MRI Acquisition Parameter Optimization for Precision and Time

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Solution Overview

Problem

Current MRI techniques face challenges in increasing signal-to-noise ratio (SNR) efficiently, particularly at higher field strengths, due to limitations in acquisition parameter optimization and the impact of radio-frequency inhomogeneity, which affects the accuracy of T1 relaxation time measurements.

Innovation Solution

The method involves determining optimal acquisition parameters based on a given imaging time to enhance SNR, using a cost function that minimizes errors and accounts for restrictions such as total imaging time, hardware limitations, and radio-frequency power deposition, allowing for faster precision gains than proportional to the square root of time.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If traditional MRI acquisition methods are used, then imaging can be performed with standard parameters, but signal-to-noise ratio (SNR) increases only proportionally to the square root of time and precision is limited

Engineering Contradiction:
Improveprecision of T1 and T2 estimatesVSAvoidimaging time
Core Design Contradiction:
Measurement precisionVSLoss of time

Solution Approach 1:

The patent applies parameter changes by systematically varying multiple acquisition parameters (flip angles, repetition times, echo times, number of averages) to optimize the precision of T1 and T2 measurements. The cost function evaluates different parameter combinations to identify those that maximize measurement precision within the given time constraint, achieving up to 90% precision improvement over traditional methods.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent implements dynamics by making the acquisition parameters adaptive rather than fixed. The system dynamically adjusts parameters based on the cost function evaluation, allowing the measurement protocol to optimize its parameters in real-time according to the specific imaging requirements and time available, thereby achieving faster precision gains than the traditional square root of time scaling.

Inventive Principle:
Principle #15Dynamics

2Measurement precision

If multiple averages are used to increase SNR, then measurement precision improves, but total imaging time increases

Engineering Contradiction:
ImproveSNRVSAvoidmeasurement time
Core Design Contradiction:
Measurement precisionVSDuration of action of moving object

Solution Approach 1:

The patent changes the parameter of number of averages from a fixed traditional value to an optimized value determined by the cost function. The cost function calculates the optimal number of averages that achieves the desired SNR improvement while minimizing the time penalty, allowing for more efficient use of averaging to improve precision without linearly increasing measurement time.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent applies partial action by using fewer averages than traditional methods would require for the same SNR level, compensating by optimizing other parameters such as flip angles and repetition times. This partial averaging approach, combined with parameter optimization, achieves comparable or superior precision with reduced total measurement time.

Inventive Principle:
Principle #16Partial or excessive action

3Measurement precision

If higher field strength MRI is used, then signal-to-noise ratio improves, but radio-frequency inhomogeneity increases affecting measurement accuracy

Engineering Contradiction:
Improvesignal-to-noise ratioVSAvoidaccuracy of T1 relaxation time measurements
Core Design Contradiction:
Measurement precisionVSReliability

Solution Approach 1:

The patent implements feedback by incorporating the actual flip angle measurements (which account for RF inhomogeneity effects) into the cost function evaluation. The system measures the actual flip angles achieved during acquisition and uses this feedback information to adjust and optimize the acquisition parameters, thereby compensating for RF inhomogeneity and maintaining measurement accuracy at higher field strengths.

Inventive Principle:
Principle #23Feedback

Solution Approach 2:

The patent applies preliminary action by performing flip angle measurements and characterizing RF inhomogeneity effects before final T1 and T2 quantification. This preliminary characterization allows the system to pre-correct for RF inhomogeneity effects in the acquisition parameter optimization, ensuring accurate measurements from the outset rather than requiring post-processing corrections.

Inventive Principle:
Principle #10Preliminary action

4Measurement precision

If acquisition parameters are fixed by hardware limitations, then system complexity is reduced, but optimization freedom is limited reducing precision gains

Engineering Contradiction:
Improvequantitative MRI metrics precisionVSAvoidparameter optimization complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent applies dynamics by implementing a systematic method that dynamically evaluates and adjusts multiple acquisition parameters within the constraints of hardware limitations. The cost function framework provides a structured approach to navigate the complex parameter space, automatically identifying optimal parameter combinations that respect hardware constraints while maximizing measurement precision, thereby managing complexity through algorithmic optimization rather than manual tuning.

Inventive Principle:
Principle #15Dynamics

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

This approach significantly improves the precision of quantitative MRI metrics, such as T1 and T2 estimates, by up to 90% for the same sample, sequence, and duration, and can achieve comparable or superior precision to existing methods while optimizing imaging time.

Implementation Method 1

Radio waves are generally transmitted through the patient's body. The pulse used to transmit waves through the patient's body may be referred to as the excitation pulse. This affects the patient's atoms by forcing the nuclei of some atoms into an excited state.

Methodology Applied
Scientific EffectRadio frequency excitation: Electromagnetic Induction

Implementation Method 2

As such nuclei return into their ground state, they transmit their own radio waves. An MRI scanner picks up or acquires those radio waves

Methodology Applied
Scientific EffectSpin relaxation:

Implementation Method 3

The T1 relaxation time is a measure of the time taken to realign with the external magnetic field. The T1 constant may indicate how quickly the spinning nuclei will emit their absorbed RF into the surrounding tissue.

Methodology Applied
Scientific EffectT1 relaxation:

Implementation Method 4

The T2 relaxation time is dependent on the exchanging of energy with nearby nuclei. T2 is the decay of the magnetization perpendicular to the main magnetic field

Methodology Applied
Scientific EffectT2 relaxation:

Implementation Method 5

An MRI scanner picks up or acquires those radio waves, and a computer transforms these waves into images, e.g., based on the location and strength of the incoming magnetic waves.

Methodology Applied
Scientific EffectMagnetic field gradient encoding: Magnetic Field

Data Source

PatentUS7906964B2Method and system for determining acquisition parameters associated with magnetic resonance imaging for a particular measurement time
Publication Date: 2011.03.15 NEW YORK UNIV
  • US7906964B2 patent drawing
  • US7906964B2 patent drawing
  • US7906964B2 patent drawing

AI summary

An exemplary embodiment of system, computer-accessible medium and method for determining exemplary values for acquisition parameters for a given time (e.g., imaging time) is provided, e.g., with the exemplary values being selectable to increase the signal-to-noise ratio. According to certain exemplary embodiments of the present disclosure, data (e.g., image data) associated with at least one portion of a target can be generated. For example, a first signal from the target resulting from at least one first excitation pulse forwarded toward the target can be acquired using a plurality of acquisition parameters having first values. Further, a second signal from the target resulting from at least one second excitation pulse forwarded toward the target can be acquired using a plurality of acquisition parameters having second values, with the second values being different from the first values. The data (e.g., image data) may be generated based on the first and second signals.