Principios Básicos de RMN en sólidos destinado a usuarios. Gustavo Monti. Fa.M.A.F. Universidad Nacional de Córdoba Argentina

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Transcription:

Principios Básicos de RMN en sólidos destinado a usuarios Gustavo Monti Fa.M.A.F. Universidad Nacional de Córdoba Argentina

magnet 1 2 4 5 6 computer 3 Block diagrama of a traditional NMR spectrometer. 1 probe, 2 signal preamplifier, 3 transmitter and power amplifier, 4 receptor, 5 detector (here the RF signal from the nuclei is converted into audio frequency signal), 6 analog to digital converter.

CPMAS probe, 7 mm rotor, coil and its stator. 4.7 T superconducting magnet, equivalent to a frequency of 300 MHz for protons. 1000 MHz (1 GHz) magnet

1 4 2 5 3 6 Nuclear Magnetic Resonance Spectrometer, Bruker Avance II 1) Computer 2) frequency generator, transmission and reception 3) High Power Amplifier 4) pneumatic unit sample rotation 5) Temperature control 6) Control of magnetic field external homogenization coils

Overview Setup procedures for magic angle adjustment probe shimming cross polarization: Hartmann-Hahn match decoupling considerations

Why Do CP/MAS? MAS = Magic Angle Spinning line narrowing 54.7! 2 ( 3cos θ 1) = 0 θ = 54. 7 CP = Cross Polarization signal enhancement: γ I /γ S 1 H 13 abundant C : x 4 spins 1 H 15 (e. g. N : x 10 1 H) rare spins (e. g. 13 C)

Magic Angle Adjustment Requirements for setup sample: sensitive to angle setting: large interaction to be averaged by MAS narrow lines achievable more sensitive than samples of interest easy to observe: large signal at desired observe frequency 54.7

Magic Angle Adjustment Standard setup sample ( 13 C work): KBr with 79 Br detection criterion: spinning sidebands sensitive to magic angle due to broad (MHz) quadrupolar interaction narrow lines close to 13 C frequency (300 MHz spectrometer: 75.16 MHz vs. 75.43 MHz), no change in routing, filters, preamplifier, probe range etc. required good S/N (single scan)

Magic Angle Adjustment x 16 setting the magic angle with KBr (79Br detection) spinning speed 5 khz angle well set x 8 0-2 -4-6 -8-10 -12-14 -16 ppm 400 200 0-200 ppm

Magic Angle Adjustment x 16 setting the magic angle with KBr (79Br detection) spinning speed 5 khz angle misset (by about 1/4 turn) x 8 0-2 -4-6 -8-10 -12-14 -16 ppm 400 200 0-200 ppm

Magic Angle Adjustment x 16 setting the magic angle with KBr (79Br detection) spinning speed 5 khz angle grossly misset (by about 1 turn) x 8 0-2 -4-6 -8-10 -12-14 -16 ppm 400 200 0-200 ppm

Probe Shimming Some hints: shimming is done on FID or spectrum (no lock used) usually requirements are less demanding as compared to liquids (e. g. 13 C: < 10 Hz) MAS on axis and off axis shims are a combination of standard on axis (z, z 2,...) and off axis (x, y,...) shims at high spinning speeds: MAS off axis shims less important

Probe Shimming relation of MAS (tilted) and laboratory frame shims first order B B B tilt z tilt x tilt y = = = 1 B 3 1 B 3 B lab y lab z lab x 2 3 2 3 B B lab x lab z z lab 54.7 z tilt x lab B tilt 2 z = B lab 2 ( x y 2 ) 2 2B lab zx A. Sodickson and D. G. Cory, J. Magn. Reso. 128, 87 (1997) second order B B tilt zx tilt zy = = 1 3 1 3 B B lab zx lab zy + 2 6 2 3 B B lab 2 z lab xy 2 6 B lab 2 2 ( x y )

Probe Shimming 13 C resolution with adamantane x 8 x 8 FWHMH > 2 Hz 13 C- 13 C satellite ~30 Hz 3900 3850 Hz 3000 2950 Hz 80 70 60 50 40 30 20 10 0 ppm

Cross Polarization - Basic Principles energy level matching: Hartmann-Hahn matching laboratory rotating laboratory frame, I spin frame frame, S spin ω0,i ω = 1,I ω1,s ω 0, S ω ω 0,I 1,I = γ B I I = γ B 0 1,I Hartmann-Hahn match: γ B = γ B I 1,I S 1, S

Basic CP(MAS) Pulse Sequence 90 x 1 H contact decoupling 13 C contact aquire

Cross Polarization What can be achieved: signal enhancement by polarization transfer: nucleus natural abundance max. enhancement factor 13 C 1.11 % 4 15 N 0.37 % 10 29 Si 4.70 % 5 31 P 100 % 2.5 γ I γ S ε = 1 1 + ε N N S I faster repetition: recycle delay ~ 5 T 1, 1 H usually T 1, 1 H << T 1, 13 C (T 1, 15 N )

Cross polarisation: criteria robustness: width of Hartmann-Hahn-condition dependence on rotation frequency γ 1 B 1 = γ 2 B 1 + n 2 πν rot efficiency f max = γ 1 γ H X recycle delay is now determined by 1 H T 1 BUT: consider probe duty cycle!!

13 C CPMAS Setup Using Glycine CPMAS spectrum of glycine (5 khz spinning speed) Carbxyl 13 C: sensitive HH match easy to decouple sensitive to angle HOOC-CH 2 -NH 2 13 C a : broad HH match high power decoupling 240 220 200 180 160 140 120 100 80 60 40 20 0-20 ppm

Hartmann-Hahn matching profiles Glycine 13 C signal amplitudes as function of 1 H RF field 13 C RF field constant at 45 khz using square pulses for CP CH 2 CH 2 CO MAS = 2500 Hz CO MAS = 12500 Hz 75 70 65 60 55 50 45 40 35 30 25 khz Ha-Ha-match 75 70 65 60 55 50 45 40 35 30 25 khz Ha-Ha-match

Hartmann-Hahn matching profiles What is the reason for these intensity modulations? The homonuclear proton-proton dipole coupling is modulated by the spin rate! Proton matching carbon energy level energy level CH 2 SR SR CO SR SR CO MAS = 12500 Hz 75 70 65 60 55 50 45 40 35 30 25 khz Ha-Ha-match

Ramped (Variable Amplitude) Cross Polarization 90 x 1 H contact decoupling 13 C contact acquire

Hartmann-Hahn matching profiles Glycine 13 C signal amplitudes as function of 1 H RF field 13 C RF field constant at 45 khz using ramp pulse for CP from 100% to 50% amplitude CH 2 CO CH 2 CO MAS MAS = 2500 = 2500 Hz Hz CO MAS = 12500 Hz CH 2 75 70 65 60 55 50 45 40 35 30 25 khz Ha-Ha-match 75 70 65 60 55 50 45 40 35 30 25 khz Ha-Ha-match

VACP: possible problems Actual transfer occurs during precise match to spinning sideband! -transfer does not occur during the whole pulse -proton spin lock field not at constant high level, proton T 1ρ may be shortened Optimum setup: Flat (10)% ramp over first sideband to higher power, just to compensate for misset and drift. However: Must be optimised for spin rate!

Cross Polarization Dynamics contact time, practical considerations for 13 C short T IS (~500 ms): directly attached protons (-CH 3, -CH 2 -, >CH-) long T IS (>1-2 ms): quaternary carbons (>C<, -COO-, substituted aromatic systems,...), high mobility short T 1ρ : paramagnetic systems/impurities (e.g. in coal), high mobility

TPPM decoupling TPPM = Two Pulse Phase Modulation ( ) ( ) ( ) ( ) τ τ τ τ p 0 p ϕ p 0 p ϕ pulse duration: τ p τ p - ε: ε 0 0.6 µs, to be optimised! phase step: ϕ 15, optimise, if needed!

TPPM: optimisation of τ p C α signal in glycine-1,2-13 C- 15 N, ν rot = 30 khz, ϕ = 15 ν dec = 150 khz 2.0 2.5 3.0 3.5 4.0 4.5 τ p /ms optimum pulse length: τ p = 2.9 µs, (τ = 3.2 µs)

SPINAL decoupling τ ϕ τ ϕ ' SPINAL = Small Phase Incremental Alternation τ ϕ '' τ ϕ '' ' basic cycle: Q= φ φ φ φ = 10-10 15-15 20-20 15-15 Q= -φ -φ -φ -φ = -10 10-15 15-20 20-15 15 super cycles: SPINAL16 = Q Q SPINAL32 = Q Q Q Q SPINAL64 = Q Q Q Q Q Q Q Q SPINAL128 = Q Q Q Q Q Q Q Q Q Q Q Q Q Q Q Q

Decoupling bandwidth - comparison Line width of C α in Glycine at ν rot = 5 khz, 400 MHz ν 1dec = 100 khz

Decoupling bandwidth - comparison Line width of C α in Glycine at ν rot = 5 khz, 400 MHz ν 1dec = 70 khz

Residual line width 13 C CP spectra of cortisone acetate at ν dec = 104 khz and ν rot = 11 khz, 400 MHz 240 220 200 180 160 140 120 100 80 60 40 20 0-20 ppm SPINAL 64 TPPM 15 CW 205 204 203 ppm 126 125 124 ppm 37 36 ppm

Residual line width 13 C CP spectra of starch at ν dec = 104 khz and ν rot = 11 khz, 400 MHz SPINAL 64 TPPM 15 190 180 170 160 150 140 130 120 110 100 90 80 70 60 50 40 30 20 10 ppm

CPMAS Setup with Glycine angle well set angle < magic angle (1/4 turn out) angle > magic angle (1/4 turn in) angle > magic angle (3/4 turn in) angle < magic angle (3/4 turn out) 13 C-carbonyl HH-match magic angle setting (probe shimming) 13 C a decoupling power offset method S/N 200 150 100 50 ppm 18000 17800 17600 Hz

Cross Polarization for Various Nuclei standard: I=1/2 S=1/2: most frequent: I = 1 H S = 13 C, 15 N, 29 Si, 31 P less common, but worthwile: I = 1 H S = 77 Se, 89 Y, 113 Cd, 119 Sn, 129 Xe, 195 Pt, 199 Hg, 207 Pb fluorinated materials: I = 19 F S = 13 C, 15 N, 29 Si, 31 P, low g nuclei (e. g. 15 N): more X and/or less 1 H power quadrupolar nuclei: different story...

15N CPMAS Setup with Glycine HOOC-CH 2 -NH 2 7mm probe ramped CP 5 khz spinning speed 4 scans 100 0-100 Hz 350 300 250 200 150 100 50 0-50 -100-150 -200-250 -300 ppm

CP throughout the periodic table

CP throughout the periodic table

CP throughout the periodic table

Chart of all 29 X nuclei with spin ½

CP of standard nuclei

CP of exotic nuclei

Some reference compounds for CP set-up