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Signal encoding in magnetic particle imaging: properties of the system function

BACKGROUND: Magnetic particle imaging (MPI) is a new tomographic imaging technique capable of imaging magnetic tracer material at high temporal and spatial resolution. Image reconstruction requires solving a system of linear equations, which is characterized by a "system function" that est...

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Detalles Bibliográficos
Autores principales: Rahmer, Jürgen, Weizenecker, Jürgen, Gleich, Bernhard, Borgert, Jörn
Formato: Texto
Lenguaje:English
Publicado: BioMed Central 2009
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2684532/
https://www.ncbi.nlm.nih.gov/pubmed/19335923
http://dx.doi.org/10.1186/1471-2342-9-4
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author Rahmer, Jürgen
Weizenecker, Jürgen
Gleich, Bernhard
Borgert, Jörn
author_facet Rahmer, Jürgen
Weizenecker, Jürgen
Gleich, Bernhard
Borgert, Jörn
author_sort Rahmer, Jürgen
collection PubMed
description BACKGROUND: Magnetic particle imaging (MPI) is a new tomographic imaging technique capable of imaging magnetic tracer material at high temporal and spatial resolution. Image reconstruction requires solving a system of linear equations, which is characterized by a "system function" that establishes the relation between spatial tracer position and frequency response. This paper for the first time reports on the structure and properties of the MPI system function. METHODS: An analytical derivation of the 1D MPI system function exhibits its explicit dependence on encoding field parameters and tracer properties. Simulations are used to derive properties of the 2D and 3D system function. RESULTS: It is found that for ideal tracer particles in a harmonic excitation field and constant selection field gradient, the 1D system function can be represented by Chebyshev polynomials of the second kind. Exact 1D image reconstruction can thus be performed using the Chebyshev transform. More realistic particle magnetization curves can be treated as a convolution of the derivative of the magnetization curve with the Chebyshev functions. For 2D and 3D imaging, it is found that Lissajous excitation trajectories lead to system functions that are closely related to tensor products of Chebyshev functions. CONCLUSION: Since to date, the MPI system function has to be measured in time-consuming calibration scans, the additional information derived here can be used to reduce the amount of information to be acquired experimentally and can hence speed up system function acquisition. Furthermore, redundancies found in the system function can be removed to arrive at sparser representations that reduce memory load and allow faster image reconstruction.
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spelling pubmed-26845322009-05-20 Signal encoding in magnetic particle imaging: properties of the system function Rahmer, Jürgen Weizenecker, Jürgen Gleich, Bernhard Borgert, Jörn BMC Med Imaging Research Article BACKGROUND: Magnetic particle imaging (MPI) is a new tomographic imaging technique capable of imaging magnetic tracer material at high temporal and spatial resolution. Image reconstruction requires solving a system of linear equations, which is characterized by a "system function" that establishes the relation between spatial tracer position and frequency response. This paper for the first time reports on the structure and properties of the MPI system function. METHODS: An analytical derivation of the 1D MPI system function exhibits its explicit dependence on encoding field parameters and tracer properties. Simulations are used to derive properties of the 2D and 3D system function. RESULTS: It is found that for ideal tracer particles in a harmonic excitation field and constant selection field gradient, the 1D system function can be represented by Chebyshev polynomials of the second kind. Exact 1D image reconstruction can thus be performed using the Chebyshev transform. More realistic particle magnetization curves can be treated as a convolution of the derivative of the magnetization curve with the Chebyshev functions. For 2D and 3D imaging, it is found that Lissajous excitation trajectories lead to system functions that are closely related to tensor products of Chebyshev functions. CONCLUSION: Since to date, the MPI system function has to be measured in time-consuming calibration scans, the additional information derived here can be used to reduce the amount of information to be acquired experimentally and can hence speed up system function acquisition. Furthermore, redundancies found in the system function can be removed to arrive at sparser representations that reduce memory load and allow faster image reconstruction. BioMed Central 2009-04-01 /pmc/articles/PMC2684532/ /pubmed/19335923 http://dx.doi.org/10.1186/1471-2342-9-4 Text en Copyright ©2009 Rahmer et al; licensee BioMed Central Ltd. http://creativecommons.org/licenses/by/2.0 This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Research Article
Rahmer, Jürgen
Weizenecker, Jürgen
Gleich, Bernhard
Borgert, Jörn
Signal encoding in magnetic particle imaging: properties of the system function
title Signal encoding in magnetic particle imaging: properties of the system function
title_full Signal encoding in magnetic particle imaging: properties of the system function
title_fullStr Signal encoding in magnetic particle imaging: properties of the system function
title_full_unstemmed Signal encoding in magnetic particle imaging: properties of the system function
title_short Signal encoding in magnetic particle imaging: properties of the system function
title_sort signal encoding in magnetic particle imaging: properties of the system function
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2684532/
https://www.ncbi.nlm.nih.gov/pubmed/19335923
http://dx.doi.org/10.1186/1471-2342-9-4
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