Feb 17, 2025
Version 1
Saturation Recovery for Quadrupolar Nuclei V.1
- Alexander L. Paterson1
- 1National Magnetic Resonance Facility at Madison (NMRFAM), University of Wisconsin-Madison, Madison, WI, United States
Protocol Citation: Alexander L. Paterson 2025. Saturation Recovery for Quadrupolar Nuclei. protocols.io https://dx.doi.org/10.17504/protocols.io.n92ldrjm7g5b/v1Version created by NMRFAM Facility
License: This is an open access protocol distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited
Protocol status: In development
We are still developing and optimizing this protocol, but it should be functional. We hope to solicit feedback primarily on clarity and usability. We intend to publish it in June 2025.
Created: February 14, 2025
Last Modified: February 17, 2025
Protocol Integer ID: 120388
Keywords: Measuring T1 via Saturation Recovery: 23Na, saturation recovery for quadrupolar nuclei purpose, quadrupolar nuclei purpose, saturation recovery, longitudinal relaxation time, resonances present in the sample, nuclei, recycle delay, recycle delays appropriate for the purpose, resonance, initial 1d experiment, completion of this sop, quadrupolar nuclei
Funders Acknowledgements:
National Science Foundation
Grant ID: 1946970
Abstract
Purpose
To measure the longitudinal relaxation time, T1, of resonances present in the sample.
Scope
This SOP should be completed after an initial 1D experiment has been completed, but before further experiments are performed. Upon completion of this SOP, the user will be able to set recycle delays appropriate for the purpose of later experiments, either to maximize signal per unit time, or to ensure quantitative intensities.
Guidelines
If acquisition of a 1D spectrum requires substantial signal averaging, this SOP may not be appropriate.
This SOP is written for acquisition using a Bruker console and TopSpin 3.6.2. It may be adapted to other TopSpin versions where appropriate. The basic process is the same on TopSpin 4.x, but requires a NEO-compatible pulse sequence. The sequence satrect1.neo.nmrfam is compatible.
This SOP is intended for a beginning user who has been trained on basic spectrometer safety and principles.
Materials
Definitions:
- T1: Longitudinal relaxation time
- l20: Number of saturation pulse loops
- d20: Presaturation loop delay
Appendix:
If the presaturation train is not completely effective, the recovery curve might initially decrease, and then follow the expected exponential curve. This is common behaviour and can be dealt with by discarding the initial points of the curve.
The values of the variable delay list T1_standard_array range from 0.25 to 128 s, increasing by a factor of two for each increment. This should provide adequate spacing to accurately determine T1 values between 1 s and 64 s. If necessary, adjust the list for shorter or longer values of T1.
Figure 1. Example of a successful 7Li saturation recovery experiment performed on a lithium silicate glass. The T1 of this environment was found to be 3.4 s.
Troubleshooting
Safety warnings
The minimum length of d1 for the 2D experiment will depend on whether decoupling is used during acquisition. If decoupling is used, d1 should be about 20 times as long as the acquisition period, typically on the order of 1 s. If decoupling is not used, a d1 value of 100 ms may be reasonable.
Before start
User is responsible for knowing the duty cycle of the probe and instrument being used.
User is responsible for knowing the high-power decoupling limits of the probe.
Expected time to completion: 1 hour or less
Procedure
Prepare the experimental environment.
Create a new experiment window.
Load the satrect1 pulse program.
Set the X pulse length, p1, and pulse power, pl1, to the previously measured pulse parameters. Ideally this would be either a non-selective or central-transition-selective 90° pulse.
Set the recycle delay, d1, to a relatively long value, e.g., 10 s.
Set the number of saturation pulse loops, l20, to 0.
Acquire an initial experiment. The number of scans should be as small as practicable to allow for adequate signal, ideally as low as 1.
Ensure that all expected resonances are visible. If some are not visible, either reduce the pulse length or increase d1, as appropriate.
Set the number of saturation pulse loops, l20, to an initial value of 10. Set the presaturation loop delay, d20, to an initial value of 100 µs. If a 90° pulse is not used, higher values of l20 may be required.
Acquire a spectrum. There should be no signal present.
If signal is still present, increase l20, up to a maximum of 100, and reacquire the spectrum.
If increasing l20 does not result in a null signal, reduce the number of loops and retry with longer presaturation loop delays d20.
If increasing d20 does not result in a null signal, retry with shorter presaturation loop delays d20.
Convert the experiment to a 2D experiment window.
Move to the acqupars window via the command ased.
Click on the button titled “Change acquisition dimension of current data set” and change the dimension to 2D.
Set the following parameters:
- vdlist: T1_standard_array.
- F1 TD: 12
- FnMODE: QF
- F1 SI: 16
- d1: A minimal value that respects the probe duty cycle, see Appendix.
Acquire the 2D experiment via the command zg.
Process the 2D experiment.
Transform the data using the command xf2.
Correct the F2 phasing of the slice with the longest delay period.
Do not transform or phase the F1 axis.
To process the data, launch the TopSpin utility t1guide and follow the workflow in the utility.
Extract the slice with the longest variable delay, i.e., the most recently acquired slice.
Integrate each resonance. Save using the option “Export Regions to Relaxation Module and .ret”.
- If resonances are not resolved, attempt to select the regions of least overlap.
- If resonances cannot be reasonably separated, integrating over all of the peaks will allow for the determination of the longest T1 component.
Enter the relaxation window and set the Fitting Function Function Type to uxnmrt1.
Calculate fit for all peaks. If successful, the fitting window should resemble the example in the appendix.
Record the T1 for each site. Use the longest value of T1 for determining the recycle delay of future experiments.
Protocol references
Bruker Solid State NMR User Manual Z4D10641B, Section 16.2.4
MacKenzie, K. J. D.; Smith, M. E. Multinuclear Solid-State NMR of Inorganic Materials; Elsevier, 2002.