2004/03/31

Similar documents
LC-MS LC-MS NMR NMR LC-NMR [1] LC-NMR LC-NMR LC-NMR NMR [2] LC-NMR MHz NMR HPLC NMR LC-NMR LC-NMR LC-NMR WET water suppression enhanced through T1 eff

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

09_organal2

25 3 4

E 1/2 3/ () +3/2 +3/ () +1/2 +1/ / E [1] B (3.2) F E 4.1 y x E = (E x,, ) j y 4.1 E int = (, E y, ) j y = (Hall ef

Nuclear Magnetic Resonance 1 H NMR spectrum PPM

磁性物理学 - 遷移金属化合物磁性のスピンゆらぎ理論

Microsoft Word - 4NMR2.doc

GJG160842_O.QXD

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

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

こんにちは由美子です

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

橡実験IIINMR.PDF

物理化学I-第12回(13).ppt

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

放射線化学, 92, 39 (2011)

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



15

Degradation Mechanism of Ethylene-propylene-diene Terpolymer by Ozone in Aqueous Solution Satoshi MIWA 1 *, 2, Takako KIKUCHI 1, 2, Yoshito OHTAKE 1 a

2 0.1 Introduction NMR 70% 1/2

スライド 1

untitled

公開用:新500MHz NMRはかり方マニュアル 第2版 2

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

Microsoft Word - 演習5_蒸発装置


0.45m1.00m 1.00m 1.00m 0.33m 0.33m 0.33m 0.45m 1.00m 2

untitled

2

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

日本統計学会誌, 第44巻, 第2号, 251頁-270頁

温度計技術資料1.PDF

朕醩佑宖醸æ−žã†®ã†�ã‡†ã†®æ··å’‹æŁ´æŁ°è¨‹çfl»ã…¢ã…⁄ã…«

Undulator.dvi


Microsoft Word - ‚²‰ÆŸ_Ł¶−®’¬.doc

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

Folie 1

(1) 1.1


(1) (kn/m 3 )

Phase Diagrams and Microstructure of Ionic Microemulsion Systems Containing Various Monoalkyl Poly(oxyalkylene) Ethers Takamitsu TAMURA, Masako FUJITS

untitled

2005 1

Unidirectional Measurement Current-Shunt Monitor with Dual Comparators (Rev. B

ASB-3000 ユーザーズマニュアル

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


news

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

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

Nosé Hoover 1.2 ( 1) (a) (b) 1:

PowerPoint Presentation

PALL NEWS vol.126 November 2017

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

untitled

A

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 (

TSP信号を用いた音響系評価の研究

UWB a) Accuracy of Relative Distance Measurement with Ultra Wideband System Yuichiro SHIMIZU a) and Yukitoshi SANADA (Ultra Wideband; UWB) UWB GHz DLL

75 unit: mm Fig. Structure of model three-phase stacked transformer cores (a) Alternate-lap joint (b) Step-lap joint 3 4)

A Study of Adaptive Array Implimentation for mobile comunication in cellular system GD133

δf = δn I [ ( FI (N I ) N I ) T,V δn I [ ( FI N I ( ) F N T,V ( ) FII (N N I ) + N I ) ( ) FII T,V N II T,V T,V ] ] = 0 = 0 (8.2) = µ (8.3) G

Microsoft Word _abstract_kasai_ikeya2_tk.docx

NMR_wakate_ ppt

(MRI) 10. (MRI) (MRI) : (NMR) ( 1 H) MRI ρ H (x,y,z) NMR (Nuclear Magnetic Resonance) spectrometry: NMR NMR s( B ) m m = µ 0 IA = γ J (1) γ: :Planck c

mpctouch_userguide_v1.0-1

SN 2007bi Yoshida, T. & Umeda, H., MNRAS 412, L78-L82 (2011)

untitled

keisoku01.dvi

Yuzo Nakamura, Kagoshima Univ., Dept Mech Engr. perfect crystal imperfect crystal point defect vacancy self-interstitial atom substitutional impurity

IEEE ZigBee 2.4GHz 250kbps O-QPSK DSSS Bluetooth IEEE GHz 3Mbps G-FSK FHSS PC LAN IEEE b 2.4GHz 11Mbps CCK DSSS LAN LAN IEE

取扱説明書[d-01G]

1

untitled

untitled

15分でわかる(?)MRI

passive passive active 1 ( ) LTP 1 1) 2) 1 1

S I. dy fx x fx y fx + C 3 C dy fx 4 x, y dy v C xt y C v e kt k > xt yt gt [ v dt dt v e kt xt v e kt + C k x v + C C k xt v k 3 r r + dr e kt S dt d

CWContinuous Wave CW XCT(Computed Tomography) MRI Magnetic Resonance Imaging)PET(Positron Emission Tomography) XCT 2

1 a b cc b * 1 Helioseismology * * r/r r/r a 1.3 FTD 9 11 Ω B ϕ α B p FTD 2 b Ω * 1 r, θ, ϕ ϕ * 2 *

LT 低コスト、シャットダウン機能付き デュアルおよびトリプル300MHz 電流帰還アンプ

15分でわかる(?)MRI

charpter0.PDF


<4D F736F F D B B83578B6594BB2D834A836F815B82D082C88C60202E646F63>

untitled

untitled


 NMRの信号がはじめて観測されてから47年になる。その後、NMRは1960年前半までPhys. Rev.等の物理学誌上を賑わせた。1960年代後半、物理学者の間では”NMRはもう死んだ”とささやかれたということであるが(1)、しかし、これほど発展した構造、物性の

NMR 測定マニュアル(改訂版)

ADC121S Bit, ksps, Diff Input, Micro Pwr Sampling ADC (jp)

160GHz

2011de.dvi

機器分析化学 3.核磁気共鳴(NMR)法(1)

(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

Transcription:

PFG-NMR 004/11/3 006/05/05 PFG calibration Radiation-Damping PGSE-NMR 004 11 JEOL Hahn NMR Radiation Damping JEOL Einstein NMR NMR NMR NMR (artifact) DOSY Diffusion Ordered Spectroscopy 1

NMR University of Western Sydney Prof. W. S. Price 1993 3 STA fellow PFG JEOL JEOL 1997 JEOL 10 T/m (1,000 gauss/cm) PFG 19 F/ 1 H 003 1 0T/m PFG 15 N NMR 1983 JEOL Oxford 4.7T SCM JEOL GSH-00 (1991 ) 1996 TecMag Galaxy-MacNMR 00 TecMag Apollo-NTNMR JEOL JEOL 004 NMR NMR 70MHz SCM(6.3T) 1 H tuning 1 H 19 F tuning Apollo 1 H/ 19 F 10, NMR Dr. W. S. Price 1998 005 0 discussion

.1 Hahn Fick NMR Pulsed-filed Gradient Spin-Echo NMR, PGSE NMR 10-6 10-8 10-13 m s -1 5 o C.30x10-9 m s -1 SI.30x10-5 cm s -1 NMR NMR Hahn Hahn PFG Hahn 90 - -180 - - 90 o - -180 o - -Echo RF x x y RF 90 y xy xy y T T xy z- RF T1 xy RF x 3

x- x xy xy 180 RF (180 90 ) xy -y xy z- z,6 z 1 x z y z y 3 x RF (90 ) z τ z PFG 4 y 5 x RF ( 0 ) τ z PFG y 6 x Hahn 4

. Hahn PFG 0.01 0 T/m 10 000 gauss/cm 0.1ms 10ms PFG 90 180 Hahn PFG Hahn PFG PFG 1 PFG xy z z- z- SCM PFG 180 xy- PFG PFG xy PFG PFG PFG PFG T1 T NMR T1 T T1 T T1 T 10-9 10-11 PGSE-NMR 10-3 10-4 5

.3 Stejskal E. O. Stejskal and J. E. Tanner, Spin diffusion measurements: Spin echoes in the presence of a time-dependent field gradient, J. Chem. Phys. 4, 88-9 (1965). PFG PFG PFG E S0 E( δ, g, ) = S S 0 = exp( γ g δ D( δ / 3)) (1) 0-1 at 50 o C.1x10-10 m s -1 Li ( 7 Li) PF 6 ( 19 F) EC ( 1 H) DEC ( 1 H) ln(e/eo) - -3 4.6x10-10 m s -1 4.1x10-10 m s -1 3.75x10-10 m s -1 0 5x10 9 1x10 10 γ δ g ( δ/3) 3 LiPF6 EC/DEC 4.7T wide-bore SCM ( 1 H NMR-199.76 MHz) 50 o C ( ) 3mm 1H NMR g = 1.7 T/m, = 50 ms, δ = 0 1 ms 19F NMR g = 1.7 T/m, = 50 ms, δ = 0 1 ms g =.61 T/m, = 0 ms, δ = 0 1 ms ( ) 7Li NMR g =.61 T/m, = 50 ms, δ = 0 ms g = 3.95 T/m, = 0 ms, δ = 0 ms Ethylene carbonate (EC) Diethyl carbonate (DEC) 0:80(v/v) 1M LiPF 6 6

3. PFG calibration PFG calibration NMR Weingärtner H. Weingärtner, Self Diffusion in Liquid Water. A Reassessment Z. Phys. Chem. NF (Leipzig) 13, 19-149 (198). Weingärtner 5 o C (98.15 K).30 x 10-9 m s -1 (.30 10-5 cm /s) 5 o C 30 o C calibration 30 o C.55 x10-9 m s -1 PFG calibration 5mm 5mm PFG PFG 40 mm (spinning rate = 0 Spinning OFF ) Galaxy-MacNMR FID-shimming GSX BMS-005J 5mm 3 Hz 10 Hz SCM PFG SCM T1 Stejskal E( δ, g, ) = S S 0 = exp( γ g δ D( δ / 3)) 7

Stejskal D PFG T/m PFG ms PFG ms PFG PFG, D PFG Hahn T1 T D T1 T 90 1 PFG 0.5ms 0ms 100ms 50ms 0.05, 0.,.09, 1ms(10 ) S/N calibration calibration T1 00 MHz 30 o C 3 s SCM T1 T1 5 1 T/m (100 Gauss/cm) PFG.05 ~ 1ms( ) 50 ms 10 90 tuning 90 Sterjskal =0 ( =0.05ms) S0 ln( S S 0 ) = 7.1568 10 7 g δ D( δ /3) T/m ms m s -1 S R -0.9999 S/So NMR, 8

.55 x 10-9 m s -1 0-1 Pure H O at 30 o C - -3 ln(s/so) -4-5 -6-7 Parameter Value Error A 0.03478 0.01043 B -.56E-9 8.09E-1 -------------------------------------------- R SD N P --------------------------------------------- -0.99996 0.0 10 <0.0001 γ=0.85 T/m = 50 ms δ=0.01-1 ms 0 1x10 9 x10 9 3x10 9 γ δ g ( δ/3) 4 30 o C g=0.85t/m PFG calibration 1 H NMR DO H NMR H NMR DO H NMR 1 H NMR 1/6 6 PFG Weingärtner DO 5 o C 1.87 x 10-9 m s -1 HO/DO.11 x 10-9 m s -1 H/D PFG DO JEOL 1 H NMR 30 o C.15 x10-9 m s -1 H NMR.10 x10-9 m s -1 H NMR T1 = 0.51s 1 H NMR Sterjskal S 8 ln( ) = 1.6864 10 g δ D( δ /3) S 0 1 T/m 9

PFG PFG PFG Sterjskal E( δ, g, ) = exp( γ g δ D(4 δ ) / π ) / 0.4 60 % digital NMR PFG PFG Hahn 90 o - -180 o - -Echo T T T T1 T T xy- xy- T T1 T1 T D, Li, 3 Na, 7 Al T T1 Stimulated Echo Pulse Sequence STE STE Hahn 180 90 T 1 T1 1 PFG 10

PFG 16 STE PFG Hahn T 7 Li T STE Hahn T =5 ms NMR 0 ms 4 ms T PFG T Sterjskal PFG PFG JEOL 0T/m PFG NMR PFG-NMR ) PFG NMR HNMR 13 CNMR T1 T H NMR 13 C NMR H 13 CNMR LiBF4 LiPF6 BF4 19 F NMR 11 B NMR BF4 11 B NMR 19 F NMR PF6 19 F NMR 31 P 710Hz doublet 31 P NMR 6 F 6 F 1 P 31 P NMR 19 F NMR 31 P NMR 1 H NMR H NMR BF4 19 F NMR 11 B NMR 005 ENC Experimental NMR Conference 19F 11 B one-bond-coupling 1 H NMR 1 H- 1 H J-coupling Hahn 11

J-modulation J Hz cps cycle per second J = 7 Hz 1/πJ 0.03 s = 3 ms J Hahn =5 ms CH3CH J- xy- J eddy current effect PFG FID P0 P1 (1) S (power-spectrum) (1) NMR FID ADC Analogue-Digital Converter FID NMR NMR FT SN ADC NMR T1 (pulse-delay) T S/N 1H NMR 19 F NMR Radiation-Dumping X.-A. Mao and C.-H. Ye, Understanding Radiation Damping in a Simple Way, Concepts in Magnetic Resonance, 9, 173-187 (1997). HO Tuning 90 1

40Hz Tuning 90 FID FID 90 Tuning 90 4.7T-SCM (00MHz- 1 HNMR) 6.35T-SCM (70MHz- 1 HNMR) Radiation-dumping 90 90 90 ( ) NMR NMR 197 5 NMR 100 NMR TMS NMR NMR T1 FID BF NMR 1997 1998 1 St. Andrews 500 MHz SCM Kent 19 F NMR St. Andrew 1.76 x 10-10 13

m s -1 30 o C 1.8 x 10-10 m s -1 PFG.8 x 10-11 m s -1 3.4 x 10-11 m s -1 1% PFG Doty calibration ( 1 H-NMR ) Kent Ph.D 19 F NMR NMR 1 H 19 F 7 Li NMR SCM 7 L inmr 00 JEOL AL400 14T/m PFG multi-probe NMR NMR 4.7T-wide-bore SCM NMR 9.4T-narrow-bore SCM 30 o C 50 o C 70 o C 80 o C 60 o C 40 o C CH3O(OCHCHO)nCH (n= 50) neat n= diglyme DG (n=3 50) 00 K. Hayamizu, E. Akiba, T. Bando and Y.Aihara, 1 H, 7 Li and 19 F NMR and ionic conductivity studies for liquid electrolytes composed of glymes and polyetheneglycol dimethyl ethers of CH 3 O(CH CH O) n CH 3 (n=3 to 50) doped with LiN(SO CF 3 ) J. Chem. Phys. 117, 599-5939 (00). n=3 triglyme(tg) DG 5 o C DG 6 DG BMS-005J 5mm 14

60 DG 5mm-height sample tube 70 o C 50 D apparent (10-10 m s -1 ) 40 30 0 10 60 o C 50 o C 40 o C 0 o C 0 0 50 100 150 00 50 (ms) 6 3 4 artifact DG 0 7 Li 19 F 1H artifact artifact calibration 5 mm 7 5 mm DG 5 o C 1.01 mpas 0.890 mpas 8 6 30 ms 50 ms 50 o C 100 o C DG bp 16 o C mm K. Hayamizu, W. S. Price, A new type of sample tube for reducing convection effects in PGSE-NMR measurements of self-diffusion coefficients of liquid samples, J. Magn. Reson. 167 (004) 38-333. 15

5 mm mm Insert mm 3 mm 4 mm Outer tube 7 mm-30ms mm-50ms D (x10-10 m s -1 ) 10 100 o C mm-50ms 3mm-50ms 4mm-30ms 4mm-50ms 5mm-30ms 5mm-50ms 30 o C D x10-10 m s -1 1.5 3.0 3.5 4.0 4.5 1.5 3.0 3.5 4.0 4.5 10 1000/T DG 1000/T -40 o C 8 DG 16

7. JEOL NMR 10 H O.30 x10-9 m s -1 at 5 o C D HO (10-9 m s -1 ) 1.55 x 10-9 m s -1 at 30 o C 0 o C JEOL KH-0T KH-10T Weingartner WSP 0.1.6.8 3.0 3. 3.4 3.6 3.8 4.0 4. 1000/T 9 JEOL 003 1 KH-0T 003 1 0 T/m PFG mm NMR KH-10T 1997 10T /m PFG 5mm Weingärtner WSP W. S. Price, H. Ide, Y. Arata, Self-Diffusion of Supercooled Water to 38K Using PGSE NMR Diffusion Measurements, J. Phys. Chem. A, 103, 448-450(1999). 17

1 H NMR 19 F NMR DEC diethylcarbonate LiN(SO(CF3)) (LiTFSI ) 1M 30 o C ( 1 H NMR) 30 o C 10 1M LiTFSI in DEC (3mm-height) Solvent ( 1 H NMR) D (10-10 m s -1 ) 1 80 o C -40 o C Probes 10T-multi 10T-F/H 0T-multi 10T-F/H 0T-multi 30 o C Anion( 19 F NMR) 3.0 3.5 4.0 1000/T 10 3 1997 10T-multi-probe PFG (0.1ms-0.5ms) 1998 F/H-probe H 1 H 90 o H NMR 1 H NMR 19 F NMR tuning 003 0T-multi-probe H, F, Li PFG PFG PFG 10 JEOL 18

Radiation Damping NMR RF NMR Radiation Damping Radiation Damping Radiation Damping Radiation Damping RF 19

Z Z Y Y (Y) FID FID Radiation Damping 0