23 2.2 ortho-ps Moderation Ps 3 ( ) 0.511MeV 20

24 2.2.1 CsI Na Moderator Al W 10cm 2.0kV 3 CsI AND Gate 14 sec phadc Moderator Al W Moderator 17 HV PMT2 CsI r-ray CsI CsI HV PMT3 PMT1 HV powder CAMAC Pulse Height ADC Shaper AMP ch3 ch2 ch1 Gate Gate Generator Gate Generator A N D veto Discriminator Discriminator Discriminator 16: 21

25 PMT4 Over view PMT2 CsI 120 r-ray PMT3 CsI CsI powder PMT1 Side view powder (moderator) PMT3 CsI CsI e + PMT1 Na22 17: 22

26 2.2.2 Moderator Al 18: 23

27 19: 3 phadc 24

28 Moderator 20: 25

29 21: 3 phadc 26

30 Moderator 22: Moderator 27

31 23: 3 phadc Moderator 28

32 Al-powder W-powder Moderator 24: phadc Al W Moderator 29

33 (24) W-powder phadc 1MeV Peak Ps counts counts/h moderator Al-powder 104h W-powder 94h no-moderator 61h moderator Al W moderator count count moderator 1 Al-powder moderator 1.18 W-powder moderator

34 25: phadc W-powder 26: normalize W-powder (26) W-powder normalize moderator 1MeV peak Ps 31

35 3 ortho-ps ortho-ps 0 para-ps 123psec ortho-ps 142nsec 2 2 TDC 3.1 t N(t) dn(t) = λn(t) (18) dt λ ( ) (18) N(t) = N(0)e λt (19) t+dt -dn τ τ = 0 tdn N(0) = λte λt = 1 dn 0 λ (20) τ 1 λ TDC t 32

36 PMT 3.2 TDC TDC 1 1 NIM TDC 12 ADC CAMAC CAMAC TDC 1 5nsec start signal stop signal τ-ortho-ps 27: TDC t powder (moderator) TDC stop signal PMT CsI CsI e + Na22 PMT TDC stop signal TDC start signal 28: TDC 33

37 3.2.1 TDC CsI PMT1 phadc HV Dis GG GG GG TDC stop TDC stop TDC stop CsI PMT2 HV Dis A N D CsI PMT3 HV Dis Na22 PMT HV Dis GG A N D GG ADC Gate GG TDC start DiS Discriminator GG Gate Generator 29: TDC 29 TDC PMT1:2.0KV PMT2:2.0KV PMT3:2.0KV Na22PMT:2.4KV Na m start 3 CsI Na22 AND start CsI stop phadc TDC 34

38 3.2.2 TDC phadc o-ps 3 3 CsI 1.2MeV fitting 35

39 3.3 TDC Moderator TDC 30: 1250KeV 36

40 31: 1250KeV KeV KeV 0 TDC 60ch TDCch60 Peak KeV ortho-ps Fitting moderator τ ortho Ps τ w = 123 ± 62nsec (21) ortho-ps (142nsec) data 37

41 4 ortho-ps ortho-ps TDC Al W 1 moderation ( 2.6 ) rate 38

42 A phadc CAMAC #include <stdio.h> #include<sys/types.h> #include <sys/errno.h> #include "camlib.h" #define read_adc 0 #define test_lam_adc 8 #define clear_adc 9 #define clear_lam_adc 10 static int data1,data2,data3, q1,q2,q3, x1,x2,x3; FILE *f1; main(argc, argv) int argc; char **argv; { int i, j,a,status, nevts,stn,channel1,channel2,channel3; char fname[20]; if (argc == 1 strcmp(argv[1], "help") == 0 strcmp(argv[1], "-h") == 0) { printf("usage : testadc (station # of the module) (# of channel1) (# of ch exit(0); } sscanf(argv[1],"%d",&stn); sscanf(argv[2],"%d",&channel1); sscanf(argv[3],"%d",&channel2); sscanf(argv[4],"%d",&channel3); sscanf(argv[5],"%d",&nevts); sscanf(argv[6],"%s",&fname); if (CAMOPN()){ 39

43 } printf("camac open error\n"); exit(1); CSETCR(1); CGENZ(); CGENC(); CREMI(); /* clear */ CAMAC(NAF(stn, channel1, clear_adc), &data1, &q1, &x1); CAMAC(NAF(stn, channel2, clear_adc), &data2, &q2, &x2); CAMAC(NAF(stn, channel3, clear_adc), &data3, &q3, &x3); // printf("data:%d q:%d x:%d \n",data,q,x); CAMAC(NAF(stn, channel1, clear_lam_adc), &data1, &q1, &x1); // printf("data:%d q:%d x:%d \n",data,q,x); data1 = 1; data2 = 1; data3 = 1; /* CAMAC */ for( i = 0; i < nevts; i++) { while(1) { status = CAMAC(NAF(stn, channel1, test_lam_adc), &data1, &q1, &x1); // printf("status:%d data:%d q:%d x:%d \n",status,data,q,x); if (q1!= 0) break; } CAMAC(NAF(stn, channel1, read_adc), &data1, &q1, &x1); CAMAC(NAF(stn, channel2, read_adc), &data2, &q2, &x2); CAMAC(NAF(stn, channel3, read_adc), &data3, &q3, &x3); 40

44 // printf("[%d:%d:%d]\n",data,q,x); f1=fopen(fname,"a"); fprintf(f1,"%d %d %d\n",data1,data2,data3); printf("%s %d %d %d %d\n",fname,data1,data2,data3,i); fclose(f1); data1=255; data2=255; data3=255; } /* clear */ CAMAC(NAF(stn, channel1, clear_adc), &data1, &q1, &x1); CAMAC(NAF(stn, channel2, clear_adc), &data2, &q2, &x2); CAMAC(NAF(stn, channel1, clear_lam_adc), &data1, &q1, &x1); CAMAC(NAF(stn, channel3, clear_adc), &data3, &q3, &x3); } /* close CAMAC */ CAM_Close(); 41

45 B TDC CAMAC #include <stdio.h> #include<stdlib.h> #include<sys/types.h> #include<time.h> #include <sys/errno.h> #include "camlib.h" #define LOOP 10 #define ADC 10 #define ADCCH 0 #define MAX 4000 static int read_adc, write_adc, clear_adc, test_lam_adc, clear_lam_adc, test_module_adc, disable_lam_adc, enable_lam_adc, dumy, q, x; FILE *f1; main(argc, argv) int argc; char **argv; { int i, j,a,status, nevts; char fname[20]; int jikan; int mon,day,hou,min; time_t ltime; struct tm*today; ltime=time(null); today=localtime(&ltime); mon=today->tm_mon+1; day=today->tm_mday; hou=today->tm_hour; min=today->tm_min; jikan=mon* day*10000+hou*100+min; sprintf(fname,"otdc%d.dat",jikan); if (argc == 1 strcmp(argv[1], "help") == 0 42

46 } strcmp(argv[1], "-h") == 0) { printf("usage : adc (# of events)\n"); exit(0); sscanf(argv[1],"%d",&nevts); read_adc = NAF(ADC, ADCCH, 0); test_lam_adc = NAF(ADC, ADCCH, 8); clear_adc = NAF(ADC, ADCCH, 9); clear_lam_adc = NAF(ADC, ADCCH, 10); disable_lam_adc = NAF(ADC, ADCCH, 24); test_module_adc = NAF(ADC, ADCCH, 25); enable_lam_adc = NAF(ADC, ADCCH, 26); if (CAMOPN()){ printf("camac open error\n"); exit(1); } CSETCR(1); CGENZ(); CGENC(); CREMI(); /* clear */ CAMAC(clear_adc, &dumy, &q, &x); // printf("dumy:%d q:%d x:%d \n",dumy,q,x); CAMAC(clear_lam_adc, &dumy, &q, &x); // printf("dumy:%d q:%d x:%d \n",dumy,q,x); dumy = 1; /* CAMAC */ for( i = 0; i < nevts; i++) { // sleep(3); 43

47 while(1) { status = CAMAC(test_lam_adc, &dumy, &q, &x); // status = CAMAC(read_adc, &dumy, &q, &x); // printf("status:%d dumy:%d q:%d x:%d \n",status,dumy,q,x); // dumy += dumy*2; // for (j=0;j<10000;j++) { // CAMAC(NAF(12,0,16),&dumy,&q,&x); // } if (q!= 0) break; } CAMAC(read_adc, &dumy, &q, &x); // printf("%s",fname); f1=fopen(fname,"a"); // if(dumy<max){ // printf("[%d:%d:%d]\n",dumy,q,x); fprintf(f1,"%d\n",dumy); printf("%d\n",i); // } else{ if(dumy>max){ i=i-1; } fclose(f1); // } /* while(1){ status = CAMAC(NAF(ADC,0,0), &dumy, &q, &x); if (status & 0x01!=0) break; } */ dumy=255; 44

48 /* clear */ CAMAC(clear_adc, &dumy, &q, &x); CAMAC(clear_lam_adc, &dumy, &q, &x); } /* close CAMAC */ CAM_Close(); // fclose(f1); } 45

49 46

50 [1] [2] [3] L A TEX2e [4] KNOLL [5] 26 [6] 47

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

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

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

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

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

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

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

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

[ ] [ ] [ ] [ ] [ ] [ ] 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

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

目次 2 1. イントロダクション 2. 実験原理 3. データ取得 4. データ解析 5. 結果 考察 まとめ

目次 2 1. イントロダクション 2. 実験原理 3. データ取得 4. データ解析 5. 結果 考察 まとめ オルソポジトロニウムの寿命測定による QED の実験的検証 課題演習 A2 2016 年後期 大田力也鯉渕駿龍澤誠之 羽田野真友喜松尾一輝三野裕哉 目次 2 1. イントロダクション 2. 実験原理 3. データ取得 4. データ解析 5. 結果 考察 まとめ 第 1 章イントロダクション 実験の目的 4 ポジトロニウム ( 後述 ) の崩壊を観測 オルソポジトロニウム ( スピン 1 状態 ) の寿命を測定

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

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

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

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

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

- 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

untitled

untitled 71 7 3,000 1 MeV t = 1 MeV = c 1 MeV c 200 MeV fm 1 MeV 3.0 10 8 10 15 fm/s 0.67 10 21 s (1) 1fm t = 1fm c 1fm 3.0 10 8 10 15 fm/s 0.33 10 23 s (2) 10 22 s 7.1 ( ) a + b + B(+X +...) (3) a b B( X,...)

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

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

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

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

Thick-GEM 06S2026A 22 3

Thick-GEM 06S2026A 22 3 Thick-GEM 06S2026A 22 3 (MWPC-Multi Wire Proportional Chamber) MPGD(Micro Pattern Gas Detector) MPGD MPGD MPGD MPGD GEM(Gas Electron Multiplier) GEM GEM GEM Thick-GEM GEM Thick-GEM 10 4 Thick-GEM 1 Introduction

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

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

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

main.dvi

main.dvi CeF 3 1 1 3 1.1 KEK E391a... 3 1.1.1 KL 0 π0 νν... 3 1.1.2 E391a... 4 1.1.3... 5 1.2... 6 2 8 2.1... 8 2.2... 10 2.3 CeF 3... 12 2.4... 13 3 15 3.1... 15 3.2... 15 3.3... 18 3.4... 22 4 23 4.1... 23 4.2...

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

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

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

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

B

B B07557 0 0 (AGN) AGN AGN X X AGN AGN Geant4 AGN X X X (AGN) AGN AGN X AGN. AGN AGN Seyfert Seyfert Seyfert AGN 94 Carl Seyfert Seyfert Seyfert z < 0. Seyfert I II I 000 km/s 00 km/s II AGN (BLR) (NLR)

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

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

I117 7 School of Information Science, Japan Advanced Institute of Science and Technology

I117 7 School of Information Science, Japan Advanced Institute of Science and Technology I117 7 School of Information Science, Japan Advanced Institute of Science and Technology time time t long typedef long time_t; 1970/01/01 0:00:00 time t = time(null); Japan Advanced Institute of Science

More information

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

H 0 H = H 0 + V (t), V (t) = gµ B S α qb e e iωt i t Ψ(t) = [H 0 + V (t)]ψ(t) Φ(t) Ψ(t) = e ih0t Φ(t) H 0 e ih0t Φ(t) + ie ih0t t Φ(t) = [ 3 3. 3.. H H = H + V (t), V (t) = gµ B α B e e iωt i t Ψ(t) = [H + V (t)]ψ(t) Φ(t) Ψ(t) = e iht Φ(t) H e iht Φ(t) + ie iht t Φ(t) = [H + V (t)]e iht Φ(t) Φ(t) i t Φ(t) = V H(t)Φ(t), V H (t) = e iht V (t)e

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

II ( ) prog8-1.c s1542h017%./prog8-1 1 => 35 Hiroshi 2 => 23 Koji 3 => 67 Satoshi 4 => 87 Junko 5 => 64 Ichiro 6 => 89 Mari 7 => 73 D

II ( ) prog8-1.c s1542h017%./prog8-1 1 => 35 Hiroshi 2 => 23 Koji 3 => 67 Satoshi 4 => 87 Junko 5 => 64 Ichiro 6 => 89 Mari 7 => 73 D II 8 2003 11 12 1 6 ( ) prog8-1.c s1542h017%./prog8-1 1 => 35 Hiroshi 2 => 23 Koji 3 => 67 Satoshi 4 => 87 Junko 5 => 64 Ichiro 6 => 89 Mari 7 => 73 Daisuke 8 =>. 73 Daisuke 35 Hiroshi 64 Ichiro 87 Junko

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

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

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

double float

double float 2015 3 13 1 2 2 3 2.1.......................... 3 2.2............................. 3 3 4 3.1............................... 4 3.2 double float......................... 5 3.3 main.......................

More information

http://radphys4.c.u-tokyo.ac.jp/~torii/lecture/radiolect-kn.html 21 KOMCEE K303 2013 / 10 / 18 / 21 KOMCEE K303 Billet de 500 Francs Français en circulation: 1993 1999 α β γ X VIDEO http://eneco.jaero.or.jp/20110322/

More information

P F ext 1: F ext P F ext (Count Rumford, ) H 2 O H 2 O 2 F ext F ext N 2 O 2 2

P F ext 1: F ext P F ext (Count Rumford, ) H 2 O H 2 O 2 F ext F ext N 2 O 2 2 1 1 2 2 2 1 1 P F ext 1: F ext P F ext (Count Rumford, 1753 1814) 0 100 H 2 O H 2 O 2 F ext F ext N 2 O 2 2 P F S F = P S (1) ( 1 ) F ext x W ext W ext = F ext x (2) F ext P S W ext = P S x (3) S x V V

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

(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

AD

AD AD 1110800673 2015 2 25 1 1 1.1..................................... 1 1.2................................... 3 2 4 2.1....................... 4 2.2 TDC................................ 5 2.2.1.....................................

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

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

A = A x x + A y y + A, B = B x x + B y y + B, C = C x x + C y y + C..6 x y A B C = A x x + A y y + A B x B y B C x C y C { B = A x x + A y y + A y B B

A = A x x + A y y + A, B = B x x + B y y + B, C = C x x + C y y + C..6 x y A B C = A x x + A y y + A B x B y B C x C y C { B = A x x + A y y + A y B B 9 7 A = A x x + A y y + A, B = B x x + B y y + B, C = C x x + C y y + C..6 x y A B C = A x x + A y y + A B x B y B C x C y C { B = A x x + A y y + A y B B x x B } B C y C y + x B y C x C C x C y B = A

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

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

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

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

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

C による数値計算法入門 ( 第 2 版 ) 新装版 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, 新装版 1 刷発行時のものです.

C による数値計算法入門 ( 第 2 版 ) 新装版 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, 新装版 1 刷発行時のものです. C による数値計算法入門 ( 第 2 版 ) 新装版 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/009383 このサンプルページの内容は, 新装版 1 刷発行時のものです. i 2 22 2 13 ( ) 2 (1) ANSI (2) 2 (3) Web http://www.morikita.co.jp/books/mid/009383

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

Baud Rate 9600 Parity NONE Number of Data Bits 8 Number of Stop Bits 1 Flow Control NONE 1 RS232C 200mm 2,000mm DIMM ( ) Telescope East/West LX200 * 1

Baud Rate 9600 Parity NONE Number of Data Bits 8 Number of Stop Bits 1 Flow Control NONE 1 RS232C 200mm 2,000mm DIMM ( ) Telescope East/West LX200 * 1 JARE54 LX200ACF 2012/2/18 2012/6/14 1 Abstract 8 LX200-ACF Linux PC meade Auto Align PC Zero Star Alignment Auto Align Zero Star Alignment 1 1 0.3 Zero Star Alignment 1 0.3 Auto Align 2 54 (2012 11 2013

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

muramatsu_ver1.key

muramatsu_ver1.key 229-ThTES α = e 2 /2ε 0 hc (John D. Barrow 2005) Radiationdominated era Matterdominated era Dark energy era 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 Time (years) Time 2 α = e 2 /2ε 0 hc (John D. Barrow

More information

t 2 2 t 2 t F ( ) p- 2 2 F 2 G F ( ) 2 2 F 2 G F ( ) 2 2 2

t 2 2 t 2 t F ( ) p- 2 2 F 2 G F ( ) 2 2 F 2 G F ( ) 2 2 2 1 2 2 0 1 2 2 2 2 2 2 2 2.1 2 2 F={f ij }, G {g ij } t f ij t g ij = 1 f ij < t g ij = 0 t p- p S 0 S p = S 0 /S t p 2 t 1 t 2 2 t 2 t 2 2 3 3 1 2 F ( ) p- 2 2 F 2 G 3 2 2 F ( ) 2 2 F 2 G 3 3 2 F ( ) 2

More information

r08.dvi

r08.dvi 19 8 ( ) 019.4.0 1 1.1 (linked list) ( ) next ( 1) (head) (tail) ( ) top head tail head data next 1: NULL nil ( ) NULL ( NULL ) ( 1 ) (double linked list ) ( ) 1 next 1 prev 1 head cur tail head cur prev

More information

£Ã¥×¥í¥°¥é¥ß¥ó¥°(2018) - Âè11²ó – ½ÉÂꣲ¤Î²òÀ⡤±é½¬£² –

£Ã¥×¥í¥°¥é¥ß¥ó¥°(2018) - Âè11²ó – ½ÉÂꣲ¤Î²òÀ⡤±é½¬£² – (2018) 11 2018 12 13 2 g v dv x dt = bv x, dv y dt = g bv y (1) b v 0 θ x(t) = v 0 cos θ ( 1 e bt) (2) b y(t) = 1 ( v 0 sin θ + g ) ( 1 e bt) g b b b t (3) 11 ( ) p14 2 1 y 4 t m y > 0 y < 0 t m1 h = 0001

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

Microsoft Word - C.....u.K...doc

Microsoft Word - C.....u.K...doc C uwêííôöðöõ Ð C ÔÖÐÖÕ ÐÊÉÌÊ C ÔÖÐÖÕÊ C ÔÖÐÖÕÊ Ç Ê Æ ~ if eíè ~ for ÒÑÒ ÌÆÊÉÉÊ ~ switch ÉeÍÈ ~ while ÒÑÒ ÊÍÍÔÖÐÖÕÊ ~ 1 C ÔÖÐÖÕ ÐÊÉÌÊ uê~ ÏÒÏÑ Ð ÓÏÖ CUI Ô ÑÊ ÏÒÏÑ ÔÖÐÖÕÎ d ÈÍÉÇÊ ÆÒ Ö ÒÐÑÒ ÊÔÎÏÖÎ d ÉÇÍÊ

More information

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

More information

ohp08.dvi

ohp08.dvi 19 8 ( ) 2019.4.20 1 (linked list) ( ) next ( 1) (head) (tail) ( ) top head tail head data next 1: 2 (2) NULL nil ( ) NULL ( NULL ) ( 1 ) (double linked list ) ( 2) 3 (3) head cur tail head cur prev data

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

untitled

untitled (a) (b) (c) (d) Wunderlich 2.5.1 = = =90 2 1 (hkl) {hkl} [hkl] L tan 2θ = r L nλ = 2dsinθ dhkl ( ) = 1 2 2 2 h k l + + a b c c l=2 l=1 l=0 Polanyi nλ = I sinφ I: B A a 110 B c 110 b b 110 µ a 110

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

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

DA100データアクイジションユニット通信インタフェースユーザーズマニュアル

DA100データアクイジションユニット通信インタフェースユーザーズマニュアル Instruction Manual Disk No. RE01 6th Edition: November 1999 (YK) All Rights Reserved, Copyright 1996 Yokogawa Electric Corporation 801234567 9 ABCDEF 1 2 3 4 1 2 3 4 1 2 3 4 1 2

More information

PowerPoint Presentation

PowerPoint Presentation For experiment coordinators CREST, JST Go IWAI 2004/09/05 Introduction to CLDAQ for experiment coordinators 2 2004/09/05 Introduction to CLDAQ for experiment coordinators 3 2004/09/05 Introduction to CLDAQ

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

TOP URL 1

TOP URL   1 TOP URL http://amonphys.web.fc.com/ 3.............................. 3.............................. 4.3 4................... 5.4........................ 6.5........................ 8.6...........................7

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

£Ã¥×¥í¥°¥é¥ß¥ó¥°ÆþÌç (2018) - Â裵²ó ¨¡ À©¸æ¹½Â¤¡§¾ò·ïʬ´ô ¨¡

£Ã¥×¥í¥°¥é¥ß¥ó¥°ÆþÌç (2018) - Â裵²ó  ¨¡ À©¸æ¹½Â¤¡§¾ò·ïʬ´ô ¨¡ (2018) 2018 5 17 0 0 if switch if if ( ) if ( 0) if ( ) if ( 0) if ( ) (0) if ( 0) if ( ) (0) ( ) ; if else if ( ) 1 else 2 if else ( 0) 1 if ( ) 1 else 2 if else ( 0) 1 if ( ) 1 else 2 (0) 2 if else

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

file"a" file"b" fp = fopen("a", "r"); while(fgets(line, BUFSIZ, fp)) {... fclose(fp); fp = fopen("b", "r"); while(fgets(line, BUFSIZ, fp)) {... fclose

filea fileb fp = fopen(a, r); while(fgets(line, BUFSIZ, fp)) {... fclose(fp); fp = fopen(b, r); while(fgets(line, BUFSIZ, fp)) {... fclose I117 9 2 School of Information Science, Japan Advanced Institute of Science and Technology file"a" file"b" fp = fopen("a", "r"); while(fgets(line, BUFSIZ, fp)) {... fclose(fp); fp = fopen("b", "r"); while(fgets(line,

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

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

1 2 1 a(=,incident particle A(target nucleus) b (projectile B( product nucleus, residual nucleus, ) ; a + A B + b a A B b 1: A(a,b)B A=B,a=b 2 1. ( 10

1 2 1 a(=,incident particle A(target nucleus) b (projectile B( product nucleus, residual nucleus, ) ; a + A B + b a A B b 1: A(a,b)B A=B,a=b 2 1. ( 10 1 2 1 a(=,incident particle A(target nucleus) b (projectile B( product nucleus, residual nucleus, ) ; a + A B + b a A B b 1: A(a,b)B A=B,a=b 2 1. ( 10 14 m) ( 10 10 m) 2., 3 1 =reaction-text20181101b.tex

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

2015/3/18

2015/3/18 2015/3/18 1 1 1.1 Overview.................................................... 1 1.1.1....................................... 1 1.1.2......................................... 1 1.1.3 C.............................................

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

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

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

O1-1 O1-2 O1-3 O1-4 O1-5 O1-6 O1-1 O1-2 O1-3 O1-4 O1-5 O1-6 O1-7 O1-8 O1-9 O1-10 O1-11 O1-12 O1-13 O1-14 O1-15 O1-16 O1-17 O1-18 O1-19 O1-20 O1-21 O1-22 O1-23 O1-24 O1-25 O1-26 O1-27 O1-28 O1-29 O1-30 O1-31 O1-32 O1-33 O1-34 O1-35

More information

II (No.2) 2 4,.. (1) (cm) (2) (cm) , (

II (No.2) 2 4,.. (1) (cm) (2) (cm) , ( II (No.1) 1 x 1, x 2,..., x µ = 1 V = 1 k=1 x k (x k µ) 2 k=1 σ = V. V = σ 2 = 1 x 2 k µ 2 k=1 1 µ, V σ. (1) 4, 7, 3, 1, 9, 6 (2) 14, 17, 13, 11, 19, 16 (3) 12, 21, 9, 3, 27, 18 (4) 27.2, 29.3, 29.1, 26.0,

More information

P6dark P6dark µ-pic 2 µ-pic 2 3 µ-pic µ-pic µ-pic 3 µ-pic (10cm ) MPGC N3035-KA195 No. SN ASD (16ns[C]) (16nsC

P6dark P6dark µ-pic 2 µ-pic 2 3 µ-pic µ-pic µ-pic 3 µ-pic (10cm ) MPGC N3035-KA195 No. SN ASD (16ns[C]) (16nsC 1 2010 P6dark 2011 2 10 1 P6dark µ-pic 2 µ-pic 2 3 µ-pic 256 256 2 3 µ-pic µ-pic 3 µ-pic (10cm ) MPGC N3035-KA195 No. SN 060830-2 ASD (16ns[C]) (16nsC ) PAN16-10A ASD ( ) 3.37V PAN16-30A ASD (+) +3.36V

More information