Spin-Lock Induced Crossing for Singlet State Creation

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Solution Overview

Problem

Nuclear magnetic resonance (NMR) spectroscopy faces challenges in chemical identification of molecules due to overlapping resonance frequencies, and existing methods for creating nuclear spin singlet states are inefficient, especially at low magnetic fields where conventional spin-lattice relaxation times are long, leading to significant magnetization loss before singlet state transfer.

Innovation Solution

The method involves using weak spin-locking with a nutation frequency matched to the J-coupling between nuclei to drive transitions between dressed states, specifically employing the spin-lock induced crossing (SLIC) sequence for efficient magnetization transfer from triplet to singlet states, which occurs throughout the spin-locking process, minimizing relaxation losses and allowing for better identification of molecules.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If conventional M2S sequences are used to create singlet states, then singlet state transfer can be achieved, but magnetization loss occurs due to spin-lattice relaxation during the sequence execution

Engineering Contradiction:
Improvesinglet state creation efficiencyVSAvoidmagnetization loss
Core Design Contradiction:
ReliabilityVSLoss of energy

Solution Approach 1:

The spin-locking sequence applies continuous RF irradiation throughout the entire singlet state creation process, maintaining the spin system in a locked state where magnetization is continuously transferred to the singlet state without interruption. This continuous action eliminates the idle periods in conventional sequences where magnetization would relax, thereby preventing magnetization loss while maintaining high singlet state creation efficiency.

Inventive Principle:
Principle #20Continuity of useful action

Solution Approach 2:

The method applies spin-locking before the singlet state creation is complete, preparing the spin system in advance by locking the magnetization and creating the conditions necessary for efficient singlet state transfer. This preliminary locking action ensures that the spin system is optimally positioned throughout the process, preventing relaxation losses that would occur if waiting until the end to create the singlet state.

Inventive Principle:
Principle #10Preliminary action

2Reliability

If longer pulse sequences are used to transfer magnetization to singlet state, then transfer can be achieved, but spin-lattice relaxation causes significant magnetization loss

Engineering Contradiction:
Improvemagnetization transferVSAvoidsequence execution time
Core Design Contradiction:
ReliabilityVSLoss of time

Solution Approach 1:

The spin-locking sequence executes the magnetization transfer process continuously in a single uninterrupted action, eliminating the multiple discrete pulse steps required by conventional sequences. This continuous transfer occurs throughout the entire spin-locking duration, achieving complete magnetization transfer to the singlet state in one efficient operation rather than through multiple time-consuming steps, thereby minimizing both time loss and relaxation losses.

Inventive Principle:
Principle #20Continuity of useful action

3Reliability

If weak spin-locking is applied continuously, then magnetization transfer to singlet state occurs throughout the process, but requires precise matching of nutation frequency to J-coupling

Engineering Contradiction:
Improvesinglet state creation efficiencyVSAvoidparameter matching precision
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The method utilizes the relationship between spin-locking strength and transfer efficiency by optimizing the nutation frequency to match the J-coupling constant. By changing the RF field strength parameter to achieve the precise matching condition, the system maximizes singlet state creation efficiency. This parameter optimization transforms a potentially complex control problem into a straightforward tuning procedure where the RF field strength is adjusted to match the known J-coupling value of the spin system.

Inventive Principle:
Principle #35Parameter changes

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

SLIC achieves 19% to 75% more efficient singlet state creation compared to existing M2S sequences, enabling effective chemical identification even at low magnetic fields by minimizing relaxation losses and allowing for immediate transfer to the singlet state, thus improving the accuracy and efficiency of NMR spectroscopy.

Implementation Method 1

weak spin locking can drive transitions between dressed states of a multi-spin system

Methodology Applied
Scientific EffectSpin-locking:

Implementation Method 2

spin-locking with a nutation frequency matched to the J-coupling between two nuclei of interest

Methodology Applied
Scientific EffectNutation:

Implementation Method 3

J-coupling between two nuclei of interest

Methodology Applied
Scientific EffectJ-coupling:

Implementation Method 4

spin lattice relaxation time, T1

Methodology Applied
Scientific EffectSpin-lattice relaxation:

Data Source

PatentUS10101423B2Creation of nearly-equivalent nuclear spin singlet states using spin-lock induced crossing
Publication Date: 2018.10.16 PRESIDENT & FELLOWS OF HARVARD COLLEGE
  • US10101423B2 patent drawing
  • US10101423B2 patent drawing
  • US10101423B2 patent drawing

AI summary

Methods and systems for Nuclear Magnetic Resonance (NMR) spectra of samples having unresolved peaks are described. The methods and systems allow for the creation nuclear spin singlet states in nearly-equivalent spin pairs, for example, using continuous spin-locking with a nutation frequency matched to the coupling strength between spins. The invention relates generally to the field Nuclear Magnetic Resonance (NMR). Nuclear magnetic resonance (NMR) spectroscopy can be used as a tool for determining the chemical structure and/or geometry of a molecule in a sample. In many samples, however, resonance frequencies of different nuclei fully or partially overlap, which makes chemical identification of molecule(s) in a sample difficult or impossible.