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Related Concept Videos

Magnetic Resonance Imaging01:24

Magnetic Resonance Imaging

Magnetic resonance imaging (MRI) is a noninvasive medical imaging technique based on a phenomenon of nuclear physics discovered in the 1930s, in which matter exposed to magnetic fields and radio waves was found to emit radio signals. In 1970, a physician and researcher named Raymond Damadian noticed that malignant (cancerous) tissue gave off different signals than normal body tissue. He applied for a patent for the first MRI scanning device in clinical use by the early 1980s. The early MRI...
NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
Atomic Nuclei: Magnetic Resonance01:05

Atomic Nuclei: Magnetic Resonance

The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
NMR Spectroscopy: Chemical Shift Overview01:15

NMR Spectroscopy: Chemical Shift Overview

The position of the absorption signal of a sample is reported relative to the position of the signal of tetramethylsilane (TMS), which is added as an internal reference while recording spectra. The difference between the absorption frequencies of the sample and TMS (in Hz) is divided by the spectrometer operating frequency (in MHz) to obtain a dimensionless quantity called the chemical shift. It is reported on the δ (delta) scale and expressed in parts per million.
For instance, the proton...
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis. This...
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...

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Frequency Mixing Magnetic Detection Scanner for Imaging Magnetic Particles in Planar Samples
07:01

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Published on: June 9, 2016

Linearity and shift invariance for quantitative magnetic particle imaging.

Kuan Lu1, Patrick W Goodwill, Emine U Saritas

  • 1Deparment of Engineering, University of California, Berkeley, CA 94720, USA.

IEEE Transactions on Medical Imaging
|April 10, 2013
PubMed
Summary

Magnetic Particle Imaging (MPI) can now be fully quantitative. A new algorithm restores lost information from filtering, ensuring linearity and shift invariance (LSI) for improved diagnostic utility in medical imaging.

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Area of Science:

  • Medical Imaging
  • Biomedical Engineering
  • Physics

Background:

  • Magnetic Particle Imaging (MPI) is a non-ionizing, high-contrast imaging technique with clinical potential.
  • Linearity and shift invariance (LSI) are critical for quantitative imaging but are compromised in practical MPI by filtering.
  • Existing filtering methods remove essential data, hindering MPI's diagnostic accuracy.

Purpose of the Study:

  • To theoretically and experimentally describe image artifacts caused by filtering in MPI.
  • To develop and validate a robust algorithm for restoring lost information in x-space MPI.
  • To re-establish the linearity and shift invariance (LSI) properties of MPI scans.

Main Methods:

  • Detailed theoretical analysis of filtering-induced artifacts in MPI.
  • Development of a novel algorithm to recover lost LSI information.
  • Simulations and experimental validation of the proposed algorithm on x-space MPI data.

Main Results:

  • Identified and characterized specific image artifacts resulting from high-pass filtering in MPI.
  • Demonstrated the algorithm's effectiveness in restoring lost spatial frequency information.
  • Provided theoretical, simulated, and experimental evidence of restored LSI properties.

Conclusions:

  • The developed algorithm successfully restores the linearity and shift invariance (LSI) of Magnetic Particle Imaging (MPI).
  • This advancement enables more accurate quantification and enhances diagnostic capabilities for various clinical applications of MPI.
  • The findings pave the way for improved clinical translation of MPI technology.